ENTRY D0295 20230627 D029500000001
SUBENT D0295001 20230627 20240316 D029500100001
BIB 7 10 D029500100002
TITLE Elastic and inelastic scattering of 30 MeV polarized D029500100003
protons on 90Zr,92Zr,and 92Mo D029500100004
AUTHOR (R.De Swiniarski, Dinh-Lien Pham, G.Bagieu) D029500100005
INSTITUTE (2FR GRE) D029500100006
REFERENCE (J,CJP,55,43,1977) D029500100007
FACILITY (CYCLO) D029500100008
STATUS (CURVE)Curves from the article D029500100009
HISTORY (20050315C) SD D029500100010
(20230627A) VT+On. Revision in 002, 004, 006, 010 and D029500100011
012 D029500100012
ENDBIB 10 0 D029500100013
COMMON 4 3 D029500100014
EN EN-RSL ANG-ERR-D ERR-DIG D029500100015
MEV MEV PER-CENT PER-CENT D029500100016
30.0 0.1 0.5 0.3 D029500100017
ENDCOMMON 3 0 D029500100018
ENDSUBENT 17 0 D029500199999
SUBENT D0295002 20230627 20240316 D029500200001
BIB 6 14 D029500200002
REACTION (40-ZR-90(P,EL)40-ZR-90,,DA) D029500200003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500200004
The purity of the 90Zr target was 97.65%. D029500200005
DETECTOR (TELES,SILI,SIBAR) Two telescopes comprising dE surfaceD029500200006
barrier detectors of 700 mu-m thickness and E Si(Li) D029500200007
detectors 5 mm thick. D029500200008
(SILI) To obtain absolute values of differential cross D029500200009
sections, a beam monitor set-up was used by two Si(Li) D029500200010
detectors placed at 30 degr. on each side of the beam. D029500200011
ERR-ANALYS (DATA-ERR) The errors on cross sections were uniformly D029500200012
set at +/-3% D029500200013
STATUS (TABLE,,R.De Swiniarski+,J,CJP,55,43,1977) Fig. 2 D029500200014
HISTORY (20230627A) VT+On. COMMON: DATA-ERR1 deleted and D029500200015
ERR-ANALYS and DATA: DATA-ERR1-> DATA-ERR replaced. D029500200016
ENDBIB 14 0 D029500200017
NOCOMMON 0 0 D029500200018
DATA 3 17 D029500200019
ANG-CM DATA-CM DATA-ERR D029500200020
ADEG MB/SR MB/SR D029500200021
23.675 372.78 35.490 D029500200022
28.884 241.48 22.990 D029500200023
33.682 211.20 13.627 D029500200024
39.326 134.54 10.762 D029500200025
43.596 41.852 3.3477 D029500200026
49.980 5.6543 0.70583 D029500200027
53.982 12.169 0.78517 D029500200028
59.304 28.942 2.7554 D029500200029
64.110 27.513 2.2008 D029500200030
68.880 17.529 1.1301 D029500200031
73.199 9.6123 0.62019 D029500200032
78.337 2.7506 0.17747 D029500200033
84.051 3.9011 0.31204 D029500200034
88.451 5.3522 0.34532 D029500200035
93.701 5.5300 0.35680 D029500200036
99.334 3.0829 0.24660 D029500200037
108.38 0.67527 0.54015E-01 D029500200038
ENDDATA 19 0 D029500200039
ENDSUBENT 38 0 D029500299999
SUBENT D0295003 20050315 D040D029500300001
BIB 6 16 D029500300002
REACTION (40-ZR-90(P,EL)40-ZR-90,,POL/DA,,ANA) fig.2 D029500300003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500300004
The purity of the 90Zr target was 97.65%. D029500300005
DETECTOR (SILI) Up to 3 nA of energy analyzed polarized protons D029500300006
were delivered on the target, with a polarization closeD029500300007
to 70% which was measured with a carbon polarimeter. D029500300008
The carbon polarimeter consists of a thin foil of D029500300009
graphite introduced into the incident beam during 1 minD029500300010
for every 20 min interval, and of two Si(Li) detectors D029500300011
of 5 mm thickness located at 60 degr. on each side of D029500300012
the beam D029500300013
MONITOR (6-C-12(P,EL)6-C-12,,POL/DA,,ANA) The analyzing power D029500300014
for elastic scattering of 29 MeV protons by 12C at D029500300015
60 degr. angle is 0.58 +-0.02. D029500300016
MONIT-REF (,Craig+,J,NP,83,493,1966) D029500300017
ERR-ANALYS (ERR-S) the errors on the polarization were statisticalD029500300018
ENDBIB 16 0 D029500300019
COMMON 4 3 D029500300020
EN-NRM ANG-NRM MONIT MONIT-ERR D029500300021
MEV ADEG NO-DIM NO-DIM D029500300022
29. 60. 0.58 0.02 D029500300023
ENDCOMMON 3 0 D029500300024
DATA 3 18 D029500300025
ANG-CM DATA-CM ERR-S D029500300026
ADEG NO-DIM NO-DIM D029500300027
19.393 0.10252E-010.21824E-01 D029500300028
23.802 0.15850 0.30554E-01 D029500300029
29.010 0.10593 0.21824E-01 D029500300030
34.164 -.99401E-010.26189E-01 D029500300031
38.453 -.28725 0.26189E-01 D029500300032
44.000 -.61045 0.26173E-01 D029500300033
48.813 -.54951 0.26189E-01 D029500300034
54.037 0.65938 0.30554E-01 D029500300035
59.108 0.22270 0.30570E-01 D029500300036
64.233 -.61198E-010.21824E-01 D029500300037
69.346 -.38002 0.34934E-01 D029500300038
74.453 -.71630 0.26189E-01 D029500300039
78.988 -.21450 0.26189E-01 D029500300040
84.139 0.78924 0.26189E-01 D029500300041
89.291 0.57954 0.26189E-01 D029500300042
93.947 0.19963 0.34934E-01 D029500300043
99.033 -.19340 0.30554E-01 D029500300044
109.42 -.39019 0.34919E-01 D029500300045
ENDDATA 20 0 D029500300046
ENDSUBENT 45 0 D029500399999
SUBENT D0295004 20230627 20240316 D029500400001
BIB 7 15 D029500400002
REACTION (40-ZR-90(P,INL)40-ZR-90,PAR,DA) D029500400003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500400004
The purity of the 90Zr target was 97.65%. D029500400005
EN-SEC (E-LVL,40-ZR-90) D029500400006
DETECTOR (TELES,SILI,SIBAR) Two telescopes comprising dE surfaceD029500400007
barrier detectors of 700 mu-m thickness and E Si(Li) D029500400008
detectors 5 mm thick. D029500400009
(SILI) To obtain absolute values of differential cross D029500400010
sections, a beam monitor set-up was used by two Si(Li) D029500400011
detectors placed at 30 degr. on each side of the beam. D029500400012
ERR-ANALYS (DATA-ERR) The errors on cross sections were uniformly D029500400013
set at +/-3% D029500400014
STATUS (TABLE,,R.De Swiniarski+,J,CJP,55,43,1977) Fig. 3+5 D029500400015
HISTORY (20230627A) VT+On. COMMON: DATA-ERR1 deleted and D029500400016
ERR-ANALYS and DATA: DATA-ERR1-> DATA-ERR replaced. D029500400017
ENDBIB 15 0 D029500400018
NOCOMMON 0 0 D029500400019
DATA 4 55 D029500400020
E-LVL ANG-CM DATA-CM DATA-ERR D029500400021
MEV ADEG MB/SR MB/SR D029500400022
2.1800 20.730 1.3314 0.14932 D029500400023
2.1800 26.019 1.3781 0.11412 D029500400024
2.1800 31.007 1.2131 0.63863E-01 D029500400025
2.1800 35.695 0.90820 0.11027 D029500400026
2.1800 40.512 0.51923 0.21926E-01 D029500400027
2.1800 45.599 0.37237 0.19551E-01 D029500400028
2.1800 50.645 0.29112 0.21172E-01 D029500400029
2.1800 55.244 0.26181 0.19005E-01 D029500400030
2.1800 60.248 0.22313 0.22786E-01 D029500400031
2.1800 65.537 0.23095 0.40520E-01 D029500400032
2.1800 70.577 0.18251 0.15089E-01 D029500400033
2.1800 75.150 0.17324 0.19382E-01 D029500400034
2.1800 80.481 0.16448 0.15195E-01 D029500400035
2.1800 85.267 0.10032 0.72823E-02 D029500400036
2.1800 90.085 0.57356E-010.75043E-02 D029500400037
2.1800 94.990 0.60000E-010.49605E-02 D029500400038
2.3200 30.185 0.32536 0.32920E-01 D029500400039
2.3200 35.101 0.33300 0.36826E-01 D029500400040
2.3200 41.194 0.31307 0.19452E-01 D029500400041
2.3200 46.059 0.35648 0.29159E-01 D029500400042
2.3200 51.035 0.32101 0.26300E-01 D029500400043
2.3200 55.325 0.24890 0.15431E-01 D029500400044
2.3200 60.221 0.26584 0.16482E-01 D029500400045
2.3200 64.874 0.21285 0.29502E-01 D029500400046
2.3200 70.382 0.13920 0.16708E-01 D029500400047
2.3200 75.516 0.90055E-010.99705E-02 D029500400048
2.3200 85.192 0.58986E-010.48172E-02 D029500400049
2.3200 95.262 0.37425E-010.41388E-02 D029500400050
2.7500 19.626 1.5207 0.11050 D029500400051
2.7500 24.481 1.9938 0.14467 D029500400052
2.7500 29.770 2.2727 0.21033 D029500400053
2.7500 33.883 2.8229 0.47259 D029500400054
2.7500 39.337 2.0685 0.87277E-01 D029500400055
2.7500 44.349 1.7814 0.11155 D029500400056
2.7500 49.831 1.2105 0.75928E-01 D029500400057
2.7500 54.526 0.87728 0.37016E-01 D029500400058
2.7500 59.523 0.78882 0.73001E-01 D029500400059
2.7500 64.507 0.73258 0.60516E-01 D029500400060
2.7500 69.640 0.45662 0.55395E-01 D029500400061
2.7500 74.563 0.49847 0.41177E-01 D029500400062
2.7500 79.896 0.50468 0.41690E-01 D029500400063
2.7500 89.624 0.29847 0.18658E-01 D029500400064
2.7500 94.661 0.24095 0.17509E-01 D029500400065
2.7500 99.465 0.13054 0.13337E-01 D029500400066
2.7500 109.48 0.10000 0.11180E-01 D029500400067
3.0800 36.225 0.17842 0.14544E-01 D029500400068
3.0800 41.035 0.14882 0.19202E-01 D029500400069
3.0800 46.174 0.10038 0.10115E-01 D029500400070
3.0800 51.051 0.11762 0.13173E-01 D029500400071
3.0800 61.409 0.79264E-010.88875E-02 D029500400072
3.0800 66.161 0.49633E-010.59395E-02 D029500400073
3.0800 70.940 0.35681E-010.39959E-02 D029500400074
3.0800 80.982 0.32033E-010.47429E-02 D029500400075
3.0800 86.258 0.42636E-010.63128E-02 D029500400076
3.0800 90.974 0.22287E-010.32984E-02 D029500400077
ENDDATA 57 0 D029500400078
ENDSUBENT 77 0 D029500499999
SUBENT D0295005 20050315 D040D029500500001
BIB 7 17 D029500500002
REACTION (40-ZR-90(P,INL)40-ZR-90,PAR,POL/DA,,ANA) fig.4,5 D029500500003
EN-SEC (E-LVL,40-ZR-90) D029500500004
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500500005
The purity of the 90Zr target was 97.65%. D029500500006
DETECTOR (SILI) Up to 3 nA of energy analyzed polarized protons D029500500007
were delivered on the target, with a polarization closeD029500500008
to 70% which was measured with a carbon polarimeter. D029500500009
The carbon polarimeter consists of a thin foil of D029500500010
graphite introduced into the incident beam during 1 minD029500500011
for every 20 min interval, and of two Si(Li) detectors D029500500012
of 5 mm thickness located at 60 degr. on each side of D029500500013
the beam D029500500014
MONITOR (6-C-12(P,EL)6-C-12,,POL/DA,,ANA) The analyzing power D029500500015
for elastic scattering of 29 MeV protons by 12C at D029500500016
60 degr. angle is 0.58 +-0.02. D029500500017
MONIT-REF (,Craig+,J,NP,83,493,1966) D029500500018
ERR-ANALYS (ERR-S) the errors on the polarization were statisticalD029500500019
ENDBIB 17 0 D029500500020
COMMON 4 3 D029500500021
EN-NRM ANG-NRM MONIT MONIT-ERR D029500500022
MEV ADEG NO-DIM NO-DIM D029500500023
29. 60. 0.58 0.02 D029500500024
ENDCOMMON 3 0 D029500500025
DATA 4 53 D029500500026
E-LVL ANG-CM DATA-CM ERR-S D029500500027
MEV ADEG NO-DIM NO-DIM D029500500028
2.1800 19.135 0.10856 0.45149E-01 D029500500029
2.1800 23.680 0.13357 0.41676E-01 D029500500030
2.1800 28.935 0.15522 0.31257E-01 D029500500031
2.1800 33.743 0.13529E-010.41676E-01 D029500500032
2.1800 39.097 -.27336E-010.24365E-01 D029500500033
2.1800 43.685 -.30107E-010.55568E-01 D029500500034
2.1800 49.508 0.78474E-010.45095E-01 D029500500035
2.1800 54.025 0.12085 0.65987E-01 D029500500036
2.1800 59.220 0.18070 0.55622E-01 D029500500037
2.1800 63.798 0.18488 0.76406E-01 D029500500038
2.1800 69.493 0.15101 0.59041E-01 D029500500039
2.1800 74.207 0.68364E-010.55568E-01 D029500500040
2.1800 78.559 -.73942E-020.76460E-01 D029500500041
2.1800 84.487 0.25753 0.90298E-01 D029500500042
2.1800 89.511 0.20271 0.12166 D029500500043
2.1800 94.904 0.35986 0.90298E-01 D029500500044
2.3200 24.139 0.12430 0.46340E-01 D029500500045
2.3200 29.577 0.25353 0.67728E-01 D029500500046
2.3200 34.480 0.51088E-010.49962E-01 D029500500047
2.3200 39.573 -.47926E-010.74800E-01 D029500500048
2.3200 45.279 0.13484 0.53526E-01 D029500500049
2.3200 49.924 0.96363E-010.67728E-01 D029500500050
2.3200 54.880 0.30753 0.71292E-01 D029500500051
2.3200 65.574 0.23438 0.14615 D029500500052
2.3200 70.712 0.10684 0.89116E-01 D029500500053
2.3200 76.006 0.10413 0.99809E-01 D029500500054
2.3200 85.614 0.48632E-010.14971 D029500500055
2.3200 95.414 0.54225 0.10694 D029500500056
2.7500 20.777 0.13582 0.41995E-01 D029500500057
2.7500 25.855 0.87605E-010.34941E-01 D029500500058
2.7500 30.740 0.15837 0.35052E-01 D029500500059
2.7500 40.630 0.22642 0.28052E-01 D029500500060
2.7500 45.044 0.14659 0.34996E-01 D029500500061
2.7500 49.652 0.16831 0.28052E-01 D029500500062
2.7500 54.933 -.58964E-020.31552E-01 D029500500063
2.7500 59.954 -.19119E-010.31497E-01 D029500500064
2.7500 64.879 0.27152E-010.31497E-01 D029500500065
2.7500 70.388 0.15402 0.62993E-01 D029500500066
2.7500 75.676 0.41738 0.48995E-01 D029500500067
2.7500 81.417 0.40077 0.45440E-01 D029500500068
2.7500 89.951 0.20257 0.77047E-01 D029500500069
2.7500 99.976 -.33911E-010.90879E-01 D029500500070
2.7500 110.60 0.68534 0.10149 D029500500071
3.0800 34.266 0.62459E-010.74091E-01 D029500500072
3.0800 39.445 -.30378E-010.77777E-01 D029500500073
3.0800 44.386 0.15828 0.88888E-01 D029500500074
3.0800 50.018 0.23209 0.88906E-01 D029500500075
3.0800 59.627 0.39043E-010.10370 D029500500076
3.0800 64.493 0.72148E-010.10741 D029500500077
3.0800 69.727 0.94124E-010.15555 D029500500078
3.0800 79.453 0.14552 0.18146 D029500500079
3.0800 89.235 0.31543 0.21113 D029500500080
3.0800 94.530 0.46333 0.88871E-01 D029500500081
ENDDATA 55 0 D029500500082
ENDSUBENT 81 0 D029500599999
SUBENT D0295006 20230627 20240316 D029500600001
BIB 6 14 D029500600002
REACTION (40-ZR-92(P,EL)40-ZR-92,,DA) D029500600003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500600004
The purity of the 92Zr target was 93.20%. D029500600005
DETECTOR (TELES,SILI,SIBAR) Two telescopes comprising dE D029500600006
surface barrier detector of 700 mu-m thickness and E D029500600007
Si(Li) detectors 5 mm thick. D029500600008
(SILI) To obtain absolute values of differential cross D029500600009
sections, a beam monitor set-up was used by two Si(Li) D029500600010
detectors placed at 30 degr. on each side of the beam. D029500600011
ERR-ANALYS (DATA-ERR) The errors on cross sections were uniformly D029500600012
set at +/-3% D029500600013
STATUS (TABLE,,R.De Swiniarski+,J,CJP,55,43,1977) Fig. 2 D029500600014
HISTORY (20230627A) VT+On. COMMON: DATA-ERR1 deleted and D029500600015
ERR-ANALYS and DATA: DATA-ERR1-> DATA-ERR replaced. D029500600016
ENDBIB 14 0 D029500600017
NOCOMMON 0 0 D029500600018
DATA 3 21 D029500600019
ANG-CM DATA-CM DATA-ERR D029500600020
ADEG MB/SR MB/SR D029500600021
18.324 2255.6 266.42 D029500600022
24.002 554.23 55.115 D029500600023
26.624 321.46 31.969 D029500600024
30.120 239.74 32.700 D029500600025
32.307 260.69 20.955 D029500600026
35.803 190.39 18.934 D029500600027
38.863 148.07 17.489 D029500600028
44.542 36.381 3.6179 D029500600029
49.342 3.7084 0.29808 D029500600030
55.030 10.793 1.0734 D029500600031
60.717 22.468 2.2343 D029500600032
69.024 21.098 1.6959 D029500600033
75.141 6.2595 0.62247 D029500600034
80.821 2.5428 0.25286 D029500600035
86.945 4.6679 0.46420 D029500600036
90.006 5.1832 0.51545 D029500600037
95.252 4.3833 0.43589 D029500600038
100.50 2.9439 0.29275 D029500600039
104.87 1.5377 0.15291 D029500600040
109.67 0.65138 0.14479 D029500600041
119.73 0.91067 0.17212 D029500600042
ENDDATA 23 0 D029500600043
ENDSUBENT 42 0 D029500699999
SUBENT D0295007 20050315 D040D029500700001
BIB 6 16 D029500700002
REACTION (40-ZR-92(P,EL)40-ZR-92,,POL/DA,,ANA) fig.2 D029500700003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500700004
The purity of the 92Zr target was 93.20%. D029500700005
DETECTOR (SILI) Up to 3 nA of energy analyzed polarized protons D029500700006
were delivered on the target, with a polarization closeD029500700007
to 70% which was measured with a carbon polarimeter. D029500700008
The carbon polarimeter consists of a thin foil of D029500700009
graphite introduced into the incident beam during 1 minD029500700010
for every 20 min interval, and of two Si(Li) detectors D029500700011
of 5 mm thickness located at 60 degr. on each side of D029500700012
the beam D029500700013
MONITOR (6-C-12(P,EL)6-C-12,,POL/DA,,ANA) The analyzing power D029500700014
for elastic scattering of 29 MeV protons by 12C at D029500700015
60 degr. angle is 0.58 +-0.02. D029500700016
MONIT-REF (,Craig+,J,NP,83,493,1966) D029500700017
ERR-ANALYS (ERR-S) the errors on the polarization were statisticalD029500700018
ENDBIB 16 0 D029500700019
COMMON 4 3 D029500700020
EN-NRM ANG-NRM MONIT MONIT-ERR D029500700021
MEV ADEG NO-DIM NO-DIM D029500700022
29. 60. 0.58 0.02 D029500700023
ENDCOMMON 3 0 D029500700024
DATA 3 19 D029500700025
ANG-CM DATA-CM ERR-S D029500700026
ADEG NO-DIM NO-DIM D029500700027
17.822 0.12747 0.17295E-01 D029500700028
23.994 0.29584 0.21619E-01 D029500700029
26.577 0.22655 0.17314E-01 D029500700030
29.191 0.22643 0.21638E-01 D029500700031
33.026 0.31696E-010.17295E-01 D029500700032
38.601 -.17176 0.17295E-01 D029500700033
45.377 -.61741 0.17314E-01 D029500700034
49.763 -.54842 0.30285E-01 D029500700035
54.901 0.25128 0.17295E-01 D029500700036
59.616 0.73796E-010.21600E-01 D029500700037
69.493 -.25092 0.25943E-01 D029500700038
74.589 -.55381 0.38914E-01 D029500700039
80.306 0.57448 0.17295E-01 D029500700040
89.373 0.38816 0.38914E-01 D029500700041
94.017 0.50704E-010.25961E-01 D029500700042
99.550 -.24788 0.30285E-01 D029500700043
104.65 -.54644 0.25943E-01 D029500700044
109.15 -.20505 0.30248E-01 D029500700045
119.18 0.81495 0.34590E-01 D029500700046
ENDDATA 21 0 D029500700047
ENDSUBENT 46 0 D029500799999
SUBENT D0295008 20050315 D040D029500800001
BIB 5 12 D029500800002
REACTION (40-ZR-92(P,INL)40-ZR-92,PAR,DA) fig.4,5 D029500800003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500800004
The purity of the 92Zr target was 93.20%. D029500800005
EN-SEC (E-LVL,40-ZR-92) D029500800006
DETECTOR (TELES,SILI,SIBAR) The measurements were made using D029500800007
four telescopes comprising dE surface barrier detector D029500800008
of 700 mu-m thickness and E Si(Li) detectors 5 mm thickD029500800009
(SILI) To obtain absolute values of differential cross D029500800010
sections, a beam monitor set-up was used by two Si(Li) D029500800011
detectors placed at 30 degr. on each side of the beam. D029500800012
ERR-ANALYS (DATA-ERR1) Errors on the cross sections were D029500800013
uniformly set at +-3% D029500800014
ENDBIB 12 0 D029500800015
COMMON 1 3 D029500800016
DATA-ERR1 D029500800017
PER-CENT D029500800018
3. D029500800019
ENDCOMMON 3 0 D029500800020
DATA 4 35 D029500800021
E-LVL ANG-CM DATA-CM ERR-S D029500800022
MEV ADEG MB/SR MB/SR D029500800023
0.93000 27.376 4.9107 0.25706 D029500800024
0.93000 30.888 4.0524 0.21213 D029500800025
0.93000 33.620 3.4900 0.14639 D029500800026
0.93000 36.500 2.2726 0.11896 D029500800027
0.93000 45.263 1.0181 0.53296E-01 D029500800028
0.93000 60.025 0.51474 0.32162E-01 D029500800029
0.93000 69.022 0.62039 0.38763E-01 D029500800030
0.93000 75.073 0.63552 0.39708E-01 D029500800031
0.93000 81.053 0.36420 0.22756E-01 D029500800032
0.93000 86.807 0.15609 0.17413E-01 D029500800033
0.93000 94.635 0.97568E-010.70745E-02 D029500800034
0.93000 99.758 0.13795 0.72213E-02 D029500800035
0.93000 104.68 0.13824 0.10024E-01 D029500800036
0.93000 109.72 0.11173 0.81011E-02 D029500800037
0.93000 119.66 0.46448E-010.33609E-02 D029500800038
2.3300 18.313 2.4578 0.10320 D029500800039
2.3300 27.283 3.5517 0.18591 D029500800040
2.3300 30.317 3.6721 0.19170 D029500800041
2.3300 32.891 4.4585 0.23275 D029500800042
2.3300 36.359 4.1416 0.25808 D029500800043
2.3300 39.053 3.9295 0.16498 D029500800044
2.3300 45.247 3.2474 0.13634 D029500800045
2.3300 50.508 1.7469 0.91194E-01 D029500800046
2.3300 60.222 1.2047 0.50579E-01 D029500800047
2.3300 69.016 1.1457 0.48102E-01 D029500800048
2.3300 74.792 1.0204 0.42844E-01 D029500800049
2.3300 80.938 0.92875 0.48485E-01 D029500800050
2.3300 86.777 0.72736 0.37971E-01 D029500800051
2.3300 89.059 0.73585 0.45854E-01 D029500800052
2.3300 90.074 0.43993 0.18533E-01 D029500800053
2.3300 94.806 0.31948 0.16678E-01 D029500800054
2.3300 100.17 0.30343 0.15840E-01 D029500800055
2.3300 104.45 0.25600 0.15952E-01 D029500800056
2.3300 109.81 0.24055 0.12524E-01 D029500800057
2.3300 119.46 0.19275 0.10063E-01 D029500800058
ENDDATA 37 0 D029500800059
ENDSUBENT 58 0 D029500899999
SUBENT D0295009 20050315 D040D029500900001
BIB 7 17 D029500900002
REACTION (40-ZR-92(P,INL)40-ZR-92,PAR,POL/DA,,ANA) fig.4,5 D029500900003
EN-SEC (E-LVL,40-ZR-92) D029500900004
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029500900005
The purity of the 92Zr target was 93.20%. D029500900006
DETECTOR (SILI) Up to 3 nA of energy analyzed polarized protons D029500900007
were delivered on the target, with a polarization closeD029500900008
to 70% which was measured with a carbon polarimeter. D029500900009
The carbon polarimeter consists of a thin foil of D029500900010
graphite introduced into the incident beam during 1 minD029500900011
for every 20 min interval, and of two Si(Li) detectors D029500900012
of 5 mm thickness located at 60 degr. on each side of D029500900013
the beam D029500900014
MONITOR (6-C-12(P,EL)6-C-12,,POL/DA,,ANA) The analyzing power D029500900015
for elastic scattering of 29 MeV protons by 12C at D029500900016
60 degr. angle is 0.58 +-0.02. D029500900017
MONIT-REF (,Craig+,J,NP,83,493,1966) D029500900018
ERR-ANALYS (ERR-S) the errors on the polarization were statisticalD029500900019
ENDBIB 17 0 D029500900020
COMMON 4 3 D029500900021
EN-NRM ANG-NRM MONIT MONIT-ERR D029500900022
MEV ADEG NO-DIM NO-DIM D029500900023
29. 60. 0.58 0.02 D029500900024
ENDCOMMON 3 0 D029500900025
DATA 4 31 D029500900026
E-LVL ANG-CM DATA-CM ERR-S D029500900027
MEV ADEG NO-DIM NO-DIM D029500900028
0.93000 26.251 0.52313E-010.35309E-01 D029500900029
0.93000 30.330 0.14481 0.52963E-01 D029500900030
0.93000 35.624 0.14216 0.56494E-01 D029500900031
0.93000 59.275 -.87034E-010.70617E-01 D029500900032
0.93000 68.922 0.26421 0.70617E-01 D029500900033
0.93000 74.594 0.32048E-010.88272E-01 D029500900034
0.93000 81.062 -.41051E-010.81268E-01 D029500900035
0.93000 87.076 0.16126 0.18360 D029500900036
0.93000 95.059 0.45219 0.77679E-01 D029500900037
0.93000 100.08 0.18813 0.84741E-01 D029500900038
0.93000 105.44 0.14310 0.49490E-01 D029500900039
0.93000 110.85 0.73358E-010.56494E-01 D029500900040
0.93000 120.52 0.19504 0.10593 D029500900041
2.3300 26.999 0.15116 0.35367E-01 D029500900042
2.3300 30.789 0.26129 0.42441E-01 D029500900043
2.3300 32.940 0.25448 0.28338E-01 D029500900044
2.3300 39.398 0.23051 0.35323E-01 D029500900045
2.3300 45.852 0.21009 0.28294E-01 D029500900046
2.3300 50.912 -.12179 0.35367E-01 D029500900047
2.3300 55.629 -.18134 0.60168E-01 D029500900048
2.3300 60.619 -.17365 0.42485E-01 D029500900049
2.3300 70.078 0.25552 0.49470E-01 D029500900050
2.3300 75.957 0.40835 0.70779E-01 D029500900051
2.3300 82.437 0.36670 0.35367E-01 D029500900052
2.3300 88.279 0.26484 0.53007E-01 D029500900053
2.3300 90.768 -.10756E-010.67198E-01 D029500900054
2.3300 95.574 -.14104 0.42441E-01 D029500900055
2.3300 101.11 -.24052E-020.53051E-01 D029500900056
2.3300 104.69 0.28102 0.46021E-01 D029500900057
2.3300 110.11 0.50807 0.35367E-01 D029500900058
2.3300 120.34 0.60838 0.38904E-01 D029500900059
ENDDATA 33 0 D029500900060
ENDSUBENT 59 0 D029500999999
SUBENT D0295010 20230627 20240316 D029501000001
BIB 6 14 D029501000002
REACTION (42-MO-92(P,EL)42-MO-92,,DA) D029501000003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029501000004
The purity of the 92Mo target was 98.27%. D029501000005
DETECTOR (TELES,SILI,SIBAR) Two telescopes comprising dE surfaceD029501000006
barrier detectors of 700 mu-m thickness and E Si(Li) D029501000007
detectors 5 mm thick. D029501000008
(SILI) To obtain absolute values of differential cross D029501000009
sections, a beam monitor set-up was used by two Si(Li) D029501000010
detectors placed at 30 degr. on each side of the beam. D029501000011
ERR-ANALYS (DATA-ERR) The errors on cross sections were uniformly D029501000012
set at +/-3% D029501000013
STATUS (TABLE,,R.De Swiniarski+,J,CJP,55,43,1977) Fig. 2 D029501000014
HISTORY (20230627A) VT+On. COMMON: DATA-ERR1 deleted and D029501000015
ERR-ANALYS and DATA: DATA-ERR1-> DATA-ERR replaced. D029501000016
ENDBIB 14 0 D029501000017
NOCOMMON 0 0 D029501000018
DATA 3 22 D029501000019
ANG-CM DATA-CM DATA-ERR D029501000020
ADEG MB/SR MB/SR D029501000021
20.011 1519.4 147.55 D029501000022
24.386 455.18 44.201 D029501000023
29.634 284.52 22.327 D029501000024
34.882 222.67 21.623 D029501000025
39.692 167.28 16.244 D029501000026
44.066 64.038 6.2185 D029501000027
49.755 8.8264 0.69264 D029501000028
54.563 13.836 1.0857 D029501000029
58.933 32.634 3.1690 D029501000030
64.617 35.414 2.7790 D029501000031
68.990 24.021 2.3327 D029501000032
74.239 10.609 1.2240 D029501000033
79.051 3.5929 0.34890 D029501000034
84.298 3.8201 0.37096 D029501000035
89.106 5.2973 0.41569 D029501000036
94.352 7.1971 0.69889 D029501000037
99.599 5.5185 0.43305 D029501000038
104.41 3.3798 0.26521 D029501000039
109.22 1.5550 0.12202 D029501000040
114.47 1.0765 0.84478E-01 D029501000041
119.71 1.7223 0.19870 D029501000042
129.33 2.3884 0.23192 D029501000043
ENDDATA 24 0 D029501000044
ENDSUBENT 43 0 D029501099999
SUBENT D0295011 20050315 D040D029501100001
BIB 6 16 D029501100002
REACTION (42-MO-92(P,EL)42-MO-92,,POL/DA,,ANA) fig.2 D029501100003
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029501100004
The purity of the 92Mo target was 98.27%. D029501100005
DETECTOR (SILI) Up to 3 nA of energy analyzed polarized protons D029501100006
were delivered on the target, with a polarization closeD029501100007
to 70% which was measured with a carbon polarimeter. D029501100008
The carbon polarimeter consists of a thin foil of D029501100009
graphite introduced into the incident beam during 1 minD029501100010
for every 20 min interval, and of two Si(Li) detectors D029501100011
of 5 mm thickness located at 60 degr. on each side of D029501100012
the beam D029501100013
MONITOR (6-C-12(P,EL)6-C-12,,POL/DA,,ANA) The analyzing power D029501100014
for elastic scattering of 29 MeV protons by 12C at D029501100015
60 degr. angle is 0.58 +-0.02. D029501100016
MONIT-REF (,Craig+,J,NP,83,493,1966) D029501100017
ERR-ANALYS (ERR-S) the errors on the polarization were statisticalD029501100018
ENDBIB 16 0 D029501100019
COMMON 4 3 D029501100020
EN-NRM ANG-NRM MONIT MONIT-ERR D029501100021
MEV ADEG NO-DIM NO-DIM D029501100022
29. 60. 0.58 0.02 D029501100023
ENDCOMMON 3 0 D029501100024
DATA 3 21 D029501100025
ANG-CM DATA-CM ERR-S D029501100026
ADEG NO-DIM NO-DIM D029501100027
19.384 -.18724E-010.21590E-01 D029501100028
23.353 0.11499 0.17272E-01 D029501100029
25.096 0.11493 0.17272E-01 D029501100030
29.459 0.13636 0.17272E-01 D029501100031
38.896 -.26555 0.17287E-01 D029501100032
44.447 -.57233 0.17272E-01 D029501100033
49.183 -.72363 0.25923E-01 D029501100034
54.503 0.72704 0.30241E-01 D029501100035
59.565 0.27346 0.30210E-01 D029501100036
64.672 -.54891E-010.34544E-01 D029501100037
68.924 -.34003 0.21590E-01 D029501100038
74.038 -.65111 0.21590E-01 D029501100039
79.795 -.39224 0.30226E-01 D029501100040
85.026 0.81230 0.30241E-01 D029501100041
89.295 0.57466 0.30241E-01 D029501100042
99.494 -.12523 0.21590E-01 D029501100043
104.61 -.42335 0.30210E-01 D029501100044
109.82 -.47104 0.43180E-01 D029501100045
114.48 0.36217 0.47482E-01 D029501100046
119.47 0.91038 0.34544E-01 D029501100047
129.80 0.56025 0.38877E-01 D029501100048
ENDDATA 23 0 D029501100049
ENDSUBENT 48 0 D029501199999
SUBENT D0295012 20230627 20240316 D029501200001
BIB 7 15 D029501200002
REACTION (42-MO-92(P,INL)42-MO-92,PAR,DA) D029501200003
EN-SEC (E-LVL,42-MO-92) D029501200004
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029501200005
The purity of the 92Mo target was 98.27%. D029501200006
DETECTOR (TELES,SILI,SIBAR) Two telescopes comprising dE surfaceD029501200007
barrier detectors of 700 mu-m thickness and E Si(Li) D029501200008
detectors 5 mm thick. D029501200009
(SILI) To obtain absolute values of differential cross D029501200010
sections, a beam monitor set-up was used by two Si(Li) D029501200011
detectors placed at 30 degr. on each side of the beam. D029501200012
ERR-ANALYS (DATA-ERR) The errors on cross sections were uniformly D029501200013
set at +/-3% D029501200014
STATUS (TABLE,,R.De Swiniarski+,J,CJP,55,43,1977) Fig. 4+5 D029501200015
HISTORY (20230627A) VT+On. COMMON: DATA-ERR1 deleted and D029501200016
ERR-ANALYS and DATA: DATA-ERR1-> DATA-ERR replaced. D029501200017
ENDBIB 15 0 D029501200018
NOCOMMON 0 0 D029501200019
DATA 4 69 D029501200020
E-LVL ANG-CM DATA-CM DATA-ERR D029501200021
MEV ADEG MB/SR MB/SR D029501200022
1.5100 20.283 2.3327 0.17080 D029501200023
1.5100 25.815 3.0685 0.19362 D029501200024
1.5100 30.681 3.4283 0.25102 D029501200025
1.5100 35.423 1.2239 0.10187 D029501200026
1.5100 40.794 1.0887 0.79713E-01 D029501200027
1.5100 45.438 0.91690 0.48472E-01 D029501200028
1.5100 50.779 0.86113 0.36759E-01 D029501200029
1.5100 54.977 0.81717 0.51561E-01 D029501200030
1.5100 59.730 0.56600 0.63660E-01 D029501200031
1.5100 65.631 0.38380 0.39567E-01 D029501200032
1.5100 70.190 0.37634 0.38739E-01 D029501200033
1.5100 80.829 0.35818 0.40341E-01 D029501200034
1.5100 85.618 0.23243 0.26214E-01 D029501200035
1.5100 90.143 0.12268 0.20151E-01 D029501200036
1.5100 95.230 0.18184 0.23079E-01 D029501200037
1.5100 99.746 0.19238 0.24456E-01 D029501200038
1.5100 105.23 0.14074 0.13130E-01 D029501200039
1.5100 109.95 0.10181 0.14363E-01 D029501200040
1.5100 115.28 0.97718E-010.11006E-01 D029501200041
1.5100 119.83 0.97921E-010.13815E-01 D029501200042
2.2800 35.920 0.44788 0.52665E-01 D029501200043
2.2800 40.715 0.33393 0.32087E-01 D029501200044
2.2800 45.502 0.23912 0.22760E-01 D029501200045
2.2800 50.337 0.22492 0.18932E-01 D029501200046
2.2800 55.167 0.20524 0.21586E-01 D029501200047
2.2800 60.427 0.26138 0.30721E-01 D029501200048
2.2800 65.297 0.30091 0.31660E-01 D029501200049
2.2800 70.818 0.20074 0.23594E-01 D029501200050
2.2800 80.743 0.90256E-010.13471E-01 D029501200051
2.2800 85.519 0.60216E-010.11016E-01 D029501200052
2.2800 90.690 0.45811E-010.96962E-02 D029501200053
2.2800 95.633 0.80611E-010.12246E-01 D029501200054
2.2800 100.91 0.11243 0.15814E-01 D029501200055
2.2800 105.34 0.88175E-010.12402E-01 D029501200056
2.2800 110.11 0.58828E-010.89340E-02 D029501200057
2.2800 115.28 0.44305E-010.57077E-02 D029501200058
2.5200 39.729 0.72046 0.59611E-01 D029501200059
2.5200 45.185 0.57561 0.75289E-01 D029501200060
2.5200 50.186 0.52909 0.59242E-01 D029501200061
2.5200 54.920 0.39182 0.40096E-01 D029501200062
2.5200 59.658 0.28705 0.34838E-01 D029501200063
2.5200 64.865 0.36878 0.41188E-01 D029501200064
2.5200 69.991 0.26731 0.29931E-01 D029501200065
2.5200 75.236 0.15446 0.20225E-01 D029501200066
2.5200 80.526 0.81866E-010.12998E-01 D029501200067
2.5200 95.278 0.49590E-010.92029E-02 D029501200068
2.5200 100.56 0.55368E-010.97856E-02 D029501200069
2.5200 105.43 0.64536E-010.84593E-02 D029501200070
2.5200 110.00 0.66072E-010.98779E-02 D029501200071
2.5200 119.76 0.42612E-010.79023E-02 D029501200072
2.5200 130.16 0.34861E-010.43956E-02 D029501200073
2.8500 39.972 3.1754 0.21334 D029501200074
2.8500 44.582 2.8842 0.19378 D029501200075
2.8500 49.656 2.0867 0.13159 D029501200076
2.8500 54.667 1.7955 0.13118 D029501200077
2.8500 59.734 1.3275 0.83575E-01 D029501200078
2.8500 64.796 0.99218 0.72486E-01 D029501200079
2.8500 69.387 0.95137 0.59795E-01 D029501200080
2.8500 74.406 0.80108 0.42254E-01 D029501200081
2.8500 79.047 0.66718 0.48673E-01 D029501200082
2.8500 84.412 0.61941 0.32672E-01 D029501200083
2.8500 89.498 0.43380 0.27311E-01 D029501200084
2.8500 94.081 0.42507 0.31055E-01 D029501200085
2.8500 99.072 0.38613 0.28210E-01 D029501200086
2.8500 104.20 0.24265 0.17727E-01 D029501200087
2.8500 108.85 0.19563 0.16247E-01 D029501200088
2.8500 113.76 0.22555 0.18732E-01 D029501200089
2.8500 119.06 0.24905 0.18221E-01 D029501200090
2.8500 128.67 0.20108 0.20653E-01 D029501200091
ENDDATA 71 0 D029501200092
ENDSUBENT 91 0 D029501299999
SUBENT D0295013 20050315 D040D029501300001
BIB 7 17 D029501300002
REACTION (42-MO-92(P,INL)42-MO-92,PAR,POL/DA,,ANA) fig.4,5 D029501300003
EN-SEC (E-LVL,42-MO-92) D029501300004
SAMPLE Enriched target of about 1 mg/cm2 thickness were used. D029501300005
The purity of the 92Mo target was 98.27%. D029501300006
DETECTOR (SILI) Up to 3 nA of energy analyzed polarized protons D029501300007
were delivered on the target, with a polarization closeD029501300008
to 70% which was measured with a carbon polarimeter. D029501300009
The carbon polarimeter consists of a thin foil of D029501300010
graphite introduced into the incident beam during 1 minD029501300011
for every 20 min interval, and of two Si(Li) detectors D029501300012
of 5 mm thickness located at 60 degr. on each side of D029501300013
the beam D029501300014
MONITOR (6-C-12(P,EL)6-C-12,,POL/DA,,ANA) The analyzing power D029501300015
for elastic scattering of 29 MeV protons by 12C at D029501300016
60 degr. angle is 0.58 +-0.02. D029501300017
MONIT-REF (,Craig+,J,NP,83,493,1966) D029501300018
ERR-ANALYS (ERR-S) the errors on the polarization were statisticalD029501300019
ENDBIB 17 0 D029501300020
COMMON 4 3 D029501300021
EN-NRM ANG-NRM MONIT MONIT-ERR D029501300022
MEV ADEG NO-DIM NO-DIM D029501300023
29. 60. 0.58 0.02 D029501300024
ENDCOMMON 3 0 D029501300025
DATA 4 63 D029501300026
E-LVL ANG-CM DATA-CM ERR-S D029501300027
MEV ADEG NO-DIM NO-DIM D029501300028
1.5100 19.539 0.40585E-010.39125E-01 D029501300029
1.5100 25.477 0.73700E-010.46312E-01 D029501300030
1.5100 30.728 0.96004E-010.46312E-01 D029501300031
1.5100 35.207 0.15737 0.92686E-01 D029501300032
1.5100 40.596 -.10538 0.53375E-01 D029501300033
1.5100 45.240 -.14020 0.60562E-01 D029501300034
1.5100 49.596 -.75862E-020.67625E-01 D029501300035
1.5100 55.610 0.18590 0.85499E-01 D029501300036
1.5100 60.003 0.29714 0.10681 D029501300037
1.5100 65.285 0.30163 0.11044 D029501300038
1.5100 69.867 0.30244 0.99625E-01 D029501300039
1.5100 80.391 0.12968 0.99749E-01 D029501300040
1.5100 84.790 -.17245 0.99810E-01 D029501300041
1.5100 91.463 0.25278 0.13537 D029501300042
1.5100 95.730 0.64196 0.11756 D029501300043
1.5100 101.15 0.36139 0.12112 D029501300044
1.5100 106.33 0.21976 0.12469 D029501300045
1.5100 110.97 0.18850 0.16037 D029501300046
1.5100 115.23 0.17143 0.14244 D029501300047
1.5100 121.75 0.72799E-010.13537 D029501300048
2.2800 34.347 0.16181 0.14094 D029501300049
2.2800 39.924 0.11337 0.11128 D029501300050
2.2800 44.679 -.12048 0.11127 D029501300051
2.2800 49.560 -.46499E-010.12241 D029501300052
2.2800 54.918 0.28338 0.12981 D029501300053
2.2800 59.797 0.35365 0.14094 D029501300054
2.2800 64.989 0.27556 0.14094 D029501300055
2.2800 79.919 0.28979 0.16691 D029501300056
2.2800 84.516 0.58261 0.20771 D029501300057
2.2800 94.944 0.53397 0.19657 D029501300058
2.2800 100.10 0.37799 0.11497 D029501300059
2.2800 104.93 0.32958 0.15576 D029501300060
2.2800 110.49 0.23293 0.19286 D029501300061
2.2800 115.34 0.23273 0.21513 D029501300062
2.5200 40.148 0.29968E-010.75794E-01 D029501300063
2.5200 44.338 0.99148E-010.79353E-01 D029501300064
2.5200 49.178 -.44567E-010.86622E-01 D029501300065
2.5200 54.574 -.72686E-010.10467 D029501300066
2.5200 60.453 0.32524 0.11910 D029501300067
2.5200 64.827 0.26088 0.13349 D029501300068
2.5200 74.583 -.80693E-010.18407 D029501300069
2.5200 80.251 -.47405E-010.18041 D029501300070
2.5200 94.821 0.51895E-020.23826 D029501300071
2.5200 100.76 0.99886E-010.19490 D029501300072
2.5200 105.34 0.40738 0.17324 D029501300073
2.5200 110.63 0.71497 0.15525 D029501300074
2.5200 132.07 -.33250 0.26713 D029501300075
2.8500 40.471 0.99008E-010.22906E-01 D029501300076
2.8500 45.870 0.83492E-010.28245E-01 D029501300077
2.8500 50.299 0.30864E-010.22929E-01 D029501300078
2.8500 55.042 -.58664E-020.24693E-01 D029501300079
2.8500 60.138 -.40809E-010.28245E-01 D029501300080
2.8500 64.967 0.21258E-010.28221E-01 D029501300081
2.8500 69.175 0.49765E-010.29985E-01 D029501300082
2.8500 80.484 0.22341 0.24693E-01 D029501300083
2.8500 89.811 0.77605E-010.38804E-01 D029501300084
2.8500 95.567 -.68433E-010.40568E-01 D029501300085
2.8500 100.71 -.11925 0.42355E-01 D029501300086
2.8500 104.77 -.39592E-010.51150E-01 D029501300087
2.8500 110.27 0.40160E-010.51150E-01 D029501300088
2.8500 115.04 0.38625 0.28269E-01 D029501300089
2.8500 120.73 0.39192 0.35276E-01 D029501300090
2.8500 130.03 0.25847 0.45859E-01 D029501300091
ENDDATA 65 0 D029501300092
ENDSUBENT 91 0 D029501399999
ENDENTRY 13 0 D029599999999