Massive binary black holes from Population II and III stars

被引:13
|
作者
Costa, Guglielmo [1 ,2 ,3 ,4 ]
Mapelli, Michela [1 ,2 ,3 ,5 ]
Iorio, Giuliano [1 ,2 ,3 ]
Santoliquido, Filippo [1 ,2 ]
Escobar, Gaston J. [1 ,2 ]
Klessen, Ralf S. [5 ]
Bressan, Alessandro [3 ,6 ]
机构
[1] Univ Padua, Dipartimento Fis & Astron Galileo Galilei, Vicolo Osservatorio 3, I-35122 Padua, Italy
[2] INFN Padova, Via Marzolo 8, I-35131 Padua, Italy
[3] INAF Padova, Vicolo Osservatorio 5, I-35122 Padua, Italy
[4] Univ Lyon1, Univ Lyon, CNRS, Ctr Rech Astrophys Lyon,Ens Lyon,UMR5574, F-69230 St Genis Laval, France
[5] Heidelberg Univ, Inst Theoret Astrophys, Zentrum Astron, Albert Ueberle Str 2, D-69120 Heidelberg, Germany
[6] SISSA, Via Bonomea 365, I-34136 Trieste, Italy
基金
欧洲研究理事会;
关键词
black hole physics; gravitational waves; methods: numerical; stars: Population II; stars: Population III; PULSATIONAL PAIR-INSTABILITY; MERGER RATE DENSITY; STELLAR EVOLUTION; GRAVITATIONAL-WAVES; 1ST STARS; IMPACT; SUPERNOVAE; EXPLOSION; SCENARIO; TRACKS;
D O I
10.1093/mnras/stad2443
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Population III stars, born from the primordial gas in the Universe, lose a negligible fraction of their mass via stellar winds and possibly follow a top-heavy mass function. Hence, they have often been regarded as the ideal progenitors of massive black holes (BHs), even above the pair instability mass gap. Here, we evolve a large set of Population III binary stars (metallicity Z = 10(-11)) with our population-synthesis code SEVN, and compare them with Population II binary stars (Z = 10(-4)). In our models, the lower edge of the pair-instability mass gap corresponds to a BH mass of approximate to 86 (approximate to 91) M-circle dot for single Population III (II) stars. Overall, we find only mild differences between the properties of binary BHs (BBHs) born from Population III and II stars, especially if we adopt the same initial mass function and initial orbital properties. Most BBH mergers born from Population III and II stars have primary BH mass below the pair-instability gap, and the maximum secondary BH mass is <50 M-circle dot. Only up to approximate to 3.3 per cent (approximate to 0.09 per cent) BBH mergers from Population III (II) progenitors have primary mass above the gap. Unlike metal-rich binary stars, the main formation channel of BBH mergers from Population III and II stars involves only stable mass transfer episodes in our fiducial model.
引用
收藏
页码:2891 / 2906
页数:16
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