4.7 Article

Simulations on high-z long gamma-ray burst rate

期刊

出版社

OXFORD UNIV PRESS
DOI: 10.1111/j.1365-2966.2010.16691.x

关键词

instrumentation: detectors; stars: evolution; stars: formation; gamma-ray burst: general; stars: luminosity function; mass function; galaxies: high-redshift

资金

  1. National Natural Science Foundation of China [10873002, 10747001, 10821061, 10725313, 10847003]
  2. National Basic Research Program ('973' Program) of China [2009CB824800]
  3. Guangxi SHI-BAI-QIAN project [2007201]
  4. Guangxi Science Foundation [2010GXNSFC013011, 2010GXNSFA13112]
  5. Chinese Academy of Science [KJCXZ-YW-T19]
  6. program for 100 Young and Middle-aged Disciplinary Leaders in Guangxi Higher Education Institution
  7. research foundation of Guangxi University

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Since the launch of Swift satellite, the detections of high-z (z > 4) long gamma-ray bursts (LGRBs) have been rapidly growing, even approaching the very early Universe (the record holder currently is z = 8.3). The observed high-z LGRB rate shows significant excess over that estimated from the star formation history. We investigate what may be responsible for this high productivity of GRBs at high-z through Monte Carlo simulations, with effective Swift/Burst Alert Telescope (BAT) trigger and redshift detection probabilities based on current Swift/BAT sample and Compton Gamma-ray Observatory/Burst and Transient Source Experiment LGRB sample. We compare our simulations to the Swift observations via log N - log P, peak luminosity (L) and redshift distributions. In the case that LGRB rate is purely proportional to the star formation rate, our simulations poorly reproduce the LGRB rate at z > 4, although the simulated log N - log P distribution is in good agreement with the observed one. Assuming that the excess of high-z GRB rate is due to the cosmic metallicity evolution or unknown LGRB rate increase parametrized as (1 + z)delta, we find that although the two scenarios alone can improve the consistency between our simulations and observations, incorporation of them gives much better consistency. We get 0.2 < epsilon < 0.6 and delta < 0.6, where epsilon is the metallicity threshold for the production of LGRBs. The best consistency is obtained with a parameter set (epsilon, delta) = (similar to 0.4, similar to 0.4), and BAT might trigger a few LGRBs at z similar or equal to 14. With increasing detections of GRBs at z > 4 (similar to 15 per cent of GRBs in current Swift LGRB sample based on our simulations), a window for very early Universe is opening by Swift and up-coming space-based multiband astronomical variable object monitor missions.

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