Abhirup Ghosh
Tata Institute of Fundamental Research
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Featured researches published by Abhirup Ghosh.
Radio Science | 2016
M. Mevius; S. van der Tol; V. N. Pandey; H. K. Vedantham; M. A. Brentjens; A. G. Bruyn; F. B. Abdalla; K. M. B. Asad; Jaap D. Bregman; W. N. Brouw; S. Bus; E. Chapman; B. Ciardi; Elizabeth R. Fernandez; Abhirup Ghosh; G. Harker; Ilian T. Iliev; Vibor Jelić; S. Kazemi; Léon V. E. Koopmans; Jan E. Noordam; A. R. Offringa; A. H. Patil; R. J. Weeren; Stefan J. Wijnholds; S. Yatawatta; Saleem Zaroubi
LOFAR is the LOw-Frequency Radio interferometer ARray located at midlatitude (52°53′N). Here we present results on ionospheric structures derived from 29 LOFAR nighttime observations during the winters of 2012/2013 and 2013/2014. We show that LOFAR is able to determine differential ionospheric total electron content values with an accuracy better than 0.001 total electron content unit = 1016m−2 over distances ranging between 1 and 100 km. For all observations the power law behavior of the phase structure function is confirmed over a long range of baseline lengths, between 1 and 80 km, with a slope that is, in general, larger than the 5/3 expected for pure Kolmogorov turbulence. The measured average slope is 1.89 with a one standard deviation spread of 0.1. The diffractive scale, i.e., the length scale where the phase variance is 1rad2, is shown to be an easily obtained single number that represents the ionospheric quality of a radio interferometric observation. A small diffractive scale is equivalent to high phase variability over the field of view as well as a short time coherence of the signal, which limits calibration and imaging quality. For the studied observations the diffractive scales at 150 MHz vary between 3.5 and 30 km. A diffractive scale above 5 km, pertinent to about 90% of the observations, is considered sufficient for the high dynamic range imaging needed for the LOFAR epoch of reionization project. For most nights the ionospheric irregularities were anisotropic, with the structures being aligned with the Earth magnetic field in about 60% of the observations.
Monthly Notices of the Royal Astronomical Society | 2015
H. K. Vedantham; Luitje Koopmans; de Antonius Bruyn; Stefan J. Wijnholds; M. A. Brentjens; F. B. Abdalla; K. M. B. Asad; G. Bernardi; S. Bus; E. Chapman; B. Ciardi; S. Daiboo; Elizabeth R. Fernandez; Abhirup Ghosh; G. Harker; Vibor Jelić; Hannes Jensen; S. Kazemi; P. Lambropoulos; O. Martinez-Rubi; Garrelt Mellema; M. Mevius; A. R. Offringa; V. N. Pandey; A. H. Patil; Rajat M. Thomas; V. Veligatla; S. Yatawatta; Saleem Zaroubi; J. Anderson
We present radio observations of the Moon between 35 and 80 MHz to demonstrate a novel technique of interferometrically measuring large-scale diffuse emission extending far beyond the primary beam (global signal) for the first time. In particular, we show that (i) the Moon appears as a negative-flux source at frequencies 35 z > 12) and the Epoch of Reionization (12 > z > 5).
Physical Review D | 2016
Abhirup Ghosh; Archisman Ghosh; Nathan K. Johnson-McDaniel; Chandra Kant Mishra; P. Ajith; Walter Del Pozzo; David A. Nichols; Yanbei Chen; Alex B. Nielsen; C. P. L. Berry; L. T. London
The coalescences of stellar-mass black-hole binaries through their inspiral, merger, and ringdown are among the most promising sources for ground-based gravitational-wave (GW) detectors. If a GW signal is observed with sufficient signal-to-noise ratio, the masses and spins of the black holes can be estimated from just the inspiral part of the signal. Using these estimates of the initial parameters of the binary, the mass and spin of the final black hole can be uniquely predicted making use of general-relativistic numerical simulations. In addition, the mass and spin of the final black hole can be independently estimated from the merger-ringdown part of the signal. If the binary black-hole dynamics is correctly described by general relativity (GR), these independent estimates have to be consistent with each other. We present a Bayesian implementation of such a test of general relativity, which allows us to combine the constraints from multiple observations. Using kludge modified GR waveforms, we demonstrate that this test can detect sufficiently large deviations from GR and outline the expected constraints from upcoming GW observations using the second-generation of ground-based GW detectors.
Classical and Quantum Gravity | 2018
Abhirup Ghosh; Nathan K. Johnson-McDaniel; Archisman Ghosh; Chandra Kant Mishra; P. Ajith; Walter Del Pozzo; C. P. L. Berry; Alex B. Nielsen; L. T. London
Advanced LIGOs recent observations of gravitational waves (GWs) from merging binary black holes have opened up a unique laboratory to test general relativity (GR) in the highly relativistic regime. One of the tests used to establish the consistency of the first LIGO event with a binary black hole merger predicted by GR was the inspiral-merger-ringdown consistency test. This involves inferring the mass and spin of the remnant black hole from the inspiral (low-frequency) part of the observed signal and checking for the consistency of the inferred parameters with the same estimated from the post-inspiral (high-frequency) part of the signal. Based on the observed rate of binary black hole mergers, we expect the advanced GW observatories to observe hundreds of binary black hole mergers every year when operating at their design sensitivities, most of them with modest signal to noise ratios (SNRs). Anticipating such observations, this paper shows how constraints from a large number of events with modest SNRs can be combined to produce strong constraints on deviations from GR. Using kludge modified GR waveforms, we demonstrate how this test could identify certain types of deviations from GR if such deviations are present in the signal waveforms. We also study the robustness of this test against reasonable variations of a variety of different analysis parameters.
Physical Review D | 2018
C. E. Patrick; L. Aliaga; A. Bashyal; L. Bellantoni; A. Bercellie; M. Betancourt; A. Bodek; A. Bravar; H. S. Budd; M. F. Carneiro; E. Chavarria; H. da Motta; S. A. Dytman; G. A. Díaz; J. Felix; L. Fields; R. Fine; A. M. Gago; R. Galindo; H. R. Gallagher; Abhirup Ghosh; R. Gran; J. Y. Han; D. A. Harris; S. Henry; K. Hurtado; D. Jena; J. Kleykamp; M. Kordosky; T. Le
We present double-differential measurements of antineutrino charged-current quasielastic scattering in the MINERvA detector. This study improves on a previous single-differential measurement by using updated reconstruction algorithms and interaction models and provides a complete description of observed muon kinematics in the form of a double-differential cross section with respect to muon transverse and longitudinal momentum. We include in our signal definition zero-meson final states arising from multinucleon interactions and from resonant pion production followed by pion absorption in the primary nucleus. We find that model agreement is considerably improved by a model tuned to MINERvA inclusive neutrino scattering data that incorporates nuclear effects such as weak nuclear screening and two-particle, two-hole enhancements.
Monthly Notices of the Royal Astronomical Society | 2018
W. Del Pozzo; C. P. L. Berry; Abhirup Ghosh; T S F Haines; L P Singer; A. Vecchio
We report on the Dirichlet Process Gaussian-mixture model, a fully Bayesian non-parametric method that can be used to estimate probability densities and compute credible volumes with a minimal set of assumptions. We illustrate its effectiveness by reconstructing posterior distributions for the position (sky area and distance) of a simulated set of binary neutron-star gravitational-waves signals observed with Advanced LIGO and Advanced Virgo. The ability to reliably reconstruct the source position is important for multimessenger astronomy, as recently demonstrated with GW170817. We show that for detector networks comparable to the early operation of Advanced LIGO and Advanced Virgo, typical localization volumes are
Physical Review Letters | 2018
R. Gran; T. Cai; M. Sultana; Kevin Scott McFarland; X. Lu; S. A. Dytman; J.R. Leistico; L. Fields; J. Wolcott; R. D. Ransome; D. Jena; P. A. Rodrigues; H. S. Budd; M. Betancourt; F. Akbar; A. Olivier; A. Bodek; L. Aliaga; C. M. Marshall; S. Manly; H. R. Gallagher; Abhirup Ghosh; B. Yaeggy; C. Nguyen; A. Lovlein; H. Ray; H. Schellman; J. K. Nelson; J. Morfin; A. M. McGowan
\sim10^4
Physical Review Letters | 2016
J. Wolcott; L. Aliaga; O. Altinok; L. Bellantoni; A. Bercellie; M. Betancourt; A. Bodek; A. Bravar; H. S. Budd; T. Cai; M. F. Carneiro; J. Chvojka; da Motta H; J. Devan; S. A. Dytman; G. A. Díaz; B. Eberly; J. Felix; L. Fields; R. Fine; A. M. Gago; R. Galindo; H. R. Gallagher; Abhirup Ghosh; T. Golan; R. Gran; D. A. Harris; A. Higuera; M. Kiveni; J. Kleykamp
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Physical Review D | 2016
C. M. Marshall; L. Aliaga; O. Altinok; L. Bellantoni; A. Bercellie; M. Betancourt; A. Bodek; A. Bravar; H. S. Budd; T. Cai; M. F. Carneiro; J. Chvojka; H. da Motta; J. Devan; S. A. Dytman; G. A. Díaz; B. Eberly; E. Endress; J. Felix; L. Fields; A. Filkins; R. Fine; A. M. Gago; R. Galindo; H. R. Gallagher; Abhirup Ghosh; T. Golan; R. Gran; S. Griswold; D. A. Harris
10^5~\mathrm{Mpc^3}
Physical Review D | 2016
S. Griswold; A. Bodek; B. Eberly; D. Rimal; T. Walton; W. A. Mann; S. A. Dytman; I. Majoros; E. Valencia; J. Devan; M. Rosenberg; D. Schmitz; L. Bellantoni; D. A. Martinez Caicedo; G. N. Perdue; P. A. Rodrigues; Joel S. Miller; J. Mousseau; M. Betancourt; A. M. Gago; P. Watkins; M. Kiveni; H. Schellman; M. Kordosky; D. A. Harris; H. da Motta; J. Park; A. M. McGowan; D. Zhang; J. Osta
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