|
par1 | low temperature (keV) |
par2 | high temperature (keV) |
par3 | abundance relative to Solar |
par4 | redshift |
par5 | switch (0 = calculate using mekal, 1 = interpolate using mekal, 2 = use AtomDB data), 3 = SPEX data |
norm | Mass accretion rate (solar mass/yr) |
For the vcoolflow variant the parameters are:
par1 | low temperature (keV) |
par2 | high temperature (keV) |
par3–par16 | Abundances for He, C, N, O, Ne, Na, Mg, Al, Si, S, Ar, Ca, Fe, Ni wrt Solar |
par17 | Redshift |
par18 | switch (0 = calculate using mekal, 1 = interpolate using mekal, 2 = use AtomDB data, 3 = SPEX data) |
norm | Mass accretion rate (solar mass/yr) |
For the bcoolflow model the parameters are:
par1 | low temperature (keV) |
par2 | high temperature (keV) |
par3 | abundance relative to Solar |
par4 | redshift |
par5 | gaussian sigma for velocity broadening (km/s) (switch=2 or 3 only) |
par6 | switch (0 = calculate using mekal, 1 = interpolate using mekal, 2 = use AtomDB data, 3 = SPEX data) |
norm | Mass accretion rate (solar mass/yr) |
For the bvcoolflow variant the parameters are:
par1 | low temperature (keV) |
par2 | high temperature (keV) |
par3–par16 | Abundances for He, C, N, O, Ne, Na, Mg, Al, Si, S, Ar, Ca, Fe, Ni wrt Solar |
par17 | Redshift |
par18 | gaussian sigma for velocity broadening (km/s) (switch=2 or 3 only) |
par19 | switch (0 = calculate using mekal, 1 = interpolate using mekal, 2 = use AtomDB data, 3 = SPEX data) |
norm | Mass accretion rate (solar mass/yr) |
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Last modified: Friday, 23-Aug-2024 13:20:40 EDT
HEASARC Staff Scientist Position - Applications are now being accepted for a Staff Scientist with significant experience and interest in the technical aspects of astrophysics research, to work in the High Energy Astrophysics Science Archive Research Center (HEASARC) at NASA Goddard Space Flight Center (GSFC) in Greenbelt, MD. Refer to the AAS Job register for full details.