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Eric Gawiser

Publications and source records attributed to Eric Gawiser.

At least 235 records · Page 13Linked to original sources

Damped Lyman alpha Systems

Observations of damped Lyman alpha systems offer a unique window on the neutral-gas reservoirs that gave rise to galaxies at high redshifts. This review focuses on critical properties such as the H I and metal content of the gas and on independent evidence for star formation. Together, these provide an emerging picture of gravitationally bound objects in which accretion of gas from the IGM replenishes gas consumed by star formation. Other properties such as dust content, molecular content, ionized-gas content, gas kinematics, and galaxy identifications are also reviewed. These properties point to a multiphase ISM in which radiative and hydrodynamic feedback processes are present. Numerical simulations and other types of models used to describe damped Lyman alpha systems within the context of galaxy formation are also discussed.

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The Calan-Yale Deep Extragalactic Research (CYDER) Survey: Optical Properties and Deep Spectroscopy of Serendipitous X-ray Sources

We present the first results from the Calán-Yale Deep Extragalactic Research (CYDER) survey. The main goal of this survey is to study serendipitous X-ray sources detected by Chandra in an intermediate flux range ($10^{-15}-10^{-12}$ ergs s$^{-1}$) that comprises most of the X-ray background. 267 X-ray sources spread over 5 archived fields were detected. The $\log N-\log S$ distribution obtained for this sample is consistent with the results of other surveys. Deep $V$ and $I$ images were taken of these fields in order to calculate X-ray-to-optical flux ratios. Identifications and redshifts were obtained for 106 sources using optical spectroscopy from 8-m class telescopes to reach the optically faintest sources, to the same level as deeper X-ray fields like the Chandra Deep Fields, showing that the nature of sources detected depends mostly on the optical limit for spectroscopy. In general, sources optically classified as obscured Active Galactic Nuclei (AGNs) have redder optical colors than unobscured AGN. A rough correlation between $f_X/f_{\rm opt}$ and hard X-ray luminosity was found for obscured AGN confirming the prediction by existing models that in obscured AGN the optical light is completely dominated by the host galaxy. The previously claimed decrease of the obscured to unobscured AGN ratio with increasing X-ray luminosity is observed. However, this correlation can be explained as a selection effect caused by the lower optical flux of obscured AGN. Comparison between the observed $N_H$ distribution and predictions by existing models shows that the sample appears complete up to $N_H<3\times 10^{22}$ cm$^{-2}$, while for more obscured sources incompleteness plays an important role in the observed obscured to unobscured AGN ratio.

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On the Nature of the Heat Source for Damped Lya Systems

We investigate the heat source of the neutral gas comprising DLAs. Unlike the Lya forest, where the extragalactic background radiation field ionizes and heats the gas, we find that grain photoelectric heating by the FUV background is not sufficient to balance the C II 158um cooling rate inferred from DLAs. In these systems, a local energy source is required. We show that in the case of the z=1.919 DLA toward Q2206-19, the local source is FUV emission from the associated galaxy found by Moller et al (2002): the mean intensity inferred from photometry is in good agreement with the intensity Jnu required to explain the cooling rate. The FUV mean intensity predicted for a cold neutral medium (CNM) model, Jnu=(1.7+2.7-1.0)x10^(-18) cgs (95% c.l.), is the largest expected from our CII* study of 45 DLAs. This may explain why this is the only confirmed DLA yet detected in emission at z>1.9. We argue that in most DLAs with detected CII* absorption, Jnu is between 10^{-19} and 10^{-18} and heats the gas which is a CNM. By contrast, in most DLAs with upper limits on CII* absorption the gas is a warm neutral medium (WNM). Surprisingly, the upper limits are compatible with the same range of Jnu values suggesting the majority of DLAs are heated by radiation fields generated by a limited range of star formation rates per unit H I area, between 10^{-3} and 10^{-2} Msol/kpc^2. We also show that CII* absorption is unlikely to arise in gas that is ionized.

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A Rejuvenated Universe Without Initial Singularity

Cosmological observations strongly suggest the presence of dark energy which comprises the majority of the current energy density of the universe. The equation of state relating the pressure and energy density of this dark energy, p = w ρ, appears to have w close to -1, with most analyses preferring w<-1 when these values are considered as part of the parameter space. If w<-1 is the future behavior of the dark energy, the scale factor, expansion rate, and energy density of the universe will diverge in a finite time as its apparent expansion age tends to zero. We hypothesize that w>-1 is restored at a late enough time, perhaps due to a phase transition of the dark energy, and show that this produces conditions observationally indistinguishable from a Hot Big Bang. This process of rejuvenation may have occurred in the past, making our universe much older than it appears and eliminating the Big Bang singularity.

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An X-ray Selected AGN at z=4.6 Discovered by the CYDER Survey

We present the discovery of a high redshift, X-ray selected AGN by the Calan-Yale Deep Extragalactic Research (CYDER) survey: CXOCY J033716.7-050153, located at $z=4.61$, the second high redshift AGN discovered by this survey. Here, we present its optical, near-IR and X-ray properties and compare it with other optical and X-ray selected high redshift AGN. The optical luminosity of this object is significantly lower than most optically selected high redshift quasars. It also has a lower rest frame UV to X-ray emission ratio than most known quasars at this redshift. This mild deviation can be explained either by dust obscuring the UV radiation of a normal radio quiet AGN emitting at 10% of its Eddington luminosity or because this is intrinsically a low luminosity radio loud AGN, with a super-massive Black Hole of $\sim 10^8M_\sun$ emitting at 1% of its Eddington luminosity. Deep radio observations can discriminate between these two hypotheses.

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The ESI/KeckII Damped Lya Abundance Database

This paper presents chemical abundance measurements for 37 damped Lya systems at z>2.5 observed with the Echellette Spectrograph and Imager on the KeckII telescope. We measure the HI column densities of these damped systems through Voigt profile fits to their Lya profiles and we implement the apparent optical depth method to determine ionic column densities. Figures and tables of all relevant data are presented. A full analysis of the chemical enrichment history described by these observations will be presented in a future paper. This dataset is also valuable for efficiently planning future echelle observations and for rough abundance pattern analyses. We aim to make this entire data set public within three years of this publication.

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The Age-Metallicity Relation of the Universe in Neutral Gas: The First 100 Damped Lya Systems

We present accurate metallicity measurements for 121 damped Lya systems at 0.5<z<5 including ~50 new measurements from our recently published Echellette Spectrograph and Imager surveys. This dataset is analysed to determine the age-metallicity relation of neutral gas in the universe. Contrary to previous datasets this sample shows statistically significant evolution in the mean metallicity. The best linear fit rate to metallicity vs. redshift is -0.26 +/- 0.07 dex corresponding to approximately a factor of 2 every Gyr at z=3. The DLA continue to maintain a floor in metallicity of ~1/700 solar independent of observational effects. This metallicity threshold limits the prevalence of primordial gas in high redshift galaxies and stresses the correspondence between damped systems and star formation (i.e. galaxy formation). This floor is significantly offset from the metallicity of the Lya forest and therefore we consider it to be more related to active star formation within these galaxies than scenarios of enrichment in the very early universe. Finally, we comment on an apparent 'missing metals problem': the mean metallicity of the damped systems is ~10x lower than the value expected from their observed star formation history. This problem is evident in current theoretical treatments of chemical evolution and galaxy formation; it may indicate a serious flaw in our understanding of the interplay between star formation and metal production.

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CII* Absorption in Damped Lyman Alpha Systems: (II) A New Window on the Star Formation History of the Universe

Starting from the SFR per unit physical area, determined for DLAs using the C II* method, we obtain the SFR per unit comoving volume at $z$ $\approx$ 3, and find that it agrees with that for the Lyman Break Galaxies (LBGs). Though the mass of produced stars indicated by the SFRs is consistent with the current densities of known stellar populations, the mass of metals produced by $z$=2.5 is 30 times larger than detected in absorption in DLAs. The most likely solutions to this ``missing metals'' problem is that star formation occurs in compact bulge regions. We search for evidence of feedback and find no correlations between the SFR per unit area and N(H I), but possible correlations between SFR per unit area and low-ion velocity width and SFR per unit area and metal abundance. We show that (a) the correlation between cooling rate and dust-to-gas ratio is positive evidence for grain photoelectric heating, (b) the CMB does not significantly populate the C II excited fine-structure states, and (c) the ratio of CII* to resonance-line optical depths is a sensitive probe of the multi-phase structure of the DLA gas. We address recent arguments that DLAs are comprised only of WNM gas, and show them to be inconclusive. Despite the rough agreement between SFR per unit comoving volume for DLAs and LBGs, current evidence indicates these are distinct populations.

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CII* Absorption in Damped Lyman Alpha Systems: (I) Star Formation Rates in a Two-Phase Medium

We describe a technique that for the first time measures star formation rates (SFRs) in damped Lyman alpha systems(DLAs) directly. We assume that massive stars form in DLAs, and that the FUV radiation they emit heats the gas by the grain photoelectric mechanism. We infer the heating rate from the cooling rate measured by the strength of CII* 1335.7 absorption. Since the heating rate is proportional to the dust-to-gas ratio and the SFR per unit area, we deduce the SFR per unit area for DLAs in which both quantities have been measured. We consider models in which the the dust comprises carbonaceous or silicate grains. We present two-phase models where the cold neutral medium (CNM) and warm neutral medium (WNM) are in pressuer equilibrium. In the CNM model the the sightline goes throught the CNM and WNM, while in the WNM model it goes only through the WNM. Since the grain photoelectric heating efficiency is at least 10 times higher in the CNM than in the WNM, CII* absorption mainly arises in the CNM in the CNM model. But in the WNM model all of the CII* absorption arises in the WNM. We use CII* absorption lines to derive the SFR per unit area for a sample of ~ 30 DLAs in which the dust-to-gas ratio has been inferred from element depletion patterns. We show that the resulting SFR per unit area corresponds to an average over the star forming volume of galaxy hosting the DLA rather than to local star formation along the line of sight. We find the average SFR per unit area and equals10$^{-2.2}$ M$_{\odot}$yr$^{-1}$kpc$^{-2}$ for the CNM model and 10$^{-1.3}$ M$_{\odot}$yr$^{-1}$kpc$^{-2}$ for the WNM model. The SFR per unit area in the CNM solution is similar to that measured in the Milky Way ISM.

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Galaxies Associated with z~4 Damped Lya Systems: I. Imaging and Photometric Selection

This paper describes the acquisition and analysis of imaging data for the identification of galaxies associated with z~4 damped Lya systems. We present deep BRI images of three fields known to contain four z~4 damped systems. We discuss the reduction and calibration of the data, detail the color criteria used to identify z~4 galaxies, and present a photometric redshift analysis to complement the color selection. We have found no galaxy candidates closer to the QSO than 7'' which could be responsible for the damped Lya systems. Assuming that at least one of the galaxies is not directly beneath the QSO, we set an upper limit on this damped Lya system of L < L*/4. Finally, we have established a web site to release these imaging data to the public.

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The UCSD HIRES/KeckI Damped Lya Abundance Database: I. The Data

We present new chemical abundance measurements of 16 damped Lya systems at z>1.5 and update our previous abundance analyses. The entire database presented here was derived from HIRES observations on the Keck I telescope, reduced with the same software package, and analysed with identical techniques. Altogether, we present a large, homogeneous database of chemical abundance measurements for protogalaxies in the early universe, ideal for studying a number of important aspects of galaxy formation. In addition, we have established an online directory for this database and will continuously update the results.

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First Investigation of the Clustering Environment of Damped Lyman Alpha Absorbers at z=4

We report the first observations of the clustering environment of damped Lyman alpha absorption systems at z=4. Color selection and photometric redshifts were used to select 44 candidate Lyman-break galaxies brighter than I_AB=25.5 from deep BRI images of the 35 sq. arcmin field containing the quasar BR 0951-04. Multislit spectroscopy of 35 candidate galaxies was performed and 8 of these candidates have been confirmed as z>3.5 Lyman-break galaxies. With only BRI photometry, the photometric redshifts are quite accurate for the spectroscopically confirmed galaxies but have a high rate of misclassification due to color degeneracies between Lyman-break galaxies and low-redshift ellipticals. Both of the z>3.5 galaxies found within 15'' of the quasar line-of-sight appear to be causing absorption systems in the quasar spectrum. We use a battery of statistical tests to look for clustering in the redshift histogram of the z>3.5 galaxies but do not find measurable clustering of these Lyman-break galaxies with the damped Lyman alpha absorbers. With a larger sample of galaxies, our method should determine the cross-correlation between these objects, which probes the bias and hence the mass of the damped Lyman alpha absorbers.

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Interpreting CMB Anisotropy Observations: Trying to Tell the Truth with Statistics

A conflict has been reported between the baryon density inferred from deuterium observations and that found from recent CMB observations by BOOMERanG and MAXIMA. Despite the flurry of papers that attempt to resolve this conflict by adding new physics to the early universe, we will show that it can instead be resolved via a more careful usage of statistics. Indeed, the Bayesian analyses that produce this conflict are by their nature poorly suited for drawing this type of conclusion. A properly defined frequentist analysis can address this question directly and appears not to find a conflict. Finally, a conservative accounting of systematic uncertainties in measuring the deuterium abundance could reduce what is nominally a 3 sigma conflict to 1 sigma.

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Galactic Chemical Abundances at z>3 I: First Results from the Echellette Spectrograph and Imager

We present the first results from an ongoing survey to discover and measure the metallicity of z>3 damped Lya systems with the Echellette Spectrograph and Imager (ESI) on the Keck II telescope. Our motivation arises from a recent study on the damped Lya systems suggesting only mild evolution in the cosmic metallicity from z~2 to 4. The Echellette Spectrograph and Imager, which provides two complementary spectroscopic modes, is the ideal instrument for a z>3 damped Lya survey. We describe our observing strategy and report on the discovery and analysis of 5 new z>3 damped Lya systems acquired in a single night of observing. These observations further support the principal conclusions of the previous study: (1) the cosmic metallicity in neutral gas inferred from the damped Lya systems does not evolve significantly from z~2 to 4; (2) the unweighted metallicity exhibits a statistically significant decrease with increasing redshift; and (3) not a single damped Lya system has a metallicity below [Fe/H]=-3. We discuss the implications of these results and comment on recent theoretical studies which attempt to explain the observations.

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Constraining Primordial Non-Gaussianity With the Abundance of High Redshift Clusters

We show how observations of the evolution of the galaxy cluster number abundance can be used to constrain primordial non-Gaussianity in the universe. We carry out a maximum likelihood analysis incorporating a number of current datasets and accounting for a wide range of sources of systematic error. Under the assumption of Gaussianity, the current data prefer a universe with matter density $Ω_m\simeq 0.3$ and are inconsistent with $Ω_m=1$ at the $2σ$ level. If we assume $Ω_m=1$, the predicted degree of cluster evolution is consistent with the data for non-Gaussian models where the primordial fluctuations have at least two times as many peaks of height $3σ$ or more as a Gaussian distribution does. These results are robust to almost all sources of systematic error considered: in particular, the $Ω_m=1$ Gaussian case can only be reconciled with the data if a number of systematic effects conspire to modify the analysis in the right direction. Given an independent measurement of $Ω_m$, the techniques described here represent a powerful tool with which to constrain non-Gaussianity in the primordial universe, independent of specific details of the non-Gaussian physics. We discuss the prospects and strategies for improving the constraints with future observations.

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Limits on Neutrino Masses from Large-Scale Structure

Massive neutrinos have a detectable effect on cosmological structure formation, in particular on the large-scale distribution of galaxies. Adding Hot Dark Matter to the now-standard Lambda CDM model leads to a worse fit to large-scale structure and CMB anisotropy data. This results in a limit on the mass of the most massive neutrino of 4 eV, assuming a power-law primordial power spectrum.

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Is the Lambda CDM Model Consistent with Observations of Large-Scale Structure?

The claim that large-scale structure data independently prefers the Lambda Cold Dark Matter model is a myth. However, an updated compilation of large-scale structure observations cannot rule out Lambda CDM at 95% confidence. We explore the possibility of improving the model by adding Hot Dark Matter but the fit becomes worse; this allows us to set limits on the neutrino mass.

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Big Bang Leftovers in the Microwave: Cosmology with the Cosmic Microwave Background Radiation

We combine detections of anisotropy in the Cosmic Microwave Background radiation with observations of inhomogeneity in the large-scale distribution of galaxies to test the predictions of models of cosmological structure formation. This combination probes spatial scales varying by three orders of magnitude, including a significant region where the two types of data overlap. We examine Cold Dark Matter models with adiabatic density perturbations, isocurvature models, and a topological defects model. We set upper limits on the neutrino mass and find the primordial power spectrum needed to reconcile an apparent disagreement between structure formation observations and direct observations of cosmological parameters. Present and future observations of Cosmic Microwave Background anisotropy suffer from foreground contamination. We develop detailed predictions for microwave emission from radio and infrared-bright galaxies and the Sunyaev-Zeldovich effect from clusters. We present realistic simulations of the microwave sky, produced as part of the `WOMBAT Challenge' exercise, and introduce a pixel-space method for subtracting foreground contamination which can be tested on these simulations.

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