Data Analysis for 23 Al Experiment Kun Wang
Data Analysis for 23 Al Experiment Background Experiment Reaction cross section P.I. Transmission Results & Gate dependence Parallel momentum distribution P.I. for fragments Results & Gate dependence Summary 20-1
Background: Measurement of reaction cross section enhanced ~30A MeV measured on RIBLL Measurement of longitudinal momentum distribution no experimental measurement 20-2
20-3 Apr. 8 ~ Apr. 14, RIKEN
Experimental Setup at RIPS Primary Beam: 135A MeV 28 Si Machine Time: 6 days (Apr. 8 ~ Apr. 14, 2004) Secondary Beam: ~70A MeV 23 Al F2 target P.I. Method: B -TOF- E (before target), TOF- E-E (after target) 20-4
Particle Identification before target Z vs. A/Z 23 Al 22 Mg 25 Si 24 Al 21 Na 20-5
23 Al Reaction cross sections 20-6
Particle Identification after target: Z 20-7
Particle identification after target: A 20-8
Transmission: target-in 20-9
Transmission: target-out 20-10
Reaction cross section can be obtained by formula below: where t is the thickness of target, N BC counts of projectile nuclei before target, N AC after target, 1 for target-in data and, 2 for target-out data. Transmission Gate width at F3 Gate dependence Transmission dependence 20-11
23 Al Parallel momentum distributions 20-12
Particle Identification after target: Z 20-13
Particle Identification after target: A 20-14
Tof23 correction tof23=tof23-f*F1ppac_x tof23=tof23-f*(a*F1ppac_x+b*F2ppacb_x) ( a 2 +b 2 =1 ) f= a=
F b = F o * P i / P o P o // folded by a gauss function P i // P oF // folded by a gauss function P b // F b /P i = F o / P o 20-16
Gate dependence Gate width at F3 Transmission 20-17
Summary 23 Al, R =1618 47, FWHM (P // ) = 233 14 MeV/c 22 Mg, R =1585 222, FWHM (P // ) = 310 20 MeV/c 21 Na, R = ?, FWHM (P // ) = 236 32 MeV/c 25 Si, R =1400 73, FWHM (P // ) = ? 24 Al, R =1350 60, FWHM (P // ) = 230 10 MeV/c Al J =5/2 + (new results by T RIPS 2005) Preliminary
20-19 The reaction cross section of 23Al can be described when the core size is enlarged
Thanks! 20-20