Limits on non-canonical heating and turbulence in the intergalactic medium from the low redshift Lyman α forest

被引:17
作者
Bolton, James S. [1 ]
Gaikwad, Prakash [2 ,3 ]
Haehnelt, Martin G. [2 ]
Kim, Tae-Sun [4 ]
Nasir, Fahad [5 ]
Puchwein, Ewald [6 ]
Viel, Matteo [7 ,8 ,9 ,10 ]
Wakker, Bart P. [4 ]
机构
[1] Univ Nottingham, Sch Phys & Astron, Nottingham NG7 2RD, England
[2] Kavli Inst Cosmol & Inst Astron, Madingley Rd, Cambridge CB3 0HA, England
[3] Max Planck Inst Astron, Konigstuhl 17, D-69117 Heidelberg, Germany
[4] Univ Wisconsin Madison, Dept Astron, 475N Charter St, Madison, WI 53706 USA
[5] Univ Calif, Dept Phys & Astron, Riverside, CA 92521 USA
[6] Leibniz Inst Astrophys, Sternwarte 16, D-14482 Potsdam, Germany
[7] SISSA Int Sch Adv Studies, Via Bonomea 265, I-34136 Trieste, Italy
[8] IFPU, Inst Fundamental Phys Univ, Via Beirut 2, I-34151 Trieste, Italy
[9] INAF Osservat Astronom Trieste, Via G B Tiepolo 11, I-34131 Trieste, Italy
[10] INFN Natl Inst Nucl Phys, Via Valerio 2, I-34127 Trieste, Italy
关键词
methods: numerical; intergalactic medium; quasars: absorption lines; EQUATION-OF-STATE; COSMOLOGICAL HYDRODYNAMICAL SIMULATIONS; PHOTON UNDERPRODUCTION CRISIS; SMALL-SCALE STRUCTURE; ILLUSTRISTNG SIMULATIONS; THERMAL HISTORY; POWER SPECTRUM; HE II; COSMIC-RAYS; CIRCUMGALACTIC MEDIUM;
D O I
10.1093/mnras/stac862
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We examine the column density distribution function (CDDF) and Doppler parameter distribution from hydrodynamical simulations and Cosmic Origins Spectrograph (COS) observations of the Ly alpha forest at redshift 0 <= z <= 0.2. Allowing for a factor of two uncertainty in the metagalactic H I photoionization rate, our hydrodynamical simulations are in good agreement (1-1.5 sigma) with the shape and amplitude of the observed CDDF at H I column densities 10(13.3 )cm(-2) <= N-H I <= 10(14.5) cm(-2). However, the Doppler widths of the simulated lines remain too narrow with respect to the COS data. We argue that invoking AGN feedback does not resolve this discrepancy. We also disfavour enhanced photoheating rates as a potential solution, as this requires an unphysically hard UV background spectrum. If instead appealing to a non-canonical source of heating, an additional specific heat injection of u less than or similar to 6.9 eV m(p)(-1) is required at z less than or similar to 2.5 for gas that has N-H I similar or equal to 10(13.5) cm(-2) by z = 0.1. Alternatively, there may be an unresolved line of sight turbulent velocity component of nu(turb) less than or similar to 8.5 km s(-1) (N-H I/10(13.5) cm(-2))(0.21) for the coldest gas in the diffuse IGM.
引用
收藏
页码:864 / 885
页数:22
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