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The primary cosmic ray composition between 10**15 and 10**16 eV from Extensive Air Showers electromagnetic and TeV muon data

Authors :
Aglietta M.
Alessandro B.
Antonioli P.
Arneodo F.
Bergamasco L.
Bertaina M.
Castagnoli C.
Castellina A.
Chiavassa A.
Cini G.
D'Ettorre Piazzoli B.
di Sciascio G.
Fulgione W.
Galeotti P.
Ghia P. L.
Iacovacci M.
Mannocchi G.
Morello C.
Navarra G.
Saavedra O.
Stamerra A.
Trinchero G. C.
Valchierotti S.
Vallania P.
Vernetto S.
Vigorito C.
Ambrosio M.
Antolini R.
Baldini A.
Barbarino G. C.
Barish B. C.
Battistoni G.
Bellotti R.
Bemporad C.
Bernardini P.
Bilokon H.
Bower C.
Brigida M.
Bussino S.
Cafagna F.
Calicchio M.
Campana D.
Carboni M.
Caruso R.
Cecchini S.
Cei F.
Chiarella V.
Choudhary B. C.
Coutu S.
de Cataldo G.
Dekhissi H.
de Marzo C.
de Mitri I.
Derkaoui J.
de Vincenzi M.
di Credico A.
Erriquez O.
Favuzzi C.
Forti C.
Fusco P.
Giannini G.
Giglietto N.
Grassi M.
Grillo A.
Guarino F.
Gustavino C.
Habig A.
Hanson K.
Heinz R.
Iarocci E.
Katsavounidis E.
Katsavounidis I.
Kearns E.
Kim H.
Kyriazopoulou S.
Lamanna E.
Lane C.
Levin D. S.
Lipari P.
Longley N. P.
Longo M. J.
Loparco F.
Maaroufi F.
Mancarella G.
Mandrioli G.
Marini A.
Martello D.
Marzari Chiesa A.
Mazziotta M. N.
Michael D. G.
Monacelli P.
Montaruli T.
Monteno M.
Mufson S.
Musser J.
Nicolò D.
Nolty R.
Orth C.
Osteria G.
Palamara O.
Patera V.
Patrizii L.
Pazzi R.
Peck C. W.
Perrone L.
Petrera S.
Popa V.
Rainò A.
Reynoldson J.
Ronga F.
Satriano C.
Scapparone E.
Scholberg K.
Sciubba A.
Sitta M.
Spinelli P.
Spinetti M.
Steinberg R.
Stone J. L.
Sulak L. R.
Surdo A.
Tarlé G.
Togo V.
Vakili M.
Walter C. W.
Webb R.
BECHERINI, YVONNE
CHIARUSI, TOMMASO
COZZI, MICHELA
GIACOMELLI, GIORGIO MARIA
GIORGINI, MIRIAM
MARGIOTTA, ANNARITA
SIOLI, MAXIMILIANO
SIRRI, GABRIELE
SPURIO, MAURIZIO
M., Aglietta
B., Alessandro
P., Antonioli
F., Arneodo
L., Bergamasco
M., Bertaina
C., Castagnoli
A., Castellina
A., Chiavassa
G., Cini
B., D’Ettorre Piazzoli
G., Di Sciascio
W., Fulgione
P., Galeotti
P. L., Ghia
M., Iacovacci
G., Mannocchi
C., Morello
G., Navarra
O., Saavedra
A., Stamerra
G. C., Trinchero
S., Valchierotti
P., Vallania
S., Vernetto
C., Vigorito
M., Ambrosio
R., Antolini
A., Baldini
G. C., Barbarino
B. C., Barish
G., Battistoni
Y., Becherini
R., Bellotti
C., Bemporad
Bernardini, Paolo
H., Bilokon
C., Bower
M., Brigida
S., Bussino
F., Cafagna
M., Calicchio
D., Campana
M., Carboni
R., Caruso
S., Cecchini
F., Cei
V., Chiarella
B. C., Choudhary
S., Coutu
M., Cozzi
G., De Cataldo
H., Dekhissi
C., De Marzo
DE MITRI, Ivan
J., Derkaoui
M., De Vincenzi
A., Di Credico
O., Erriquez
C., Favuzzi
C., Forti
P., Fusco
G., Giacomelli
G., Giannini
N., Giglietto
M., Giorgini
M., Grassi
A., Grillo
F., Guarino
C., Gustavino
A., Habig
K., Hanson
R., Heinz
E., Iarocci
E., Katsavounidi
I., Katsavounidi
E., Kearn
H., Kim
S., Kyriazopoulou
E., Lamanna
C., Lane
D. S., Levin
P., Lipari
N. P., Longley
M. J., Longo
F., Loparco
F., Maaroufi
Mancarella, Giovanni
G., Mandrioli
A., Margiotta
A., Marini
Martello, Daniele
A., Marzari Chiesa
M. N., Mazziotta
D. G., Michael
P., Monacelli
T., Montaruli
M., Monteno
S., Mufson
J., Musser
D., Nicolo'
R., Nolty
C., Orth
G., Osteria
O., Palamara
V., Patera
L., Patrizii
R., Pazzi
C. W., Peck
Perrone, Lorenzo
S., Petrera
V., Popa
A., Raino'
J., Reynoldson
F., Ronga
C., Satriano
E., Scapparone
K., Scholberg
A., Sciubba
P., Serra
M., Sioli
G., Sirri
M., Sitta
P., Spinelli
M., Spinetti
M., Spurio
R., Steinberg
J. L., Stone
L. R., Sulak
A., Surdo
G., Tarle'
V., Togo
M., Vakili
C. W., Walter
R., Webb
Aglietta M.
Alessandro B.
Antonioli P.
Arneodo F.
Bergamasco L.
Bertaina M.
Castagnoli C.
Castellina A.
Chiavassa A.
Cini G.
D'Ettorre Piazzoli B.
di Sciascio G.
Fulgione W.
Galeotti P.
Ghia P. L.
Iacovacci M.
Mannocchi G.
Morello C.
Navarra G.
Saavedra O.
Stamerra A.
Trinchero G. C.
Valchierotti S.
Vallania P.
Vernetto S.
Vigorito C.
Ambrosio M.
Antolini R.
Baldini A.
Barbarino G. C.
Barish B. C.
Battistoni G.
Becherini Y.
Bellotti R.
Bemporad C.
Bernardini P.
Bilokon H.
Bower C.
Brigida M.
Bussino S.
Cafagna F.
Calicchio M.
Campana D.
Carboni M.
Caruso R.
Cecchini S.
Cei F.
Chiarella V.
Chiarusi T.
Choudhary B. C.
Coutu S.
Cozzi M.
de Cataldo G.
Dekhissi H.
de Marzo C.
de Mitri I.
Derkaoui J.
de Vincenzi M.
di Credico A.
Erriquez O.
Favuzzi C.
Forti C.
Fusco P.
Giacomelli G.
Giannini G.
Giglietto N.
Giorgini M.
Grassi M.
Grillo A.
Guarino F.
Gustavino C.
Habig A.
Hanson K.
Heinz R.
Iarocci E.
Katsavounidis E.
Katsavounidis I.
Kearns E.
Kim H.
Kyriazopoulou S.
Lamanna E.
Lane C.
Levin D. S.
Lipari P.
Longley N. P.
Longo M. J.
Loparco F.
Maaroufi F.
Mancarella G.
Mandrioli G.
Margiotta A.
Marini A.
Martello D.
Marzari-Chiesa A.
Mazziotta M. N.
Michael D. G.
Monacelli P.
Montaruli T.
Monteno M.
Mufson S.
Musser J.
Nicolò D.
Nolty R.
Orth C.
Osteria G.
Palamara O.
Patera V.
Patrizii L.
Pazzi R.
Peck C. W.
Perrone L.
Petrera S.
Popa V.
Rainò A.
Reynoldson J.
Ronga F.
Satriano C.
Scapparone E.
Scholberg K.
Sciubba A.
Sioli M.
Sirri G.
Sitta M.
Spinelli P.
Spinetti M.
Spurio M.
Steinberg R.
Stone J. L.
Sulak L. R.
Surdo A.
Tarlé G.
Togo V.
Vakili M.
Walter C. W.
Webb R.
Publication Year :
2004
Publisher :
Amsterdam Netherlands: Elsevier BV -Amsterdam : North-Holland, 2004.

Abstract

The cosmic ray primary composition in the energy range between 10**15 and 10**16 eV, i.e., around the "knee" of the primary spectrum, has been studied through the combined measurements of the EAS-TOP air shower array (2005 m a.s.l., 10**5 m**2 collecting area) and the MACRO underground detector (963 m a.s.l., 3100 m w.e. of minimum rock overburden, 920 m**2 effective area) at the National Gran Sasso Laboratories. The used observables are the air shower size (Ne) measured by EAS-TOP and the muon number (Nmu) recorded by MACRO. The two detectors are separated on average by 1200 m of rock, and located at a respective zenith angle of about 30 degrees. The energy threshold at the surface for muons reaching the MACRO depth is approximately 1.3 TeV. Such muons are produced in the early stages of the shower development and in a kinematic region quite different from the one relevant for the usual Nmu-Ne studies. The measurement leads to a primary composition becoming heavier at the knee of the primary spectrum, the knee itself resulting from the steepening of the spectrum of a primary light component (p, He). The result confirms the ones reported from the observation of the low energy muons at the surface (typically in the GeV energy range), showing that the conclusions do not depend on the production region kinematics. Thus, the hadronic interaction model used (CORSIKA/QGSJET) provides consistent composition results from data related to secondaries produced in a rapidity region exceeding the central one. Such an evolution of the composition in the knee region supports the "standard" galactic acceleration/propagation models that imply rigidity dependent breaks of the different components, and therefore breaks occurring at lower energies in the spectra of the light nuclei.

Details

Database :
OpenAIRE
Accession number :
edsair.dedup.wf.001..734739fa7fea0ed6d6d5bf8cfc66887a