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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.

Prof. Niranjan Thatte

Professor of Astrophysics

Research theme

  • Astronomy and astrophysics
  • Instrumentation
  • Exoplanets and planetary physics

Sub department

  • Astrophysics

Research groups

  • Astronomical instrumentation
  • Exoplanets and Stellar Physics
  • Galaxy formation and evolution
  • Extremely Large Telescope
Niranjan.Thatte@physics.ox.ac.uk
Telephone: 01865 (2)73412
Denys Wilkinson Building, room 709
  • About
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Teaching Insights

Education

School is to make students 'Yearn to Learn'. College is to get students to 'Learn to Learn'

The dark mass concentration in the central parsec of the milky way

Astrophysical Journal 472:1 PART I (1996) 153-172

Authors:

R Genzel, N Thatte, A Krabbe, H Kroker, LE Tacconi-Garman

Abstract:

We report ∼1″ resolution K-band (2 μm) imaging spectroscopy of the central parsec of our Galaxy. The derived radial velocities for 223 early- and late-type stars probe the nuclear mass distribution to spatial scales of 0.1 pc. We find a statistically very significant increase of projected stellar velocity dispersion from about 55 km s-1 at p ∼ 5 pc to 180 km s-1 at p ∼ 0.1 pc. The stars are also rotating about the dynamic center. The late-type stars follow general Galactic rotation, while the early-type stars show counter-rotation. Fitting simultaneously the observed projected surface densities and velocity dispersions, we derive the intrinsic volume densities and radial velocity dispersions as a function of distance from the dynamic center for both types of stars. We then derive the mass distribution between 0.1 and 5 pc from the Jeans equation assuming an isotropic velocity field. Our analysis requires a compact central dark mass of 2.5-3.2 × 106 M⊙, at 6-8 σ significance. The dark mass has a density of 109 M⊙ pc-3 or greater and a mass to 2 μm luminosity of ≥ 100. The increase in mass-to-luminosity ratio can be reduced but not eliminated even if extreme anisotropic velocity destributions are considered. The dark mass cannot be a cluster of solar mass remnants (such as neutron stars). It is either a compact cluster of 10-20 M⊙ black holes or a single massive black hole. © 1996. The American Astronomical Society. All rights reserved.
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NIR Imaging Spectroscopy of F10214: Evidence for a Starburst Around an AGN at Z = 2.284

Chapter in Spiral Galaxies in the Near-IR, Springer Nature (1996) 336-338

Authors:

H Kroker, R Genzel, A Krabbe, LE Tacconi-Garman, M Tecza, N Thatte
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Near IR and mm Imaging Spectroscopy of the Nuclear Region of NGC 1068

Chapter in Spiral Galaxies in the Near-IR, Springer Nature (1996) 333-335

Authors:

N Thatte, L Tacconi, H Kroker, A Krabbe, LE Tacconi-Garman, R Genzel
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Near infrared imaging spectroscopy of cD galaxy NGC1275

ASTR SOC P 98 (1996) 515-516

Authors:

BJ Sams, R Genzel, A Krabbe, N Thatte, F Prada
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Near-IR imaging spectroscopy of CD galaxy NGC1275

IAU SYMP (1996) 440-440

Authors:

BJ Sams, R Genzel, A Krabbe, N Thatte, H Kroker
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