Localization of gamma-ray bursts using AstroSat Mass Model

Author:

Saraogi Divita1ORCID,Aditya J Venkata2ORCID,Bhalerao Varun1ORCID,Bala Suman13ORCID,Balasubramanian Arvind4ORCID,Mate Sujay4ORCID,Chattopadhyay Tanmoy5ORCID,Gupta Soumya6ORCID,Prasad Vipul7,Waratkar Gaurav1,Navaneeth P K7,Gopalakrishnan Rahul7,Bhattacharya Dipankar8ORCID,Dewangan Gulab7ORCID,Vadawale Santosh9ORCID

Affiliation:

1. Department of Physics, Indian Institute of Technology Bombay , Powai, Mumbai, Maharashtra 400076 , India

2. Department of Computer Science and Engineering, Indian Institute of Technology Bombay , Powai, Mumbai, Maharashtra 400076 , India

3. Science and Technology Institute, Universities Space Research Association , Huntsville, AL 35805 , USA

4. Department of Astronomy and Astrophysics, Tata Institute of Fundamental Research , Mumbai, Maharashtra 400005 , India

5. Kavli Institute of Astrophysics and Cosmology, Stanford University , 452 Lomita Mall, Stanford, CA 94305 , USA

6. Astrophysical Science Division, Homi Bhabha National Institute , Anushakti Nagar, Mumbai, Maharashtra 400094 , India

7. Inter University Centre for Astronomy and Astrophysics , Pune, Maharashtra 411007 , India

8. Department of Physics, Ashoka University , Sonepat, Haryana 131029 , India

9. Physical Research Laboratory , Ahmedabad, Gujarat 380009 , India

Abstract

ABSTRACT The Cadmium Zinc Telluride Imager (CZTI) aboard AstroSat has good sensitivity to gamma-ray bursts (GRBs), with close to 600 detections including about 50 discoveries undetected by other missions. However, CZTI was not designed to be a GRB monitor and lacks localization capabilities. We introduce a new method of localizing GRBs using ‘shadows’ cast on the CZTI detector plane due to absorption and scattering by satellite components and instruments. Comparing the observed distribution of counts on the detector plane with simulated distributions with the AstroSat Mass Model, we can localize GRBs in the sky. Our localization uncertainty is defined by a two-component model, with a narrow Gaussian component that has close to 50  per cent probability of containing the source, and the remaining spread over a broader Gaussian component with an 11.3 times higher σ. The width (σ) of the Gaussian components scales inversely with source counts. We test this model by applying the method to GRBs with known positions and find good agreement between the model and observations. This new ability expands the utility of CZTI in the study of GRBs and other rapid high-energy transients.

Funder

Tata Institute of Fundamental Research

ISRO

Publisher

Oxford University Press (OUP)

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