Optical and X-ray GRB Fundamental Planes as cosmological distance indicators

Author:

Dainotti M G123,Nielson V45ORCID,Sarracino G67,Rinaldi E8910,Nagataki S1011,Capozziello S6712ORCID,Gnedin O Y5,Bargiacchi G712ORCID

Affiliation:

1. National Astronomical Observatory of Japan , 2 Chome-21-1 Osawa, Mitaka, Tokyo 181-8588, Japan

2. The Graduate University for Advanced Studies, SOKENDAI , Shonankokusaimura, Hayama, Miura District, Kanagawa 240-0193, Japan

3. Space Science Institute , Boulder, CO 80301, USA

4. SLAC National Accelerator Laboratory , 2575 Sand Hill Road, Menlo Park, CA 94025, USA

5. Astronomy Department, University of Michigan , Ann Arbor, MI 48109, USA

6. Dipartimento di Fisica, ‘E. Pancini’ Università ‘Federico II’ di Napoli, Compl. Univ. Monte S. Angelo Ed. G , Via Cinthia, I-80126 Napoli, Italy

7. INFN Sez. di Napoli, Compl. Univ. Monte S. Angelo Ed. G , Via Cinthia, I-80126 Napoli, Italy

8. Physics Department, University of Michigan , Ann Arbor, MI 48109, USA

9. RIKEN Cluster for Pioneering Research, Theoretical Quantum Physics Laboratory , 2-1 Hirosawa, Wako, Saitama 351-0198, Japan

10. Interdisciplinary Theoretical and Mathematical Science Program, RIKEN (iTHEMS) , 2-1 Hirosawa, Wako, Saitama 351-0198, Japan

11. RIKEN Cluster for Pioneering Research, Astrophysical Big Bang Laboratory (ABBL) , 2-1 Hirosawa, Wako, Saitama 351-0198, Japan

12. Scuola Superiore Meridionale, Università di Napoli Federico II , Largo San Marcellino 10, I-80138 Napoli, Italy

Abstract

ABSTRACT Gamma-ray bursts (GRBs), can be employed as standardized candles, extending the distance ladder beyond Type Ia supernovae (SNe Ia, z = 2.26). We standardize GRBs using the three-dimensional (3D) Fundamental Plane relation (the Dainotti relation) among the rest-frame end time of the X-ray plateau emission, its corresponding luminosity, and the peak prompt luminosity. Combining SNe Ia and GRBs, we constrain ΩM = 0.299 ± 0.009 assuming a flat Λ cold dark matter (ΛCDM) cosmology with and without correcting GRBs for selection biases and redshift evolution. Using a 3D optical Dainotti correlation, we find this sample is as efficacious in the determination of ΩM as the X-ray sample. We trimmed our GRB samples to achieve tighter planes to simulate additional GRBs. We determined how many GRBs are needed as stand-alone probes to achieve a comparable precision on ΩM to the one obtained by SNe Ia only. We reach the same error measurements derived using SNe Ia in 2011 and 2014 with 142 and 284 simulated optical GRBs, respectively, considering the error bars on the variables halved. These error limits will be reached in 2038 and in 2047, respectively. Using a doubled sample (obtained by future machine learning approaches allowing a light-curve reconstruction and the estimates of GRB redshifts when z is unknown) compared to the current sample, with error bars halved we will reach the same precision as SNe Ia in 2011 and 2014, now and in 2026, respectively. If we consider the current SNe precision, this will be reached with 390 optical GRBs by 2054.

Funder

KAKENHI

RIKEN

University of Leicester

United States Department of Energy

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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