MASS AND NUCLEAR-CHARGE YIELDS FOR NP-237(2NTH,F) AT DIFFERENT FISSION FRAGMENT KINETIC ENERGIES

被引:21
作者
MARTINEZ, G
BARREAU, G
SICRE, A
DOAN, TP
AUDOUARD, P
LEROUX, B
ARAFA, W
BRISSOT, R
BOCQUET, JP
FAUST, H
KOCZON, P
MUTTERER, M
GONNENWEIN, F
ASGHAR, M
QUADE, U
RUDOLPH, K
ENGELHARDT, D
PIASECKI, E
机构
[1] INST SCI NUCL GRENOBLE,F-38042 GRENOBLE,FRANCE
[2] TH DARMSTADT,INST KERNPHYS,W-6100 DARMSTADT,GERMANY
[3] INST MAX VON LAUE PAUL LANGEVIN,F-38042 GRENOBLE,FRANCE
[4] UNIV TUBINGEN,INST PHYS,W-7400 TUBINGEN 1,GERMANY
[5] UNIV SCI & TECHNOL HOVARI BOUMERIENE,INST PHYS,ALGIERS,ALGERIA
[6] UNIV MUNICH,W-8000 MUNICH 2,GERMANY
[7] TECH UNIV KARLSRUHE,W-7500 KARLSRUHE,GERMANY
[8] UNIV WARSAW,PL-00325 WARSAW,POLAND
关键词
Nuclear Reactions;
D O I
10.1016/0375-9474(90)90593-B
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 recoil mass separator LOHENGRIN of the Laue-Langevin Institute Grenoble has been used to measure for the first time, the yields of light fission fragments from the fissioning system: 23993Np; this odd-Z nucleus is formed after double thermal neutron capture in a 23993Np target. The mass distributions were measured for different kinetic energies between 92 and 115.5 MeV, but the nuclear charge distributions were determined only up to 112 MeV. These distributions are compared to the distributions obtained for the even-even system 24094Pu. At high kinetic energy, the mass distribution shows a prominent peak around mass number AL = 106. These cold fragmentations are discussed in terms of a calculation based on a scission point model extrapolated to the cold fission case. As expected for an odd-Z fissioning nucleus, the nuclear charge distributions do not reveal any odd-even effect. The global neutron odd-even effect is found to be (8.1 ± 1.5)%. A simple model has been used to show that most of the neutron odd-even effect results from prompt neutron evaporation from the fragments. © 1990.
引用
收藏
页码:433 / 465
页数:33
相关论文
共 28 条
[21]   FISSION YIELDS AT DIFFERENT FISSION-PRODUCT KINETIC ENERGIES FOR THERMAL-NEUTRON-INDUCED FISSION OF PU-239 [J].
SCHMITT, C ;
GUESSOUS, A ;
BOCQUET, JP ;
CLERC, HG ;
BRISSOT, R ;
ENGELHARDT, D ;
FAUST, HR ;
GONNENWEIN, F ;
MUTTERER, M ;
NIFENECKER, H ;
PANNICKE, J ;
RISTORI, C ;
THEOBALD, JP .
NUCLEAR PHYSICS A, 1984, 430 (01) :21-60
[22]   EVIDENCE FOR NUCLEON PAIR BREAKING EVEN IN THE COLDEST SCISSION CONFIGURATIONS OF 234U AND 236U. [J].
Signarbieux, C. ;
Montoya, M. ;
Ribrag, M. ;
Mazur, C. ;
Guet, C. ;
Perrin, P. ;
Maurel, M. .
Journal de physique. Lettres, 1981, 42 (19) :437-440
[23]  
SIGNARBIEUX C, 1986, 9E P JOURN ET FISS N
[24]   RB AND CS ISOTOPIC CROSS-SECTIONS FROM 40-60-MEV-PROTON FISSION OF U-238, TH-232, AND U-235 [J].
TRACY, BL ;
THIBAULT, C ;
ROECKL, E ;
CHAUMONT, J ;
POSKANZER, AM ;
KLAPISCH, R ;
NITSCHKE, JM .
PHYSICAL REVIEW C, 1972, 5 (01) :222-+
[25]  
TROCHON J, 1989, 50 YEARS NUCLEAR FIS, P313
[26]  
WAHL AC, 1989, AT DATA NUCL DATA TA, V39
[27]   SCISSION-POINT MODEL OF NUCLEAR-FISSION BASED ON DEFORMED-SHELL EFFECTS [J].
WILKINS, BD ;
STEINBERG, EP ;
CHASMAN, RR .
PHYSICAL REVIEW C, 1976, 14 (05) :1832-1863
[28]  
Ziegler J.F., 1980, HDB STOPPING CROSS S