Physics Options#

YREC is generally called by two namelists: the “control” namelist, or nml1; and the “physics” namelist, or nml2. This page is a reference that will document various current and deprecated possible commands in the namelist files.

Physics (.nml2)#

Constants#

YREC does computations in CGS but outputs in solar units.

Parameter

Description

CLSUN

Definition of \(L_\odot\) used for tracks and output

CRSUN

Definition of \(R_\odot\) used for tracks and output

Core fitting options#

Parameter

Description

LCORE

If .TRUE., move the central fitting point inward using a Taylor expansion approximation.

FCORE

Factor in mass by which the central fitting point is moved inward.

Gravitational settling & microscopic diffusion#

Parameter

Description

LDIFY

Enable gravitational settling of helium.

LDIFZ

Enable gravitational settling of metals.

LDIFLI

Enable gravitational settling of light species.

FGRY

Scaling factor for helium-settling diffusion coefficients (e.g., 0.75 if no rotational mixing).

FGRZ

Scaling factor for metal-settling diffusion coefficients.

DT_GS

Settling solved in multiple timesteps if global timestep < DT_GS * τ(CZ base).

XMIN

Disable diffusion once central hydrogen X < XMIN.

YMIN

Disable diffusion once surface helium Y < YMIN.

GRTOL

Numerical tolerance for diffusion abundance changes.

NITER_GS

Maximum iterations for diffusion abundance solver.

ILAMBDA

Formula for Coulomb logarithm, used in collision integrals; 4 (recommended) is a constant, 2.2.

Numerical convergence options#

Parameter

Description

LNEWS

Extrapolate changes from prior step for next step in initial entropy change estimate; can improve convergence.

NITER1

Iterations before SBC (surface boundary condition) is checked.

NITER2

Iterations after SBC check, assumes start of T nuclear burning rates.

NITER3

Iterate between model solution and nuclear burning rates (set to 0 if you encounter convergence difficulties).

NITER4

Iterate betweeen model solution, rotation, and rotationally induced mixing. Set to 0 for models without rotation.

ITDIF1

Iterations between structure equations and rotational mixing (1=none). This is the same as NITER3 unless >1. Recommend 2 for rotational mixing models.

FCORR0

The code predicts corrections to the structure variables, which can initially be overestimated. This is the iteration 1 scale factor by which they are multipled.

FCORRI

This is the increment to the factor for each successive interation, for example it reaches the max of 1 in 8 steps if (0.6,0.05). larger factor = faster convergence, less stable.

HTOLER(1,1)

Convergence tol for log P. If the maximum correction in a given stage anywhere is below this threshold (for all 4 state variables), the run is converged.

HTOLER(2,1)

Convergence tol for log T.

HTOLER(3,1)

Convergence tol for log R.

HTOLER(4,1)

Convergence tol for L/Ltot. Note: all are local

HTOLER(5,1)

If the difference between analytic and numerical derivatives is better than this, iteration is skipped. (5,1) is for P+R

HTOLER(5,2)

If the difference between analytic and numerical derivatives is better than this, iteration is skipped. (5,2) is for T+L

Convective mixing & overshoot#

Parameter

Description

LSEMIC

Enable semi-convection.

LOVSTC

Enable core overshoot mixing. Note: unless LOVAD=.TRUE., this is overmixing only, and does not impact the thermal structure

ALPHAC

Core overshoot in pressure scale heights.

LOVMAX

Alternative test (only checked if LOVSTC = .TRUE.) to avoid pathologies in overshoot of small cores.

BETAC

Alternative test - maximum overshoot in fraction of physical size of core

LOVSTE

Enable envelope overshoot.

ALPHAE

Envelope overshoot in pressure scale heights.

LOVSTM

Enable overshoot in intermediate convection zones (recommend not on, needs to be checked).

ALPHAM

Intermediate overshoot (above and below) in pressure scale heights.

TGCUT

Adiabatic convection assumed above this log T.

Equation of state (EOS)#

Parameter

Description

LSCV

Use SCV EOS in domain where it is valid and OPAL is not.

LOPALE06

Use OPAL EOS. Note - a simplified Boltzmann/Saha solver, fully ionized at high T, is used when this is disabled, or outside the table.

LNumDeriv

Use numerical derivatives instead of analytic ones (very slow).

LDH

Use Debye–Hückel correction for the Yale EOS.

ETADH0

Lower Debye–Hückel parameter limit.

ETADH1

Upper Debye–Hückel parameter limit.

TSCUT

Threshold above which the default EOS assumes full ionization.

Opacity options#

Parameter

Description

LCondOpacP

Use updated conductive opacity tables.

OPTOL

The code generates a 2D surface abundance opacity table, useful for outer CZs and envelope integration. It switches to a 3D/4D solution when x, z differ from it by more than this.

TMOLMIN

Below this log T, use only molecular opacity (if available).

TMOLMAX

Above this log T, use only atomic opacity. Ramp used between TMOLMIN and TMOLMAX.

Nuclear reaction & burning options#

Numerics

The numerics of abundance change solutions and thresholds for computing reaction rates. Only TCUT1 is adjusted from default. Do not change without good reason.

Parameter

Description

WEAKSCREENING

Threshold for using weak-screening in reaction rates.

LSNU

Compute solar neutrino fluxes.

TCUT(1)

Temperature threshold for computing \(\epsilon _{\mathrm{nuc}}\). Others are thresholds for progressively more advanced burning stages (Default 6.5, bad for D burning in preMS)

CMIN

Minimum abundance tracked in solver.

ABSTOL

Absolute convergence criterion for abundance changes.

RELTOL

Relative convergence criterion for abundance changes.

KEMMAX

Maximum substeps for abundance integration.

Light-element burning cross-sections#

Parameter

Description

LXLI6

Use manually specified p+⁶Li cross-section.

LXLI7

Use manually specified p+⁷Li cross-section.

XSLI6

Value of p+⁶Li cross-section (keV barns).

XSLI7

Value of p+⁷Li cross-section (keV barns).

LXBE91

Toggle p+⁹Be → γ channel.

LXBE92

Toggle p+⁶Li → d channel.

LXBE93

Toggle p+⁶Li → α channel.

XSBE91

Cross-section for p(⁹Be,γ).

XSBE92

Cross-section for p(⁹Be,d).

XSBE93

Cross-section for p(⁹Be,α).

Surface boundary conditions#

Parameter

Description

KTTAU

SBC model selector (0=Eddington, 1=Krishnaswamy, 3=Kurucz, 4=Allard).

TRIDT

The code solves for a SBC between 3 models. This is the spacing between 2 of them in Log Teff. The third is a different L at the average Teff.

TRIDL

Spacing between the lower pair and upper point in Log L.

Atmospheric integration#

Parameter

Description

ATMERR

Numerical tolerance for atmosphere integration.

ATMMAX

Maximum step size in log τ for atmosphere integrator.

ATMMIN

Minimum step size in log τ for atmosphere integrator.

ATMBEG

Initial step size in log τ for atmosphere integrator.

ATMD0

log10 of starting density at τ = 0 in the atmosphere integrator (may need adjusting for massive stars).

Envelope integrator#

Parameter

Description

ENVERR

Numerical tolerance for envelope integration.

ENVMAX

Maximum step size in log P for envelope integrator.

ENVMIN

Minimum step size in log P for envelope integrator.

ENVBEG

Initial step size in log P for envelope integrator.

STOLR0

Required fractional agreement between envelope mass and mass at fitting point.

IMAX

Integrators start with a large step, divide to smaller, and extrapolate to zero. Maximum number of loops to infer integration step size (envelope + atmosphere).

NUSE

Number of prior steps used for extrapolation to zero step size (atm+env).

Spatial tolerances#

Parameter

Description

TOL_DM_MIN

Minimum mass spacing (most important for thin outer fitting points).

TOL_DM_MAX

Maximum log mass spacing (most important for stellar cores).

TOL_DL_MAX

Maximum spacing in L/Lsurf (most important for energy generating regions).

TOL_DP_ENV_MAX

Maximum log P spacing in outer CZ (most important for outer layers).

TOL_DP_CZBASE_MAX

Maximum log P spacing at SCZ base.

TOL_DP_CORE_MAX

Maximum log P spacing below SCZ (important between burning, SCZ base).

FLAG_DX

Minimum threshold for preserving discontinuities in X.

FLAG_DZ

Minimum threshold for preserving discontinuities in Z.

TOL_CZBASE_FINE_WIDTH

Width of fine-zoned region at CZ base (0.4 for red giant models).

FLAG_DW

Minimum threshold for preserving Ω discontinuities.

Timestep criteria#

Parameter

Description

LTRIST

Restrict timestep during Hertzsprung gap.

TIME_CORE_MIN

Minimum X,Y for using core vs shell burning criteria.

TIME_DX_CORE_TOT

Max absolute ΔX in core H-burning.

TIME_DX_CORE_FRAC

Max fractional ΔX in core H-burning.

TIME_DY_CORE_TOT

Max absolute ΔY/Z in core He-burning (red clump/HB).

TIME_DY_CORE_FRAC

Max fractional ΔY/Z in core He-burning (red clump/HB).

TIME_DX_TOTAL

Max absolute H burned per timestep (post-MS).

TIME_DX_SHELL

Max fractional ΔX in shell H-burning (post-MS).

TIME_DY_TOTAL

Max absolute He burned (AGB).

TIME_DY_SHELL

Max fractional ΔY in He shell.

LSTRUCT_TIME

Restrict timestep based on structural changes - disabled once Lgrav<0 (minimum radius, close to ZAMS).

TIME_DT

Max local ΔT (pre-MS).

TIME_DP

Max local ΔP (pre-MS).

TIME_DR

Max local ΔR (pre-MS).

TIME_DL

Max local ΔL (pre-MS).

TIME_MAX_DT_FRAC

Max fractional timestep change step-to-step.

TIME_DW_MIX

Max ΔΩ per mixing substep (can be more than one per full model step).

TIME_DW_GLOBAL

Max ΔΩ per model.

Rotation#

Parameter

Description

LROT

Enable rotation.

LNEW0

Force new SBC each model when rotation enabled. Required for models with rotation, as rotation is held fixed in the solution. LROT = .TRUE. sets this .TRUE.

Rotation & mixing timesteps#

Parameter

Description

TIME_DW_GLOBAL

Maximum ΔΩ per model step (replaces DTWIND).

TIME_DW_MIX

Maximum ΔΩ per mixing step (replaces DTDIF).

ITDIF2

Iterations between nuclear burning and rotational mixing (1=none).

DJOK

Numerical tolerance for rotational mixing.

Structural effects of rotation#

Parameter

Description

ACFPFT

Fractional accuracy for departures from spherical symmetry (cubed).

ITFP1

Iterations between equipotential shape and effective radius solutions (structural effects of rotation).

ITFP2

Iterations for measuring effective radius given shape parameter (structural effects of rotation).

Initializing rotation#

Parameter

Description

LWNEW

Convert non-rotating model to rotating.

WNEW

Uniform angular velocity if LWNEW = TRUE. If star-disk coupling is being used, should be set to the same value as the disk period. Check your units!

LDISK

Enforce disk locking.

TDISK

Disk lifetime in Gyr. 1e5yr = 1e-4 Gyr is the D burning BL. 1e-4 to 1e-2 is the recommended range

PDISK

Disk rotation period (rad/s). 8 days (9.0902e-6) is the observed median period in solar-mass disked stars in star forming regions.

Angular momentum loss & winds#

Parameter

Description

LJDOT0

Enable angular momentum loss.

LMWIND

Use Matt et al. 2012 wind model.

AWIND

Wind law selector (V13 (van Saders & Pinsonneault 2013 model), K97 (legacy Krishnamurthi et al. 1997), CUS is custom. PMMA, PMMB, PMMC, PMMD, PMMM are only used if this is set to CUS.).

FK

Scale factor for angular momentum loss. Typically used as a free parameter to reproduce the solar rotation at the solar age.

LROSSBY

Scale the loss rate relative to the Rossby number. Should be used with a saturation threshold (WMAX or WMAXSUN below).

WMAX

Maximum angular velocity (rad/s) for scaling the mass loss rate and magnetic fields in the scaled solar wind. This is over-written if WMAX_SUN is below 1000; the latter expresses WMAX relative to the solar angular velocity.

WMAX_SUN

WMAX expressed in solar Ω units.

PMMSOLP

log P at Teff in solar model (for B-field calibration).

PMMSOLTAU

Solar convective overturn timescale.

Angular momentum transport#

Parameter

Description

LINSTB

Include rotationally induced mixing and hydrodynamic AM transport.

LSOLID

Enforce solid-body rotation everywhere. Set true for strongly coupled magnetic models.

WALPCZ

Angular velocity in CZ scales as R^WALPCZ. 0 = solid body -2 = uniform specific angular momentum

IMPJMOD

Global angular momentum coupling settings. 0 = no effect 1 = solid body everywhere 2 = solid body core, decoupled cz 3 = solid body core, coupled at base of CZ rate.

LCODM

Include magnetic diffusion term.

CODM

Magnetic diffusion term for angular momentum transport. 0 = Pure hydro. Nonzero=extra diffusive mechanism. 9e4 matches the solar core rotation constraints.

FW

Global factor for scaling the angular momentum transport diffusion coefficients.

FC

Scale factor for mixing diffusion coefficeints relative to angular momentum. Typicaly calibrated to match Li depletion in a benchmark (cluster stars or the Sun).

IGSF

Toggle for the stability condition used to evaluate the GSF and ABCD instabilties. 1 is recommended.

Starspots#

Parameter

Description

LSDEPTH

Control that descreases spot contrast with depth, assuming a constant B. This does not have a dramatic effect on the results.

SPOTF

Starspot filling factor. 0.25 is the active star bound in main sequence stars.

SPOTX

Starspot temperature contrast; only alter if SPOTF > 0. 0.85 is a typical sunspot value.

Rarely used options#

Parameter

Description

LTHOUL

Use Thoul formalism for settling.

LTHOULFIT

Use published fit instead of full solution (not recommended).

HTOLER(1,2)

Abort threshold for log P divergence greater than this.

HTOLER(2,2)

Abort threshold for log T divergence greater than this.

HTOLER(3,2)

Abort threshold for log R divergence greater than this.

HTOLER(4,2)

Abort threshold for L/Ltot divergence greater than this.

TENV0

Minimum T for envelope integration. Code stops below this.

TENV1

Maximum T for envelope integration. Code stops above this.

ATMSTP

Max step for atmosphere integrator (LENVG).

ENVSTP

Max step for envelope integrator (LENVG).

Legacy options#

Parameter

Description

LEXCOM

Extend tracked isotopes to include D, Li6/7, Be9.

LNEWDIF

Enable updated settling routines.

LNEWNUC

Use new nuclear cross-section format.

LNULOS1

Use Itoh et al. (1996) neutrino loss rates.

LNEWVARS

Use updated variable names for tolerances.

TOL_DX_MAX

Legacy mesh spacing in X.

TOL_DZ_MAX

Legacy mesh spacing in Z.

Experimental options#

Parameter

Description

DPENV

Full mixing from center to fractional mass depth.

LADOV

Experimental adiabatic overshoot.

LVFC

Zahn 1991 variable-FC model.

LDIFAD

Treat meridional circulation as diffusion + advection.

LMDOT

Enable experimental mass-loss module.

LSOLWIND

Remove mass loss scaled to solar wind (not implemented).

Unused parameters#

Parameter

Description

TCUT(2)

Not used. Former pp-chain equilibrium threshold.

TCUT(3)

Not used. Former CNO-cycle equilibrium threshold.

MCORE

Not used. Obsolete core mesh allocation parameter.

LENVG

Not used. Outer-layer structure calculation after convergence.

ALFA

Not used. Legacy exponent for Kawaler (1988) wind law.