SI-28(S-32) FRAGMENTATION AT 3.7A, 14.6A AND 200A GEV

被引:22
作者
ADAMOVICH, MI
AGGARWAL, MM
ALEXANDROV, YA
AMIRIKAS, R
ANDREEVA, NP
ANZON, ZV
ARORA, R
AVETYAN, FA
BADAYAL, SK
BAKICH, AM
BASOVA, ES
BAZAROV, IK
BHALLA, KB
BHASIN, A
BHATIA, VS
BOGDANOV, VG
BRADNOVA, V
BUBNOV, VI
BURNETT, TH
CAI, X
CARSHIEV, DA
CHASNIKOV, IY
CHERNOVA, LP
CHERNYAVSKI, MM
DHAMIA, S
ELIGBAEVA, GZ
EREMENKO, LE
GAITINOV, AS
GANSSAUGE, ER
GARPMAN, S
GERASSIMOV, SG
GRAF, C
GROTE, J
GULAMOV, KG
GUPTA, SK
GUPTA, VK
JAKOBSSON, B
JUST, L
KACHROO, S
KALYACHKINA, GS
KANYGINA, EK
KARABOVA, M
KITROO, S
KHARLAMOV, SP
KOVALENKO, AD
KARSNOV, SA
KUMAR, V
LARIONOYA, VG
LI, YD
LIU, LS
机构
[1] ACAD SINICA, INST HIGH ENERGY PHYS, BEIJING, PEOPLES R CHINA
[2] PANJAB UNIV, DEPT PHYS, CHANDIGARH 160014, INDIA
[3] HUNAN EDUC INST, DEPT PHYS, CHANGSHA, PEOPLES R CHINA
[4] JOINT INST NUCL RES, HIGH ENERGIES LAB, DUBNA, RUSSIA
[5] UNIV RAJASTHAN, DEPT PHYS, JAIPUR 302004, RAJASTHAN, INDIA
[6] UNIV JAMMU, DEPT PHYS, JAMMU, INDIA
[7] SAFARIK UNIV, DEPT NUCL PHYS & BIOPHYS, KOSICE, SLOVAKIA
[8] SHANXI NORMAL UNIV, DEPT PHYS, LINFEN, PEOPLES R CHINA
[9] LUND UNIV, DEPT PHYS, LUND, SWEDEN
[10] UNIV MARBURG, FACHBEREICH PHYS, W-3550 MARBURG, GERMANY
[11] PN LEBEDEV PHYS INST, COSM PHYS LAB, MOSCOW 117924, RUSSIA
[12] UNIV WASHINGTON, DEPT PHYS, SEATTLE, WA 98195 USA
[13] VG KHOLPIN RADIUM INST, ST PETERSBURG, RUSSIA
[14] UNIV SYDNEY, SCH PHYS, SYDNEY, NSW 2006, AUSTRALIA
[15] UKBEK ACAD SCI, INST NUCL PHYS,RELATIVIST NUCL PHYS LAB, TASHKENT 702132, UZBEKISTAN
[16] PHYS TECH INST, HIGH ENERGIES LAB, TASHKENT, UZBEKISTAN
[17] HUA ZHONG NORMAL UNIV, INST PARTICLE PHYS, WUHAN 430070, PEOPLES R CHINA
[18] YEREVAN PHYS INST, YEREVAN 375036, ARMENIA
来源
ZEITSCHRIFT FUR PHYSIK A-HADRONS AND NUCLEI | 1995年 / 351卷 / 03期
关键词
D O I
10.1007/BF01290914
中图分类号
O57 [原子核物理学、高能物理学];
学科分类号
070202 ;
摘要
The fragmentation topology of Si-28 at 3.7 A GeV and 14.6A GeV and S-32 at 200A GeV in reactions with emulsion nuclei is presented. The fragmentation cross sections are very similar at all three energies. A statistical percolation model can qualitatively describe the data for Z greater than or equal to 6. The He production is underestimated and the 3 less than or equal to Z less than or equal to 5 fragments overestimated by this model.
引用
收藏
页码:311 / 316
页数:6
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