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Eqpair, eqtherm, compth: Paolo Coppi's hybrid (thermal/non-thermal) hot plasma emission models.

These models are based on Paolo Coppi's hybrid thermal/non-thermal hot plasma emission model for X-ray binaries. The underlying physics and a detailed description of the code are included in the draft paper

Do not use these models without reading and understanding this paper. Simplified models eqtherm and compth are provided for cases where non-thermal processes are not important and photon-photon pair production can be ignored. These should only be used if $l_{bb} <~ 10$.

The temperature of the thermal component of the electron distribution and the total electron optical depth (for both ionization electrons and electron-positron pairs) are written out if the chatter level is set to 15. This information is important for checking self-consistency.

In versions 1.10 and above the Compton reflection is done by a call to the ireflect model code and the relativistic blurring by a call to rdblur. This does introduce some changes in the spectrum from earlier versions. For the case of a neutral reflector (i.e. the ionization parameter is zero) more accurate opacities are calculated. For the case of an ionized reflector the old version assumed that for the purposes of calculating opacities the input spectrum was a power-law (with index based on the 2-10 keV spectrum). The new version uses the actual input spectrum, which is usually not a power law, giving different opacities for a given ionization parameter and disk temperature. The Greens' function integration required for the Compton reflection calculation is performed to an accuracy of 0.01 (i.e. 1%). This can be changed using e.g. xset EQPAIR_PRECISION 0.05.

The parameters for all three models are:
par1 lh/ls, ratio of the hard to soft compactnesses
par2 lbb, the soft photon compactness
par3 kTbb, if >0 then temperature of a blackbody; if <0 then abs(kTbb) is the Tmax parameter for the diskpn model
par4 lnt/lh, fraction of power supplied to energetic particles which goes into accelerating non-thermal particles
par5 tp, the Thomson scattering depth
par6 radius, the size of the scattering region (cm)
par7 gmin, minimum Lorentz factor of the pairs
par8 gmax, maximum Lorentz factor of the pairs
par9 Ginj, if <0 then non-thermal spectrum is assumed mono-energetic at gmax; if >0 then a power-law from gmin to gmax
par10 pairinj, if = 0 then accelerated particles are electrons from thermal pool; if = 1 then accelerated particles are electrons and positrons
par11 cosIncl, inclination of reflecting material wrt line-of-sight
par12 Refl, fraction of scattering region's emission intercepted by reflecting material
par13 Fe_abund, relative abundance of iron
par14 Ab$>$He, relative abundance of other metals
par15 Tdisk, temperature of reflecting disk
par16 x, ionization parameter of reflector
par17 b, power-law index with radius of disk reflection emissivity
par18 Rin, inner radius of reflecting material (GM/c$^2$)
par19 Rout, outer radius of reflecting material (GM/c$^2$)
par20 Redshift, z

next up previous contents
Next: equil, vequil: collisional plasma, Up: Additive Model Components Previous: eplogpar: log-parabolic blazar model