ENSDF dataset for 8Be

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ENSDF dataset for 8Be

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8BE ADOPTED LEVELS, GAMMAS 2004TI06 04NP 200505 8BE H TYP=FUL$AUT=J.H. KELLEY, J.L. GODWIN, C.G. SHEU, ET AL.$ 8BE H TYP=FUL$AUT=J.H. KELLEY, J.L. GODWIN, C.G. SHEU, ET AL.$ 8BE2 H CIT=NP A745, 155 (2004)$CUT=31-Mar-2004$ 8BE Q -17979.8 1018899.681217255.44 9 91.84 4 2003AU02 8BE C SEE ALSO TABLE 8.10: ELECTROMAGNETIC TRANSITIONS IN 8BE (2004TI06) AND 8BE2C REACTION: 4HE(A,A). 8BE CG E FROM E(LEVEL) DIFFERENCE; RECOIL CORRECTION APPLIED 8BE CL E(A) GIANT RESONANCE: SEE REACTION 7LI(P,G) 8BE XA8LI B- DECAY 8BE XB8B B+ DECAY 8BE XC4HE(A,G) 8BE XD4HE(A,A) 8BE XE6LI(D,G) 8BE XF6LI(D,N), 6LI(D,P) 8BE XG6LI(D,A), 6LI(D,PA) 8BE XH6LI(T,N) 8BE XI6LI(3HE,P) 8BE XJ6LI(A,D), 6LI(A,2A) 8BE XK6LI(6LI,A) 8BE XL7LI(P,G) 8BE XM7LI(P,N) 8BE XN7LI(P,P), 7LI(P,P') 8BE XO7LI(P,A) 8BE XP7LI(D,N) 8BE XQ7LI(3HE,D), 7LI(3HE,DA) 8BE XR7LI(A,T) 8BE XS7LI(7LI,6HE) 8BE XT7BE(N,P) 8BE XU9BE(P,D), 9BE(P,NP) 8BE XV9BE(D,T) 8BE XW9BE(3HE,A) 8BE XX10BE(P,T) 8BE XY10B(P,3HE) 8BE XZ10B(D,A) 8BE Xa11B(3HE,6LI) 8BE Xb12C(D,6LI) 8BE Xc12C(3HE,7BE) 8BE Xd12C(A,2A), 12C(A,8BE) 8BE XeAG(14N,8BE) 8BE L 0.0 0+ 5.57 EV 25 8BE2 L ISPIN=0 $ %A=100 8BE3 L XREF=ABCDEHIJKLPQRSUVWYZabcde 8BE CL WIDTH FROM 4HE(A,A)(1992WA09). 8BE2CL PREVIOUS VALUE WIDTH=6.8 EV 17 (1968BE02). 8BE3CL OTHER VALUE WIDTH=5.5 EV 13 9BE(P,D). 8BE L 3030 102+ 1513 KEV 15 8BE2 L ISPIN=0 $ %A AP 100 8BE3 L XREF=ABCDEHIJKLPQRSUVWYZabcd 8BE CL E SEE 2004TI06 TABLE 8.11. 8BE G 3029 E2 8BE2 G WIDTHG=8.3E-3 EV 8BE L 11.35E+3 154+ 3.5 MEV AP 8BE2 L ISPIN=0 $ %A AP 100 8BE3 L XREF=CDJKPRUVWZbcd 8BE CL E VALUES IN THE LITERATURE ARE 8BE2CL 11.4 MEV 3 4HE(A,A) (1959BR71), 8BE3CL 11.7 MEV 4 4HE(A,A) (1974CH45), 8BE4CL 11.3 MEV 4 6LI(A,D) (1962CE01), 8BE5CL 11.3 MEV 2 7LI(D,N)(1995AR25), 8BE6CL 11.40 MEV 5 7LI(D,N) (1969HO11) AND 8BE7CL 11.3 MEV 3 9BE(P,D) (1969SU02), 8BE CL WIDTH VALUES FOUND IN THE LITERATURE ARE 8BE2CL 4.0 MEV 4 4HE(A,A) (1974CH45), 8BE3CL AP 4.3 MEV 4HE(A,A) (1967KE10), 8BE4CL 3.7 MEV 2 7LI(D,N)(1995AR25), 8BE5CL 2.8 MEV 2 7LI(D,N) (1969HO11). 8BE6CL 5.2 MEV 1 9BE(P,D) (1981BE53) 8BE7CL AP 2.6 MEV 9BE(3HE,A) (1966CA13,1967CA13) AND 8BE8CL AP 4 MEV 10B(D,A) (1966LO18,1968LO01). 8BE G 11350 E4 8BE2 G WIDTHG=0.46E-3 EV 8BE L 16626 3 2+ 108.1 KEV 5 8BE2 L ISPIN=0&1 $ %IT LT 2.65E-3 $ %A AP 100 8BE3 L XREF=BCDHIKLPQRUVWYZabc 8BE CL E FROM WEIGHTED AVERAGE OF 8BE2CL E=16627 KEV 5 7LI(3HE,D), 8BE3CL 16623 KEV 3 4HE(A,A) AND 8BE4CL 16630 KEV 3 4HE(A,A). 8BE CL WIDTH FROM WEIGHTED AVERAGE OF 8BE2CL WIDTH=113 KEV 3 7LI(3HE,D), 8BE3CL 90 KEV 5 10B(D,A), 8BE4CL 107.7 KEV 5 4HE(A,A) AND 8BE5CL 108.5 KEV 5 4HE(A,A). 8BE G 13580 M1 8BE2 G WIDTHG LT 2.80 EV 18$BM1W LT 5.3E-2 3 8BE G 16607 E2 8BE2 G WIDTHG=7.0E-2 EV 25$BE2W=7.1E-2 25 8BE L 16922 3 2+ 74.0 KEV 4 8BE2 L ISPIN=0&1 $ %IT LT 3.89E-3 $ %A AP 100 8BE3 L XREF=CDHIKLPQRUVWYZabc 8BE CL E FROM WEIGHTED AVERAGE OF 8BE2CL E=16901 KEV 5 7LI(3HE,D), 8BE3CL 16925 KEV 3 4HE(A,A) AND 8BE4CL 16918 KEV 3 4HE(A,A). 8BE CL WIDTH FROM WEIGHTED AVERAGE OF 8BE2CL WIDTH=77 KEV 3 7LI(3HE,D), 8BE3CL 70 KEV 5 10B(D,A), 8BE4CL 74.4 KEV 4 4HE(A,A) AND 8BE5CL 73.6 KEV 4 4HE(A,A). 8BE G 13879 M1 8BE2 G WIDTHG LT 2.80 EV 18$BM1W LT 5.3E-2 3 8BE G 16903 E2 8BE2 G WIDTHG=8.4E-2 EV 14$BE2W=7.8E-2 13 8BE L 17640.0 101+ 10.7 KEV 5 8BE2 L ISPIN=1 $ %IT=0.204 $ %P=99.8 8BE3 L XREF=EILNPQUVWZac 8BE CL E FROM 7LI(P,G) 8BE CL WIDTH FROM 7LI(P,G) 8BE G 718 M1 8BE2 G WIDTHG=1.3E-3 EV 3$BM1W=0.17 4 8BE G 1014 M1+E2 -0.014 13 8BE2 G WIDTHG=3.2E-2 EV 3$BM1W=1.5 2 8BE G 14586 M1+E2 0.21 4 8BE2 G WIDTHG= 6.8 EV 13 $BM1W=0.10 2 $BE2W=0.23 10 8BE G 17619 M1 8BE2 G WIDTHG=15.0 EV 18 $ BM1W=0.13 2 8BE L 18150 4 1+ 138 KEV 6 8BE2 L ISPIN=0 $ %IT=4.6E-3 $ %P AP 100 8BE3 L XREF=ILNPQUVZa 8BE CL E FROM WEIGHTED AVERAGE OF 8BE2CL E=18155 KEV 5 7LI(P,P'' G), 8BE3CL 18150 KEV 5 10B(D,A) AND 8BE4CL 18144 KEV 5 9BE(D,T). 8BE CL WIDTH FROM 10B(D,A) 8BE G 1228 M1 8BE2 G WIDTHG=6.2E-2 EV 7$BM1W=1.6 2 8BE G 1524 M1 8BE2 G WIDTHG=7.7E-2 EV 19$BM1W=1.0 3 8BE G 15095 M1 8BE2 G WIDTHG=4.3 EV 12$BM1W=5.9E-2 17 8BE G 18128 M1 8BE2 G WIDTHG=1.9 EV 4 $BM1W=1.5E-2 3 8BE L 18910 2- 122 KEV 8BE2 L %IT=2.2E-4 $ %N=? $ %P=? 8BE3 L XREF=ILMNPT 8BE CL WIDTH FROM R-MATRIX FIT TO 7BE(N,P), (N,A) AND (N,AG) DATA. 8BE2CL OTHER VALUES ARE WIDTH=131 KEV 44 7LI(P,G), 8BE3CL 50 KEV 20 7LI(P,N) AND 8BE4CL 48 KEV 18 7LI(P,P). 8BE G 1988 E1 8BE2 G WIDTHG=9.9E-2 EV 43 $ BE1W=4.6E-2 20 8BE G 2284 E1 8BE2 G WIDTHG=0.17 EV 7 $ BE1W=5.3E-2 20 8BE L 19069 103+ 271 KEV 15 8BE2 L ISPIN=1 $ %IT=3.87E-3 $ %P AP 100 8BE3 L XREF=ILNPUV 8BE CL ISPIN TENTATIVE 8BE CL E FROM WEIGHTED AVERAGE OF 8BE2CL E=19060 KEV 20 7LI(P,G) AND 8BE3CL 19071 KEV 10 9BE(D,T). 8BE CL WIDTH FROM WEIGHTED AVERAGE OF 8BE2CL WIDTH=271 KEV 17 7LI(P,G) AND 8BE3CL 270 KEV 30 9BE(D,T). 8BE G 16013 M1 8BE2 G WIDTHG=10.5 EV$BM1W=0.122 8BE L 19235 103+ 227 KEV 16 8BE2 L ISPIN=0 $ %N AP 50 $ %P AP 50 8BE3 L XREF=MNPTUVWZe 8BE CL ISPIN TENTATIVE 8BE CL E FROM WEIGHTED AVERAGE OF 8BE2CL E=19220 KEV 30 9BE(3HE,A), 8BE3CL 19260 KEV 30 9BE(D,T) AND 8BE4CL 19234 KEV 12 ^Ag(14N,8BE). 8BE CL WIDTH FROM WEIGHTED AVERAGE OF 8BE2CL WIDTH=208 KEV 30 9BE(P,D), 8BE3CL 265 KEV 30 9BE(3HE,A), 8BE4CL 220 KEV 30 9BE(D,T) AND 8BE5CL 210 KEV 35 ^Ag(14N,8BE). 8BE CL BRANCHING RATIO FROM 7LI(P,N) 8BE L 19400 1- 645 KEV AP 8BE2 L %N=? $ %P=? 8BE3 L XREF=IMNU 8BE CL WIDTH FROM 7LI(P,P),(P,P'). 8BE L 19860 504+ 0.7 MEV 1 8BE2 L ISPIN=0 $ %P=30 $ %A=70 8BE3 L XREF=DIKORSVWZ 8BE CL WIDTHA/WIDTHP=2.3 5 10B(D,2A), 10B(D,P+7LI)(1992PU06). OTHER 8BE2CL MEASUREMENT WIDTHA/WIDTH=0.96 FROM 4HE(A,A). 8BE CL E FROM 9BE(D,T). 8BE CL WIDTH FROM 9BE(D,T). 8BE L 20100 2+ 880 KEV 20 8BE2 L ISPIN=0 $ %N=? $ %P=? $ %A=? 8BE3 L XREF=DMNOPSVZ 8BE CL WIDTHA/WIDTHP=4.5 6 10B(D,A),10B(D,P)(1992PU06). 8BE CL WIDTH FROM 7LI(D,N) 8BE L 20200 0+ 720 KEV 20 8BE2 L ISPIN=0 $ %A AP 50 $ %N=? 8BE3 L XREF=DMPZ 8BE CL WIDTH FROM 7LI(D,N). 8BE CL WIDTHA/WIDTH AP 0.50 4HE(A,A) 8BE L 20.9E+3 4- 1.6 MEV 2 8BE2 L %P=? 8BE3 L XREF=N 8BE CL WIDTH FROM 7LI(P,P). 8BE L 21.5E+3 3(+) 1.1 MEV 8BE2 L %IT=? $ %N=? $ %P=? 8BE3 L XREF=LMTZ 8BE CL WIDTH FROM 7LI(P,N). 8BE L 22000 1- 4 MEV AP A 8BE2 L %IT=? $ %P=? $ ISPIN=1 8BE3 L XREF=L 8BE CL WIDTH FROM 7LI(P,G). 8BE L 22.05E+3 10 270 KEV 70 8BE2 L XREF=UW 8BE CL E FROM 9BE(3HE,A). 8BE CL WIDTH FROM 9BE(3HE,A). 8BE L 22.24E3 2 2+ 0.8 MEV AP 8BE2 L %N=? $ %P=? $ %D=? $ %A=? $ ISPIN=0 8BE3 L XREF=DGMNOZ 8BE CL E FROM 6LI(D,A) (1997CZ01). 8BE CL WIDTH FROM 6LI(D,A) (1965FR02). 8BE L 22.63E+3 10 100 KEV 50 8BE2 L XREF=KW 8BE CL E FROM 9BE(3HE,A). 8BE CL WIDTH FROM 9BE(3HE,A). 8BE L 22.98E+3 10 230 KEV 50 8BE2 L XREF=W 8BE CL E FROM 9BE(3HE,A). 8BE CL WIDTH FROM 9BE(3HE,A). 8BE L 24000 (1,2)- 7 MEV AP A 8BE2 L ISPIN=1 8BE2 L %IT=? $ %P=? $ %A=? $ XREF=LOZ 8BE CL WIDTH FROM 7LI(P,G). 8BE L 25200 2+ 8BE2 L ISPIN=0 $ %P=? $ %D=? $ %A=? 8BE3 L XREF=DGOZ 8BE L 25500 4+ 8BE2 L %D=? $ %A=? $ ISPIN=0 8BE3 L XREF=DG 8BE CL WIDTH BROAD 8BE L 27494.1 180+ 5.5 KEV 20 8BE2 L %IT=0.60$ %N=39.4$ %P=6.9$ %D=27.0$ %3H=11.7$ %3HE=6.6$ %A=7.9$ ISPIN=2 8BE3 L XREF=EFGX 8BE CL E FROM WEIGHTED AVERAGE OF 8BE2CL E=27492.2 KEV 26 10B(P,3HE) (1975RO01) AND 8BE3CL 27495.8 KEV 24 6LI(D,G) (1976NO07). 8BE CL WIDTH FROM 6LI(D,G). 8BE2CL OTHER VALUES ARE 8BE2CL WIDTH=10 KEV 3 6LI(D,P),(D,D),(D,A) (1969BL14), 8BE3CL 14.7 KEV 40 4HE(A,A),(A,P) (1976HI04) AND 8BE4CL 12.3 KEV 3 10B(P,3HE) (1975RO01). 8BE CL E FOR PARAMETERS OF THIS STATE SEE (1979FR04). HOWEVER, THE SUM 8BE2CL OF THE BRANCHING RATIOS GIVEN IN (1979FR04) GREATLY EXCEEDS 100%. 8BE G 9847.6 M1 8BE2 G WIDTHG=21.9 EV 39 $ BM1W=1.10 20 8BE CG WIDTHG FROM (1979FR04). REVISED FROM WIDTHG=24 EV 3 (1976NO07). 8BE L 28600 ? 8BE2 L %IT=? $ %P=? 8BE3 L XREF=L 8BE CL WIDTH BROAD 8BE L 32E3 1 MEV ? 8BE2 L XREF=Z 8BE CL E FROM 10B(D,A) (1993PA31). 8BE CL WIDTH FROM 10B(D,A) (1993PA31). 8BE L 41E3 AP ? 8BE2 L XREF=G