ENTRY D0019 20060725 D048D001900000001 SUBENT D0019001 20060725 D048D001900100001 BIB 7 10 D001900100002 TITLE -evaluation of T(t,2n) cross-section.- D001900100003 AUTHOR (G.M.Hale) D001900100004 INSTITUTE (1USALAS) D001900100005 REFERENCE (P,LA-7722-PR,1,197812) D001900100006 (P,LA-7596-PR,2,197809) D001900100007 (W,HALE,19790423) note and numerical data. D001900100008 METHOD R-matrix fitting using EDA code. D001900100009 ERR-ANALYS no errors given. D001900100010 HISTORY (19790508C) KO. D001900100011 (20060725A) BIB section upgrated D001900100012 ENDBIB 10 0 D001900100013 NOCOMMON 0 0 D001900100014 ENDSUBENT 13 0 D001900199999 SUBENT D0019002 20060725 D048D001900200001 BIB 4 13 D001900200002 REACTION (1-H-3(T,2N)2-HE-4,,SIG,,,EVAL) D001900200003 REL-REF (E,A1089001,H.M.AGNEW+,J,PR,84,862,1951) D001900200004 (E,D0015001,N.JARMIE+,J,PR,111,1121,1958) D001900200005 (E,A0027001,A.M.GOVOROV+,J,JET,15,(2),266,1962) D001900200006 (E,A0007001,V.I.SEROV+,J,AE,42,(1),59,197701) D001900200007 COMMENT === the author's note to NDS = D001900200008 the experimental data of T(t,2n)He-3 are rather sparseD001900200009 and not in particularly good agreement, so that his D001900200010 extrapolations of the cross section below 30 keV to D001900200011 10 eV and above 2 to 5 MeV must be used with great D001900200012 caution. the author will write up a more detailed D001900200013 description for publication soon. 79/04/23. === D001900200014 STATUS (TABLE) data from G.M.Hale, as priv.comm.,79/04/23. D001900200015 ENDBIB 13 0 D001900200016 NOCOMMON 0 0 D001900200017 DATA 2 54 D001900200018 EN DATA D001900200019 EV B D001900200020 2.0000E+03 3.7603E-15 D001900200021 4.0000E+03 1.4492E-10 D001900200022 6.0000E+03 1.4117E-08 D001900200023 8.0000E+03 2.0655E-07 D001900200024 1.0000E+04 1.2544E-06 D001900200025 1.2000E+04 4.6658E-06 D001900200026 1.4000E+04 1.2787E-05 D001900200027 1.6000E+04 2.8548E-05 D001900200028 1.8000E+04 5.5114E-05 D001900200029 2.0000E+04 9.5579E-05 D001900200030 4.0000E+04 1.6532E-03 D001900200031 6.0000E+04 5.2409E-03 D001900200032 8.0000E+04 9.8843E-03 D001900200033 1.0000E+05 1.4769E-02 D001900200034 1.2000E+05 1.9469E-02 D001900200035 1.4000E+05 2.3806E-02 D001900200036 1.6000E+05 2.7730E-02 D001900200037 1.8000E+05 3.1253E-02 D001900200038 2.0000E+05 3.4408E-02 D001900200039 2.2000E+05 3.7241E-02 D001900200040 2.4000E+05 3.9793E-02 D001900200041 2.6000E+05 4.2105E-02 D001900200042 2.8000E+05 4.4212E-02 D001900200043 3.0000E+05 4.6145E-02 D001900200044 3.5000E+05 5.0377E-02 D001900200045 4.0000E+05 5.3985E-02 D001900200046 4.5000E+05 5.7180E-02 D001900200047 5.0000E+05 6.0104E-02 D001900200048 5.5000E+05 6.2854E-02 D001900200049 6.0000E+05 6.5499E-02 D001900200050 7.0000E+05 7.0659E-02 D001900200051 8.0000E+05 7.5838E-02 D001900200052 9.0000E+05 8.1176E-02 D001900200053 1.0000E+06 8.6742E-02 D001900200054 1.1000E+06 9.2559E-02 D001900200055 1.2000E+06 9.8610E-02 D001900200056 1.3000E+06 1.0484E-01 D001900200057 1.4000E+06 1.1114E-01 D001900200058 1.5000E+06 1.1739E-01 D001900200059 1.6000E+06 1.2338E-01 D001900200060 1.7000E+06 1.2890E-01 D001900200061 1.8000E+06 1.3370E-01 D001900200062 1.9000E+06 1.3752E-01 D001900200063 2.0000E+06 1.4013E-01 D001900200064 2.1000E+06 1.4135E-01 D001900200065 2.2000E+06 1.4106E-01 D001900200066 2.3000E+06 1.3928E-01 D001900200067 2.4000E+06 1.3608E-01 D001900200068 2.5000E+06 1.3165E-01 D001900200069 3.0000E+06 9.9658E-02 D001900200070 3.5000E+06 6.8974E-02 D001900200071 4.0000E+06 4.7680E-02 D001900200072 4.5000E+06 3.4005E-02 D001900200073 5.0000E+06 2.5173E-02 D001900200074 ENDDATA 56 0 D001900200075 ENDSUBENT 74 0 D001900299999 ENDENTRY 2 0 D001999999999