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Fermi_Diffuse_ASJ_2009Sep.ppt
FermiFermi--LAT Study of LAT Study of Galactic CosmicGalactic Cosmic--Rays Rays yyby Observing Diffuse by Observing Diffuse
GammaGamma--raysraysGammaGamma raysrays(Fermi(Fermi衛星による拡散衛星による拡散γγ線放射の観測と銀河系線放射の観測と銀河系線放射の観測と銀河系線放射の観測と銀河系
宇宙線宇宙線))Ts nef miTs nef mi Mi noMi noTsunefumiTsunefumi MizunoMizuno
Hiroshima Univ.Hiroshima Univ.on behalf of the Fermion behalf of the Fermi--LAT LAT
Tsunefumi Mizuno 1
CollaborationCollaborationASJ 2009 Autumn MeetingASJ 2009 Autumn Meeting
September 15, 2009, Yamaguchi, JapanSeptember 15, 2009, Yamaguchi, Japan
Fermi_Diffuse_ASJ_2009Sep.pptIntroduction Introduction 銀河宇宙線と拡散銀河宇宙線と拡散γγ線放射線放射
HE γ-rays are produced via interactions between Galactic cosmic-rays (CRs) and the interstellar medium (or interstellar radiation field)
(CR accelerator) (Interstellar space) (Observer)
X,γISMSNR SNR
RX J1713RX J1713--39463946Chandra Suzaku
(CR accelerator) (Interstellar space) (Observer)
e+-
diffusiondiffusionHESS
B
PP
Chandra, Suzaku, Radio telescopes
ICISRFdiffusiondiffusionenergy losses energy losses
reaccelerationreaccelerationconvectionconvection
etcetcπ0Pulsar,
μ-QSO
HeHeCNOCNO
ACT d Fermi
gase +-
π+-etc.etc. ACTs and Fermi(see K. Hayashi’s talk)gas
π(GMC is one of the best
target matter)
Pioneering theoretical works by Hayakawa (1952), Morrison (1958), etc.
Tsunefumi Mizuno 2
A powerful probe to study CRs in distant locationsPioneering theoretical works by Hayakawa (1952), Morrison (1958), etc.
拡散γ線は宇宙線を探るプローブ
Fermi_Diffuse_ASJ_2009Sep.ppt
FermiFermi衛星による拡散衛星による拡散γγ線放射の観測線放射の観測 (1)(1)
[1]: GMCs (e.g., Orion, Cham): matter distribution, correlation with mol. gas tracer[2]: Mid/low-latitude region (EGRET GeV excess). submitted to PRL.See also ArXiv:0907.0294
[3]: Mid/high latitude region to study local CRs (Abdo et al 2009; contact: T Mizuno)
Tsunefumi Mizuno 3
[3]: Mid/high-latitude region to study local CRs. (Abdo et al. 2009; contact: T. Mizuno)[4]: Galactic plane (CR distribution in the MW)
[1]~[3]について、これまでの結果を簡単に紹介(次項)[4]について若干詳しく
Fermi_Diffuse_ASJ_2009Sep.ppt
FermiFermi衛星による拡散衛星による拡散γγ線放射の観測線放射の観測 (2)(2)
[2]: non-GeV-excessGeV-excessの否定
EGRETLATOrion MC
(M~105M )
0.1 1 10 GeV
(M 10 Msun)[1]:GMCs物質分布
[3]: local CRs
LAT datamodel for the LIS
[3]: local CRs近傍の宇宙線はLISに酷似
nucleon-nucleonCham MC(M~104Msun)
Tsunefumi Mizuno 4
electron-bremsstrahlung
Fermi_Diffuse_ASJ_2009Sep.ppt
銀河系内の宇宙線分布銀河系内の宇宙線分布• CR distribution in our Galaxy is a key to understand their origin and propagation• Distribution of SNRs not well measured• Previous Gamma-ray data suggests a flatter distribution than SNR/pulsar distributions (e.g., Strong et al. 2004)
宇宙線の空間分布は、起源・伝播を探る鍵
G l
• Fermi-LAT is able to map out CR distributions in the Galaxy with unprecedented accuracy• Large scale analysis in progress.Gal.
Center
Large scale analysis in progress. (arXiv:0907.0304)
• We will focus on the preliminary l i f th 3rd d t ( t
Inner Galaxy
Outer
analysis of the 3rd quadrant (outer Galaxy). See also the relevant study of the 2nd quadrant (arXiv:0907.0312)
local arm
Tsunefumi Mizuno 5
GalaxyPerseus arm
銀河系の外側の領域の結果の紹介
Fermi_Diffuse_ASJ_2009Sep.ppt
FermiFermi--LATLATのカウントマップのカウントマップ• One of the best studied regions in γ-rays
Vela, Geminga, Crab and Orion A/B• Galactic plane between Vela and Geminga (green square) is ideal to study diffuse γ-rays and CRs.
small point source contamination, kinematically well-separated arms (local arm and Perseus arm) 宇宙線分布の研究に適した領域
VelaGeminga
Vela
Crab
Orion A/B
Tsunefumi Mizuno 6Count Map (E>100 MeV)
Orion A/B
Fermi_Diffuse_ASJ_2009Sep.ppt
ΓΓ線線 = = 星間物質からの放射星間物質からの放射++点源点源Local arm
+2 HI maps(profile fitting technique;+
Perseus arm
(profile fitting technique;arXiv:0907.0312)
詳細は林の講演参照(Q28a)• Fit γ-ray data with 8 maps + 15 point sources (11 month source list)
詳細は林の講演参照(Q28a)
L l
)• CR spectrum (γ-ray emissivity) is assumed to be uniform in each Galactocentric ringLocal arm
+ 1 CO map + excess E(B-V) map (Grenier et al. 2005)+ IC map (galprop model) + point sources (11 month list)
Galactocentric ring
Tsunefumi Mizuno 7
+ IC map (galprop model) + point sources (11 month list)
I(E, l, b) = ΣA(E)*HI(l,b) + ΣB(E)*Wco(l,b) +Σothers+Σpoint_sources
Fermi_Diffuse_ASJ_2009Sep.ppt
ΓΓ線スペクトル線スペクトル (~(~宇宙線スペクトル宇宙線スペクトル))HI Emissivity Spectrum of each ring
(local arm)(interarm)(P )(Perseus arm)
Point sources with Ts>=100 are included in the fitting宇宙線陽子で1-100GeVに対応(主成分)
• Emissivity (CR) spectrum of local arm (R=8.5-10 kpc) is slightly smaller than the model for LIS• Decreasing emissivity (local arm => interarm => Perseus arm) are consistent with decreasing CR density across the Galaxy 宇宙線の強度分布・スペクトルが得られた
Tsunefumi Mizuno 8
decreasing CR density across the Galaxy• Similar CR spectral shape up to R=16 kpc• Can constrain the CR source distribution and propagation parameters
study in progress
宇宙線の強度分布・スペクトルが得られたモデルとの比較で宇宙線源や伝播に制限
Fermi_Diffuse_ASJ_2009Sep.ppt
SummarySummary• Diffuse gamma-ray emission is a powerful probe to study the CR (and matter) distribution in distant locations in our Galaxy• Extensive analysis by Fermi-LAT is in progressExtensive analysis by Fermi-LAT is in progress
individual GMCsnon-GeV-excessMid/high-latitude region (local CRs)
拡散γ線放射は宇宙線を探るプローブ様々な成果(分子雲,non-GeV-excess,近傍の宇宙線)
Mid/high-latitude region (local CRs)large scale analysis (CR distribution throughout the
Galaxy)• Preliminary analysis of the 3rd quadrant is disucssed• Preliminary analysis of the 3rd quadrant is disucssed
See also the relevant study of the 2nd quadrantSimilar CR spectral shape up to R=16 kpcCR d it di t t d th t G l i bt i dCR density gradient toward the outer Galaxy is obtained
Comparison with the CR source/propagation model prediction is in progress 銀河系、とくに外側の領域で宇宙線分布が
あきらか なり ある
Tsunefumi Mizuno 9Thank you for your attention!あきらかになりつつある
Fermi_Diffuse_ASJ_2009Sep.ppt
Backup SlidesBackup SlidesBackup SlidesBackup Slides
Tsunefumi Mizuno 10
Fermi_Diffuse_ASJ_2009Sep.ppt
LAT LAT vsvs prepre--Fermi ModelFermi Model• Compare with a CR propagation model prediction based on pre-F i CR d t (St t l 2004 LATFermi CR data (Strong et al. 2004, Porter et al. 2008)π0-decay, e-Brems, Inverse Compton
LATmodel total
π0-decay
• Source and isotropic (w/ residual BG) component come from fitting the data to the sky above 30 deg
ICe-Bremsthe data to the sky above 30 deg latitude with model fixed • Although there is a uniform
b th d l d t iexcess above the model, data is reasonably reproduced by the model
Th d l i f l id i i i i i
Tsunefumi Mizuno 11
The model is successful considering it is a priori pre-Fermi model
Fermi_Diffuse_ASJ_2009Sep.ppt
Probing CRs using GammaProbing CRs using Gamma--rays from ISMrays from ISM• Correlation with gas column density reveals the CR spectrum• Fermi-LAT’s high performance + CR propagation model (e.g. GALPROP) to predict IC
S iti it i ifi tl i dSensitivity significantly improvedISM
(e.g., LAB HI survey)(http://www.astro.uni-bonn.de/~webaiub/english/tools_labsurvey.php)
Gamma-ray intensity(Fermi LAT data)
Mid/high latitude region & Galactic plane:Study of the local CRs and CR gradient in the outer Galaxy
Tsunefumi Mizuno 12GCsun
(From Wikipedia)
Fermi_Diffuse_ASJ_2009Sep.ppt
Accurate Measurements of Local CRs (1)Accurate Measurements of Local CRs (1)Mid-high lat. region in 3rd quadrant:
• small contamination of IC and molecular gas• correlate γ-ray intensity and HI• correlate γ-ray intensity and HI gas column densityAbdo et al. 2009, accepeted by ApJ(arXiv:0908.1171) contact author: TM
(error bars are statistical only)
ity 1 6 2 3 G V400-560 MeV
400-566 MeV
HI column density (1020 cm-2)
y In
tens
i 1.6-2.3 GeV400-560 MeV
E2x γ-
ray
Tsunefumi Mizuno 13HI column density (1020 cm-2)
Fermi_Diffuse_ASJ_2009Sep.ppt
Accurate Measurement of Local CRs (2)Accurate Measurement of Local CRs (2)• Best quality γ-ray emissivity spectrum in 100 MeV-10 GeV (Tp = 1-100 GeV)• Agree with the model prediction from the local interstellar spectrum (LIS)
EGRET (Digel et al. 2001)
LAT datamodel from the LIS ( g )
nucleon-nucleon
electron-bremsstrahlung
• Prove that local CR nuclei spectra are close to those directly
102 103 MeV 104
Tsunefumi Mizuno 14
measured at the Earth• Eγ<100 MeV constrain the e- spectrum
Fermi_Diffuse_ASJ_2009Sep.ppt
CR Flux DistributionCR Flux Distribution
LAT “measured” CR density
SNR distribution by radio survey or traced by pulsar
• Emissivity gradient traces the CR density. Robust against the thresholds for point sources included. • Significantly flatter than the SNR distributions
may indicate more CR sources than previously thought in the outer Galaxy large
Tsunefumi Mizuno 15
may indicate more CR sources than previously thought in the outer Galaxy, large halo size, etc.
• Comparison with the model prediction is in progress.
Fermi_Diffuse_ASJ_2009Sep.ppt
HI MapsHI MapsR<=10 kpc R<=10-12.5 kpc
R<=12.5-16 kpc R>=16 kpc
Tsunefumi Mizuno 16