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Black Hole

Lensing of space time around a black hole. At Oxford we study black holes observationally and theoretically on all size and time scales - it is some of our core work.

Credit: ALAIN RIAZUELO, IAP/UPMC/CNRS. CLICK HERE TO VIEW MORE IMAGES.

Dr Siddharth Maharana

Visitor

Research theme

  • Astronomy and astrophysics
  • Instrumentation
  • Exoplanets and planetary physics

Sub department

  • Astrophysics

Research groups

  • Extremely Large Telescope
siddharth.maharana@physics.ox.ac.uk
Telephone: 01865 (2)73503
Denys Wilkinson Building, room 361A
  • About
  • Current projects
  • Research
  • Publications

Improving polarimetric accuracy of RoboPol to $<$ 0.05 % using a half-wave plate calibrator system

ArXiv 2407.1347 (2024)

Authors:

Siddharth Maharana, Dmitry Blinov, AN Ramaprakash, Vasiliki Pavlidou, Konstantinos Tassis

Comparing the contrast performance of two IFU technologies for exoplanet direct imaging with ELT-PCS

Advances in Optical and Mechanical Technologies for Telescopes and Instrumentation VII SPIE 14154 (2026)

Authors:

Ryan Griffiths, Siddharth Maharana, Matthias Tecza

Abstract:

A key science goal for the Planetary Camera and Spectrograph (ELT-PCS) instrument is to image rocky exoplanets in reflected light around nearby M- and K-dwarfs. These observations will require a contrast of 10−9 at 100 mas angular separation, and 10−8 at 10 mas. To achieve such an extreme performance, every instrument design choice must be carefully evaluated. For ELT-PCS’s science instruments, perhaps the most critical design choice is which integral field unit (IFU) technology to use. To this end, we have developed a modular, lab-based integral field spectrograph test bench with which to compare the performance of two popular IFU technologies: image slicers and lenslet arrays. The test bench implements a Lyot coronagraph and a spatial light modulator to simulate a high-contrast imaging system, which feeds each IFU with a diffraction-limited PSF image. Each IFU is coupled to the spectrograph, which achieves R≈3000 with the image slicer and R≈100 with the lenslet array. The calibration and data reduction for each IFU design are described and the initial results of a contrast comparison are presented. The lenslet array achieves a deeper contrast at angular separations of less than 6λ/D. The image slicer, however, gains more at small separations from applying spectral deconvolution, with a 3.4× greater gain at 4λ/D. Spectral deconvolution further yields a contrast curve close to the detector noise floor. Further work will focus on carrying out a fully-controlled characterisation of the lenslet array IFU and a more comprehensive study into the effects of adaptive optics residuals on the contrast.

Commissioning and on-sky performance of FiberPol: a fiber-fed spectropolarimetric system for the SAAO 1.9 m telescope

ArXiv 2607.16111 (2026)

Authors:

Siddharth Maharana, KCJ Dennison-Farrar, Sabyasachi Chattopadhyay, Nikita Rawat, Nidhi Mehandiratta, JC Viljoen, Matthew Bershady, David Buckley, Lisa A Crause, Hitesh Gajjar, Stephen Potter

Evidence for cloud-to-cloud variations in the ratio of polarized thermal dust emission to starlight polarization

Astronomy & Astrophysics EDP Sciences 708 (2026) A53-A53

Authors:

N Mehandiratta, G Panopoulou, E Gjerløw, V Pelgrims, K Tassis, D Blinov, B Hensley, JA Kypriotakis, S Maharana, N Mandarakas, V Pavlidou, SB Potter, AN Ramaprakash, R Skalidis, N Uppal

Abstract:

The correlation between optical starlight polarization and polarized thermal dust emission can be used to infer intrinsic dust properties. This correlation is quantified by the ratio R P / p , which has been measured by the Planck Collaboration to be 5.42 ± 0.05 MJy sr −1 at 353 GHz when averaged over large areas of the sky. We investigated this correlation using newly published stellar polarimetric data densely sampling a continuous sky region of about four square degrees at intermediate Galactic latitude. We combined RoboPol optical polarization measurements for 1430 stars with submillimeter data from the Planck satellite at 353 GHz. We performed linear fits between the Planck ( Q s , U s ) and optical ( q v , u v ) Stokes parameters, taking into account the differences in resolution between the two datasets as well as the distribution of clouds along the line of sight. We find in this region of the sky that the R P / p value is 3.67 ± 0.05 MJy sr −1 , indicating a significantly shallower slope than that found previously using different stellar samples. We also find significant differences in the fitted slopes when fitting the Q s – q v and U s – u v data separately. We explore two explanations using mock data: the miscalibration of the polarization angle and the variations in R P / p along the line of sight due to multiple clouds. We show that the former can produce differences in the correlations of Q s – q v and U s – u v , but large miscalibration angles would be needed to reproduce the magnitude of the observed differences. Our simulations favor the interpretation that R P / p differs between the two dominant clouds that overlap on the sky in this region. The difference in R P / p suggests that the two clouds may have distinct dust polarimetric properties. With knowledge from the tomographic decomposition of the stellar polarization, we find that one cloud appears to dominate the correlation of U s – u v , while both clouds contribute to the correlation of the Q s – q v data.

Evidence for cloud-to-cloud variations in the ratio of polarized thermal dust emission to starlight polarization

ArXiv 2510.15389 (2025)

Authors:

Nidhi Mehandiratta, Georgia V Panopoulou, Eirik Gjerløw, Vincent Pelgrims, Konstantinos Tassis, Dmitry Blinov, Brandon Hensley, John A Kypriotakis, Siddharth Maharana, Nikos Mandarakas, Vasiliki Pavlidou, Stephen B Potter, AN Ramaprakash, Raphael Skalidis, Namita Uppal

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