ENTRY 41564 20140130 41634156400000001
SUBENT 41564001 20140130 41634156400100001
BIB 12 49 4156400100002
TITLE Study of Neutron-Neutron Scattering in nd Breakup 4156400100003
Reaction. 4156400100004
AUTHOR (E.Konobeevski,S.V.Zuyev, M.V.Mordovskoy, S.I.Potashev,4156400100005
I.M.Sharapov) 4156400100006
INSTITUTE (4RUSJIA) 4156400100007
REFERENCE (J,YF,76,(11),1398,2013) 4156400100008
(J,PAN,76,1398,2013) Engl.translation of J,YF,76 . 4156400100009
#doi:10.1134/S1063778813110100 4156400100010
(J,JP/CS,340,012047,2012) 4156400100011
#doi:10.1088/1742-6596/340/1/012047 4156400100012
REL-REF (I,,S.V.Zuyev+,J,IET,51,327,2008) 4156400100013
#doi:10.1134/S0020441208030019 4156400100014
Engl.trans.of PTE,,(3),5,2008 4156400100015
FACILITY Moscow Meson Factory of the Institute 4156400100016
for Nuclear Research. 4156400100017
(LINAC,4RUSJIA) Beam stop of 200 MeV protons of the 4156400100018
linear accelerator. 4156400100019
INC-SOURCE (SPALL) Neutrons produced in the tungsten target (60mm 4156400100020
W) are collimated at zero angle at a length of 12 m in 4156400100021
order to form a beam with a diameter of about 60 mm at 4156400100022
the reaction CD2 target. 4156400100023
INC-SPECT Neutrons incident on the deuterium target have a 4156400100024
continuous energy spectrum, with an endpoint energy 4156400100025
equal to the proton beam energy. Detection of three 4156400100026
particles in coincidence makes it possible to 4156400100027
reconstruct the primary neutron energy in the 4156400100028
n+d -> p+n+n reaction and obtain data on the reaction 4156400100029
yield in a wide range of neutron energies, determined 4156400100030
only by the statistics of the experiment. 4156400100031
DETECTOR (TELES,SCIN) dE-E telescope consisting of two fast 4156400100032
plastic scintillation detectors. For proton detection. 4156400100033
The neutron time-of-flight hodoscope consists of 4156400100034
several (5-6 at the moment) detectors, located at 4156400100035
different angles with respect to the primary neutron 4156400100036
direction at a flight distance of 4-5 m from the CD2 4156400100037
target,on the left from the incident neutron beam axis.4156400100038
The time resolution of all detectors was about 0.6 ns. 4156400100039
The angular resolution was defined by the detector 4156400100040
cross section size and the time-of-flight distance; 4156400100041
it was about +-0.5deg. 4156400100042
SAMPLE CD2 of 100 mg/cm**2 thickness. 4156400100043
METHOD (TOF) 4156400100044
(EDE) 4156400100045
(COINC) Three particles in coincidence - proton and two4156400100046
neutrons. 4156400100047
HISTORY (20121003C) M.M. 4156400100048
(20140130A) Ref. J,YF,76,(11),1398,2013 and its English4156400100049
translation were added. 4156400100050
Data of Subent 002 were updated by last published. 4156400100051
ENDBIB 49 0 4156400100052
NOCOMMON 0 0 4156400100053
ENDSUBENT 52 0 4156400199999
SUBENT 41564002 20140130 41634156400200001
BIB 5 9 4156400200002
REACTION (0-NN-1(N,EL)0-NN-1,,AMP) Neutron scattering length 4156400200003
METHOD Experiments have been performed in the final state 4156400200004
interaction (FSI) geometry. The neutron-neutron FSI 4156400200005
manifests itself as a peak in the reaction yield 4156400200006
distribution versus the relative energy of two neutrons4156400200007
ANALYSIS Simulation based on the Watson-Migdal approximation. 4156400200008
ERR-ANALYS (ERR-S) Statistical uncertainty . 4156400200009
STATUS (TABLE) Text,page 1482 of J,YF,76,(11),1398 . 4156400200010
Text,page 5 of J,JP/CS,340,012047,2012 - 17.9+-0.9 Fm.4156400200011
ENDBIB 9 0 4156400200012
NOCOMMON 0 0 4156400200013
DATA 4 1 4156400200014
EN EN-ERR DATA ERR-S 4156400200015
MEV MEV FERMI FERMI 4156400200016
40. 5. -17.9 1.0 4156400200017
ENDDATA 3 0 4156400200018
ENDSUBENT 17 0 4156400299999
ENDENTRY 2 0 4156499999999