J/ApJ/717/257     Synthetic spectra of dark stars   (Zackrisson+, 2010)
================================================================================
Finding High-redshift Dark Stars with the James Webb Space Telescope
     Zackrisson E., Scott P., Rydberg C.-E., Iocco F., Edvardsson B.,
     Ostlin G., Sivertsson S., Zitrin A., Broadhurst T., Gondolo P.
    <Astrophys. J. 717, 257 (2010)>
    =2010ApJ...717..257Z
================================================================================
ADC_Keywords:  Models, atmosphere ; Photometry, infrared
Keywords: dark ages ; reionization ; first stars ; dark matter ;
          galaxies: high-redshift ; stars: Population III

Abstract:
    The first stars in the history of the Universe are likely to form in
    the dense central regions of {sim.to}10^5^-10^6^ M_{sun}_ cold dark
    matter halos at z{approx}10--50. The annihilation of dark matter
    particles in these environments may lead to the formation of so-called
    dark stars, which are predicted to be cooler, larger, more massive and
    potentially more long-lived than conventional population III stars.
    Here, we investigate the prospects of detecting high-redshift dark
    stars with the upcoming James Webb Space Telescope (JWST). We find
    that all dark stars with masses up to 10^3^ M_{sun}_ are intrinsically
    too faint to be detected by JWST at z above 6. However, by exploiting
    foreground galaxy clusters as gravitational telescopes, certain
    varieties of cool (T_eff_<=30000K) dark stars should be within reach
    at redshifts up to z{approx}10. If the lifetimes of dark stars are
    sufficiently long, many such objects may also congregate inside the
    first galaxies. We demonstrate that this could give rise to peculiar
    features in the integrated spectra of galaxies at high redshifts,
    provided that dark stars make up at least {sim.to}1% of the total
    stellar mass in such objects.

Description:
    Model spectra and JWST broadband magnitudes for the 18 dark star
    models discussed in the paper.

File Summary:
--------------------------------------------------------------------------------
 FileName  Lrecl    Records    Explanations
--------------------------------------------------------------------------------
ReadMe        80          .   This file
param.dat     23         18   Basic parameters for the dark star models
spectra.dat   33     729465   Synthetic stellar atmosphere spectra
miri.dat     102        738   JWST/MIRI magnitudes as a function of z
nircam.dat    82        738   JWST/NIRCam magnitudes as a function of z
--------------------------------------------------------------------------------

Byte-by-byte Description of file: param.dat
--------------------------------------------------------------------------------
 Bytes Format  Units  Label    Explanations
--------------------------------------------------------------------------------
   4-  5  I02   ---   Model    Model number
   6- 14  E9.1  eV    MWIMP    WIMP (weakly interacting massive particles) mass
  15- 23  I9  solMass MDS      Dark star mass
--------------------------------------------------------------------------------

Byte-by-byte Description of file: spectra.dat
--------------------------------------------------------------------------------
  Bytes  Format  Units  Label     Explanations
--------------------------------------------------------------------------------
   4-  5  I02    ---    Model     Model number
   7- 19  E13.6  0.1nm  lambda    Rest frame wavelength
  21- 33  E13.6  uW/nm  L.lambda  Rest frame specific luminosity (in erg/s/{AA})
--------------------------------------------------------------------------------

Byte-by-byte Description of file: miri.dat
--------------------------------------------------------------------------------
   Bytes Format  Units   Label    Explanations
--------------------------------------------------------------------------------
  4-  5  I02     ---     Model    Model number
  6- 12  F7.3    ---     z        Redshift
 13- 22  F10.3   mag     F560W    ?=999.0 Flux in JWST/MIRI F560W filter (G1)
 23- 32  F10.3   mag     F770W    ?=999.0 Flux in JWST/MIRI F770W filter (G1)
 33- 42  F10.3   mag     F1100W   ?=999.0 Flux in JWST/MIRI F1100W filter (G1)
 43- 52  F10.3   mag     F1130W   ?=999.0 Flux in JWST/MIRI F1130W filter (G1)
 53- 62  F10.3   mag     F1280W   ?=999.0 Flux in JWST/MIRI F1280W filter (G1)
 63- 72  F10.3   mag     F1500W   ?=999.0 Flux in JWST/MIRI F1500W filter (G1)
 73- 82  F10.3   mag     F1800W   ?=999.0 Flux in JWST/MIRI F1800W filter (G1)
 83- 92  F10.3   mag     F2100W   ?=999.0 Flux in JWST/MIRI F2100W filter (G1)
 93-102  F10.3   mag     F2550W   ?=999.0 Flux in JWST/MIRI F2550W filter (G1)
--------------------------------------------------------------------------------

Byte-by-byte Description of file: nircam.dat
--------------------------------------------------------------------------------
   Bytes Format  Units   Label    Explanations
--------------------------------------------------------------------------------
  4-  5  I02     ---     Model    Model number
  6- 12  F7.3    ---     z        Redshift
 13- 22  F10.3   mag     F070W    ?=999.0 Flux in JWST/NIRCam F070W filter (G1)
 23- 32  F10.3   mag     F115W    ?=999.0 Flux in JWST/NIRCam F115W filter (G1)
 33- 42  F10.3   mag     F150W    ?=999.0 Flux in JWST/NIRCam F150W filter (G1)
 43- 52  F10.3   mag     F200W    ?=999.0 Flux in JWST/NIRCam F200W filter (G1)
 53- 62  F10.3   mag     F277W    ?=999.0 Flux in JWST/NIRCam F277W filter (G1)
 63- 72  F10.3   mag     F356W    ?=999.0 Flux in JWST/NIRCam F356W filter (G1)
 73- 82  F10.3   mag     F444W    ?=999.0 Flux in JWST/NIRCam F444W filter (G1)
--------------------------------------------------------------------------------

Global Notes:
Note (G1): Apparent magnitudes in the AB system.
     At z = 0.0, these magnitudes are absolute, i.e. based on an assumed
     distance of 10pc. At higher redshifts, the magnitudes are based on
     luminosity distances calculated using the cosmology {Omega}_M_=0.27,
     {Omega}_{Lambda}_=0.73 and H_0_=72km/s/Mpc. When calculating these
     magnitudes, the intergalactic medium (IGM) shortward of Lyman {alpha}
     (1216{AA} in the rest frame) has been assumed to be completely opaque
     at z>6. Whenever the upper or lower wavelength limit of the stellar
     atmosphere spectrum is redshifted into one of the JWST filters, the
     corresponding AB magnitude is set to 999.000.
--------------------------------------------------------------------------------


================================================================================
(End)            Erik Zackrisson [Stockholm Observatory, Sweden]     25-Aug-2010
