ENTRY O1590 20080123 O034O159000000001 SUBENT O1590001 20080123 O034O159000100001 BIB 13 51 O159000100002 TITLE Experimental study of proton-induced nuclear reactions O159000100003 in Li-6, Li-7. O159000100004 AUTHOR (J.Cruz, H.Luis, M.Fonseca, Z.Fulop, G.Gyurky, O159000100005 F.Raiola, M.Aliotta, K.U.Kettner, A.P.Jesus, O159000100006 J.P.Ribeiro, F.C.Barker, C.Rolfs) O159000100007 INSTITUTE (2PRTNOV) O159000100008 (2PRTLIS) O159000100009 (3HUNDEB) O159000100010 (2GERBOC) O159000100011 (2UK EDG) School of Physics. O159000100012 (2GERGER) Fachhochschule Bieleferd. O159000100013 (3AULCBR) O159000100014 REFERENCE (J,JP/G,35,014004,2008) O159000100015 (J,PL/B,624,181,2005) it is O1282 and data for same O159000100016 reactions but with incident energy from 30 to 100 keV.O159000100017 ADD-RES (THEO) The plasma model of Debye. O159000100018 DETECTOR (SIBAR) Two mobile Si-detectors, active area=50 mm**2. O159000100019 FACILITY (VDG,2PRTJES) The 2.5 MV Van de Graaff accelerator. O159000100020 SAMPLE A Li-7 implanted into Al target with (6.6+-0.4)E+17 O159000100021 Li-7/cm**2 was used for the measurement of angular O159000100022 distributions for Li-7(p,a). O159000100023 Excitation functions for both Li reactions were O159000100024 measured with three targets- two LiF targets- O159000100025 (6.1+-0.2)*E+17 Li-7/cm**2 and (9.0+-0.4)*E+17 Li-7/ O159000100026 cm**2- vacuum-evaporated on Ag and Cu backing( Li of O159000100027 natural isotopic composition-92.58% Li-7, 7.42% Li-6) O159000100028 and the Li-7 implanted into Al target, which were O159000100029 positioned inside the target chamber. O159000100030 METHOD (BCINT) The beam current on target was kept below O159000100031 200 nA. O159000100032 (SITA) O159000100033 COMMENT *By authors*.The effective energy E within the target O159000100034 was derived from the incident energy of the ion beam O159000100035 and the energy loss of the beam in the target. O159000100036 ERR-ANALYS (ERR-1). The quoted uncertainties for S(E) arise from O159000100037 uncertainty in the number of incident protons, measuredO159000100038 by a charge integrator and was obtained as 4%. O159000100039 The statistical uncertainty associated with N(E(o),ang-O159000100040 lab). O159000100041 (ERR-2).A 5% uncertainty in stopping cross sections O159000100042 affects not only S(E) but also the effective energy. O159000100043 However, simulations show that the 5% uncertainty O159000100044 propagates into very small variations in energy- O159000100045 less 0.5% and in S(E) less 3.7%. O159000100046 (ERR-3).The uncertainty associated with the measurementO159000100047 of the angular distributions is very small, less than O159000100048 0.2%. O159000100049 These uncertainties were added quadratically. O159000100050 (DATA-ERR).The data were received from authors in tableO159000100051 STATUS (TABLE).The data were received from Joao Cruz 22.01.08 O159000100052 HISTORY (20080123C) SB O159000100053 ENDBIB 51 0 O159000100054 COMMON 3 3 O159000100055 ERR-1 ERR-2 ERR-3 O159000100056 PER-CENT PER-CENT PER-CENT O159000100057 4. 5. 0.2 O159000100058 ENDCOMMON 3 0 O159000100059 ENDSUBENT 58 0 O159000199999 SUBENT O1590002 20080123 O034O159000200001 BIB 2 3 O159000200002 REACTION (3-LI-7(P,A)2-HE-4,,SIG,,SFC) Figure 2 O159000200003 ADD-RES Electron screening potential has been found as O159000200004 237(+133/-77) eV. O159000200005 ENDBIB 3 0 O159000200006 NOCOMMON 0 0 O159000200007 DATA 3 94 O159000200008 EN DATA DATA-ERR O159000200009 KEV B*KEV B*KEV O159000200010 89.71 77.23 9.28 O159000200011 92.35 71.05 4.14 O159000200012 95.09 71.92 4.73 O159000200013 101.11 72.05 3.45 O159000200014 110.32 69.43 3.13 O159000200015 115.83 73.6 5.04 O159000200016 119.96 73.85 3. O159000200017 127.94 73.39 2.37 O159000200018 138.54 72.76 2.41 O159000200019 148.72 77.04 2.85 O159000200020 161.4 77.78 2.45 O159000200021 172.66 81.68 4. O159000200022 186.28 78.94 2.4 O159000200023 199.69 84.81 4.08 O159000200024 213.02 81.37 2.43 O159000200025 228.75 82.12 3.73 O159000200026 239.02 81.17 3.11 O159000200027 244.05 82.75 3.83 O159000200028 259.72 84.45 5.91 O159000200029 267.52 81.67 3.31 O159000200030 270.64 82. 3.84 O159000200031 274.73 84.9 3.2 O159000200032 286.52 81.98 3.46 O159000200033 292.44 84.17 5.84 O159000200034 297.41 81.84 3.27 O159000200035 302.83 85.05 3.07 O159000200036 307.94 86.96 2.4 O159000200037 319.18 88.51 2.89 O159000200038 328.91 88.16 2.56 O159000200039 336.73 87.45 3.16 O159000200040 344.71 86.76 6.07 O159000200041 352.89 88.08 1.89 O159000200042 362.09 85.9 3.25 O159000200043 372.35 90.1 3.18 O159000200044 375.64 91.18 3.27 O159000200045 381.71 89.53 4.12 O159000200046 389.19 89.46 2.47 O159000200047 398.41 92.39 3.21 O159000200048 417.02 87.65 4.27 O159000200049 421.89 91.83 3.35 O159000200050 424.91 90.95 2.58 O159000200051 432.69 90.86 3.44 O159000200052 443.99 88.13 3.32 O159000200053 453. 93.22 3.24 O159000200054 462.45 89.33 4.03 O159000200055 470.42 89.71 2.54 O159000200056 483.4 92.77 3.48 O159000200057 501.98 92.26 2.94 O159000200058 509.34 93. 3.53 O159000200059 514.8 96.6 3.49 O159000200060 529.98 95.51 3.41 O159000200061 543.28 93.63 4.26 O159000200062 547.08 94.06 3.11 O159000200063 550.61 92.71 2.72 O159000200064 558.88 97.35 3.63 O159000200065 580.46 95.69 3.14 O159000200066 587.25 96.81 2.79 O159000200067 592.03 96.58 3.6 O159000200068 614.62 100.17 3.78 O159000200069 618.89 97.38 4.17 O159000200070 630.12 97.37 4.47 O159000200071 635.63 95.71 3.59 O159000200072 649.86 100.9 5.11 O159000200073 675.65 98.75 4.81 O159000200074 681.31 98.05 3.15 O159000200075 685.24 101.98 3.49 O159000200076 714.42 100.36 6.77 O159000200077 722.85 104.4 2.8 O159000200078 747.26 103.97 3.53 O159000200079 762.35 106.56 3.33 O159000200080 770.87 106.17 3.45 O159000200081 779.3 105.83 3.34 O159000200082 800.25 109.14 2.64 O159000200083 817.11 107.3 4.96 O159000200084 820.25 109.61 3.95 O159000200085 860.75 110.52 4.61 O159000200086 902.15 117.62 4.16 O159000200087 944.54 120.2 4.43 O159000200088 949.38 123.15 5.67 O159000200089 988.03 126.03 5.31 O159000200090 1032.43 133.08 5.9 O159000200091 1077.73 135.99 4.83 O159000200092 1081.41 139.06 6.64 O159000200093 1123.03 144.86 3.77 O159000200094 1171.49 153.98 5.06 O159000200095 1214.26 152.86 7.64 O159000200096 1223.6 160.08 4.22 O159000200097 1278.4 173.47 6.95 O159000200098 1343.31 187.21 5.66 O159000200099 1405.73 198.02 8.26 O159000200100 1471.66 216.99 9.63 O159000200101 1477.06 222.98 10.46 O159000200102 1608.73 265.03 12.78 O159000200103 1740.31 319.57 16.15 O159000200104 ENDDATA 96 0 O159000200105 ENDSUBENT 104 0 O159000299999 SUBENT O1590003 20080123 O034O159000300001 BIB 2 3 O159000300002 REACTION (3-LI-6(P,HE3)2-HE-4,,SIG,,SFC) Figure 3. O159000300003 ADD-RES Electron screening potential has been found as O159000300004 273+/-111 eV. O159000300005 ENDBIB 3 0 O159000300006 NOCOMMON 0 0 O159000300007 DATA 3 20 O159000300008 EN DATA DATA-ERR O159000300009 KEV B*MEV B*MEV O159000300010 90.46 3.42 0.15 O159000300011 99.04 3.21 0.17 O159000300012 108.06 2.99 0.1 O159000300013 117.51 3.09 0.08 O159000300014 127.39 3.08 0.09 O159000300015 137.67 2.98 0.08 O159000300016 159.47 2.92 0.07 O159000300017 182.83 2.84 0.07 O159000300018 207.72 2.8 0.08 O159000300019 234.13 2.72 0.07 O159000300020 262.05 2.65 0.08 O159000300021 291.44 2.63 0.12 O159000300022 322.31 2.47 0.07 O159000300023 354.67 2.43 0.06 O159000300024 388.51 2.5 0.09 O159000300025 423.84 2.4 0.11 O159000300026 460.64 2.26 0.09 O159000300027 498.92 2.29 0.08 O159000300028 538.67 2.18 0.12 O159000300029 579.91 2.18 0.13 O159000300030 ENDDATA 22 0 O159000300031 ENDSUBENT 30 0 O159000399999 ENDENTRY 3 0 O159099999999