[terroreman]

204Hg *204HG(P,P') 1991HO07 94NDS 199411
204 80 I 47 0 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
C E(P)=28 MEV, 98.2% 204HG, mag spect FWHM=17 KEV, p'(THETA), coupled
2C channel calc (1991Ho07).
CL J$From 1991Ho07 based on p'(THETA) and on unpublished (E,E') data of
2CL 1989BuZP
CL S$BETA(L) values are quoted based on coupled-channels analysis
1 L 0 0+
2 L 437 3 2+ -0.069
3 L 1128 4 4+ -0.049
4 L 1632 11 0+
5 L 1714 6
6 L 1836 5
7 L 1985 7
8 L 2099 8
9 L 2137 9
10 L 2183 4 6+ -0.013
11 L 2257 4 5- 0.033
12 L 2293 4 7- -0.021
13 L 2398 9
14 L 2463 9
15 L 2509 5
16 L 2672 4 3- 0.089
17 L 2710 4
18 L 2759 4
19 L 2813 4 3- 0.046
20 L 2866 4
21 L 3021 4 (4+) 0.016
22 L 3112 4 (4+) 0.016
23 L 3227 4 (5-) 0.020
24 L 3315 4 3- 0.048
25 L 3364 4 5- 0.049
26 L 3417 4
27 L 3439 4
28 L 3496 5
29 L 3528 6
30 L 3585 4
31 L 3618 6
32 L 3664 9
33 L 3697 5
34 L 3712 7
35 L 3750 4
36 L 3779 4
37 L 3833 8
38 L 3869 7
39 L 3923 9
40 L 3954 10
41 L 4113 5 4+ 0.039
42 L 4164 5
43 L 4225 6
44 L 4262 5
45 L 4321 6
46 L 4356 6
47 L 4406 6

204Hg *204HG(D,PNG) 1984SC19 94NDS 199411
204 80 I 14 16 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
C 98% 204HG, E(D)=25 MEV. PG-coin GE(LI) plastic scin; GG; CE(T)
2C magnetic spectrometer; G(THETA) (1984Sc19)
CG RI Estimated uncertainty 10-20%
CG M From G(THETA) and CE (1984Sc19)
CL J$From 1984Sc19 based on G(THETA) and EKC, and from adopted levels
1 L 0 0+
2 L 436.60 10 2+
1 G 436.6 1 100 E2
3 L 1128.50 15 4+
2 G 691.9 1 63
4 L 1828.6 5 (2)
2 G 1392.0 5 3.1
5 L 1851.69 24 (2+)
3 G 723.2 2 3.7
2 G 1414.8
6 L 1947.3 5 1+,2+
2 G 1510.7 5 2.6
7 L 1988.7 5 (2+,3-)
2 G 1552.1 5 2.6
8 L 2190.90 25 6+
3 G 1062.4 2 17
9 L 2236.0 4
3 G 1107.5 3 2.9
3 CG E$placement based on the placement of the 1107.7 1 GAMMA in (N,N'G)
10 L 2262.9 4 5-
3 G 1134.4 3 18 E1
3 CG M from CE and G(THETA) this is a stretched E1.
11 L 2300.5 4 (2)
3 G 1172.0 3 3.1
3 CG E$placement based on the placement of the 1172.0 1 GAMMA in (N,N'G)
12 L 2300.5 4 7- 6.7 NS 5
12 CL J see adopted levels
8 G 109.6 2 6.0 E1
13 L 2724.2 4 GE 5
11 G 423.7 2 4.0
? 10 G 460.5 10 1 AP
14 L 2760.4 4 GE 3
10 G 497.5 2 3.2
? 8 G 569.5 10 1 AP

204Hg *204HG(D,D') 1972MO12 94NDS 199411
204 80 I 4 0 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
C E(D)=17 MEV, 95.8% 204HG; FWHM=9 KEV; d'(THETA) (1972Mo12).
1 L 0
2 L 443 8
3 L 1140 12
? 4 L 1851 15

204Hg *204HG(A,A') 1981BA45 94NDS 199411
204 80 I 5 0 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
1C 84% 204HG, E(A)=27 MEV, magnetic spectrograph A'(THETA), FWHM=40 KEV
2C coupled-channels analysis (1981Ba45).
CL J From 1981Ba45 based on A'(THETA).
1 L 0 0+
2 L 437 5 2+
2 CL BETA(2)=0.061
3 L 1128 5
4 L 2272 5
5 L 2674 5 (3-)
5 CL BETA(3)=0.076 octupole vibration

204Hg *COULOMB EXCITATION 94NDS 199411
204 80 I 7 5 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
C 98% 204HG sulphide target. 1040-MEV 208PB beam. Particle-GAMMA coin
2C GE(LI) and position-sensitive plate avalanche detectors, G(THETA).
3C BE2 values are normalized to 0.0849 for the 2+ to 0+ transition (an
4C average of 1981Es03 and 1979Bo02). A 5% systematic error was included
5C in the quoted uncertainties in BE2 (1985Ag01).
1C 4HE 13.5-16.5 MEV, 12C 45-56 MEV, 16O 63-65 MEV; 93% 204HG
2C annular SI detector for backward scattering. E(P)=18 MEV E-DE counter
3C telescope, Winther-de Boer analysis (1981Es03).
1C Natural HG; 15 MEV 4HE, 56-64 MEV 16O; gammas GE(LI); MOME2 of
2C 436 level measured by reorientation effect (1979Bo02)
C E(A)=11-15 MEV, E(16O)=56 MEV, Winther-de Boer analysis (1977BoYP)
C E(16O)=36 MEV, RI(THETA) in vacuum and HE gas (1974Do01)
1C E(12C)=54, 55 MEV. 92.6% 204HG, mag spect. BE3 deduced (1991Li03).
CG RI From 1985Ag01
CG E$From 1985Ag01, 1979Bo02
CG M$From 1981Es03, 1985Ag01
CL J From adopted levels
1 L 0 0+
2 L 436.55 32+
22 L MOME2=0.40 20 (1981ES03)
2 CL MOME2: 0.39 20 or 0.24 20 (1979Bo02)
21CL From attenuation of G(THETA) of recoils in vacuum
22CL OMEGA**2*TAU=4.1 7 (changed by evaluator from 4.6 8 of 1974Do01 because
23CL of change in T1/2(436 level) from 36 PS to 40.4 PS); therefore,
24CL MOMM1(204HG)/MOMM1(198HG)=0.89 8. Using MOMM1(198HG)=1.1 2
25CL (1977Ha26,1964Ko15) we get MOMM1(204HG)=1.0 3. Others: 1970Ka09,
2xCL 1973Di15
1 G 436.55 3 100 E2 0.04
1 CG BE2=0.0849 8 (from 0.0846 10 (1981Es03) and 0.0854 12
1xCG (1979Bo02))
3 L 1128.45 21 4+
2 G 691.9 2 19.9 6 E2 0.013
2 CG BE2=0.121 9 (1985Ag01), 0.19 6 (1981Es03)
4 L 1987.9 (2+,3-)
? 2 G 1551.3 2 0.11 1
? 2 CG Placement from (D,PNG) and 204AU B- decay, adopted
? 22CG EG=1552.78 10
5 L 2191.0 4 6+
3 G 1062.5 3 1.36 4 E2 0.005
3 CG BE2=0.139 17 (1985Ag01)
6 L 2515.1 6
3 G 1386.6 5 0.24 3
3 CG E$placement based on (N,N'G), adopted EG=1386.2 2
7 L 2682 3 3-
7 CL E seen in (P,P') of 1981Es03 and 1991Ho07
72 L BE3=0.37 5
7 CL The BE3 value corresponds to 22 W.u. ^and is comparable
72CL to the values for collective 3- states in the even HG isotopes GE 198
73CL (in (E,E') the measured BE3W=24 2)

204Hg *205TL(E,E'P) 1987QU01 94NDS 199411
204 80 I 4 0 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
C E(E)=410 MEV, spectra at the missing momentum values of
2C 15, 80, and 160 ^MEV/c were measured. FWHM=135 KEV for the proton
3C energy.
CL S$Spectroscopic factor for 3s1/2 is listed.
1 L 0 0.32 3
2 L 1640 10 0.22 2
3 L 2370 20 0.08 1
4 L 2620 30 0.05 1

204Hg *205TL(MU-,NG) 94NDS 199411
204 80 I 14 13 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
C The decay scheme is suggested by evaluator on the basis of
2C 204AU B- decay and (D,PNG).
CL J From adopted levels
CG RI Per 100 MU- stops in natural TL (1972Ba53)
CG E From 1972Ba53 except for the 436G from 1978Du01
CG E(E) Assigned to 204HG by evaluator
1 L 0 0+
2 L 436.551 8 2+
1 G 436.551 8 25.4 41
3 L 1128.26 17 4+
2 G 691.71 17 7.6 9
2F G FLAG=E
4 L 1827.9 4 (2)
2 G 1391.3 4 0.68 17
2F G FLAG=E
5 L 1841.4 10 1+,2+
S 2 G 1404.82
6 L 1948.2 3 1+,2+
2 G 1511.6 3 1.5 3
2F G FLAG=E
7 L 1990.5 4 (2+,3-)
2 G 1553.9 4 0.96 24
2F G FLAG=E
8 L 2140.5 4 1,2,3
2 G 1703.9 4 0.7 2
2F G FLAG=E
9 L 2191.0 11 6+
S 3 G 1062.7
10 L 2262.9 3 5-
3 G 1134.67 20 3.0 6
3F G FLAG=E
11 L 2264.6 5 1,2,3
2 G 1828.0 5 0.50 16
12 L 2300.6 11 7-
9 G 109.68 12 0.98 18
9F G FLAG=E
13 L 2726.2 6 (2+,3)
3 G 1597.9 5 0.62 17
3F G FLAG=E
14 L 2760.7 4 GE 3
10 G 497.8 3 0.77 22
10F G FLAG=E

204Hg *205TL(D,3HE) 1989GR09 94NDS 199411
204 80 I 21 0 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
C JPI(target)=1/2+
1C Enriched 205TL, E(D)=45 MEV, magnetic spectrometer. Results are
2C preliminary, no uncertainties given (1983AgZY)
1C 99.5% 205TL, E(D)=52 MEV, polarized beam average polarization of 0.54
2C FWHM=110 KEV for vector-polarized beam, FWHM=70 KEV for unpolarized
3C beam. DWBA calc normalized to 208PB(D,3HE) (1989Gr09)
CL E,L$From 1989Gr09, DE AP 15 KEV. See also: 1987Cl01
CL J$From 1989Gr09 based on L transfer, vector analyzing power and
2CL previous NDS assignments.
CL E(C) Unresolved multiplet
CL S$Spectroscopic factors for L=0 are from 3s1/2, for L=2 below 2.7
2CL MEV are from 2d3/2 and above 2.7 MEV from 2d5/2 (except for 3320
3CL level 2d3/2), for L=5 are from 1h11/2. For cases of two L values,
4CL the ^S factors are listed in the order s1/2,d3/2,h11/2,d5/2. In
5CL cases where one of the L values is even and the other is odd, it
6CL is clear that at least two levels with opposite parities contribute.
1 L 0 0+ 0 .21
2 L 437 2+ 2 .18
3 L 1130 4+
4 L 1630 (0,1)+ 0 .16
5 L 1840 1+,2+ 2 .14
6 L 1950 2+ 2 .28
7 L 2060 AP (1,2,3)+ 2 .05
8 L 2120 (1,2)+ 2 .14
9 L 2250 5- 2,5 .04, .21
9F L FLAG=C
10 L 2380 (0,1,2,3)+ 0,2 .05, .04
10 CL J$JPI=1+ if only one state contributes
11 L 2470 (1,2,3)+ 2 .03
12 L 2650 (0,1,2,3)+ 0,2 .08, .03
12F L FLAG=C
13 L 2770 2,5 .20, .16
13F L FLAG=C
14 L 2890 2,5 .16, .10
14F L FLAG=C
15 L 3050 2,5 .12, .05
15F L FLAG=C
16 L 3190 (2,3)+ 2 .41
17 L 3320 2,5 .07, .05
17F L FLAG=C
18 L 3460 (1,2,3)+ 2 .13
19 L 3600 2,5 .03, .11
19F L FLAG=C
20 L 3770 (1,2,3)+ 2 .05
21 L 3890 (0,1,2,3)+ 0,2 .05, .06

204Hg *208PB(D,6LI) 1979BE14 94NDS 199411
204 80 I 9 0 0 0 0 0
H TYP=FUL$AUT=M. R. SCHMORAK$CIT=NDS 72,409 (1994)$CUT=1-Sep-1994$
1C E(D)=55 MEV; magnetic spectrograph, E DE counter; 99% 208PB,
2C FWHM=150-300 KEV; 6LI(THETA). ALPHA clustering calculated (1979Be14)
CL J From 1979Be14 based on DWBA, natural parity favored
1 L 0 0+
2 L 430 50 2+
3 L 1085 50(4+)
? 4 L 1810 50
5 L 2240 50 GE 3
6 L 2740 50 GE 2
7 L 2800 50
8 L 3040 50 GE 2
9 L 3550 50 GE 2