Mahesh P. Burse
Inter-University Centre for Astronomy and Astrophysics
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Featured researches published by Mahesh P. Burse.
The Astrophysical Journal | 2014
Christoph Baranec; Reed Riddle; Nicholas M. Law; A. N. Ramaprakash; Shriharsh P. Tendulkar; Kristina Hogstrom; Khanh Bui; Mahesh P. Burse; Pravin Chordia; H. K. Das; Richard G. Dekany; S. R. Kulkarni; Sujit Punnadi
As new large-scale astronomical surveys greatly increase the number of objects targeted and discoveries made, the requirement for efficient follow-up observations is crucial. Adaptive optics imaging, which compensates for the image-blurring effects of Earths turbulent atmosphere, is essential for these surveys, but the scarcity, complexity and high demand of current systems limit their availability for following up large numbers of targets. To address this need, we have engineered and implemented Robo-AO, a fully autonomous laser adaptive optics and imaging system that routinely images over 200 objects per night with an acuity 10 times sharper at visible wavelengths than typically possible from the ground. By greatly improving the angular resolution, sensitivity, and efficiency of 1-3 m class telescopes, we have eliminated a major obstacle in the follow-up of the discoveries from current and future large astronomical surveys.
The Astrophysical Journal | 2012
Nicholas M. Law; Adam L. Kraus; R. A. Street; Benjamin J. Fulton; Lynne A. Hillenbrand; Avi Shporer; Tim Lister; Christoph Baranec; Joshua S. Bloom; Khanh Bui; Mahesh P. Burse; S. Bradley Cenko; H. K. Das; Jack Davis; Richard G. Dekany; Alexei V. Filippenko; Mansi M. Kasliwal; S. R. Kulkarni; Peter E. Nugent; Eran O. Ofek; Dovi Poznanski; Robert Michael Quimby; A. N. Ramaprakash; Reed Riddle; Jeffrey M. Silverman; Suresh Sivanandam; Shriharsh P. Tendulkar
We present three new eclipsing white-dwarf/M-dwarf binary systems discovered during a search for transiting planets around M-dwarfs. Unlike most known eclipsing systems of this type, the optical and infrared emission is dominated by the M-dwarf components, and the systems have optical colors and discovery light curves consistent with being Jupiter-radius transiting planets around early M-dwarfs. We detail the PTF/M-dwarf transiting planet survey, part of the Palomar Transient Factory (PTF). We present a graphics processing unit (GPU)-based box-least-squares search for transits that runs approximately 8 × faster than similar algorithms implemented on general purpose systems. For the discovered systems, we decompose low-resolution spectra of the systems into white-dwarf and M-dwarf components, and use radial velocity measurements and cooling models to estimate masses and radii for the white dwarfs. The systems are compact, with periods between 0.35 and 0.45 days and semimajor axes of approximately 2 R_☉ (0.01 AU). The M-dwarfs have masses of approximately 0.35 M_☉, and the white dwarfs have hydrogen-rich atmospheres with temperatures of around 8000 K and have masses of approximately 0.5 M_☉. We use the Robo-AO laser guide star adaptive optics system to tentatively identify one of the objects as a triple system. We also use high-cadence photometry to put an upper limit on the white-dwarf radius of 0.025 R_☉ (95% confidence) in one of the systems. Accounting for our detection efficiency and geometric factors, we estimate that 0.08%^(+0.10%)_(-0.05%) (90% confidence) of M-dwarfs are in these short-period, post-common-envelope white-dwarf/M-dwarf binaries where the optical light is dominated by the M-dwarf. The lack of detections at shorter periods, despite near-100% detection efficiency for such systems, suggests that binaries including these relatively low-temperature white dwarfs are preferentially found at relatively large orbital radii. Similar eclipsing binary systems can have arbitrarily small eclipse depths in red bands and generate plausible small-planet-transit light curves. As such, these systems are a source of false positives for M-dwarf transiting planet searches. We present several ways to rapidly distinguish these binaries from transiting planet systems.
The Astrophysical Journal | 2013
Philip S. Muirhead; Andrew Vanderburg; Avi Shporer; Juliette C. Becker; Jonathan J. Swift; James P. Lloyd; Jim Fuller; Ming Zhao; Sasha Hinkley; J. Sebastian Pineda; Michael Bottom; Andrew W. Howard; Kaspar von Braun; Tabetha S. Boyajian; Nicholas M. Law; Christoph Baranec; Reed Riddle; A. N. Ramaprakash; Shriharsh P. Tendulkar; Khanh Bui; Mahesh P. Burse; Pravin Chordia; H. K. Das; Richard G. Dekany; Sujit Punnadi; John Asher Johnson
We report that Kepler Object of Interest 256 (KOI-256) is a mutually eclipsing post-common envelope binary (ePCEB), consisting of a cool white dwarf (M_★ = 0.592 ± 0.089 M_☉, R_★ = 0.01345 ± 0.00091 R_☉, T_(eff) = 7100 ± 700 K) and an active M3 dwarf (M_★ = 0.51 ± 0.16 M_☉, R_★ = 0.540 ± 0.014 R_☉, T_(eff) = 3450 ± 50 K) with an orbital period of 1.37865 ± 0.00001 days. KOI-256 is listed as hosting a transiting planet-candidate by Borucki et al. and Batalha et al.; here we report that the planet-candidate transit signal is in fact the occultation of a white dwarf as it passes behind the M dwarf. We combine publicly-available long- and short-cadence Kepler light curves with ground-based measurements to robustly determine the system parameters. The occultation events are readily apparent in the Kepler light curve, as is spin-orbit synchronization of the M dwarf, and we detect the transit of the white dwarf in front of the M dwarf halfway between the occultation events. The size of the white dwarf with respect to the Einstein ring during transit (R_(Ein) = 0.00473 ± 0.00055 R ☉) causes the transit depth to be shallower than expected from pure geometry due to gravitational lensing. KOI-256 is an old, long-period ePCEB and serves as a benchmark object for studying the evolution of binary star systems as well as white dwarfs themselves, thanks largely to the availability of near-continuous, ultra-precise Kepler photometry.
Proceedings of SPIE | 2012
Christoph Baranec; Reed Riddle; A. N. Ramaprakash; Nicholas M. Law; Shriharsh P. Tendulkar; S. R. Kulkarni; Richard G. Dekany; K. Bui; Jack Davis; Mahesh P. Burse; H. K. Das; S. Hildebrandt; Sujit Punnadi; Roger Smith
We have created a new autonomous laser-guide-star adaptive-optics (AO) instrument on the 60-inch (1.5-m) telescope at Palomar Observatory called Robo-AO. The instrument enables diffraction-limited resolution observing in the visible and near-infrared with the ability to observe well over one-hundred targets per night due to its fully robotic operation. Robo-AO is being used for AO surveys of targets numbering in the thousands, rapid AO imaging of transient events and long-term AO monitoring not feasible on large diameter telescope systems. We have taken advantage of cost-effective advances in deformable mirror and laser technology while engineering Robo-AO with the intention of cloning the system for other few-meter class telescopes around the world.
Proceedings of SPIE | 2012
Reed Riddle; Mahesh P. Burse; Nicholas M. Law; Shriharsh P. Tendulkar; Christoph Baranec; Alexander Rudy; Marland Sitt; Ankit S. Arya; Athanasios I. Papadopoulos; A. N. Ramaprakash; Richard G. Dekany
Robo-AO is the first astronomical laser guide star adaptive optics (AO) system designed to operate completely independent of human supervision. A single computer commands the AO system, the laser guide star, visible and near-infrared science cameras (which double as tip-tip sensors), the telescope, and other instrument functions. Autonomous startup and shutdown sequences as well as concatenated visible observations were demonstrated in late 2011. The fully robotic software is currently operating during a month long demonstration of Robo- AO at the Palomar Observatory 60-inch telescope.
Proceedings of SPIE | 2010
A. N. Ramaprakash; Mahesh P. Burse; Pravin Chordia; Kalpesh Chillal; Abhay Kohok; Vilas Mestry; Sujit Punnadi; Sakya Sinha
SIDECAR is an Application Specific Integrated Circuit (ASIC), which can be used for control and data acquisition from near-IR HAWAII detectors offered by Teledyne Imaging Sensors (TIS), USA. The standard interfaces provided by Teledyne are COM API and socket servers running under MS Windows platform. These interfaces communicate to the ASIC (and the detector) through an intermediate card called JWST ASIC Drive Electronics (JADE2). As part of an ongoing programme of several years, for developing astronomical focal plane array (CCDs, CMOS and Hybrid) controllers and data acquisition systems (CDAQs), IUCAA is currently developing the next generation controllers employing Virtex-5 family FPGA devices. We present here the capabilities which are built into these new CDAQs for handling HAWAII detectors. In our system, the computer which hosts the application programme, user interface and device drivers runs on a Linux platform. It communicates through a hot-pluggable USB interface (with an optional optical fibre extender) to the FPGA-based card which replaces the JADE2. The FPGA board in turn, controls the SIDECAR ASIC and through it a HAWAII-2RG detector, both of which are located in a cryogenic test Dewar set up which is liquid nitrogen cooled. The system can acquire data over 1, 4, or 32 readout channels, with or without binning, at different speeds, can define sub-regions for readout, offers various readout schemes like Fowler sampling, up-theramp etc. In this paper, we present the performance results obtained from a prototype system.
Proceedings of SPIE | 2014
M. Wolf; Mark P. Mulligan; Michael P. Smith; Douglas P. Adler; Curtis M. Bartosz; Matthew A. Bershady; David A. H. Buckley; Mahesh P. Burse; Pravin Chordia; J. Christopher Clemens; Harland W. Epps; Kristine Garot; Briana L. Indahl; Kurt P. Jaehnig; Ron J. Koch; William P. Mason; Gregory Mosby; Kenneth H. Nordsieck; Jeffrey W. Percival; Sujit Punnadi; A. N. Ramaprakash; J. Alan Schier; Andrew Sheinis; Stephen A. Smee; Donald J. Thielman; Mark W. Werner; Theodore B. Williams; Jeffrey P. Wong
The Robert Stobie Spectrograph Near Infrared Instrument (RSS-NIR), a prime focus facility instrument for the 11-meter Southern African Large Telescope (SALT), is well into its laboratory integration and testing phase. RSS-NIR will initially provide imaging and single or multi-object medium resolution spectroscopy in an 8 arcmin field of view at wavelengths of 0.9 - 1.7 μm. Future modes, including tunable Fabry-Perot spectral imaging and polarimetry, have been designed in and can be easily added later. RSS-NIR will mate to the existing visible wavelength RSS-VIS via a dichroic beamsplitter, allowing simultaneous operation of the two instruments in all modes. Multi-object spectroscopy covering a wavelength range of 0.32 - 1.7 μm on 10-meter class telescopes is a rare capability and once all the existing VIS modes are incorporated into the NIR, the combined RSS will provide observational modes that are completely unique. The VIS and NIR instruments share a common telescope focal plane, and slit mask for spectroscopic modes, and collimator optics that operate at ambient observatory temperature. Beyond the dichroic beamsplitter, RSS-NIR is enclosed in a pre-dewar box operating at -40 °C, and within that is a cryogenic dewar operating at 120 K housing the detector and final camera optics and filters. This semi-warm configuration with compartments at multiple operating temperatures poses a number of design and implementation challenges. In this paper we present overviews of the RSSNIR instrument design and solutions to design challenges, measured performance of optical components, detector system optimization results, and an update on the overall project status.
arXiv: Instrumentation and Methods for Astrophysics | 2011
Christoph Baranec; Reed Riddle; A. N. Ramaprakash; Nicholas M. Law; Shriharsh P. Tendulkar; S. R. Kulkarni; Richard G. Dekany; Khanh Bui; Jack Davis; Jeff Zolkower; Jason Fucik; Mahesh P. Burse; H. K. Das; Pravin Chordia; Mansi M. Kasliwal; Eran O. Ofek; Timothy D. Morton; John Asher Johnson
Robo-AO, a fully autonomous, laser guide star adaptive optics and science system, is being commissioned at Palomar Observatory’s 60-inch telescope. Here we discuss the instrument, scientific goals and results of initial on-sky operation.
The Astronomical Journal | 2015
Lewis C. Roberts; Brian D. Mason; Christopher R. Neyman; Yanqin Wu; Reed Riddle; J. Christopher Shelton; John Angione; Christoph Baranec; Antonin Bouchez; Khanh Bui; Rick Burruss; Mahesh P. Burse; Pravin Chordia; Ernest Croner; H. K. Das; Richard G. Dekany; Stephen R. Guiwits; David Hale; John R. Henning; S. R. Kulkarni; Nicholas M. Law; Dan McKenna; Jennifer Milburn; Dean L. Palmer; Sujit Punnadi; A. N. Ramaprakash; Jennifer E. Roberts; Shriharsh P. Tendulkar; Thang Trinh; Mitchell Troy
HD 8673 hosts a massive exoplanet in a highly eccentric orbit (e = 0.723). Based on two epochs of speckle interferometry a previous publication identified a candidate stellar companion. We observed HD 8673 multiple times with the 10 m Keck II telescope, the 5 m Hale telescope, the 3.63 m Advanced Electro-Optical System telescope, and the 1.5 m Palomar telescope in a variety of filters with the aim of confirming and characterizing the stellar companion. We did not detect the candidate companion, which we now conclude was a false detection, but we did detect a fainter companion. We collected astrometry and photometry of the companion on six epochs in a variety of filters. The measured differential photometry enabled us to determine that the companion is an early M dwarf with a mass estimate of 0.33–0.45 M_☉. The companion has a projected separation of 10 AU, which is one of the smallest projected separations of an exoplanet host binary system. Based on the limited astrometry collected, we are able to constrain the orbit of the stellar companion to a semimajor axis of 35–60 AU, an eccentricity ≤0.5, and an inclination of 75°–85°. The stellar companion has likely strongly influenced the orbit of the exoplanet and quite possibly explains its high eccentricity.
Proceedings of SPIE | 2016
Sabyasachi Chattopadhyay; Pravin Chordia; A. N. Ramaprakash; Mahesh P. Burse; Bhushan Joshi; Kalpesh Chillal
In order to run the large format detector arrays and mosaics that are required by most astronomical instruments, readout electronic controllers are required which can process multiple CCD outputs simultaneously at high speeds and low noise levels. These CCD controllers need to be modular and configurable, should be able to run multiple detector types to cater to a wide variety of requirements. IUCAA Digital Sampler Array Controller (IDSAC), is a generic CCD Controller based on a fully scalable architecture which is adequately flexible and powerful enough to control a wide variety of detectors used in ground based astronomy. The controller has a modular backplane architecture that consists of Single Board Controller Cards (SBCs) and can control up to 5 CCDs (mosaic or independent). Each Single Board Controller (SBC) has all the resources to a run Single large format CCD having up to four outputs. All SBCs are identical and are easily interchangeable without needing any reconfiguration. A four channel video processor on each SBC can process up to four output CCDs with or without dummy outputs at 0.5 Megapixels/Sec/Channel with 16 bit resolution. Each SBC has a USB 2.0 interface which can be connected to a host computer via optional USB to Fibre converters. The SBC uses a reconfigurable hardware (FPGA) as a Master Controller. IDSAC offers Digital Correlated Double Sampling (DCDS) to eliminate thermal kTC noise. CDS performed in Digital domain (DCDS) has several advantages over its analog counterpart, such as - less electronics, faster readout and easier post processing. It is also flexible with sampling rate and pixel throughput while maintaining the core circuit topology intact. Noise characterization of the IDSAC CDS signal chain has been performed by analytical modelling and practical measurements. Various types of noise such as white, pink, power supply, bias etc. has been considered while creating an analytical noise model tool to predict noise of a controller system like IDSAC. Several tests are performed to measure the actual noise of IDSAC. The theoretical calculation matches very well with practical measurements within 10% accuracy.