the cosmic ray air shower and its radio detection
DESCRIPTION
The Cosmic Ray Air Shower and its Radio Detection. 陈学雷 国家天文台. C osmic Ray Energy S pectrum. The maximum energy observed so far is about 3.2x10 20 eV eq. 50 J Many discoveries in particle physics: positron, muon, pion, Kaon, ... Now: astrophysical side. EAS Exp. O rigin of Cosmic Ray. - PowerPoint PPT PresentationTRANSCRIPT
The Cosmic Ray Air Shower and its Radio Detection
陈学雷
国家天文台
EAS
Exp.
Cosmic Ray Energy Spectrum
The maximum energy observed so far is about
3.2x1020eV eq. 50 J
Many discoveries in particle physics: positron, muon, pion, Kaon, ...
Now: astrophysical side
Origin of Cosmic Ray
Fermi acceleration
Propagation of Cosmic Ray
charged particle moving in random magnetic field
E< 1015 eV, confined around galaxy
(some diffuse out)
Puzzle of Ultra High Energy Cosmic Ray: the GZK cutoff
Greisen 1966, Zatsepin & Kuzmin 1966
Possible solutions
• Incorrect measurement? Heavy nuclei?
• produced nearby: superheavvy dark matter? topological defects?
• produced nearyby: strong IGM magnetic field?
• produced far away: neutrino?
• produced far away: break down of relativity (violation of Lorentz invariance)?
GZK or not?
Detection of air showers
• Ground Array: small area emulsion, scintillator, water Cherenkov
• Optical: low duty cycle atmosphere Cherenkov Fluorescence
• radio: large area, high duty cycle
Radio Signal
Geosynchrotron (Kahn & Lerche 1966) charge seperation by geomagnetic field
Negative charge excess in EAS and radio signal (Askayran 1962): production of delta-ray (knocked out electrons) annihilation of positron in flight
First detection (Jelley et al 1965)
Review (Allan 1971), loss of interest
Revival (Falcke & Gorham 2002)
CASA-MIA, LOPES/LOFAR, CODALEMA
EM wave ~ apparant acceleration of electric charge
Coherent Emission: Radio Pulse
Radio pulse for a 1017 eV shower, at 0, 100,250 m from axis (Huege & Falcke astro-ph/0309622)
Signal Strength
Allan’s formula:
Spectrum
Monte Carlo Simulation by Huege & Falcke, astro-ph/0501580,
at 20m, 140m, 260m, 380m, 500m
distribution and polarization
total EW pol NS pol vertical pol
0o
30o
60o
90o
Energy Dependence
Background Noise
Falcke & Gorham, astro-ph/0207226
LOPESLOfar PrototypE Station
Measurements of air showers in the energy range E0 = 100 TeV - 1 EeV
KASCADE-Grande= KArlsruhe Shower Core and Array
DEtector + Grande
•10 antennas at KASCADE array•frequency band 40-80 MHz•trigger: >10/16 cluster of KASCADE
( E0 > 1016 eV)•2004: 7 months runtime•~630.000 triggered events
(and correlated EAS information) sufficient sample of events for detailed analyses
Progress
LOPES-10
LOPES-30
LOPES-STAR, LOPES-Auger
LOPES collaboration, Nature 425 (2005) 313
LOPES 10 Results
CODALEMA experiment
current setup (astro-ph/0608550)
Nancay DAM
COsmic ray Detection Array with Logarithmic ElectroMagnetic Antennas
Auger Detector
Results
Radio Detection in China
• relatively easy and cheap
• particularly suitable for UHECR
• not yet well-developed, room for exploration
• technology spin-off (application in military & technology)
Road Map
(1) concept design
(2) preliminary test: site selection, RFI background, instrument basics
(3) prototype: 4-10 antenna
(4) after analyzing prototype data, decide what to do
(5) Large scale deployment: core array for lower energy (10 17 eV) flux and sparse array for high energy. Area: 103-4 km2 with spacing 0.5-1 km.
prototype proposal
已申请本年度天文联合基金(仪器研制类重点项目 , 200万)
PI: 陈学雷
coI:施浒立 , 秦波等
Preliminary Design
• center frequency: 30 MHz
• wide bandwidth or multi-band (to overcome artificial RFI which is usually narrow band)
• multi-polarization loaded-dipole/half-wave antenna (ominidirectional, wide and smooth frequency response)
Amplification: 30-40 dB (to 0.1 V signal)
ADC: 10-100 MHz, 14 bit,
Simulated detection rate
Site Selection
西藏羊八井 : coincidence test (AS, ARGO) but: (1) high altitude, (2) RFI, (3) too far
内蒙正镶白旗: good EM environment, nearby, logistics readybut need coincidence detector, est. 100k per piece (Cao Zhen)
Plan
2008年,研究大气簇射射电机制,设计模拟程序,进行天线和探测系统的初步设计、试制和实验室检测,对羊八井和正镶白旗站址进行测试, 对数据处理方法进行调研和初步设计;与国外有关研究人员联系,探讨国际合作研究的可能性。
2009年,完成大气簇射射电模拟程序并进行模拟研究,对天线和探测系统进行野外测试和优化,设计、调试数据处理软件,邀请国外有关专家参与实验。
2010年,收集数据并进行分析处理,研究大规模宇宙线实验的可行性。