ENTRY C0006 20230116 C227C0006000 1 SUBENT C0006001 20230116 C227C0006001 1 BIB 9 19 C0006001 2 TITLE Low Energy Cross Section of the D-T Reaction and C0006001 3 Angular Distribution of the Alpha-Particles Emitted C0006001 4 AUTHOR (E.Bretscher,A.P.French) C0006001 5 REFERENCE (J,PR,75,1154,1949) C0006001 6 #doi:10.1103/PhysRev.75.1154 C0006001 7 INSTITUTE (1USALAS) C0006001 8 FACILITY (ACCEL,1USALAS) C0006001 9 SAMPLE Deuterium ice target. Thickness not given. C0006001 10 METHOD (BCINT) C0006001 11 DETECTOR (PROPC) C0006001 12 HISTORY (19780522C) TWB C0006001 13 (19800303A) TWB C0006001 14 (19880304A) reaction sequence corrected. C0006001 15 (19960222A) Status added, converted to lower case. C0006001 16 (19970127A) BIB update. Reactions corrected. C0006001 17 (20020213A) Converted to new date formats. C0006001 18 (20030626A) BIB update. C0006001 19 (20230116A) BP: Updated entry, ERR-ANALYS and STATUS, C0006001 20 added doi and FACILITY. C0006001 21 ENDBIB 19 0 C0006001 22 NOCOMMON 0 0 C0006001 23 ENDSUBENT 22 0 C000600199999 SUBENT C0006002 20230116 C227C0006002 1 BIB 4 19 C0006002 2 REACTION (1-H-2(T,N)2-HE-4,,DA,A,TT/RSD) C0006002 3 ERR-ANALYS (DATA-ERR,3.5,10.) The counting errors at the lowest C0006002 4 energies are about three percent, and at the higher C0006002 5 energies are negligible, The geometry of the counter C0006002 6 used at low energies is known within about nine C0006002 7 percent; for the other counter it is better known to C0006002 8 about two percent. The current measurements with the C0006002 9 integrator are probably good to two percent. The C0006002 10 error due to the presence of neutral particles in the C0006002 11 beam is, in general, not more than one percent; any C0006002 12 errors due to target contamination or secondary C0006002 13 electron emission were together not more than one C0006002 14 percent. The bombarding voltage is known within one C0006002 15 percent. The combination of these factors leads to an C0006002 16 aggregate error in the thick-target yield amounting C0006002 17 to 3.5% at high energies and about 10% at low energies.C0006002 18 STATUS (CURVE) Fig. 2, page 1157 of J,PR,75,1154,1949. C0006002 19 HISTORY (20030626A) Units corrected. C0006002 20 (20230116A) BP: Added ERR-ANALYS. C0006002 21 ENDBIB 19 0 C0006002 22 COMMON 1 3 C0006002 23 EN C0006002 24 KEV C0006002 25 75. C0006002 26 ENDCOMMON 3 0 C0006002 27 DATA 2 12 C0006002 28 ANG DATA C0006002 29 ADEG NO-DIM C0006002 30 40. 1.2 C0006002 31 45. 1.15 C0006002 32 50. 1.17 C0006002 33 60. 1.15 C0006002 34 70. 1.15 C0006002 35 80. 1.05 C0006002 36 90. 1.000 C0006002 37 100. 0.90 C0006002 38 110. 0.85 C0006002 39 120. 0.80 C0006002 40 130. 0.80 C0006002 41 140. 0.80 C0006002 42 ENDDATA 14 0 C0006002 43 ENDSUBENT 42 0 C000600299999 SUBENT C0006003 20230116 C227C0006003 1 BIB 6 25 C0006003 2 REACTION (1-H-2(T,N)2-HE-4,,PY,,TT/CH) C0006003 3 DETECTOR Measured with 2 different detector geometries (below C0006003 4 and above 40 keV). C0006003 5 ANALYSIS (4PI1A) Measured at 90 degrees. C0006003 6 ERR-ANALYS (DATA-ERR) The counting errors at the lowest C0006003 7 energies are about three percent, and at the higher C0006003 8 energies are negligible, The geometry of the counter C0006003 9 used at low energies is known within about nine C0006003 10 percent; for the other counter it is better known to C0006003 11 about two percent. The current measurements with the C0006003 12 integrator are probably good to two percent. The C0006003 13 error due to the presence of neutral particles in the C0006003 14 beam is, in general, not more than one percent; any C0006003 15 errors due to target contamination or secondary C0006003 16 electron emission were together not more than one C0006003 17 percent. The bombarding voltage is known within one C0006003 18 percent. The combination of these factors leads to an C0006003 19 aggregate error in the thick-target yield amounting C0006003 20 to 3.5% at high energies and about 10% at low energies.C0006003 21 STATUS (TABLE) Table II, page 1158 of J,PR,75,1154,1949. C0006003 22 HISTORY (19970124A) Data corrected C0006003 23 (20020213A) data heading updated. C0006003 24 (20030626A) Data replaced with data in author's units. C0006003 25 Data error corrected. C0006003 26 (20230116A) BP: Updated Reaction string and ERR-ANALYS.C0006003 27 ENDBIB 25 0 C0006003 28 NOCOMMON 0 0 C0006003 29 DATA 3 26 C0006003 30 EN DATA DATA-ERR C0006003 31 KEV PRD/MUCOUL PER-CENT C0006003 32 15.0 2.90E-03 10. C0006003 33 18.1 9.61E-03 10. C0006003 34 21.1 3.34E-04 10. C0006003 35 24.1 5.42E-04 10. C0006003 36 27.2 1.45E-05 10. C0006003 37 30.2 2.22E-05 10. C0006003 38 36.4 4.92E-05 10. C0006003 39 38.8 6.92E-05 10. C0006003 40 43.7 1.28E-06 3.5 C0006003 41 47.5 1.97E-06 3.5 C0006003 42 50.9 2.47E-06 3.5 C0006003 43 54. 3.64E-06 3.5 C0006003 44 58.2 4.20E-06 3.5 C0006003 45 64.3 6.41E-06 3.5 C0006003 46 69.1 7.56E-06 3.5 C0006003 47 72.3 1.02E-07 3.5 C0006003 48 75.3 1.16E-07 3.5 C0006003 49 79.2 1.49E-07 3.5 C0006003 50 80.8 1.65E-07 3.5 C0006003 51 84.4 1.76E-07 3.5 C0006003 52 87.1 1.95E-07 3.5 C0006003 53 95. 2.75E-07 3.5 C0006003 54 105.6 4.01E-07 3.5 C0006003 55 116. 5.87E-07 3.5 C0006003 56 118.8 5.77E-07 3.5 C0006003 57 126.7 7.20E-07 3.5 C0006003 58 ENDDATA 28 0 C0006003 59 ENDSUBENT 58 0 C000600399999 SUBENT C0006004 20230116 C227C0006004 1 BIB 5 8 C0006004 2 REACTION (1-H-2(T,N)2-HE-4,,SIG,,,DERIV) C0006004 3 REL-REF (R,A1143002,E.Bretscher+,J,PR,73,815,1948) C0006004 4 ANALYSIS (TTUNF) Calculated from fit to measured thick-target C0006004 5 yields using stopping powers taken from Bretscher C0006004 6 et al., Phys. Rev. 73, 815 (1948). C0006004 7 ERR-ANALYS No uncertainties given. C0006004 8 STATUS (DEP,C0006003) C0006004 9 (TABLE) Table III, page 1158 of J,PR,75,1154,1949. C0006004 10 ENDBIB 8 0 C0006004 11 NOCOMMON 0 0 C0006004 12 DATA 2 24 C0006004 13 EN DATA C0006004 14 KEV B C0006004 15 15. 0.00105 C0006004 16 17.5 0.00251 C0006004 17 20. 0.00510 C0006004 18 25. 0.0156 C0006004 19 30. 0.0363 C0006004 20 35. 0.0714 C0006004 21 40. 0.125 C0006004 22 45. 0.200 C0006004 23 50. 0.290 C0006004 24 55. 0.410 C0006004 25 60. 0.555 C0006004 26 65. 0.730 C0006004 27 70. 0.896 C0006004 28 75. 1.11 C0006004 29 80. 1.30 C0006004 30 85. 1.56 C0006004 31 90. 1.82 C0006004 32 95. 2.11 C0006004 33 100. 2.41 C0006004 34 105. 2.76 C0006004 35 110. 3.02 C0006004 36 115. 3.34 C0006004 37 120. 3.71 C0006004 38 125. 4.04 C0006004 39 ENDDATA 26 0 C0006004 40 ENDSUBENT 39 0 C000600499999 ENDENTRY 4 0 C000699999999