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GAMMA Experiment. Rigidity-dependent cosmic ray energy spectra in the knee region obtained with the GAMMA experiment. 4 Y.Gallant, 1 A.Garyaka, 2 A.D.Erlykin 5 L.Jones, 1 R.Martirosov, 2 N.Nikolskaya, 3 J.Procureur, 1 S.Ter-Antonyan. 1 Yerevan Physics Institute - PowerPoint PPT Presentation
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04/21/23 1
Rigidity-dependent cosmic ray energy spectra in the Rigidity-dependent cosmic ray energy spectra in the knee region obtained with the GAMMA experimentknee region obtained with the GAMMA experiment
Astroparticle Physics 28/2 (2007) 169/ arXiv: 0704.320v1 [astro-ph]
4Y.Gallant, 1A.Garyaka, 2A.D.Erlykin5L.Jones, 1R.Martirosov,2N.Nikolskaya,
3J.Procureur, 1S.Ter-Antonyan
1 Yerevan Physics Institute2 Moscow Physics Institute
3 Centre d Etudes Nucleaires Bordeaux-Gradignan, 4 Universite Montpellier II
5 University of Michigan
GAMMA ExperimentGAMMA Experiment
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GAMMA FacilityGAMMA Facility
GAMMA ExperimentGAMMA Experiment
• Location: Armenia, Mt.Aragats 3200 m a.s.l.
• EAS array: 33x3 (1x1x0.05) m3+ +9 (0.3x0.3x0.05) m3
• Muon hall: 2500 g/cm2 of rock 150 (1x1x0.05)m3
• EAS data:
Nch > 5 105 (100%)
R < 25 m (50 m)
< 300
N(R<50m) > 103
E > 5 GeV
T = 6.2107 sec
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Measurement errors and particle spectra
GAMMA ExperimentGAMMA Experiment
/)( k
Ln(Nch ) 0.1, s0.05, x,y0.5-1m, 1.50
Ln(N ) 0.35-0.2 at N(R<50m)103-105
15 detectors
Particle density spectra
Single particle spectra
Ri < 50 m
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Detector response
)(
)()(
,dE
MeV1eEANch EGS
NKG
ch
ch
N
N δ
s(7m < ri < 90m)
)()()( ,E1EA de MeVsEGSNKG ss δ
CORSIKA(EGS,NKG)NA=200, A p, He, O, Fe
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A SIBYLL2.1 QGSJET01 Emin [PeV]
P 1.0·105 1.0·105 0.5
He 7.1·104 6.0·104 0.7
O 4.6·104 4.4·104 1.0
Fe 4.8·104 4.0·104 1.2
Ee, > 1 MeVE > 150 MeVMuon hall:
E > 4 GeV (e,FLUKA)
CORSIKA6.031(NKG)
GAMMA ExperimentGAMMA Experiment
Emax= 50000 PeVPeV = -1.5 < 300
R < 25m
Simulated database: WA(EA , X) {A, EA} X(Ne , Nµ , Nh , s , x0 , y0 , θ, )
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EAS Inverse Problem:EAS Inverse Problem: A
AA dEEfXEWXF )(),()(
kkZZ EEEEf /)( 1 i
2iFiFii
2 FF )]/()~
[( ,~,
3) 4D-Analysis, F(X) d4F/dNedNds dcos, nd.f.= 1640
1) Combined Analysis, nd.f.= 350
2) 2D-Analysis, F(X) d2F/dNedN , nd.f.= 240
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Primary energy spectra
kkZZ E
EEEf 1)(
0206821 .. kEE0301932 .. kEE
Rk EZE
1 = 0.0950.008 [m-2s-1sr-1TeV-1]
2 = 0.100.012
3-16 = 0.0430.007 ( O - like )
17-26 = 0.0240.004 ( Fe - like )
ER = 2500200 TV
2/nd.f. 2.0 B.Wiebel & P.Biermann, 24th ICRC (1995)
A.Lagutin et al., 29th ICRC (2005)
Results of 1-2D Combined AnalysisSIBYLL
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Verification Enlarged EAS data (R<50m)
Test of KASCADE primary energy spectra
WZ(E,X) fZ(E) dE = F(X)
Knee positions
by GAMMA EAS data
z
fp , fHe , fO=fC+fSi , fFe
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Conclusion The obtained primary energy spectra strongly depend on interaction model. The SIBYLL interaction model is more preferable. Rigidity-dependent spectra describe the EAS data at least up to E~100 PeV.All-particle primary energy spectrum slightly depends on interaction model.
The energy spectra of primary nuclei disagree with the same KASCADE data in 1-100 PeV energy range, however, the discrepancies of the all-particle energy spectra obtained by the GAMMA and KASCADE are sufficiently small (~20%).
GAMMA ExperimentGAMMA Experiment