Maheswar Gopinathan
Aryabhatta Research Institute of Observational Sciences
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Maheswar Gopinathan.
The Astrophysical Journal | 2016
Mauri J. Valtonen; S. Zola; S. Ciprini; A. Gopakumar; Katsura Matsumoto; Kozo Sadakane; M. Kidger; Kosmas D. Gazeas; K. Nilsson; A. Berdyugin; V. Piirola; H. Jermak; Kiran S. Baliyan; F. Alicavus; David Boyd; M. Campas Torrent; F. Campos; J. Carrillo Gómez; Daniel B. Caton; V. Chavushyan; J. Dalessio; B. Debski; D. Dimitrov; M. Drozdz; H. Er; A. Erdem; A. Escartin Pérez; V. Fallah Ramazani; A. V. Filippenko; Shashikiran Ganesh
OJ 287 is a quasi-periodic quasar with roughly 12 year optical cycles. It displays prominent outbursts that are predictable in a binary black hole model. The model predicted a major optical outburst in 2015 December. We found that the outburst did occur within the expected time range, peaking on 2015 December 5 at magnitude 12.9 in the optical R-band. Based on Swift/XRT satellite measurements and optical polarization data, we find that it included a major thermal component. Its timing provides an accurate estimate for the spin of the primary black hole,
The Astrophysical Journal | 2008
Sami Dib; Axel Brandenburg; Jongsoo Kim; Maheswar Gopinathan; Philippe André
\chi =0.313\pm 0.01
The Astrophysical Journal | 2016
Gwanjeong Kim; Chang Won Lee; Maheswar Gopinathan; Woong-Seob Jeong; Mi-Ryang Kim
. The present outburst also confirms the established general relativistic properties of the system such as the loss of orbital energy to gravitational radiation at the 2% accuracy level, and it opens up the possibility of testing the black hole no-hair theorem with 10% accuracy during the present decade.
Current Science | 2017
Amitesh Omar; Brijesh Kumar; Maheswar Gopinathan; Ram Sagar
We analyze the mass distribution of cores formed in an isothermal, magnetized, turbulent, and self-gravitating nearly critical molecular cloud model. Cores are identified at two density threshold levels. Our main results are that the presence of self-gravity modifies the slopes of the core mass function (CMF) at the high-mass end. At low thresholds, the slope is shallower than the one predicted by pure turbulent fragmentation. The shallowness of the slope is due to the effects of core coalescence and gas accretion. Most importantly, the slope of the CMF at the high-mass end steepens when cores are selected at higher density thresholds, or alternatively, if the CMF is fitted with a lognormal function, the width of the lognormal distribution decreases with increasing threshold. This is due to the fact that gravity plays a more important role in denser structures selected at higher density threshold and leads to the conclusion that the role of gravity is essential in generating a CMF that bears more resemblance to the IMF when cores are selected with an increasing density threshold in the observations.
Proceedings of SPIE | 2016
Krishna Reddy Bheemireddy; Maheswar Gopinathan; Jayshreekar Pant; Amitesh Omar; Brijesh Kumar; Wahab Uddin; Nirmal Kumar
We present results of our study on eight dense cores, previously classified as starless, using infrared (3-160 {\micron}) imaging observations with \textit{AKARI} telescope and molecular line (HCN and N
Proceedings of SPIE | 2016
Maheswar Gopinathan; Sanjit Sahu; Shobhit Yadava; Purshottam Jangid; Biman J. Medhi; Pramesh Rao; Brijesh Kumar; Amitesh Omar; Wahab Uddin
_2
Archive | 2011
Ram Sagar; Amitesh Omar; Brijesh Kumar; Maheswar Gopinathan; Shashi Pandey; Tarun Bangia; Jayshreekar Pant; Vishal Shukla; Shobhit Yadava
H
Galaxies | 2016
S. Zola; Mauri J. Valtonen; G. Bhatta; A. Goyal; B. Debski; A. Baran; J. Krzesinski; Michal Siwak; S. Ciprini; A. Gopakumar; H. Jermak; K. Nilsson; Daniel E. Reichart; Katsura Matsumoto; Kozo Sadakane; Kosmas D. Gazeas; M. Kidger; V. Piirola; F. Alicavus; K. S. Baliyan; A. Berdyugin; David Boyd; M. Campas Torrent; F. Campos; J. Carrillo Gómez; Daniel B. Caton; V. Chavushyan; J. Dalessio; D. Dimitrov; M. Drozdz
^+
Sciprints | 2016
S. Zola; Mauri J. Valtonen; G. Bhatta; A. Goyal; B. Debski; A. Baran; J. Krzesinski; M. Siwak; S. Ciprini; A. Gopakumar; H. Jermak; K. Nilsson; Daniel E. Reichart; Katsura Matsumoto; Kozo Sadakane; Kosmas D. Gazeas; M. Kidger; V. Piirola; F. Alicavus; K. S. Baliyan; A. Berdyugin; David Boyd; M. Campas Torrent; F. Campos; J. Carrillo Gómez; Daniel B. Caton; V. Chavushyan; J. Dalessio; D. Dimitrov; M. Drozdz
) mapping observations with \textit{KVN} telescope. Combining our results with the archival IR to mm continuum data, we examined the starless nature of these eight cores. Two of the eight cores are found to harbor faint protostars having luminosity of