Puragra Guhathakurta
University of California, Santa Cruz
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Featured researches published by Puragra Guhathakurta.
The Astrophysical Journal | 2007
Kai G. Noeske; Benjamin J. Weiner; S. M. Faber; Casey Papovich; David C. Koo; Rachel S. Somerville; Kevin Bundy; Christopher J. Conselice; J. A. Newman; David Schiminovich; E. Le Floc'h; Alison L. Coil; G. H. Rieke; Jennifer M. Lotz; Joel R. Primack; P. Barmby; Michael C. Cooper; M. Davis; Richard S. Ellis; Giovanni G. Fazio; Puragra Guhathakurta; Jing Huang; Susan A. Kassin; D. C. Martin; Andrew C. Phillips; Robert Michael Rich; Todd Small; C. A. N. Willmer; Graham Wallace Wilson
We analyze star formation (SF) as a function of stellar mass (M☉) and redshift z in the All-Wavelength Extended Groth Strip International Survey. For 2905 field galaxies, complete to 10^10(10^10.8 )M at z < 0.7(1), with Keck spectroscopic redshifts out to z = 1.1, we compile SF rates (SFRs) from emission lines, GALEX, and Spitzer MIPS 24 µm photometry, optical-NIR M* measurements, and HST morphologies. Galaxies with reliable signs of SF form a distinct “main sequence” (MS), with a limited range of SFRs at a given M* and z (1 σ ≾ ±0.3 dex), and log (SFR) approximately proportional to log M*. The range of log (SFR) remains constant to z > 1, while the MS as a whole moves to higher SFR as z increases. The range of the SFR along the MS constrains the amplitude of episodic variations of SF and the effect of mergers on the SFR. Typical galaxies spend ∼67%(95%) of their lifetime since z = 1 within a factor of ≾2(4) of their average SFR at a given M* and z. The dominant mode of the evolution of SF since z ∼ 1 is apparently a gradual decline of the average SFR in most individual galaxies, not a decreasing frequency of starburst episodes, or a decreasing factor by which SFRs are enhanced in starbursts. LIRGs at z ∼ 1 seem to mostly reflect the high SFR typical for massive galaxies at that epoch. The smooth MS may reflect that the same set of few physical processes governs SF prior to additional quenching processes. A gradual process like gas exhaustion may play a dominant role.
The Astrophysical Journal | 2007
M. Davis; Puragra Guhathakurta; Nicholas P. Konidaris; Jeffrey A. Newman; M. L. N. Ashby; A. D. Biggs; Pauline Barmby; Kevin Bundy; S. C. Chapman; Alison L. Coil; Christopher J. Conselice; Michael C. Cooper; Darren J. Croton; Peter R. M. Eisenhardt; Richard S. Ellis; S. M. Faber; Taotao Fang; Giovanni G. Fazio; A. Georgakakis; Brian F. Gerke; W. M. Goss; Stephen D. J. Gwyn; Justin Harker; Andrew M. Hopkins; Jia-Sheng Huang; R. J. Ivison; Susan A. Kassin; Evan N. Kirby; Anton M. Koekemoer; David C. Koo
In this the first of a series of Letters, we present a panchromatic data set in the Extended Groth Strip region of the sky. Our survey, the All-Wavelength Extended Groth Strip International Survey (AEGIS), aims to study the physical properties and evolutionary processes of galaxies at z ~ 1. It includes the following deep, wide-field imaging data sets: Chandra/ACIS X-ray, GALEX ultraviolet, CFHT/MegaCam Legacy Survey optical, CFHT/CFH12K optical, Hubble Space Telescope/ACS optical and NICMOS near-infrared, Palomar/WIRC near-infrared, Spitzer/IRAC mid-infrared, Spitzer/MIPS far-infrared, and VLA radio continuum. In addition, this region of the sky has been targeted for extensive spectroscopy using the Deep Imaging Multi-Object Spectrograph (DEIMOS) on the Keck II 10 m telescope. Our survey is compared to other large multiwavelength surveys in terms of depth and sky coverage.
The Astrophysical Journal | 2006
Christopher N. A. Willmer; S. M. Faber; David C. Koo; Benjamin J. Weiner; Jeffrey A. Newman; Alison L. Coil; A. J. Connolly; Charlie Conroy; Michael C. Cooper; M. Davis; Douglas P. Finkbeiner; Brian F. Gerke; Puragra Guhathakurta; Justin Harker; Nick Kaiser; Susan A. Kassin; Nicholas P. Konidaris; Lihwai Lin; Gerard A. Luppino; Darren Madgwick; Kai G. Noeske; Andrew C. Phillips; Renbin Yan
The evolution of the B-band galaxy luminosity function is measured using a sample of more than 11,000 galaxies with spectroscopic redshifts from the DEEP2 Redshift Survey. The rest-frame MB versus U - B color-magnitude diagram of DEEP2 galaxies shows that the color-magnitude bimodality seen in galaxies locally is still present at redshifts z > 1. Dividing the sample at the trough of this color bimodality into predominantly red and blue galaxies, we find that the luminosity function of each galaxy color type evolves differently. Blue counts tend to shift to brighter magnitudes at constant number density, while the red counts remain largely constant at a fixed absolute magnitude. Using Schechter functions with fixed faint-end slopes we find that M for blue galaxies brightens by ~1.3 ? 0.14 mag per unit redshift, with no significant evolution in number density. For red galaxies M brightens somewhat less with redshift, while the formal value of * declines. When the population of blue galaxies is subdivided into two halves using the rest-frame color as the criterion, the measured evolution of both blue subpopulations is very similar.The evolution of the B-band galaxy luminosity function is measured using a sample of more than 11,000 galaxies with spectroscopic redshifts from the DEEP2 Redshift Survey. The rest-frame M_B versus U-B color-magnitude diagram of DEEP2 galaxies shows that the color-magnitude bi-modality seen in galaxies locally is still present at redshifts z > 1. Dividing the sample at the trough of this color bimodality into predominantly red and blue galaxies, we find that the luminosity function of each galaxy color type evolves differently. Blue counts tend to shift to brighter magnitudes at constant number density, while the red counts remain largely constant at a fixed absolute magnitude. Using Schechter functions with fixed faint-end slopes we find that M*_B for blue galaxies brightens by ~ 1.3 magnitudes per unit redshift, with no significant evolution in number density. For red galaxies M*_B brightens somewhat less with redshift, while the formal value of phi* declines. When the population of blue galaxies is subdivided into two halves using the rest-frame color as the criterion, the measured evolution of both blue subpopulations is very similar.
Astrophysical Journal Supplement Series | 2013
Jeffrey A. Newman; Michael C. Cooper; Marc Davis; S. M. Faber; Alison L. Coil; Puragra Guhathakurta; David C. Koo; Andrew C. Phillips; Charlie Conroy; Aaron A. Dutton; Douglas P. Finkbeiner; Brian F. Gerke; D. Rosario; Benjamin J. Weiner; Christopher N. A. Willmer; Renbin Yan; Justin Harker; Susan A. Kassin; Nicholas P. Konidaris; Kamson Lai; Darren Madgwick; Kai G. Noeske; Gregory D. Wirth; Andrew J. Connolly; Nick Kaiser; Evan N. Kirby; Brian C. Lemaux; Lihwai Lin; Jennifer M. Lotz; Gerard A. Luppino
We describe the design and data analysis of the DEEP2 Galaxy Redshift Survey, the densest and largest high-precision redshift survey of galaxies at z ~ 1 completed to date. The survey was designed to conduct a comprehensive census of massive galaxies, their properties, environments, and large-scale structure down to absolute magnitude M_B = −20 at z ~ 1 via ~90 nights of observation on the Keck telescope. The survey covers an area of 2.8 deg^2 divided into four separate fields observed to a limiting apparent magnitude of R_(AB) = 24.1. Objects with z ≾0.7 are readily identifiable using BRI photometry and rejected in three of the four DEEP2 fields, allowing galaxies with z > 0.7 to be targeted ~2.5 times more efficiently than in a purely magnitude-limited sample. Approximately 60% of eligible targets are chosen for spectroscopy, yielding nearly 53,000 spectra and more than 38,000 reliable redshift measurements. Most of the targets that fail to yield secure redshifts are blue objects that lie beyond z ~ 1.45, where the [O ii] 3727 A doublet lies in the infrared. The DEIMOS 1200 line mm^(−1) grating used for the survey delivers high spectral resolution (R ~ 6000), accurate and secure redshifts, and unique internal kinematic information. Extensive ancillary data are available in the DEEP2 fields, particularly in the Extended Groth Strip, which has evolved into one of the richest multiwavelength regions on the sky. This paper is intended as a handbook for users of the DEEP2 Data Release 4, which includes all DEEP2 spectra and redshifts, as well as for the DEEP2 DEIMOS data reduction pipelines. Extensive details are provided on object selection, mask design, biases in target selection and redshift measurements, the spec2d two-dimensional data-reduction pipeline, the spec1d automated redshift pipeline, and the zspec visual redshift verification process, along with examples of instrumental signatures or other artifacts that in some cases remain after data reduction. Redshift errors and catastrophic failure rates are assessed through more than 2000 objects with duplicate observations. Sky subtraction is essentially photon-limited even under bright OH sky lines; we describe the strategies that permitted this, based on high image stability, accurate wavelength solutions, and powerful B-spline modeling methods. We also investigate the impact of targets that appear to be single objects in ground-based targeting imaging but prove to be composite in Hubble Space Telescope data; they constitute several percent of targets at z ~ 1, approaching ~5%–10% at z > 1.5. Summary data are given that demonstrate the superiority of DEEP2 over other deep high-precision redshift surveys at z ~ 1 in terms of redshift accuracy, sample number density, and amount of spectral information. We also provide an overview of the scientific highlights of the DEEP2 survey thus far.
The Astrophysical Journal | 2008
Jennifer M. Lotz; M. Davis; S. M. Faber; Puragra Guhathakurta; Stephen D. J. Gwyn; Jia-Sheng Huang; David C. Koo; Lihwai Lin; Jeffrey A. Newman; Kai G. Noeske; Casey Papovich; Christopher N. A. Willmer; Alison L. Coil; Christopher J. Conselice; Michael C. Cooper; Andrew M. Hopkins; Anne Julie Metevier; Joel R. Primack; G. H. Rieke; Benjamin J. Weiner
We present the quantitative rest-frame B morphological evolution and galaxy merger fraction at 0.2 1011 L☉ are disk galaxies, and only ~15% are classified as major merger candidates. Edge-on and dusty disk galaxies (Sb-Ir) are almost a third of the red sequence at z ~ 1.1, while E/S0/Sa make up over 90% of the red sequence at z ~ 0.3. Approximately 2% of our full sample are red mergers. We conclude (1) the merger rate does not evolve strongly between 0.2 < z < 1.2; (2) the decrease in the volume-averaged star formation rate density since z ~ 1 is a result of declining star formation in disk galaxies rather than a disappearing population of major mergers; (3) the build-up of the red sequence at z < 1 can be explained by a doubling in the number of spheroidal galaxies since z ~ 1.2.
The Astrophysical Journal | 2013
Evan N. Kirby; Judith G. Cohen; Puragra Guhathakurta; Lucy Cheng; James S. Bullock; Anna Gallazzi
We present spectroscopic metallicities of individual stars in seven gas-rich dwarf irregular galaxies (dIrrs), and we show that dIrrs obey the same mass-metallicity relation as the dwarf spheroidal (dSph) satellites of both the Milky Way and M31: Z_* ∝ M_*^(0.30±0.02). The uniformity of the relation is in contradiction to previous estimates of metallicity based on photometry. This relationship is roughly continuous with the stellar mass-stellar metallicity relation for galaxies as massive as M_* = 10^(12) M_☉. Although the average metallicities of dwarf galaxies depend only on stellar mass, the shapes of their metallicity distributions depend on galaxy type. The metallicity distributions of dIrrs resemble simple, leaky box chemical evolution models, whereas dSphs require an additional parameter, such as gas accretion, to explain the shapes of their metallicity distributions. Furthermore, the metallicity distributions of the more luminous dSphs have sharp, metal-rich cut-offs that are consistent with the sudden truncation of star formation due to ram pressure stripping.
Monthly Notices of the Royal Astronomical Society | 2006
Michael C. Cooper; Jeffrey A. Newman; Darren J. Croton; Benjamin J. Weiner; Christopher N. A. Willmer; Brian F. Gerke; Darren Madgwick; S. M. Faber; Marc Davis; Alison L. Coil; Douglas P. Finkbeiner; Puragra Guhathakurta; David C. Koo
We study the mean environment of galaxies in the DEEP2 Galaxy Redshift Survey as a function of rest-frame color, luminosity, and [OII] 3727u equivalent width. The local galaxy overdensity for > 14,000 galaxies at 0.75 < z < 1.35 is estimated using the projected 3 rd -nearest-neighbor surface density. Of the galaxy properties studied, mean environment is found to depend most strongly on galaxy color; all major features of the correlation between mean overdensity and rest-frame color observed in the local universe were already in place at z ∼ 1. In contrast to local results, we find a substantial slope in the mean dependence of environment on luminosity for blue, star-forming galaxies at z ∼ 1, with brighter blue galaxies being found on average in regions of greater overdensity. We discuss the roles of galaxy clusters and groups in establishing the observed correlations between environment and galaxy properties at high redshift, and we also explore the evidence for a “downsizing of quenching” from z ∼ 1 to z ∼ 0. Our results add weight to existing evidence that the mechanism(s) that result in star-formation quenching are efficient in group environments as well as clusters. This work is the first of its kind at high redshift and represents the first in a series of papers addressing the role of environment in galaxy formation at 0 < z < 1. Subject headings: galaxies:high-redshift, galaxies:evolution, galaxies:statistics, galaxies:fundamental parameters, large-scale structure of universe
Monthly Notices of the Royal Astronomical Society | 2007
Michael C. Cooper; Jeffrey A. Newman; Benjamin J. Weiner; Renbin Yan; Christopher N. A. Willmer; Kevin Bundy; Alison L. Coil; Christopher J. Conselice; Marc Davis; S. M. Faber; Brian F. Gerke; Puragra Guhathakurta; David C. Koo; Kai G. Noeske
Using galaxy samples drawn from the Sloan Digital Sky Survey and the DEEP2 Galaxy Redshift Survey, we study the relationship between star formation and environment at z ∼ 0.1 and 1. We estimate the total star formation rate (SFR) and specific star formation rate (sSFR) for each galaxy according to the measured [O II] λ 3727 A nebular line luminosity, corrected using empirical calibrations to match more robust SFR indicators. Echoing previous results, we find that in the local Universe star formation depends on environment such that galaxies in regions of higher overdensity, on average, have lower SFRs and longer star formation time-scales than their counterparts in lower density regions. At z ∼ 1, we show that the relationship between sSFR and environment mirrors that found locally. However, we discover that the relationship between total SFR and overdensity at z ∼ 1 is inverted relative to the local relation. This observed evolution in the SFR-density relation is driven, in part, by a population of bright, blue galaxies in dense environments at z ∼ 1. This population, which lacks a counterpart at z ∼ 0, is thought to evolve into members of the red sequence from z ∼ 1 to ∼ 0. Finally, we conclude that environment does not play a dominant role in the cosmic star formation history at z < 1: the dependence of the mean galaxy SFR on local galaxy density at constant redshift is small compared to the decline in the global SFR space density over the last 7 Gyr.
The Astrophysical Journal | 2011
Evan N. Kirby; Gustavo A. Lanfranchi; Joshua D. Simon; Judith G. Cohen; Puragra Guhathakurta
We present metallicity distribution functions (MDFs) for the central regions of eight dwarf satellite galaxies of the Milky Way: Fornax, Leo I and II, Sculptor, Sextans, Draco, Canes Venatici I, and Ursa Minor. We use the published catalog of abundance measurements from the previous paper in this series. The measurements are based on spectral synthesis of iron absorption lines. For each MDF, we determine maximum likelihood fits for Leaky Box, Pre-Enriched, and Extra Gas (wherein the gas supply available for star formation increases before it decreases to zero) analytic models of chemical evolution. Although the models are too simplistic to describe any MDF in detail, a Leaky Box starting from zero metallicity gas fits none of the galaxies except Canes Venatici I well. The MDFs of some galaxies, particularly the more luminous ones, strongly prefer the Extra Gas Model to the other models. Only for Canes Venatici I does the Pre-Enriched Model fit significantly better than the Extra Gas Model. The best-fit effective yields of the less luminous half of our galaxy sample do not exceed 0.02 Z� , indicating that gas outflow is important in the chemical evolution of the less luminous galaxies. We surmise that the ratio of the importance of gas infall to gas outflow increases with galaxy luminosity. Strong correlations of average [Fe/H] and metallicity spread with luminosity support this hypothesis.
The Astrophysical Journal | 2008
Evan N. Kirby; Joshua D. Simon; Marla Geha; Puragra Guhathakurta; Anna Frebel
We present new metallicity measurements for 298 individual red giant branch stars in eight of the least luminous dwarf spheroidal galaxies (dSphs) in the Milky Way (MW) system. Our technique is based on medium-resolution Keck DEIMOS spectroscopy coupled with spectral synthesis. We present the first spectroscopic metallicities at [ Fe/H ] < − 3.0 of stars in a dwarf galaxy, with individual stellar metallicities as low as [ Fe/H ] = − 3.3. Because our [Fe/H] measurements are not tied to empirical metallicity calibrators and are sensitive to arbitrarily low metallicities, we are able to probe this extremely metal-poor regime accurately. The metallicity distribution of stars in these dSphs is similar to the MW halo at the metal-poor end. We also demonstrate that the luminosity-metallicity relation previously seen in more luminous dSph galaxies (MV = − 13.4 to –8.8) extends smoothly down to an absolute magnitude of MV = − 3.7. The discovery of extremely metal-poor stars in dSphs lends support to the ΛCDM galaxy assembly paradigm wherein dwarf galaxies dissolve to form the stellar halo of the MW.