3-cosmic_ray1

Similar documents
13-darkenergy

< C6AFC1FD28B1C7C7F5C1DF292E687770>

12-bbcosmology2


KAERI/RR-2245/2001 : 원전 주기적 안전성 평가기술 개발 : 방사선 안전성능 및 환경방사선 감시기술 개발

1 n dn dt = f v = 4 π m 2kT 3/ 2 v 2 mv exp 2kT 2 f v dfv = 0 v = 0, v = /// fv = max = 0 dv 2kT v p = m 1/ 2 vfvdv 0 2 2kT = = vav = v f dv π m

e01.PDF

1 뮤온 검출기의 측정 각도에 따른 뮤온 검출량 변화의 분석 배 기 훈 무룡고등학교, 울산 (2015년 2월 3일 받음) 뮤온 검출기의 측정 각도에 따른 단위 시간당 뮤온 검출량의 변화를 분석하고, 감소 추세를 계산하여 결과값을 분석, 원인을 추론하였다.

목차 ⅰ ⅲ ⅳ Abstract v Ⅰ Ⅱ Ⅲ i

29 Ⅰ. 서론 물리학자들이 전파의 이론을 정립한 이후, 이를 기술적으로 실현함은 물론 적정 수준의 19세기 물리학자인 페러데이, 맥스웰, 헤르츠 등의 연구 결과로 인류는 전기장과 자기장의 변화 에 따른 전파를 만들어 낼 수 있게 되었고, 인류에 게 있어 없어서는 안되

(Vacuum) Vacuum)? `Vacua` (1 ) Gas molecular/cm 3

Slide 1

03 장태헌.hwp

<C1B6BBE7BFF9BAB85F335F28C3D6C1BE292E687770>

슬라이드 제목 없음

KSKSKSKS SKSKSKS KSKSKS SKSKS KSKS SKS KS KS C 3004 KS C

THE JOURNAL OF KOREAN INSTITUTE OF ELECTROMAGNETIC ENGINEERING AND SCIENCE Mar.; 25(3),

Vertical Probe Card Technology Pin Technology 1) Probe Pin Testable Pitch:03 (Matrix) Minimum Pin Length:2.67 High Speed Test Application:Test Socket

82-01.fm

15(4장1절 P).PDF

歯99-16.PDF

유해중금속안정동위원소의 분석정밀 / 정확도향상연구 (I) 환경기반연구부환경측정분석센터,,,,,,,, 2012

KAERI/AR-636/2002 : 技術現況分析報告書 : 방사선 계측기술 및 중성자 계측기 기술 개발 현황

서강대학교 기초과학연구소대학중점연구소 심포지엄기초과학연구소

<C8ADB7C220C5E4C3EBC0E52E687770>

입자와 물질과의 상호작용

Precipitation prediction of numerical analysis for Mg-Al alloys

현대대학물리학 12(415~456p)

저작자표시 - 비영리 - 변경금지 2.0 대한민국 이용자는아래의조건을따르는경우에한하여자유롭게 이저작물을복제, 배포, 전송, 전시, 공연및방송할수있습니다. 다음과같은조건을따라야합니다 : 저작자표시. 귀하는원저작자를표시하여야합니다. 비영리. 귀하는이저작물을영리목적으로이용할

歯전용]

박선영무선충전-내지

(Exposure) Exposure (Exposure Assesment) EMF Unknown to mechanism Health Effect (Effect) Unknown to mechanism Behavior pattern (Micro- Environment) Re

THE JOURNAL OF KOREAN INSTITUTE OF ELECTROMAGNETIC ENGINEERING AND SCIENCE Jul.; 27(7),

歯제2장.PDF

THE JOURNAL OF KOREAN INSTITUTE OF ELECTROMAGNETIC ENGINEERING AND SCIENCE Nov.; 25(11),

현대대학물리학 36(545~583p)

THE JOURNAL OF KOREAN INSTITUTE OF ELECTROMAGNETIC ENGINEERING AND SCIENCE Dec.; 27(12),

1112 물리 화학 N ok.indd

-


00....

사용자 설명서 SERVO DRIVE (FARA-CSD,CSDP-XX)

<3034B1E2B9DD32302DBAB8B0EDBCAD2D DC0FCC6C4C0DABFF BAB0C3A53420C8A8B3D7C6AEBFF6C5A9292E687770>

04 박영주.hwp

Ä¡¿ì³»ÁöÃÖÁ¾

<BDC9BEEEBDBA D >

환경중잔류의약물질대사체분석방법확립에 관한연구 (Ⅱ) - 테트라사이클린계항생제 - 환경건강연구부화학물질연구과,,,,,, Ⅱ 2010


untitled

롯데여 영원하라

12.077~081(A12_이종국).fm

KAA2005.9/10 Ãâ·Â

歯174구경회.PDF

제 3 편

02-1기록도전( )

03-1영역형( )

목 록( 目 錄 )

µµÅ¥¸àÆ®1

Backlight Unit의 광학적 특성 해석 및 Prism Sheet의 최적화 설계

44(3)-16.fm

THE JOURNAL OF KOREAN INSTITUTE OF ELECTROMAGNETIC ENGINEERING AND SCIENCE. vol. 29, no. 10, Oct ,,. 0.5 %.., cm mm FR4 (ε r =4.4)

Microsoft PowerPoint - 7-Work and Energy.ppt

September Vol

°¡°Ç6¿ù³»ÁöÃÖÁ¾

October Vol

<B9E9B3E2C5CDBFEFB4F5B5EBBEEE20B0A1C1A4B8AE20B1E6C0BB20B0C8B4C2B4D92E687770>

특집....,.,., (good jobs) (rent-sharing) (fairness)..... Ⅱ. 임금과생산성구조의분석모형 ) 1),,,, 2_ 노동리뷰

<3136C2F720C6F7B7B3BFF8B0ED2E687770>

한약재품질표준화연구사업단 고삼 ( 苦參 ) Sophorae Radix 생약연구과

12(4) 10.fm

170

006- 5¿ùc03ÖÁ¾T300çÃâ

164

¼º¿øÁø Ãâ·Â-1

12.2 Molecular Spectroscopy ( 분자분광학 ) 분자에전자기복사선을쪼여주면분자가낮은에너지상태에서높은에너지상태로이동하게되며, 이때특정흡수진동수를이용하여분자의구조를알아낼수있다. Figure 12.1 : Absorption of energy in elec

학습법 2 초등 수학 서술형 평가 대비법 수식을 문장으로, 문장을 수식으로 바꾸는 연습해야 2009 개정교육과정이 도입되면서부터 초등과정 수학이 어려워졌다. 타 교과 간 연계성이 강화되고, 문제 해결 능력과 서술형 답을 요구하는 문제가 늘어나고 있기 때문이다. 특히 서

<313920C0CCB1E2BFF82E687770>

untitled

전기정보 11월(내지).qxp

Microsoft PowerPoint - [ ][금요과학터치]-upload 버전.ppt

개최요강

Ⅰ. 머리말 각종 기록에 따르면 백제의 초기 도읍은 위례성( 慰 禮 城 )이다. 위례성에 관한 기록은 삼국사기, 삼국유사, 고려사, 세종실록, 동국여지승람 등 많은 책에 실려 있는데, 대부분 조선시대에 편 찬된 것이다. 가장 오래된 사서인 삼국사기 도 백제가 멸망한지

THE JOURNAL OF KOREAN INSTITUTE OF ELECTROMAGNETIC ENGINEERING AND SCIENCE Jun.; 27(6),

1. Features IR-Compact non-contact infrared thermometer measures the infrared wavelength emitted from the target spot and converts it to standard curr

QYQABILIGOUI.hwp

untitled

<BACFC7D1B3F3BEF7B5BFC7E22D3133B1C733C8A BFEB2E687770>


09È«¼®¿µ 5~152s

歯49손욱.PDF

untitled

Microsoft PowerPoint - ch25ysk.pptx

KAERIAR hwp

04 최진규.hwp

Microsoft PowerPoint - ch03ysk2012.ppt [호환 모드]

<BFECBCF6B1E2BCFAC0DAB7E1C1FDB3BBC1F62DC3D6C1BE2D312E706466>

FTTH 기술발표


½Éº´È¿ Ãâ·Â

QbD 적용을위한품질심사해설서 ( 예시 )

Transcription:

Special Topics in Nuclear and Particle Physics Astroparticle Physics Lecture 3 Cosmic Rays Sept. 15, 2015 Sun Kee Kim Seoul National University

High Energy Cosmic rays? >,? > ( )? > source & acceleration mechanism

: (98%), (2%) : 87%, 12%, : 1% :,

20km 까지증가 40km 까지감소 50km 이상일정 > 무엇인가외부로부터와서대기와의반응에의해증가한후대기에의해서흡수된다.

(2 ) 1 2. N + N π 's,k 's,! p + p,n + n,! hadronic shower, EM shower hadron, π + µ + +ν µ π µ +ν µ τ = 2.6 10 8 s (Electromagnetic shower), π 0 γγ τ = 8 10 17 s

(2 ) 1 π + µ + +ν µ τ = 2.6 10 8 s cτ = 7.8m 1 GeV: γ =1/0.14 ~ 7 γβcτ ~ 55m 100 GeV: γ =1/0.14 ~ 714 γβcτ ~ 5.5km 100 GeV 100 GeV µ + e + +ν e +ν µ τ = 2.2 10 6 s cτ = 660m 3 GeV: γ =3/0.1 ~ 30 γβcτ ~ 20km, 80% : 70 / m 2 /s/sr at 1 GeV 1/ cm 2 /min

(2 )

(2 ) / : 1 p + N p + N + kπ + kπ + + mπ 0 p + N n + N + kπ + (k +1)π + + mπ 0 N(π + ) N(π ) = 2k +1 2k = 1+ 1 2k k 2 N(π + ) N(π ) 1.25 N(µ + ) N(µ ) 1.27 PDG

Vertical flux measurement of muons

Muons at Surface

Stopping power Bethe-Bloch equation maximum energy transfer : : : ( ) minimum at βγ 3.5 minimum ionizing particle *equivalent thickness g/cm 2 g/cm 2 /ρ(g/cm 3 ) cm MeV/(g/cm 2 ) ρ(g/cm 3 ) MeV/cm

de dx & = $ % de dx #! " rad & + $ % de dx #! " coll Radiation length ( de / dx) rad = E / X 0 E = E 0 e x/x 0 σ rad 2 2 ( e / mc ) 2 ~ 300 m Critical energy E C ~ 0.56 cm

de dx & = $ % de dx #! " rad = be µ & + $ % de dx #! " = a coll

ν µ + N µ + N

Electromagnetic Shower Shower stops at E<Ec N( t) 2 E( t) E E( t max t 0 / 2 ) = E 0 t / t 2 max = E c t max N max E = ln E E 0 0 c / ln 2 / E c ~9.6 MeV for Pb ~100 MeV for air Radiation length

Electromagnetic Shower Longitudinal Shower profile ( EGS4 Simulation ) lateral spread à Moliere radius 90%(99%) contained in 1 (3.5)R M

Hadronic Shower Hadron interaction Interaction length λ I 17

Hadronic Shower

Hadronic Shower

Hadronic Shower ( ) 1030 g/cm 2 : ~ 27 X 0, ~12λ I x = X exp( h / H ) X=1030 g/cm 2, H = 6.5 km

(Balloon, Satelite) protons ~ 87%, He ~ 12% Li, Be, B produced by interaction - - 2

(<1 GeV/n).

Cosmic ray energy spectrum 1 GeV 10 15 ev power law

Measurement of cosmic ray energy spectrum E.S.Seo(2014)

Direct measurement of primary cosmic ray 1,, ) Calorimeter : sampling EM component ATIC, CREAM, Fermi-LAT Spectrometer : sign of charge, momenta AMS, PAMELA,

BESS Spectrometer with a Superconducting magnet(1t) TOF ODC MAGNET JET/IDC

BESS

ATIC Thin calorimeter, balloon borne experiment

CREAM Thin calorimeter, balloon & ISS de/dx : Silicon charge detector of CREAM for cosmic ray measurment

de/dx : Silicon charge detector of CREAM for cosmic ray measurment de / dx z 2

Indirect measurement of primary cosmic ray - Extensive air shower 1 air shower Particle counting : Ground Detector Array scintillators, water cherenkov detectors Air fluorescence : Telescope Hybrid : Telescope + ground detector array * :,

Extensive Air Shower Air shower ( E 0 >100 TeV ) shower core : number of muons above 1GeV at ground level * Ne : total number of charged particles number of muons/m 2 at distance r from the shower core

Air shower simulation Extensive Air Shower Watson (2002)

Extensive Air Shower Composition : Shower maximum depth λ I ~ 80 g/cm 2 for proton ~ 15 g/cm 2 for Fe Shower maximum depth 1. Watson (2002)

Air Shower Measurement Air fluorescence detectors samples longitudinal shower profile Ground arrays sample the shower front

Cosmic Ray Experiments for UHECRs Past Volcano Ranch, USA à Scintillators Haverah Park, UK à Water Cerernkov SUGAR, Austrailia à Scintillators Fly s Eye, USA à Fluorescence Future Telescope Array Auger North à Fluorescence + Scintillator Present Yakutsk, Russia à Scintillators, atmospheric cerenkov Agasa, Japan à Scintillators, Muon detectors HiRes, USA à Fluorescence Auger-South, USA à Fluorescence à Water Cerenkov Telescope Array à Fluorescence à Scintillator array

Air Shower Measurement Ground detector array by Ground detector array 1% : 100% duty cycle ~O(m 2 ) Plastic scintillator Water Cherenkov detector

AGASA ~100 km 2

AGASA

Air Shower Measurement by Fluorescence telescope Air fluorescence detectors duty cycle ~10% Fly s eye (or HiRes)

Pierre Auger Observatory 3000 km 2 Hybrid : ground detector array(water Cherenkov) + fluorescent detector 27 FD at 5 station FD : 440 PMTs

Auger-South 12,000 liter x 1600 1.5 km Lateral density distribution Fitted Electromagnetic Shower

Telescope Array (TA) 730 km 2 Hybrid : ground detector array(scintillator) + fluorescent detector 3m 2 Scint. x 507 1.3 km

Telescope Array (TA) 730 km 2 Hybrid : ground detector array(scintillator) + fluorescent detector

Greisen-Zatsepin-Kuzmin (GZK) Cutoff (Cosmic Microwave Background). Cosmic microwave background (CMB) ρ γ 400 / cm 3 T γ = 2.725K E γ E γ = kt = 8.617 10 5 ev/k 2.725K=2.35 10 4 ev 6 10 4 ev Photoproduction γ + p (Δ + ) p + π 0 n + π +

p p = (E p,p p ) p γ = (E γ = p γ,p γ ) p p + p γ = (E p + p γ,p p + p γ ) (p p + p γ ) 2 = (E p + p γ ) 2 (p p + p γ ) 2 = E 2 2 2 2 p + p γ + 2Ep p γ p p pγ 2p p p γ = m 2 p + 2E p p γ 2p p p γ = m 2 p + 2E p E γ (1 cosθ) = m 2 p + 4E p E γ p p = (E p = m p,0) p π 0 = (E π 0 = m π 0,0) p p + p π 0 = (m p + m π 0,0), (p p + p π 0 ) 2 = m 2 p + m 2 π 0 + 2m p m π 0 m 2 p + 4E p E γ = m 2 p + m 2 π 0 + 2m p m π 0 E p = m 2 + 2m π 0 p m π 0 4E γ = m 0 (2m π p + m π 0 ) 4E γ E γ 6 10 4 ev E p 10 20 ev

10 20 ev UHECR on the atmosphere or on a detector S = ( p 1 + 2 p p p ) CM energy 1 2 2 2 2E 1 m N 450 TeV 2 10 20 ev 10 9 ev Two orders of magnitude higher than LHC!!

Radio Emission from Cosmic Ray Air Shower Geo-synchrotron radiation of electrons in the shower Radio-wave below 100 MHz Discovered in 1965 by Jelly et al.(nature 205, 327) Difficulties in radio measurement/interpretation of data Shifted to Ground arrays/fluorescence tecniques Digital data processing technology Renaissance?

LOPES A LOFAR Prototype Station LOPES at KASCADE-Grande Detection and imaging of atmospheric radio flashes from cosmic ray air shower, LOPES collaboration, Falcke et al, 2005, Nature, May 19

LOFAR LOFAR : Radio telescope array for 10-210MHz with >100 km baseline, www.lofar.org ADetecting cosmic rays with the LOFAR radio telescope A&A 560, A98(2013)