ENTRY O2268 20151031 O055O226800000001 SUBENT O2268001 20151031 O055O226800100001 BIB 11 27 O226800100002 TITLE The Be-9(p,p)Be-9, Be-9(p,d)Be-8 and Be-9(p,a)Li-6 O226800100003 cross-sections for analytical purposes. O226800100004 AUTHOR (S.Krat, M.Mayer, C.Porosnicu) O226800100005 REFERENCE (J,NIM/B,358,72,2015) O226800100006 REL-REF (I,O0864001,M.Mayer+,J,NIM/B,143,244,1998) O226800100007 INSTITUTE (4RUSMIF,2GERGAR) O226800100008 (3RUMRUM) National Institute for Laser, Plasma and O226800100009 Radiation Physics, Bucharest, Romania O226800100010 FACILITY (VDGT,2GERGAR) 3 MV tandem accelerator O226800100011 METHOD (SITA) O226800100012 DETECTOR (SOLST) O226800100013 SAMPLE Three samples were used. The samples consisted of O226800100014 polished pyrolytic graphite with a sputter-deposited AlO226800100015 layer on top- 3.3*E+18 at/cm**2, 27*E+18 at/cm**2, O226800100016 58*E+18 at/cm**2, respectively. On top of the aluminum O226800100017 a thin Au layer with a thickness of 7.7*E+16 at/cm**2 O226800100018 was evaporated, and on top of the gold a Be layer with O226800100019 a thickness of 4.4*E+18 at/cm**2. The purpose of the AlO226800100020 layers was to shift the signal of the C substrate O226800100021 towards lower energies in order to separate it from theO226800100022 Be signal, so that the Be signal could be measured moreO226800100023 precisely with smaller background contribution from theO226800100024 substrate. O226800100025 HISTORY (20151101C) SB O226800100026 CORRECTION Rutherford Cross section for gold was corrected on O226800100027 influence of electron shielding of the gold nuclear O226800100028 charge. O226800100029 ENDBIB 27 0 O226800100030 COMMON 1 3 O226800100031 ANG O226800100032 ADEG O226800100033 165. O226800100034 ENDCOMMON 3 0 O226800100035 ENDSUBENT 34 0 O226800199999 SUBENT O2268002 20151031 O055O226800200001 BIB 3 11 O226800200002 REACTION (4-BE-9(P,EL)4-BE-9,,DA) O226800200003 ERR-ANALYS (ERR-S,1.2,7.5).The error bars take into account the O226800200004 statistical error for the p(0) and Au peak integrals O226800200005 ranging from 1.2% to 7.5% with an average error of 3%. O226800200006 (ERR-1).The uncertainty of the solid angle for the bulkO226800200007 beryllium measurements. O226800200008 (ERR-2).The uncertainty of the SRIM 2013 stopping O226800200009 power used to quantify the cross-section O226800200010 (ERR-T).The total uncertainty is between 4.4% and 8.6%,O226800200011 with an average uncertainty of 5.4%. O226800200012 STATUS (TABLE).Table 2 of J,NIM/B,358,72,2015 O226800200013 ENDBIB 11 0 O226800200014 COMMON 2 3 O226800200015 ERR-1 ERR-2 O226800200016 PER-CENT PER-CENT O226800200017 1.5 4. O226800200018 ENDCOMMON 3 0 O226800200019 DATA 3 71 O226800200020 EN DATA ERR-T O226800200021 KEV MB/SR MB/SR O226800200022 490. 157. 7. O226800200023 591. 109. 5. O226800200024 692. 85. 4. O226800200025 792. 58. 3. O226800200026 812. 53. 3. O226800200027 833. 49. 3. O226800200028 853. 39. 3. O226800200029 873. 32. 2. O226800200030 893. 26.1 2.0 O226800200031 913. 21.0 1.8 O226800200032 933. 18.4 1.6 O226800200033 953. 23.5 1.9 O226800200034 973. 52.3 2.9 O226800200035 993. 100. 5. O226800200036 1013. 144. 6. O226800200037 1033. 162. 7. O226800200038 1054. 145. 7. O226800200039 1074. 124. 6. O226800200040 1094. 129. 6. O226800200041 1114. 121. 6. O226800200042 1134. 116. 5. O226800200043 1154. 106. 5. O226800200044 1174. 101. 4. O226800200045 1194. 102. 5. O226800200046 1244. 102. 5. O226800200047 1294. 116. 5. O226800200048 1345. 129. 6. O226800200049 1395. 127. 6. O226800200050 1445. 115. 5. O226800200051 1495. 105. 5. O226800200052 1545. 101. 5. O226800200053 1595. 94. 5. O226800200054 1645. 87. 4. O226800200055 1746. 75. 3. O226800200056 1796. 73. 3. O226800200057 1846. 74. 3. O226800200058 1896. 71. 3. O226800200059 1946. 73. 3. O226800200060 1996. 75. 3. O226800200061 2046. 75. 3. O226800200062 2096. 80. 4. O226800200063 2146. 80. 4. O226800200064 2196. 85. 4. O226800200065 2246. 84. 4. O226800200066 2296. 87. 4. O226800200067 2346. 90. 4. O226800200068 2397. 103. 5. O226800200069 2997. 34.7 2.2 O226800200070 3047. 37.6 2.4 O226800200071 3097. 35.1 2.4 O226800200072 3147. 36.4 1.9 O226800200073 3197. 35.1 1.8 O226800200074 3247. 33.9 1.7 O226800200075 3297. 34.4 1.7 O226800200076 3347. 35.9 1.9 O226800200077 3397. 35.6 1.8 O226800200078 3447. 32.9 1.7 O226800200079 3497. 33.9 1.8 O226800200080 3547. 34.6 1.8 O226800200081 3597. 33.6 1.7 O226800200082 3647. 35.9 1.9 O226800200083 3698. 35.5 1.9 O226800200084 3748. 39.5 2.1 O226800200085 3798. 36.8 2.0 O226800200086 3848. 35.2 1.9 O226800200087 3898. 36.9 2.0 O226800200088 3948. 36.9 2.0 O226800200089 3998. 37.3 2.0 O226800200090 4048. 40.6 2.7 O226800200091 4098. 39.5 2.7 O226800200092 4148. 39.7 2.6 O226800200093 ENDDATA 73 0 O226800200094 ENDSUBENT 93 0 O226800299999 SUBENT O2268003 20151031 O055O226800300001 BIB 5 10 O226800300002 REACTION ((4-BE-9(P,EL)4-BE-9,,DA)+ O226800300003 (4-BE-9(P,D)4-BE-8,PAR,DA)) O226800300004 EN-SEC (E-LVL,4-BE-8) O226800300005 COMMENT *By authors*.For energies from 2.45 to 2.95 MeV the O226800300006 energies of backscattered protons and of deuterons fromO226800300007 the 9Be(p,d0)8Be reaction overlap and cannot be O226800300008 distinguished.In that energy range, only the sum of theO226800300009 cross-sections was obtained. O226800300010 ERR-ANALYS (DATA-ERR).No information on source of uncertainty O226800300011 STATUS (TABLE).Table 2 of J,NIM/B,358,72,2015 O226800300012 ENDBIB 10 0 O226800300013 COMMON 1 3 O226800300014 E-LVL O226800300015 MEV O226800300016 0. O226800300017 ENDCOMMON 3 0 O226800300018 DATA 3 11 O226800300019 EN DATA DATA-ERR O226800300020 KEV MB/SR MB/SR O226800300021 2447. 122. 5. O226800300022 2497. 180. 8. O226800300023 2547. 203. 9. O226800300024 2597. 119. 6. O226800300025 2647. 83. 4. O226800300026 2697. 67. 4. O226800300027 2747. 57. 3. O226800300028 2797. 53. 3. O226800300029 2847. 45.8 2.6 O226800300030 2897. 45.5 2.9 O226800300031 2947. 36.8 2.3 O226800300032 ENDDATA 13 0 O226800300033 ENDSUBENT 32 0 O226800399999 SUBENT O2268004 20151031 O055O226800400001 BIB 4 20 O226800400002 REACTION (4-BE-9(P,D)4-BE-8,PAR,DA) O226800400003 ERR-ANALYS (ERR-S,1.7,23.).The error bars take into account the O226800400004 statistical error for the d(0) and Au peak integrals O226800400005 ranging from 1.7% to 23% with an average error of 11%. O226800400006 (ERR-1).The uncertainty for the product of solid angle O226800400007 times integrated beam charge for the bulk beryllium O226800400008 measurement used for absolute quantification of the O226800400009 cross-section. O226800400010 (ERR-2).The uncertainty of the SRIM 2013 stopping O226800400011 power used to quantify the cross-section O226800400012 (ERR-T).The total uncertainty is between 4.6% and 24%, O226800400013 with an average uncertainty of 12%. The highest O226800400014 uncertainties are in the range of incident energies O226800400015 from 3 to 4.15 MeV. O226800400016 STATUS (TABLE).Table 3 of J,NIM/B,358,72,2015 O226800400017 COMMENT *By authors*.The deuterons from the 9Be(p,d)8Be nuclearO226800400018 reaction overlap with protons backscattered from 9Be O226800400019 for incident proton energies from 2450 to 2950 keV. O226800400020 Within this energy range the 9Be(p,d)8Be nuclear O226800400021 reaction cross-section therefore cannot be determined. O226800400022 ENDBIB 20 0 O226800400023 COMMON 3 3 O226800400024 ERR-1 ERR-2 E-LVL O226800400025 PER-CENT PER-CENT MEV O226800400026 1.5 4. 0. O226800400027 ENDCOMMON 3 0 O226800400028 DATA 3 51 O226800400029 EN DATA ERR-T O226800400030 KEV MB/SR MB/SR O226800400031 389. 24.3 1.2 O226800400032 490. 19.0 0.9 O226800400033 591. 12.9 0.6 O226800400034 692. 6.6 0.3 O226800400035 953. 7.2 0.5 O226800400036 973. 4.3 0.3 O226800400037 993. 2.1 0.23 O226800400038 1294. 16.8 0.8 O226800400039 1345. 26.2 1.2 O226800400040 1395. 26.3 1.2 O226800400041 1445. 23.8 1.1 O226800400042 1545. 27.1 1.3 O226800400043 1595. 29.0 1.3 O226800400044 1645. 28.1 1.3 O226800400045 1695. 28.7 1.4 O226800400046 1746. 33.2 1.9 O226800400047 1796. 19.0 1.3 O226800400048 2046. 15.6 0.8 O226800400049 2096. 15.8 0.8 O226800400050 2146. 13.6 0.8 O226800400051 2196. 12.5 0.9 O226800400052 2246. 10.1 0.8 O226800400053 2296. 8.8 0.8 O226800400054 2346. 6.1 0.7 O226800400055 2397. 4.4 0.6 O226800400056 2447. 2.8 0.26 O226800400057 2947. 5.0 1.1 O226800400058 2997. 5.5 1.3 O226800400059 3047. 6.5 1.2 O226800400060 3097. 4.5 0.7 O226800400061 3147. 5.1 0.8 O226800400062 3197. 5.3 0.7 O226800400063 3247. 6.4 1.0 O226800400064 3297. 7.6 1.7 O226800400065 3347. 10.0 1.7 O226800400066 3397. 10.7 1.5 O226800400067 3447. 8.4 1.5 O226800400068 3497. 7.8 1.4 O226800400069 3547. 8.0 1.6 O226800400070 3597. 9.5 1.6 O226800400071 3647. 10.9 2.1 O226800400072 3698. 11.0 1.6 O226800400073 3748. 11.3 1.8 O226800400074 3798. 11.2 1.6 O226800400075 3848. 8.7 1.7 O226800400076 3898. 12.1 1.9 O226800400077 3948. 9.7 1.3 O226800400078 3998. 11.5 1.4 O226800400079 4048. 11.3 1.3 O226800400080 4098. 10.6 1.5 O226800400081 4148. 13.2 1.5 O226800400082 ENDDATA 53 0 O226800400083 ENDSUBENT 82 0 O226800499999 SUBENT O2268005 20151031 O055O226800500001 BIB 3 13 O226800500002 REACTION (4-BE-9(P,A)3-LI-6,PAR,DA) O226800500003 ERR-ANALYS (ERR-S,1.5,2.7).The error bars take into account the O226800500004 statistical error for the a(0) and Au peak integrals O226800500005 ranging from 1.5% to 2.7% with an average error of 1.8%O226800500006 (ERR-1).The uncertainty for the product of solid angle O226800500007 times integrated beam charge for the bulk beryllium O226800500008 measurement used for absolute quantification of the O226800500009 cross-section. O226800500010 (ERR-2).The uncertainty of the SRIM 2013 stopping O226800500011 power used to quantify the cross-section O226800500012 (ERR-T).The total uncertainty is between 4.5% and 5%, O226800500013 with an average uncertainty of 4.6%. O226800500014 STATUS (TABLE).Table 4 of J,NIM/B,358,72,2015 O226800500015 ENDBIB 13 0 O226800500016 COMMON 3 3 O226800500017 ERR-1 ERR-2 E-LVL O226800500018 PER-CENT PER-CENT MEV O226800500019 1.5 4. 0. O226800500020 ENDCOMMON 3 0 O226800500021 DATA 3 27 O226800500022 EN DATA ERR-T O226800500023 KEV MB/SR MB/SR O226800500024 389. 23.1 1.1 O226800500025 490. 7.8 0.4 O226800500026 591. 8.1 0.4 O226800500027 692. 8.8 0.4 O226800500028 792. 9.8 0.5 O226800500029 812. 10.3 0.5 O226800500030 833. 11.1 0.5 O226800500031 853. 11.3 0.5 O226800500032 873. 11.3 0.5 O226800500033 893. 12.4 0.6 O226800500034 913. 12.6 0.6 O226800500035 933. 13.0 0.6 O226800500036 953. 12.1 0.6 O226800500037 973. 9.5 0.4 O226800500038 993. 8.1 0.4 O226800500039 1013. 7.1 0.3 O226800500040 1033. 6.8 0.3 O226800500041 1054. 6.9 0.3 O226800500042 1074. 6.9 0.3 O226800500043 1094. 7.5 0.4 O226800500044 1114. 7.6 0.4 O226800500045 1134. 7.7 0.4 O226800500046 1154. 8.3 0.4 O226800500047 1174. 8.3 0.4 O226800500048 1194. 8.9 0.4 O226800500049 1244. 10.6 0.5 O226800500050 1294. 10.0 0.5 O226800500051 ENDDATA 29 0 O226800500052 ENDSUBENT 51 0 O226800599999 ENDENTRY 5 0 O226899999999