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“The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra INFN and University, Torino, Italy For the EAS-TOP Collaboration XIII International Symposium on Very High Energy Cosmic Ray Interactions Pylos Greece, 6 -12 September 2004

“The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

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“The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra INFN and University, Torino, Italy For the EAS-TOP Collaboration. XIII International Symposium on Very High Energy Cosmic Ray Interactions Pylos Greece, 6 -12 September 2004. EAS-TOP at LNGS - PowerPoint PPT Presentation

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Page 1: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

 “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. NavarraINFN and University, Torino, ItalyFor the EAS-TOP Collaboration

XIII International Symposium on Very High Energy Cosmic Ray InteractionsPylos Greece, 6 -12 September 2004

Page 2: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

EAS-TOP at LNGSCampo Imperatore 2000 m a.s.l. 820 g.cm-2 data taking: 1989-2000

Page 3: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

The Cosmic

Ray primary

spectrum

THE HIGH ENERGY GALACTIC RADIATION

KNEEDIRECT EXP.

Page 4: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

EAS-TOP

Energy range from the direct measurements up to above the knee:Cosmic Ray primary spectrum & compositionVerification of the hadronic physics

DETECTORS:HADRONS ATMOSPHERIC C.l.ELECTROMAGNETICMUONS (E > 1 GeV)+ MUONS (E > 1.3 TeV)Deep underground GS labs.: MACRO, LVD

Page 5: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

EAS-TOP: THE CALORIMETER& MUON TRACKER

8 x 13 cm Fe layers; 144 m2 streamer + q. proportional tubes

Page 6: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

DETECTORS & METHODS

Hadrons p-spectrum @ E0 ~ 0.5 - 50 TeV

Cherenkov light + TeV muons p, He, CNO fluxes @ E0 ~ 100 TeV

e.m. spectrum in “knee” region E0 ~ 103 - 104 TeV

e.m. + GeV muons composition in “knee” region

e.m. + TeV muons composition in “knee” region

Verifications of methods and HE physics used

e.m. anisotropies & search for gamma primaries

CORSIKA-QGSJET

Page 7: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Size and energy spectra:

Ne Eo

Astrop. Phys. 10 (1999) 1

Page 8: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Ne-N distributions

3-component fit: L, CNO, H in LogNe = 0.2 intervals of Ne

2 = i (fci – fexp

i)2/i2 fci = wLfsL

i + wCNOfsCNOi + wHfsH

i

Simulations with = 2.75 spectraL = “p” or “50%p + 50% He” ; CNO = N; H = Fe

Frac

tion

of

even

ts

Frac

tion

of

even

ts

Page 9: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

The composition in the ‘knee’ region

Mass group Heavier primary spectra harder Ek Z ?

l > 3.1

CNO ~ 2.75

Fe = 2.3 – 2.7

Page 10: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

TeV muon multiplicity fits in MACRO (TeV )

L = p + He

H = Mg + Fe

L+H

Measured

Page 11: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

EAS-TOP & MACRO (TeV )

L = p + He H = Mg + Fe

Astrop. Phys., 20 (2004) 641

Page 12: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

< ln A > vs. E0

Page 13: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

particle and energy flux in p-p

MACRO EAS-TOP

E. M.

Page 14: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

The hadronic interaction models (CORSIKA)

Primary protons:

N Ne

= 0.820 ± 0.007

= 0.792 ± 0.007

= 0.789 ± 0.008

= 0.77 ± 0.02

Page 15: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Evolution of composition< Ne-N

EXP= 0.907 ± 0.004

EXTRCMP= 0.79 ± 0.02

MAX-VENUS= 0.820 ± 0.007

QGSJET: agreement with extrapolated direct measurements!

NO INTERACTION MODEL CAN ACCOUNT FOR THE INCREASING N vs. Ne WITHOUT INCREASING PRIMARY MASS

Page 16: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Component dominating at the “knee”?

He – p spectra similar RUNJOB

He spectrum harder JACEE

From “direct” measurements:JACEE

RUNJOB

JACEERUNJOBEAS-TOP

Page 17: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

THE EAS-TOP CHERENKOV DETECTOR

2 wide angle detectors per telescope(MIRROR: A = 0.5 m2 , f.l. = 40 cm , f.o.v. = 0.16 sr)

equipped with 7 photomultipliers (d = 6.8 cm , f.o.v. = 0.023 sr)

Trigger threshold: Nphe,th = 120 phe / mirror (Ethr 40 TeV at r = 130 m) Trigger rate: 7 Hz/telescopeCherenkov event: coincidence in T = 30 ns , between any 2 corresponding PMs.

5

MACRO UndergroundGran Sasso Labs.depth: 3100 m w.e. Eth ~ 1.3 TeV 76.6 x 12 x 4.8 m

< 1o

20 m at surface level

Astrop. Phys., 21 (2004) 223

Proc. 28th ICRC, 1 (2003) 115

A different approach: EAS-TOP & MACRO

Page 18: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

EAS-TOP (Cherenkov detector):

total energy through the amplitude

of the detected Cherenkov light signal.

MACRO (muondetector):

EAS primaries with En > 1.3 TeV/n

EAS geometry through the track

( r ~ 20 m, ~ 10 uncertainties)

MACRO and EAS-TOP are separated by 1100-1300 m of rock: E 1.3 - 1.6 TeV

Page 19: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

DATA SET

t = 7s

September 1998 – May 2000

Tot. Time T = 208 h

5 telescopes

exposure 830 day m2 sr

angular window:

: 16 < < 58 , 127 < <

210

MACRO events in T and :

35814

with EAS-TOP in t = 7s:

3830

(expected accidental events < 3.0)

Event coincidence is established

off-line (GPS system - T < 1s)

Coincidence Peak

tMACRO–t Cherenkov (s)

t = 7s

7

Page 20: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

E ≈ 80 TeV Np ≈ N

He

E ≈ 250 Tev Np ≈ N

He ≈ NCNO

C.l. yield: p ~ He ~ CNO

p

He

CNO

Fe

C.l. + TeV muon analysis

Mg

Page 21: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

p, He, CNO @ ~ 100-200 TeVInformation EAS-TOP

& MACROJACEE RUNJOB

Jp+He

(80 TeV)

18 ± 4 12 ± 3 8 ± 2

Jp+He+CNO

(250 TeV)

1.1 ± 0.3 0.7 ± 0.2 0.5 ± 0.1

Jp/ Jp+He

(80 TeV)

0.29 ± 0.09 0.45 ± 0.12 0.63 ± 0.20

Jp+He/ Jp+He+CNO

(250 TeV)

0.78 ± 0.17 0.70 ± 0.20 0.76 ± 0.25

JHe

(80 TeV)

12.7 ± 4.4 6.4 ± 1.4 3.1 ± 0.7

x 10-7 m-2s-1sr-1TeV-1

EAS-TOP & MACRO data

EAS-TOP & MACRO data + p-flux

p+He p+He+CNO

Page 22: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

The Cherenkov light LDF

WITH JACEE FLUX

Test of energy release in the atmosphere of QGSJET:

R = (42 m) / (134 m)

= Ne (370 g/cm2) / Ne (505 g/cm2)

(Rexp – Rth)/Rth = 0.14 ± 0.09

Page 23: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Ne and N spectra

Ne N

Page 24: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Sec Ik*107 Nk chi**2/df m-2s-1sr-1

1.00-1.05 2.56 2.96 0.06 1.1 0.1 6.08 0.03 7.8/111.05-1.10 2.56 2.86 0.05 1.3 0.2 5.95 0.04 8.4/111.10-1.15 2.56 2.84 0.04 1.0 0.1 5.95 0.04 5.3/111.15-1.20 2.56 2.82 0.08 0.8 0.2 5.92 0.06 7.6/111.20-1.25 2.56 2.92 0.09 0.5 0.1 5.94 0.05 4.6/111.25-1.30 2.56 2.75 0.07 1.4 0.4 5.62 0.07 2.8/11

chi**2/df (1slope)1.00-1.05 3.21 0.06 3.42 0.10 1.2 0.3 4.65 0.10 10.4/10 18.7/121.05-1.10 3.18 0.08 3.45 0.10 1.4 0.2 4.65 0.10 9.3/10 20.7/121.10-1.15 3.18 0.09 3.40 0.20 0.6 0.2 4.75 0.15 6.9/10 9.9/121.15-1.20 3.12 0.15 3.4 0.10 1.6 0.5 4.55 0.15 5.9/10 14/12

Agreement inside errors (~ 30%)

2 slopes

Decreasing with increasing zenith angle

Ne

N

N Ne

= (e –1) /(-1) = 0.7 – 0.8

In agreement with models SAME BENDING COMPONENT ?

Page 25: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

IFSAME BENDING COMPONENTin Ne and N spectra

We can identify it.

We construct for each component (p, He, CNO, Mg, Fe) the energy spectrum fitting the size spectrum in the region of the knee.

From such energy spectra we construct for each component the corresponding N spectrum, to be compared with the measured one.

The result of such comparison

Page 26: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Muon size spectrum: measured and expected for different primaries

on the base of the Ne spectrum

If “Knee” on Helium primaries

Ek (He) = (3.5 0.3) 1015 eV

VENUS

QGSJET

NEXUS

Page 27: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

The primary spectrum from EAS-TOP

Page 28: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Natural evolution…..

KASCADE-Grande

Page 29: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

KASCADE-Grande

If : E k,Z = Z * E k,1

SEARCH FOR IRON “KNEE” AT ~ 1017 eV

PRIMARY COMPOSITION: 1016 - 1018 eV

STUDY OF C.R. INTERACTIONS AT UHE

N (> 1018 eV) ~ 250 (3 y data taking)

At the threshold of Auger (High Resolution)

P,He

iron

Eknee = 3 – 4 PeV

EAS-TOP/KASCADE

Page 30: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

Hadron spectrum at 820 g/cm2 & comparison with sea level (1033 g/cm2)

Calculated QGSJET

Exp. KASCADE/EAS-TOP

Page 31: “The Cosmic Ray composition in the knee region and the hadronic interaction models” G. Navarra

E0 = 0.5 – 50 TeVProton spectrum at TOP

Astrop. Phys. 19 (2003) 329 He contribution subtracted

S(Eo) = (9.8 1.1stat 1.6sys) 10–5 (Eo/1000) –2.80 0.06 m-2 s-1 sr-1 GeV-1