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M.Tamada Kinki University

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1 M.Tamada Kinki University
Air showers accompanied by high energy atmospheric families observed by Chacaltaya hybrid experimemt M.Tamada Kinki University ICRC2007, Merida ; 10 Jul. 07

2 H.Aoki、K.Honda, N.Inoue, T.Ishii, N.Kawasumi, N.Martinic,
N.Ochi, N.Ohmori, A.Ohsawa, M.Tamada and R.Ticona

3 (Mt. Chacaltaya, 5200m, Bolivia)
45 scintillation counters

4 emulsion chamber burst detector hadron calorimeter

5 EAS-array: shower size, Ne
time, theta, phi time, position Hadron calorimeter: burst size, nb position, theta, phi Emulsion chamber: atmospehric family (ng,nh,SEg, SEh, E≥2TeV)

6 Coupling the family with the accompanied air shower
1. List the families in one block of the emulsion chamber 2. List the bursts which have their centers on the concerned block 3. Correspond the families to the bursts 4. Examine the consistency of the arrival direction, position between family and air shower Coupling rate ~ 80 % <Dq>=5.4 ± 0.5 deg, <Df>=17.0 ± 1.8 deg, <DR>=0.49 ± 0.04m

7 Selection of the events
Air-showers Shower-size : Ne ≥ 106 & families: Eg, Eh(g) ≥ 2TeV Ng ≥ 5, Eg ≥2TeV (SEg ≥10TeV) 72 events in m2year exposure of emulsion chambers

8 Simulations EAS above the detector
CORSIKA v QGSJET01c, Sibyll 2.1 shower size : NKG-option Ecut=0.3GeV for hadrons, muons Ecut=0.003GeV for e,gamma Proton-dominant primary composition Heavy-dominant primay composition 20,000 events E0≥1015eV 6,000 events E0≥1016eV

9 Simulations inside the emulsion chamber
(e,g) & hadrons in the families Hadron-Pb int. : QGSJET01 EM-cascade : Okamoto-Shibata algorithm electron number ---> spot darkness shower transition on spot darkness fitting using standard cascade curve : DT, E(g) showers of DT > 6 c.u. : hadron-induced

10 effect of gap between neighboring blocks
families: Ng ≥ 5, Eg≥2TeV (SEg≥10TeV) in a block

11 effect of gap between neighboring blocks
Random sampling of family-center in the emulsion chamber area including gaps of two neighboring blocks 613 among 2108 families with Ne ≥ 7 x 106 have its center outside the emulsion chamber. Effective area is 1.41 times of emulsion chambers : 1.41 x 8 m2 = m2

12 air showers accompanied by families SEg≥10TeV
Proton-dominant-composition sampled primary particles air showers accompanied by families SEg≥10TeV

13 heavy-dominant-composition
sampled primary particles air showers accompanied by families SEg≥10TeV

14 EAS triggered family Proton-dominant

15 EAS triggered family

16 distribution of normalized family energy
E0 ~ Ne x 2 GeV f = SEg/E0

17 proton-dominant

18 observed events are mainly due to Fe-primaries !?

19 lateral spread of g-rays in the family
107 ≤ Ne < 108 QGSJET01c Sibyll 2.1

20 lateral spread of g-rays in the family
QGSJET01c Sibyll

21 107 ≤ Ne < 108

22 106 ≤ Ne < 107

23 size spectrum of air showers with families
Chacaltaya

24 observed number of EAS with families is smaller than expectation in Ne<107.

25 106 ≤ Ne < 107

26 conclusion How is in Tibet Asg data ?
Models can not well describe characteristics of air-shower triggered families with Ne≥106 • necessary to check validity of interaction model; Ne-SEg, Ne-sp., ER-sp., Correlation etc. How is in Tibet Asg data ? • necessary more statistics of EAS with families ! • necessary to modify the model of nuclear interactions !?


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