Eric C. Bellm
California Institute of Technology
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Featured researches published by Eric C. Bellm.
The Astrophysical Journal | 2013
Fiona A. Harrison; William W. Craig; Finn Erland Christensen; Charles J. Hailey; William W. Zhang; Steven E. Boggs; Daniel Stern; W. Rick Cook; Karl Forster; Paolo Giommi; Brian W. Grefenstette; Yunjin Kim; Takao Kitaguchi; Jason E. Koglin; Kristin K. Madsen; Peter H. Mao; Hiromasa Miyasaka; Kaya Mori; Matteo Perri; Michael J. Pivovaroff; S. Puccetti; V. Rana; Niels Jørgen Stenfeldt Westergaard; Jason Willis; Andreas Zoglauer; Hongjun An; Matteo Bachetti; Eric C. Bellm; Varun Bhalerao; Nicolai F. Brejnholt
The Nuclear Spectroscopic Telescope Array (NuSTAR) is a National Aeronautics and Space Administration (NASA) Small Explorer mission that carried the first focusing hard X-ray (6-79 keV) telescope into orbit. It was launched on a Pegasus rocket into a low-inclination Earth orbit on June 13, 2012, from Reagan Test Site, Kwajalein Atoll. NuSTAR will carry out a two-year primary science mission. The NuSTAR observatory is composed of the X-ray instrument and the spacecraft. The NuSTAR spacecraft is three-axis stabilized with a single articulating solar array based on Orbital Sciences Corporations LEOStar-2 design. The NuSTAR science instrument consists of two co-aligned grazing incidence optics focusing on to two shielded solid state CdZnTe pixel detectors. The instrument was launched in a compact, stowed configuration, and after launch, a 10-meter mast was deployed to achieve a focal length of 10.15 m. The NuSTAR instrument provides sub-arcminute imaging with excellent spectral resolution over a 12-arcminute field of view. The NuSTAR observatory will be operated out of the Mission Operations Center (MOC) at UC Berkeley. Most science targets will be viewed for a week or more. The science data will be transferred from the UC Berkeley MOC to a Science Operations Center (SOC) located at the California Institute of Technology (Caltech). In this paper, we will describe the mission architecture, the technical challenges during the development phase, and the post-launch activities.
Science | 2017
Mansi M. Kasliwal; Ehud Nakar; L. P. Singer; David L. Kaplan; David O. Cook; A. Van Sistine; Ryan M. Lau; C. Fremling; O. Gottlieb; Jacob E. Jencson; S. M. Adams; U. Feindt; Kenta Hotokezaka; S. Ghosh; Daniel A. Perley; Po-Chieh Yu; Tsvi Piran; J. R. Allison; G. C. Anupama; A. Balasubramanian; Keith W. Bannister; John Bally; J. Barnes; Sudhanshu Barway; Eric C. Bellm; V. Bhalerao; D. Bhattacharya; N. Blagorodnova; J. S. Bloom; P. R. Brady
GROWTH observations of GW170817 The gravitational wave event GW170817 was caused by the merger of two neutron stars (see the Introduction by Smith). In three papers, teams associated with the GROWTH (Global Relay of Observatories Watching Transients Happen) project present their observations of the event at wavelengths from x-rays to radio waves. Evans et al. used space telescopes to detect GW170817 in the ultraviolet and place limits on its x-ray flux, showing that the merger generated a hot explosion known as a blue kilonova. Hallinan et al. describe radio emissions generated as the explosion slammed into the surrounding gas within the host galaxy. Kasliwal et al. present additional observations in the optical and infrared and formulate a model for the event involving a cocoon of material expanding at close to the speed of light, matching the data at all observed wavelengths. Science, this issue p. 1565, p. 1579, p. 1559; see also p. 1554 Observations of a binary neutron star merger at multiple wavelengths can be explained by an off-axis relativistic cocoon model. Merging neutron stars offer an excellent laboratory for simultaneously studying strong-field gravity and matter in extreme environments. We establish the physical association of an electromagnetic counterpart (EM170817) with gravitational waves (GW170817) detected from merging neutron stars. By synthesizing a panchromatic data set, we demonstrate that merging neutron stars are a long-sought production site forging heavy elements by r-process nucleosynthesis. The weak gamma rays seen in EM170817 are dissimilar to classical short gamma-ray bursts with ultrarelativistic jets. Instead, we suggest that breakout of a wide-angle, mildly relativistic cocoon engulfing the jet explains the low-luminosity gamma rays, the high-luminosity ultraviolet-optical-infrared, and the delayed radio and x-ray emission. We posit that all neutron star mergers may lead to a wide-angle cocoon breakout, sometimes accompanied by a successful jet and sometimes by a choked jet.
The Astrophysical Journal | 2014
Eran O. Ofek; Andreas Zoglauer; Steven E. Boggs; Stephen P. Reynolds; Chris L. Fryer; Fiona A. Harrison; S. Bradley Cenko; S. R. Kulkarni; Avishay Gal-Yam; Iair Arcavi; Eric C. Bellm; Joshua S. Bloom; Finn Erland Christensen; William W. Craig; Wesley Even; Alexei V. Filippenko; Brian W. Grefenstette; Charles J. Hailey; Russ R. Laher; Kristin K. Madsen; Ehud Nakar; Peter E. Nugent; Daniel Stern; M. Sullivan; Jason A. Surace; William W. Zhang
Some supernovae (SNe) may be powered by the interaction of the SN ejecta with a large amount of circumstellar matter (CSM). However, quantitative estimates of the CSM mass around such SNe are missing when the CSM material is optically thick. Specifically, current estimators are sensitive to uncertainties regarding the CSM density profile and the ejecta velocity. Here we outline a method to measure the mass of the optically thick CSM around such SNe. We present new visible-light and X-ray observations of SN 2010jl (PTF 10aaxf), including the first detection of an SN in the hard X-ray band using NuSTAR. The total radiated luminosity of SN 2010jl is extreme—at least 9 × 10^50 erg. By modeling the visible-light data, we robustly show that the mass of the circumstellar material within ~10^16 cm of the progenitor of SN 2010jl was in excess of 10 M_☉. This mass was likely ejected tens of years prior to the SN explosion. Our modeling suggests that the shock velocity during shock breakout was ~6000 km s^–1, decelerating to ~2600 km s^–1 about 2 yr after maximum light. Furthermore, our late-time NuSTAR and XMM spectra of the SN presumably provide the first direct measurement of SN shock velocity 2 yr after the SN maximum light—measured to be in the range of 2000-4500 km s^–1 if the ions and electrons are in equilibrium, and ≳ 2000 km s^–1 if they are not in equilibrium. This measurement is in agreement with the shock velocity predicted by our modeling of the visible-light data. Our observations also show that the average radial density distribution of the CSM roughly follows an r^–2 law. A possible explanation for the ≳ 10 M_☉ of CSM and the wind-like profile is that they are the result of multiple pulsational pair instability events prior to the SN explosion, separated from each other by years.
The Astrophysical Journal | 2013
Branimir Sesar; Carl J. Grillmair; Judith G. Cohen; Eric C. Bellm; Varun Bhalerao; David Levitan; Russ R. Laher; Eran O. Ofek; Jason A. Surace; Sumin Tang; Adam Waszczak; S. R. Kulkarni; Thomas A. Prince
We report positions, velocities and metallicities of 50ab-type RR Lyrae (RRab) stars observed in the vicinity of the Orphan stellar stream. Using about 30 RRab stars classied as being likely members of the Orphan stream, we study the metallicity and the spatial extent of the stream. We nd that RRab stars in the Orphan stream have a wide range of metallicities, from -1.5 dex to -2.7 dex. The average metallicity of the stream is -2.1 dex, identical to the value obtained by Newberg et al. (2010) using blue horizontal branch stars. We nd that the most distant parts of the stream (40-50 kpc from the Sun) are about 0.3 dex more metal-poor than the closer parts (within 30 kpc), suggesting a possible metallicity gradient along the stream’s length. We have extended the previous studies and have mapped the stream up to 55 kpc from the Sun. Even after a careful search, we did not identify any more distant RRab stars that could plausibly be members of the Orphan stream. If conrmed with other tracers, this result would indicate a detection of the end of the leading arm of the stream. We have compared the distances of Orphan stream RRab stars with the best-t orbits obtained by Newberg et al. (2010). We nd that model 6 of Newberg et al. (2010) cannot explain the distances of the most remote Orphan stream RRab stars, and conclude that the best t to distances of Orphan stream RRab stars and to the local circular velocity is provided by potentials where the total mass of the Galaxy within 60 kpc is M60 2:7 10 11 M , or about 60% of the mass found by previous studies. More extensive modelling that would consider non-spherical potentials and the possibility of misalignment between the stream and the orbit, is highly encouraged.
The Astrophysical Journal | 2014
Shriharsh P. Tendulkar; Chengwei Yang; Hongjun An; Victoria M. Kaspi; Anne M. Archibald; C. G. Bassa; Eric C. Bellm; S. Bogdanov; Fiona A. Harrison; J. W. T. Hessels; G. H. Janssen; A. G. Lyne; Alessandro Patruno; B. W. Stappers; Daniel Stern; John A. Tomsick; Steven E. Boggs; Deepto Chakrabarty; Finn Erland Christensen; William W. Craig; C. Hailey; William W. Zhang
We report NuSTAR observations of the millisecond pulsar-low-mass X-ray binary (LMXB) transition system PSR J1023+0038 from 2013 June and October, before and after the formation of an accretion disk around the neutron star. Between June 10 and 12, a few days to two weeks before the radio disappearance of the pulsar, the 3-79 keV X-ray spectrum was well fit by a simple power law with a photon index of Γ = 1.17^(+0.08)_(-0.07) (at 90% confidence) with a 3-79 keV luminosity of 7.4 ± 0.4 × 10^(32) erg s^(–1). Significant orbital modulation was observed with a modulation fraction of 36% ± 10%. During the October 19-21 observation, the spectrum is described by a softer power law (Γ = 1.66^(+0.06)_(-0.05)) with an average luminosity of 5.8 ± 0.2 × 10^(33) erg s^(–1) and a peak luminosity of ≈1.2 × 10^(34) erg s^(–1) observed during a flare. No significant orbital modulation was detected. The spectral observations are consistent with previous and current multiwavelength observations and show the hard X-ray power law extending to 79 keV without a spectral break. Sharp-edged, flat-bottomed dips are observed with widths between 30 and 1000 s and ingress and egress timescales of 30-60 s. No change in hardness ratio was observed during the dips. Consecutive dip separations are log-normal in distribution with a typical separation of approximately 400 s. These dips are distinct from dipping activity observed in LMXBs. We compare and contrast these dips to observations of dips and state changes in the similar transition systems PSR J1824–2452I and XSS J1227.0–4859 and discuss possible interpretations based on the transitions in the inner disk.
The Astrophysical Journal | 2013
C. Kouveliotou; Jonathan Granot; Judith Lea Racusin; Eric C. Bellm; G. Vianello; S. R. Oates; Christopher L. Fryer; S. E. Boggs; Finn Erland Christensen; William W. Craig; C. D. Dermer; Neil Gehrels; Charles J. Hailey; Fiona A. Harrison; Andrea Melandri; J. E. McEnery; Carole G. Mundell; D. Stern; G. Tagliaferri; William W. Zhang
GRB 130427A occurred in a relatively nearby galaxy; its prompt emission had the largest GRB fluence ever recorded. The afterglow of GRB 130427A was bright enough for the Nuclear Spectroscopic Telescope ARray (NuSTAR) to observe it in the 3-79 keV energy range long after its prompt emission (~1.5 and 5 days). This range, where afterglow observations were previously not possible, bridges an important spectral gap. Combined with Swift, Fermi, and ground-based optical data, NuSTAR observations unambiguously establish a single afterglow spectral component from optical to multi-GeV energies a day after the event, which is almost certainly synchrotron radiation. Such an origin of the late-time Fermi/Large Area Telescope >10 GeV photons requires revisions in our understanding of collisionless relativistic shock physics.
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 | 2013
L. P. Singer; S. Bradley Cenko; Mansi M. Kasliwal; Daniel A. Perley; Eran O. Ofek; D. A. Brown; Peter E. Nugent; S. R. Kulkarni; A. Corsi; Dale A. Frail; Eric C. Bellm; John S. Mulchaey; Iair Arcavi; Tom A. Barlow; Joshua S. Bloom; Yi Cao; Neil Gehrels; Assaf Horesh; Frank J. Masci; J. E. McEnery; Jason A. Surace; Ofer Yaron
We report the discovery of the optical afterglow of the γ-ray burst (GRB) 130702A, identified upon searching 71 deg^2 surrounding the Fermi Gamma-ray Burst Monitor (GBM) localization. Discovered and characterized by the intermediate Palomar Transient Factory, iPTF13bxl is the first afterglow discovered solely based on a GBM localization. Real-time image subtraction, machine learning, human vetting, and rapid response multi-wavelength follow-up enabled us to quickly narrow a list of 27,004 optical transient candidates to a single afterglow-like source. Detection of a new, fading X-ray source by Swift and a radio counterpart by CARMA and the Very Large Array confirmed the association between iPTF13bxl and GRB 130702A. Spectroscopy with the Magellan and Palomar 200 inch telescopes showed the afterglow to be at a redshift of z = 0.145, placing GRB 130702A among the lowest redshift GRBs detected to date. The prompt γ-ray energy release and afterglow luminosity are intermediate between typical cosmological GRBs and nearby sub-luminous events such as GRB 980425 and GRB 060218. The bright afterglow and emerging supernova offer an opportunity for extensive panchromatic follow-up. Our discovery of iPTF13bxl demonstrates the first observational proof-of-principle for ~10 Fermi-iPTF localizations annually. Furthermore, it represents an important step toward overcoming the challenges inherent in uncovering faint optical counterparts to comparably localized gravitational wave events in the Advanced LIGO and Virgo era.
The Astrophysical Journal | 2013
Felix Fürst; Brian W. Grefenstette; Rüdiger Staubert; John A. Tomsick; Matteo Bachetti; Didier Barret; Eric C. Bellm; Steven E. Boggs; J. Chenevez; Finn Erland Christensen; William W. Craig; Charles J. Hailey; Fiona A. Harrison; D. Klochkov; Kristin K. Madsen; Katja Pottschmidt; Daniel Stern; D. J. Walton; J. Wilms; William W. Zhang
Her X-1, one of the brightest and best studied X-ray binaries, shows a cyclotron resonant scattering feature (CRSF) near 37 keV. This makes it an ideal target for a detailed study with the Nuclear Spectroscopic Telescope Array (NuSTAR), taking advantage of its excellent hard X-ray spectral resolution. We observed Her X-1 three times, coordinated with Suzaku, during one of the high flux intervals of its 35 day superorbital period. This paper focuses on the shape and evolution of the hard X-ray spectrum. The broadband spectra can be fitted with a power law with a high-energy cutoff, an iron line, and a CRSF. We find that the CRSF has a very smooth and symmetric shape in all observations and at all pulse phases. We compare the residuals of a line with a Gaussian optical-depth profile to a Lorentzian optical-depth profile and find no significant differences, strongly constraining the very smooth shape of the line. Even though the line energy changes dramatically with pulse phase, we find that its smooth shape does not. Additionally, our data show that the continuum only changes marginally between the three observations. These changes can be explained with varying amounts of Thomson scattering in the hot corona of the accretion disk. The average, luminosity-corrected CRSF energy is lower than in past observations and follows a secular decline. The excellent data quality of NuSTAR provides the best constraint on the CRSF energy to date.
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.