Title: High Resolution Spectroscopy of the IGM: How High? Jill Bechtold, University of Arizona
1High Resolution Spectroscopy of the IGM How
High?Jill Bechtold, University of Arizona
- Central Question How were large galaxies like
our Milky Way assembled out of small star forming
fragments and the intergalactic gas during the
last 10 billion years? - Technique UV spectra of background quasars and
starburst galaxies to study the IGM and its
evolving relationship to luminous and dark matter
in the Universe
2Outline
- Science which really requires gt10m aperture
- IGM tomography using multiple sight-lines
-
Simulation of H I from Cen
Simcoe (1997) - Spectral resolution how high?
3A 3D map of Galaxies and Gas
- How does gas collapse to form galaxies?
- How do large-scale structures affect the
formation of stars and galaxies? - How do galaxies and AGN enrich the gas?
- What environmental processes effect the variety
of morphological type, stellar populations, age
and metallicity we see in present-day galaxies?
4Key MeasurementMeasure Lyman series, metals and
H2 absorption using multiple background AGN and
correlate with galaxy redshift survey
- Need to sample a volume large enough to sample
cosmic variance - --gt similar volume to 2dF or SDSS survey, so
several hundred Mpc on a side - --gt 5x5 square degrees
- --gt 100,000 galaxy redshifts
- --gt mean separation of background AGN needs to be
0.1 arcmin2 or few hundred per square degree
5Surface density of probes
6Why do you need high spectral resolution?
- Resolve line widths, in order to fit profiles
and derive temperatures and column densities - Resolve velocity structure of profile into
components ie physically distinct clouds of gas
moving in the gravitational potential of the host
galaxy - Detect weak transitions of rare elements, to be
on the linear part of the curve-of-growth, and to
probe diagnostics of nucleosynthesis and depletion
7Why do you need high spectral resolution?
- FOS
- 280 km/s
- STIS
- 12 km/s
- Jannuzi 2004
8Lines-of-site Observed to date by STIS
9Simulated Lyman alpha forest spectra
R16 Quasar z(em)1.7 30 HST orbits E(B-V)0.05
STIS E230M
10R19
11R23
12What spectral resolution?Thermal Widths of
Absorption Lines
- 100 K 6,000 K
100,000 K - (diffuse ISM) (WHIM) (Coronal,
IGM) - A b R b
R b R - Hydrogen 1 1.29 140,000 9.99 18,000
40.8 4400 - Helium 4 0.64 280,000 5.00 36,000
20.4 8900 - Carbon 12 0.37 485,000 2.88 62,000
11.8 15,000 - Nitrogen 14 0.35 523,000 2.67 67,000
10.9 27,000 - Oxygen 16 0.32 560,000 2.50 72,000
10.2 18,000 - Iron 56 0.17 1,052,000 1.34 134,000
5.5 33,000 - A atomic weight
- b Doppler width in km/sec (2kT/m)1/2
- R (FWHM)
13Spectral resolution
- Follow Schroeder (2000) for a classical echelle
spectrograph
Where R spectral resolution d1
the size of the spectrograph beam D
diameter of primary mirror d blaze
angle of the echelle grating f
width of slit if diffraction limited then
14Spectral resolution
Assume 10 inch beam, blaze 67 degrees then the
spectral resolution, R, is
The slit projects to the detector with width w in
microns given by
Where r anamorphic demagnification ( 1)
f focal ratio of the spectrograph
camera So for 5 micron pixels, 2 pixel sampling,
slit width 3x the diffraction limit, f 5,
camera is 4 feet long --gt ok
15Summary
- Pairs of quasars --gt IGM structure require 4m
class telescope - IGM tomography --gt m23 quasars, 20m or greater
telescope aperture multiplexed - R 106 spectrographs feasible, and would be
necessary to probe T100 K diffuse ISM - R20,000 100,000 have adequate resolution for
coronal gas, WHIM, and IGM