R. R. Laher
California Institute of Technology
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Featured researches published by R. R. Laher.
Nature | 2013
Eran O. Ofek; S. B. Cenko; Mansi M. Kasliwal; Avishay Gal-Yam; S. R. Kulkarni; I. Arcavi; Lars Bildsten; J. S. Bloom; Assaf Horesh; Dale Andrew Howell; A. V. Filippenko; R. R. Laher; D. Murray; Ehud Nakar; P. Nugent; Jeffrey M. Silverman; Nir J. Shaviv; Jason A. Surace; O. Yaron
Some observations suggest that very massive stars experience extreme mass-loss episodes shortly before they explode as supernovae, as do several models. Establishing a causal connection between these mass-loss episodes and the final explosion would provide a novel way to study pre-supernova massive-star evolution. Here we report observations of a mass-loss event detected 40 days before the explosion of the type IIn supernova SN 2010mc (also known as PTF 10tel). Our photometric and spectroscopic data suggest that this event is a result of an energetic outburst, radiating at least 6 × 1047 erg of energy and releasing about 10−2 solar masses of material at typical velocities of 2,000 km s−1. The temporal proximity of the mass-loss outburst and the supernova explosion implies a causal connection between them. Moreover, we find that the outburst luminosity and velocity are consistent with the predictions of the wave-driven pulsation model, and disfavour alternative suggestions.
The Astrophysical Journal | 2000
Derek L. Buzasi; J. Catanzarite; R. R. Laher; T. Conrow; D. L. Shupe; Thomas N. Gautier; Tobias J. Kreidl; D. Everett
We have used the star camera on the Wide-Field Infrared Explorer satellite to observe the K0 III star α UMa, and we report the apparent detection of 10 oscillation modes. The lowest frequency mode is at 1.82 μHz, and it appears to be the fundamental mode. The mean spacing between the mode frequencies is 2.94 μHz, which implies that all detected modes are radial. The mode frequencies are consistent with the physical parameters of a K0 III star, if we assume that only radial modes are excited. Mode amplitudes are 100-400 μmag, which is consistent with the scaling relation of Kjeldsen & Bedding.
The Astrophysical Journal | 2013
Eran O. Ofek; Derek B. Fox; S. B. Cenko; Orly Gnat; Dale A. Frail; Assaf Horesh; A. Corsi; Robert Michael Quimby; N. Gehrels; S. R. Kulkarni; Avishay Gal-Yam; P. Nugent; Ofer Yaron; A. V. Filippenko; Mansi M. Kasliwal; Lars Bildsten; J. S. Bloom; Dovi Poznanski; Iair Arcavi; R. R. Laher; David Levitan; Branimir Sesar; Jason A. Surace
The optical light curve of some supernovae (SNe) may be powered by the outward diffusion of the energy deposited by the explosion shock (so-called shock breakout) in optically thick (� > 30) circumstellar matter (CSM). Recently, it was shown that the radiation-mediated and -dominated shock in an optically thick wind must transform into a collisionless shock and can produce hard Xrays. The X-rays are expected to peak at late times, relative to maximum visible light. Here we report on a search, using Swift-XRT and Chandra, for X-ray emission from 28 SNe that belong to classes whose progenitors are suspected to be embedded in dense CSM. Our sample includes 19 type-IIn SNe, one type-Ibn SN and eight hydrogen-poor super-luminous SNe (SLSN-I; SN2005ap like). Two SNe (SN2006jc and SN2010jl) have X-ray properties that are roughly consistent with the expectation for X-rays from a collisionless shock in optically thick CSM. Therefore, we suggest that their optical light curves are powered by shock breakout in CSM. We show that two other events (SN2010al and SN2011ht) were too X-ray bright during the SN maximum optical light to be explained by the shock breakout model. We conclude that the light curves of some, but not all, type-IIn/Ibn SNe are powered by shock breakout in CSM. For the rest of the SNe in our sample, including all the SLSN-I events, our X-ray limits are not deep enough and were typically obtained at too early times (i.e., near the SN maximum light) to conclude about their nature. Late time X-ray observations are required in order to further test if these SNe are indeed embedded in dense CSM. We review the conditions required for a shock breakout in a wind profile. We argue that the time scale, relative to maximum light, for the SN to peak in X-rays is a probe of the column density and the density profile above the shock region. The optical light curves of SNe, for which the X-ray emission peaks at late times, are likely powered by the diffusion of shock energy from a dense CSM. We note that if the CSM density profile falls faster than a constant-rate wind density profile, then X-rays may escape at earlier times than estimated for the wind profile case. Furthermore, if the CSM have a region in which the density profile is very steep, relative to a steady wind density profile, or the CSM is neutral, then the radio free-free absorption may be low enough, and radio emission may be detected. Subject headings: stars: mass-loss — supernovae: general — supernovae: individual
Monthly Notices of the Royal Astronomical Society | 2014
Y.-C. Pan; M. Sullivan; K. Maguire; Isobel M. Hook; Peter E. Nugent; D. A. Howell; Iair Arcavi; J. Botyanszki; S. B. Cenko; J. DeRose; H. K. Fakhouri; Avishay Gal-Yam; E. Y. Hsiao; S. R. Kulkarni; R. R. Laher; C. Lidman; J. Nordin; Emma S. Walker; Dong-Ling Xu
We present spectroscopic observations of the host galaxies of 82 low-redshift Type Ia supernovae (SNe Ia) discovered by the Palomar Transient Factory. We determine star formation rates, gas-phase/stellar metallicities, and stellar masses and ages of these objects. As expected, strong correlations between the SN Ia light-curve width (stretch) and the host age/mass/metallicity are found: fainter, faster declining events tend to be hosted by older/massive/metal-rich galaxies. There is some evidence that redder SNe Ia explode in higher metallicity galaxies, but we found no relation between the SN colour and host galaxy extinction based on the Balmer decrement, suggesting that the colour variation of these SNe does not primarily arise from this source. SNe Ia in higher mass/metallicity galaxies also appear brighter after stretch/colour corrections than their counterparts in lower mass hosts, and the stronger correlation is with gas-phase metallicity suggesting this may be the more important variable. We also compared the host stellar mass distribution to that in galaxy-targeted SN surveys and the high-redshift untargeted Supernova Legacy Survey (SNLS). SNLS has many more low-mass galaxies, while the targeted searches have fewer. This can be explained by an evolution in the galaxy stellar mass function, coupled with an SN delay-time distribution proportional to t^−1. Finally, we found no significant difference in the mass–metallicity relation of our SN Ia hosts compared to field galaxies, suggesting any metallicity effect on the SN Ia rate is small.
Monthly Notices of the Royal Astronomical Society | 2016
Maria Charisi; I. Bartos; Zoltan Haiman; Adrian M. Price-Whelan; Matthew J. Graham; Eric C. Bellm; R. R. Laher; S. Márka
Supermassive black hole binaries (SMBHBs) at sub-parsec separations should be common in galactic nuclei, as a result of frequent galaxy mergers. Hydrodynamical simulations of circum-binary discs predict strong periodic modulation of the mass accretion rate on time-scales comparable to the orbital period of the binary. As a result, SMBHBs may be recognized by the periodic modulation of their brightness. We conducted a statistical search for periodic variability in a sample of 35 383 spectroscopically confirmed quasars in the photometric data base of the Palomar Transient Factory (PTF). We analysed Lomb–Scargle periodograms and assessed the significance of our findings by modelling each individual quasars variability as a damped random walk (DRW). We identified 50 quasars with significant periodicity beyond the DRW model, typically with short periods of a few hundred days. We find 33 of these to remain significant after a re-analysis of their periodograms including additional optical data from the intermediate-PTF and the Catalina Real-Time Transient Survey. Assuming that the observed periods correspond to the redshifted orbital periods of SMBHBs, we conclude that our findings are consistent with a population of unequal-mass SMBHBs, with a typical mass ratio as low as q ≡ M_2/M_1 ≈ 0.01.
The Astrophysical Journal | 2005
Derek L. Buzasi; H. Bruntt; Timothy R. Bedding; Alon Retter; Hans Kjeldsen; Heather L. Preston; W.J. Mandeville; J. C. Suárez; J. Catanzarite; T. Conrow; R. R. Laher
We present an analysis of observations of the bright star Altair (α Aql) obtained using the star camera on the Wide Field Infrared Explorer (WIRE) satellite. Although Altair lies within the δ Scuti instability strip, previous observations have not revealed the presence of oscillations. However, the WIRE observations show Altair to be a low-amplitude (Δm < 1 parts per thousand [ppt]) δ Scuti star with at least seven modes present.
Monthly Notices of the Royal Astronomical Society | 2013
S. Hachinger; Paolo A. Mazzali; Richard S. Ellis; K. Maguire; Avishay Gal-Yam; D. A. Howell; P. Nugent; E. Baron; Jeff Cooke; Iair Arcavi; D. F. Bersier; Benjamin E. P. Dilday; P. A. James; Mansi M. Kasliwal; S. R. Kulkarni; Eran O. Ofek; R. R. Laher; Jerod T. Parrent; Jason A. Surace; Ofer Yaron; Emma S. Walker
Radiative transfer studies of Type Ia supernovae (SNe Ia) hold the promise of constraining both the density profile of the SN ejecta and its stratification by element abundance which, in turn, may discriminate between different explosion mechanisms and progenitor classes. Here we analyse the Type Ia SN 2010jn (PTF10ygu) in detail, presenting and evaluating near-ultraviolet (near-UV) spectra from the Hubble Space Telescope and ground-based optical spectra and light curves. SN 2010jn was discovered by the Palomar Transient Factory (PTF) 15 d before maximum light, allowing us to secure a time series of four near-UV spectra at epochs from −10.5 to +4.8 d relative to B-band maximum. The photospheric near-UV spectra are excellent diagnostics of the iron-group abundances in the outer layers of the ejecta, particularly those at very early times. Using the method of ‘Abundance Tomography’ we derive iron-group abundances in SN 2010jn with a precision better than in any previously studied SN Ia. Optimum fits to the data can be obtained if burned material is present even at high velocities, including significant mass fractions of iron-group elements. This is consistent with the slow decline rate (or high ‘stretch’) of the light curve of SN 2010jn, and consistent with the results of delayed-detonation models. Early-phase UV spectra and detailed time-dependent series of further SNe Ia offer a promising probe of the nature of the SN Ia mechanism.
Monthly Notices of the Royal Astronomical Society | 2014
T. Hovatta; Vasiliki Pavlidou; O. G. King; Ashish A. Mahabal; Branimir Sesar; R. Dancikova; S. G. Djorgovski; Andrew J. Drake; R. R. Laher; David Levitan; W. Max-Moerbeck; Eran O. Ofek; T. J. Pearson; Thomas A. Prince; Anthony C. S. Readhead; J. L. Richards; Jason A. Surace
We use optical data from the Palomar Transient Factory (PTF) and the Catalina Real-Time Transient Survey (CRTS) to study the variability of γ-ray detected and non-detected objects in a large population of active galactic nuclei (AGN) selected from the Candidate Gamma-Ray Blazar Survey and Fermi Gamma-Ray Space Telescope catalogs. Our samples include 714 sources with PTF data and 1244 sources with CRTS data. We calculate the intrinsic modulation index to quantify the optical variability amplitude in these samples. We find the γ-ray detected objects to be more variable than the non-detected ones. The flat spectrum radio quasars (FSRQs) are more variable than the BL Lac objects in our sample, but the significance of the difference depends on the sample used. When dividing the objects based on their synchrotron peak frequency, we find the low synchrotron peaked (LSP) objects to be significantly more variable than the high synchrotron peaked (HSP) ones, explaining the difference between the FSRQs and BL Lacs. This could be due to the LSPs being observed near their electron energy peak, while in the HSPs the emission is caused by lower energy electrons, which cool more slowly. We also find a significant correlation between the optical and γ-ray fluxes that is stronger in the HSP BL Lacs than in the FSRQs. The FSRQs in our sample are also more Compton dominated than the HSP BL Lacs. These findings are consistent with models where the γ-ray emission of HSP objects is produced by the synchrotron self-Compton mechanism, while the LSP objects need an additional external Compton component that increases the scatter in the flux-flux correlation.
Nature Physics | 2017
O. Yaron; Daniel A. Perley; Avishay Gal-Yam; Jose H. Groh; Assaf Horesh; Eran O. Ofek; S. R. Kulkarni; Jesper Sollerman; Claes Fransson; Adam Rubin; P. Szabo; N. Sapir; F. Taddia; S. B. Cenko; S. Valenti; I. Arcavi; D. A. Howell; Mansi M. Kasliwal; Paul M. Vreeswijk; Danny Khazov; Ori D. Fox; Y. Cao; Orly Gnat; Patrick L. Kelly; Peter E. Nugent; A. V. Filippenko; R. R. Laher; Przemyslaw Remigiusz Wozniak; W. H. Lee; Umaa Rebbapragada
With the advent of new wide-field, high-cadence optical transient surveys, our understanding of the diversity of core-collapse supernovae has grown tremendously in the last decade. However, the pre-supernova evolution of massive stars, which sets the physical backdrop to these violent events, is theoretically not well understood and difficult to probe observationally. Here we report the discovery of the supernova iPTF 13dqy = SN 2013fs a mere ~3 h after explosion. Our rapid follow-up observations, which include multiwavelength photometry and extremely early (beginning at ~6 h post-explosion) spectra, map the distribution of material in the immediate environment (≲10^(15) cm) of the exploding star and establish that it was surrounded by circumstellar material (CSM) that was ejected during the final ~1 yr prior to explosion at a high rate, around 10^(−3) solar masses per year. The complete disappearance of flash-ionized emission lines within the first several days requires that the dense CSM be confined to within ≲10^(15) cm, consistent with radio non-detections at 70–100 days. The observations indicate that iPTF 13dqy was a regular type II supernova; thus, the finding that the probable red supergiant progenitor of this common explosion ejected material at a highly elevated rate just prior to its demise suggests that pre-supernova instabilities may be common among exploding massive stars.
The Astrophysical Journal | 2016
Mansi M. Kasliwal; S. B. Cenko; L. P. Singer; A. Corsi; Y. Cao; Tom A. Barlow; Varun Bhalerao; Eric C. Bellm; David O. Cook; G. Duggan; Raphael Ferretti; Dale A. Frail; Assaf Horesh; R. Kendrick; S. R. Kulkarni; R. Lunnan; N. Palliyaguru; R. R. Laher; Frank J. Masci; I. Manulis; Adam A. Miller; Peter E. Nugent; Daniel A. Perley; Thomas A. Prince; Robert Michael Quimby; J. Rana; Umaa Rebbapragada; Branimir Sesar; A. Singhal; Jason A. Surace
The intermediate Palomar Transient Factory (iPTF) autonomously responded to and promptly tiled the error region of the first gravitational-wave event GW150914 to search for an optical counterpart. Only a small fraction of the total localized region was immediately visible in the northern night sky, due both to Sun-angle and elevation constraints. Here, we report on the transient candidates identified and rapid follow-up undertaken to determine the nature of each candidate. Even in the small area imaged of 126 deg^2, after extensive filtering, eight candidates were deemed worthy of additional follow-up. Within two hours, all eight were spectroscopically classified by the Keck II telescope. Curiously, even though such events are rare, one of our candidates was a superluminous supernova. We obtained radio data with the Jansky Very Large Array and X-ray follow-up with the Swift satellite for this transient. None of our candidates appear to be associated with the gravitational-wave trigger, which is unsurprising given that GW150914 came from the merger of two stellar-mass black holes. This end-to-end discovery and follow-up campaign bodes well for future searches in this post-detection era of gravitational waves.