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Gamma-ray absorption by cosmic radiation fields Susumu Inoue (Kyoto University) with (more than) a little help from my friends Fermi z~60-6 blazar GRB CTA outline 1. probe of high-z UV background SI, R. Salvaterra, T. R. Choudhury, A. Ferrara, B. Ciardi, R. Schneider, MNRAS in press (arXiv:0906.2495) Y. Inoue, M. Kobayashi, T. Totani, SI et al., work in prep. 2. probe of Lorentz invariance violation effect in Galactic sources? diffuse extragalactic background radiation at z=0 EBL= extragalactic background light 1. gamma-ray absorption: probe of diffuse radiation fields g + g → e+ + eE e threshold condition: E e (1-cos q )>2 me2c4 s peak ,, =4 me2c4 e.g. TeV + 1eV (IR) 100 GeV + 10 eV (UV) pair production cross section CM energy Costamante et al 03 probe of local IRB through gamma absorption in TeV blazars probing local IR background with gamma-ray absorption HESS observations of TeV blazars @z=0.165, 0.186 Aharonian+ 06 Nat. • strongly disfavors NIR peak no strong Pop III • close to lower limits from galaxy counts EBL constraints at z=0.536 Albert+ 08 Sci. Eg(=1) QuickTimeý Dz TIFFÅiîÒà• èkÅj êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB MAGIC observation 80-500 GeV 3C279 @z=0.536 close to lower limits from galaxy counts (little missing light) if “normal” blazar spectra >1.5 EBL constraints at z=4.35 Abdo+ 09, Sci. 323, 1688 Fermi/LAT detection of GRB 080916C up to 13 GeV without cutoff QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB slides from T. R. Choudhury QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB cosmic reionization epoch z>6 current observational frontier When? early? late? two-epoch? How? topology? What? Pop III? Pop II? mini-QSOs? dark matter decay? So what? suppression of dwarf galaxy formation QuickTimeý Dz TIFFÅiîÒà• èkÅj êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB Madau 07 slides from T. R. Choudhury QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB high-z UV radiation field (“background”) crucial for understanding early universe • reionizes the IGM (feedback on later galaxy formation) • dissociates H2 molecules (feedback on later star formation) • Ly pumping (determines HI hyperfine 21cm level population) but direct detection impossible! model of cosmic reionization Choudhury & Ferrara 05, 06, Choudhury 09 parameters e*II, e*III, hesc, l0IGM semi-analytical model with Pop III+II stars+QSOs, radiative+chemical feedback consistent with large set of high-z observations: WMAP, xHI, HUDF NIR counts, etc. xHI WMAP3 (WMAP5 OK) SFR Ly LLS reionization begins z~15 90% z~8 100% z~6 Gphotoion QuickTimeý Dz TIFFÅiîÒà• èkÅj êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB HUDF Lyb TIGM intergalactic radiation field (volume average) caveat: model only for 4<z<22, no Pop I/dust SI+ arXiv:0906.2945 spectra “local’’ optical depth QuickTimeý Dz QuickTimeý Dz TIFFÅiîÒà• èkÅj êLí£ÉvÉçÉOÉâÉÄ TIFFÅiîÒà• èkÅj êLí£ÉvÉçÉOÉâÉÄ ÅB ǙDZÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB ǙDZÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• • realistic UV IRF -> opaque for Erest~10’s-100’s GeV at z<~10 • sharp cutoff at Erest~18 GeV from HI absorption above Ly edge (reionizing radiation cannot be probed directly) gg absorption optical depth (high UV) SI+ arXiv:0906.2495 low z model Kneiske+ 04 (high stellar UV) see also e.g. Stecker+ 06 Razzaque+ 09 Gilmore+ 09 gg~0.4 @z=4.35, E=13.2GeV (GRB 080916C) Qui ck Ti meý Dz TIFFÅi îÒà• è k Åj êLí£Év Éç ÉOÉâÉÄ Ç™Ç±ÇÃÉs ÉNÉ`ÉÉǾå©ÇÈÇž ǽDžÇÕïKóv ÇÇ• ÅB QuickTi meý Dz TIFFÅiîÒà• èkÅj êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz TIFFÅiîÒà• èkÅj êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB significant optical depth >12 GeV at z~5, down to 6-8 GeV at z~8-10 but not much effect z>~8 due to declining star formation, path length gg absorption attenuation factor low z model Kneiske+ 04 (high stellar UV) (high UV) Fermi CTA, AGIS 5@5 appreciable differences in attenuation between z~5-8 at several GeV → unique, important info on evolution of UV IRF below Ly edge during cosmic reionization/first star formation alternative models e.g. late reionization model with no Pop III stars differences not large, attenuation not sensitive to reionization history → predictions reasonably robust? detectability GRBs most luminous GRBs (LGeV~1054 erg/s, e.g. GRB 080916C) detectable @10GeV by Fermi out to z~7 out to higher z by future large arrays! CTA, AGIS, 5@5 blazars most luminous blazars (LGeV~1049 erg/s, e.g. 3C454.3) detectable @10GeV by Fermi out to z~7 few such objects plausible Y. Inoue, SI, Totani+, in prep. distinction between intrinsic cutoffs spectral variability: IRF cutoff t-indep. <-> intrinsic cutoff t-dep. statistical: similar cutoffs for similar z, decreasing trend with z cosmic star formation rate Y. Inoue, Totani, SI et al. in prep. QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB CAUTION: data at z>6 mostly lower limits to cosmic SFR large uncertainties in SFR at z>6 models with low Pop II but high Pop III also possible? cosmic star formation rate estimated from GRB rate Kistler+ 09 QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB gg optical depth: comparison Y. Inoue et al., in prep. QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB large differences in absorption! -> distinguishable through CTA obs. 2. gg absorption: probe of Lorentz invariance violation? Kifune 99, Aloisio+ 00, Protheroe & Meyer 00… following Jacob & Piran 08, PRD 78, 124010 QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB n=1 0.1 1 10 100 E*(TeV) 11 23 50 110 c.f. n=2 E*(=1)=0.9x1017 TeV modified threshold QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB Jacob & Piran 08 modified absorption feature QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB Jacob & Piran 08 caveat: assume LIV affects only eth effect on blazar spectra CTA 100 TeV observations! QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB Jacob & Piran 08 BUT - depends on EBL uncertainties - blazar spectra to >10 TeV unlikely? effect on Galactic sources? 20,0,90 R,z, 0,0,0 20,0,180 QuickTimeý Dz êLí£ÉvÉçÉOÉâÉÄ Ç™Ç±ÇÃÉsÉNÉ`ÉÉǾå©ÇÈǞǽDžÇÕïKóvÇÇ• ÅB Moskalenko+ 06 - Galactic 100 TeV sources likely (e.g. SNRs) - appreciable >10 TeV absorption in Galactic Center region - probe of >20 TeV LIV recovery summary g-ray absorption by cosmic radiation fields probe of UV intergalactic radiation fields at high z based on a model of cosmic reionization significant >12 GeV at z~5, down to 6-8 GeV at z>~8 -> valuable info on evolution of UV IRF below Ly edge (constraints on Ly/H2 dissociating radiation) but not much effect above z~8 detectable in high-L GRBs/blazars to z~<7 by Fermi possibly to higher z by CTA, AGIS, 5@5 BUT alternative models with different Pop II/III SFRs possible? -> distinguishable through GeV observations? crucial contribution to understanding early star/galaxy formation probe of Lorentz invariance violation? recovery of absorption feature above ~20 TeV effect in Galactic center sources promising?