%% $Id$
%% This file was automatically generated by Pencil::DocExtractor,
%% so think twice before you modify it.
%%
%% Source files:
%%   cdata.f90
%%   hydro.f90
%%   density.f90
%%   entropy.f90
%%   magnetic.f90
%%   pscalar.f90
%%   1D_loop.f90
%%   advective_gauge.f90
%%   anelastic.f90
%%   axionSU2back.f90
%%   axionSU2back_using_ode.f90
%%   axionSU2back_using_ode2.f90
%%   backreact_infl.f90
%%   bfield.f90
%%   chemistry.f90
%%   chemistry_simple.f90
%%   chiral_mhd.f90
%%   collapse.f90
%%   coronae.f90
%%   cosmicray_current.f90
%%   density_stratified.f90
%%   detonate.f90
%%   disp_current.f90
%%   dustdensity.f90
%%   entropy_anelastic.f90
%%   gravitational_waves.f90
%%   gravitational_waves_hTXk.f90
%%   gravitational_waves_hTXk_no_xpara.f90
%%   gravitational_waves_hij6.f90
%%   gravity_simple.f90
%%   heatflux.f90
%%   hydro_kinematic.f90
%%   hydro_marked.f90
%%   hydro_potential.f90
%%   interstellar.f90
%%   lorenz_gauge.f90
%%   lucky_droplet.f90
%%   magnetic_shearboxJ.f90
%%   maxwell.f90
%%   meanfield.f90
%%   meanfield_demfdt.f90
%%   neutralvelocity.f90
%%   noentropy.f90
%%   particles_caustics.f90
%%   particles_chemistry.f90
%%   particles_dust.f90
%%   particles_dust_brdeplete.f90
%%   particles_lagrangian.f90
%%   particles_mass_swarm.f90
%%   particles_surfspec.f90
%%   particles_tetrad.f90
%%   polymer.f90
%%   radial_dist_func.f90
%%   reaction_0D.f90
%%   rel_1d.f90
%%   selfgravity.f90
%%   shear.f90
%%   shock.f90
%%   shock_highorder.f90
%%   solar_corona.f90
%%   solid_cells_CGEO.f90
%%   solid_cells_ogrid_chemistry.f90
%%   solid_cells_reactive.f90
%%   temperature_idealgas.f90
%%   temperature_ionization.f90
%%   test_chemistry.f90
%%   testfield_axisym.f90
%%   testfield_axisym2.f90
%%   testfield_axisym4.f90
%%   testfield_compress_z.f90
%%   testfield_meri.f90
%%   testfield_nonlin_z.f90
%%   testfield_x.f90
%%   testfield_xz.f90
%%   testfield_z.f90
%%   testflow_z.f90
%%   testperturb.f90
%%   testscalar.f90
%%   testscalar_axisym.f90
%%   testscalar_simple.f90
%%   thermal_energy.f90
%%   visc_smagorinsky.f90
%%   viscosity.f90

% ---------------------------------------------------------------- %
\begin{longtable}{lp{0.7\textwidth}}
\toprule
  \multicolumn{1}{c}{\emph{Variable}} & {\emph{Meaning}} \\
\midrule
  \multicolumn{2}{c}{Module \file{cdata.f90}} \\
\midrule
  \var{it}        & number of time step
                    \quad(since beginning of job only) \\
  \var{t}         & time $t$ \quad(since start.csh) \\
  \var{dt}        & time step $\delta t$ \\
  \var{walltime}  & wall clock time since start of
                    run.x, in seconds \\
  \var{Rmesh}     & $R_{\rm mesh}$ \\
  \var{Rmesh3}    & $R_{\rm mesh}^{(3)}$ \\
  \var{maxadvec}  & maxadvec \\
\midrule
  \multicolumn{2}{c}{Module \file{hydro.f90}} \\
\midrule
  \var{u2tm}      & $\left<\uv(t)\cdot\int_0^t\uv(t')
                    dt'\right>$ \\
  \var{uotm}      & $\left<\uv(t)\cdot\int_0^t\omv(t')
                    dt'\right>$ \\
  \var{outm}      & $\left<\omv(t)\cdot\int_0^t\uv(t')
                    dt'\right>$ \\
  \var{fkinzm}    & $\left<{1\over2} \varrho\uv^2 u_z\right>$ \\
  \var{gamm}      & $\left<gamma\right>$ \\
  \var{gamrms}    & $\left<\gamma^2\right>^{1/2}$ \\
  \var{gammax}    & $\max(\gamma)$ \\
  \var{u2m}       & $\left<\uv^2\right>$ \\
  \var{u2sphm}    & $\int_{r=0}^{r=r_{\rm diag}} \uv^2 dV$,
                    where $r=\sqrt{x^2+y^2+z^2}$ \\
  \var{uxpt}      & $u_x(x_1,y_1,z_1,t)$ \\
  \var{uypt}      & $u_y(x_1,y_1,z_1,t)$ \\
  \var{uzpt}      & $u_z(x_1,y_1,z_1,t)$ \\
  \var{uxp2}      & $u_x(x_2,y_2,z_2,t)$ \\
  \var{uyp2}      & $u_y(x_2,y_2,z_2,t)$ \\
  \var{uzp2}      & $u_z(x_2,y_2,z_2,t)$ \\
  \var{uxuypt}    & $(u_x u_y)(x_1,y_1,z_1,t)$ \\
  \var{uyuzpt}    & $(u_y u_z)(x_1,y_1,z_1,t)$ \\
  \var{uzuxpt}    & $(u_z u_x)(x_1,y_1,z_1,t)$ \\
  \var{urms}      & $\left<\uv^2\right>^{1/2}$ \\
  \var{urmsx}     & $\left<\uv^2\right>^{1/2}$ for
                    the hydro_xaver_range \\
  \var{urmsz}     & $\left<\uv^2\right>^{1/2}$ for
                    the hydro_zaver_range \\
  \var{durms}     & $\left<\delta\uv^2\right>^{1/2}$ \\
  \var{umax}      & $\max(|\uv|)$ \\
  \var{umin}      & $\min(|\uv|)$ \\
  \var{uxrms}     & $\left<u_x^2\right>^{1/2}$ \\
  \var{uyrms}     & $\left<u_y^2\right>^{1/2}$ \\
  \var{uzrms}     & $\left<u_z^2\right>^{1/2}$ \\
  \var{uxmin}     & $\min(|u_x|)$ \\
  \var{uymin}     & $\min(|u_y|)$ \\
  \var{uzmin}     & $\min(|u_z|)$ \\
  \var{uxmax}     & $\max(|u_x|)$ \\
  \var{uymax}     & $\max(|u_y|)$ \\
  \var{uzmax}     & $\max(|u_z|)$ \\
  \var{uxm}       & $\left<u_x\right>$ \\
  \var{uym}       & $\left<u_y\right>$ \\
  \var{uzm}       & $\left<u_z\right>$ \\
  \var{uzcx10m}   & $\left<u_z\cos10x\right>$ \\
  \var{uzsx10m}   & $\left<u_z\sin10x\right>$ \\
  \var{uduum}     & $\left<\boldsymbol{u}\cdot\boldsymbol{u}\right>$ \\
  \var{ux2m}      & $\left<u_x^2\right>$ \\
  \var{uy2m}      & $\left<u_y^2\right>$ \\
  \var{uz2m}      & $\left<u_z^2\right>$ \\
  \var{ux3m}      & $\left<u_x^3\right>$ \\
  \var{uy3m}      & $\left<u_y^3\right>$ \\
  \var{uz3m}      & $\left<u_z^3\right>$ \\
  \var{ux4m}      & $\left<u_x^4\right>$ \\
  \var{uy4m}      & $\left<u_y^4\right>$ \\
  \var{uz4m}      & $\left<u_z^4\right>$ \\
  \var{uxuy2m}    & $\left<u_x^2u_y^2\right>$ \\
  \var{uyuz2m}    & $\left<u_y^2u_z^2\right>$ \\
  \var{uzux2m}    & $\left<u_z^2u_x^2\right>$ \\
  \var{ux2ccm}    & $\left<u_x^2\cos^2kz\right>$ \\
  \var{ux2ssm}    & $\left<u_x^2\sin^2kz\right>$ \\
  \var{uy2ccm}    & $\left<u_y^2\cos^2kz\right>$ \\
  \var{uy2ssm}    & $\left<u_y^2\sin^2kz\right>$ \\
  \var{uxuycsm}   & $\left<u_xu_y\cos kz\sin kz\right>$ \\
  \var{uxuym}     & $\left<u_x u_y\right>$ \\
  \var{uxuzm}     & $\left<u_x u_z\right>$ \\
  \var{uyuzm}     & $\left<u_y u_z\right>$ \\
  \var{umx}       & $\left< u_x \right>$ \\
  \var{umy}       & $\left< u_y \right>$ \\
  \var{umz}       & $\left< u_z \right>$ \\
  \var{omumz}     & $\left<\left<\Wv\right>_{xy}
                    \cdot\left<\Uv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean cross helicity production) \\
  \var{umamz}     & $\left<\left<\uv\right>_{xy}\cdot\left<\Av\right>_{xy}\right>$ \\
  \var{umbmz}     & $\left<\left<\Uv\right>_{xy}
                    \cdot\left<\Bv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean cross helicity production) \\
  \var{umxbmz}    & $\left<\left<\Uv\right>_{xy}
                    \times\left<\Bv\right>_{xy}
                    \right>_z$ \quad($xy$-averaged
                    mean emf) \\
  \var{rux2m}     & $\left<\rho u_x^2\right>$ \\
  \var{ruy2m}     & $\left<\rho u_y^2\right>$ \\
  \var{ruz2m}     & $\left<\rho u_z^2\right>$ \\
  \var{divum}     & $\left<{\rm div}\uv)\right>$ \\
  \var{rdivum}    & $\left<\varrho{\rm div}\uv)\right>$ \\
  \var{divu2m}    & $\left<({\rm div}\uv)^2\right>$ \\
  \var{gdivu2m}   & $\left<({\rm grad\,div}\uv)^2\right>$ \\
  \var{u3u21m}    & $\left<u_3 u_{2,1}\right>$ \\
  \var{u1u32m}    & $\left<u_1 u_{3,2}\right>$ \\
  \var{u2u13m}    & $\left<u_2 u_{1,3}\right>$ \\
  \var{u2u31m}    & $\left<u_2 u_{3,1}\right>$ \\
  \var{u3u12m}    & $\left<u_3 u_{1,2}\right>$ \\
  \var{u1u23m}    & $\left<u_1 u_{2,3}\right>$ \\
  \var{ruxm}      & $\left<\varrho u_x\right>$
                    \quad(mean $x$-momentum density) \\
  \var{ruym}      & $\left<\varrho u_y\right>$
                    \quad(mean $y$-momentum density) \\
  \var{ruzm}      & $\left<\varrho u_z\right>$
                    \quad(mean $z$-momentum density) \\
  \var{ruxtot}    & $\left<\rho |u|\right>$
                    \quad(mean absolute $x$-momentum density) \\
  \var{rumax}     & $\max(\varrho |\uv|)$
                    \quad(maximum modulus of momentum) \\
  \var{ruxuym}    & $\left<\varrho u_x u_y\right>$
                    \quad(mean Reynolds stress) \\
  \var{ruxuzm}    & $\left<\varrho u_x u_z\right>$
                    \quad(mean Reynolds stress) \\
  \var{ruyuzm}    & $\left<\varrho u_y u_z\right>$
                    \quad(mean Reynolds stress) \\
  \var{divrhourms} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm rms}$ \\
  \var{divrhoumax} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm max}$ \\
  \var{rlxm}      & $\left< \rho y u_z - z u_y \right>$ \\
  \var{rlym}      & $\left< \rho z u_x - x u_z \right>$ \\
  \var{rlzm}      & $\left< \rho x u_y - y u_x \right>$ \\
  \var{rlx2m}     & $\left<(\rho y u_z-z u_y)^2\right>$ \\
  \var{rly2m}     & $\left<(\rho z u_x-x u_z)^2\right>$ \\
  \var{rlz2m}     & $\left<(\rho x u_y-y u_x)^2\right>$ \\
  \var{tot_ang_mom} & Total angular momentum in spherical
                    coordinates about the axis. \\
  \var{dtu}       & $\delta t/[c_{\delta t}\,\delta x
                    /\max|\mathbf{u}|]$
                    \quad(time step relative to
                    advective time step;
                    see \S~\ref{time-step}) \\
  \var{oum}       & $\left<\boldsymbol{\omega}\cdot\uv\right>$ \\
  \var{oxum}      & $\left<\boldsymbol{\omega}\times\uv\right>$ \\
  \var{ourms}     & $\left<(\boldsymbol{\omega}\cdot\uv)^2\right>^{1/2}$ \\
  \var{oxurms}    & $\left<(\boldsymbol{\omega}\times\uv)^2\right>^{1/2}$ \\
  \var{ou_int}    & $\int_V\boldsymbol{\omega}\cdot\uv\,dV$ \\
  \var{fum}       & $\left<\fv\cdot\uv\right>$ \\
  \var{odel2um}   & $\left<\boldsymbol{\omega}\nabla^2\uv\right>$ \\
  \var{o2m}       & $\left<\boldsymbol{\omega}^2\right>
                    \equiv \left<(\curl\uv)^2\right>$ \\
  \var{o2u2m}     & $\left<\uv^2\boldsymbol{\omega}^2\right>$ \\
  \var{o2sphm}    & $\int_{r=0}^{r=r_{\rm diag}} \boldsymbol{\omega}^2 dV$,
                    where $r=\sqrt{x^2+y^2+z^2}$ \\
  \var{orms}      & $\left<\boldsymbol{\omega}^2\right>^{1/2}$ \\
  \var{omax}      & $\max(|\boldsymbol{\omega}|)$ \\
  \var{ox2m}      & $\left<\omega_x^2\right>$ \\
  \var{oy2m}      & $\left<\omega_y^2\right>$ \\
  \var{oz2m}      & $\left<\omega_z^2\right>$ \\
  \var{ox3m}      & $\left<\omega_x^3\right>$ \\
  \var{oy3m}      & $\left<\omega_y^3\right>$ \\
  \var{oz3m}      & $\left<\omega_z^3\right>$ \\
  \var{ox4m}      & $\left<\omega_x^4\right>$ \\
  \var{oy4m}      & $\left<\omega_y^4\right>$ \\
  \var{oz4m}      & $\left<\omega_z^4\right>$ \\
  \var{oxuzxm}    & $\left<\omega_x u_{z,x} \right>$ \\
  \var{oyuzym}    & $\left<\omega_y u_{z,y} \right>$ \\
  \var{oxoym}     & $\left<\omega_x\omega_y\right>$ \\
  \var{oxozm}     & $\left<\omega_x\omega_z\right>$ \\
  \var{oyozm}     & $\left<\omega_y\omega_z\right>$ \\
  \var{qfm}       & $\left<\qv\cdot\fv\right>$ \\
  \var{q2m}       & $\left<\qv^2\right>$ \\
  \var{qrms}      & $\left<\qv^2\right>^{1/2}$ \\
  \var{qmax}      & $\max(|\qv|)$ \\
  \var{qom}       & $\left<\qv\cdot\omv\right>$ \\
  \var{quxom}     & $\left<\qv\cdot(\uv\times\omv)\right>$ \\
  \var{pvzm}      & $\left<\omega_z + 2\Omega/\varrho\right>$
                    \quad(z component of potential vorticity) \\
  \var{oumphi}    & $\left<\omv\cdot\uv\right>_\varphi$ \\
  \var{ugurmsx}   & $\left<\left(\uv\nabla\uv\right)^2\right>^{1/2}$
                    for the hydro_xaver_range \\
  \var{ugu2m}     & $\left<\uv\nabla\uv\right>^2$ \\
  \var{dudx}      & $\left<\frac{\delta \uv}{\delta x}\right>$ \\
  \var{Marms}     & $\left<\uv^2/\cs^2\right>$
                    \quad(rms Mach number) \\
  \var{Mamax}     & $\max |\uv|/\cs$
                    \quad(maximum Mach number) \\
  \var{EEK}       & $\left<\varrho\uv^2\right>/2$ \\
  \var{ekin}      & $\left<{1\over2}\varrho\uv^2\right>$ \\
  \var{ekintot}   & $\int_V{1\over2}\varrho\uv^2\, dV$ \\
  \var{uxglnrym}  & $\left<u_x\partial_y\ln\varrho\right>$ \\
  \var{uyglnrxm}  & $\left<u_y\partial_x\ln\varrho\right>$ \\
  \var{uzdivum}   & $\left<u_z\nabla\cdot\uv\right>$ \\
  \var{uxuydivum} & $\left<u_x u_y\nabla\cdot\uv\right>$ \\
  \var{divuHrms}  & $(\nabla_{\rm H}\cdot\uv_{\rm H})^{\rm rms}$ \\
  \var{uxxrms}    & $u_{x,x}^{\rm rms}$ \\
  \var{uyyrms}    & $u_{y,y}^{\rm rms}$ \\
  \var{uxzrms}    & $u_{x,z}^{\rm rms}$ \\
  \var{uyzrms}    & $u_{y,z}^{\rm rms}$ \\
  \var{uzyrms}    & $u_{z,y}^{\rm rms}$ \\
  \var{dtF}       & $\delta t/[c_{\delta t}\,\delta x
                    /\max|\mathbf{F}|]$
                    \quad(time step relative to
                    max force time step;
                    see \S~\ref{time-step})
                    $ \int u_r(\theta,\phi)Y^m_{\ell}(\theta,\phi)\sin(\theta)d\theta d\phi$ \\
  \var{udpxxm}    & components of symmetric tensor
                    $\left< u_i \partial_j p + u_j \partial_i p \right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{density.f90}} \\
\midrule
  \var{rhom}      & $\left<\varrho\right>$
                    \quad(mean density) \\
  \var{rhomxmask} & $\left<\varrho\right>$ for
                    the density_xaver_range \\
  \var{rhomzmask} & $\left<\varrho\right>$ for
                    the density_zaver_range \\
  \var{rho2m}     & $\left<\varrho^2\right>$ \\
  \var{rho4m}     & $\left<\varrho^4\right>$ \\
  \var{rho6m}     & $\left<\varrho^6\right>$ \\
  \var{rho12m}    & $\left<\varrho^{12}\right>$ \\
  \var{rhof2m}    & $\left<\varrho'^2\right>$ \\
  \var{drho2m}    & $<(\varrho-\varrho_0)^2>$ \\
  \var{drhom}     & $<\varrho-\varrho_0>$ \\
  \var{rhomin}    & $\min(\rho)$ \\
  \var{rhomax}    & $\max(\rho)$ \\
  \var{lnrhomin}  & $\min(\log\rho)$ \\
  \var{lnrhomax}  & $\max(\log\rho)$ \\
  \var{rhorms}    & $\sqrt{<\varrho^2>}$ \\
  \var{lnrhorms}  & $\sqrt{<(\ln\varrho)^2>}$ \\
  \var{ugrhom}    & $\left<\uv\cdot\nabla\varrho\right>$ \\
  \var{uglnrhom}  & $\left<\uv\cdot\nabla\ln\varrho\right>$ \\
  \var{totmass}   & $\int\varrho\,dV$ \\
  \var{mass}      & $\int\varrho\,dV$ \\
  \var{sphmass}   & $\int\varrho\,dV$ inside $r < r_{\rm diag}$. \\
  \var{inertiaxx} & $xx$ component of the inertia tensor (spherical coordinates) \\
  \var{inertiayy} & $yy$ component of the inertia tensor (spherical coordinates) \\
  \var{inertiazz} & $zz$ component of the inertia tensor (spherical coordinates) \\
  \var{inertiaxx_car} & $xx$ component of the inertia tensor (Cartesian coordinates) \\
  \var{inertiayy_car} & $xx$ component of the inertia tensor (Cartesian coordinates) \\
  \var{inertiazz_car} & $xx$ component of the inertia tensor (Cartesian coordinates) \\
  \var{vol}       & $\int\,dV$ (volume) \\
  \var{grhomax}   & $\max (|\nabla \varrho|)$ \\
\midrule
  \multicolumn{2}{c}{Module \file{entropy.f90}} \\
\midrule
  \var{dtc}       & $\delta t/[c_{\delta t}\,\delta_x
                    /\max c_{\rm s}]$
                    \quad(time step relative to
                    acoustic time step;
                    see \S~\ref{time-step}) \\
  \var{ethm}      & $\left<\varrho e\right>$
                    \quad(mean thermal
                    [=internal] energy) \\
  \var{ssruzm}    & $\left<s \varrho u_z/c_p\right>$ \\
  \var{ssuzm}     & $\left<s u_z/c_p\right>$ \\
  \var{ssm}       & $\left<s/c_p\right>$
                    \quad(mean entropy) \\
  \var{ss2m}      & $\left<(s/c_p)^2\right>$
                    \quad(mean squared entropy) \\
  \var{eem}       & $\left<e\right>$ \\
  \var{ppm}       & $\left<p\right>$ \\
  \var{csm}       & $\left<c_{\rm s}\right>$ \\
  \var{csmax}     & $\max (c_{\rm s})$ \\
  \var{cgam}      & $\left<c_{\gamma}\right>$ \\
  \var{pdivum}    & $\left<p\nabla\cdot\uv\right>$ \\
  \var{fradbot}   & $\int F_{\rm bot}\cdot d\vec{S}$ \\
  \var{fradtop}   & $\int F_{\rm top}\cdot d\vec{S}$ \\
  \var{TTtop}     & $\int T_{\rm top} d\vec{S}$ \\
  \var{ethtot}    & $\int_V\varrho e\,dV$
                    \quad(total thermal
                    [=internal] energy) \\
  \var{dtchi}     & $\delta t / [c_{\delta t,{\rm v}}\,
                    \delta x^2/\chi_{\rm max}]$
                    \quad(time step relative to time
                    step based on heat conductivity;
                    see \S~\ref{time-step}) \\
  \var{Hmax}      & $H_{\rm max}$\quad(net heat sources
                    summed see \S~\ref{time-step}) \\
  \var{tauhmin}   & $\min(\tau_{\rm heat})$ \\
  \var{dtH}       & $\delta t / [c_{\delta t,{\rm s}}\,
                    c_{\rm v}T /H_{\rm max}]$
                    \quad(time step relative to time
                    step based on heat sources;
                    see \S~\ref{time-step}) \\
  \var{yHm}       & mean hydrogen ionization \\
  \var{yHmax}     & max of hydrogen ionization \\
  \var{TTm}       & $\left<T\right>$ \\
  \var{TTmax}     & $T_{\max}$ \\
  \var{TTmin}     & $T_{\min}$ \\
  \var{gTmax}     & $\max (|\nabla T|)$ \\
  \var{ssmax}     & $s_{\max}$ \\
  \var{ssmin}     & $s_{\min}$ \\
  \var{gTrms}     & $(\nabla T)_{\rm rms}$ \\
  \var{gsrms}     & $(\nabla s)_{\rm rms}$ \\
  \var{gTxgsrms}  & $(\nabla T\times\nabla s)_{\rm rms}$ \\
  \var{fconvm}    & $\left< c_p \varrho u_z T \right>$ \\
  \var{ufpresm}   & $\left< -u/\rho\nabla p \right>$ \\
  \var{Kkramersm} & $\left< K_{\rm kramers} \right>$ \\
  \var{chikrammin} & $\min (\chi_{\rm kramers})$ \\
  \var{chikrammax} & $\max (\chi_{\rm kramers})$ \\
  \var{TT2m}      & $\left<(T)^2\right>$
                    \quad(mean squared temperature) \\
\midrule
  \multicolumn{2}{c}{Module \file{magnetic.f90}} \\
\midrule
  \var{eta_tdep}  & $t$-dependent $\eta$ \\
  \var{ab_int}    & $\int\Av\cdot\Bv\;dV$ \\
  \var{jb_int}    & $\int\jv\cdot\Bv\;dV$ \\
  \var{b2tm}      & $\left<\bv(t)\cdot\int_0^t\bv(t')
                    dt'\right>$ \\
  \var{bjtm}      & $\left<\bv(t)\cdot\int_0^t\jv(t')
                    dt'\right>$ \\
  \var{jbtm}      & $\left<\jv(t)\cdot\int_0^t\bv(t')
                    dt'\right>$ \\
  \var{ujtm}      & $\left<\uv(t)\cdot\int_0^t\jv(t')
                    dt'\right>$ \\
  \var{jutm}      & $\left<\jv(t)\cdot\int_0^t\uv(t')
                    dt'\right>$ \\
  \var{ubtm}      & $\left<\uv(t)\cdot\int_0^t\bv(t')
                    dt'\right>$ \\
  \var{butm}      & $\left<\bv(t)\cdot\int_0^t\uv(t')
                    dt'\right>$ \\
  \var{b2ruzm}    & $\left<\Bv^2\rho u_z\right>$ \\
  \var{b2uzm}     & $\left<\Bv^2u_z\right>$ \\
  \var{ubbzm}     & $\left<(\uv\cdot\Bv)B_z\right>$ \\
  \var{b1m}       & $\left<|\Bv|\right>$ \\
  \var{b2m}       & $\left<\Bv^2\right>$ \\
  \var{EEM}       & $\left<\Bv^2\right>/2$ \\
  \var{b4m}       & $\left<\Bv^4\right>$ \\
  \var{b6m}       & $\left<\Bv^6\right>$ \\
  \var{b12m}      & $\left<\Bv^12\right>$ \\
  \var{bm2}       & $\max(\Bv^2)$ \\
  \var{j2m}       & $\left<\jv^2\right>$ \\
  \var{jm2}       & $\max(\jv^2)$ \\
  \var{abm}       & $\left<\Av\cdot\Bv\right>$ \\
  \var{gLamam}    & $\left<\nabla\Lambda\cdot\Av\right>$ \\
  \var{gLambm}    & $\left<\nabla\Lambda\cdot\Bv\right>$ \\
  \var{abumx}     & $\left<u_x\Av\cdot\Bv\right>$ \\
  \var{abumy}     & $\left<u_y\Av\cdot\Bv\right>$ \\
  \var{abumz}     & $\left<u_z\Av\cdot\Bv\right>$ \\
  \var{abmh}      & $\left<\Av\cdot\Bv\right>$ (temp) \\
  \var{abmn}      & $\left<\Av\cdot\Bv\right>$ (north) \\
  \var{abms}      & $\left<\Av\cdot\Bv\right>$ (south) \\
  \var{abrms}     & $\left<(\Av\cdot\Bv)^2\right>^{1/2}$ \\
  \var{jbrms}     & $\left<(\jv\cdot\Bv)^2\right>^{1/2}$ \\
  \var{ajm}       & $\left<\jv\cdot\Av\right>$ \\
  \var{jbm}       & $\left<\jv\cdot\Bv\right>$ \\
  \var{a2b2m}     & $\left<\Av^2\cdot\Bv^2\right>$ \\
  \var{j2b2m}     & $\left<\jv^2\cdot\Bv^2\right>$ \\
  \var{jbmh}      & $\left<\Jv\cdot\Bv\right>$ (temp) \\
  \var{jbmn}      & $\left<\Jv\cdot\Bv\right>$ (north) \\
  \var{jbms}      & $\left<\Jv\cdot\Bv\right>$ (south) \\
  \var{ubm}       & $\left<\uv\cdot\Bv\right>$ \\
  \var{dubrms}    & $\left<(\uv-\Bv)^2\right>^{1/2}$ \\
  \var{dobrms}    & $\left<(\boldsymbol{\omega}-\Bv)^2
                    \right>^{1/2}$ \\
  \var{uxbxm}     & $\left<u_xB_x\right>$ \\
  \var{uybxm}     & $\left<u_yB_x\right>$ \\
  \var{uzbxm}     & $\left<u_zB_x\right>$ \\
  \var{uxbym}     & $\left<u_xB_y\right>$ \\
  \var{uybym}     & $\left<u_yB_y\right>$ \\
  \var{uzbym}     & $\left<u_zB_y\right>$ \\
  \var{uxbzm}     & $\left<u_xB_z\right>$ \\
  \var{uybzm}     & $\left<u_yB_z\right>$ \\
  \var{uzbzm}     & $\left<u_zB_z\right>$ \\
  \var{uxjxm}     & $\left<u_xJ_x\right>$ \\
  \var{uxjym}     & $\left<u_xJ_y\right>$ \\
  \var{uxjzm}     & $\left<u_xJ_z\right>$ \\
  \var{uyjxm}     & $\left<u_yJ_x\right>$ \\
  \var{uyjym}     & $\left<u_yJ_y\right>$ \\
  \var{uyjzm}     & $\left<u_yJ_z\right>$ \\
  \var{uzjxm}     & $\left<u_zJ_x\right>$ \\
  \var{uzjym}     & $\left<u_zJ_y\right>$ \\
  \var{uzjzm}     & $\left<u_zJ_z\right>$ \\
  \var{cosubm}    & $\left<\Uv\cdot\Bv/(|\Uv|\,|\Bv|)
                    \right>$ \\
  \var{jxbxm}     & $\left<j_xB_x\right>$ \\
  \var{jybxm}     & $\left<j_yB_x\right>$ \\
  \var{jzbxm}     & $\left<j_zB_x\right>$ \\
  \var{jxbym}     & $\left<j_xB_y\right>$ \\
  \var{jybym}     & $\left<j_yB_y\right>$ \\
  \var{jzbym}     & $\left<j_zB_y\right>$ \\
  \var{jxbzm}     & $\left<j_xB_z\right>$ \\
  \var{jybzm}     & $\left<j_yB_z\right>$ \\
  \var{jzbzm}     & $\left<j_zB_z\right>$ \\
  \var{uam}       & $\left<\uv\cdot\Av\right>$ \\
  \var{obm}       & $\left<\ov\cdot\Bv\right>$ \\
  \var{ujm}       & $\left<\uv\cdot\Jv\right>$ \\
  \var{fbm}       & $\left<\fv\cdot\Bv\right>$ \\
  \var{fxbxm}     & $\left<f_x B_x\right>$ \\
  \var{epsM}      & $\left<\eta\mu_0\jv^2\right>$ \\
  \var{epsAD}     & $\left<\rho^{-1} t_{\rm AD}
                    (\vec{J}\times\vec{B})^2\right>$
                    (heating by ion-neutrals friction) \\
  \var{bxpt}      & $B_x(x_1,y_1,z_1,t)$ \\
  \var{bypt}      & $B_y(x_1,y_1,z_1,t)$ \\
  \var{bzpt}      & $B_z(x_1,y_1,z_1,t)$ \\
  \var{bxbypt}    & $(B_x B_y)(x_1,y_1,z_1,t)$ \\
  \var{bybzpt}    & $(B_y B_z)(x_1,y_1,z_1,t)$ \\
  \var{bzbxpt}    & $(B_z B_x)(x_1,y_1,z_1,t)$ \\
  \var{jxpt}      & $J_x(x_1,y_1,z_1,t)$ \\
  \var{jypt}      & $J_y(x_1,y_1,z_1,t)$ \\
  \var{jzpt}      & $J_z(x_1,y_1,z_1,t)$ \\
  \var{Expt}      & ${\cal E}_x(x_1,y_1,z_1,t)$ \\
  \var{Eypt}      & ${\cal E}_y(x_1,y_1,z_1,t)$ \\
  \var{Ezpt}      & ${\cal E}_z(x_1,y_1,z_1,t)$ \\
  \var{axpt}      & $A_x(x_1,y_1,z_1,t)$ \\
  \var{aypt}      & $A_y(x_1,y_1,z_1,t)$ \\
  \var{azpt}      & $A_z(x_1,y_1,z_1,t)$ \\
  \var{bxp2}      & $B_x(x_2,y_2,z_2,t)$ \\
  \var{byp2}      & $B_y(x_2,y_2,z_2,t)$ \\
  \var{bzp2}      & $B_z(x_2,y_2,z_2,t)$ \\
  \var{jxp2}      & $J_x(x_2,y_2,z_2,t)$ \\
  \var{jyp2}      & $J_y(x_2,y_2,z_2,t)$ \\
  \var{jzp2}      & $J_z(x_2,y_2,z_2,t)$ \\
  \var{Exp2}      & ${\cal E}_x(x_2,y_2,z_2,t)$ \\
  \var{Eyp2}      & ${\cal E}_y(x_2,y_2,z_2,t)$ \\
  \var{Ezp2}      & ${\cal E}_z(x_2,y_2,z_2,t)$ \\
  \var{axp2}      & $A_x(x_2,y_2,z_2,t)$ \\
  \var{ayp2}      & $A_y(x_2,y_2,z_2,t)$ \\
  \var{azp2}      & $A_z(x_2,y_2,z_2,t)$ \\
  \var{exabot}    & $\int\Ev\times\Av\,dS|_{\rm bot}$ \\
  \var{exatop}    & $\int\Ev\times\Av\,dS|_{\rm top}$ \\
  \var{emag}      & $\int_V{1\over2\mu_0}\Bv^2\, dV$ \\
  \var{brms}      & $\left<\Bv^2\right>^{1/2}$ \\
  \var{bfrms}     & $\left<{\Bv'}^2\right>^{1/2}$ \\
  \var{bf2m}      & $\left<{\Bv'}^2\right>$ \\
  \var{bf4m}      & $\left<{\Bv'}^4\right>$ \\
  \var{bmax}      & $\max(|\Bv|)$ \\
  \var{bxmin}     & $\min(|B_x|)$ \\
  \var{bymin}     & $\min(|B_y|)$ \\
  \var{bzmin}     & $\min(|B_z|)$ \\
  \var{bxmax}     & $\max(|B_x|)$ \\
  \var{bymax}     & $\max(|B_y|)$ \\
  \var{bzmax}     & $\max(|B_z|)$ \\
  \var{bbxmax}    & $\max(|B_x|) excluding Bv_{ext}$ \\
  \var{bbymax}    & $\max(|B_y|) excluding Bv_{ext}$ \\
  \var{bbzmax}    & $\max(|B_z|) excluding Bv_{ext}$ \\
  \var{jxmax}     & $\max(|jv_x|)$ \\
  \var{jymax}     & $\max(|jv_y|)$ \\
  \var{jzmax}     & $\max(|jv_z|)$ \\
  \var{jrms}      & $\left<\jv^2\right>^{1/2}$ \\
  \var{hjrms}     & $\left<\jv^2\right>^{1/2}$ \\
  \var{jmax}      & $\max(|\jv|)$ \\
  \var{vA23rms}   & $\left<\Bv^2/\varrho^{4/3}\right>^{1/2}$ \\
  \var{vArms}     & $\left<\Bv^2/\varrho\right>^{1/2}$ \\
  \var{vAmax}     & $\max(\Bv^2/\varrho)^{1/2}$ \\
  \var{dtb}       & $\delta t / [c_{\delta t}\,\delta x
                    /v_{\rm A,max}]$
                    \quad(time step relative to
                    Alfv{\'e}n time step;
                    see \S~\ref{time-step}) \\
  \var{dteta}     & $\delta t/[c_{\delta t,{\rm v}}\,
                    \delta x^2/\eta_{\rm max}]$
                    \quad(time step relative to
                    resistive time step;
                    see \S~\ref{time-step}) \\
  \var{dteta3}    & $\delta t/[c_{\delta t,{\rm v3}}\,
                    \delta x^6/\eta^{\rm hyper}_{\rm max}]$
                    \quad(time step relative to
                    hyper resistive time step;
                    see \S~\ref{time-step}) \\
  \var{a2m}       & $\left<\Av^2\right>$ \\
  \var{arms}      & $\left<\Av^2\right>^{1/2}$ \\
  \var{amax}      & $\max(|\Av|)$ \\
  \var{divarms}   & $\langle(\nabla\cdot\Av)^2\rangle^{1/2}$ \\
  \var{beta1m}    & $\left<\Bv^2/(2\mu_0 p)\right>$
                    \quad(mean inverse plasma beta) \\
  \var{beta1max}  & $\max[\Bv^2/(2\mu_0 p)]$
                    \quad(maximum inverse plasma beta) \\
  \var{betam}     & $\langle\beta\rangle$ \\
  \var{betamax}   & $\max\beta$ \\
  \var{betamin}   & $\min\beta$ \\
  \var{bxm}       & $\left<B_x\right>$ \\
  \var{bym}       & $\left<B_y\right>$ \\
  \var{bzm}       & $\left<B_z\right>$ \\
  \var{bxbym}     & $\left<B_x B_y\right>$ \\
  \var{bxbzm}     & $\left<B_x B_z\right>$ \\
  \var{bybzm}     & $\left<B_y B_z\right>$ \\
  \var{bij_cov_diffmax} & difference between two implementations of covariant derivatives \\
  \var{bmx}       & $\left<\left<\Bv\right>_{yz}^2
                    \right>^{1/2}$
                    \quad(energy of $yz$-averaged
                    mean field) \\
  \var{bmy}       & $\left<\left<\Bv\right>_{xz}^2
                    \right>^{1/2}$
                    \quad(energy of $xz$-averaged
                    mean field) \\
  \var{bmz}       & $\left<\left<\Bv\right>_{xy}^2
                    \right>^{1/2}$
                    \quad(energy of $xy$-averaged
                    mean field) \\
  \var{bmzS2}     & $\left<\left<\Bv_S\right>_{xy}^2\right>$ \\
  \var{bmzA2}     & $\left<\left<\Bv_A\right>_{xy}^2\right>$ \\
  \var{jmx}       & $\left<\left<\Jv\right>_{yz}^2
                    \right>^{1/2}$
                    \quad(energy of $yz$-averaged
                    mean current density) \\
  \var{jmy}       & $\left<\left<\Jv\right>_{xz}^2
                    \right>^{1/2}$
                    \quad(energy of $xz$-averaged
                    mean current density) \\
  \var{jmz}       & $\left<\left<\Jv\right>_{xy}^2
                    \right>^{1/2}$
                    \quad(energy of $xy$-averaged
                    mean current density) \\
  \var{bmzph}     & Phase of a Beltrami field \\
  \var{bmzphe}    & Error of phase of a Beltrami field \\
  \var{bsinphz}   & sine of phase of a Beltrami field \\
  \var{bcosphz}   & cosine of phase of a Beltrami field \\
  \var{emxamz3}   & $\left<\left<\Ev\right>_{xy}\times\left<\Av\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean field helicity flux) \\
  \var{embmz}     & $\left<\left<\Ev\right>_{xy}\cdot\left<\Bv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean field helicity production ) \\
  \var{ambmz}     & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field) \\
  \var{ambmzh}    & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field, temp) \\
  \var{ambmzn}    & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field, north) \\
  \var{ambmzs}    & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field, south) \\
  \var{jmbmz}     & $\left<\left<\Jv\right>_{xy}\cdot\left<\Bv\right>_{xy}
                    \right>$ \quad(current helicity
                    of $xy$-averaged mean field) \\
  \var{Rmmz}      & $\left<\frac{|\uv\times\Bv|}{|\eta\Jv|}
                    \right>_{xy}$ \\
  \var{kx_aa}     & $k_x$ \\
  \var{kmz}       & $\left<\left<\Jv\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>/
                    \left<\left<\Bv\right>_{xy}^2\right>$ \\
  \var{bx2m}      & $\left< B_x^2 \right>$ \\
  \var{by2m}      & $\left< B_y^2 \right>$ \\
  \var{bz2m}      & $\left< B_z^2 \right>$ \\
  \var{bx3m}      & $\left< B_x^3 \right>$ \\
  \var{by3m}      & $\left< B_y^3 \right>$ \\
  \var{bz3m}      & $\left< B_z^3 \right>$ \\
  \var{bx4m}      & $\left< B_x^4 \right>$ \\
  \var{by4m}      & $\left< B_y^4 \right>$ \\
  \var{bz4m}      & $\left< B_z^4 \right>$ \\
  \var{jx2m}      & $\left< J_x^2 \right>$ \\
  \var{jy2m}      & $\left< J_y^2 \right>$ \\
  \var{jz2m}      & $\left< J_z^2 \right>$ \\
  \var{jx4m}      & $\left< J_x^4 \right>$ \\
  \var{jy4m}      & $\left< J_y^4 \right>$ \\
  \var{jz4m}      & $\left< J_z^4 \right>$ \\
  \var{uxbm}      & $\left<\uv\times\Bv\right>\cdot\Bv_0/B_0^2$ \\
  \var{jxbm}      & $\left<\jv\times\Bv\right>\cdot\Bv_0/B_0^2$ \\
  \var{vmagfricmax} & $\max(1/\nu_{\rm mag}|\jv\times\Bv/\Bv^2|)$ \\
  \var{vmagfricrms} & $\left<1/\nu_{\rm mag}|\jv\times\Bv/\Bv^2|^2\right>^{1/2}$ \\
  \var{b3b21m}    & $\left<B_3 B_{2,1} \right>$ \\
  \var{b3b12m}    & $\left<B_3 B_{1,2} \right>$ \\
  \var{b1b32m}    & $\left<B_1 B_{3,2} \right>$ \\
  \var{b1b23m}    & $\left<B_1 B_{2,3} \right>$ \\
  \var{b2b13m}    & $\left<B_2 B_{1,3} \right>$ \\
  \var{b2b31m}    & $\left<B_2 B_{3,1} \right>$ \\
  \var{uxbmx}     & $\left<(\uv\times\Bv)_x\right>$ \\
  \var{uxbmy}     & $\left<(\uv\times\Bv)_y\right>$ \\
  \var{uxbmz}     & $\left<(\uv\times\Bv)_z\right>$ \\
  \var{jxbmx}     & $\left<(\jv\times\Bv)_x\right>$ \\
  \var{jxbmy}     & $\left<(\jv\times\Bv)_y\right>$ \\
  \var{jxbmz}     & $\left<(\jv\times\Bv)_z\right>$ \\
  \var{examx}     & $\left<\Ev\times\Av\right>|_x$ \\
  \var{examy}     & $\left<\Ev\times\Av\right>|_y$ \\
  \var{examz}     & $\left<\Ev\times\Av\right>|_z$ \\
  \var{exatotalmx} & $\left<\Ev\times\Av\right>|_x$ \\
  \var{exatotalmy} & $\left<\Ev\times\Av\right>|_y$ \\
  \var{exatotalmz} & $\left<\Ev\times\Av\right>|_z$ \\
  \var{exjmx}     & $\left<\Ev\times\Jv\right>|_x$ \\
  \var{exjmy}     & $\left<\Ev\times\Jv\right>|_y$ \\
  \var{exjmz}     & $\left<\Ev\times\Jv\right>|_z$ \\
  \var{dexbmx}    & $\left<\nabla\times\Ev\times\Bv\right>|_x$ \\
  \var{dexbmy}    & $\left<\nabla\times\Ev\times\Bv\right>|_y$ \\
  \var{dexbmz}    & $\left<\nabla\times\Ev\times\Bv\right>|_z$ \\
  \var{phibmx}    & $\left<\phi\Bv\right>|_x$ \\
  \var{phibmy}    & $\left<\phi\Bv\right>|_y$ \\
  \var{phibmz}    & $\left<\phi\Bv\right>|_z$ \\
  \var{b2divum}   & $\left<\Bv^2\nabla\cdot\uv\right>$ \\
  \var{jdel2am}   & $\left<\Jv\cdot\nabla^2\Av)\right>$ \\
  \var{jem}       & $\left<\jv\cdot\Ev\right>$ \\
  \var{aem}       & $\left<\Av\cdot\Ev\right>$ \\
  \var{ujxbm}     & $\left<\uv\cdot(\Jv\times\Bv)\right>$ \\
  \var{WL2D}      & $\left<J_i u_j A_{i,j} \right>$ \\
  \var{WL3D}      & $-\left<J_i u_j A_{j,i} \right>$ \\
  \var{WL3D2}     & $\left<J_i A_j u_{j,i} \right>$ \\
  \var{bij2m}     & $\left<|\hat{B}_{i,j}|^2\right>$ \\
  \var{sijbibjm}  & $\left<S_{i,j} B_i B_j\right>$ \\
  \var{ubgbpm}    & $\left<\uv\cdot(\Bv\cdot\nabla\Bv)\right>$ \\
  \var{ugb22m}    & $\left<\uv\cdot\nabla\Bv^2/2)\right>$ \\
  \var{jxbrmax}   & $\max(|\Jv\times\Bv/\rho|)$ \\
  \var{jxbr2m}    & $\left<(\Jv\times\Bv/\rho)^2\right>$ \\
  \var{bmxy_rms}  & $\sqrt{[\left<b_x\right>_z(x,y)]^2 +
                    [\left<b_y\right>_z(x,y)]^2 +
                    [\left<b_z\right>_z(x,y)]^2} $ \\
  \var{etasmagm}  & Mean of Smagorinsky resistivity \\
  \var{etasmagmin} & Min of Smagorinsky resistivity \\
  \var{etasmagmax} & Max of Smagorinsky resistivity \\
  \var{etavamax}  & Max of artificial resistivity
                    $\eta\sim v_A$ \\
  \var{etajmax}   & Max of artificial resistivity
                    $\eta\sim J / \sqrt{\rho}$ \\
  \var{etaj2max}  & Max of artificial resistivity
                    $\eta\sim J^2 / \rho$ \\
  \var{etajrhomax} & Max of artificial resistivity
                    $\eta\sim J / \rho$ \\
  \var{etaaniso}  & $\eta_1$ \\
  \var{etaanisoBB} & $\eta_{BB}$ \\
  \var{cosjbm}    & $\left<\Jv\cdot\Bv/(|\Jv|\,|\Bv|)\right>$ \\
  \var{jparallelm} & Mean value of the component
                    of J parallel to B \\
  \var{jperpm}    & Mean value of the component
                    of J perpendicular to B \\
  \var{hjparallelm} & Mean value of the component
                    of $J_{\rm hyper}$ parallel to B \\
  \var{hjperpm}   & Mean value of the component
                    of $J_{\rm hyper}$ perpendicular to B \\
  \var{b2sphm}    & $\int_{r=0}^{r=r_{\rm diag}} \Bv^2 dV$,
                    where $r=\sqrt{x^2+y^2+z^2}$ \\
  \var{brmsx}     & $\left<\Bv^2\right>^{1/2}$ for
                    the magnetic_xaver_range \\
  \var{brmsz}     & $\left<\Bv^2\right>^{1/2}$ for
                    the magnetic_zaver_range \\
  \var{Exmxy}     & $\left<{\cal E}_x\right>_{z}$ \\
  \var{Eymxy}     & $\left<{\cal E}_y\right>_{z}$ \\
  \var{Ezmxy}     & $\left<{\cal E}_z\right>_{z}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{pscalar.f90}} \\
\midrule
  \var{rhoccm}    & $\left<\varrho c\right>$ \\
  \var{ccmax}     & $\max(c)$ \\
  \var{ccglnrm}   & $\left<c\nabla_z\varrho\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{1D_loop.f90}} \\
\midrule
  \var{dtchi2}    & heatconduction \\
  \var{dtrad}     & radiative loss from RTV \\
  \var{dtspitzer} & Spitzer heat conduction
                    time step \\
  \var{qmax}      & max of heat flux vector \\
  \var{qrms}      & rms of heat flux vector \\
\midrule
  \multicolumn{2}{c}{Module \file{advective_gauge.f90}} \\
\midrule
  \var{Lamm}      & $\left<\Lambda\right>$ \\
  \var{Lampt}     & $\Lambda(x1,y1,z1)$ \\
  \var{Lamp2}     & $\Lambda(x2,y2,z2)$ \\
  \var{Lamrms}    & $\left<\Lambda^2\right>^{1/2}$ \\
  \var{Lambzm}    & $\left<\Lambda B_z\right>$ \\
  \var{Lambzmz}   & $\left<\Lambda B_z\right>_{xy}$ \\
  \var{gLambm}    & $\left<\Lambda\Bv\right>$ \\
  \var{apbrms}    & $\left<(\Av'\Bv)^2\right>^{1/2}$ \\
  \var{jxarms}    & $\left<(\Jv\times\Av)^2\right>^{1/2}$ \\
  \var{jxaprms}   & $\left<(\Jv\times\Av')^2\right>^{1/2}$ \\
  \var{jxgLamrms} & $\left<(\Jv\times\nabla\Lambda)^2\right>^{1/2}$ \\
  \var{gLamrms}   & $\left<(\nabla\Lambda)^2\right>^{1/2}$ \\
  \var{divabrms}  & $\left<[(\nabla\cdot\Av)\Bv]^2\right>^{1/2}$ \\
  \var{divapbrms} & $\left<[(\nabla\cdot\Av')\Bv]^2\right>^{1/2}$ \\
  \var{d2Lambrms} & $\left<[(\nabla^2\Lambda)\Bv]^2\right>^{1/2}$ \\
  \var{d2Lamrms}  & $\left<[\nabla^2\Lambda]^2\right>^{1/2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{anelastic.f90}} \\
\midrule
  \var{rhom}      & $\left<\varrho\right>$
                    \quad(mean density) \\
  \var{ugrhom}    & $\left<\uv\cdot\nabla\varrho\right>$ \\
  \var{mass}      & $\int\varrho\,dV$ \\
  \var{divrhoum}  & $\left<\nabla\cdot(\varrho\uv)\right>$ \\
  \var{divrhourms} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm rms}$ \\
  \var{divrhoumax} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm max}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{axionSU2back.f90}} \\
\midrule
  \var{Q}         & $Q$ \\
  \var{Qdot}      & $\dot{Q}$ \\
  \var{Qddot}     & $\ddot{Q}$ \\
  \var{chi}       & $\chi$ \\
  \var{chidot}    & $\dot{\chi}$ \\
  \var{chiddot}   & $\ddot{\chi}$ \\
  \var{psi}       & $\psi$ \\
  \var{psiL}      & $\psi_L$ \\
  \var{psidot}    & $\dot\psi$ \\
  \var{psiddot}   & $\ddot\psi$ \\
  \var{TR}        & $T_R$ \\
  \var{TL}        & $T_L$ \\
  \var{TRdot}     & $\dot T_R$ \\
  \var{TRddot}    & $\ddot T_R$ \\
  \var{imTR}      & $\Im T_R$ \\
  \var{psi_anal}  & $\psi^{\rm anal}$ \\
  \var{TR_anal}   & $T_R^{\rm anal}$ \\
  \var{TReff2m}   & $|T_R|^2_{\rm eff}$ \\
  \var{TReff2km}  & $k|T_R|^2_{\rm eff}$ \\
  \var{TRdoteff2m} & $|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TRdoteff2km} & $k|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TLeff2m}   & $|T_R|^2_{\rm eff}$ \\
  \var{TLeff2km}  & $k|T_R|^2_{\rm eff}$ \\
  \var{TLdoteff2m} & $|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TLdoteff2km} & $k|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{grand}     & ${\cal T}^Q$ \\
  \var{grant}     & ${\cal T}^\chi$ \\
  \var{dgrant_up} & ${\cal T}^\chi$ \\
  \var{grand2}    & ${\cal T}^Q$ (test) \\
  \var{dgrant}    & $\dot{\cal T}^\chi$ \\
  \var{fact}      & $\Theta(t)$ \\
  \var{k0}        & $k0$ \\
  \var{dk}        & $dk$ \\
\midrule
  \multicolumn{2}{c}{Module \file{axionSU2back_using_ode.f90}} \\
\midrule
  \var{Q}         & $Q$ \\
  \var{Qdot}      & $\dot{Q}$ \\
  \var{Qddot}     & $\ddot{Q}$ \\
  \var{chi}       & $\chi$ \\
  \var{chidot}    & $\dot{\chi}$ \\
  \var{chiddot}   & $\ddot{\chi}$ \\
  \var{psi}       & $\psi$ \\
  \var{psiL}      & $\psi_L$ \\
  \var{psidot}    & $\dot\psi$ \\
  \var{psiddot}   & $\ddot\psi$ \\
  \var{TR}        & $T_R$ \\
  \var{TL}        & $T_L$ \\
  \var{TRdot}     & $\dot T_R$ \\
  \var{TRddot}    & $\ddot T_R$ \\
  \var{imTR}      & $\Im T_R$ \\
  \var{psi_anal}  & $\psi^{\rm anal}$ \\
  \var{TR_anal}   & $T_R^{\rm anal}$ \\
  \var{TReff2m}   & $|T_R|^2_{\rm eff}$ \\
  \var{TReff2km}  & $k|T_R|^2_{\rm eff}$ \\
  \var{TRdoteff2m} & $|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TRdoteff2km} & $k|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TLeff2m}   & $|T_R|^2_{\rm eff}$ \\
  \var{TLeff2km}  & $k|T_R|^2_{\rm eff}$ \\
  \var{TLdoteff2m} & $|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TLdoteff2km} & $k|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{grand}     & ${\cal T}^Q$ \\
  \var{grant}     & ${\cal T}^\chi$ \\
  \var{dgrant_up} & ${\cal T}^\chi$ \\
  \var{grand2}    & ${\cal T}^Q$ (test) \\
  \var{dgrant}    & $\dot{\cal T}^\chi$ \\
  \var{fact}      & $\Theta(t)$ \\
  \var{k0}        & $k0$ \\
  \var{dk}        & $dk$ \\
\midrule
  \multicolumn{2}{c}{Module \file{axionSU2back_using_ode2.f90}} \\
\midrule
  \var{Q}         & $Q$ \\
  \var{Qdot}      & $\dot{Q}$ \\
  \var{Qddot}     & $\ddot{Q}$ \\
  \var{chi}       & $\chi$ \\
  \var{chidot}    & $\dot{\chi}$ \\
  \var{chiddot}   & $\ddot{\chi}$ \\
  \var{psi}       & $\psi$ \\
  \var{psiL}      & $\psi_L$ \\
  \var{psidot}    & $\dot\psi$ \\
  \var{psiddot}   & $\ddot\psi$ \\
  \var{TR}        & $T_R$ \\
  \var{TL}        & $T_L$ \\
  \var{TRdot}     & $\dot T_R$ \\
  \var{TRddot}    & $\ddot T_R$ \\
  \var{imTR}      & $\Im T_R$ \\
  \var{psi_anal}  & $\psi^{\rm anal}$ \\
  \var{TR_anal}   & $T_R^{\rm anal}$ \\
  \var{TReff2m}   & $|T_R|^2_{\rm eff}$ \\
  \var{TReff2km}  & $k|T_R|^2_{\rm eff}$ \\
  \var{TRdoteff2m} & $|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TRdoteff2km} & $k|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TLeff2m}   & $|T_R|^2_{\rm eff}$ \\
  \var{TLeff2km}  & $k|T_R|^2_{\rm eff}$ \\
  \var{TLdoteff2m} & $|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{TLdoteff2km} & $k|T_R\dot{T}_R|_{\rm eff}$ \\
  \var{grand}     & ${\cal T}^Q$ \\
  \var{grant}     & ${\cal T}^\chi$ \\
  \var{dgrant_up} & ${\cal T}^\chi$ \\
  \var{grand2}    & ${\cal T}^Q$ (test) \\
  \var{dgrant}    & $\dot{\cal T}^\chi$ \\
  \var{fact}      & $\Theta(t)$ \\
  \var{k0}        & $k0$ \\
  \var{dk}        & $dk$ \\
\midrule
  \multicolumn{2}{c}{Module \file{backreact_infl.f90}} \\
\midrule
  \var{phim}      & $\left<\phi\right>$ \\
  \var{phi2m}     & $\left<\phi^2\right>$ \\
  \var{phirms}    & $\left<\phi^2\right>^{1/2}$ \\
  \var{dphim}     & $\left<\phi'\right>$ \\
  \var{dphi2m}    & $\left<(\phi')^2\right>$ \\
  \var{dphirms}   & $\left<(\phi')^2\right>^{1/2}$ \\
  \var{Hubblem}   & $\left<{\cal H}\right>$ \\
  \var{lnam}      & $\left<\ln a\right>$ \\
  \var{ddotam}    & $a''/a$ \\
  \var{a2rhopm}   & $a^2 (rho+p)$ \\
  \var{a2rhom}    & $a^2 rho$ \\
\midrule
  \multicolumn{2}{c}{Module \file{bfield.f90}} \\
\midrule
  \var{bmax}      & $\max B$ \\
  \var{bmin}      & $\min B$ \\
  \var{brms}      & $\langle B^2\rangle^{1/2}$ \\
  \var{bm}        & $\langle B\rangle$ \\
  \var{b2m}       & $\langle B^2\rangle$ \\
  \var{bxmax}     & $\max|B_x|$ \\
  \var{bymax}     & $\max|B_y|$ \\
  \var{bzmax}     & $\max|B_z|$ \\
  \var{bxm}       & $\langle B_x\rangle$ \\
  \var{bym}       & $\langle B_y\rangle$ \\
  \var{bzm}       & $\langle B_z\rangle$ \\
  \var{bx2m}      & $\langle B_x^2\rangle$ \\
  \var{by2m}      & $\langle B_y^2\rangle$ \\
  \var{bz2m}      & $\langle B_z^2\rangle$ \\
  \var{bxbym}     & $\langle B_x B_y\rangle$ \\
  \var{bxbzm}     & $\langle B_x B_z\rangle$ \\
  \var{bybzm}     & $\langle B_y B_z\rangle$ \\
  \var{dbxmax}    & $\max|B_x - B_{\mathrm{ext,}x}|$ \\
  \var{dbymax}    & $\max|B_y - B_{\mathrm{ext,}y}|$ \\
  \var{dbzmax}    & $\max|B_z - B_{\mathrm{ext,}z}|$ \\
  \var{dbxm}      & $\langle B_x - B_{\mathrm{ext,}x}\rangle$ \\
  \var{dbym}      & $\langle B_y - B_{\mathrm{ext,}y}\rangle$ \\
  \var{dbzm}      & $\langle B_z - B_{\mathrm{ext,}z}\rangle$ \\
  \var{dbx2m}     & $\langle\left(B_x - B_{\mathrm{ext,}x}\right)^2\rangle$ \\
  \var{dby2m}     & $\langle\left(B_y - B_{\mathrm{ext,}y}\right)^2\rangle$ \\
  \var{dbz2m}     & $\langle\left(B_z - B_{\mathrm{ext,}z}\right)^2\rangle$ \\
  \var{jmax}      & $\max J$ \\
  \var{jmin}      & $\min J$ \\
  \var{jrms}      & $\langle J^2\rangle^{1/2}$ \\
  \var{jm}        & $\langle J\rangle$ \\
  \var{j2m}       & $\langle J^2\rangle$ \\
  \var{jxmax}     & $\max|J_x|$ \\
  \var{jymax}     & $\max|J_y|$ \\
  \var{jzmax}     & $\max|J_z|$ \\
  \var{jxm}       & $\langle J_x\rangle$ \\
  \var{jym}       & $\langle J_y\rangle$ \\
  \var{jzm}       & $\langle J_z\rangle$ \\
  \var{jx2m}      & $\langle J_x^2\rangle$ \\
  \var{jy2m}      & $\langle J_y^2\rangle$ \\
  \var{jz2m}      & $\langle J_z^2\rangle$ \\
  \var{divbmax}   & $\max|\nabla\cdot\vec{B}|$ \\
  \var{divbrms}   & $\langle\left(\nabla\cdot\vec{B}\right)^2\rangle^{1/2}$ \\
  \var{betamax}   & $\max\beta$ \\
  \var{betamin}   & $\min\beta$ \\
  \var{betam}     & $\langle\beta\rangle$ \\
  \var{vAmax}     & $\max v_A$ \\
  \var{vAmin}     & $\min v_A$ \\
  \var{vAm}       & $\langle v_A\rangle$ \\
\midrule
  \multicolumn{2}{c}{Module \file{chemistry.f90}} \\
\midrule
  \var{dtchem}    & $dt_{chem}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{chemistry_simple.f90}} \\
\midrule
  \var{dtchem}    & $dt_{chem}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{chiral_mhd.f90}} \\
\midrule
  \var{muSm}      & $\left<\mu_S\right>$ \\
  \var{muSrms}    & $\left<\mu_S^2\right>^{1/2}$ \\
  \var{muSmax}    & $\max\mu$ \\
  \var{mu5m}      & $\left<\mu_5\right>$ \\
  \var{mu51m}     & $\left<|\mu_5|\right>$ \\
  \var{mu53m}     & $\left<\mu_5^3\right>$ \\
  \var{mu54m}     & $\left<\mu_5^4\right>$ \\
  \var{mu5rms}    & $\left<\mu_5^2\right>^{1/2}$ \\
  \var{mu5min}    & $\min\mu_5$ \\
  \var{mu5max}    & $\max\mu_5$ \\
  \var{mu5abs}    & $\max|\mu_5|$ \\
  \var{gamf5m}    & $\left<\Gamma_5\right>$ \\
  \var{gmu5rms}   & $\left<(\nabla\mu_5)^2\right>^{1/2}$ \\
  \var{gmuSrms}   & $\left<(\nabla\mu_S)^2\right>^{1/2}$ \\
  \var{gmu5mx}    & $\left<\nabla\mu_5\right>_x$ \\
  \var{gmu5my}    & $\left<\nabla\mu_5\right>_y$ \\
  \var{gmu5mz}    & $\left<\nabla\mu_5\right>_z$ \\
  \var{bgmu5rms}  & $\left<(\Bv\cdot\nabla\mu_5)^2\right>^{1/2}$ \\
  \var{bgmuSrms}  & $\left<(\Bv\cdot\nabla\mu_S)^2\right>^{1/2}$ \\
  \var{mu5bjm}    & $\left<\mu_5 ((\nabla\times\Bv)\cdot\Bv) \right>$ \\
  \var{mu5bjrms}  & $\left<(\mu_5 ((\nabla\times\Bv)\cdot\Bv))^2 \right>^{1/2}$ \\
  \var{dt_lambda5} & $\mathrm{min}(\mu_5/\Bv^2) \delta x/(\lambda \eta)$ \\
  \var{dt_D5}     & $(\lambda \eta \mathrm{min}(\Bv^2))^{-1}$ \\
  \var{dt_gammaf5} & $1/\Gamma_\mathrm{f}$ \\
  \var{dt_CMW}    & $\delta x/((C_\mu C_5)^{1/2} \mathrm{max}(|\Bv|))$ \\
  \var{dt_Dmu}    & $(\lambda \eta \mathrm{min}(\Bv^2))^{-1}$ \\
  \var{dt_vmu}    & $\delta x /(\eta \mathrm{max}(|\mu_5 |))$ \\
  \var{dt_chiral} & total time-step contribution from chiral MHD \\
  \var{mu5bxm}    & $\left<\mu_5B_x\right>$ \\
  \var{mu5b2m}    & $\left<\mu_5B^2\right>$ \\
  \var{mu5jbm}    & $\left<\mu_5\Jv\cdot\Bv\right>$ \\
  \var{jxm}       & $\langle J_x\rangle$ \\
  \var{Dmu5_tdep} & $D(t)$ \\
\midrule
  \multicolumn{2}{c}{Module \file{collapse.f90}} \\
\midrule
  \var{betm}      & $\left<\beta\right>$ \\
  \var{massm}     & $\left<m\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{coronae.f90}} \\
\midrule
  \var{dtchi2}    & $\delta t / [c_{\delta t,{\rm v}}\,
                    \delta x^2/\chi_{\rm max}]$
                    \quad(time step relative to time
                    step based on heat conductivity;
                    see \S~\ref{time-step}) \\
  \var{dtspitzer} & Spitzer heat conduction time step \\
  \var{dtrad}     & radiative loss from RTV \\
\midrule
  \multicolumn{2}{c}{Module \file{cosmicray_current.f90}} \\
\midrule
  \var{ekincr}    & $\left<{1\over2}\varrho\uv_{\rm cr}^2\right>$ \\
  \var{ethmcr}    & $\left<\varrho_{\rm cr} e_{\rm cr}\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{density_stratified.f90}} \\
\midrule
  \var{mass}      & $\int\rho\,d^3x$ \\
  \var{rhomin}    & $\min\left|\rho\right|$ \\
  \var{rhomax}    & $\max\left|\rho\right|$ \\
  \var{drhom}     & $\langle\Delta\rho/\rho_0\rangle$ \\
  \var{drho2m}    & $\langle\left(\Delta\rho/\rho_0\right)^2\rangle$ \\
  \var{drhorms}   & $\langle\Delta\rho/\rho_0\rangle_{rms}$ \\
  \var{drhomax}   & $\max\left|\Delta\rho/\rho_0\right|$ \\
\midrule
  \multicolumn{2}{c}{Module \file{detonate.f90}} \\
\midrule
  \var{detn}      & Number of detonated sites (summed over time steps between adjacent outputs) \\
  \var{dettot}    & Total energy input (summed over time steps between adjacent outputs) \\
\midrule
  \multicolumn{2}{c}{Module \file{disp_current.f90}} \\
\midrule
  \var{EEEM}      & $\left<\Ev^2+\Bv^2\right>/2$ \\
  \var{erms}      & $\left<\Ev^2\right>^{1/2}$ \\
  \var{edotrms}   & $\left<\dot{\Ev}^2\right>^{1/2}$ \\
  \var{emax}      & $\max(|\Ev|)$ \\
  \var{a0rms}     & $\left<A_0^2\right>^{1/2}$ \\
  \var{grms}      & $\left<C-\nabla\cdot\Av\right>^{1/2}$ \\
  \var{da0rms}    & $\left<C-\nabla\cdot\Av\right>^{1/2}$ \\
  \var{BcurlEm}   & $\left<\Bv\cdot\nabla\times\Ev\right>$ \\
  \var{mfpf}      & $-f'/f$ \\
  \var{fppf}      & $f''/f$ \\
  \var{afact}     & $a$ (scale factor) \\
\midrule
  \multicolumn{2}{c}{Module \file{dustdensity.f90}} \\
\midrule
  \var{KKm}       & $\sum {\cal T}_k^{\rm coag}$ \\
  \var{KK2m}      & $\sum {\cal T}_k^{\rm coag}$ \\
  \var{MMxm}      & $\sum {\cal M}^x_{k,{\rm coag}}$ \\
  \var{MMym}      & $\sum {\cal M}^y_{k,{\rm coag}}$ \\
  \var{MMzm}      & $\sum {\cal M}^z_{k,{\rm coag}}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{entropy_anelastic.f90}} \\
\midrule
  \var{dtc}       & $\delta t/[c_{\delta t}\,\delta_x
                    /\max c_{\rm s}]$
                    \quad(time step relative to
                    acoustic time step;
                    see \S~\ref{time-step}) \\
  \var{ethm}      & $\left<\varrho e\right>$
                    \quad(mean thermal
                    [=internal] energy) \\
  \var{ssm}       & $\left<s/c_p\right>$
                    \quad(mean entropy) \\
  \var{ss2m}      & $\left<(s/c_p)^2\right>$
                    \quad(mean squared entropy) \\
  \var{eem}       & $\left<e\right>$ \\
  \var{ppm}       & $\left<p\right>$ \\
  \var{csm}       & $\left<c_{\rm s}\right>$ \\
  \var{pdivum}    & $\left<p\nabla\uv\right>$ \\
  \var{fradbot}   & $\int F_{\rm bot}\cdot d\vec{S}$ \\
  \var{fradtop}   & $\int F_{\rm top}\cdot d\vec{S}$ \\
  \var{TTtop}     & $\int T_{\rm top} d\vec{S}$ \\
  \var{ethtot}    & $\int_V\varrho e\,dV$
                    \quad(total thermal
                    [=internal] energy) \\
  \var{dtchi}     & $\delta t / [c_{\delta t,{\rm v}}\,
                    \delta x^2/\chi_{\rm max}]$
                    \quad(time step relative to time
                    step based on heat conductivity;
                    see \S~\ref{time-step}) \\
  \var{ssmxy}     & $\left< s \right>_{z}$ \\
  \var{ssmxz}     & $\left< s \right>_{y}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{gravitational_waves.f90}} \\
\midrule
  \var{hhT2m}     & $\left<h_{\rm T}^2\right>$ \\
  \var{hhX2m}     & $\left<h_{\rm X}^2\right>$ \\
  \var{hhThhXm}   & $\left<h_{\rm T}h_{\rm X}\right>$ \\
  \var{ggTpt}     & $g_{\rm T}(x_1,y_1,z_1,t)$ \\
  \var{strTpt}    & $S_{\rm T}(x_1,y_1,z_1,t)$ \\
  \var{strXpt}    & $S_{\rm X}(x_1,y_1,z_1,t)$ \\
\midrule
  \multicolumn{2}{c}{Module \file{gravitational_waves_hTXk.f90}} \\
\midrule
  \var{STrept}    & $Re S_{T}(k_1,k_1,k_1,t)$ \\
  \var{STimpt}    & $Im S_{T}(k_1,k_1,k_1,t)$ \\
  \var{SXrept}    & $Re S_{X}(k_1,k_1,k_1,t)$ \\
  \var{SXimpt}    & $Im S_{X}(k_1,k_1,k_1,t)$ \\
  \var{hTrept}    & $Re h_{T}(k_1,k_1,k_1,t)$ \\
  \var{hTimpt}    & $Im h_{T}(k_1,k_1,k_1,t)$ \\
  \var{hXrept}    & $Re h_{X}(k_1,k_1,k_1,t)$ \\
  \var{hXimpt}    & $Im h_{X}(k_1,k_1,k_1,t)$ \\
  \var{gTrept}    & $Re h_{T}(k_1,k_1,k_1,t)$ \\
  \var{gTimpt}    & $Im h_{T}(k_1,k_1,k_1,t)$ \\
  \var{gXrept}    & $Re h_{X}(k_1,k_1,k_1,t)$ \\
  \var{gXimpt}    & $Im h_{X}(k_1,k_1,k_1,t)$ \\
  \var{STrep2}    & $Re S_{T}(k_2,k_2,k_2,t)$ \\
  \var{STimp2}    & $Im S_{T}(k_2,k_2,k_2,t)$ \\
  \var{SXrep2}    & $Re S_{X}(k_2,k_2,k_2,t)$ \\
  \var{SXimp2}    & $Im S_{X}(k_2,k_2,k_2,t)$ \\
  \var{hTrep2}    & $Re h_{T}(k_2,k_2,k_2,t)$ \\
  \var{hTimp2}    & $Im h_{T}(k_2,k_2,k_2,t)$ \\
  \var{hXrep2}    & $Re h_{X}(k_2,k_2,k_2,t)$ \\
  \var{hXimp2}    & $Im h_{X}(k_2,k_2,k_2,t)$ \\
  \var{gTrep2}    & $Re g_{T}(k_2,k_2,k_2,t)$ \\
  \var{gTimp2}    & $Im g_{T}(k_2,k_2,k_2,t)$ \\
  \var{gXrep2}    & $Re g_{X}(k_2,k_2,k_2,t)$ \\
  \var{gXimp2}    & $Im g_{X}(k_2,k_2,k_2,t)$ \\
  \var{g11pt}     & $g_{11}(x_1,y_1,z_1,t)$ \\
  \var{g22pt}     & $g_{22}(x_1,y_1,z_1,t)$ \\
  \var{g33pt}     & $g_{33}(x_1,y_1,z_1,t)$ \\
  \var{g12pt}     & $g_{12}(x_1,y_1,z_1,t)$ \\
  \var{g23pt}     & $g_{23}(x_1,y_1,z_1,t)$ \\
  \var{g31pt}     & $g_{31}(x_1,y_1,z_1,t)$ \\
  \var{hhTpt}     & $h_{T}(x_1,y_1,z_1,t)$ \\
  \var{hhXpt}     & $h_{X}(x_1,y_1,z_1,t)$ \\
  \var{ggTpt}     & $\dot{h}_{T}(x_1,y_1,z_1,t)$ \\
  \var{ggXpt}     & $\dot{h}_{X}(x_1,y_1,z_1,t)$ \\
  \var{hhTp2}     & $h_{T}(x_1,y_1,z_1,t)$ \\
  \var{hhXp2}     & $h_{X}(x_1,y_1,z_1,t)$ \\
  \var{ggTp2}     & $\dot{h}_{T}(x_1,y_1,z_1,t)$ \\
  \var{ggXp2}     & $\dot{h}_{X}(x_1,y_1,z_1,t)$ \\
  \var{hrms}      & $\bra{h_T^2+h_X^2}^{1/2}$ \\
  \var{EEGW}      & $\bra{g_T^2+g_X^2}\,c^2/(32\pi G)$ \\
  \var{gg2m}      & $\bra{g_T^2+g_X^2}$ \\
  \var{Stgm}      & $\bra{S_Tg_T+S_Xg_X}$ \\
  \var{hhT2m}     & $\bra{h_T^2}$ \\
  \var{hhX2m}     & $\bra{h_X^2}$ \\
  \var{hhTXm}     & $\bra{h_T h_X}$ \\
  \var{ggT2m}     & $\bra{g_T^2}$ \\
  \var{ggX2m}     & $\bra{g_X^2}$ \\
  \var{ggTXm}     & $\bra{g_T g_X}$ \\
  \var{nlin0}     & $\bra{nlin0}$ \\
  \var{nlin1}     & $\bra{nlin1}$ \\
  \var{nlin2}     & $\bra{nlin2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{gravitational_waves_hTXk_no_xpara.f90}} \\
\midrule
  \var{g11pt}     & $g_{11}(x_1,y_1,z_1,t)$ \\
  \var{g22pt}     & $g_{22}(x_1,y_1,z_1,t)$ \\
  \var{g33pt}     & $g_{33}(x_1,y_1,z_1,t)$ \\
  \var{g12pt}     & $g_{12}(x_1,y_1,z_1,t)$ \\
  \var{g23pt}     & $g_{23}(x_1,y_1,z_1,t)$ \\
  \var{g31pt}     & $g_{31}(x_1,y_1,z_1,t)$ \\
  \var{hhTpt}     & $h_{T}(x_1,y_1,z_1,t)$ \\
  \var{hhXpt}     & $h_{X}(x_1,y_1,z_1,t)$ \\
  \var{ggTpt}     & $\dot{h}_{T}(x_1,y_1,z_1,t)$ \\
  \var{ggXpt}     & $\dot{h}_{X}(x_1,y_1,z_1,t)$ \\
  \var{hhTp2}     & $h_{T}(x_1,y_1,z_1,t)$ \\
  \var{hhXp2}     & $h_{X}(x_1,y_1,z_1,t)$ \\
  \var{ggTp2}     & $\dot{h}_{T}(x_1,y_1,z_1,t)$ \\
  \var{ggXp2}     & $\dot{h}_{X}(x_1,y_1,z_1,t)$ \\
  \var{hrms}      & $\bra{h_T^2+h_X^2}^{1/2}$ \\
  \var{EEGW}      & $\bra{g_T^2+g_X^2}\,c^2/(32\pi G)$ \\
  \var{gg2m}      & $\bra{g_T^2+g_X^2}$ \\
  \var{hhT2m}     & $\bra{h_T^2}$ \\
  \var{hhX2m}     & $\bra{h_X^2}$ \\
  \var{hhTXm}     & $\bra{h_T h_X}$ \\
  \var{ggT2m}     & $\bra{g_T^2}$ \\
  \var{ggX2m}     & $\bra{g_X^2}$ \\
  \var{ggTXm}     & $\bra{g_T g_X}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{gravitational_waves_hij6.f90}} \\
\midrule
  \var{h22rms}    & $h_{22}^{\rm rms}$ \\
  \var{h33rms}    & $h_{33}^{\rm rms}$ \\
  \var{h23rms}    & $h_{23}^{\rm rms}$ \\
  \var{g11pt}     & $g_{11}(x_1,y_1,z_1,t)$ \\
  \var{g22pt}     & $g_{22}(x_1,y_1,z_1,t)$ \\
  \var{g33pt}     & $g_{33}(x_1,y_1,z_1,t)$ \\
  \var{g12pt}     & $g_{12}(x_1,y_1,z_1,t)$ \\
  \var{g23pt}     & $g_{23}(x_1,y_1,z_1,t)$ \\
  \var{g31pt}     & $g_{31}(x_1,y_1,z_1,t)$ \\
  \var{hhTpt}     & $h_{T}(x_1,y_1,z_1,t)$ \\
  \var{hhXpt}     & $h_{X}(x_1,y_1,z_1,t)$ \\
  \var{ggTpt}     & $\dot{h}_{T}(x_1,y_1,z_1,t)$ \\
  \var{ggXpt}     & $\dot{h}_{X}(x_1,y_1,z_1,t)$ \\
  \var{hhTp2}     & $h_{T}(x_1,y_1,z_1,t)$ \\
  \var{hhXp2}     & $h_{X}(x_1,y_1,z_1,t)$ \\
  \var{ggTp2}     & $\dot{h}_{T}(x_1,y_1,z_1,t)$ \\
  \var{ggXp2}     & $\dot{h}_{X}(x_1,y_1,z_1,t)$ \\
  \var{hrms}      & $\bra{h_T^2+h_X^2}^{1/2}$ \\
  \var{EEGW}      & $\bra{g_T^2+g_X^2}\,c^2/(32\pi G)$ \\
  \var{gg2m}      & $\bra{g_T^2+g_X^2}$ \\
  \var{hhT2m}     & $\bra{h_T^2}$ \\
  \var{hhX2m}     & $\bra{h_X^2}$ \\
  \var{hhTXm}     & $\bra{h_T h_X}$ \\
  \var{ggT2m}     & $\bra{g_T^2}$ \\
  \var{ggX2m}     & $\bra{g_X^2}$ \\
  \var{ggTXm}     & $\bra{g_T g_X}$ \\
  \var{ggTm}      & $\bra{g_T}$ \\
  \var{ggXm}      & $\bra{g_X}$ \\
  \var{hijij2m}   & $\bra{h_{ij,ij}^2}$ \\
  \var{gijij2m}   & $\bra{g_{ij,ij}^2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{gravity_simple.f90}} \\
\midrule
  \var{epot}      & $\left<\varrho \Phi_{\rm grav}
                    \right>$ \quad(mean potential
                    energy) \\
  \var{epottot}   & $\int_V\varrho \Phi_{\rm grav}
                    dV$ \quad(total potential
                    energy) \\
  \var{ugm}       & $\left<\uv \cdot \gv\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{heatflux.f90}} \\
\midrule
  \var{dtspitzer} & Spitzer heat conduction time step \\
  \var{dtq}       & heatflux time step \\
  \var{dtq2}      & heatflux time step due to tau \\
  \var{qmax}      & $\max(|\qv|)$ \\
  \var{tauqmax}   & $\max(|\tau_{\rm Spitzer}|)$ \\
  \var{qxmin}     & $\min(|q_x|)$ \\
  \var{qymin}     & $\min(|q_y|)$ \\
  \var{qzmin}     & $\min(|q_z|)$ \\
  \var{qxmax}     & $\max(|q_x|)$ \\
  \var{qymax}     & $\max(|q_y|)$ \\
  \var{qzmax}     & $\max(|q_z|)$ \\
  \var{qrms}      & $\sqrt(|\qv|^2)$ \\
  \var{qsatmin}   & minimum of qsat/qabs \\
  \var{qsatrms}   & rms of qsat/abs \\
\midrule
  \multicolumn{2}{c}{Module \file{hydro_kinematic.f90}} \\
\midrule
  \var{ourms}     & $\left<(\boldsymbol{\omega}\cdot\uv)^2\right>^{1/2}$ \\
  \var{oxurms}    & $\left<(\boldsymbol{\omega}\times\uv)^2\right>^{1/2}$ \\
  \var{EEK}       & $\left<\varrho\uv^2\right>/2$ \\
\midrule
  \multicolumn{2}{c}{Module \file{hydro_marked.f90}} \\
\midrule
  \var{u2tm}      & $\left<\uv(t)\cdot\int_0^t\uv(t')
                    dt'\right>$ \\
  \var{uotm}      & $\left<\uv(t)\cdot\int_0^t\omv(t')
                    dt'\right>$ \\
  \var{outm}      & $\left<\omv(t)\cdot\int_0^t\uv(t')
                    dt'\right>$ \\
  \var{fkinzm}    & $\left<{1\over2} \varrho\uv^2 u_z\right>$ \\
  \var{gamm}      & $\left<gamma\right>$ \\
  \var{gamrms}    & $\left<\gamma^2\right>^{1/2}$ \\
  \var{gammax}    & $\max(\gamma)$ \\
  \var{u2m}       & $\left<\uv^2\right>$ \\
  \var{u2sphm}    & $\int_{r=0}^{r=r_{\rm diag}} \uv^2 dV$,
                    where $r=\sqrt{x^2+y^2+z^2}$ \\
  \var{uxpt}      & $u_x(x_1,y_1,z_1,t)$ \\
  \var{uypt}      & $u_y(x_1,y_1,z_1,t)$ \\
  \var{uzpt}      & $u_z(x_1,y_1,z_1,t)$ \\
  \var{uxp2}      & $u_x(x_2,y_2,z_2,t)$ \\
  \var{uyp2}      & $u_y(x_2,y_2,z_2,t)$ \\
  \var{uzp2}      & $u_z(x_2,y_2,z_2,t)$ \\
  \var{uxuypt}    & $(u_x u_y)(x_1,y_1,z_1,t)$ \\
  \var{uyuzpt}    & $(u_y u_z)(x_1,y_1,z_1,t)$ \\
  \var{uzuxpt}    & $(u_z u_x)(x_1,y_1,z_1,t)$ \\
  \var{urms}      & $\left<\uv^2\right>^{1/2}$ \\
  \var{urmsx}     & $\left<\uv^2\right>^{1/2}$ for
                    the hydro_xaver_range \\
  \var{urmsz}     & $\left<\uv^2\right>^{1/2}$ for
                    the hydro_zaver_range \\
  \var{durms}     & $\left<\delta\uv^2\right>^{1/2}$ \\
  \var{umax}      & $\max(|\uv|)$ \\
  \var{umin}      & $\min(|\uv|)$ \\
  \var{uxrms}     & $\left<u_x^2\right>^{1/2}$ \\
  \var{uyrms}     & $\left<u_y^2\right>^{1/2}$ \\
  \var{uzrms}     & $\left<u_z^2\right>^{1/2}$ \\
  \var{uxmin}     & $\min(|u_x|)$ \\
  \var{uymin}     & $\min(|u_y|)$ \\
  \var{uzmin}     & $\min(|u_z|)$ \\
  \var{uxmax}     & $\max(|u_x|)$ \\
  \var{uymax}     & $\max(|u_y|)$ \\
  \var{uzmax}     & $\max(|u_z|)$ \\
  \var{uxm}       & $\left<u_x\right>$ \\
  \var{uym}       & $\left<u_y\right>$ \\
  \var{uzm}       & $\left<u_z\right>$ \\
  \var{uzcx10m}   & $\left<u_z\cos10x\right>$ \\
  \var{uzsx10m}   & $\left<u_z\sin10x\right>$ \\
  \var{uduum}     & $\left<\boldsymbol{u}\cdot\boldsymbol{u}\right>$ \\
  \var{ux2m}      & $\left<u_x^2\right>$ \\
  \var{uy2m}      & $\left<u_y^2\right>$ \\
  \var{uz2m}      & $\left<u_z^2\right>$ \\
  \var{ux3m}      & $\left<u_x^3\right>$ \\
  \var{uy3m}      & $\left<u_y^3\right>$ \\
  \var{uz3m}      & $\left<u_z^3\right>$ \\
  \var{ux4m}      & $\left<u_x^4\right>$ \\
  \var{uy4m}      & $\left<u_y^4\right>$ \\
  \var{uz4m}      & $\left<u_z^4\right>$ \\
  \var{uxuy2m}    & $\left<u_x^2u_y^2\right>$ \\
  \var{uyuz2m}    & $\left<u_y^2u_z^2\right>$ \\
  \var{uzux2m}    & $\left<u_z^2u_x^2\right>$ \\
  \var{ux2ccm}    & $\left<u_x^2\cos^2kz\right>$ \\
  \var{ux2ssm}    & $\left<u_x^2\sin^2kz\right>$ \\
  \var{uy2ccm}    & $\left<u_y^2\cos^2kz\right>$ \\
  \var{uy2ssm}    & $\left<u_y^2\sin^2kz\right>$ \\
  \var{uxuycsm}   & $\left<u_xu_y\cos kz\sin kz\right>$ \\
  \var{uxuym}     & $\left<u_x u_y\right>$ \\
  \var{uxuzm}     & $\left<u_x u_z\right>$ \\
  \var{uyuzm}     & $\left<u_y u_z\right>$ \\
  \var{umx}       & $\left< u_x \right>$ \\
  \var{umy}       & $\left< u_y \right>$ \\
  \var{umz}       & $\left< u_z \right>$ \\
  \var{omumz}     & $\left<\left<\Wv\right>_{xy}
                    \cdot\left<\Uv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean cross helicity production) \\
  \var{umamz}     & $\left<\left<\uv\right>_{xy}\cdot\left<\Av\right>_{xy}\right>$ \\
  \var{umbmz}     & $\left<\left<\Uv\right>_{xy}
                    \cdot\left<\Bv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean cross helicity production) \\
  \var{umxbmz}    & $\left<\left<\Uv\right>_{xy}
                    \times\left<\Bv\right>_{xy}
                    \right>_z$ \quad($xy$-averaged
                    mean emf) \\
  \var{rux2m}     & $\left<\rho u_x^2\right>$ \\
  \var{ruy2m}     & $\left<\rho u_y^2\right>$ \\
  \var{ruz2m}     & $\left<\rho u_z^2\right>$ \\
  \var{divum}     & $\left<{\rm div}\uv)\right>$ \\
  \var{rdivum}    & $\left<\varrho{\rm div}\uv)\right>$ \\
  \var{divu2m}    & $\left<({\rm div}\uv)^2\right>$ \\
  \var{gdivu2m}   & $\left<({\rm grad\,div}\uv)^2\right>$ \\
  \var{u3u21m}    & $\left<u_3 u_{2,1}\right>$ \\
  \var{u1u32m}    & $\left<u_1 u_{3,2}\right>$ \\
  \var{u2u13m}    & $\left<u_2 u_{1,3}\right>$ \\
  \var{u2u31m}    & $\left<u_2 u_{3,1}\right>$ \\
  \var{u3u12m}    & $\left<u_3 u_{1,2}\right>$ \\
  \var{u1u23m}    & $\left<u_1 u_{2,3}\right>$ \\
  \var{ruxm}      & $\left<\varrho u_x\right>$
                    \quad(mean $x$-momentum density) \\
  \var{ruym}      & $\left<\varrho u_y\right>$
                    \quad(mean $y$-momentum density) \\
  \var{ruzm}      & $\left<\varrho u_z\right>$
                    \quad(mean $z$-momentum density) \\
  \var{ruxtot}    & $\left<\rho |u|\right>$
                    \quad(mean absolute $x$-momentum density) \\
  \var{rumax}     & $\max(\varrho |\uv|)$
                    \quad(maximum modulus of momentum) \\
  \var{ruxuym}    & $\left<\varrho u_x u_y\right>$
                    \quad(mean Reynolds stress) \\
  \var{ruxuzm}    & $\left<\varrho u_x u_z\right>$
                    \quad(mean Reynolds stress) \\
  \var{ruyuzm}    & $\left<\varrho u_y u_z\right>$
                    \quad(mean Reynolds stress) \\
  \var{divrhourms} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm rms}$ \\
  \var{divrhoumax} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm max}$ \\
  \var{rlxm}      & $\left< \rho y u_z - z u_y \right>$ \\
  \var{rlym}      & $\left< \rho z u_x - x u_z \right>$ \\
  \var{rlzm}      & $\left< \rho x u_y - y u_x \right>$ \\
  \var{rlx2m}     & $\left<(\rho y u_z-z u_y)^2\right>$ \\
  \var{rly2m}     & $\left<(\rho z u_x-x u_z)^2\right>$ \\
  \var{rlz2m}     & $\left<(\rho x u_y-y u_x)^2\right>$ \\
  \var{tot_ang_mom} & Total angular momentum in spherical
                    coordinates about the axis. \\
  \var{dtu}       & $\delta t/[c_{\delta t}\,\delta x
                    /\max|\mathbf{u}|]$
                    \quad(time step relative to
                    advective time step;
                    see \S~\ref{time-step}) \\
  \var{oum}       & $\left<\boldsymbol{\omega}\cdot\uv\right>$ \\
  \var{oxum}      & $\left<\boldsymbol{\omega}\times\uv\right>$ \\
  \var{ourms}     & $\left<(\boldsymbol{\omega}\cdot\uv)^2\right>^{1/2}$ \\
  \var{oxurms}    & $\left<(\boldsymbol{\omega}\times\uv)^2\right>^{1/2}$ \\
  \var{ou_int}    & $\int_V\boldsymbol{\omega}\cdot\uv\,dV$ \\
  \var{fum}       & $\left<\fv\cdot\uv\right>$ \\
  \var{odel2um}   & $\left<\boldsymbol{\omega}\nabla^2\uv\right>$ \\
  \var{o2m}       & $\left<\boldsymbol{\omega}^2\right>
                    \equiv \left<(\curl\uv)^2\right>$ \\
  \var{o2u2m}     & $\left<\uv^2\boldsymbol{\omega}^2\right>$ \\
  \var{o2sphm}    & $\int_{r=0}^{r=r_{\rm diag}} \boldsymbol{\omega}^2 dV$,
                    where $r=\sqrt{x^2+y^2+z^2}$ \\
  \var{orms}      & $\left<\boldsymbol{\omega}^2\right>^{1/2}$ \\
  \var{omax}      & $\max(|\boldsymbol{\omega}|)$ \\
  \var{ox2m}      & $\left<\omega_x^2\right>$ \\
  \var{oy2m}      & $\left<\omega_y^2\right>$ \\
  \var{oz2m}      & $\left<\omega_z^2\right>$ \\
  \var{ox3m}      & $\left<\omega_x^3\right>$ \\
  \var{oy3m}      & $\left<\omega_y^3\right>$ \\
  \var{oz3m}      & $\left<\omega_z^3\right>$ \\
  \var{ox4m}      & $\left<\omega_x^4\right>$ \\
  \var{oy4m}      & $\left<\omega_y^4\right>$ \\
  \var{oz4m}      & $\left<\omega_z^4\right>$ \\
  \var{oxuzxm}    & $\left<\omega_x u_{z,x} \right>$ \\
  \var{oyuzym}    & $\left<\omega_y u_{z,y} \right>$ \\
  \var{oxoym}     & $\left<\omega_x\omega_y\right>$ \\
  \var{oxozm}     & $\left<\omega_x\omega_z\right>$ \\
  \var{oyozm}     & $\left<\omega_y\omega_z\right>$ \\
  \var{qfm}       & $\left<\qv\cdot\fv\right>$ \\
  \var{q2m}       & $\left<\qv^2\right>$ \\
  \var{qrms}      & $\left<\qv^2\right>^{1/2}$ \\
  \var{qmax}      & $\max(|\qv|)$ \\
  \var{qom}       & $\left<\qv\cdot\omv\right>$ \\
  \var{quxom}     & $\left<\qv\cdot(\uv\times\omv)\right>$ \\
  \var{pvzm}      & $\left<\omega_z + 2\Omega/\varrho\right>$
                    \quad(z component of potential vorticity) \\
  \var{oumphi}    & $\left<\omv\cdot\uv\right>_\varphi$ \\
  \var{ugurmsx}   & $\left<\left(\uv\nabla\uv\right)^2\right>^{1/2}$
                    for the hydro_xaver_range \\
  \var{ugu2m}     & $\left<\uv\nabla\uv\right>^2$ \\
  \var{dudx}      & $\left<\frac{\delta \uv}{\delta x}\right>$ \\
  \var{Marms}     & $\left<\uv^2/\cs^2\right>$
                    \quad(rms Mach number) \\
  \var{Mamax}     & $\max |\uv|/\cs$
                    \quad(maximum Mach number) \\
  \var{EEK}       & $\left<\varrho\uv^2\right>/2$ \\
  \var{ekin}      & $\left<{1\over2}\varrho\uv^2\right>$ \\
  \var{ekintot}   & $\int_V{1\over2}\varrho\uv^2\, dV$ \\
  \var{uxglnrym}  & $\left<u_x\partial_y\ln\varrho\right>$ \\
  \var{uyglnrxm}  & $\left<u_y\partial_x\ln\varrho\right>$ \\
  \var{uzdivum}   & $\left<u_z\nabla\cdot\uv\right>$ \\
  \var{uxuydivum} & $\left<u_x u_y\nabla\cdot\uv\right>$ \\
  \var{divuHrms}  & $(\nabla_{\rm H}\cdot\uv_{\rm H})^{\rm rms}$ \\
  \var{uxxrms}    & $u_{x,x}^{\rm rms}$ \\
  \var{uyyrms}    & $u_{y,y}^{\rm rms}$ \\
  \var{uxzrms}    & $u_{x,z}^{\rm rms}$ \\
  \var{uyzrms}    & $u_{y,z}^{\rm rms}$ \\
  \var{uzyrms}    & $u_{z,y}^{\rm rms}$ \\
  \var{dtF}       & $\delta t/[c_{\delta t}\,\delta x
                    /\max|\mathbf{F}|]$
                    \quad(time step relative to
                    max force time step;
                    see \S~\ref{time-step})
                    $ \int u_r(\theta,\phi)Y^m_{\ell}(\theta,\phi)\sin(\theta)d\theta d\phi$ \\
  \var{udpxxm}    & components of symmetric tensor
                    $\left< u_i \partial_j p + u_j \partial_i p \right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{hydro_potential.f90}} \\
\midrule
  \var{u2tm}      & $\left<\uv(t)\cdot\int_0^t\uv(t')
                    dt'\right>$ \\
  \var{fkinzm}    & $\left<{1\over2} \varrho\uv^2 u_z\right>$ \\
  \var{u2m}       & $\left<\uv^2\right>$ \\
  \var{uxpt}      & $u_x(x_1,y_1,z_1,t)$ \\
  \var{uypt}      & $u_y(x_1,y_1,z_1,t)$ \\
  \var{uzpt}      & $u_z(x_1,y_1,z_1,t)$ \\
  \var{uxp2}      & $u_x(x_2,y_2,z_2,t)$ \\
  \var{uyp2}      & $u_y(x_2,y_2,z_2,t)$ \\
  \var{uzp2}      & $u_z(x_2,y_2,z_2,t)$ \\
  \var{urms}      & $\left<\uv^2\right>^{1/2}$ \\
  \var{urmsx}     & $\left<\uv^2\right>^{1/2}$ for
                    the hydro_xaver_range \\
  \var{urmsz}     & $\left<\uv^2\right>^{1/2}$ for
                    the hydro_zaver_range \\
  \var{durms}     & $\left<\delta\uv^2\right>^{1/2}$ \\
  \var{umax}      & $\max(|\uv|)$ \\
  \var{umin}      & $\min(|\uv|)$ \\
  \var{uxrms}     & $\left<u_x^2\right>^{1/2}$ \\
  \var{uyrms}     & $\left<u_y^2\right>^{1/2}$ \\
  \var{uzrms}     & $\left<u_z^2\right>^{1/2}$ \\
  \var{uxmin}     & $\min(|u_x|)$ \\
  \var{uymin}     & $\min(|u_y|)$ \\
  \var{uzmin}     & $\min(|u_z|)$ \\
  \var{uxmax}     & $\max(|u_x|)$ \\
  \var{uymax}     & $\max(|u_y|)$ \\
  \var{uzmax}     & $\max(|u_z|)$ \\
  \var{uxm}       & $\left<u_x\right>$ \\
  \var{uym}       & $\left<u_y\right>$ \\
  \var{uzm}       & $\left<u_z\right>$ \\
  \var{ux2m}      & $\left<u_x^2\right>$ \\
  \var{uy2m}      & $\left<u_y^2\right>$ \\
  \var{uz2m}      & $\left<u_z^2\right>$ \\
  \var{ux2ccm}    & $\left<u_x^2\cos^2kz\right>$ \\
  \var{ux2ssm}    & $\left<u_x^2\sin^2kz\right>$ \\
  \var{uy2ccm}    & $\left<u_y^2\cos^2kz\right>$ \\
  \var{uy2ssm}    & $\left<u_y^2\sin^2kz\right>$ \\
  \var{uxuycsm}   & $\left<u_xu_y\cos kz\sin kz\right>$ \\
  \var{uxuym}     & $\left<u_x u_y\right>$ \\
  \var{uxuzm}     & $\left<u_x u_z\right>$ \\
  \var{uyuzm}     & $\left<u_y u_z\right>$ \\
  \var{umx}       & $\left< u_x \right>$ \\
  \var{umy}       & $\left< u_y \right>$ \\
  \var{umz}       & $\left< u_z \right>$ \\
  \var{omumz}     & $\left<\left<\Wv\right>_{xy}
                    \cdot\left<\Uv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean cross helicity production) \\
  \var{umamz}     & $\left<\left<\uv\right>_{xy}\cdot\left<\Av\right>_{xy}\right>$ \\
  \var{umbmz}     & $\left<\left<\Uv\right>_{xy}
                    \cdot\left<\Bv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean cross helicity production) \\
  \var{umxbmz}    & $\left<\left<\Uv\right>_{xy}
                    \times\left<\Bv\right>_{xy}
                    \right>_z$ \quad($xy$-averaged
                    mean emf) \\
  \var{rux2m}     & $\left<\rho u_x^2\right>$ \\
  \var{ruy2m}     & $\left<\rho u_y^2\right>$ \\
  \var{ruz2m}     & $\left<\rho u_z^2\right>$ \\
  \var{divum}     & $\left<{\rm div}\uv)\right>$ \\
  \var{rdivum}    & $\left<\varrho{\rm div}\uv)\right>$ \\
  \var{divu2m}    & $\left<({\rm div}\uv)^2\right>$ \\
  \var{gdivu2m}   & $\left<({\rm grad\,div}\uv)^2\right>$ \\
  \var{u3u21m}    & $\left<u_3 u_{2,1}\right>$ \\
  \var{u1u32m}    & $\left<u_1 u_{3,2}\right>$ \\
  \var{u2u13m}    & $\left<u_2 u_{1,3}\right>$ \\
  \var{u2u31m}    & $\left<u_2 u_{3,1}\right>$ \\
  \var{u3u12m}    & $\left<u_3 u_{1,2}\right>$ \\
  \var{u1u23m}    & $\left<u_1 u_{2,3}\right>$ \\
  \var{ruxm}      & $\left<\varrho u_x\right>$
                    \quad(mean $x$-momentum density) \\
  \var{ruym}      & $\left<\varrho u_y\right>$
                    \quad(mean $y$-momentum density) \\
  \var{ruzm}      & $\left<\varrho u_z\right>$
                    \quad(mean $z$-momentum density) \\
  \var{ruxtot}    & $\left<\rho |u|\right>$
                    \quad(mean absolute $x$-momentum density) \\
  \var{rumax}     & $\max(\varrho |\uv|)$
                    \quad(maximum modulus of momentum) \\
  \var{ruxuym}    & $\left<\varrho u_x u_y\right>$
                    \quad(mean Reynolds stress) \\
  \var{ruxuzm}    & $\left<\varrho u_x u_z\right>$
                    \quad(mean Reynolds stress) \\
  \var{ruyuzm}    & $\left<\varrho u_y u_z\right>$
                    \quad(mean Reynolds stress) \\
  \var{divrhourms} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm rms}$ \\
  \var{divrhoumax} & $\left|\nabla\cdot(\varrho\uv)\right|_{\rm max}$ \\
  \var{rlxm}      & $\left< \rho y u_z - z u_y \right>$ \\
  \var{rlym}      & $\left< \rho z u_x - x u_z \right>$ \\
  \var{rlzm}      & $\left< \rho x u_y - y u_x \right>$ \\
  \var{rlx2m}     & $\left<(\rho y u_z-z u_y)^2\right>$ \\
  \var{rly2m}     & $\left<(\rho z u_x-x u_z)^2\right>$ \\
  \var{rlz2m}     & $\left<(\rho x u_y-y u_x)^2\right>$ \\
  \var{tot_ang_mom} & Total angular momentum in spherical
                    coordinates about the axis. \\
  \var{dtu}       & $\delta t/[c_{\delta t}\,\delta x
                    /\max|\mathbf{u}|]$
                    \quad(time step relative to
                    advective time step;
                    see \S~\ref{time-step}) \\
  \var{oum}       & $\left<\boldsymbol{\omega}
                    \cdot\uv\right>$ \\
  \var{ou_int}    & $\int_V\boldsymbol{\omega}\cdot\uv\,dV$ \\
  \var{fum}       & $\left<\fv\cdot\uv\right>$ \\
  \var{odel2um}   & $\left<\boldsymbol{\omega}\nabla^2\uv\right>$ \\
  \var{o2m}       & $\left<\boldsymbol{\omega}^2\right>
                    \equiv \left<(\curl\uv)^2\right>$ \\
  \var{orms}      & $\left<\boldsymbol{\omega}^2\right>^{1/2}$ \\
  \var{omax}      & $\max(|\boldsymbol{\omega}|)$ \\
  \var{ox2m}      & $\left<\omega_x^2\right>$ \\
  \var{oy2m}      & $\left<\omega_y^2\right>$ \\
  \var{oz2m}      & $\left<\omega_z^2\right>$ \\
  \var{oxuzxm}    & $\left<\omega_x u_{z,x} \right>$ \\
  \var{oyuzym}    & $\left<\omega_y u_{z,y} \right>$ \\
  \var{oxoym}     & $\left<\omega_x\omega_y\right>$ \\
  \var{oxozm}     & $\left<\omega_x\omega_z\right>$ \\
  \var{oyozm}     & $\left<\omega_y\omega_z\right>$ \\
  \var{qfm}       & $\left<\qv\cdot\fv\right>$ \\
  \var{q2m}       & $\left<\qv^2\right>$ \\
  \var{qrms}      & $\left<\qv^2\right>^{1/2}$ \\
  \var{qmax}      & $\max(|\qv|)$ \\
  \var{qom}       & $\left<\qv\cdot\omv\right>$ \\
  \var{quxom}     & $\left<\qv\cdot(\uv\times\omv)\right>$ \\
  \var{oumphi}    & $\left<\omv\cdot\uv\right>_\varphi$ \\
  \var{dudx}      & $\left<\frac{\delta \uv}{\delta x}\right>$ \\
  \var{Marms}     & $\left<\uv^2/\cs^2\right>$
                    \quad(rms Mach number) \\
  \var{Mamax}     & $\max |\uv|/\cs$
                    \quad(maximum Mach number) \\
  \var{EEK}       & $\left<\varrho\uv^2\right>/2$ \\
  \var{ekin}      & $\left<{1\over2}\varrho\uv^2\right>$ \\
  \var{ekintot}   & $\int_V{1\over2}\varrho\uv^2\, dV$ \\
  \var{uxglnrym}  & $\left<u_x\partial_y\ln\varrho\right>$ \\
  \var{uyglnrxm}  & $\left<u_y\partial_x\ln\varrho\right>$ \\
  \var{uzdivum}   & $\left<u_z\nabla\cdot\uv\right>$ \\
  \var{uxuydivum} & $\left<u_x u_y\nabla\cdot\uv\right>$ \\
  \var{divuHrms}  & $(\nabla_{\rm H}\cdot\uv_{\rm H})^{\rm rms}$ \\
  \var{uxxrms}    & $u_{x,x}^{\rm rms}$ \\
  \var{uyyrms}    & $u_{y,y}^{\rm rms}$ \\
  \var{uxzrms}    & $u_{x,z}^{\rm rms}$ \\
  \var{uyzrms}    & $u_{y,z}^{\rm rms}$ \\
  \var{uzyrms}    & $u_{z,y}^{\rm rms}$ \\
  \var{udpxxm}    & components of symmetric tensor
                    $\left< u_i \partial_j p + u_j \partial_i p \right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{interstellar.f90}} \\
\midrule
  \var{taucmin}   & $\min(\tau_{\rm cool})$ \\
  \var{Hmax_ism}  & $\max(\Gamma-\rho\Lambda)$ \\
  \var{Lamm}      & $\left<\Lambda\right>$ \\
  \var{nrhom}     & TBC \\
  \var{rhoLm}     & $\left<\rho\Lambda\right>$ \\
  \var{Gamm}      & $\left<\Gamma\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{lorenz_gauge.f90}} \\
\midrule
  \var{phim}      & $\left<\phi\right>$ \\
  \var{phipt}     & $\phi(x1,y1,z1)$ \\
  \var{phip2}     & $\phi(x2,y2,z2)$ \\
  \var{phibzm}    & $\left<\phi B_z\right>$ \\
  \var{phibzmz}   & $\left<\phi B_z\right>_{xy}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{lucky_droplet.f90}} \\
\midrule
  \var{rad}       & $r/r_\ast$ \\
  \var{tauk}      & $\tau_k$ \\
  \var{tt1m}      & $\langle T \rangle$ \\
  \var{qq1m}      & $\langle \ln T \rangle$ \\
  \var{qq2m}      & $\langle \ln T^2 \rangle$ \\
  \var{qq3m}      & $\langle \ln T^3 \rangle$ \\
  \var{qq4m}      & $\langle \ln T^4 \rangle$ \\
\midrule
  \multicolumn{2}{c}{Module \file{magnetic_shearboxJ.f90}} \\
\midrule
  \var{ab_int}    & $\int\Av\cdot\Bv\;dV$ \\
  \var{jb_int}    & $\int\jv\cdot\Bv\;dV$ \\
  \var{b2tm}      & $\left<\bv(t)\cdot\int_0^t\bv(t')
                    dt'\right>$ \\
  \var{bjtm}      & $\left<\bv(t)\cdot\int_0^t\jv(t')
                    dt'\right>$ \\
  \var{jbtm}      & $\left<\jv(t)\cdot\int_0^t\bv(t')
                    dt'\right>$ \\
  \var{b2ruzm}    & $\left<\Bv^2\rho u_z\right>$ \\
  \var{b2uzm}     & $\left<\Bv^2u_z\right>$ \\
  \var{ubbzm}     & $\left<(\uv\cdot\Bv)B_z\right>$ \\
  \var{b1m}       & $\left<|\Bv|\right>$ \\
  \var{b2m}       & $\left<\Bv^2\right>$ \\
  \var{bm2}       & $\max(\Bv^2)$ \\
  \var{j2m}       & $\left<\jv^2\right>$ \\
  \var{jm2}       & $\max(\jv^2)$ \\
  \var{abm}       & $\left<\Av\cdot\Bv\right>$ \\
  \var{abumx}     & $\left<u_x\Av\cdot\Bv\right>$ \\
  \var{abumy}     & $\left<u_y\Av\cdot\Bv\right>$ \\
  \var{abumz}     & $\left<u_z\Av\cdot\Bv\right>$ \\
  \var{abmh}      & $\left<\Av\cdot\Bv\right>$ (temp) \\
  \var{abmn}      & $\left<\Av\cdot\Bv\right>$ (north) \\
  \var{abms}      & $\left<\Av\cdot\Bv\right>$ (south) \\
  \var{abrms}     & $\left<(\Av\cdot\Bv)^2\right>^{1/2}$ \\
  \var{jbrms}     & $\left<(\jv\cdot\Bv)^2\right>^{1/2}$ \\
  \var{ajm}       & $\left<\jv\cdot\Av\right>$ \\
  \var{jbm}       & $\left<\jv\cdot\Bv\right>$ \\
  \var{jbmh}      & $\left<\Jv\cdot\Bv\right>$ (temp) \\
  \var{jbmn}      & $\left<\Jv\cdot\Bv\right>$ (north) \\
  \var{jbms}      & $\left<\Jv\cdot\Bv\right>$ (south) \\
  \var{ubm}       & $\left<\uv\cdot\Bv\right>$ \\
  \var{dubrms}    & $\left<(\uv-\Bv)^2\right>^{1/2}$ \\
  \var{dobrms}    & $\left<(\boldsymbol{\omega}-\Bv)^2
                    \right>^{1/2}$ \\
  \var{uxbxm}     & $\left<u_xB_x\right>$ \\
  \var{uybxm}     & $\left<u_yB_x\right>$ \\
  \var{uzbxm}     & $\left<u_zB_x\right>$ \\
  \var{uxbym}     & $\left<u_xB_y\right>$ \\
  \var{uybym}     & $\left<u_yB_y\right>$ \\
  \var{uzbym}     & $\left<u_zB_y\right>$ \\
  \var{uxbzm}     & $\left<u_xB_z\right>$ \\
  \var{uybzm}     & $\left<u_yB_z\right>$ \\
  \var{uzbzm}     & $\left<u_zB_z\right>$ \\
  \var{cosubm}    & $\left<\Uv\cdot\Bv/(|\Uv|\,|\Bv|)
                    \right>$ \\
  \var{jxbxm}     & $\left<j_xB_x\right>$ \\
  \var{jybxm}     & $\left<j_yB_x\right>$ \\
  \var{jzbxm}     & $\left<j_zB_x\right>$ \\
  \var{jxbym}     & $\left<j_xB_y\right>$ \\
  \var{jybym}     & $\left<j_yB_y\right>$ \\
  \var{jzbym}     & $\left<j_zB_y\right>$ \\
  \var{jxbzm}     & $\left<j_xB_z\right>$ \\
  \var{jybzm}     & $\left<j_yB_z\right>$ \\
  \var{jzbzm}     & $\left<j_zB_z\right>$ \\
  \var{uam}       & $\left<\uv\cdot\Av\right>$ \\
  \var{ujm}       & $\left<\uv\cdot\Jv\right>$ \\
  \var{fbm}       & $\left<\fv\cdot\Bv\right>$ \\
  \var{fxbxm}     & $\left<f_x B_x\right>$ \\
  \var{epsM}      & $\left<\eta\mu_0\jv^2\right>$ \\
  \var{epsAD}     & $\left<\rho^{-1} t_{\rm AD}
                    (\vec{J}\times\vec{B})^2\right>$
                    (heating by ion-neutrals friction) \\
  \var{bxpt}      & $B_x(x_1,y_1,z_1,t)$ \\
  \var{bypt}      & $B_y(x_1,y_1,z_1,t)$ \\
  \var{bzpt}      & $B_z(x_1,y_1,z_1,t)$ \\
  \var{jxpt}      & $J_x(x_1,y_1,z_1,t)$ \\
  \var{jypt}      & $J_y(x_1,y_1,z_1,t)$ \\
  \var{jzpt}      & $J_z(x_1,y_1,z_1,t)$ \\
  \var{Expt}      & ${\cal E}_x(x_1,y_1,z_1,t)$ \\
  \var{Eypt}      & ${\cal E}_y(x_1,y_1,z_1,t)$ \\
  \var{Ezpt}      & ${\cal E}_z(x_1,y_1,z_1,t)$ \\
  \var{axpt}      & $A_x(x_1,y_1,z_1,t)$ \\
  \var{aypt}      & $A_y(x_1,y_1,z_1,t)$ \\
  \var{azpt}      & $A_z(x_1,y_1,z_1,t)$ \\
  \var{bxp2}      & $B_x(x_2,y_2,z_2,t)$ \\
  \var{byp2}      & $B_y(x_2,y_2,z_2,t)$ \\
  \var{bzp2}      & $B_z(x_2,y_2,z_2,t)$ \\
  \var{jxp2}      & $J_x(x_2,y_2,z_2,t)$ \\
  \var{jyp2}      & $J_y(x_2,y_2,z_2,t)$ \\
  \var{jzp2}      & $J_z(x_2,y_2,z_2,t)$ \\
  \var{Exp2}      & ${\cal E}_x(x_2,y_2,z_2,t)$ \\
  \var{Eyp2}      & ${\cal E}_y(x_2,y_2,z_2,t)$ \\
  \var{Ezp2}      & ${\cal E}_z(x_2,y_2,z_2,t)$ \\
  \var{axp2}      & $A_x(x_2,y_2,z_2,t)$ \\
  \var{ayp2}      & $A_y(x_2,y_2,z_2,t)$ \\
  \var{azp2}      & $A_z(x_2,y_2,z_2,t)$ \\
  \var{exabot}    & $\int\Ev\times\Av\,dS|_{\rm bot}$ \\
  \var{exatop}    & $\int\Ev\times\Av\,dS|_{\rm top}$ \\
  \var{emag}      & $\int_V{1\over2\mu_0}\Bv^2\, dV$ \\
  \var{brms}      & $\left<\Bv^2\right>^{1/2}$ \\
  \var{bfrms}     & $\left<{\Bv'}^2\right>^{1/2}$ \\
  \var{bmax}      & $\max(|\Bv|)$ \\
  \var{bxmin}     & $\min(|B_x|)$ \\
  \var{bymin}     & $\min(|B_y|)$ \\
  \var{bzmin}     & $\min(|B_z|)$ \\
  \var{bxmax}     & $\max(|B_x|)$ \\
  \var{bymax}     & $\max(|B_y|)$ \\
  \var{bzmax}     & $\max(|B_z|)$ \\
  \var{bbxmax}    & $\max(|B_x|) excluding Bv_{ext}$ \\
  \var{bbymax}    & $\max(|B_y|) excluding Bv_{ext}$ \\
  \var{bbzmax}    & $\max(|B_z|) excluding Bv_{ext}$ \\
  \var{jxmax}     & $\max(|jv_x|)$ \\
  \var{jymax}     & $\max(|jv_y|)$ \\
  \var{jzmax}     & $\max(|jv_z|)$ \\
  \var{jrms}      & $\left<\jv^2\right>^{1/2}$ \\
  \var{hjrms}     & $\left<\jv^2\right>^{1/2}$ \\
  \var{jmax}      & $\max(|\jv|)$ \\
  \var{vArms}     & $\left<\Bv^2/\varrho\right>^{1/2}$ \\
  \var{vAmax}     & $\max(\Bv^2/\varrho)^{1/2}$ \\
  \var{dtb}       & $\delta t / [c_{\delta t}\,\delta x
                    /v_{\rm A,max}]$
                    \quad(time step relative to
                    Alfv{\'e}n time step;
                    see \S~\ref{time-step}) \\
  \var{dteta}     & $\delta t/[c_{\delta t,{\rm v}}\,
                    \delta x^2/\eta_{\rm max}]$
                    \quad(time step relative to
                    resistive time step;
                    see \S~\ref{time-step}) \\
  \var{a2m}       & $\left<\Av^2\right>$ \\
  \var{arms}      & $\left<\Av^2\right>^{1/2}$ \\
  \var{amax}      & $\max(|\Av|)$ \\
  \var{divarms}   & $\langle(\nabla\cdot\Av)^2\rangle^{1/2}$ \\
  \var{beta1m}    & $\left<\Bv^2/(2\mu_0 p)\right>$
                    \quad(mean inverse plasma beta) \\
  \var{beta1max}  & $\max[\Bv^2/(2\mu_0 p)]$
                    \quad(maximum inverse plasma beta) \\
  \var{betam}     & $\langle\beta\rangle$ \\
  \var{betamax}   & $\max\beta$ \\
  \var{betamin}   & $\min\beta$ \\
  \var{bxm}       & $\left<B_x\right>$ \\
  \var{bym}       & $\left<B_y\right>$ \\
  \var{bzm}       & $\left<B_z\right>$ \\
  \var{bxbym}     & $\left<B_x B_y\right>$ \\
  \var{bmx}       & $\left<\left<\Bv\right>_{yz}^2
                    \right>^{1/2}$
                    \quad(energy of $yz$-averaged
                    mean field) \\
  \var{bmy}       & $\left<\left<\Bv\right>_{xz}^2
                    \right>^{1/2}$
                    \quad(energy of $xz$-averaged
                    mean field) \\
  \var{bmz}       & $\left<\left<\Bv\right>_{xy}^2
                    \right>^{1/2}$
                    \quad(energy of $xy$-averaged
                    mean field) \\
  \var{bmzS2}     & $\left<\left<\Bv_S\right>_{xy}^2\right>$ \\
  \var{bmzA2}     & $\left<\left<\Bv_A\right>_{xy}^2\right>$ \\
  \var{jmx}       & $\left<\left<\Jv\right>_{yz}^2
                    \right>^{1/2}$
                    \quad(energy of $yz$-averaged
                    mean current density) \\
  \var{jmy}       & $\left<\left<\Jv\right>_{xz}^2
                    \right>^{1/2}$
                    \quad(energy of $xz$-averaged
                    mean current density) \\
  \var{jmz}       & $\left<\left<\Jv\right>_{xy}^2
                    \right>^{1/2}$
                    \quad(energy of $xy$-averaged
                    mean current density) \\
  \var{bmzph}     & Phase of a Beltrami field \\
  \var{bmzphe}    & Error of phase of a Beltrami field \\
  \var{bsinphz}   & sine of phase of a Beltrami field \\
  \var{bcosphz}   & cosine of phase of a Beltrami field \\
  \var{emxamz3}   & $\left<\left<\Ev\right>_{xy}\times\left<\Av\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean field helicity flux) \\
  \var{embmz}     & $\left<\left<\Ev\right>_{xy}\cdot\left<\Bv\right>_{xy}
                    \right>$ \quad($xy$-averaged
                    mean field helicity production ) \\
  \var{ambmz}     & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field) \\
  \var{ambmzh}    & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field, temp) \\
  \var{ambmzn}    & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field, north) \\
  \var{ambmzs}    & $\left<\left<\Av\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>$
                    \quad (magnetic helicity of $xy$-averaged mean field, south) \\
  \var{jmbmz}     & $\left<\left<\Jv\right>_{xy}\cdot\left<\Bv\right>_{xy}
                    \right>$ \quad(current helicity
                    of $xy$-averaged mean field) \\
  \var{kx_aa}     & $k_x$ \\
  \var{kmz}       & $\left<\left<\Jv\right>_{xy}\cdot\left<\Bv\right>_{xy}\right>/
                    \left<\left<\Bv\right>_{xy}^2\right>$ \\
  \var{bx2m}      & $\left< B_x^2 \right>$ \\
  \var{by2m}      & $\left< B_y^2 \right>$ \\
  \var{bz2m}      & $\left< B_z^2 \right>$ \\
  \var{uxbm}      & $\left<\uv\times\Bv\right>\cdot\Bv_0/B_0^2$ \\
  \var{jxbm}      & $\left<\jv\times\Bv\right>\cdot\Bv_0/B_0^2$ \\
  \var{magfricmax} & Magneto-Frictional velocity $\left<\jv\times\Bv\right>\cdot\Bv^2$ \\
  \var{b3b21m}    & $\left<B_3 B_{2,1} \right>$ \\
  \var{b3b12m}    & $\left<B_3 B_{1,2} \right>$ \\
  \var{b1b32m}    & $\left<B_1 B_{3,2} \right>$ \\
  \var{b1b23m}    & $\left<B_1 B_{2,3} \right>$ \\
  \var{b2b13m}    & $\left<B_2 B_{1,3} \right>$ \\
  \var{b2b31m}    & $\left<B_2 B_{3,1} \right>$ \\
  \var{uxbmx}     & $\left<(\uv\times\Bv)_x\right>$ \\
  \var{uxbmy}     & $\left<(\uv\times\Bv)_y\right>$ \\
  \var{uxbmz}     & $\left<(\uv\times\Bv)_z\right>$ \\
  \var{jxbmx}     & $\left<(\jv\times\Bv)_x\right>$ \\
  \var{jxbmy}     & $\left<(\jv\times\Bv)_y\right>$ \\
  \var{jxbmz}     & $\left<(\jv\times\Bv)_z\right>$ \\
  \var{examx}     & $\left<\Ev\times\Av\right>|_x$ \\
  \var{examy}     & $\left<\Ev\times\Av\right>|_y$ \\
  \var{examz}     & $\left<\Ev\times\Av\right>|_z$ \\
  \var{exjmx}     & $\left<\Ev\times\Jv\right>|_x$ \\
  \var{exjmy}     & $\left<\Ev\times\Jv\right>|_y$ \\
  \var{exjmz}     & $\left<\Ev\times\Jv\right>|_z$ \\
  \var{dexbmx}    & $\left<\nabla\times\Ev\times\Bv\right>|_x$ \\
  \var{dexbmy}    & $\left<\nabla\times\Ev\times\Bv\right>|_y$ \\
  \var{dexbmz}    & $\left<\nabla\times\Ev\times\Bv\right>|_z$ \\
  \var{phibmx}    & $\left<\phi\Bv\right>|_x$ \\
  \var{phibmy}    & $\left<\phi\Bv\right>|_y$ \\
  \var{phibmz}    & $\left<\phi\Bv\right>|_z$ \\
  \var{b2divum}   & $\left<\Bv^2\nabla\cdot\uv\right>$ \\
  \var{ujxbm}     & $\left<\uv\cdot(\Jv\times\Bv)\right>$ \\
  \var{jxbrmax}   & $\max(|\Jv\times\Bv/\rho|)$ \\
  \var{jxbr2m}    & $\left<(\Jv\times\Bv/\rho)^2\right>$ \\
  \var{bmxy_rms}  & $\sqrt{[\left<b_x\right>_z(x,y)]^2 +
                    [\left<b_y\right>_z(x,y)]^2 +
                    [\left<b_z\right>_z(x,y)]^2} $ \\
  \var{etasmagm}  & Mean of Smagorinsky resistivity \\
  \var{etasmagmin} & Min of Smagorinsky resistivity \\
  \var{etasmagmax} & Max of Smagorinsky resistivity \\
  \var{etavamax}  & Max of artificial resistivity
                    $\eta\sim v_A$ \\
  \var{etajmax}   & Max of artificial resistivity
                    $\eta\sim J / \sqrt{\rho}$ \\
  \var{etaj2max}  & Max of artificial resistivity
                    $\eta\sim J^2 / \rho$ \\
  \var{etajrhomax} & Max of artificial resistivity
                    $\eta\sim J / \rho$ \\
  \var{cosjbm}    & $\left<\Jv\cdot\Bv/(|\Jv|\,|\Bv|)\right>$ \\
  \var{jparallelm} & Mean value of the component
                    of J parallel to B \\
  \var{jperpm}    & Mean value of the component
                    of J perpendicular to B \\
  \var{hjparallelm} & Mean value of the component
                    of $J_{\rm hyper}$ parallel to B \\
  \var{hjperpm}   & Mean value of the component
                    of $J_{\rm hyper}$ perpendicular to B \\
  \var{brmsx}     & $\left<\Bv^2\right>^{1/2}$ for
                    the magnetic_xaver_range \\
  \var{brmsz}     & $\left<\Bv^2\right>^{1/2}$ for
                    the magnetic_zaver_range \\
  \var{Exmxy}     & $\left<{\cal E}_x\right>_{z}$ \\
  \var{Eymxy}     & $\left<{\cal E}_y\right>_{z}$ \\
  \var{Ezmxy}     & $\left<{\cal E}_z\right>_{z}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{maxwell.f90}} \\
\midrule
  \var{aa2m}      & $\langle A^2\rangle$ \\
  \var{ee2m}      & $\langle E^2\rangle$ \\
  \var{EEEM}      & $\langle(E^2+B^2)/2\rangle$ \\
  \var{akxpt}     & $Akx^{pt}$ \\
  \var{ekxpt}     & $Ekx^{pt}$ \\
  \var{sigma}     & $\sigma$ \\
  \var{emag}      & $\int_V{1\over2\mu_0}\Bv^2\, dV$ \\
  \var{bmax}      & $\max(|\Bv|)$ \\
  \var{brms}      & $\left<\Bv^2\right>^{1/2}$ \\
  \var{arms}      & $\left<\Av^2\right>^{1/2}$ \\
  \var{erms}      & $\left<\Ev^2\right>^{1/2}$ \\
  \var{bfrms}     & $\left<{\Bv'}^2\right>^{1/2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{meanfield.f90}} \\
\midrule
  \var{qsm}       & $\left<q_p(\overline{B})\right>$ \\
  \var{qpm}       & $\left<q_p(\overline{B})\right>$ \\
  \var{qem}       & $\left<q_e(\overline{B})\right>$,
                    in the paper referred to as
                    $\left<q_g(\overline{B})\right>$ \\
  \var{qam}       & $\left<q_a(\overline{B})\right>$ \\
  \var{alpm}      & $\left<\alpha\right>$ \\
  \var{etatm}     & $\left<\eta_{\rm t}\right>$ \\
  \var{EMFmz1}    & $\left<{\cal E}\right>_{xy}|_x$ \\
  \var{EMFmz2}    & $\left<{\cal E}\right>_{xy}|_y$ \\
  \var{EMFmz3}    & $\left<{\cal E}\right>_{xy}|_z$ \\
  \var{EMFdotBm}  & $\left<{\cal E}\cdot\Bv \right>$ \\
  \var{EMFdotB_int} & $\int{\cal E}\cdot\Bv dV$ \\
\midrule
  \multicolumn{2}{c}{Module \file{meanfield_demfdt.f90}} \\
\midrule
  \var{EMFrms}    & $(\left<{\cal E}\right>)_{\rm rms}$ \\
  \var{EMFmax}    & $\max(\left<{\cal E}\right>)$ \\
  \var{EMFmin}    & $\min(\left<{\cal E}\right>)$ \\
\midrule
  \multicolumn{2}{c}{Module \file{neutralvelocity.f90}} \\
\midrule
  \var{epsKn}     & $\left<2\nu_n\varrho_n\Strain_n^2\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{noentropy.f90}} \\
\midrule
  \var{dtc}       & $\delta t/[c_{\delta t}\,\delta_x
                    /\max c_{\rm s}]$
                    \quad(time step relative to
                    acoustic time step;
                    see \S~\ref{time-step}) \\
  \var{ethm}      & $\left<\varrho e\right>$
                    \quad(mean thermal
                    [=internal] energy) \\
  \var{pdivum}    & $\left<p\nabla\uv\right>$ \\
  \var{csm}       & $\left<c_{\rm s}\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_caustics.f90}} \\
\midrule
  \var{TrSigmapm} & $\langle{\rm Tr}\left[\sigma\right]\rangle$ \\
  \var{blowupm}   & Mean no. of times $\sigma$ falls below cutoff \\
  \var{lnVpm}     & Mean of (logarithm of) Volume around an inertial particle \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_chemistry.f90}} \\
\midrule
  \var{Shchm}     & $\rm{mean particle Sherwood number}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_dust.f90}} \\
\midrule
  \var{xpm}       & $x_{part}$ \\
  \var{xpmin}     & $x_{part}$ \\
  \var{xpmax}     & $x_{part}$ \\
  \var{xp2m}      & $x^2_{part}$ \\
  \var{vrelpabsm} & $\rm{Absolute value of mean relative velocity}$ \\
  \var{vpxm}      & $u_{part}$ \\
  \var{vpx2m}     & $u^2_{part}$ \\
  \var{ekinp}     & $E_{kin,part}$ \\
  \var{vpxmax}    & $MAX(u_{part})$ \\
  \var{vpxmin}    & $MIN(u_{part})$ \\
  \var{npm}       & $\rm{mean particle number density}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_dust_brdeplete.f90}} \\
\midrule
  \var{xpm}       & $x_{part}$ \\
  \var{xp2m}      & $x^2_{part}$ \\
  \var{vrelpabsm} & $\rm{Absolute value of mean relative velocity}$ \\
  \var{vpxm}      & $u_{part}$ \\
  \var{vpx2m}     & $u^2_{part}$ \\
  \var{ekinp}     & $E_{kin,part}$ \\
  \var{vpxmax}    & $MAX(u_{part})$ \\
  \var{vpxmin}    & $MIN(u_{part})$ \\
  \var{npm}       & $\rm{mean particle number density}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_lagrangian.f90}} \\
\midrule
  \var{xpm}       & $x_{part}$ \\
  \var{xp2m}      & $x^2_{part}$ \\
  \var{vrelpabsm} & $\rm{Absolute value of mean relative velocity}$ \\
  \var{vpxm}      & $u_{part}$ \\
  \var{vpx2m}     & $u^2_{part}$ \\
  \var{ekinp}     & $E_{kin,part}$ \\
  \var{vpxmax}    & $MAX(u_{part})$ \\
  \var{vpxmin}    & $MIN(u_{part})$ \\
  \var{npm}       & $\rm{mean particle number density}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_mass_swarm.f90}} \\
\midrule
  \var{mpm}       & $\overline{m_p}$ \\
  \var{mpmin}     & $\min_j m_{p,j}$ \\
  \var{mpmax}     & $\max_j m_{p,j}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_surfspec.f90}} \\
\midrule
  \var{dtpchem}   & $dt_{particle,chemistry}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{particles_tetrad.f90}} \\
\midrule
  \var{TVolm}     & Mean absolute volume of the tetrads \\
  \var{TVolpm}    & Mean of positive volume of the tetrads \\
  \var{TVolnm}    & Mean of negative volume of the tetrads \\
  \var{VelVolm}   & Mean absolute volume of the tetrads in velocity space \\
  \var{VelVolpm}  & Mean of positive volume of the tetrads in velocity space \\
  \var{VelVolnm}  & Mean of negative volume of the tetrads in velocity space. \\
\midrule
  \multicolumn{2}{c}{Module \file{polymer.f90}} \\
\midrule
  \var{polytrm}   & $\left\langle Tr[C_{ij}]\right\rangle$ \\
  \var{frmax}     & $\max(f(r))$ \\
\midrule
  \multicolumn{2}{c}{Module \file{radial_dist_func.f90}} \\
\midrule
  \var{rad}       & $r/r_\ast$ \\
  \var{tauk}      & $\tau_k$ \\
  \var{tt1m}      & $\langle T \rangle$ \\
  \var{qq1m}      & $\langle \ln T \rangle$ \\
  \var{qq2m}      & $\langle \ln T^2 \rangle$ \\
  \var{qq3m}      & $\langle \ln T^3 \rangle$ \\
  \var{qq4m}      & $\langle \ln T^4 \rangle$ \\
\midrule
  \multicolumn{2}{c}{Module \file{reaction_0D.f90}} \\
\midrule
  \var{eem}       & $\langle \eta \rangle$ \\
  \var{ee1m}      & $\langle |\eta| \rangle$ \\
  \var{ee2m}      & $\langle \eta^2 \rangle$ \\
  \var{ee3m}      & $\langle \eta^3 \rangle$ \\
  \var{ee4m}      & $\langle \eta^4 \rangle$ \\
  \var{ee10}      & $\langle \eta_{10\%} \rangle$ \\
  \var{ee50}      & $\langle \eta_{50\%} \rangle$ \\
  \var{ee90}      & $\langle \eta_{90\%} \rangle$ \\
  \var{ee99}      & $\langle \eta_{99\%} \rangle$ \\
  \var{AAm}       & $\langle [A] \rangle$ \\
  \var{DDm}       & $\langle [D] \rangle$ \\
  \var{LLm}       & $\langle [L] \rangle$ \\
  \var{DLm}       & $\langle [D]+[L] \rangle$ \\
  \var{kC}        & $k_C$ \\
  \var{A1}        & $A_1$ \\
  \var{A2}        & $A_2$ \\
  \var{A3}        & $A_3$ \\
  \var{A4}        & $A_4$ \\
  \var{A5}        & $A_5$ \\
  \var{D1}        & $D_1$ \\
  \var{D2}        & $D_2$ \\
  \var{D3}        & $D_3$ \\
  \var{D4}        & $D_4$ \\
  \var{D5}        & $D_5$ \\
  \var{L1}        & $L_1$ \\
  \var{L2}        & $L_2$ \\
  \var{L3}        & $L_3$ \\
  \var{L4}        & $L_4$ \\
  \var{L5}        & $L_5$ \\
\midrule
  \multicolumn{2}{c}{Module \file{rel_1d.f90}} \\
\midrule
  \var{betm}      & $\left<\beta\right>$ \\
  \var{betmax}    & $\beta_{\max}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{selfgravity.f90}} \\
\midrule
  \var{rugpotselfm} & $\left<\rho\uv\cdot\nabla\Phi\right>$ \\
  \var{gpotself2m} & $\left<(\nabla\Phi)^2\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{shear.f90}} \\
\midrule
  \var{dtshear}   & advec\_shear/cdt \\
  \var{deltay}    & deltay \\
\midrule
  \multicolumn{2}{c}{Module \file{shock.f90}} \\
\midrule
  \var{shockmax}  & Max shock number \\
\midrule
  \multicolumn{2}{c}{Module \file{shock_highorder.f90}} \\
\midrule
  \var{gshockmax} & $\max\left|\nabla\nu_{shock}\right|$ \\
\midrule
  \multicolumn{2}{c}{Module \file{solar_corona.f90}} \\
\midrule
  \var{dtvel}     & Velocity driver time step \\
  \var{dtnewt}    & Radiative cooling time step \\
  \var{dtradloss} & Radiative losses time step \\
  \var{dtchi2}    & $\delta t / [c_{\delta t,{\rm v}}\,
                    \delta x^2/\chi_{\rm max}]$
                    \quad(time step relative to time
                    step based on heat conductivity;
                    see \S~\ref{time-step}) \\
  \var{dtspitzer} & Spitzer heat conduction time step \\
  \var{mag_flux}  & Total vertical magnetic flux at \\
\midrule
  \multicolumn{2}{c}{Module \file{solid_cells_CGEO.f90}} \\
\midrule
\midrule
  \multicolumn{2}{c}{Module \file{solid_cells_ogrid_chemistry.f90}} \\
\midrule
  \var{dtchem}    & $dt_{chem}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{solid_cells_reactive.f90}} \\
\midrule
\midrule
  \multicolumn{2}{c}{Module \file{temperature_idealgas.f90}} \\
\midrule
  \var{TTmax}     & $\max (T)$ \\
  \var{gTmax}     & $\max (|\nabla T|)$ \\
  \var{TTmin}     & $\min (T)$ \\
  \var{TTm}       & $\left< T \right>$ \\
  \var{TTzmask}   & $\left< T \right>$ for
                    the temp_zaver_range \\
  \var{TT2m}      & $\left< T^2 \right>$ \\
  \var{TugTm}     & $\left< T\uv\cdot\nabla T \right>$ \\
  \var{Trms}      & $\sqrt{\left< T^2 \right>}$ \\
  \var{uxTm}      & $\left< u_x T \right>$ \\
  \var{uyTm}      & $\left< u_y T \right>$ \\
  \var{uzTm}      & $\left< u_z T \right>$ \\
  \var{gT2m}      & $\left< (\nabla T)^2 \right>$ \\
  \var{guxgTm}    & $\left< \nabla u_x \cdot \nabla T \right>$ \\
  \var{guygTm}    & $\left< \nabla u_y \cdot \nabla T \right>$ \\
  \var{guzgTm}    & $\left< \nabla u_z \cdot \nabla T \right>$ \\
  \var{Tugux_uxugTm} & $\left< T \uv\cdot\nabla u_x + u_x \uv\cdot\nabla T \right>
                    =\left< \uv\cdot\nabla(u_x T) \right>$ \\
  \var{Tuguy_uyugTm} & $\left< T \uv\cdot\nabla u_y + u_y \uv\cdot\nabla T \right>
                    =\left< \uv\cdot\nabla(u_y T) \right>$ \\
  \var{Tuguz_uzugTm} & $\left< T \uv\cdot\nabla u_z + u_z \uv\cdot\nabla T \right>
                    =\left< \uv\cdot\nabla(u_z T) \right>$ \\
  \var{Tdxpm}     & $\left< T dp/dx \right>$ \\
  \var{Tdypm}     & $\left< T dp/dy \right>$ \\
  \var{Tdzpm}     & $\left< T dp/dz \right>$ \\
  \var{fradtop}   & $<-K{dT\over dz}>_{\text{top}}$
                    \quad(top radiative flux) \\
  \var{fradbot}   & $<-K{dT\over dz}>_{\text{bot}}$
                    \quad(bottom radiative flux) \\
  \var{yHmax}     & DOCUMENT ME \\
  \var{yHmin}     & DOCUMENT ME \\
  \var{yHm}       & DOCUMENT ME \\
  \var{ethm}      & $\left< e_{\text{th}}\right> =
                    \left< c_v \rho T \right> $
                    \quad(mean thermal energy) \\
  \var{eem}       & $\left< e \right> =
                    \left< c_v T \right>$
                    \quad(mean internal energy) \\
  \var{ethtot}    & $\int_V\varrho e\,dV$
                    \quad(total thermal energy) \\
  \var{ssm}       & $\overline{S}$ \\
  \var{thcool}    & $\tau_{\rm cool}$ \\
  \var{ppm}       & $\overline{P}$ \\
  \var{csm}       & $\overline{c}_{\rm s}$ \\
  \var{csmax}     & $\max (c_{\rm s})$ \\
  \var{dtc}       & $\delta t/[c_{\delta t}\,\delta_x
                    /\max c_{\rm s}]$
                    \quad(time step relative to
                    acoustic time step;
                    see \S~\ref{time-step}) \\
  \var{dtchi}     & $\delta t / [c_{\delta t,{\rm v}}\,
                    \delta x^2/\chi_{\rm max}]$
                    \quad(time step relative to time
                    step based on heat conductivity;
                    see \S~\ref{time-step}) \\
\midrule
  \multicolumn{2}{c}{Module \file{temperature_ionization.f90}} \\
\midrule
  \var{TTmax}     & $\max (T)$ \\
  \var{TTmin}     & $\min (T)$ \\
  \var{TTm}       & $\left< T \right>$ \\
  \var{ethm}      & $\left< e_{\text{th}}\right> =
                    \left< c_v \rho T \right> $
                    \quad(mean thermal energy) \\
  \var{eem}       & $\left< e \right> $
                    \quad(mean internal energy) \\
  \var{ppm}       & $\left< p \right> $ \\
  \var{Tppm}      & $\left<\max(p_{\rm thresh}-p,0)_{\rm norm}\right> $ \\
\midrule
  \multicolumn{2}{c}{Module \file{test_chemistry.f90}} \\
\midrule
  \var{dtchem}    & $dt_{chem}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_axisym.f90}} \\
\midrule
  \var{alpPERP}   & $\alpha_\perp$ \\
  \var{alpPARA}   & $\alpha_\perp$ \\
  \var{gam}       & $\gamma$ \\
  \var{betPERP}   & $\beta_\perp$ \\
  \var{betPARA}   & $\beta_\perp$ \\
  \var{del}       & $\delta$ \\
  \var{kapPERP}   & $\kappa_\perp$ \\
  \var{kapPARA}   & $\kappa_\perp$ \\
  \var{mu}        & $\mu$ \\
  \var{alpPERPz}  & $\alpha_\perp(z)$ \\
  \var{alpPARAz}  & $\alpha_\perp(z)$ \\
  \var{gamz}      & $\gamma(z)$ \\
  \var{betPERPz}  & $\beta_\perp(z)$ \\
  \var{betPARAz}  & $\beta_\perp(z)$ \\
  \var{delz}      & $\delta(z)$ \\
  \var{kapPERPz}  & $\kappa_\perp(z)$ \\
  \var{kapPARAz}  & $\kappa_\perp(z)$ \\
  \var{muz}       & $\mu(z)$ \\
  \var{bx1pt}     & $b_x^{1}$ \\
  \var{bx2pt}     & $b_x^{2}$ \\
  \var{bx3pt}     & $b_x^{3}$ \\
  \var{b1rms}     & $\left<b_{1}^2\right>^{1/2}$ \\
  \var{b2rms}     & $\left<b_{2}^2\right>^{1/2}$ \\
  \var{b3rms}     & $\left<b_{3}^2\right>^{1/2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_axisym2.f90}} \\
\midrule
  \var{alpPERP}   & $\alpha_\perp$ \\
  \var{alpPARA}   & $\alpha_\perp$ \\
  \var{gam}       & $\gamma$ \\
  \var{betPERP}   & $\beta_\perp$ \\
  \var{betPARA}   & $\beta_\perp$ \\
  \var{del}       & $\delta$ \\
  \var{kapPERP}   & $\kappa_\perp$ \\
  \var{kapPARA}   & $\kappa_\perp$ \\
  \var{mu}        & $\mu$ \\
  \var{bx1pt}     & $b_x^{1}$ \\
  \var{bx2pt}     & $b_x^{2}$ \\
  \var{bx3pt}     & $b_x^{3}$ \\
  \var{b1rms}     & $\left<b_{1}^2\right>^{1/2}$ \\
  \var{b2rms}     & $\left<b_{2}^2\right>^{1/2}$ \\
  \var{b3rms}     & $\left<b_{3}^2\right>^{1/2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_axisym4.f90}} \\
\midrule
  \var{alpPERP}   & $\alpha_\perp$ \\
  \var{alpPARA}   & $\alpha_\perp$ \\
  \var{gam}       & $\gamma$ \\
  \var{betPERP}   & $\beta_\perp$ \\
  \var{betPERP2}  & $\beta_\perp^{(2)}$ \\
  \var{betPARA}   & $\beta_\perp$ \\
  \var{del}       & $\delta$ \\
  \var{del2}      & $\delta^{(2)}$ \\
  \var{kapPERP}   & $\kappa_\perp$ \\
  \var{kapPERP2}  & $\kappa_\perp^{(2)}$ \\
  \var{kapPARA}   & $\kappa_\perp$ \\
  \var{mu}        & $\mu$ \\
  \var{mu2}       & $\mu^{(2)}$ \\
  \var{alpPERPz}  & $\alpha_\perp(z)$ \\
  \var{alpPARAz}  & $\alpha_\perp(z)$ \\
  \var{gamz}      & $\gamma(z)$ \\
  \var{betPERPz}  & $\beta_\perp(z)$ \\
  \var{betPARAz}  & $\beta_\perp(z)$ \\
  \var{delz}      & $\delta(z)$ \\
  \var{kapPERPz}  & $\kappa_\perp(z)$ \\
  \var{kapPARAz}  & $\kappa_\perp(z)$ \\
  \var{muz}       & $\mu(z)$ \\
  \var{bx1pt}     & $b_x^{1}$ \\
  \var{bx2pt}     & $b_x^{2}$ \\
  \var{bx3pt}     & $b_x^{3}$ \\
  \var{b1rms}     & $\left<b_{1}^2\right>^{1/2}$ \\
  \var{b2rms}     & $\left<b_{2}^2\right>^{1/2}$ \\
  \var{b3rms}     & $\left<b_{3}^2\right>^{1/2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_compress_z.f90}} \\
\midrule
  \var{alp11}     & $\alpha_{11}$ \\
  \var{alp21}     & $\alpha_{21}$ \\
  \var{alp31}     & $\alpha_{31}$ \\
  \var{alp12}     & $\alpha_{12}$ \\
  \var{alp22}     & $\alpha_{22}$ \\
  \var{alp32}     & $\alpha_{32}$ \\
  \var{eta11}     & $\eta_{11}k$ \\
  \var{eta21}     & $\eta_{21}k$ \\
  \var{eta12}     & $\eta_{12}k$ \\
  \var{eta22}     & $\eta_{22}k$ \\
  \var{alpK}      & $\alpha^K$ \\
  \var{alpM}      & $\alpha^M$ \\
  \var{alpMK}     & $\alpha^{MK}$ \\
  \var{phi11}     & $\phi_{11}$ \\
  \var{phi21}     & $\phi_{21}$ \\
  \var{phi12}     & $\phi_{12}$ \\
  \var{phi22}     & $\phi_{22}$ \\
  \var{phi32}     & $\phi_{32}$ \\
  \var{psi11}     & $\psi_{11}k$ \\
  \var{psi21}     & $\psi_{21}k$ \\
  \var{psi12}     & $\psi_{12}k$ \\
  \var{psi22}     & $\psi_{22}k$ \\
  \var{sig1}      & $\sigma_1$ \\
  \var{sig2}      & $\sigma_2$ \\
  \var{sig3}      & $\sigma_3$ \\
  \var{tau1}      & $\tau_1$ \\
  \var{tau2}      & $\tau_2$ \\
  \var{phiK}      & $\phi^K$ \\
  \var{phiM}      & $\phi^M$ \\
  \var{phiMK}     & $\phi^{MK}$ \\
  \var{alp11cc}   & $\alpha_{11}\cos^2 kz$ \\
  \var{alp21sc}   & $\alpha_{21}\sin kz\cos kz$ \\
  \var{alp12cs}   & $\alpha_{12}\cos kz\sin kz$ \\
  \var{alp22ss}   & $\alpha_{22}\sin^2 kz$ \\
  \var{eta11cc}   & $\eta_{11}\cos^2 kz$ \\
  \var{eta21sc}   & $\eta_{21}\sin kz\cos kz$ \\
  \var{eta12cs}   & $\eta_{12}\cos kz\sin kz$ \\
  \var{eta22ss}   & $\eta_{22}\sin^2 kz$ \\
  \var{s2kzDFm}   & $\left<\sin2kz\nabla\cdot F\right>$ \\
  \var{M11}       & ${\cal M}_{11}$ \\
  \var{M22}       & ${\cal M}_{22}$ \\
  \var{M33}       & ${\cal M}_{33}$ \\
  \var{M11cc}     & ${\cal M}_{11}\cos^2 kz$ \\
  \var{M11ss}     & ${\cal M}_{11}\sin^2 kz$ \\
  \var{M22cc}     & ${\cal M}_{22}\cos^2 kz$ \\
  \var{M22ss}     & ${\cal M}_{22}\sin^2 kz$ \\
  \var{M12cs}     & ${\cal M}_{12}\cos kz\sin kz$ \\
  \var{bx11pt}    & $b_x^{11}$ \\
  \var{bx21pt}    & $b_x^{21}$ \\
  \var{bx12pt}    & $b_x^{12}$ \\
  \var{bx22pt}    & $b_x^{22}$ \\
  \var{bx0pt}     & $b_x^{0}$ \\
  \var{by11pt}    & $b_y^{11}$ \\
  \var{by21pt}    & $b_y^{21}$ \\
  \var{by12pt}    & $b_y^{12}$ \\
  \var{by22pt}    & $b_y^{22}$ \\
  \var{by0pt}     & $b_y^{0}$ \\
  \var{u11rms}    & $\left<u_{11}^2\right>^{1/2}$ \\
  \var{u21rms}    & $\left<u_{21}^2\right>^{1/2}$ \\
  \var{u12rms}    & $\left<u_{12}^2\right>^{1/2}$ \\
  \var{u22rms}    & $\left<u_{22}^2\right>^{1/2}$ \\
  \var{h11rms}    & $\left<h_{11}^2\right>^{1/2}$ \\
  \var{h21rms}    & $\left<h_{21}^2\right>^{1/2}$ \\
  \var{h12rms}    & $\left<h_{12}^2\right>^{1/2}$ \\
  \var{h22rms}    & $\left<h_{22}^2\right>^{1/2}$ \\
  \var{j11rms}    & $\left<j_{11}^2\right>^{1/2}$ \\
  \var{b11rms}    & $\left<b_{11}^2\right>^{1/2}$ \\
  \var{b21rms}    & $\left<b_{21}^2\right>^{1/2}$ \\
  \var{b12rms}    & $\left<b_{12}^2\right>^{1/2}$ \\
  \var{b22rms}    & $\left<b_{22}^2\right>^{1/2}$ \\
  \var{ux0m}      & $\left<u_{0_x}\right>$ \\
  \var{uy0m}      & $\left<u_{0_y}\right>$ \\
  \var{ux11m}     & $\left<u_{11_x}\right>$ \\
  \var{uy11m}     & $\left<u_{11_y}\right>$ \\
  \var{u0rms}     & $\left<u_{0}^2\right>^{1/2}$ \\
  \var{b0rms}     & $\left<b_{0}^2\right>^{1/2}$ \\
  \var{h0rms}     & $\left<h_{0}^2\right>^{1/2}$ \\
  \var{rho0m}     & $\left<\exp h_{0}\right>$ \\
  \var{u0max}     & $\operatorname{max}\left|\boldsymbol{u}_{0}\right|$ \\
  \var{b0max}     & $\operatorname{max}\left|\boldsymbol{b}_{0}\right|$ \\
  \var{h0max}     & $\operatorname{max}h_{0}$ \\
  \var{bhrms}     & $\left<b_{h}^2\right>^{1/2}$ \\
  \var{jb0m}      & $\left<jb_{0}\right>$ \\
  \var{E11rms}    & $\left<{\cal E}_{11}^2\right>^{1/2}$ \\
  \var{E21rms}    & $\left<{\cal E}_{21}^2\right>^{1/2}$ \\
  \var{E12rms}    & $\left<{\cal E}_{12}^2\right>^{1/2}$ \\
  \var{E22rms}    & $\left<{\cal E}_{22}^2\right>^{1/2}$ \\
  \var{E0rms}     & $\left<{\cal E}_{0}^2\right>^{1/2}$ \\
  \var{E0mrms}    & $\left<{\cal E}_{0}^2\right>^{1/2}$ \\
  \var{E0xrms}    & $\left<{\cal E}_{0,x}^2\right>^{1/2}$ \\
  \var{E0yrms}    & $\left<{\cal E}_{0,y}^2\right>^{1/2}$ \\
  \var{Ex11pt}    & ${\cal E}_x^{11}$ \\
  \var{Ex21pt}    & ${\cal E}_x^{21}$ \\
  \var{Ex12pt}    & ${\cal E}_x^{12}$ \\
  \var{Ex22pt}    & ${\cal E}_x^{22}$ \\
  \var{Ex0pt}     & ${\cal E}_x^{0}$ \\
  \var{Ey11pt}    & ${\cal E}_y^{11}$ \\
  \var{Ey21pt}    & ${\cal E}_y^{21}$ \\
  \var{Ey12pt}    & ${\cal E}_y^{12}$ \\
  \var{Ey22pt}    & ${\cal E}_y^{22}$ \\
  \var{Ey0pt}     & ${\cal E}_y^{0}$ \\
  \var{bamp}      & bamp \\
  \var{E111z}     & ${\cal E}_1^{11}$ \\
  \var{E211z}     & ${\cal E}_2^{11}$ \\
  \var{E311z}     & ${\cal E}_3^{11}$ \\
  \var{E121z}     & ${\cal E}_1^{21}$ \\
  \var{E221z}     & ${\cal E}_2^{21}$ \\
  \var{E321z}     & ${\cal E}_3^{21}$ \\
  \var{E112z}     & ${\cal E}_1^{12}$ \\
  \var{E212z}     & ${\cal E}_2^{12}$ \\
  \var{E312z}     & ${\cal E}_3^{12}$ \\
  \var{E122z}     & ${\cal E}_1^{22}$ \\
  \var{E222z}     & ${\cal E}_2^{22}$ \\
  \var{E322z}     & ${\cal E}_3^{22}$ \\
  \var{alp11z}    & $\alpha_{11}(z,t)$ \\
  \var{alp21z}    & $\alpha_{21}(z,t)$ \\
  \var{alp12z}    & $\alpha_{12}(z,t)$ \\
  \var{alp22z}    & $\alpha_{22}(z,t)$ \\
  \var{eta11z}    & $\eta_{11}(z,t)$ \\
  \var{eta21z}    & $\eta_{21}(z,t)$ \\
  \var{eta12z}    & $\eta_{12}(z,t)$ \\
  \var{eta22z}    & $\eta_{22}(z,t)$ \\
  \var{E10z}      & ${\cal E}_1^{0}$ \\
  \var{E20z}      & ${\cal E}_2^{0}$ \\
  \var{E30z}      & ${\cal E}_3^{0}$ \\
  \var{EBpq}      & ${\cal E}\cdot\Bv^{pq}$ \\
  \var{E0Um}      & ${\cal E}^0\cdot\Uv$ \\
  \var{E0Wm}      & ${\cal E}^0\cdot\Wv$ \\
  \var{bx0mz}     & $\left<b_{x}\right>_{xy}$ \\
  \var{by0mz}     & $\left<b_{y}\right>_{xy}$ \\
  \var{bz0mz}     & $\left<b_{z}\right>_{xy}$ \\
  \var{M11z}      & $\left<{\cal M}_{11}\right>_{xy}$ \\
  \var{M22z}      & $\left<{\cal M}_{22}\right>_{xy}$ \\
  \var{M33z}      & $\left<{\cal M}_{33}\right>_{xy}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_meri.f90}} \\
\midrule
  \var{E11xy}     & $E_{11xy}$ \\
  \var{E12xy}     & $E_{12xy}$ \\
  \var{E13xy}     & $E_{13xy}$ \\
  \var{E21xy}     & $E_{21xy}$ \\
  \var{E22xy}     & $E_{22xy}$ \\
  \var{E23xy}     & $E_{23xy}$ \\
  \var{E31xy}     & $E_{31xy}$ \\
  \var{E32xy}     & $E_{32xy}$ \\
  \var{E33xy}     & $E_{33xy}$ \\
  \var{E41xy}     & $E_{41xy}$ \\
  \var{E42xy}     & $E_{42xy}$ \\
  \var{E43xy}     & $E_{43xy}$ \\
  \var{E51xy}     & $E_{51xy}$ \\
  \var{E52xy}     & $E_{52xy}$ \\
  \var{E53xy}     & $E_{53xy}$ \\
  \var{E61xy}     & $E_{61xy}$ \\
  \var{E62xy}     & $E_{62xy}$ \\
  \var{E63xy}     & $E_{63xy}$ \\
  \var{E71xy}     & $E_{71xy}$ \\
  \var{E72xy}     & $E_{72xy}$ \\
  \var{E73xy}     & $E_{73xy}$ \\
  \var{E81xy}     & $E_{81}$ \\
  \var{E82xy}     & $E_{82}$ \\
  \var{E83xy}     & $E_{83}$ \\
  \var{E91xy}     & $E_{91}$ \\
  \var{E92xy}     & $E_{92}$ \\
  \var{E93xy}     & $E_{93}$ \\
  \var{a11xy}     & $\alpha_{11}$ \\
  \var{a12xy}     & $\alpha_{12}$ \\
  \var{a13xy}     & $\alpha_{13}$ \\
  \var{a21xy}     & $\alpha_{21}$ \\
  \var{a22xy}     & $\alpha_{22}$ \\
  \var{a23xy}     & $\alpha_{23}$ \\
  \var{a31xy}     & $\alpha_{31}$ \\
  \var{a32xy}     & $\alpha_{32}$ \\
  \var{a33xy}     & $\alpha_{33}$ \\
  \var{b111xy}    & $\b_{111}$ \\
  \var{b121xy}    & $\b_{121}$ \\
  \var{b131xy}    & $\b_{131}$ \\
  \var{b211xy}    & $\b_{211}$ \\
  \var{b221xy}    & $\b_{221}$ \\
  \var{b231xy}    & $\b_{231}$ \\
  \var{b311xy}    & $\b_{311}$ \\
  \var{b321xy}    & $\b_{321}$ \\
  \var{b331xy}    & $\b_{331}$ \\
  \var{b112xy}    & $\b_{112}$ \\
  \var{b122xy}    & $\b_{122}$ \\
  \var{b132xy}    & $\b_{132}$ \\
  \var{b212xy}    & $\b_{212}$ \\
  \var{b222xy}    & $\b_{222}$ \\
  \var{b232xy}    & $\b_{232}$ \\
  \var{b312xy}    & $\b_{312}$ \\
  \var{b322xy}    & $\b_{322}$ \\
  \var{b332xy}    & $\b_{332}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_nonlin_z.f90}} \\
\midrule
  \var{alp11}     & $\alpha_{11}$ \\
  \var{alp21}     & $\alpha_{21}$ \\
  \var{alp31}     & $\alpha_{31}$ \\
  \var{alp12}     & $\alpha_{12}$ \\
  \var{alp22}     & $\alpha_{22}$ \\
  \var{alp32}     & $\alpha_{32}$ \\
  \var{eta11}     & $\eta_{11}k$ \\
  \var{eta21}     & $\eta_{21}k$ \\
  \var{eta12}     & $\eta_{12}k$ \\
  \var{eta22}     & $\eta_{22}k$ \\
  \var{alpK}      & $\alpha^K$ \\
  \var{alpM}      & $\alpha^M$ \\
  \var{alpMK}     & $\alpha^{MK}$ \\
  \var{phi11}     & $\phi_{11}$ \\
  \var{phi21}     & $\phi_{21}$ \\
  \var{phi12}     & $\phi_{12}$ \\
  \var{phi22}     & $\phi_{22}$ \\
  \var{phi32}     & $\phi_{32}$ \\
  \var{psi11}     & $\psi_{11}k$ \\
  \var{psi21}     & $\psi_{21}k$ \\
  \var{psi12}     & $\psi_{12}k$ \\
  \var{psi22}     & $\psi_{22}k$ \\
  \var{phiK}      & $\phi^K$ \\
  \var{phiM}      & $\phi^M$ \\
  \var{phiMK}     & $\phi^{MK}$ \\
  \var{alp11cc}   & $\alpha_{11}\cos^2 kz$ \\
  \var{alp21sc}   & $\alpha_{21}\sin kz\cos kz$ \\
  \var{alp12cs}   & $\alpha_{12}\cos kz\sin kz$ \\
  \var{alp22ss}   & $\alpha_{22}\sin^2 kz$ \\
  \var{eta11cc}   & $\eta_{11}\cos^2 kz$ \\
  \var{eta21sc}   & $\eta_{21}\sin kz\cos kz$ \\
  \var{eta12cs}   & $\eta_{12}\cos kz\sin kz$ \\
  \var{eta22ss}   & $\eta_{22}\sin^2 kz$ \\
  \var{s2kzDFm}   & $\left<\sin2kz\nabla\cdot F\right>$ \\
  \var{M11}       & ${\cal M}_{11}$ \\
  \var{M22}       & ${\cal M}_{22}$ \\
  \var{M33}       & ${\cal M}_{33}$ \\
  \var{M11cc}     & ${\cal M}_{11}\cos^2 kz$ \\
  \var{M11ss}     & ${\cal M}_{11}\sin^2 kz$ \\
  \var{M22cc}     & ${\cal M}_{22}\cos^2 kz$ \\
  \var{M22ss}     & ${\cal M}_{22}\sin^2 kz$ \\
  \var{M12cs}     & ${\cal M}_{12}\cos kz\sin kz$ \\
  \var{bx11pt}    & $b_x^{11}$ \\
  \var{bx21pt}    & $b_x^{21}$ \\
  \var{bx12pt}    & $b_x^{12}$ \\
  \var{bx22pt}    & $b_x^{22}$ \\
  \var{bx0pt}     & $b_x^{0}$ \\
  \var{by11pt}    & $b_y^{11}$ \\
  \var{by21pt}    & $b_y^{21}$ \\
  \var{by12pt}    & $b_y^{12}$ \\
  \var{by22pt}    & $b_y^{22}$ \\
  \var{by0pt}     & $b_y^{0}$ \\
  \var{u11rms}    & $\left<u_{11}^2\right>^{1/2}$ \\
  \var{u21rms}    & $\left<u_{21}^2\right>^{1/2}$ \\
  \var{u12rms}    & $\left<u_{12}^2\right>^{1/2}$ \\
  \var{u22rms}    & $\left<u_{22}^2\right>^{1/2}$ \\
  \var{j11rms}    & $\left<j_{11}^2\right>^{1/2}$ \\
  \var{b11rms}    & $\left<b_{11}^2\right>^{1/2}$ \\
  \var{b21rms}    & $\left<b_{21}^2\right>^{1/2}$ \\
  \var{b12rms}    & $\left<b_{12}^2\right>^{1/2}$ \\
  \var{b22rms}    & $\left<b_{22}^2\right>^{1/2}$ \\
  \var{ux0m}      & $\left<u_{0_x}\right>$ \\
  \var{uy0m}      & $\left<u_{0_y}\right>$ \\
  \var{ux11m}     & $\left<u_{11_x}\right>$ \\
  \var{uy11m}     & $\left<u_{11_y}\right>$ \\
  \var{u0rms}     & $\left<u_{0}^2\right>^{1/2}$ \\
  \var{b0rms}     & $\left<b_{0}^2\right>^{1/2}$ \\
  \var{u0max}     & $\operatorname{max}\left|\boldsymbol{u}_{0}\right|$ \\
  \var{b0max}     & $\operatorname{max}\left|\boldsymbol{b}_{0}\right|$ \\
  \var{jb0m}      & $\left<j_0\cdot b_0\right>$ \\
  \var{ub0m}      & $\left<u_0\cdot b_0\right>$ \\
  \var{uj0m}      & $\left<u_0\cdot j_0\right>$ \\
  \var{E11rms}    & $\left<{\cal E}_{11}^2\right>^{1/2}$ \\
  \var{E21rms}    & $\left<{\cal E}_{21}^2\right>^{1/2}$ \\
  \var{E12rms}    & $\left<{\cal E}_{12}^2\right>^{1/2}$ \\
  \var{E22rms}    & $\left<{\cal E}_{22}^2\right>^{1/2}$ \\
  \var{E0rms}     & $\left<{\cal E}_{0}^2\right>^{1/2}$ \\
  \var{Ex11pt}    & ${\cal E}_x^{11}$ \\
  \var{Ex21pt}    & ${\cal E}_x^{21}$ \\
  \var{Ex12pt}    & ${\cal E}_x^{12}$ \\
  \var{Ex22pt}    & ${\cal E}_x^{22}$ \\
  \var{Ex0pt}     & ${\cal E}_x^{0}$ \\
  \var{Ey11pt}    & ${\cal E}_y^{11}$ \\
  \var{Ey21pt}    & ${\cal E}_y^{21}$ \\
  \var{Ey12pt}    & ${\cal E}_y^{12}$ \\
  \var{Ey22pt}    & ${\cal E}_y^{22}$ \\
  \var{Ey0pt}     & ${\cal E}_y^{0}$ \\
  \var{bamp}      & bamp \\
  \var{E111z}     & ${\cal E}_1^{11}$ \\
  \var{E211z}     & ${\cal E}_2^{11}$ \\
  \var{E311z}     & ${\cal E}_3^{11}$ \\
  \var{E121z}     & ${\cal E}_1^{21}$ \\
  \var{E221z}     & ${\cal E}_2^{21}$ \\
  \var{E321z}     & ${\cal E}_3^{21}$ \\
  \var{E112z}     & ${\cal E}_1^{12}$ \\
  \var{E212z}     & ${\cal E}_2^{12}$ \\
  \var{E312z}     & ${\cal E}_3^{12}$ \\
  \var{E122z}     & ${\cal E}_1^{22}$ \\
  \var{E222z}     & ${\cal E}_2^{22}$ \\
  \var{E322z}     & ${\cal E}_3^{22}$ \\
  \var{E10z}      & ${\cal E}_1^{0}$ \\
  \var{E20z}      & ${\cal E}_2^{0}$ \\
  \var{E30z}      & ${\cal E}_3^{0}$ \\
  \var{EBpq}      & ${\cal E}\cdot\Bv^{pq}$ \\
  \var{E0Um}      & ${\cal E}^0\cdot\Uv$ \\
  \var{E0Wm}      & ${\cal E}^0\cdot\Wv$ \\
  \var{bx0mz}     & $\left<b_{x}\right>_{xy}$ \\
  \var{by0mz}     & $\left<b_{y}\right>_{xy}$ \\
  \var{bz0mz}     & $\left<b_{z}\right>_{xy}$ \\
  \var{M11z}      & $\left<{\cal M}_{11}\right>_{xy}$ \\
  \var{M22z}      & $\left<{\cal M}_{22}\right>_{xy}$ \\
  \var{M33z}      & $\left<{\cal M}_{33}\right>_{xy}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_x.f90}} \\
\midrule
  \var{alp11}     & $\alpha_{11}$ \\
  \var{alp21}     & $\alpha_{21}$ \\
  \var{alp31}     & $\alpha_{31}$ \\
  \var{alp12}     & $\alpha_{12}$ \\
  \var{alp22}     & $\alpha_{22}$ \\
  \var{alp32}     & $\alpha_{32}$ \\
  \var{eta11}     & $\eta_{11}k$ \\
  \var{eta21}     & $\eta_{21}k$ \\
  \var{eta12}     & $\eta_{12}k$ \\
  \var{eta22}     & $\eta_{22}k$ \\
  \var{alp11cc}   & $\alpha_{11}\cos^2 kx$ \\
  \var{alp21sc}   & $\alpha_{21}\sin kx\cos kx$ \\
  \var{alp12cs}   & $\alpha_{12}\cos kx\sin kx$ \\
  \var{alp22ss}   & $\alpha_{22}\sin^2 kx$ \\
  \var{eta11cc}   & $\eta_{11}\cos^2 kx$ \\
  \var{eta21sc}   & $\eta_{21}\sin kx\cos kx$ \\
  \var{eta12cs}   & $\eta_{12}\cos kx\sin kx$ \\
  \var{eta22ss}   & $\eta_{22}\sin^2 kx$ \\
  \var{alp11_x}   & $\alpha_{11}x$ \\
  \var{alp21_x}   & $\alpha_{21}x$ \\
  \var{alp12_x}   & $\alpha_{12}x$ \\
  \var{alp22_x}   & $\alpha_{22}x$ \\
  \var{eta11_x}   & $\eta_{11}kx$ \\
  \var{eta21_x}   & $\eta_{21}kx$ \\
  \var{eta12_x}   & $\eta_{12}kx$ \\
  \var{eta22_x}   & $\eta_{22}kx$ \\
  \var{alp11_x2}  & $\alpha_{11}x^2$ \\
  \var{alp21_x2}  & $\alpha_{21}x^2$ \\
  \var{alp12_x2}  & $\alpha_{12}x^2$ \\
  \var{alp22_x2}  & $\alpha_{22}x^2$ \\
  \var{eta11_x2}  & $\eta_{11}kx^2$ \\
  \var{eta21_x2}  & $\eta_{21}kx^2$ \\
  \var{eta12_x2}  & $\eta_{12}kx^2$ \\
  \var{eta22_x2}  & $\eta_{22}kx^2$ \\
  \var{b11rms}    & $\left<b_{11}^2\right>^{1/2}$ \\
  \var{b21rms}    & $\left<b_{21}^2\right>^{1/2}$ \\
  \var{b12rms}    & $\left<b_{12}^2\right>^{1/2}$ \\
  \var{b22rms}    & $\left<b_{22}^2\right>^{1/2}$ \\
  \var{b0rms}     & $\left<b_{0}^2\right>^{1/2}$ \\
  \var{E11rms}    & $\left<{\cal E}_{11}^2\right>^{1/2}$ \\
  \var{E21rms}    & $\left<{\cal E}_{21}^2\right>^{1/2}$ \\
  \var{E12rms}    & $\left<{\cal E}_{12}^2\right>^{1/2}$ \\
  \var{E22rms}    & $\left<{\cal E}_{22}^2\right>^{1/2}$ \\
  \var{E0rms}     & $\left<{\cal E}_{0}^2\right>^{1/2}$ \\
  \var{E111z}     & ${\cal E}_1^{11}$ \\
  \var{E211z}     & ${\cal E}_2^{11}$ \\
  \var{E311z}     & ${\cal E}_3^{11}$ \\
  \var{E121z}     & ${\cal E}_1^{21}$ \\
  \var{E221z}     & ${\cal E}_2^{21}$ \\
  \var{E321z}     & ${\cal E}_3^{21}$ \\
  \var{E112z}     & ${\cal E}_1^{12}$ \\
  \var{E212z}     & ${\cal E}_2^{12}$ \\
  \var{E312z}     & ${\cal E}_3^{12}$ \\
  \var{E122z}     & ${\cal E}_1^{22}$ \\
  \var{E222z}     & ${\cal E}_2^{22}$ \\
  \var{E322z}     & ${\cal E}_3^{22}$ \\
  \var{E10z}      & ${\cal E}_1^{0}$ \\
  \var{E20z}      & ${\cal E}_2^{0}$ \\
  \var{E30z}      & ${\cal E}_3^{0}$ \\
  \var{EBpq}      & ${\cal E}\cdot\Bv^{pq}$ \\
  \var{bx0mz}     & $\left<b_{x}\right>_{xy}$ \\
  \var{by0mz}     & $\left<b_{y}\right>_{xy}$ \\
  \var{bz0mz}     & $\left<b_{z}\right>_{xy}$ \\
  \var{alp11x}    & $\alpha_{11}(x,t)$ \\
  \var{alp21x}    & $\alpha_{21}(x,t)$ \\
  \var{alp12x}    & $\alpha_{12}(x,t)$ \\
  \var{alp22x}    & $\alpha_{22}(x,t)$ \\
  \var{eta11x}    & $\eta_{11}(x,t)$ \\
  \var{eta21x}    & $\eta_{21}(x,t)$ \\
  \var{eta12x}    & $\eta_{12}(x,t)$ \\
  \var{eta22x}    & $\eta_{22}(x,t)$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_xz.f90}} \\
\midrule
  \var{E111z}     & ${\cal E}_1^{11}$ \\
  \var{E211z}     & ${\cal E}_2^{11}$ \\
  \var{E311z}     & ${\cal E}_3^{11}$ \\
  \var{E121z}     & ${\cal E}_1^{21}$ \\
  \var{E221z}     & ${\cal E}_2^{21}$ \\
  \var{E321z}     & ${\cal E}_3^{21}$ \\
  \var{alp11}     & $\alpha_{11}$ \\
  \var{alp21}     & $\alpha_{21}$ \\
  \var{eta11}     & $\eta_{113}k$ \\
  \var{eta21}     & $\eta_{213}k$ \\
  \var{b11rms}    & $\left<b_{11}^2\right>$ \\
  \var{b21rms}    & $\left<b_{21}^2\right>$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testfield_z.f90}} \\
\midrule
  \var{alp11}     & $\alpha_{11}$ \\
  \var{alp21}     & $\alpha_{21}$ \\
  \var{alp31}     & $\alpha_{31}$ \\
  \var{alp12}     & $\alpha_{12}$ \\
  \var{alp22}     & $\alpha_{22}$ \\
  \var{alp32}     & $\alpha_{32}$ \\
  \var{alp13}     & $\alpha_{13}$ \\
  \var{alp23}     & $\alpha_{23}$ \\
  \var{eta11}     & $\eta_{113}k$ or $\eta_{11}k$ if leta_rank2=T \\
  \var{eta21}     & $\eta_{213}k$ or $\eta_{21}k$ if leta_rank2=T \\
  \var{eta31}     & $\eta_{313}k$ \\
  \var{eta12}     & $\eta_{123}k$ or $\eta_{12}k$ if leta_rank2=T \\
  \var{eta22}     & $\eta_{223}k$ or $\eta_{22}k$ if leta_rank2=T \\
  \var{eta32}     & $\eta_{323}k$ \\
  \var{alp11cc}   & $\alpha_{11}\cos^2 kz$ \\
  \var{alp21sc}   & $\alpha_{21}\sin kz\cos kz$ \\
  \var{alp12cs}   & $\alpha_{12}\cos kz\sin kz$ \\
  \var{alp22ss}   & $\alpha_{22}\sin^2 kz$ \\
  \var{eta11cc}   & $\eta_{11}\cos^2 kz$ \\
  \var{eta21sc}   & $\eta_{21}\sin kz\cos kz$ \\
  \var{eta12cs}   & $\eta_{12}\cos kz\sin kz$ \\
  \var{eta22ss}   & $\eta_{22}\sin^2 kz$ \\
  \var{s2kzDFm}   & $\left<\sin2kz\nabla\cdot F\right>$ \\
  \var{M11}       & ${\cal M}_{11}$ \\
  \var{M22}       & ${\cal M}_{22}$ \\
  \var{M33}       & ${\cal M}_{33}$ \\
  \var{M11cc}     & ${\cal M}_{11}\cos^2 kz$ \\
  \var{M11ss}     & ${\cal M}_{11}\sin^2 kz$ \\
  \var{M22cc}     & ${\cal M}_{22}\cos^2 kz$ \\
  \var{M22ss}     & ${\cal M}_{22}\sin^2 kz$ \\
  \var{M12cs}     & ${\cal M}_{12}\cos kz\sin kz$ \\
  \var{bx11pt}    & $b_x^{11}$ \\
  \var{bx21pt}    & $b_x^{21}$ \\
  \var{bx12pt}    & $b_x^{12}$ \\
  \var{bx22pt}    & $b_x^{22}$ \\
  \var{bx0pt}     & $b_x^{0}$ \\
  \var{by11pt}    & $b_y^{11}$ \\
  \var{by21pt}    & $b_y^{21}$ \\
  \var{by12pt}    & $b_y^{12}$ \\
  \var{by22pt}    & $b_y^{22}$ \\
  \var{by0pt}     & $b_y^{0}$ \\
  \var{b11rms}    & $\left<b_{11}^2\right>^{1/2}$ \\
  \var{b21rms}    & $\left<b_{21}^2\right>^{1/2}$ \\
  \var{b12rms}    & $\left<b_{12}^2\right>^{1/2}$ \\
  \var{b22rms}    & $\left<b_{22}^2\right>^{1/2}$ \\
  \var{b0rms}     & $\left<b_{0}^2\right>^{1/2}$ \\
  \var{jb0m}      & $\left<jb_{0}\right>$ \\
  \var{E11rms}    & $\left<{\cal E}_{11}^2\right>^{1/2}$ \\
  \var{E21rms}    & $\left<{\cal E}_{21}^2\right>^{1/2}$ \\
  \var{E12rms}    & $\left<{\cal E}_{12}^2\right>^{1/2}$ \\
  \var{E22rms}    & $\left<{\cal E}_{22}^2\right>^{1/2}$ \\
  \var{E0rms}     & $\left<{\cal E}_{0}^2\right>^{1/2}$ \\
  \var{Ex11pt}    & ${\cal E}_x^{11}$ \\
  \var{Ex21pt}    & ${\cal E}_x^{21}$ \\
  \var{Ex12pt}    & ${\cal E}_x^{12}$ \\
  \var{Ex22pt}    & ${\cal E}_x^{22}$ \\
  \var{Ex0pt}     & ${\cal E}_x^{0}$ \\
  \var{Ey11pt}    & ${\cal E}_y^{11}$ \\
  \var{Ey21pt}    & ${\cal E}_y^{21}$ \\
  \var{Ey12pt}    & ${\cal E}_y^{12}$ \\
  \var{Ey22pt}    & ${\cal E}_y^{22}$ \\
  \var{Ey0pt}     & ${\cal E}_y^{0}$ \\
  \var{bamp}      & bamp \\
  \var{alp11z}    & $\alpha_{11}(z,t)$ \\
  \var{alp21z}    & $\alpha_{21}(z,t)$ \\
  \var{alp12z}    & $\alpha_{12}(z,t)$ \\
  \var{alp22z}    & $\alpha_{22}(z,t)$ \\
  \var{alp13z}    & $\alpha_{13}(z,t)$ \\
  \var{alp23z}    & $\alpha_{23}(z,t)$ \\
  \var{eta11z}    & $\eta_{11}(z,t)$ \\
  \var{eta21z}    & $\eta_{21}(z,t)$ \\
  \var{eta12z}    & $\eta_{12}(z,t)$ \\
  \var{eta22z}    & $\eta_{22}(z,t)$ \\
  \var{uzjx1z}    & $u_z j^{11}_x$ \\
  \var{uzjy1z}    & $u_z j^{11}_y$ \\
  \var{uzjz1z}    & $u_z j^{11}_z$ \\
  \var{uzjx2z}    & $u_z j^{21}_x$ \\
  \var{uzjy2z}    & $u_z j^{21}_y$ \\
  \var{uzjz2z}    & $u_z j^{21}_z$ \\
  \var{uzjx3z}    & $u_z j^{12}_x$ \\
  \var{uzjy3z}    & $u_z j^{12}_y$ \\
  \var{uzjz3z}    & $u_z j^{12}_z$ \\
  \var{uzjx4z}    & $u_z j^{22}_x$ \\
  \var{uzjy4z}    & $u_z j^{22}_y$ \\
  \var{uzjz4z}    & $u_z j^{22}_z$ \\
  \var{E111z}     & ${\cal E}_1^{11}$ \\
  \var{E211z}     & ${\cal E}_2^{11}$ \\
  \var{E311z}     & ${\cal E}_3^{11}$ \\
  \var{E121z}     & ${\cal E}_1^{21}$ \\
  \var{E221z}     & ${\cal E}_2^{21}$ \\
  \var{E321z}     & ${\cal E}_3^{21}$ \\
  \var{E112z}     & ${\cal E}_1^{12}$ \\
  \var{E212z}     & ${\cal E}_2^{12}$ \\
  \var{E312z}     & ${\cal E}_3^{12}$ \\
  \var{E122z}     & ${\cal E}_1^{22}$ \\
  \var{E222z}     & ${\cal E}_2^{22}$ \\
  \var{E322z}     & ${\cal E}_3^{22}$ \\
  \var{E10z}      & ${\cal E}_1^{0}$ \\
  \var{E20z}      & ${\cal E}_2^{0}$ \\
  \var{E30z}      & ${\cal E}_3^{0}$ \\
  \var{EBpq}      & ${\cal E}\cdot\Bv^{pq}$ \\
  \var{E0Um}      & ${\cal E}^0\cdot\Uv$ \\
  \var{E0Wm}      & ${\cal E}^0\cdot\Wv$ \\
  \var{bx0mz}     & $\left<b_{x}\right>_{xy}$ \\
  \var{by0mz}     & $\left<b_{y}\right>_{xy}$ \\
  \var{bz0mz}     & $\left<b_{z}\right>_{xy}$ \\
  \var{M11z}      & $\left<{\cal M}_{11}\right>_{xy}$ \\
  \var{M22z}      & $\left<{\cal M}_{22}\right>_{xy}$ \\
  \var{M33z}      & $\left<{\cal M}_{33}\right>_{xy}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testflow_z.f90}} \\
\midrule
  \var{gal}       & GAL-coefficients,     couple  $\overline F$ and $\overline U$ \\
  \var{aklam}     & AKA-$\lambda$-tensor, couples $\overline F$ and $\overline W = \nabla\times{\overline U}$ \\
  \var{gamma}     & $\gamma$-vector,      couples $\overline F$ and $\nabla\cdot{\overline U}$ \\
  \var{nu}        & $\nu$-tensor,         couples $\overline F$ and $\partial^2 {\overline U}/\partial z^2$ \\
  \var{zeta}      & $\zeta$-vector,       couples $\overline F$ and ${\overline G}_z = \nabla_z {\overline H}$ \\
  \var{xi}        & $\xi$-vector,         couples $\overline F$ and $\partial^2 {\overline H}/\partial z^2$ \\
  \var{aklamQ}    & $aklam^Q$-vector,     couples $\overline Q$ and $\overline W$ \\
  \var{gammaQ}    & $\gamma^Q$-scalar,    couples $\overline Q$ and $\nabla\cdot{\overline U}=dU_z/dz$ \\
  \var{nuQ}       & $\nu^Q$-vector,       couples $\overline Q$ and $\partial^2 \overline U/\partial z^2$ \\
  \var{zetaQ}     & $\zeta^Q$-scalar,      couples $\overline Q$ and ${\overline G}_z$ \\
  \var{xiQ}       & $\xi^Q$-scalar,        couples $\overline Q$ and $\partial^2 {\overline H}/\partial z^2$
                    
                    $\alpha_{K,ij}$
                    $\gamma_i$
                    $\nu_{ij}$
                    $\zeta_i$
                    $\xi_i$
                    $\nu^Q_i$
                    $aklam^Q_i$
                    ${\cal F}_i^{pq}$
                    ${\cal Q}^{pq}$
                    $\left<{u^{pq}}^2\right>$
                    $\left<{h^{pq}}^2\right>$ \\
  \var{ux0mz}     & $\left<u_{x}\right>_{xy}$ \\
  \var{uy0mz}     & $\left<u_{y}\right>_{xy}$ \\
  \var{uz0mz}     & $\left<u_{z}\right>_{xy}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testperturb.f90}} \\
\midrule
  \var{alp11}     & $\alpha_{11}$ \\
  \var{alp21}     & $\alpha_{21}$ \\
  \var{alp31}     & $\alpha_{31}$ \\
  \var{alp12}     & $\alpha_{12}$ \\
  \var{alp22}     & $\alpha_{22}$ \\
  \var{alp32}     & $\alpha_{32}$ \\
  \var{eta11}     & $\eta_{113}k$ \\
  \var{eta21}     & $\eta_{213}k$ \\
  \var{eta31}     & $\eta_{313}k$ \\
  \var{eta12}     & $\eta_{123}k$ \\
  \var{eta22}     & $\eta_{223}k$ \\
  \var{eta32}     & $\eta_{323}k$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testscalar.f90}} \\
\midrule
  \var{gam11}     & $\gamma_{1}^{(1)}$ \\
  \var{gam12}     & $\gamma_{2}^{(1)}$ \\
  \var{gam13}     & $\gamma_{3}^{(1)}$ \\
  \var{gam21}     & $\gamma_{1}^{(2)}$ \\
  \var{gam22}     & $\gamma_{2}^{(2)}$ \\
  \var{gam23}     & $\gamma_{3}^{(2)}$ \\
  \var{gam31}     & $\gamma_{1}^{(3)}$ \\
  \var{gam32}     & $\gamma_{2}^{(3)}$ \\
  \var{gam33}     & $\gamma_{3}^{(3)}$ \\
  \var{kap11}     & $\kappa_{11}$ \\
  \var{kap21}     & $\kappa_{21}$ \\
  \var{kap31}     & $\kappa_{31}$ \\
  \var{kap12}     & $\kappa_{12}$ \\
  \var{kap22}     & $\kappa_{22}$ \\
  \var{kap32}     & $\kappa_{32}$ \\
  \var{kap13}     & $\kappa_{13}$ \\
  \var{kap23}     & $\kappa_{23}$ \\
  \var{kap33}     & $\kappa_{33}$ \\
  \var{gam11z}    & $\gamma_{1}^{(1)}(z,t)$ \\
  \var{gam12z}    & $\gamma_{2}^{(1)}(z,t)$ \\
  \var{gam13z}    & $\gamma_{3}^{(1)}(z,t)$ \\
  \var{gam21z}    & $\gamma_{1}^{(2)}(z,t)$ \\
  \var{gam22z}    & $\gamma_{2}^{(2)}(z,t)$ \\
  \var{gam23z}    & $\gamma_{3}^{(2)}(z,t)$ \\
  \var{gam31z}    & $\gamma_{1}^{(3)}(z,t)$ \\
  \var{gam32z}    & $\gamma_{2}^{(3)}(z,t)$ \\
  \var{gam33z}    & $\gamma_{3}^{(3)}(z,t)$ \\
  \var{kap11z}    & $\kappa_{11}(z,t)$ \\
  \var{kap21z}    & $\kappa_{21}(z,t)$ \\
  \var{kap31z}    & $\kappa_{31}(z,t)$ \\
  \var{kap12z}    & $\kappa_{12}(z,t)$ \\
  \var{kap22z}    & $\kappa_{22}(z,t)$ \\
  \var{kap32z}    & $\kappa_{32}(z,t)$ \\
  \var{kap13z}    & $\kappa_{13}(z,t)$ \\
  \var{kap23z}    & $\kappa_{23}(z,t)$ \\
  \var{kap33z}    & $\kappa_{33}(z,t)$ \\
  \var{mgam33}    & $\tilde\gamma_{33}$ \\
  \var{mkap33}    & $\tilde\kappa_{33}$ \\
  \var{ngam33}    & $\hat\gamma_{33}$ \\
  \var{nkap33}    & $\hat\kappa_{33}$ \\
  \var{c1rms}     & $\left<c_{1}^2\right>^{1/2}$ \\
  \var{c2rms}     & $\left<c_{2}^2\right>^{1/2}$ \\
  \var{c3rms}     & $\left<c_{3}^2\right>^{1/2}$ \\
  \var{c4rms}     & $\left<c_{4}^2\right>^{1/2}$ \\
  \var{c5rms}     & $\left<c_{5}^2\right>^{1/2}$ \\
  \var{c6rms}     & $\left<c_{6}^2\right>^{1/2}$ \\
  \var{c1pt}      & $c^{1}$ \\
  \var{c2pt}      & $c^{2}$ \\
  \var{c3pt}      & $c^{3}$ \\
  \var{c4pt}      & $c^{4}$ \\
  \var{c5pt}      & $c^{5}$ \\
  \var{c6pt}      & $c^{6}$ \\
  \var{F11z}      & ${\cal F}_1^{1}$ \\
  \var{F21z}      & ${\cal F}_2^{1}$ \\
  \var{F31z}      & ${\cal F}_3^{1}$ \\
  \var{F12z}      & ${\cal F}_1^{2}$ \\
  \var{F22z}      & ${\cal F}_2^{2}$ \\
  \var{F32z}      & ${\cal F}_3^{2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testscalar_axisym.f90}} \\
\midrule
  \var{muc1}      & $\mu^{(c1)}$ \\
  \var{muc2}      & $\mu^{(c2)}$ \\
  \var{gamc}      & $\gamma^{(c)}$ \\
  \var{kapcPERP1} & $\kappa_\perp^{(1)}$ \\
  \var{kapcPERP2} & $\kappa_\perp^{(2)}$ \\
  \var{kapcPARA}  & $\kappa_\parallel$ \\
  \var{mucz}      & $\mu^{(c)}(z,t)$ \\
  \var{gamcz}     & $\gamma^{(c)}(z,t)$ \\
  \var{kapcPERPz} & $\kappa_\perp(z,t)$ \\
  \var{kapcPARAz} & $\kappa_\parallel(z,t)$ \\
  \var{gam11}     & $\gamma_{1}^{(1)}$ \\
  \var{gam12}     & $\gamma_{2}^{(1)}$ \\
  \var{gam13}     & $\gamma_{3}^{(1)}$ \\
  \var{gam21}     & $\gamma_{1}^{(2)}$ \\
  \var{gam22}     & $\gamma_{2}^{(2)}$ \\
  \var{gam23}     & $\gamma_{3}^{(2)}$ \\
  \var{gam31}     & $\gamma_{1}^{(3)}$ \\
  \var{gam32}     & $\gamma_{2}^{(3)}$ \\
  \var{gam33}     & $\gamma_{3}^{(3)}$ \\
  \var{kap11}     & $\kappa_{11}$ \\
  \var{kap21}     & $\kappa_{21}$ \\
  \var{kap31}     & $\kappa_{31}$ \\
  \var{kap12}     & $\kappa_{12}$ \\
  \var{kap22}     & $\kappa_{22}$ \\
  \var{kap32}     & $\kappa_{32}$ \\
  \var{kap13}     & $\kappa_{13}$ \\
  \var{kap23}     & $\kappa_{23}$ \\
  \var{kap33}     & $\kappa_{33}$ \\
  \var{gam11z}    & $\gamma_{1}^{(1)}(z,t)$ \\
  \var{gam12z}    & $\gamma_{2}^{(1)}(z,t)$ \\
  \var{gam13z}    & $\gamma_{3}^{(1)}(z,t)$ \\
  \var{gam21z}    & $\gamma_{1}^{(2)}(z,t)$ \\
  \var{gam22z}    & $\gamma_{2}^{(2)}(z,t)$ \\
  \var{gam23z}    & $\gamma_{3}^{(2)}(z,t)$ \\
  \var{gam31z}    & $\gamma_{1}^{(3)}(z,t)$ \\
  \var{gam32z}    & $\gamma_{2}^{(3)}(z,t)$ \\
  \var{gam33z}    & $\gamma_{3}^{(3)}(z,t)$ \\
  \var{gam3z}     & $\gamma^{(c)}(z,t)$ \\
  \var{kap11z}    & $\kappa_{11}(z,t)$ \\
  \var{kap21z}    & $\kappa_{21}(z,t)$ \\
  \var{kap31z}    & $\kappa_{31}(z,t)$ \\
  \var{kap12z}    & $\kappa_{12}(z,t)$ \\
  \var{kap22z}    & $\kappa_{22}(z,t)$ \\
  \var{kap32z}    & $\kappa_{32}(z,t)$ \\
  \var{kap13z}    & $\kappa_{13}(z,t)$ \\
  \var{kap23z}    & $\kappa_{23}(z,t)$ \\
  \var{kap33z}    & $\kappa_{33}(z,t)$ \\
  \var{mgam33}    & $\tilde\gamma_{33}$ \\
  \var{mkap33}    & $\tilde\kappa_{33}$ \\
  \var{ngam33}    & $\hat\gamma_{33}$ \\
  \var{nkap33}    & $\hat\kappa_{33}$ \\
  \var{c1rms}     & $\left<c_{1}^2\right>^{1/2}$ \\
  \var{c2rms}     & $\left<c_{2}^2\right>^{1/2}$ \\
  \var{c3rms}     & $\left<c_{3}^2\right>^{1/2}$ \\
  \var{c4rms}     & $\left<c_{4}^2\right>^{1/2}$ \\
  \var{c5rms}     & $\left<c_{5}^2\right>^{1/2}$ \\
  \var{c6rms}     & $\left<c_{6}^2\right>^{1/2}$ \\
  \var{c1pt}      & $c^{1}$ \\
  \var{c2pt}      & $c^{2}$ \\
  \var{c3pt}      & $c^{3}$ \\
  \var{c4pt}      & $c^{4}$ \\
  \var{c5pt}      & $c^{5}$ \\
  \var{c6pt}      & $c^{6}$ \\
  \var{F11z}      & ${\cal F}_1^{1}$ \\
  \var{F21z}      & ${\cal F}_2^{1}$ \\
  \var{F31z}      & ${\cal F}_3^{1}$ \\
  \var{F12z}      & ${\cal F}_1^{2}$ \\
  \var{F22z}      & ${\cal F}_2^{2}$ \\
  \var{F32z}      & ${\cal F}_3^{2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{testscalar_simple.f90}} \\
\midrule
  \var{gam11}     & $\gamma_{1}^{(1)}$ \\
  \var{gam12}     & $\gamma_{2}^{(1)}$ \\
  \var{gam13}     & $\gamma_{3}^{(1)}$ \\
  \var{gam21}     & $\gamma_{1}^{(2)}$ \\
  \var{gam22}     & $\gamma_{2}^{(2)}$ \\
  \var{gam23}     & $\gamma_{3}^{(2)}$ \\
  \var{gam31}     & $\gamma_{1}^{(3)}$ \\
  \var{gam32}     & $\gamma_{2}^{(3)}$ \\
  \var{gam33}     & $\gamma_{3}^{(3)}$ \\
  \var{kap11}     & $\kappa_{11}$ \\
  \var{kap21}     & $\kappa_{21}$ \\
  \var{kap31}     & $\kappa_{31}$ \\
  \var{kap12}     & $\kappa_{12}$ \\
  \var{kap22}     & $\kappa_{22}$ \\
  \var{kap32}     & $\kappa_{32}$ \\
  \var{kap13}     & $\kappa_{13}$ \\
  \var{kap23}     & $\kappa_{23}$ \\
  \var{kap33}     & $\kappa_{33}$ \\
  \var{gam11z}    & $\gamma_{1}^{(1)}(z,t)$ \\
  \var{gam12z}    & $\gamma_{2}^{(1)}(z,t)$ \\
  \var{gam13z}    & $\gamma_{3}^{(1)}(z,t)$ \\
  \var{gam21z}    & $\gamma_{1}^{(2)}(z,t)$ \\
  \var{gam22z}    & $\gamma_{2}^{(2)}(z,t)$ \\
  \var{gam23z}    & $\gamma_{3}^{(2)}(z,t)$ \\
  \var{gam31z}    & $\gamma_{1}^{(3)}(z,t)$ \\
  \var{gam32z}    & $\gamma_{2}^{(3)}(z,t)$ \\
  \var{gam33z}    & $\gamma_{3}^{(3)}(z,t)$ \\
  \var{kap11z}    & $\kappa_{11}(z,t)$ \\
  \var{kap21z}    & $\kappa_{21}(z,t)$ \\
  \var{kap31z}    & $\kappa_{31}(z,t)$ \\
  \var{kap12z}    & $\kappa_{12}(z,t)$ \\
  \var{kap22z}    & $\kappa_{22}(z,t)$ \\
  \var{kap32z}    & $\kappa_{32}(z,t)$ \\
  \var{kap13z}    & $\kappa_{13}(z,t)$ \\
  \var{kap23z}    & $\kappa_{23}(z,t)$ \\
  \var{kap33z}    & $\kappa_{33}(z,t)$ \\
  \var{mgam33}    & $\tilde\gamma_{33}$ \\
  \var{mkap33}    & $\tilde\kappa_{33}$ \\
  \var{ngam33}    & $\hat\gamma_{33}$ \\
  \var{nkap33}    & $\hat\kappa_{33}$ \\
  \var{c1rms}     & $\left<c_{1}^2\right>^{1/2}$ \\
  \var{c2rms}     & $\left<c_{2}^2\right>^{1/2}$ \\
  \var{c3rms}     & $\left<c_{3}^2\right>^{1/2}$ \\
  \var{c4rms}     & $\left<c_{4}^2\right>^{1/2}$ \\
  \var{c5rms}     & $\left<c_{5}^2\right>^{1/2}$ \\
  \var{c6rms}     & $\left<c_{6}^2\right>^{1/2}$ \\
  \var{c1pt}      & $c^{1}$ \\
  \var{c2pt}      & $c^{2}$ \\
  \var{c3pt}      & $c^{3}$ \\
  \var{c4pt}      & $c^{4}$ \\
  \var{c5pt}      & $c^{5}$ \\
  \var{c6pt}      & $c^{6}$ \\
  \var{F11z}      & ${\cal F}_1^{1}$ \\
  \var{F21z}      & ${\cal F}_2^{1}$ \\
  \var{F31z}      & ${\cal F}_3^{1}$ \\
  \var{F12z}      & ${\cal F}_1^{2}$ \\
  \var{F22z}      & ${\cal F}_2^{2}$ \\
  \var{F32z}      & ${\cal F}_3^{2}$ \\
\midrule
  \multicolumn{2}{c}{Module \file{thermal_energy.f90}} \\
\midrule
  \var{TTmax}     & $\max (T)$ \\
  \var{TTmin}     & $\min (T)$ \\
  \var{ppm}       & $\left< p \right>$ \\
  \var{TTm}       & $\left<T\right>$ \\
  \var{ethm}      & $\left< e_{\text{th}}\right> =
                    \left< c_v \rho T \right> $
                    \quad(mean thermal energy) \\
  \var{ethtot}    & $\int_V e_{\text{th}}\,dV$
                    \quad(total thermal energy) \\
  \var{ethmin}    & $\mathrm{min} e_\text{th}$ \\
  \var{ethmax}    & $\mathrm{max} e_\text{th}$ \\
  \var{eem}       & $\left< e \right> =
                    \left< c_v T \right>$
                    \quad(mean internal energy) \\
  \var{etot}      & $\langle e_\textrm{th} + \rho u^2 / 2\rangle$ \\
\midrule
  \multicolumn{2}{c}{Module \file{visc_smagorinsky.f90}} \\
\midrule
  \var{nu_LES}    & Mean value of Smagorinsky viscosity \\
\midrule
  \multicolumn{2}{c}{Module \file{viscosity.f90}} \\
\midrule
  \var{nu_tdep}   & time-dependent viscosity \\
  \var{fviscm}    & Mean value of viscous acceleration \\
  \var{fviscmin}  & Min value of viscous acceleration \\
  \var{fviscmax}  & Max value of viscous acceleration \\
  \var{fviscrmsx} & Rms value of viscous acceleration
                    for the vis_xaver_range \\
  \var{num}       & Mean value of viscosity \\
  \var{nusmagm}   & Mean value of Smagorinsky viscosity \\
  \var{nusmagmin} & Min value of Smagorinsky viscosity \\
  \var{nusmagmax} & Max value of Smagorinsky viscosity \\
  \var{nu_LES}    & Mean value of Smagorinsky viscosity \\
  \var{visc_heatm} & Mean value of viscous heating \\
  \var{qfviscm}   & $\left<\qv\cdot
                    \fv_{\rm visc}\right>$ \\
  \var{ufviscm}   & $\left<\uv\cdot
                    \fv_{\rm visc}\right>$ \\
  \var{Sij2m}     & $\left<\Strain^2\right>$ \\
  \var{epsK}      & $\left<2\nu\varrho\Strain^2\right>$ \\
  \var{epsKint}   & $\int(2\nu\varrho\Strain^2)\,dV$ \\
  \var{sijoiojm}  & $\left<S_{i,j} \omega_i \omega_j\right>$ \\
  \var{dtnu}      & $\delta t/[c_{\delta t,{\rm v}}\,
                    \delta x^2/\nu_{\rm max}]$
                    \quad(time step relative to
                    viscous time step;
                    see \S~\ref{time-step}) \\
  \var{meshRemax} & Max mesh Reynolds number \\
  \var{mesh3Remax} & Max hyper3 mesh Reynolds number \\
  \var{Reshock}   & Mesh Reynolds number at shock \\
%
\bottomrule
\end{longtable}

