7-1yamazaki.pptx
|
|
- なごみ えいさか
- 5 years ago
- Views:
Transcription
1
2 Suzaku/ASTRO-H Suzaku/ASTRO-H
3 1. Vela ( Watchman ) ( ): GRB (1969) 2. GINGA ( ): X-ray counterpart GRB (galactic) X-ray burst? 3. BATSE ( ): Galactic origin models!!! 4. BeppoSAX ( ): X-ray (optical) afterglow cosmological distance!!! 5. HETE-2 (2000 ): long GRB/SN association 6. Swift (2004 ) high-z GRB (z > 6) => 7. Fermi (2008~) : GeV GRB
4 (=>calorimetry) VLA (redshift, localization, jet structure) (localization, jet structure) Swift/XRT available. *10keV-MeV GeV (jet speed, radiation mechanism, CR) Fermi 7events/yr TeV (radiation mechanism, CR) CTA events/yr.
5 GRB research in the Fermi era GRB GeV (1) Γ (2) GRB (~MeV ) (synchrotron or SSC?) (3) GRB Γ=300 Γ=1000 2ndary e ± (pγ π ± e ± ) Γ=100 Asano, Inoue primary e -
6 GRB research in the Fermi era GRB GeV (1) Γ (2) GRB (~MeV ) (synchrotron or SSC?) (3) GRB Γ=300 Γ=1000 2ndary e ± (pγ π ± e ± ) Γ=100 Asano, Inoue primary e -
7 GRB research in the Fermi era GRB GeV (1) Γ (2) GRB (~MeV ) (synchrotron or SSC?) (3) GRB Γ=300 Γ=1000 2ndary e ± (pγ π ± e ± ) Γ=100 Swift WAM LAT Swift WAM primary e - LAT
8 Fermi LAT detection of GRB C First GeV γ detection of a GRB with known redshift. * High-z, bright event: z = 4.35±0.15 E iso (10keV-10GeV) = 8.8x10 55 erg ~ 5 M sun c 2 => Jet collimation * GeV photons avoiding pair-creation annihilation => Relativistic motion: Γ > 890±20 (bin b ) Fermi LAT collaboration (2009)
9 Fermi GeV GRBs GeV delay (delay ) (leptonic model) IC emission? (Hadronic model) proton acceleration time? GeV lepton proton proton
10
11 Ahlers UHECRs in internal shocks of GRBs In internal shock, P 10^ γ GRB => π 0, π +, n UHECRs γ, e +/- : => GeV gamma s (1) Hires Fermi diffuse gamma IcuCube (γ, E max ) N(E) E γ exp ( E / E max ) β n => p + e - + ν e UHECRs UHE-Nu s CMB => GeV gamma s (2), UHE-Nu s(gzk-nu)
12 (GRB rate) SFR (GRB rate) SFR x (1+z) 1.4 GeV Gamma s (1),(2) GeV Gamma s (2) GeV Gamma UHECRs Fermi diffuse gamma
13 (GRB rate) SFR (GRB rate) SFR x (1+z) 1.4 GeV Gamma s (1),(2) GeV Gamma s (2) GeV Gamma UHECRs Fermi diffuse gamma
14 Ahlers GRB Internal shock UHECRs UHECR flux UHECR (γ<2.1) ev UHECR ev Fermi Diffuse gamma
15 Neutrino upper limit from IceCube GRB IceCube: Abbasi+2011
16 Neutrino upper limit from IceCube GRB Waxman GRB photon spectrum Guetta IceCube: Abbasi+2011
17 Neutrino upper limit from IceCube GRB AMANDA IceCube (40strings) IceCube (22strings) Waxman GRB photon spectrum Guetta IceCube: Abbasi+2011
18 Waxman Bahcall (upper) bound CR proton ν µ p+p or p+γ => π + or π - => ν µ or ν µ CR proton ( GeV/cm 2 /s/sr ) energy production rate (n p CR E p -2 ) factor 0.25 = 0.5 ( = loss via π 0 production) x 0.5 ( = E ν /E π ) t H : Hubble time (CR proton ) ξ Z ~1 : redshift evolution & energy loss
19 Waxman Bahcall (upper) bound CR proton WB bound τ (source size) / (CR proton m.f.p.) τ 1 WB bound τ < 1 WB bound (e.g. : τ << 1 for GRB external shocks, Galactic SNRs ) τ > 1 CR proton WB bound => IceCube
20 GRB? Short GRB = Soft gamma-ray repeater giant flare? NS-NS merger UV and localized region
21 Fermi(Ext.Gal.Diffuse GeV), Icecube( ), LIGO( )
22 GRB is a relativistic version of SNR (Piran99) particle acceleration *internal-external shock model, *models of jet dynamics, jet emission, polarization, external compton, *<V/Vmax> of QSOs, * particle acceleration
23
24 2000 X-ray flash γ (Heise et al. 2001) (in t Zand et al. 1999)
25 Spectral properties of XRFs and GRBs Ep=19 kev Ep=126 kev Kippen et al. 02 Barraud et al. 03 Photon indices α, β ( ) GRB XRF XRF Ep (peak energy) GRB
26 Motivation : AGN X- ray flash GRB
27 X-ray flash 1 XRF/XRR classical GRB by HETE-2 XRF/XRR GRB GRB viewing angle, gamma factor, Lamb et al. (2003)
28 Theoretical Models of the X-ray flash
29 X-ray flash X-ray flash Amati relation low-energy (by HETE-2) Amati relation Yonetoku, Ghirlanda,Tsutsui relations Ep Sakamoto, RY+08 X-ray flash
30 Relativistic beaming and Doppler effects 1/γ v = 0 (matter comoving frame) v (observer frame) γ (1 β ) v/c
31 ff-axis Jet Model of XRFs
32 Off-axis model Ep E iso : detected by HETE (on-axis) : detected by HETE (off-axis) : not detected by HETE
33 Off-axis afterglow Granot On-axis Off-axis Observed light curves have a rising part at days.
34 2004 Swift Swift ( ~)
35 X-ray/Optical Ghisellini+
36 2005 Swift X-ray flash/x-ray rich GRB off-axis model Sakamoto, RY+ (08) XRF: Ep < 100 kev XRR: Ep = keV GRB: Ep > 300keV
37 Off- axis model rising part Guidorzi+09 XRF XRF XRF Kruhler+07 de Ugarte Pos<go+07
38 GRB Kruhler et al T90(15-350keV) = 120s, Gamma= (BAT) (Ep = kev) S(25-50keV)/S(50-100keV) = / classical GRB z = => Ep (1+z) 200keV log(eiso) =
39 GRB = on-axis prompt & off-axis afterglow? (a) (b) (c) prompt prompt prompt prompt: GRB(on-axis), AG: on-axis prompt: XRF(off-axis), AG: on-axis Prompt: XRF(off-axis), AG: off-axis (a) GRB (a) (b), (c) (c) 1 (b) Prompt
40 GRB off-axis emission Fermi AGN( ) Cygnus A (700 )
41 Prompt 1 1. Jets-in-a-jet: magnetic reconnection in prompt Blazer TeV prompt
42
43 Prompt 2 2. Bent jet, (like AGN; Fermi/KANATA 2010): * collision with stars or MCs? prompt * current driven kink, KH insta. prompt
44 Prompt 3 3. Inhomogeneous prompt efficiency of mini-jets. -high efficiency jets: little energy after prompt -low efficiency jets: little dissipative in prompt
45 Summary GRB GRB X-ray flash off-axis jet model Off-axis jet *prompt jets-in-a-jet, bent jet, inhomogeneous efficiency
Akira MIZUTA(KEK) AM, Nagataki, Aoi (ApJ, , 2011) AM + (in prep)
Akira MIZUTA(KEK) AM, Nagataki, Aoi (ApJ, 732 26, 2011) AM + (in prep) 2011.12.28 GRB GRB. ex. GRB980425/SN1998bw, GRB030329/SN2003dh XRF060218/SN2006aj. GRB091127/SN2009nz XRF100316D/SN2010bh Spectrum
More informationFermi ( )
Fermi ( ) Outline Introduction Blazar Spectral Energy Distribution (SED) Predictions for the Fermi mission (Prospects for CTA) Summary The Blazar Sequence and the Cosmic Gamma-ray Background Radiation
More informationKamLAND (µ) ν e RSFP + ν e RSFP(Resonant Spin Flavor Precession) ν e RSFP 1. ν e ν µ ν e RSFP.ν e νµ ν e νe µ KamLAND νe KamLAND (ʼ4). kton-day 8.3 < E ν < 14.8 MeV candidates Φ(νe) < 37 cm - s -1 P(νe
More informationスーパーカミオカンデにおける 高エネルギーニュートリノ研究
2009 11 20 Cosmic Ray PD D M P4 ? CR M f M PD MOA M1 ν ν p+p+p+p 4 He +2e - +2ν e MeV e - + p n+ ν e γ e + + e - ν x + ν x p + p, γ + p π + X π µ + ν µ e + ν µ + ν e TeV p + p π + X π µ + ν µ e + ν µ +
More informationE 1 GeV E 10 GeV 1 2, X X , GeV 10 GeV 1 GeV GeV π
169 8555 3 4 1 e-mail: kataoka.jun@waseda.jp 606 8502 e-mail: totani@kuastro.kyoto-u.ac.jp 305 0801 1 1 e-mail: kunihito.ioka@kek.jp 50 5 X 1 10 10 2008 3 2,000 542 2012 9 5 2. 1 3 E 1 GeV E 10 GeV 1 2,
More informationMicrosoft PowerPoint - takaahara
相対論的ジェット 高原文郎 ( 阪大理 ) Dec.27 2005 理論懇シンポ ( 基研 ) BH 天体に普遍的 GRB 超相対論的 AGN( 電波銀河 ) 相対論的 AGN( セイファート ) 非相対論的 マイクロクェーサー 準相対論的 アクリションとのとの相関 エネルギー源は重力 光学的に薄い高温高温プラズマプラズマに起源 Fender & Belloni (2004) 1915+105 Willott
More informationΜ粒子電子転換事象探索実験による世界最高感度での 荷電LFV探索 第3回機構シンポジューム 2009年5月11日 素粒子原子核研究所 三原 智
µ COMET LFV esys clfv (Charged Lepton Flavor Violation) J-PARC µ COMET ( ) ( ) ( ) ( ) B ( ) B ( ) B ( ) B ( ) B ( ) B ( ) B 2016 J- PARC µ KEK 3 3 3 3 3 3 3 3 3 3 3 clfv clfv clfv clfv clfv clfv clfv
More informationuntitled
masato@icrr.u-tokyo.ac.jp 996 Start 997 998 999 000 00 00 003 004 005 006 007 008 SK-I Accident Partial Reconstruction SK-II Full reconstruction ( SK-III ( ),46 (40%) 5,8 (9%),9 (40%) 5MeV 7MeV 4MeV(plan)
More informationnenmatsu5c19_web.key
KL π ± e νe + e - (Ke3ee) Ke3ee ν e + e - Ke3 K 0 γ e + π - Ke3 KL ; 40.67(%) Ke3ee K 0 ν γ e + π - Ke3 KL ; 40.67(%) Me + e - 10 4 10 3 10 2 : MC Ke3γ : data K L real γ e detector matter e e 10 1 0 0.02
More informationSolar Flare neutrino for Super Novae Conference
KamLAND 2019/01/07-08 KamLAND KamLAND 1. 10 2 ~10 3 sec 10 32 ~10 33 erg (http://www.isas.jaxa.jp/home/solar/yohkoh/) X,γ ( ) νe,νe,νµ,νµ. 2. p π ν/x /γ N π 0, π ± 2.22 MeV from 1 H(n,γ) 2 H p,n Solar
More informationPowerPoint Presentation
ガンマ線バースト : ブラックホールの誕生 井岡邦仁 ( 天体核 ) E=mc 2 = = 原子爆弾 太陽 ~10 33 g GRB ~10 52 erg 太陽が一生かけて出すエネルギーを数秒で放出 GRB は宇宙一明るい謎の天体 電磁波 高エネルギー宇宙物理 1967 Vela 衛星が発見核実験の監視衛星ところが γ 線は地球外から! 1973 発表 偶然の発見 高度 12 万 km 周期 5 日
More informationatomic line spectrum emission line absorption line atom proton neutron nuclei electron Z atomic number A mass number neutral atom ion energy
1 22 22.1 atomic line spectrum emission line absorption line atom proton neutronnuclei electron Z atomic number A mass number neutral atom ion energy level ground stateexcited state ionized state 22.2
More informationLHC-ATLAS Hà WWà lνlν A A A A A A
LHC-ATLAS Hà WWà lνlν A A A A A A 2011 1 Introduction 1fb -1 results and physics motivation -- ATLAS combined results with 1 fb -1 ZZà llnunu WWà lnulnu ZZà llll WWà lnuqq ATLAS official ATLAS 200-300
More informationuntitled
71 7 3,000 1 MeV t = 1 MeV = c 1 MeV c 200 MeV fm 1 MeV 3.0 10 8 10 15 fm/s 0.67 10 21 s (1) 1fm t = 1fm c 1fm 3.0 10 8 10 15 fm/s 0.33 10 23 s (2) 10 22 s 7.1 ( ) a + b + B(+X +...) (3) a b B( X,...)
More information総研大恒星進化概要.dvi
The Structure and Evolution of Stars I. Basic Equations. M r r =4πr2 ρ () P r = GM rρ. r 2 (2) r: M r : P and ρ: G: M r Lagrange r = M r 4πr 2 rho ( ) P = GM r M r 4πr. 4 (2 ) s(ρ, P ) s(ρ, P ) r L r T
More informationpositron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) MeV : thermalization m psec 100
positron 1930 Dirac 1933 Anderson m 22Na(hl=2.6years), 58Co(hl=71days), 64Cu(hl=12hour) 68Ge(hl=288days) 0.5 1.5MeV : thermalization 10 100 m psec 100psec nsec E total = 2mc 2 + E e + + E e Ee+ Ee-c mc
More informationB 1 B.1.......................... 1 B.1.1................. 1 B.1.2................. 2 B.2........................... 5 B.2.1.......................... 5 B.2.2.................. 6 B.2.3..................
More informationW 1983 W ± Z cm 10 cm 50 MeV TAC - ADC ADC [ (µs)] = [] (2.08 ± 0.36) 10 6 s 3 χ µ + µ 8 = (1.20 ± 0.1) 10 5 (Ge
22 2 24 W 1983 W ± Z 0 3 10 cm 10 cm 50 MeV TAC - ADC 65000 18 ADC [ (µs)] = 0.0207[] 0.0151 (2.08 ± 0.36) 10 6 s 3 χ 2 2 1 20 µ + µ 8 = (1.20 ± 0.1) 10 5 (GeV) 2 G µ ( hc) 3 1 1 7 1.1.............................
More informationPowerPoint Presentation
Sgr A* の赤外線観測 西山正吾 ( 京都大学 ) NIR obserbvations of the Galactic center 2/46 NIR obserbvations of the Galactic center 3/46 NIR obserbvations of the Galactic center 4/46 Dereddened flux density [mjy] 40 20
More informationスライド 1
上原岳士 植村誠 川端弘治 大杉節 山中雅之 笹田真人 先本清志 伊藤亮介 小松智之 奥嶋貴子 原尾達也 吉田道利 ( 広島大 ), 山崎了 ( 青山学院 ) 当真賢二 (Penn State Univ.) GCOE 研究会 ガンマ線バーストによるダークな宇宙の観測に向けたワークショップ 2010 年 8 月 26-27 日京都大学理学部 5 号館第四講義室 T.Uehara 1 X 線残光の光度曲線の特徴
More informationB
B09170 5 8 ) ( ) π 0-1 s -1 sr -1 MeV HI Emissivity (3rd quadrant) -3-4 Abdo et al. 009 (6 months, P6V3_DIFFUSE) Local arm interarm Perseus arm and beyond Emissivity (MeV E -5-6 3 4 Energy (MeV) 5 1: 1
More information(e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ,µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) [ ] [ ] [ ] ν e ν µ ν τ e µ τ, e R,µ R,τ R (2.1a
1 2 2.1 (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ,µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) [ ] [ ] [ ] ν e ν µ ν τ e µ τ, e R,µ R,τ R (2.1a) L ( ) ) * 2) W Z 1/2 ( - ) d u + e + ν e 1 1 0 0
More informationΛ (Λ ) Λ (Ge) Hyperball γ ΛN J-PARC Λ dead time J-PARC flash ADC 1 dead time ( ) 1 µsec 3
19 Λ (Λ ) Λ (Ge) Hyperball γ ΛN J-PARC Λ dead time J-PARC flash ADC 1 dead time ( ) 1 µsec 3 1 1 1.1 γ ΛN................. 1 1.2 KEK J-PARC................................ 2 1.2.1 J-PARC....................................
More information天体物理特論
高エネルギー宇宙ニュートリノ : 突発天体起源の可能性について 浅野勝晃 ( 東工大 ) IceCube による PeV ニュートリノ検出 2 イベント 7.8x10 5-5.6x10 6 GeV 8.9x10 5-8.5x10 6 GeV 当初は最高エネルギー宇宙線起源の 10 18 ev(eev) 程度のニュートリノ検出が期待されていた 予想を裏切って 10 15 ev(pev) のニュートリノが最初に検出された!
More informationRecent results from Swift
Some recent results from Swift Masaki Mori Goro Sato, presentation for Ph.D. thesis defense (January 2006) P. Jakobsson et al., A&A 447, 897 (2006) N. Kawai et al., astro-ph/0512052 ICRR CANGAROO group
More information2 X-ray 6 gamma-ray 7 1 17.1 0:38m 0:77m nm 17.2 Hz Hz 1 E p E E = h = ch= (17.2) p = E=c = h=c = h= (17.3) continuum continuous spectrum line spectru
1 17 object 1 observation 17.1 X electromagnetic wave photon 1 = c (17.1) c =3 10 8 ms ;1 m mm = 10 ;3 m m =10 ;6 m nm = 10 ;9 m 1 Hz 17.1 spectrum radio 2 infrared 3 visual light optical light 4 ultraviolet
More information加速器の基本概念 V : 高周波加速の基礎
.... V : KEK koji.takata@kek.jp http://research.kek.jp/people/takata/home.html 2015 2015 4 16 1 2 (1) 3 (2) 4 5 6 ERL: Energy Recovery Linac LCLS: Linac Coherent Light Source LC : µ-µ Koji Takata (KEK)
More information2
III 0713011005 2009 3 23 2 i (Gamma-Ray Burst : GRB) 10 msec 100 sec GRB 10 52 erg 10 48 erg GRB GRB GRB GRB 2007 Ikaros (Interplanetary Kite craft Accelerated by Radiation Of the Sun) (GAmma-ray burst
More information放射線化学, 92, 39 (2011)
V. M. S. V. 1 Contents of the lecture note by Prof. V. M. Byakov and Dr. S. V. Stepanov (Institute of Theoretical and Experimental Physics, Russia) are described in a series of articles. The first article
More information( ) Note (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ, µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) 3 * 2) [ ] [ ] [ ] ν e ν µ ν τ e
( ) Note 3 19 12 13 8 8.1 (e ) (µ ) (τ ) ( (ν e,e ) e- (ν µ, µ ) µ- (ν τ,τ ) τ- ) ( ) ( ) (SU(2) ) (W +,Z 0,W ) * 1) 3 * 2) [ ] [ ] [ ] ν e ν µ ν τ e µ τ, e R, µ R, τ R (1a) L ( ) ) * 3) W Z 1/2 ( - )
More informationBethe-Bloch Bethe-Bloch (stopping range) Bethe-Bloch FNAL (Fermi National Accelerator Laboratory) - (SciBooNE ) SciBooNE Bethe-Bloch FNAL - (SciBooNE
21 2 27 Bethe-Bloch Bethe-Bloch (stopping range) Bethe-Bloch FNAL (Fermi National Accelerator Laboratory) - (SciBooNE ) SciBooNE Bethe-Bloch FNAL - (SciBooNE ) Bethe-Bloch 1 0.1..............................
More informationcm λ λ = h/p p ( ) λ = cm E pc [ev] 2.2 quark lepton u d c s t b e 1 3e electric charge e color charge red blue green qq
2007 2007 7 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 1 2007 2 4 5 6 6 2 2.1 1: KEK Web page 1 1 1 10 16 cm λ λ = h/p p ( ) λ = 10 16 cm E pc [ev] 2.2 quark lepton 2 2.2.1 u d c s t b + 2 3 e 1 3e electric charge
More informationAppendix 1. CRC 13 Appendix Appendix LCGT 18 DECIGO 18 XMASS 19 GADZOOKS! 20 NEWAGE(
CRC 22 1 3 2 4 2-1 2-2 2-3 2-4 3 9 3-1 3-2 3-3 3-4 3-5 4 12 Appendix 1. CRC 13 Appendix 2. 14 Appendix 3. 17 LCGT 18 DECIGO 18 XMASS 19 GADZOOKS! 20 NEWAGE( ) 21 22 24 CTA (Cherenkov Telescope Array) 25
More informationPowerPoint Presentation
超高エネルギーニュートリノ観測の将来展望と ARA ν 千葉大学大学院理学研究科 ハドロン宇宙国際研究センター 吉田滋 The most energetic universe The Cosmic Rays Mostly protons Some light nuculei He, Li,. Heavy nuclei (ex. Fe) may dominate at higher energies
More information[2] ATMUKN [3] (ATMU ATMUKN)[4] ( ) X tr = f photo photo + f incoh incoh + f pair pair = E h 0 (2) h 0 E 1 f photo =1; X h 0 f incoh f pair =1;
2001 4 17 1 ICRP90 (AP ) ICRP 2 2.1 (photoelectric eect) (coherent scattering) (incoherent scattering) ( (pair creation) (triplet creation)) = photo + coh + incoh + pair (cm ;1 ) (1) (linear attenuation
More informationスライド 1
201381 43 1 AGN SNR Pulsar e P e + χ e - χ JEM-EF ISS CALET CALorimetric Electron Telescope 201381 43 2 JAPAN Aoyama Gakuin University Hirosaki University Institute for Cosmic Ray Research, University
More informationnews
ETL NEWS 1999.9 ETL NEWS 1999.11 Establishment of an Evaluation Technique for Laser Pulse Timing Fluctuations Optoelectronics Division Hidemi Tsuchida e-mail:tsuchida@etl.go.jp A new technique has been
More informationMott散乱によるParity対称性の破れを検証
Mott Parity P2 Mott target Mott Parity Parity Γ = 1 0 0 0 0 1 0 0 0 0 1 0 0 0 0 1 t P P ),,, ( 3 2 1 0 1 γ γ γ γ γ γ ν ν µ µ = = Γ 1 : : : Γ P P P P x x P ν ν µ µ vector axial vector ν ν µ µ γ γ Γ ν γ
More information24 10 10 1 2 1.1............................ 2 2 3 3 8 3.1............................ 8 3.2............................ 8 3.3.............................. 11 3.4........................ 12 3.5.........................
More information25 3 4
25 3 4 1 µ e + ν e +ν µ µ + e + +ν e + ν µ e e + TAC START STOP START veto START (2.04 ± 0.18)µs 1/2 STOP (2.09 ± 0.11)µs 1/8 G F /( c) 3 (1.21±0.09) 5 /GeV 2 (1.19±0.05) 5 /GeV 2 Weinberg θ W sin θ W
More information6 2 T γ T B (6.4) (6.1) [( d nm + 3 ] 2 nt B )a 3 + nt B da 3 = 0 (6.9) na 3 = T B V 3/2 = T B V γ 1 = const. or T B a 2 = const. (6.10) H 2 = 8π kc2
1 6 6.1 (??) (P = ρ rad /3) ρ rad T 4 d(ρv ) + PdV = 0 (6.1) dρ rad ρ rad + 4 da a = 0 (6.2) dt T + da a = 0 T 1 a (6.3) ( ) n ρ m = n (m + 12 ) m v2 = n (m + 32 ) T, P = nt (6.4) (6.1) d [(nm + 32 ] )a
More information輻射の量子論、選択則、禁制線、許容線
Radiative Processes in Astrophysics 005/8/1 http://wwwxray.ess.sci.osaka- u.ac.jp/~hayasida Semi-Classical Theory of Radiative Transitions r r 1/ 4 H = ( cp ea) m c + + eφ nonrelativistic limit, Coulomb
More informationX 20, 1 1 HETE-2 Swift CCD GRB CCD CCD CCD
CCD 04RP019 20 3 7 X 20, 1 1 HETE-2 Swift CCD GRB CCD CCD CCD 1 6 1.1................... 6 1.2................... 8 1.3....................... 10 1.4............. 10 1.5................. 13 2 15 2.1..........................
More informationMicrosoft PowerPoint - okamura.ppt[読み取り専用]
TKK の物理的可能性 an extension of the TK neutrino oscillation experiment with a far detector in Korea 岡村直利 ( 京大 基研 ) 関西セミナーハウス (007/03/7( 007/03/7) based on hep-ph/050406 [Phys.Lett.B637,66 (006)] hep-ph/060755
More information研修コーナー
l l l l l l l l l l l α α β l µ l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l
More information2005 4 18 3 31 1 1 8 1.1.................................. 8 1.2............................... 8 1.3.......................... 8 1.4.............................. 9 1.5.............................. 9
More informationpptx
Based on N. Nagata, S. Shirai, JHEP 1403 (2014) 049. Ø Ø Y. Okada, M. Yamaguchi, T. Yanagida (1991), H. E. Haber, R. Hempfling (1991) J. R. Ellis, G. Ridolfi, F. Zwirner (1991) Scalar Par cles Gravi no
More informationBig Bang Planck Big Bang 1 43 Planck Planck quantum gravity Planck Grand Unified Theories: GUTs X X W X 1 15 ev 197 Glashow Georgi 1 14 GeV 1 2
12 Big Bang 12.1 Big Bang Big Bang 12.1 1-5 1 32 K 1 19 GeV 1-4 time after the Big Bang [ s ] 1-3 1-2 1-1 1 1 1 1 2 inflationary epoch gravity strong electromagnetic weak 1 27 K 1 14 GeV 1 15 K 1 2 GeV
More information(Compton Scattering) Beaming 1 exp [i (k x ωt)] k λ k = 2π/λ ω = 2πν k = ω/c k x ωt ( ω ) k α c, k k x ωt η αβ k α x β diag( + ++) x β = (ct, x) O O x
Compton Scattering Beaming exp [i k x ωt] k λ k π/λ ω πν k ω/c k x ωt ω k α c, k k x ωt η αβ k α x β diag + ++ x β ct, x O O x O O v k α k α β, γ k γ k βk, k γ k + βk k γ k k, k γ k + βk 3 k k 4 k 3 k
More information1 223 KamLAND 2014 ( 26 ) KamLAND 144 Ce CeLAND 8 Li IsoDAR CeLAND IsoDAR ν e ν µ ν τ ν 1 ν 2 ν MNS m 2 21
1 3 KamLAND shimizu@awa.tohoku.ac.jp 014 ( 6 ) 1 31 1 KamLAND 144 Ce CeLAND 8 Li IsoDAR CeLAND IsoDAR.1 ν e ν µ ν τ ν 1 ν ν 3 3 3 MNS m 1 = 7.5 10 5 ev m 31 m 3 =.3 10 3 ev 100 m ν e [1] 71 Ga SAGEGallex
More informationuntitled
--- = ---- 16 Z 8 0 8 8 0 Big Bang 8 8 s-process 50 r-process 8 50 N r-process s-process Hydrogen 71% Helium 8% Others 1.9% Heay 4-4% lements(>ni p-process (γ process? r-process s-process Big Bang H,He
More informationLHC ALICE (QGP) QGP QGP QGP QGP ω ϕ J/ψ ALICE s = ev + J/ψ
8 + J/ψ ALICE B597 : : : 9 LHC ALICE (QGP) QGP QGP QGP QGP ω ϕ J/ψ ALICE s = ev + J/ψ 6..................................... 6. (QGP)..................... 6.................................... 6.4..............................
More information23 1 Section ( ) ( ) ( 46 ) , 238( 235,238 U) 232( 232 Th) 40( 40 K, % ) (Rn) (Ra). 7( 7 Be) 14( 14 C) 22( 22 Na) (1 ) (2 ) 1 µ 2 4
23 1 Section 1.1 1 ( ) ( ) ( 46 ) 2 3 235, 238( 235,238 U) 232( 232 Th) 40( 40 K, 0.0118% ) (Rn) (Ra). 7( 7 Be) 14( 14 C) 22( 22 Na) (1 ) (2 ) 1 µ 2 4 2 ( )2 4( 4 He) 12 3 16 12 56( 56 Fe) 4 56( 56 Ni)
More informationSpacecraft Propulsion Using Solar Energy Spacecraft with Magnetic Field Light from the Sun Solar Wind Thrust Mirror Solar Sail Thrust production by li
2004.3.28 物理学会シンポジウム 磁気プラズマセイル の可能性と 深宇宙探査への挑戦 宇宙航空研究開発機構 船木一幸 Spacecraft Propulsion Using Solar Energy Spacecraft with Magnetic Field Light from the Sun Solar Wind Thrust Mirror Solar Sail Thrust production
More informationB
B07557 0 0 (AGN) AGN AGN X X AGN AGN Geant4 AGN X X X (AGN) AGN AGN X AGN. AGN AGN Seyfert Seyfert Seyfert AGN 94 Carl Seyfert Seyfert Seyfert z < 0. Seyfert I II I 000 km/s 00 km/s II AGN (BLR) (NLR)
More informationX線分析の進歩36 別刷
X X X-Ray Fluorescence Analysis on Environmental Standard Reference Materials with a Dry Battery X-Ray Generator Hideshi ISHII, Hiroya MIYAUCHI, Tadashi HIOKI and Jun KAWAI Copyright The Discussion Group
More informationPowerPoint Presentation
2010 KEK (Japan) (Japan) (Japan) Cheoun, Myun -ki Soongsil (Korea) Ryu,, Chung-Yoe Soongsil (Korea) 1. S.Reddy, M.Prakash and J.M. Lattimer, P.R.D58 #013009 (1998) Magnetar : ~ 10 15 G ~ 10 17 19 G (?)
More informationMathews Grant J. (University of Notre Dame) Boyd Richard N. (Lawrence Livermore National Laboratory) 2009/5/21
Mathews Grant J. (University of Notre Dame) Boyd Richard N. (Lawrence Livermore National Laboratory) 2009/5/21 Abstract strongly interacting massive particles (SIMPs, X) Big Bang (BBN) X heavy colored
More informationJAXA Sep., 2010 p.1/36
JAXA Sep., 2 p./36 Contents Sep., 2 p.2/36 ffi(e;v) ) =3 dv (E=W M X ψ( ;u) W=W du P X ψ(w;u) ) =3 du (W=W n3:9 = 6 (H=H c ) 2=3 GeV =3 o =cm =W =3 ; with H c =4:4 3 G M X Comparison of the cross-sections
More information1.7 D D 2 100m 10 9 ev f(x) xf(x) = c(s)x (s 1) (x + 1) (s 4.5) (1) s age parameter x f(x) ev 10 9 ev 2
2005 1 3 5.0 10 15 7.5 10 15 ev 300 12 40 Mrk421 Mrk421 1 3.7 4 20 [1] Grassberger-Procaccia [2] Wolf [3] 11 11 11 11 300 289 11 11 1 1.7 D D 2 100m 10 9 ev f(x) xf(x) = c(s)x (s 1) (x + 1) (s 4.5) (1)
More informationMW鹿児島
NGC1068 Dark Matter Halo baryon gas stars SMBH SMBH 1 SMBHs? (AGN) AGN Seyfertization Taniguchi 1987, ApJ, 317, L57 AGN The dead quasar problem (Rees 1990, Science, 247, 817) T AGN ~ 10 8 yrs AGN AGN
More information1. 2. 3. 2010-02- 22-24 1.1 1.1.1 1.1.2 1.1.3 F10.7 1.2 1.2.1 1.2.2 1.2.3 14 C 1.2.4 10 Be 1.2.5 14 C 10 Be 1.1 太陽放射とその変動 20100223-24森羅万象学校 1.1.1 (from Encyclopedia of Earth) op1cal depth (Lean et al.,
More informationrcnp01may-2
E22 RCP Ring-Cyclotron 97 953 K beam K-atom HF X K, +,K + e,e K + -spectroscopy OK U U I= First-order -exchange - coupling I= U LS U LS Meson-exchange model /5/ I= Symmetric LS Anti-symmetric LS ( σ Λ
More information500 6 LHC ALICE ( 25 ) µsec MeV QGP
5 6 LHC ALICE shigaki@hiroshima-u.ac.jp chujo.tatsuya.fw@u.tsukuba.ac.jp gunji@cns.s.u-tokyo.ac.jp 3 ( 5 ) 5. µsec MeV QGP 98 RHIC QGP CERN LHC. LHC ALICE LHC p+p RHIC QGP ALICE 3 5 36 3, [, ] ALICE [,
More informationmain.dvi
SGC - 48 208X Y Z Z 2006 1930 β Z 2006! 1 2 3 Z 1930 SGC -12, 2001 5 6 http://www.saiensu.co.jp/support.htm http://www.shinshu-u.ac.jp/ haru/ xy.z :-P 3 4 2006 3 ii 1 1 1.1... 1 1.2 1930... 1 1.3 1930...
More information放射線化学, 97, 29 (2014)
20 5 Absorption spectra of biomolecules over wide energy range are very important to study their radiation effects in terms of the optical approximation proposed by Platzman. Using synchrotron radiation
More information磁性物理学 - 遷移金属化合物磁性のスピンゆらぎ理論
email: takahash@sci.u-hyogo.ac.jp May 14, 2009 Outline 1. 2. 3. 4. 5. 6. 2 / 262 Today s Lecture: Mode-mode Coupling Theory 100 / 262 Part I Effects of Non-linear Mode-Mode Coupling Effects of Non-linear
More information19 σ = P/A o σ B Maximum tensile strength σ % 0.2% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional
19 σ = P/A o σ B Maximum tensile strength σ 0. 0.% 0.% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional limit ε p = 0.% ε e = σ 0. /E plastic strain ε = ε e
More informationDrift Chamber
Quench Gas Drift Chamber 23 25 1 2 5 2.1 Drift Chamber.............................................. 5 2.2.............................................. 6 2.2.1..............................................
More information1 2 2 (Dielecrics) Maxwell ( ) D H
2003.02.13 1 2 2 (Dielecrics) 4 2.1... 4 2.2... 5 2.3... 6 2.4... 6 3 Maxwell ( ) 9 3.1... 9 3.2 D H... 11 3.3... 13 4 14 4.1... 14 4.2... 14 4.3... 17 4.4... 19 5 22 6 THz 24 6.1... 24 6.2... 25 7 26
More information/ Christopher Essex Radiation and the Violation of Bilinearity in the Thermodynamics of Irreversible Processes, Planet.Space Sci.32 (1984) 1035 Radiat
/ Christopher Essex Radiation and the Violation of Bilinearity in the Thermodynamics of Irreversible Processes, Planet.Space Sci.32 (1984) 1035 Radiation and the Continuing Failure of the Bilinear Formalism,
More informationELECTRONIC IMAGING IN ASTRONOMY Detectors and Instrumentation 5 Instrumentation and detectors
ELECTRONIC IMAGING IN ASTRONOMY Detectors and Instrumentation 5 Instrumentation and detectors 4 2017/5/10 Contents 5.4 Interferometers 5.4.1 The Fourier Transform Spectrometer (FTS) 5.4.2 The Fabry-Perot
More information1 2 3 4 1 2 3 4 5 1 2 3 4 5 1 2 3 4
1 2 3 4 1 2 3 4 5 1 2 3 4 5 1 2 3 4 -1- -2- 1-3- 2 3 - -4- nm 7. nm -5- APS Advanced Photon Source ESRF European Synchrotron Radiation Facility, APS ESRF, APS, ESRF, APS ESRF -6- 1,, APS ESRF APS ESRF
More informationMicrosoft PowerPoint - hoshino_part1.pptx
天体プラズマにおける粒子加速機構 無衝突系粒子シミュレーション 星野真弘理学系研究科 地惑惑星科学専攻 内容 ** PIC (Particle In Cell) シミュレーション ** プラズマ輸送係数の研究 (MHD では現象論的に扱う粘性 電気抵抗 熱伝導に関わる物理 ) 非熱的プラズマ ( 局所的熱平衡ではない物理 ) 電子とイオンのエネルギー分配 宇宙での高エネルギー粒子の観測 数値チェレンコフ問題
More information1 9 v.0.1 c (2016/10/07) Minoru Suzuki T µ 1 (7.108) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1)
1 9 v..1 c (216/1/7) Minoru Suzuki 1 1 9.1 9.1.1 T µ 1 (7.18) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1) E E µ = E f(e ) E µ (9.1) µ (9.2) µ 1 e β(e µ) 1 f(e )
More information201711grade1ouyou.pdf
2017 11 26 1 2 52 3 12 13 22 23 32 33 42 3 5 3 4 90 5 6 A 1 2 Web Web 3 4 1 2... 5 6 7 7 44 8 9 1 2 3 1 p p >2 2 A 1 2 0.6 0.4 0.52... (a) 0.6 0.4...... B 1 2 0.8-0.2 0.52..... (b) 0.6 0.52.... 1 A B 2
More information¼§À�ÍýÏÀ – Ê×ÎòÅŻҼ§À�¤È¥¹¥Ô¥ó¤æ¤é¤® - No.7, No.8, No.9
No.7, No.8, No.9 email: takahash@sci.u-hyogo.ac.jp Spring semester, 2012 Introduction (Critical Behavior) SCR ( b > 0) Arrott 2 Total Amplitude Conservation (TAC) Global Consistency (GC) TAC 2 / 25 Experimental
More information銀河団衝突にともなう 高温ガスの運動がひきおこす特徴的な磁場構造 (Takizawa 2008 ApJ, 687, 951)
JVLA S-band and X-band Polarimetry of Abell 2256 Ozawa,,,,,Takizawa, Takahashi,,,,et al. to be submitted to PASJ 滝沢元和 2015.5.8 研究室談話会 Introduction: 銀河団 可視光 ( 数 100 個の銀河の集まり ) X 線数 kev の高温ガス ( シンクロトロン )
More informationuntitled
MPPC 18 2 16 MPPC(Multi Pixel Photon Counter), MPPC T2K MPPC T2K (HPK) CPTA, MPPC T2K p,π T2K > 5 10 5 < 1MHz > 15% 200p.e. MIP 5p.e. p/π MPPC HPK MPPC 2 1 MPPC 5 1.1...................................
More informationBH BH BH BH Typeset by FoilTEX 2
GR BH BH 2015.10.10 BH at 2015.09.07 NICT 2015.05.26 Typeset by FoilTEX 1 BH BH BH BH Typeset by FoilTEX 2 1. BH 1.1 1 Typeset by FoilTEX 3 1.2 2 A B A B t = 0 A: m a [kg] B: m b [kg] t = t f star free
More informationO1-1 O1-2 O1-3 O1-4 O1-5 O1-6
O1-1 O1-2 O1-3 O1-4 O1-5 O1-6 O1-7 O1-8 O1-9 O1-10 O1-11 O1-12 O1-13 O1-14 O1-15 O1-16 O1-17 O1-18 O1-19 O1-20 O1-21 O1-22 O1-23 O1-24 O1-25 O1-26 O1-27 O1-28 O1-29 O1-30 O1-31 O1-32 O1-33 O1-34 O1-35
More information案 A 003b-2 放 射 線 を 科 学 的 に 理 解 す る 右側の緑の人 放射 線 鳥居 寛之 小豆川勝見 渡辺雄一郎 著 中川 恵一 執筆協力 基 礎 か ら わ か る 東 大 教 養 の 講 義 新刊書籍 発売 2012年10月10日 刊行 を に 的 学 科 理解する 基礎からわか
案 A 003b-2 放 射 線 を 科 学 的 に 理 解 す る 右側の緑の人 放射 線 鳥居 寛之 小豆川勝見 渡辺雄一郎 著 中川 恵一 執筆協力 基 礎 か ら わ か る 東 大 教 養 の 講 義 新刊書籍 発売 2012年10月10日 刊行 を に 的 学 科 理解する 基礎からわかる東大教養の講義 放射線を科学的に理解する 基礎からわかる東大教養の講義 鳥居寛之 小豆川勝見 渡辺雄一郎
More informationReport10.dvi
[76 ] Yuji Chinone - t t t = t t t = fl B = ce () - Δθ u u ΔS /γ /γ observer = fl t t t t = = =fl B = ce - Eq.() t ο t v ο fl ce () c v fl fl - S = r = r fl = v ce S =c t t t ο t S c = ce ce v c = ce v
More information(Blackbody Radiation) (Stefan-Boltzmann s Law) (Wien s Displacement Law)
( ) ( ) 2002.11 1 1 1.1 (Blackbody Radiation).............................. 1 1.2 (Stefan-Boltzmann s Law)................ 1 1.3 (Wien s Displacement Law)....................... 2 1.4 (Kirchhoff s Law)...........................
More informationmuramatsu_ver1.key
229-ThTES α = e 2 /2ε 0 hc (John D. Barrow 2005) Radiationdominated era Matterdominated era Dark energy era 10 3 10 4 10 5 10 6 10 7 10 8 10 9 10 10 Time (years) Time 2 α = e 2 /2ε 0 hc (John D. Barrow
More informationq quark L left-handed lepton. λ Gell-Mann SU(3), a = 8 σ Pauli, i =, 2, 3 U() T a T i 2 Ỹ = 60 traceless tr Ỹ 2 = 2 notation. 2 off-diagonal matrices
Grand Unification M.Dine, Supersymmetry And String Theory: Beyond the Standard Model 6 2009 2 24 by Standard Model Coupling constant θ-parameter 8 Charge quantization. hypercharge charge Gauge group. simple
More informationtsuchiya_090307
2/26 雷活動からのX線やガンマ線(1) 短時間バースト 継続時間:ミリ秒かそれ以下 自然の雷放電および誘来放電からの観測 衛星による大気上層からの観測(TGFs) Dwyer et al. 2003 Smith et al. 2005 長時間バースト もんじゅ 継続時間:数秒から数分 もんじゅHPより 雷放電に必ずしも同期しない おもに雷雲中 日本海側の冬季や高山で観測 される McCarthy
More information