ENTRY F0145 20050517 F022F014500000001 SUBENT F0145001 20050517 F022F014500100001 BIB 12 36 F014500100002 TITLE The polarization of protons from the 2H(d,p)3H reactionF014500100003 for deutron energies below 1 MeV. F014500100004 AUTHOR (P.Kozma,P.Bem) F014500100005 INSTITUTE (3CZRUJF) F014500100006 REFERENCE (J,NP/A,442,17,1985) F014500100007 FACILITY (VDG) F014500100008 INC-SOURCE Magnetically-analyzed deuteron beam. The mean reaction F014500100009 energy calculated from the energy loss of the deuteronsF014500100010 on appropriate foils of a sandwich target was taken to F014500100011 be Ed0-1/2DeltaEd0, Ed0 being the energy of deuterons F014500100012 which passed the first gold foil of the target block F014500100013 and DeltaEd the energy the energy thickness of the F014500100014 (CD2)n foil. For measurements covering the range of F014500100015 mean energies of 1200 t0 300 keV the DeltaEd thickness F014500100016 of the target ranged from 30 to 90 keV. F014500100017 SAMPLE Target consisted of a deuterated-polyethylene (CD2)n F014500100018 foil of thickness 0.5 mg/cm2 sandwiched between two F014500100019 gold layers. Thickness and homogenity of targets were F014500100020 determined with an accuracy of 0.01 mg/cm2. F014500100021 DETECTOR (SI) Polarimeter consisted of two silicon F014500100022 detectors as a target and two silicon detectors for theF014500100023 detection of protons scattered to the left and right atF014500100024 95 degrees lab. angle. The analyzing power of the F014500100025 polarimeter was determined to an accuracy of 3%. F014500100026 The average detection efficiency of the polarimeter F014500100027 was 2.5*10-6. F014500100028 METHOD (DSCAT) F014500100029 CORRECTION The correction of measured asymmetry data for a F014500100030 nonsymmetrical arrangment of the two "left" and "right"F014500100031 scattering planes in the present polarimeter was F014500100032 calculated to be less than 1% in the whole range of F014500100033 reaction angles. F014500100034 ERR-ANALYS (DATA-ERR) Errors correspond to the statistical F014500100035 uncertainty and to errors in the background F014500100036 subtraction. F014500100037 HISTORY (20050201C) F014500100038 ENDBIB 36 0 F014500100039 NOCOMMON 0 0 F014500100040 ENDSUBENT 39 0 F014500199999 SUBENT F0145002 20050517 F022F014500200001 BIB 2 2 F014500200002 REACTION (1-H-2(D,P)1-H-3,,POL/DA) F014500200003 STATUS (TABLE) Table 1 F014500200004 ENDBIB 2 0 F014500200005 COMMON 1 3 F014500200006 EN-MEAN F014500200007 KEV F014500200008 975. F014500200009 ENDCOMMON 3 0 F014500200010 DATA 3 7 F014500200011 ANG DATA DATA-ERR F014500200012 ADEG NO-DIM NO-DIM F014500200013 15.000 -.64000E-010.29000E-01 F014500200014 30.000 -.12200 0.24000E-01 F014500200015 45.000 -.14700 0.17000E-01 F014500200016 60.000 -.10600 0.18000E-01 F014500200017 70.000 -.31000E-010.17000E-01 F014500200018 80.000 0.40000E-020.16000E-01 F014500200019 85.000 0.35000E-010.25000E-01 F014500200020 ENDDATA 9 0 F014500200021 ENDSUBENT 20 0 F014500299999 SUBENT F0145003 20050517 F022F014500300001 BIB 2 2 F014500300002 REACTION (1-H-2(D,P)1-H-3,,POL/DA) F014500300003 STATUS (TABLE) Table 2 F014500300004 ENDBIB 2 0 F014500300005 COMMON 1 3 F014500300006 ANG F014500300007 ADEG F014500300008 45. F014500300009 ENDCOMMON 3 0 F014500300010 DATA 3 14 F014500300011 EN-MEAN DATA DATA-ERR F014500300012 KEV NO-DIM NO-DIM F014500300013 250.00 -.65000E-010.38000E-01 F014500300014 312.00 -.96000E-010.31000E-01 F014500300015 377.00 -.11900 0.19000E-01 F014500300016 455.00 -.11500 0.18000E-01 F014500300017 509.00 -.14400 0.18000E-01 F014500300018 564.00 -.14200 0.17000E-01 F014500300019 620.00 -.14300 0.17000E-01 F014500300020 676.00 -.15300 0.18000E-01 F014500300021 743.00 -.14700 0.19000E-01 F014500300022 798.00 -.15100 0.18000E-01 F014500300023 860.00 -.14100 0.19000E-01 F014500300024 906.00 -.14600 0.20000E-01 F014500300025 962.00 -.13800 0.18000E-01 F014500300026 975.00 -.14700 0.17000E-01 F014500300027 ENDDATA 16 0 F014500300028 ENDSUBENT 27 0 F014500399999 ENDENTRY 3 0 F014599999999