ENTRY F0909 20080505 F031F090900000001 SUBENT F0909001 20080505 F031F090900100001 BIB 7 25 F090900100002 TITLE Neutron transfer reactions on 204Hg. F090900100003 AUTHOR (M.L.Andersen,S.A.Andersen,O.Nathan,K.M.Bisgard, F090900100004 K.Gregersen,Ole Hansen,S.Hinds,R.Chapman) F090900100005 INSTITUTE (2DENNBI,2DENAAU,1USALAS,2UK ALD) F090900100006 (2DENDEN)Physics Laboratory, Royal Veterinary and F090900100007 Agricultural University, Copenhagen,Denmark. F090900100008 REFERENCE (J,NP/A,153,17,1970) F090900100009 MONITOR Absolute reaction cross sections were determined by F090900100010 comparison of the (d,p) and (d,t) intensities with the F090900100011 yield of elastically scattered deuterons. F090900100012 SAMPLE Two different methods have been used to fabricate 204HgF090900100013 targets. In the first method macromolecular F090900100014 electrospraying was used. The target was finally F090900100015 covered with a thin foil of formvar to reduce the F090900100016 evaporation of the target material. The target had a F090900100017 mercury thickness of about 340 mu-g/cm2. The mercuro F090900100018 nitrate solution used for the preparation of the F090900100019 sprayed targets had the following isotopic composition:F090900100020 68.6% 204Hg, 10.7% 202Hg, 4.4% 201Hg, 7.6% 200 Hg, F090900100021 5.5% 199Hg and 3.2% 198Hg. F090900100022 In the second method the Aarhus mass separator was usedF090900100023 The targets had a mercury thickness of about 50mu-g/cm2F090900100024 deposited in a layer of 2Al3O about 125 mu-g/cm2 thick.F090900100025 The isotopic composition was 100% 204Hg. F090900100026 HISTORY (20080409C) F090900100027 ENDBIB 25 0 F090900100028 NOCOMMON 0 0 F090900100029 ENDSUBENT 28 0 F090900199999 SUBENT F0909002 20080505 F031F090900200001 BIB 5 9 F090900200002 REACTION (80-HG-204(D,P)80-HG-205,PAR,DA) F090900200003 FACILITY (VDGT,2DENNBI) F090900200004 DETECTOR (MAGSP,PLATE) In the NBI experiments, the reaction F090900200005 products were analyzed at 90 and 125 degr. in a single-F090900200006 gap, magnetic spectrograph, with photographic detectionF090900200007 ERR-ANALYS The experimental cross sections have a relative F090900200008 uncertainty of +-10%. The absolute scale has an F090900200009 uncertainty of +-30%. F090900200010 STATUS (TABLE) Tbl.1 p. 21 F090900200011 ENDBIB 9 0 F090900200012 COMMON 2 3 F090900200013 EN EN-RSL-FW F090900200014 MEV KEV F090900200015 12.11 12. F090900200016 ENDCOMMON 3 0 F090900200017 DATA 3 8 F090900200018 ANG-CM E-LVL DATA-CM F090900200019 ADEG MEV MU-B/SR F090900200020 90. 0. 278. F090900200021 90. 0.376 120. F090900200022 90. 0.468 251. F090900200023 90. 1.853 1267. F090900200024 125. 0. 133. F090900200025 125. 0.376 75. F090900200026 125. 0.468 122. F090900200027 125. 1.853 738. F090900200028 ENDDATA 10 0 F090900200029 ENDSUBENT 28 0 F090900299999 SUBENT F0909003 20080505 F031F090900300001 BIB 5 10 F090900300002 REACTION (80-HG-204(D,P)80-HG-205,PAR,DA,,REL) F090900300003 FACILITY (VDGT,2UK ALD) F090900300004 DETECTOR (MAGSP,PLATE)In the Aldermaston experiments, the F090900300005 reaction products were momentum analyzed in the F090900300006 multiangle spectrograph and detected in the F090900300007 photographic Ilford K2 emulsions. F090900300008 ERR-ANALYS (ANG-ERR-D) Angle digitizing error F090900300009 (ERR-DIG) Data digitizing error F090900300010 (DATA-ERR) Error from the graphic bars F090900300011 STATUS (CURVE)Fig.3 F090900300012 ENDBIB 10 0 F090900300013 COMMON 4 3 F090900300014 EN EN-RSL ANG-ERR-D ERR-DIG F090900300015 MEV KEV ADEG PER-CENT F090900300016 12.96 25. 0.134 0.004 F090900300017 ENDCOMMON 3 0 F090900300018 DATA 4 72 F090900300019 E-LVL ANG-CM DATA-CM DATA-ERR F090900300020 MEV ADEG ARB-UNITS ARB-UNITS F090900300021 0. 35.528 397.37 32.707 F090900300022 0. 42.772 644.33 46.932 F090900300023 0. 50.702 503.77 41.464 F090900300024 0. 57.944 574.74 36.468 F090900300025 0. 65.53 627.53 45.708 F090900300026 0. 73.116 521.76 33.106 F090900300027 0. 80.701 373.61 27.214 F090900300028 0. 87.941 297.29 24.469 F090900300029 0. 93.113 284.5 26.135 F090900300030 0. 100.7 256.02 25.986 F090900300031 0. 107.59 203.72 22.658 F090900300032 0. 115.52 144.6 17.501 F090900300033 0. 123.11 123.44 16.162 F090900300034 0. 130.69 92.362 11.407 F090900300035 0. 137.94 73.494 11.843 F090900300036 0. 145.52 60.042 11.538 F090900300037 1.853 35.21 780.25 74.929 F090900300038 1.853 42.026 1126.2 83.25 F090900300039 1.853 57.377 1424.1 120.94 F090900300040 1.853 65.226 1468.6 124.71 F090900300041 1.853 72.738 1313.1 111.51 F090900300042 1.853 79.896 1838.2 156.11 F090900300043 1.853 87.069 1484.4 109.73 F090900300044 1.853 92.531 1410.9 119.82 F090900300045 1.853 100.04 1248.8 92.313 F090900300046 1.853 107.22 998.19 84.767 F090900300047 1.853 115.07 806.08 59.588 F090900300048 1.853 130.09 720.89 53.291 F090900300049 1.853 137.6 664.58 56.437 F090900300050 1.853 145.46 494.67 42.008 F090900300051 1.853 152.29 437.82 37.18 F090900300052 1.853 160.14 387.51 28.646 F090900300053 1.853 167.32 297.38 25.254 F090900300054 1.853 174.82 346.55 25.618 F090900300055 2.917 57.994 813.74 59.983 F090900300056 2.917 72.727 954.56 79.515 F090900300057 2.917 80.247 686.84 44.101 F090900300058 2.917 88.105 440.26 36.674 F090900300059 2.917 93.247 494.13 36.423 F090900300060 2.917 100.78 472.54 34.832 F090900300061 2.917 107.62 391.99 32.653 F090900300062 2.917 115.49 339.94 25.058 F090900300063 2.917 122.67 267.34 17.166 F090900300064 2.917 130.2 223.74 18.638 F090900300065 2.917 137.4 251.11 23.346 F090900300066 2.917 145.62 279.31 25.969 F090900300067 2.917 152.45 187.18 15.592 F090900300068 2.917 159.63 148.52 15.258 F090900300069 2.917 174.7 144.55 16.274 F090900300070 2.952 58.077 2229.7 164.83 F090900300071 2.952 72.702 2323.3 197.3 F090900300072 2.952 80.19 1914.8 141.55 F090900300073 2.952 88.027 1198.6 101.78 F090900300074 2.952 93.123 1484.7 109.75 F090900300075 2.952 100.27 1396.9 118.63 F090900300076 2.952 108.1 1116.6 94.823 F090900300077 2.952 114.91 856.9 63.345 F090900300078 2.952 122.73 781.97 66.406 F090900300079 2.952 130.22 618.73 52.543 F090900300080 2.952 137.71 460.53 34.044 F090900300081 2.952 145.2 451.33 38.327 F090900300082 2.952 152.68 424.64 36.061 F090900300083 2.952 160.17 297.33 21.98 F090900300084 2.952 174.8 309.81 26.309 F090900300085 3.576 58.579 6350.3 468.1 F090900300086 3.576 73.355 6182.1 514.97 F090900300087 3.576 100.84 3858. 211.38 F090900300088 3.576 115.96 3286.9 273.8 F090900300089 3.576 123.17 2751.3 202.8 F090900300090 3.576 130.38 2585. 215.34 F090900300091 3.576 145.5 2182.9 99.222 F090900300092 3.576 160.28 2032.7 149.83 F090900300093 ENDDATA 74 0 F090900300094 ENDSUBENT 93 0 F090900399999 SUBENT F0909004 20080505 F031F090900400001 BIB 5 10 F090900400002 REACTION (80-HG-204(D,T)80-HG-203,PAR,DA,,REL) F090900400003 FACILITY (VDGT,2UK ALD) F090900400004 DETECTOR (MAGSP,PLATE)In the Aldermaston experiments, the F090900400005 reaction products were momentum analyzed in the F090900400006 multiangle spectrograph and detected in the F090900400007 photographic Ilford K2 emulsions. F090900400008 ERR-ANALYS (ANG-ERR-D) Angle digitizing error F090900400009 (ERR-DIG) Data digitizing error F090900400010 (DATA-ERR) Error from the graphic bars F090900400011 STATUS (CURVE)Fig.5 F090900400012 ENDBIB 10 0 F090900400013 COMMON 4 3 F090900400014 EN EN-RSL ANG-ERR-D ERR-DIG F090900400015 MEV KEV ADEG PER-CENT F090900400016 12. 50. 0.177 0.005 F090900400017 ENDCOMMON 3 0 F090900400018 DATA 4 67 F090900400019 E-LVL ANG-CM DATA-CM DATA-ERR F090900400020 MEV ADEG ARB-UNITS ARB-UNITS F090900400021 0. 43.814 891.48 65.192 F090900400022 0. 51.405 1854. 153.21 F090900400023 0. 59.339 3119.9 228.15 F090900400024 0. 67.273 4849.6 400.75 F090900400025 0. 74.86 5734.4 419.34 F090900400026 0. 82.447 6374.6 466.16 F090900400027 0. 90.033 6430.8 531.42 F090900400028 0. 95.206 6487.7 474.43 F090900400029 0. 102.45 6603. 482.86 F090900400030 0. 117.62 5939.3 434.33 F090900400031 0. 132.45 5202.8 380.47 F090900400032 0. 147.62 4361. 360.38 F090900400033 0. 169.69 3786.5 276.9 F090900400034 0. 176.93 3853.8 281.82 F090900400035 0.048 43.242 610.89 50.482 F090900400036 0.048 51.362 1037.6 75.879 F090900400037 0.048 59.471 1994.2 164.79 F090900400038 0.048 66.923 2889.8 211.32 F090900400039 0.048 74.403 3021.3 249.67 F090900400040 0.048 82.216 3390. 247.9 F090900400041 0.048 90.033 3671.7 268.5 F090900400042 0.048 94.798 3545.3 259.26 F090900400043 0.048 101.95 3026. 250.06 F090900400044 0.048 116.92 2872.4 210.05 F090900400045 0.048 131.9 2474.4 180.94 F090900400046 0.048 146.87 2328.1 170.25 F090900400047 0.048 168.67 1609.2 148.42 F090900400048 0.048 176.15 1682.5 123.04 F090900400049 0.221 43.805 22.979 5.6224 F090900400050 0.221 51.41 51.875 8.8545 F090900400051 0.221 59.365 76.257 12.238 F090900400052 0.221 66.629 95.755 13.438 F090900400053 0.221 74.586 122.36 12.37 F090900400054 0.221 81.505 143.25 14.482 F090900400055 0.221 89.118 122.37 11.197 F090900400056 0.221 94.655 116.11 12.863 F090900400057 0.221 102.27 109.22 15.327 F090900400058 0.221 116.45 120.27 15.683 F090900400059 0.221 132.03 101.85 12.277 F090900400060 0.221 146.91 88.54 11.546 F090900400061 0.221 169.4 65.181 11.126 F090900400062 0.221 176.67 59.719 10.808 F090900400063 0.544 43.06 4.0166 1.9876 F090900400064 0.544 58.685 12.985 3.9953 F090900400065 0.544 73.64 24.182 5.2572 F090900400066 0.544 88.941 30.636 6.4495 F090900400067 0.544 101.52 41.264 7.526 F090900400068 0.544 116.15 42.369 7.423 F090900400069 0.544 130.43 48.748 7.4706 F090900400070 0.544 146.08 42.757 6.868 F090900400071 0.544 168.2 24.209 5.2631 F090900400072 0.925 58.969 83.17 11.069 F090900400073 0.925 73.372 228.18 21.301 F090900400074 0.925 88.858 341.23 28.539 F090900400075 0.925 101.23 557.84 41.285 F090900400076 0.925 116.06 578.57 42.819 F090900400077 0.925 130.89 568.77 42.094 F090900400078 0.925 146.06 589.92 43.658 F090900400079 0.925 167.79 498.48 27.42 F090900400080 1.752 58.239 31.652 5.8943 F090900400081 1.752 73.919 176.88 14.854 F090900400082 1.752 88.973 246.51 20.701 F090900400083 1.752 101.3 284.61 18.421 F090900400084 1.752 116.36 346.77 29.12 F090900400085 1.752 131.42 376.06 27.944 F090900400086 1.752 146.15 328.91 24.44 F090900400087 1.752 168.41 314.71 26.97 F090900400088 ENDDATA 69 0 F090900400089 ENDSUBENT 88 0 F090900499999 SUBENT F0909005 20080505 F031F090900500001 BIB 5 9 F090900500002 REACTION (80-HG-204(D,T)80-HG-203,PAR,DA) F090900500003 FACILITY (VDGT,2DENNBI) F090900500004 DETECTOR (MAGSP,PLATE) In the NBI experiments, the reaction F090900500005 products were analyzed at 90 and 125 degr in a single- F090900500006 gap, magnetic spectrograph, with photographic detectionF090900500007 ERR-ANALYS The experimental cross sections have a relative F090900500008 uncertainty of +-10%. The absolute scale has an F090900500009 uncertainty of +-30%. F090900500010 STATUS (TABLE) Tbl.2 p.24 F090900500011 ENDBIB 9 0 F090900500012 COMMON 2 3 F090900500013 EN EN-RSL F090900500014 MEV KEV F090900500015 12.11 10. F090900500016 ENDCOMMON 3 0 F090900500017 DATA 3 27 F090900500018 ANG-CM E-LVL DATA-CM F090900500019 ADEG MEV MU-B/SR F090900500020 90. 0.048 1097. F090900500021 90. 0.221 861. F090900500022 90. 0.544 175. F090900500023 90. 0.747 49. F090900500024 90. 0.765 48. F090900500025 90. 0.925 74. F090900500026 90. 1.023 60. F090900500027 90. 1.041 272. F090900500028 90. 1.109 6. F090900500029 90. 1.326 9. F090900500030 90. 1.462 24. F090900500031 90. 1.64 15. F090900500032 90. 1.752 109. F090900500033 125. 0. 1279. F090900500034 125. 0.048 615. F090900500035 125. 0.221 546. F090900500036 125. 0.544 159. F090900500037 125. 0.747 48. F090900500038 125. 0.765 34. F090900500039 125. 0.925 123. F090900500040 125. 1.023 51. F090900500041 125. 1.041 208. F090900500042 125. 1.109 6. F090900500043 125. 1.326 7. F090900500044 125. 1.462 23. F090900500045 125. 1.64 19. F090900500046 125. 1.752 129. F090900500047 ENDDATA 29 0 F090900500048 ENDSUBENT 47 0 F090900599999 ENDENTRY 5 0 F090999999999