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Dive into the research topics where Maria Rebecca Drout is active.

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Featured researches published by Maria Rebecca Drout.


The Astrophysical Journal | 2014

Cosmological Constraints from Measurements of Type Ia Supernovae Discovered During the First 1.5 Yr of the Pan-STARRS1 Survey

Armin Rest; D. Scolnic; Ryan J. Foley; M. Huber; Ryan Chornock; Gautham S. Narayan; John L. Tonry; Edo Berger; Alicia M. Soderberg; Christopher W. Stubbs; Adam G. Riess; Robert P. Kirshner; S. J. Smartt; Edward F. Schlafly; Steven A. Rodney; M. T. Botticella; D. Brout; Peter M. Challis; Ian Czekala; Maria Rebecca Drout; Michael J. Hudson; R. Kotak; C. Leibler; R. Lunnan; G. H. Marion; M. McCrum; D. Milisavljevic; Andrea Pastorello; Nathan Edward Sanders; K. W. Smith

We present griz P1 light curves of 146 spectroscopically confirmed Type Ia supernovae (SNe Ia; 0.03 < z < 0.65) discovered during the first 1.5 yr of the Pan-STARRS1 Medium Deep Survey. The Pan-STARRS1 natural photometric system is determined by a combination of on-site measurements of the instrument response function and observations of spectrophotometric standard stars. We find that the systematic uncertainties in the photometric system are currently 1.2% without accounting for the uncertainty in the Hubble Space Telescope Calspec definition of the AB system. A Hubble diagram is constructed with a subset of 113 out of 146 SNe Ia that pass our light curve quality cuts. The cosmological fit to 310 SNe Ia (113 PS1 SNe Ia + 222 light curves from 197 low-z SNe Ia), using only supernovae (SNe) and assuming a constant dark energy equation of state and flatness, yields . When combined with BAO+CMB(Planck)+H 0, the analysis yields and including all identified systematics. The value of w is inconsistent with the cosmological constant value of –1 at the 2.3σ level. Tension endures after removing either the baryon acoustic oscillation (BAO) or the H 0 constraint, though it is strongest when including the H 0 constraint. If we include WMAP9 cosmic microwave background (CMB) constraints instead of those from Planck, we find , which diminishes the discord to <2σ. We cannot conclude whether the tension with flat ΛCDM is a feature of dark energy, new physics, or a combination of chance and systematic errors. The full Pan-STARRS1 SN sample with ~three times as many SNe should provide more conclusive results.


The Astrophysical Journal | 2013

A PANCHROMATIC VIEW OF THE RESTLESS SN 2009ip REVEALS THE EXPLOSIVE EJECTION OF A MASSIVE STAR ENVELOPE

R. Margutti; D. Milisavljevic; Alicia M. Soderberg; Ryan Chornock; B. A. Zauderer; Kohta Murase; C. Guidorzi; Nathan Edward Sanders; Paul Kuin; Claes Fransson; Emily M. Levesque; P. Chandra; Edo Berger; Federica B. Bianco; Peter J. Brown; P. Challis; Emmanouil Chatzopoulos; C. C. Cheung; Changsu Choi; Laura Chomiuk; N. N. Chugai; Carlos Contreras; Maria Rebecca Drout; Robert A. Fesen; Ryan J. Foley; William. Fong; Andrew S. Friedman; Christa Gall; N. Gehrels; J. Hjorth

The double explosion of SN 2009ip in 2012 raises questions about our understanding of the late stages of massive star evolution. Here we present a comprehensive study of SN 2009ip during its remarkable rebrightenings. High-cadence photometric and spectroscopic observations from the GeV to the radio band obtained from a variety of ground-based and space facilities (including the Very Large Array, Swift, Fermi, Hubble Space Telescope, and XMM) constrain SN 2009ip to be a low energy (E similar to 1050 erg for an ejecta mass similar to 0.5 M-circle dot) and asymmetric explosion in a complex medium shaped by multiple eruptions of the restless progenitor star. Most of the energy is radiated as a result of the shock breaking out through a dense shell of material located at similar to 5 x 10(14) cm with M similar to 0.1 M-circle dot, ejected by the precursor outburst similar to 40 days before the major explosion. We interpret the NIR excess of emission as signature of material located further out, the origin of which has to be connected with documented mass-loss episodes in the previous years. Our modeling predicts bright neutrino emission associated with the shock break-out if the cosmic-ray energy is comparable to the radiated energy. We connect this phenomenology with the explosive ejection of the outer layers of the massive progenitor star, which later interacted with material deposited in the surroundings by previous eruptions. Future observations will reveal if the massive luminous progenitor star survived. Irrespective of whether the explosion was terminal, SN 2009ip brought to light the existence of new channels for sustained episodic mass loss, the physical origin of which has yet to be identified.


The Astrophysical Journal | 2014

Hydrogen-Poor Superluminous Supernovae and Long-Duration Gamma-Ray Bursts Have Similar Host Galaxies

R. Lunnan; Ryan Chornock; Edo Berger; Tanmoy Laskar; William. Fong; Armin Rest; Nathan Edward Sanders; Peter M. Challis; Maria Rebecca Drout; Ryan J. Foley; M. E. Huber; Robert P. Kirshner; C. Leibler; G. H. Marion; M. McCrum; D. Milisavljevic; Gautham S. Narayan; D. Scolnic; S. J. Smartt; K. W. Smith; Alicia M. Soderberg; John L. Tonry; W. S. Burgett; K. C. Chambers; H. Flewelling; Klaus-Werner Hodapp; Nick Kaiser; E. A. Magnier; P. A. Price; R. J. Wainscoat

We present optical spectroscopy and optical/near-IR photometry of 31 host galaxies of hydrogen-poor superluminous supernovae (SLSNe), including 15 events from the Pan-STARRS1 Medium Deep Survey. Our sample spans the redshift range 0.1 ~ -17.3 mag), low stellar mass ( ~ 2 x 10^8 M_sun) population, with a high median specific star formation rate ( ~ 2 Gyr^-1). The median metallicity of our spectroscopic sample is low, 12 + log(O/H}) ~ 8.35 ~ 0.45 Z_sun, although at least one host galaxy has solar metallicity. The host galaxies of H-poor SLSNe are statistically distinct from the hosts of GOODS core-collapse SNe (which cover a similar redshift range), but resemble the host galaxies of long-duration gamma-ray bursts (LGRBs) in terms of stellar mass, SFR, sSFR and metallicity. This result indicates that the environmental causes leading to massive stars forming either SLSNe or LGRBs are similar, and in particular that SLSNe are more effectively formed in low metallicity environments. We speculate that the key ingredient is large core angular momentum, leading to a rapidly-spinning magnetar in SLSNe and an accreting black hole in LGRBs.


The Astrophysical Journal | 2013

The Ultraviolet-Bright, Slowly Declining Transient PS1-11af as a Partial Tidal Disruption Event

Ryan Chornock; Edo Berger; S. Gezari; B. A. Zauderer; Armin Rest; Laura Chomiuk; Atish Kamble; Alicia M. Soderberg; Ian Czekala; Jason A. Dittmann; Maria Rebecca Drout; Ryan J. Foley; William. Fong; M. Huber; Robert P. Kirshner; A. Lawrence; R. Lunnan; G. H. Marion; Gautham S. Narayan; Adam G. Riess; Kathy Roth; Nathan Edward Sanders; D. Scolnic; S. J. Smartt; K. W. Smith; Christopher W. Stubbs; John L. Tonry; W. S. Burgett; K. C. Chambers; H. Flewelling

We present the Pan-STARRS1 discovery of the long-lived and blue transient PS1-11af, which was also detected by Galaxy Evolution Explorer with coordinated observations in the near-ultraviolet (NUV) band. PS1-11af is associated with the nucleus of an early type galaxy at redshift z = 0.4046 that exhibits no evidence for star formation or active galactic nucleus activity. Four epochs of spectroscopy reveal a pair of transient broad absorption features in the UV on otherwise featureless spectra. Despite the superficial similarity of these features to P-Cygni absorptions of supernovae (SNe), we conclude that PS1-11af is not consistent with the properties of known types of SNe. Blackbody fits to the spectral energy distribution are inconsistent with the cooling, expanding ejecta of a SN, and the velocities of the absorption features are too high to represent material in homologous expansion near a SN photosphere. However, the constant blue colors and slow evolution of the luminosity are similar to previous optically selected tidal disruption events (TDEs). The shape of the optical light curve is consistent with models for TDEs, but the minimum accreted mass necessary to power the observed luminosity is only ~0.002 M ☉, which points to a partial disruption model. A full disruption model predicts higher bolometric luminosities, which would require most of the radiation to be emitted in a separate component at high energies where we lack observations. In addition, the observed temperature is lower than that predicted by pure accretion disk models for TDEs and requires reprocessing to a constant, lower temperature. Three deep non-detections in the radio with the Very Large Array over the first two years after the event set strict limits on the production of any relativistic outflow comparable to Swift J1644+57, even if off-axis.


The Astrophysical Journal | 2014

Rapidly-Evolving and Luminous Transients from Pan-STARRS1

Maria Rebecca Drout; Ryan Chornock; Alicia M. Soderberg; Nathan Edward Sanders; R. McKinnon; Armin Rest; Ryan J. Foley; D. Milisavljevic; Raffaella Margutti; Edo Berger; Michael L. Calkins; William. Fong; S. Gezari; M. Huber; E. Kankare; Robert P. Kirshner; C. Leibler; R. Lunnan; Seppo Mattila; G. H. Marion; Gautham S. Narayan; A. G. Riess; Kathy Roth; D. Scolnic; S. J. Smartt; John L. Tonry; W. S. Burgett; K. C. Chambers; K. W. Hodapp; Robert Jedicke

In the past decade, several rapidly evolving transients have been discovered whose timescales and luminosities are not easily explained by traditional supernovae (SNe) models. The sample size of these objects has remained small due, at least in part, to the challenges of detecting short timescale transients with traditional survey cadences. Here we present the results from a search within the Pan-STARRS1 Medium Deep Survey (PS1-MDS) for rapidly evolving and luminous transients. We identify 10 new transients with a time above half-maximum (t 1/2) of less than 12 days and –16.5 > M > –20 mag. This increases the number of known events in this region of SN phase space by roughly a factor of three. The median redshift of the PS1-MDS sample is z = 0.275 and they all exploded in star-forming galaxies. In general, the transients possess faster rise than decline timescale and blue colors at maximum light (g P1 – r P1 lsim –0.2). Best-fit blackbodies reveal photospheric temperatures/radii that expand/cool with time and explosion spectra taken near maximum light are dominated by a blue continuum, consistent with a hot, optically thick, ejecta. We find it difficult to reconcile the short timescale, high peak luminosity (L > 1043 erg s–1), and lack of UV line blanketing observed in many of these transients with an explosion powered mainly by the radioactive decay of 56Ni. Rather, we find that many are consistent with either (1) cooling envelope emission from the explosion of a star with a low-mass extended envelope that ejected very little (<0.03 M ☉) radioactive material, or (2) a shock breakout within a dense, optically thick, wind surrounding the progenitor star. After calculating the detection efficiency for objects with rapid timescales in the PS1-MDS we find a volumetric rate of 4800-8000 events yr–1 Gpc–3 (4%-7% of the core-collapse SN rate at z = 0.2).


The Astrophysical Journal | 2014

NO X-RAYS FROM THE VERY NEARBY TYPE Ia SN 2014J: CONSTRAINTS ON ITS ENVIRONMENT

Raffaella Margutti; Jerod T. Parrent; Atish Kamble; Alicia M. Soderberg; Ryan J. Foley; D. Milisavljevic; Maria Rebecca Drout; Robert P. Kirshner

Deep X-ray observations of the post-explosion environment around the very nearby Type Ia SN 2014J (d{sub L} = 3.5 Mpc) reveal no X-ray emission down to a luminosity L{sub x} < 7 × 10{sup 36} erg s{sup –1} (0.3-10 keV) at δt ∼ 20 days after the explosion. We interpret this limit in the context of inverse Compton emission from upscattered optical photons by the supernova shock and constrain the pre-explosion mass-loss rate of the stellar progenitor system to be M-dot <10{sup −9} M{sub ⊙} yr{sup −1} (for wind velocity v{sub w} = 100 km s{sup –1}). Alternatively, the SN shock might be expanding into a uniform medium with density n{sub CSM} < 3 cm{sup –3}. These results rule out single-degenerate (SD) systems with steady mass loss until the terminal explosion and constrain the fraction of transferred material lost at the outer Lagrangian point to be ≤1%. The allowed progenitors are (1) white dwarf-white dwarf progenitors, (2) SD systems with unstable hydrogen burning experiencing recurrent nova eruptions with recurrence time t < 300 yr, and (3) stars where the mass loss ceases before the explosion.


Monthly Notices of the Royal Astronomical Society | 2014

The superluminous supernova PS1-11ap: bridging the gap between low and high redshift

M. McCrum; S. J. Smartt; R. Kotak; Armin Rest; A. Jerkstrand; C. Inserra; Steven A. Rodney; Ting-Wan Chen; D. A. Howell; M. Huber; Andrea Pastorello; John L. Tonry; Fabio Bresolin; R.-P. Kudritzki; Ryan Chornock; Edo Berger; K. W. Smith; M. T. Botticella; Ryan J. Foley; M. Fraser; D. Milisavljevic; M. Nicholl; Adam G. Riess; Christopher W. Stubbs; S. Valenti; William Michael Wood-Vasey; D. Wright; D. R. Young; Maria Rebecca Drout; Ian Czekala

We present optical photometric and spectroscopic coverage of the superluminous supernova (SLSN) PS1-11ap, discovered with the Pan-STARRS1 Medium Deep Survey at z = 0.524. This intrinsically blue transient rose slowly to reach a peak magnitude ofMu =− 21.4 mag and bolometric luminosity of 8 × 10 43 erg s −1 before settling on to a relatively shallow gradient of decline. The observed decline is significantly slower than those of the SLSNe-Ic which have been the focus of much recent attention. Spectroscopic similarities with the lower redshift SN2007bi and a decline rate similar to 56 Co decay time-scale initially indicated that this transient could be a candidate for a pair instability supernova (PISN) explosion. Overall the transient appears quite similar to SN2007bi and the lower redshift object PTF12dam. The extensive data set, from 30 d before peak to 230 d after, allows a detailed and quantitative comparison with published models of PISN explosions. We find that the PS1-11ap data do not match these model explosion parameters well, supporting the recent claim that these SNe are not pair instability explosions. We show that PS1-11ap has many features in common with the faster declining SLSNe-Ic, and the light-curve evolution can also be quantitatively explained by the magnetar spin-down model. At a redshift of z = 0.524, the observer-frame optical coverage provides comprehensive rest-frame UV data and allows us to compare it with the SLSNe recently found at high redshifts between z = 2 and 4. While these high-z explosions


The Astrophysical Journal | 2013

GRB 130606A as a Probe of the Intergalactic Medium and the Interstellar Medium in a Star-forming Galaxy in the First Gyr After the Big Bang

Ryan Chornock; Edo Berger; Derek B. Fox; R. Lunnan; Maria Rebecca Drout; Wen-fai Fong; Tanmoy Laskar; Katherine C. Roth

We present high signal-to-noise ratio Gemini and MMT spectroscopy of the optical afterglow of the gamma-ray burst (GRB) 130606A at redshift z = 5.913, discovered by Swift. This is the first high-redshift GRB afterglow to have spectra of comparable quality to those of z ≈ 6 quasars. The data exhibit a smooth continuum at near-infrared wavelengths that is sharply cut off blueward of 8410 A due to absorption from Lyα at redshift z ≈ 5.91, with some flux transmitted through the Lyα forest between 7000 and 7800 A. We use column densities inferred from metal absorption lines to constrain the metallicity of the host galaxy between a lower limit of [Si/H] –1.7 and an upper limit of [S/H] –0.5 set by the non-detection of S II absorption. We demonstrate consistency between the dramatic evolution in the transmission fraction of Lyα seen in this spectrum over the redshift range z = 4.9-5.85 with that previously measured from observations of high-redshift quasars. There is an extended redshift interval of Δz = 0.12 in the Lyα forest at z = 5.77 with no detected transmission, leading to a 3σ upper limit on the mean Lyα transmission fraction of 0.2% (or (Lyα) > 6.4). This is comparable to the lowest-redshift Gunn-Peterson troughs found in quasar spectra. Some Lyβ and Lyγ transmission is detected in this redshift window, indicating that it is not completely opaque, and hence that the intergalactic medium (IGM) is nonetheless mostly ionized at these redshifts. We set a 2σ upper limit of 0.11 on the neutral fraction of the IGM at the redshift of the GRB from the lack of a Lyα red damping wing, assuming a model with a constant neutral density. GRB 130606A thus for the first time realizes the promise of GRBs as probes of the first galaxies and cosmic reionization.


The Astrophysical Journal | 2016

SN 2015bn: A DETAILED MULTI-WAVELENGTH VIEW OF A NEARBY SUPERLUMINOUS SUPERNOVA

M. Nicholl; Edo Berger; S. J. Smartt; Raffaella Margutti; Atish Kamble; K. D. Alexander; T.-W. Chen; C. Inserra; I. Arcavi; P. K. Blanchard; R. Cartier; K. C. Chambers; Michael J. Childress; Ryan Chornock; P. S. Cowperthwaite; Maria Rebecca Drout; H. Flewelling; M. Fraser; Avishay Gal-Yam; L. Galbany; J. Harmanen; T. W.-S. Holoien; G. Hosseinzadeh; D. A. Howell; M. Huber; A. Jerkstrand; E. Kankare; C. S. Kochanek; Z.-Y. Lin; R. Lunnan

We present observations of SN 2015bn (= PS15ae = CSS141223-113342+004332 = MLS150211-113342+004333), a Type I superluminous supernova (SLSN) at redshift


The Astrophysical Journal | 2014

Relativistic supernovae have shorter-lived central engines or more extended progenitors: The case of SN 2012ap

Raffaella Margutti; D. Milisavljevic; Alicia M. Soderberg; C. Guidorzi; Brian J. Morsony; Nathan Edward Sanders; Sayan Chakraborti; A. Ray; Atish Kamble; Maria Rebecca Drout; Jerod T. Parrent; Ashley Zauderer; Laura Chomiuk

z=0.1136

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Ryan J. Foley

University of California

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R. Lunnan

California Institute of Technology

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