ENTRY A0632 20210317 A098A063200000001 SUBENT A0632001 20210317 A098A063200100001 BIB 8 46 A063200100002 TITLE Isotopic dependence of electron screening in fusion A063200100003 reactions A063200100004 AUTHOR (S.Engstler, G.Raimann, C.Angulo, U.Greife, C.Rolfs, A063200100005 U.Schroder, E.Somorjai, B.Kirch, K.Langanke) A063200100006 REFERENCE (J,ZP/A,342,471,1992) - final publ., data tables A063200100007 (J,PL/B,279,20,1992) - data only on figs. A063200100008 INSTITUTE (2GERBOC,2GERMST) A063200100009 FACILITY (CCW,2GERMST) The accelerator (350 kV) A063200100010 (CCW,2GERBOC) the accelerators (100 kV and 400 kV) A063200100011 (VDG,2GERBOC) the accelerator (4 MV) A063200100012 The energy spread: A063200100013 +-0.020 keV for 100 kV accelerator. A063200100014 +-0.3 keV for 350 kV accelerator. A063200100015 +-1.0 keV for 400 kV and 4. MV accelerators. A063200100016 Accelerators provided p, d, 6Li, and 7Li ion beams in A063200100017 the c.m. energy range E = 10 to 1450 keV. At the lowestA063200100018 energies, the p and d beam currents on target were A063200100019 600 uA and those of the 6-Li and 7-Li beams were 40 uA.A063200100020 At higher energies the currents were limited by A063200100021 dead time effects in the detectors (kept below 3%) or A063200100022 by requirements of the beam calorimeters. The A063200100023 absolute ion beam energy of the accelerators is known A063200100024 to sufficient precision and has been tested for the A063200100025 350 and 400 KV accelerators during the course of the A063200100026 experiments. A063200100027 COMMENT The fusion reactions 6Li(p,alpha)3He, 6Li(d,alpha) A063200100028 4He, and 7Li(p,alpha) 4He have been studied over the A063200100029 c.m. energy range E= 10 to 1450 keV. Each reaction A063200100030 involved the use of hydrogen projectiles and LiF A063200100031 solid targets as well as Li projectiles and hydrogen A063200100032 molecular gas targets. In all cases the effects of A063200100033 electron screening on the low-energy fusion cross A063200100034 sections (exponential enhancement) have been A063200100035 observed; the effects are somewhat stronger in the A063200100036 case of atomic p or d projectiles compared to the A063200100037 case of molecular H2 or D2 gas targets. If isotopic A063200100038 effects on electron screening are negligible, all A063200100039 three reactions should exhibit the same enhancements A063200100040 for each set of experimental techniques. The A063200100041 measurements confirmed this expectation to a large A063200100042 extent. A063200100043 ADD-RES Screening potential energies. A063200100044 HISTORY (19990601C) by F.C. A063200100045 (19990621A) Date is corrected A063200100046 (20000427U) last checking has been done. A063200100047 (20210317A) SD: Entry re-compiled. A063200100048 ENDBIB 46 0 A063200100049 NOCOMMON 0 0 A063200100050 ENDSUBENT 49 0 A063200199999 SUBENT A0632002 20210317 A098A063200200001 BIB 7 24 A063200200002 REACTION ((1-H-1(3-LI-6,HE3)2-HE-4,,SIG,,SFC)= A063200200003 (3-LI-6(P,HE3)2-HE-4,,SIG,,SFC)) A063200200004 SAMPLE The hydrogen gas (H2 = 99.99% or D2 = 99.9%) was A063200200005 not recirculated. The H2 (D2) gas pressure given above A063200200006 was reduced to 1.8 x 10**(-2) (7.5 x 10**(-3)) mbar A063200200007 and 1.8 x 10**(-5) (5 x 10**(-6)) mbar in the region A063200200008 of the first and fourth pumping stage, respectively. A063200200009 Disk-shaped target chamber (20 cm diameter, A063200200010 3 cm height) was used. A063200200011 METHOD Inverse kinematics A063200200012 DETECTOR (SIBAR) Seven surface-barrier detectors were A063200200013 placed at 30. to 135. degr. A063200200014 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063200200015 number of counts, angular distributions, and A063200200016 effective energy. A063200200017 (ERR-2) All values have an additional common error A063200200018 of 7% due to A063200200019 * uncertainties in proton beam (1% and 2.5%) A063200200020 * uncertainties in pressure (2%), and A063200200021 * uncertainty in target thickness and solid A063200200022 angle 6.4% A063200200023 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063200200024 HISTORY (20210317A) SD: SF6=SGV -> SIG; SF9=EXP deleted from A063200200025 REACTION code. Subent was split in three. ERR-T->ERR-1.A063200200026 ENDBIB 24 0 A063200200027 COMMON 1 3 A063200200028 ERR-2 A063200200029 PER-CENT A063200200030 7.0 A063200200031 ENDCOMMON 3 0 A063200200032 DATA 3 16 A063200200033 EN-CM DATA ERR-1 A063200200034 KEV B*MEV B*MEV A063200200035 30.28 3.67 0.31 A063200200036 35.16 3.94 0.32 A063200200037 40.05 3.85 0.30 A063200200038 44.04 3.78 0.29 A063200200039 49.91 3.51 0.27 A063200200040 54.86 3.62 0.27 A063200200041 59.76 3.57 0.27 A063200200042 98.00 3.66 0.28 A063200200043 147.50 3.24 0.23 A063200200044 198.80 2.93 0.21 A063200200045 249.10 2.84 0.20 A063200200046 299.40 2.57 0.18 A063200200047 349.80 2.43 0.17 A063200200048 400.10 2.29 0.16 A063200200049 450.40 2.12 0.15 A063200200050 500.80 2.07 0.16 A063200200051 ENDDATA 18 0 A063200200052 ENDSUBENT 51 0 A063200299999 SUBENT A0632003 20210317 A098A063200300001 BIB 7 24 A063200300002 REACTION ((1-H-2(3-LI-6,A)2-HE-4,,SIG,,SFC)= A063200300003 (3-LI-6(D,A)2-HE-4,,SIG,,SFC)) A063200300004 SAMPLE The hydrogen gas (H2 = 99.99% or D2 = 99.9%) was A063200300005 not recirculated. The H2 (D2) gas pressure given above A063200300006 was reduced to 1.8 x 10**(-2) (7.5 x 10**(-3)) mbar A063200300007 and 1.8 x 10**(-5) (5 x 10**(-6)) mbar in the region A063200300008 of the first and fourth pumping stage, respectively. A063200300009 Disk-shaped target chamber (20 cm diameter, A063200300010 3 cm height) was used. A063200300011 METHOD Inverse kinematics A063200300012 DETECTOR (SIBAR) Seven surface-barrier (Si) detectors were A063200300013 placed at 30. to 135. degr. A063200300014 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063200300015 number of counts, angular distributions, and A063200300016 effective energy. A063200300017 (ERR-2) All values have an additional common error A063200300018 of 7% due to A063200300019 * uncertainties in proton beam (1% and 2.5%) A063200300020 * uncertainties in pressure (2%), and A063200300021 * uncertainty in target thickness and solid A063200300022 angle 6.4% A063200300023 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063200300024 HISTORY (20210317A) SD: SF6=SGV -> SIG; SF9=EXP deleted from A063200300025 REACTION code. Subent was split in three. ERR-T->ERR-1.A063200300026 ENDBIB 24 0 A063200300027 COMMON 1 3 A063200300028 ERR-2 A063200300029 PER-CENT A063200300030 7.0 A063200300031 ENDCOMMON 3 0 A063200300032 DATA 3 25 A063200300033 EN-CM DATA ERR-1 A063200300034 KEV B*MEV B*MEV A063200300035 36.91 15.8 1.5 A063200300036 41.84 15.2 1.4 A063200300037 51.70 17.3 1.4 A063200300038 61.60 17.2 1.4 A063200300039 71.59 16.8 1.3 A063200300040 81.49 16.3 1.2 A063200300041 91.39 16.0 1.2 A063200300042 101.4 15.0 1.1 A063200300043 148.7 13.0 1.0 A063200300044 198.5 10.1 0.7 A063200300045 248.3 8.1 0.6 A063200300046 299.2 6.2 0.4 A063200300047 349.4 5.0 0.4 A063200300048 399.6 4.0 0.3 A063200300049 449.8 3.33 0.23 A063200300050 500.1 2.78 0.19 A063200300051 550.3 2.31 0.16 A063200300052 600.5 1.99 0.14 A063200300053 650.7 1.69 0.12 A063200300054 701.0 1.46 0.10 A063200300055 751.2 1.28 0.09 A063200300056 801.4 1.12 0.08 A063200300057 851.6 1.02 0.07 A063200300058 901.8 0.93 0.06 A063200300059 952.0 0.84 0.06 A063200300060 ENDDATA 27 0 A063200300061 ENDSUBENT 60 0 A063200399999 SUBENT A0632004 20210317 A098A063200400001 BIB 7 24 A063200400002 REACTION ((1-H-1(3-LI-7,A)2-HE-4,,SIG,,SFC)= A063200400003 (3-LI-7(P,A)2-HE-4,,SIG,,SFC)) A063200400004 SAMPLE The hydrogen gas (H2 = 99.99% or D2 = 99.9%) was A063200400005 not recirculated. The H2 (D2) gas pressure given above A063200400006 was reduced to 1.8 x 10**(-2) (7.5 x 10**(-3)) mbar A063200400007 and 1.8 x 10**(-5) (5 x 10**(-6)) mbar in the region A063200400008 of the first and fourth pumping stage, respectively. A063200400009 Disk-shaped target chamber (20 cm diameter, A063200400010 3 cm height) was used. A063200400011 METHOD Inverse kinematics A063200400012 DETECTOR (SIBAR) Seven surface-barrier (Si) detectors were A063200400013 placed at 30. to 135. degr. A063200400014 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063200400015 number of counts, angular distributions, and A063200400016 effective energy. A063200400017 (ERR-2) All values have an additional common error A063200400018 of 7% due to A063200400019 * uncertainties in proton beam (1% and 2.5%) A063200400020 * uncertainties in pressure (2%), and A063200400021 * uncertainty in target thickness and solid A063200400022 angle 6.4% A063200400023 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063200400024 HISTORY (20210317A) SD: SF6=SGV -> SIG; SF9=EXP deleted from A063200400025 REACTION code. Subent was split in three. ERR-T->ERR-1.A063200400026 ENDBIB 24 0 A063200400027 COMMON 1 3 A063200400028 ERR-2 A063200400029 PER-CENT A063200400030 7.0 A063200400031 ENDCOMMON 3 0 A063200400032 DATA 3 14 A063200400033 EN-CM DATA ERR-1 A063200400034 KEV B*MEV B*MEV A063200400035 40.37 68. 5. A063200400036 45.34 70. 5. A063200400037 50.26 73. 6. A063200400038 55.13 73. 6. A063200400039 98.59 79. 6. A063200400040 199.5 84. 6. A063200400041 300.1 89. 6. A063200400042 400.7 85. 6. A063200400043 501.3 85. 6. A063200400044 601.9 97. 7. A063200400045 702.5 94. 7. A063200400046 803.0 99. 7. A063200400047 903.6 110. 8. A063200400048 1004.1 113. 8. A063200400049 ENDDATA 16 0 A063200400050 ENDSUBENT 49 0 A063200499999 SUBENT A0632005 20210317 A098A063200500001 BIB 7 20 A063200500002 REACTION ((1-H-1(3-LI-6,HE3)2-HE-4,,DA,A,REL)= A063200500003 (3-LI-6(P,HE3)2-HE-4,,DA,,REL)) A063200500004 The observed number of counts in each detector A063200500005 corrected for its solid angle. A063200500006 SAMPLE The hydrogen gas (H2 = 99.99% or D2 = 99.9%) was A063200500007 not recirculated. The H2 (D2) gas pressure given above A063200500008 was reduced to 1.8 x 10**(-2) (7.5 x 10**(-3)) mbar A063200500009 and 1.8 x 10**(-5) (5 x 10**(-6)) mbar in the region A063200500010 of the first and fourth pumping stage, respectively. A063200500011 Disk-shaped target chamber (20 cm diameter, A063200500012 3 cm height) was used. A063200500013 METHOD Inverse kinematics A063200500014 DETECTOR (SIBAR) Seven surface-barrier detectors were A063200500015 placed at 30. to 135. degr. A063200500016 STATUS (CURVE) Fig. 5 from Z.Phys.,A342(1992)471 A063200500017 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063200500018 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063200500019 Data from Subent 006 were added. A063200500020 ANG-ERR -> ANG-ERR-D; DATA-ERR -> ERR-DIG; A063200500021 ERR-T -> DATA-ERR. A063200500022 ENDBIB 20 0 A063200500023 COMMON 3 3 A063200500024 ANG-ERR-D ERR-DIG EN-RSL-HW A063200500025 ADEG PER-CENT KEV A063200500026 0.6 1. 1.0 A063200500027 ENDCOMMON 3 0 A063200500028 DATA 4 23 A063200500029 EN-CM ANG-CM DATA-CM DATA-ERR A063200500030 KEV ADEG ARB-UNITS PER-CENT A063200500031 300. 30.3 1.970E+04 5. A063200500032 300. 42.4 2.010E+04 3. A063200500033 300. 51.5 1.897E+04 A063200500034 300. 56.9 1.980E+04 A063200500035 300. 73.0 1.905E+04 A063200500036 300. 78.4 1.889E+04 A063200500037 300. 80.4 1.597E+04 A063200500038 300. 91.6 1.666E+04 A063200500039 300. 111.9 1.500E+04 A063200500040 300. 121.4 1.392E+04 A063200500041 300. 133.8 1.201E+04 A063200500042 300. 138.4 1.236E+04 A063200500043 300. 150.8 1.280E+04 4. A063200500044 300. 161.0 9.300E+03 9. A063200500045 500. 22.2 6.620E+04 4. A063200500046 500. 31.2 5.550E+04 5. A063200500047 500. 45.8 6.050E+04 A063200500048 500. 61.9 5.690E+04 A063200500049 500. 87.2 4.760E+04 A063200500050 500. 97.5 4.960E+04 A063200500051 500. 106.2 4.070E+04 A063200500052 500. 114.8 3.750E+04 A063200500053 500. 141.2 2.468E+04 A063200500054 ENDDATA 25 0 A063200500055 ENDSUBENT 54 0 A063200599999 NOSUBENT A0632006 20210317 A098A063200600001 SUBENT A0632007 20210317 A098A063200700001 BIB 7 17 A063200700002 REACTION (3-LI-6(P,HE3)2-HE-4,,DA,,REL) A063200700003 The observed number of counts in each detector A063200700004 corrected for its solid angle. A063200700005 SAMPLE (3-LI-6,ENR=0.95) A 1.1 ug/cm2 thick LiF target on a A063200700006 Ta backing A063200700007 Cyclindrical target chamber (close geometry) A063200700008 DETECTOR (SI) Six Si detectors (300 to 600 mm2 active area) wereA063200700009 mounted at 60. to 160. degr. and covered with 1.25 um A063200700010 thick Ni foils to stop the elastically scattered A063200700011 particles. A063200700012 METHOD Normal kinematics. A063200700013 STATUS (CURVE) Fig. 5 from Z.Phys.,A342(1992)471 A063200700014 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063200700015 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063200700016 Data from Subents 008-009 were added. A063200700017 ANG-ERR -> ANG-ERR-D; DATA-ERR -> ERR-DIG; A063200700018 ERR-T -> DATA-ERR. A063200700019 ENDBIB 17 0 A063200700020 COMMON 3 3 A063200700021 ANG-ERR-D ERR-DIG EN-RSL-HW A063200700022 ADEG PER-CENT KEV A063200700023 0.6 1. 0.3 A063200700024 ENDCOMMON 3 0 A063200700025 DATA 4 32 A063200700026 EN-CM ANG-CM DATA-CM DATA-ERR A063200700027 KEV ADEG ARB-UNITS PER-CENT A063200700028 26. 19.3 2170. 10. A063200700029 26. 38.7 1720. 8. A063200700030 26. 61.7 2310. 6. A063200700031 26. 77.8 2330. 5. A063200700032 26. 106.9 2480. 8. A063200700033 26. 118.5 2300. 7. A063200700034 26. 121.3 1770. 11. A063200700035 26. 140.9 2680. 5. A063200700036 26. 160.4 2610. 5. A063200700037 86. 18.4 4040. A063200700038 86. 38.3 4000. A063200700039 86. 63.2 4010. A063200700040 86. 71.9 4250. A063200700041 86. 78.9 4000. A063200700042 86. 100.9 3710. A063200700043 86. 107.1 4070. A063200700044 86. 116.6 3780. A063200700045 86. 122.9 3750. A063200700046 86. 141.9 3740. A063200700047 86. 160.6 3700. A063200700048 100. 44.7 5700. 9. A063200700049 100. 56.8 6300. 6. A063200700050 100. 63.4 6260. A063200700051 100. 70.9 6600. 5. A063200700052 100. 83.7 6060. A063200700053 100. 93.7 6950. 2.3 A063200700054 100. 100.3 6550. A063200700055 100. 102.8 6130. A063200700056 100. 116.8 5700. 7. A063200700057 100. 120.6 6020. A063200700058 100. 130.1 6100. 8. A063200700059 100. 143. 5700. 9. A063200700060 ENDDATA 34 0 A063200700061 ENDSUBENT 60 0 A063200799999 NOSUBENT A0632008 20210317 A098A063200800001 NOSUBENT A0632009 20210317 A098A063200900001 SUBENT A0632010 20210317 A098A063201000001 BIB 7 20 A063201000002 REACTION ((1-H-2(3-LI-6,A)2-HE-4,,DA,A,REL)= A063201000003 (3-LI-6(D,A)2-HE-4,,DA,,REL)) A063201000004 The observed number of counts in each detector A063201000005 corrected for its solid angle. A063201000006 SAMPLE The hydrogen gas (H2 = 99.99% or D2 = 99.9%) was A063201000007 not recirculated. The H2 (D2) gas pressure given above A063201000008 was reduced to 1.8 x 10**(-2) (7.5 x 10**(-3)) mbar A063201000009 and 1.8 x 10**(-5) (5 x 10**(-6)) mbar in the region A063201000010 of the first and fourth pumping stage, respectively. A063201000011 Disk-shaped target chamber (20 cm diameter, A063201000012 3 cm height) was used. A063201000013 METHOD Inverse kinematics A063201000014 DETECTOR (SIBAR) Seven surface-barrier detectors were A063201000015 placed at 30. to 135. degr. A063201000016 STATUS (CURVE) Fig. 5 from Z.Phys.,A342(1992)471 A063201000017 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063201000018 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063201000019 Data from Subents 011-013 were added. A063201000020 ANG-ERR -> ANG-ERR-D; DATA-ERR -> ERR-DIG; A063201000021 ERR-T -> DATA-ERR. A063201000022 ENDBIB 20 0 A063201000023 COMMON 3 3 A063201000024 ANG-ERR-D ERR-DIG EN-RSL-HW A063201000025 ADEG PER-CENT KEV A063201000026 0.6 1. 1.0 A063201000027 ENDCOMMON 3 0 A063201000028 DATA 4 28 A063201000029 EN-CM ANG-CM DATA-CM DATA-ERR A063201000030 KEV ADEG ARB-UNITS PER-CENT A063201000031 200. 35.5 3380. A063201000032 200. 52.2 3550. A063201000033 200. 68.4 3290. A063201000034 200. 83.9 3560. A063201000035 200. 99.3 3450. A063201000036 200. 114.3 3220. 5. A063201000037 200. 128.4 3390. 4. A063201000038 600. 37.9 7700. A063201000039 600. 57.5 7250. A063201000040 600. 74.5 6530. A063201000041 600. 90.3 6750. A063201000042 600. 106.2 6690. 2.7 A063201000043 600. 120.8 6970. 4. A063201000044 600. 134.1 7300. 4. A063201000045 1000. 40.7 1.859E+04 A063201000046 1000. 60.2 1.534E+04 A063201000047 1000. 78.9 1.332E+04 A063201000048 1000. 85.6 1.38E+04 A063201000049 1000. 111.4 1.395E+04 A063201000050 1000. 125.2 1.56E+04 4. A063201000051 1000. 138.6 1.86E+04 4. A063201000052 1450. 42.2 4.46E+04 A063201000053 1450. 62.6 3.7E+04 A063201000054 1450. 82.1 2.924E+04 A063201000055 1450. 100. 3.024E+04 A063201000056 1450. 115.5 3.67E+04 A063201000057 1450. 128.8 3.8E+04 6. A063201000058 1450. 141.8 4.9E+04 5. A063201000059 ENDDATA 30 0 A063201000060 ENDSUBENT 59 0 A063201099999 NOSUBENT A0632011 20210317 A098A063201100001 NOSUBENT A0632012 20210317 A098A063201200001 NOSUBENT A0632013 20210317 A098A063201300001 SUBENT A0632014 20210317 A098A063201400001 BIB 7 16 A063201400002 REACTION (3-LI-6(D,A)2-HE-4,,DA,,REL) A063201400003 The observed number of counts in each detector A063201400004 corrected for its solid angle. A063201400005 SAMPLE (3-LI-6,ENR=0.95) A 1.1 ug/cm2 thick LiF target on a A063201400006 Ta backing A063201400007 Cyclindrical target chamber (close geometry) A063201400008 DETECTOR (SI) Six Si detectors (300 to 600 mm2 active area) wereA063201400009 mounted at 60. to 160. degr. and covered with 1.25 um A063201400010 thick Ni foils to stop the elastically scattered A063201400011 particles. A063201400012 METHOD Normal kinematics. A063201400013 STATUS (CURVE) Fig. 5 from Z.Phys.,A342(1992)471 A063201400014 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063201400015 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063201400016 ANG-ERR -> ANG-ERR-D; DATA-ERR -> ERR-DIG; A063201400017 ERR-T -> DATA-ERR. A063201400018 ENDBIB 16 0 A063201400019 COMMON 4 3 A063201400020 EN-CM ANG-ERR-D ERR-DIG EN-RSL-HW A063201400021 KEV ADEG PER-CENT KEV A063201400022 43. 0.6 1. 0.3 A063201400023 ENDCOMMON 3 0 A063201400024 DATA 3 7 A063201400025 ANG-CM DATA-CM DATA-ERR A063201400026 ADEG ARB-UNITS PER-CENT A063201400027 32.4 1552. A063201400028 47.8 1580. 3. A063201400029 79.5 1620. 4. A063201400030 94.9 1610. 4. A063201400031 109.1 1840. 6. A063201400032 124.0 1500. 7. A063201400033 137.8 1640. 7. A063201400034 ENDDATA 9 0 A063201400035 ENDSUBENT 34 0 A063201499999 SUBENT A0632015 20210317 A098A063201500001 BIB 7 20 A063201500002 REACTION ((1-H-1(3-LI-7,A)2-HE-4,,DA,,REL)= A063201500003 (3-LI-7(P,A)2-HE-4,,DA,,REL)) A063201500004 The observed number of counts in each detector A063201500005 corrected for its solid angle. A063201500006 SAMPLE The hydrogen gas (H2 = 99.99% or D2 = 99.9%) was A063201500007 not recirculated. The H2 (D2) gas pressure given above A063201500008 was reduced to 1.8 x 10**(-2) (7.5 x 10**(-3)) mbar A063201500009 and 1.8 x 10**(-5) (5 x 10**(-6)) mbar in the region A063201500010 of the first and fourth pumping stage, respectively. A063201500011 Disk-shaped target chamber (20 cm diameter, A063201500012 3 cm height) was used. A063201500013 METHOD Inverse kinematics A063201500014 DETECTOR (SIBAR) Seven surface-barrier detectors were A063201500015 placed at 30. to 135. degr. A063201500016 STATUS (CURVE) Fig. 5 from Z.Phys.,A342(1992)471 A063201500017 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063201500018 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063201500019 Data from Subents 016-019 were added. A063201500020 ANG-ERR -> ANG-ERR-D; DATA-ERR -> ERR-DIG; A063201500021 ERR-T -> DATA-ERR. A063201500022 ENDBIB 20 0 A063201500023 COMMON 3 3 A063201500024 ANG-ERR-D ERR-DIG EN-RSL-HW A063201500025 ADEG PER-CENT KEV A063201500026 0.6 1. 1.0 A063201500027 ENDCOMMON 3 0 A063201500028 DATA 4 21 A063201500029 EN-CM ANG-CM DATA-CM DATA-ERR A063201500030 KEV ADEG ARB-UNITS PER-CENT A063201500031 1000. 48.4 3.63E+04 A063201500032 1000. 71.4 2.172E+04 A063201500033 1000. 111.7 2.24E+04 A063201500034 1000. 127.8 3.56E+04 4. A063201500035 1000. 141.7 3.48E+04 8. A063201500036 1000. 151.9 5.1E+04 8. A063201500037 1000. 160.4 6.3E+04 8. A063201500038 700. 44.7 1.319E+04 A063201500039 700. 66.0 8490. A063201500040 700. 106.3 8690. A063201500041 700. 122.4 1.063E+04 A063201500042 700. 135.9 1.42E+04 5. A063201500043 700. 146.5 1.66E+04 5. A063201500044 700. 155.8 1.81E+04 5. A063201500045 400. 40.7 6140. A063201500046 400. 62.0 4960. A063201500047 400. 82.2 4330. 2.3 A063201500048 400. 113.7 4410. 5. A063201500049 400. 129.3 5400. 7. A063201500050 400. 141.2 7200. 7. A063201500051 400. 151.6 6900. 6. A063201500052 ENDDATA 23 0 A063201500053 ENDSUBENT 52 0 A063201599999 NOSUBENT A0632016 20210317 A098A063201600001 NOSUBENT A0632017 20210317 A098A063201700001 SUBENT A0632018 20210317 A098A063201800001 BIB 7 18 A063201800002 REACTION (3-LI-7(P,A)2-HE-4,,DA,,REL) A063201800003 The observed number of counts in each detector A063201800004 corrected for its solid angle. A063201800005 SAMPLE (3-LI-7,NAT=0.92) A 1.1 ug/cm 2 thick LiF target on a A063201800006 Ta backing (Li of natural isotopic composition: A063201800007 6Li= 8%, 7Li= 92%) A063201800008 Cyclindrical target chamber (close geometry) A063201800009 DETECTOR (SI) Six Si detectors (300 to 600 mm2 active area) wereA063201800010 mounted at 60. to 160. degr. and covered with 1.25 um A063201800011 thick Ni foils to stop the elastically scattered A063201800012 particles. A063201800013 METHOD Normal kinematics. A063201800014 STATUS (CURVE) Fig. 5 from Z.Phys.,A342(1992)471 A063201800015 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063201800016 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063201800017 Data from Subent 019 were added. A063201800018 ANG-ERR -> ANG-ERR-D; DATA-ERR -> ERR-DIG; A063201800019 ERR-T -> DATA-ERR. A063201800020 ENDBIB 18 0 A063201800021 COMMON 3 3 A063201800022 ANG-ERR-D ERR-DIG EN-RSL-HW A063201800023 ADEG PER-CENT KEV A063201800024 0.6 1. 0.3 A063201800025 ENDCOMMON 3 0 A063201800026 DATA 4 13 A063201800027 EN-CM ANG-CM DATA-CM DATA-ERR A063201800028 KEV ADEG ARB-UNITS PER-CENT A063201800029 100. 37.0 2120. 5. A063201800030 100. 53.0 2290. 5. A063201800031 100. 86.2 2350. 7. A063201800032 100. 102.5 2090. 9. A063201800033 100. 116.4 2460. 9. A063201800034 100. 130.6 1960. 10. A063201800035 100. 143.3 2520. 9. A063201800036 26. 60.7 1250. 4. A063201800037 26. 76.3 1430. 2.8 A063201800038 26. 106.6 1440. 8. A063201800039 26. 120.9 1410. 5. A063201800040 26. 140.5 1120. 8. A063201800041 26. 160.7 1210. 6. A063201800042 ENDDATA 15 0 A063201800043 ENDSUBENT 42 0 A063201899999 NOSUBENT A0632019 20210317 A098A063201900001 SUBENT A0632020 20210317 A098A063202000001 BIB 5 9 A063202000002 REACTION (3-LI-6(P,HE3)2-HE-4,,DA,,LEG/RS) A063202000003 COMMENT In the case of 6Li(p,alpha)3He, the data are A063202000004 dominated by an A1 coefficient, with a small A2 A063202000005 coefficient of the analytic form A063202000006 A2(E) =-0.029 -2.6 x 10**(-4) x E, with E in keV. A063202000007 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063202000008 STATUS (CURVE) Fig. 6a from Z.Phys.,A342(1992)471 A063202000009 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063202000010 EN-ERR -> EN-ERR-DIG; ERR-T -> DATA-ERR. A063202000011 ENDBIB 9 0 A063202000012 COMMON 2 3 A063202000013 EN-ERR-DIG NUMBER-CM A063202000014 PER-CENT NO-DIM A063202000015 1.6 1. A063202000016 ENDCOMMON 3 0 A063202000017 DATA 3 35 A063202000018 EN-CM DATA-CM DATA-ERR A063202000019 KEV NO-DIM NO-DIM A063202000020 2.57E+01 -0.131 0.028 A063202000021 3.20E+01 -0.145 0.015 A063202000022 3.44E+01 -0.090 0.006 A063202000023 3.69E+01 -0.074 0.006 A063202000024 4.12E+01 -0.042 0.006 A063202000025 4.27E+01 -0.073 0.006 A063202000026 4.71E+01 -0.049 0.006 A063202000027 5.06E+01 -0.037 0.020 A063202000028 5.64E+01 -0.005 0.007 A063202000029 6.00E+01 -0.024 0.006 A063202000030 6.29E+01 -0.004 0.006 A063202000031 6.86E+01 -0.023 0.006 A063202000032 7.74E+01 0.009 0.006 A063202000033 8.73E+01 0.053 0.006 A063202000034 8.74E+01 0.021 0.006 A063202000035 9.50E+01 0.049 0.006 A063202000036 1.01E+02 0.026 0.006 A063202000037 1.06E+02 0.066 0.006 A063202000038 1.14E+02 0.093 0.013 A063202000039 1.23E+02 0.106 0.007 A063202000040 1.29E+02 0.102 0.007 A063202000041 1.38E+02 0.142 0.008 A063202000042 1.47E+02 0.173 0.006 A063202000043 1.52E+02 0.134 0.006 A063202000044 1.60E+02 0.170 0.006 A063202000045 1.78E+02 0.182 0.007 A063202000046 2.03E+02 0.226 0.006 A063202000047 2.04E+02 0.191 0.007 A063202000048 2.56E+02 0.263 0.008 A063202000049 2.99E+02 0.322 0.008 A063202000050 3.50E+02 0.378 0.006 A063202000051 4.04E+02 0.414 0.006 A063202000052 4.09E+02 0.395 0.006 A063202000053 4.50E+02 0.438 0.006 A063202000054 5.08E+02 0.494 0.013 A063202000055 ENDDATA 37 0 A063202000056 ENDSUBENT 55 0 A063202099999 SUBENT A0632021 20210317 A098A063202100001 BIB 5 12 A063202100002 REACTION (3-LI-6(D,A)2-HE-4,,DA,,LEG/RS) A063202100003 COMMENT Due to the identical boson character of the ejectiles A063202100004 in 6Li(d,alpha) 4He and 7Li(p,alpha) 4He, the A063202100005 distributions are symmetrical about angle=90 degr. A063202100006 and thus can be described by even Legendre A063202100007 polynomials. Fits to the distributions of both A063202100008 reactions have shown that the data can be described A063202100009 sufficiently with an A2 coefficient (A4=~0) . A063202100010 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063202100011 STATUS (CURVE) Fig. 6b from Z.Phys.,A342(1992)471 A063202100012 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063202100013 EN-ERR -> EN-ERR-DIG; ERR-T -> DATA-ERR. A063202100014 ENDBIB 12 0 A063202100015 COMMON 2 3 A063202100016 EN-ERR-DIG NUMBER-CM A063202100017 PER-CENT NO-DIM A063202100018 1.6 2. A063202100019 ENDCOMMON 3 0 A063202100020 DATA 3 37 A063202100021 EN-CM DATA-CM DATA-ERR A063202100022 KEV NO-DIM NO-DIM A063202100023 3.71E+01 0.020 0.060 A063202100024 4.31E+01 -0.060 0.050 A063202100025 5.25E+01 -0.080 0.040 A063202100026 6.13E+01 -0.020 0.040 A063202100027 7.37E+01 -0.065 0.030 A063202100028 7.44E+01 -0.009 0.030 A063202100029 8.22E+01 -0.050 0.030 A063202100030 8.30E+01 0.003 0.027 A063202100031 9.06E+01 -0.040 0.030 A063202100032 1.02E+02 -0.040 0.023 A063202100033 1.02E+02 -0.058 0.030 A063202100034 1.03E+02 -0.011 0.020 A063202100035 1.05E+02 0.020 0.030 A063202100036 1.51E+02 0.010 0.040 A063202100037 2.05E+02 -0.020 0.040 A063202100038 2.51E+02 0.050 0.040 A063202100039 3.01E+02 0.030 0.040 A063202100040 3.56E+02 0.090 0.040 A063202100041 4.09E+02 0.030 0.040 A063202100042 4.55E+02 0.083 0.028 A063202100043 5.01E+02 0.090 0.030 A063202100044 5.51E+02 0.130 0.030 A063202100045 5.99E+02 0.170 0.040 A063202100046 6.53E+02 0.160 0.040 A063202100047 7.09E+02 0.200 0.030 A063202100048 7.52E+02 0.240 0.030 A063202100049 7.97E+02 0.300 0.030 A063202100050 8.37E+02 0.300 0.030 A063202100051 9.12E+02 0.290 0.030 A063202100052 9.52E+02 0.390 0.040 A063202100053 1.01E+03 0.385 0.014 A063202100054 1.05E+03 0.360 0.030 A063202100055 1.13E+03 0.380 0.040 A063202100056 1.14E+03 0.410 0.030 A063202100057 1.23E+03 0.430 0.030 A063202100058 1.30E+03 0.430 0.040 A063202100059 1.43E+03 0.470 0.040 A063202100060 ENDDATA 39 0 A063202100061 ENDSUBENT 60 0 A063202199999 SUBENT A0632022 20210317 A098A063202200001 BIB 5 12 A063202200002 REACTION (3-LI-7(P,A)2-HE-4,,DA,,LEG/RS) A063202200003 COMMENT Due to the identical boson character of the ejectiles A063202200004 in 6Li(d,alpha) 4He and 7Li(p,alpha) 4He, the A063202200005 distributions are symmetrical about angle=90 degr. A063202200006 and thus can be described by even Legendre A063202200007 polynomials. Fits to the distributions of both A063202200008 reactions have shown that the data can be described A063202200009 sufficiently with an A2 coefficient (A4=~0) . A063202200010 ERR-ANALYS (DATA-ERR) No information about source of uncertainty A063202200011 STATUS (CURVE) Fig. 6c from Z.Phys.,A342(1992)471 A063202200012 HISTORY (20210317A) SD: SF9=EXP deleted from REACTION code. A063202200013 EN-ERR -> EN-ERR-DIG; ERR-T -> DATA-ERR. A063202200014 ENDBIB 12 0 A063202200015 COMMON 2 3 A063202200016 EN-ERR-DIG NUMBER-CM A063202200017 PER-CENT NO-DIM A063202200018 1.6 2. A063202200019 ENDCOMMON 3 0 A063202200020 DATA 3 34 A063202200021 EN-CM DATA-CM DATA-ERR A063202200022 KEV NO-DIM NO-DIM A063202200023 2.64E+01 -0.150 0.040 A063202200024 3.56E+01 -0.020 0.040 A063202200025 4.07E+01 -0.030 0.060 A063202200026 4.29E+01 -0.090 0.040 A063202200027 4.57E+01 -0.170 0.060 A063202200028 5.21E+01 -0.090 0.060 A063202200029 5.38E+01 0.010 0.030 A063202200030 5.65E+01 0.020 0.050 A063202200031 5.74E+01 -0.080 0.060 A063202200032 6.23E+01 0.012 0.026 A063202200033 6.97E+01 -0.050 0.040 A063202200034 7.95E+01 0.017 0.028 A063202200035 8.96E+01 0.060 0.030 A063202200036 9.09E+01 -0.010 0.040 A063202200037 9.76E+01 0.073 0.026 A063202200038 1.03E+02 -0.040 0.080 A063202200039 1.06E+02 0.068 0.026 A063202200040 1.16E+02 0.068 0.028 A063202200041 1.24E+02 0.105 0.015 A063202200042 1.32E+02 0.096 0.021 A063202200043 1.42E+02 0.110 0.028 A063202200044 1.51E+02 0.161 0.021 A063202200045 1.58E+02 0.142 0.024 A063202200046 1.68E+02 0.156 0.026 A063202200047 2.04E+02 0.170 0.060 A063202200048 3.04E+02 0.350 0.060 A063202200049 4.10E+02 0.470 0.060 A063202200050 5.07E+02 0.660 0.060 A063202200051 6.00E+02 0.730 0.060 A063202200052 6.94E+02 0.760 0.050 A063202200053 8.03E+02 0.770 0.060 A063202200054 9.01E+02 0.960 0.050 A063202200055 9.03E+02 0.880 0.050 A063202200056 9.96E+02 0.870 0.060 A063202200057 ENDDATA 36 0 A063202200058 ENDSUBENT 57 0 A063202299999 SUBENT A0632023 20210317 A098A063202300001 BIB 7 17 A063202300002 REACTION ((1-H-1(3-LI-6,HE3)2-HE-4,,SIG,,SFC)= A063202300003 (3-LI-6(P,HE3)2-HE-4,,SIG,,SFC)) A063202300004 SAMPLE rectangular target chamber (close geometry) A063202300005 METHOD Inverse kinematics. A063202300006 DETECTOR (SI) A pair of Si detectors (450 mm2 active area) was A063202300007 placed at opposite sides to the beam axis, and with A063202300008 each detector at a distance of 9 mm from the beam axis.A063202300009 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063202300010 number of counts, and effective energy. A063202300011 (ERR-2) All values have an additional common error A063202300012 of 5% due to A063202300013 * uncertainties in proton beam (2.5%) A063202300014 * uncertainties in pressure (1.7%), and A063202300015 * uncertainty in target thickness and solid A063202300016 angle 3.6% A063202300017 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063202300018 HISTORY (20210317T) SD: Part of Subent 002. A063202300019 ENDBIB 17 0 A063202300020 COMMON 2 3 A063202300021 ERR-2 EN-RSL-HW A063202300022 PER-CENT KEV A063202300023 5.0 0.3 A063202300024 ENDCOMMON 3 0 A063202300025 DATA 3 17 A063202300026 EN-CM DATA ERR-1 A063202300027 KEV B*MEV B*MEV A063202300028 10.94 5.13 0.21 A063202300029 11.94 4.53 0.19 A063202300030 12.98 4.92 0.16 A063202300031 13.94 4.41 0.18 A063202300032 14.93 4.57 0.15 A063202300033 15.93 4.25 0.18 A063202300034 16.99 4.20 0.14 A063202300035 17.99 4.32 0.12 A063202300036 19.00 4.20 0.13 A063202300037 19.99 4.17 0.12 A063202300038 25.00 4.13 0.10 A063202300039 30.02 3.95 0.10 A063202300040 35.00 3.81 0.10 A063202300041 39.99 3.77 0.09 A063202300042 45.02 3.71 0.09 A063202300043 50.05 3.73 0.09 A063202300044 51.90 3.67 0.10 A063202300045 ENDDATA 19 0 A063202300046 ENDSUBENT 45 0 A063202399999 SUBENT A0632024 20210317 A098A063202400001 BIB 8 17 A063202400002 REACTION (3-LI-6(P,HE3)2-HE-4,,SIG,,SFC) A063202400003 SAMPLE (3-LI-6,ENR=0.95) A 1.1 ug/cm2 thick LiF target on a A063202400004 Ta backing A063202400005 Cyclindrical target chamber (close geometry) A063202400006 DETECTOR (SI) Six Si detectors (300 to 600 mm2 active area) wereA063202400007 mounted at 60. to 160. degr. and covered with 1.25 um A063202400008 thick Ni foils to stop the elastically scattered A063202400009 particles. A063202400010 METHOD Normal kinematics. A063202400011 REL-REF (R,C0417001,C.Rolfs+,J,NP/A,455,179,1986) A063202400012 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063202400013 number of counts, effective energy, angular A063202400014 distributions, and target stoichometry. A063202400015 (ERR-2) All values have an additional common error A063202400016 due to the uncertainty in normalization (see REL-REF). A063202400017 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063202400018 HISTORY (20210317T) SD: Part of Subent 002. A063202400019 ENDBIB 17 0 A063202400020 COMMON 2 3 A063202400021 ERR-2 EN-RSL-HW A063202400022 PER-CENT KEV A063202400023 10.0 0.3 A063202400024 ENDCOMMON 3 0 A063202400025 DATA 3 24 A063202400026 EN-CM DATA ERR-1 A063202400027 KEV B*MEV B*MEV A063202400028 10.74 4.50 0.20 A063202400029 11.59 4.72 0.23 A063202400030 12.44 4.83 0.22 A063202400031 13.29 4.61 0.21 A063202400032 14.14 4.38 0.20 A063202400033 14.99 4.28 0.19 A063202400034 15.84 4.28 0.19 A063202400035 16.69 4.57 0.21 A063202400036 19.51 4.36 0.20 A063202400037 23.70 4.20 0.20 A063202400038 27.92 3.79 0.18 A063202400039 32.15 3.66 0.18 A063202400040 36.39 3.41 0.16 A063202400041 40.64 3.30 0.16 A063202400042 44.89 3.15 0.15 A063202400043 49.15 3.36 0.17 A063202400044 53.40 3.15 0.15 A063202400045 57.66 3.16 0.16 A063202400046 61.91 3.32 0.17 A063202400047 66.17 2.86 0.16 A063202400048 70.43 3.25 0.19 A063202400049 74.68 2.77 0.17 A063202400050 78.94 2.74 0.17 A063202400051 83.04 2.68 0.18 A063202400052 ENDDATA 26 0 A063202400053 ENDSUBENT 52 0 A063202499999 SUBENT A0632025 20210317 A098A063202500001 BIB 7 17 A063202500002 REACTION ((1-H-2(3-LI-6,A)2-HE-4,,SIG,,SFC)= A063202500003 (3-LI-6(D,A)2-HE-4,,SIG,,SFC)) A063202500004 SAMPLE rectangular target chamber (close geometry) A063202500005 METHOD Inverse kinematics. A063202500006 DETECTOR (SI) A pair of Si detectors (450 mm2 active area) was A063202500007 placed at opposite sides to the beam axis, and with A063202500008 each detector at a distance of 9 mm from the beam axis.A063202500009 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063202500010 number of counts, and effective energy. A063202500011 (ERR-2) All values have an additional common error A063202500012 of 5% due to A063202500013 * uncertainties in proton beam (2.5%) A063202500014 * uncertainties in pressure (1.7%), and A063202500015 * uncertainty in target thickness and solid A063202500016 angle 3.6% A063202500017 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063202500018 HISTORY (20210317T) SD: Part of Subent 003. A063202500019 ENDBIB 17 0 A063202500020 COMMON 2 3 A063202500021 ERR-2 EN-RSL-HW A063202500022 PER-CENT KEV A063202500023 5.0 0.3 A063202500024 ENDCOMMON 3 0 A063202500025 DATA 3 18 A063202500026 EN-CM DATA ERR-1 A063202500027 KEV B*MEV B*MEV A063202500028 15.89 25.4 2.7 A063202500029 16.90 21.8 2.1 A063202500030 17.89 23.8 2.1 A063202500031 19.88 22.3 1.2 A063202500032 24.91 21.8 0.8 A063202500033 29.89 21.6 0.6 A063202500034 34.93 20.0 0.7 A063202500035 39.93 19.9 0.7 A063202500036 44.89 19.6 0.7 A063202500037 49.89 18.9 0.5 A063202500038 54.88 18.5 0.5 A063202500039 59.90 18.1 0.5 A063202500040 64.90 17.7 0.5 A063202500041 69.90 17.5 0.4 A063202500042 74.97 17.1 0.4 A063202500043 79.91 16.5 0.4 A063202500044 84.99 16.2 0.4 A063202500045 89.97 15.7 0.4 A063202500046 ENDDATA 20 0 A063202500047 ENDSUBENT 46 0 A063202599999 SUBENT A0632026 20210317 A098A063202600001 BIB 8 17 A063202600002 REACTION (3-LI-6(D,A)2-HE-4,,SIG,,SFC) A063202600003 SAMPLE (3-LI-6,ENR=0.95) A 1.1 ug/cm2 thick LiF target on a A063202600004 Ta backing A063202600005 Cyclindrical target chamber (close geometry) A063202600006 DETECTOR (SI) Six Si detectors (300 to 600 mm2 active area) wereA063202600007 mounted at 60. to 160. degr. and covered with 1.25 um A063202600008 thick Ni foils to stop the elastically scattered A063202600009 particles. A063202600010 METHOD Normal kinematics. A063202600011 REL-REF (R,C0417001,C.Rolfs+,J,NP/A,455,179,1986) A063202600012 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063202600013 number of counts, effective energy, angular A063202600014 distributions, and target stoichometry. A063202600015 (ERR-2) All values have an additional common error A063202600016 due to the uncertainty in normalization (see REL-REF). A063202600017 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063202600018 HISTORY (20210317T) SD: Part of Subent 003. A063202600019 ENDBIB 17 0 A063202600020 COMMON 2 3 A063202600021 ERR-2 EN-RSL-HW A063202600022 PER-CENT KEV A063202600023 10.0 0.3 A063202600024 ENDCOMMON 3 0 A063202600025 DATA 3 21 A063202600026 EN-CM DATA ERR-1 A063202600027 KEV B*MEV B*MEV A063202600028 14.31 24.0 1.7 A063202600029 16.01 24.5 1.7 A063202600030 17.20 24.7 1.7 A063202600031 17.86 24.6 1.6 A063202600032 19.71 22.4 1.1 A063202600033 20.83 21.8 1.1 A063202600034 21.56 20.6 1.0 A063202600035 24.50 20.6 1.0 A063202600036 28.19 19.9 1.0 A063202600037 31.90 19.6 0.9 A063202600038 35.61 18.8 0.9 A063202600039 39.32 18.8 0.9 A063202600040 43.04 17.4 0.9 A063202600041 46.76 16.8 0.8 A063202600042 50.48 17.7 0.9 A063202600043 54.20 16.2 0.9 A063202600044 57.92 16.0 0.9 A063202600045 61.64 15.8 0.9 A063202600046 65.37 15.2 0.9 A063202600047 69.09 15.9 1.0 A063202600048 72.81 14.7 1.0 A063202600049 ENDDATA 23 0 A063202600050 ENDSUBENT 49 0 A063202699999 SUBENT A0632027 20210317 A098A063202700001 BIB 7 17 A063202700002 REACTION ((1-H-1(3-LI-7,A)2-HE-4,,SIG,,SFC)= A063202700003 (3-LI-7(P,A)2-HE-4,,SIG,,SFC)) A063202700004 SAMPLE Rectangular target chamber (close geometry) A063202700005 METHOD Inverse kinematics. A063202700006 DETECTOR (SI) A pair of Si detectors (450 mm2 active area) was A063202700007 placed at opposite sides to the beam axis, and with A063202700008 each detector at a distance of 9 mm from the beam axis.A063202700009 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063202700010 number of counts, and effective energy. A063202700011 (ERR-2) All values have an additional common error A063202700012 of 5% due to A063202700013 * uncertainties in proton beam (2.5%) A063202700014 * uncertainties in pressure (1.7%), and A063202700015 * uncertainty in target thickness and solid A063202700016 angle 3.6% A063202700017 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063202700018 HISTORY (20210317T) SD: Part of Subent 004. A063202700019 ENDBIB 17 0 A063202700020 COMMON 1 3 A063202700021 ERR-2 A063202700022 PER-CENT A063202700023 5.0 A063202700024 ENDCOMMON 3 0 A063202700025 DATA 3 17 A063202700026 EN-CM DATA ERR-1 A063202700027 KEV MB*MEV MB*MEV A063202700028 12.97 74. 5. A063202700029 13.97 75. 4. A063202700030 16.00 73. 3. A063202700031 16.98 72. 6. A063202700032 18.49 76. 4. A063202700033 19.97 73. 2. A063202700034 22.52 75. 3. A063202700035 24.98 73. 2. A063202700036 27.53 74. 2. A063202700037 30.03 72. 2. A063202700038 32.55 73. 2. A063202700039 35.02 72. 2. A063202700040 38.20 72. 2. A063202700041 40.04 73. 2. A063202700042 41.34 73. 2. A063202700043 43.81 70. 2. A063202700044 45.08 74. 2. A063202700045 ENDDATA 19 0 A063202700046 ENDSUBENT 45 0 A063202799999 SUBENT A0632028 20210317 A098A063202800001 BIB 9 19 A063202800002 REACTION (3-LI-7(P,A)2-HE-4,,SIG,,SFC) A063202800003 METHOD Normal kinematics. A063202800004 SAMPLE (3-LI-7,NAT=0.92) A 1.1 ug/cm 2 thick LiF target on a A063202800005 Ta backing (Li of natural isotopic composition: A063202800006 6Li= 8%, 7Li= 92%) A063202800007 Cyclindrical target chamber (close geometry) A063202800008 DETECTOR (SI) Six Si detectors (300 to 600 mm2 active area) wereA063202800009 mounted at 60. to 160. degr. and covered with 1.25 um A063202800010 thick Ni foils to stop the elastically scattered A063202800011 particles. A063202800012 MONITOR (3-LI-7(P,A)2-HE-4,,SIG,,SFC) A063202800013 MONIT-REF (C0417001,C.Rolfs+,J,NP/A,455,179,1986) A063202800014 ERR-ANALYS (ERR-1) Errors quoted arise from uncertainties in A063202800015 number of counts, effective energy, angular A063202800016 distributions, and target stoich!ometry. A063202800017 (ERR-2) All values have an additional common error of A063202800018 10% due to the uncertainty in normalisation. A063202800019 STATUS (TABLE) Table 1 from Z.Phys.,A342(1992)471 A063202800020 HISTORY (20210317T) SD: Part of Subent 004. A063202800021 ENDBIB 19 0 A063202800022 COMMON 2 3 A063202800023 ERR-2 EN-RSL-HW A063202800024 PER-CENT KEV A063202800025 10.0 0.020 A063202800026 ENDCOMMON 3 0 A063202800027 DATA 3 22 A063202800028 EN-CM DATA ERR-1 A063202800029 KEV MB*MEV MB*MEV A063202800030 12.70 90. 7. A063202800031 13.57 77. 5. A063202800032 14.43 72. 4. A063202800033 15.30 70. 4. A063202800034 16.17 75. 4. A063202800035 17.04 78. 4. A063202800036 19.92 72. 4. A063202800037 24.19 71. 3. A063202800038 28.50 72. 3. A063202800039 32.81 70. 3. A063202800040 37.15 70. 3. A063202800041 41.48 71. 4. A063202800042 45.83 69. 3. A063202800043 50.17 70. 3. A063202800044 54.51 70. 3. A063202800045 58.86 69. 3. A063202800046 63.20 70. 4. A063202800047 67.55 75. 4. A063202800048 71.89 75. 4. A063202800049 76.24 74. 4. A063202800050 80.58 53. 5. A063202800051 84.93 69. 5. A063202800052 ENDDATA 24 0 A063202800053 ENDSUBENT 52 0 A063202899999 ENDENTRY 28 0 A063299999999