ADOPTED LEVELS, GAMMAS for 91Ru

Author: Coral M. Baglin |  Citation: Nucl. Data Sheets 114, 1293 (2013) |  Cutoff date: 1-Sep-2013 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-9440 keV SYS(n)= 11427 keV 4S(p)= 4803.8 keV 24Q(α)= -3780 keV 4
Reference: 2012WA38

References:
  A  58Ni(36Ar,2pnγ): E=149 MeV  B  58Ni(40Ca,A2PNG)
  C  91Rh ε decay (1.47 S)  D  58Ni(36Ar,2pnγ): E=111 MeV

General Comments:

Other Reactions:

91Ru εp decay (1983Ha06): ΔE,E counter telescope, FWHM=65 keV; observed ε-delayed p spectrum; inferred existence of low-spin 91Ru isomer.

Theory (partial list):

Nuclear structure: 1994He09, 1996Ru02 (shell-model calculations).

Q-value: ΔQ(β-)=400 (2012Wa38).

Q-value: Q(εp)=4644 4 (2012Wa38).










E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
     0.0ABCD (9/2+) 8.0 s 4 
% ε = 100
     
     0.0+X     (1/2-) 7.6 s 8 
% IT = ?
% β+p > 0
% ε > 0
     
    46   D (7/2+)       46S
 

     0.0
(9/2+)
   436.0 5    D (11/2+)      436.0 5 
  100

     0.0
(9/2+)
   889.8 2   CD (11/2+)      844
   889.8 2 
 
  100


    46
     0.0
(7/2+)
(9/2+)
   973.5AB D (13/2+)      538.0 5 
   973.1 1 
   <0.40
  100
M1
E2
   436.0
     0.0
(11/2+)
(9/2+)
  1660   D (11/2+)      686
  1614
  1660
 
 
 



   973.5
    46
     0.0
(13/2+)
(7/2+)
(9/2+)
  1872.0AB D (17/2+)      898.5 5 
  100
E2
   973.5
(13/2+)
  1893.0AB D (13/2-)      234
   919.8 5 
  1003
 
  100.0 9 
 

E1

  1660
   973.5
   889.8
(11/2+)
(13/2+)
(11/2+)
  2179   D (15/2+)      519
  100

  1660
(11/2+)
  2200.0AB D (17/2-)      306.8 5 
   328.0 5 
    7.6 8 
  100.0 4 
Q
E1
  1893.0
  1872.0
(13/2-)
(17/2+)
  2253.8AB D (15/2-)      360.6 5 
  1280.7 5 
  100 3 
   36 14 
M1
E1
  1893.0
   973.5
(13/2-)
(13/2+)
  2363   D (17/2+)      491.4 5 
  100
M1
  1872.0
(17/2+)
  2369.4AB D (21/2+)      497.2 5 
  100
E2
  1872.0
(17/2+)
  2409.3AB D (17/2-)      155.4 5 
   209.4 5 
   516.4 5 
   67 4 
  100 4 
   24.4 22 
D

E2
  2253.8
  2200.0
  1893.0
(15/2-)
(17/2-)
(13/2-)
  2709.3AB D (19/2-)      299.9 5 
   509.4
  100 14 
   57 29 
M1

  2409.3
  2200.0
(17/2-)
(17/2-)
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
  2799   D (21/2+)      436.0 5 
  100
E2
  2363
(17/2+)
  2927.6A  D (19/2-)      218
   727.5 5 
   33 17 
  100 17 

M1
  2709.3
  2200.0
(19/2-)
(17/2-)
  2985.3AB D (23/2+)      615.8 5 
  100
M1
  2369.4
(21/2+)
  3004.9A    (19/2-)      296.3
   804
  100 33 
   67 33 


  2709.3
  2200.0
(19/2-)
(17/2-)
  3164.3AB D (21/2-)      236.8 5 
   455.0 5 
   754.5 5 
   964.5 5 
   16.8 17 
    5.8 6 
    9.8 12 
  100.0 17 

D

E2
  2927.6
  2709.3
  2409.3
  2200.0
(19/2-)
(19/2-)
(17/2-)
(17/2-)
  3192.5AB D (25/2+)      206.9 5 
   823.0 5 
  100.0 25 
   42.5 13 
D
E2
  2985.3
  2369.4
(23/2+)
(21/2+)
  3258   D (21/2-)      549.3 5 
  100
M1
  2709.3
(19/2-)
  3554.6AB D (23/2-)      296.0 5 
   390.5 5 
   549.3 5 
   845.3 5 
   59 7 
  100 7 
   25 8 
   74 4 

M1

E2
  3258
  3164.3
  3004.9
  2709.3
(21/2-)
(21/2-)
(19/2-)
(19/2-)
  3633.6AB D (25/2+)      648.0 5 
  1263.9 5 
   57 4 
  100 21 

E2
  2985.3
  2369.4
(23/2+)
(21/2+)
  3893.9A    (23/2-)      339
   889.4
   29 14 
  100 14 


  3554.6
  3004.9
(23/2-)
(19/2-)
  3969.8AB D (27/2+)      336.5 5 
   777.5 5 
   67 4 
  100.0 21 

M1
  3633.6
  3192.5
(25/2+)
(25/2+)
  4035.8AB D (25/2-)      142
   871.2 5 
   11 6 
  100 11 

E2
  3893.9
  3164.3
(23/2-)
(21/2-)
  4151.6AB D (29/2+)      181.6 5 
   959.4 5 
   28.1 10 
  100 3 
D
E2
  3969.8
  3192.5
(27/2+)
(25/2+)
  4379.7AB D (27/2-)      343.8 5 
   824.7 5 
  100.0 19 
   69 4 
M1
Q
  4035.8
  3554.6
(25/2-)
(23/2-)
  4847   D (27/2-)      811.6 5 
  100
M1
  4035.8
(25/2-)
E(level)
(keV)		XREFJπ(level) T1/2(level)E(γ)
(keV)		I(γ)M(γ)Final Levels
  4991.9AB D (29/2-)      612.3 5 
  1022
  100 9 
    9 4 
M1

  4379.7
  3969.8
(27/2-)
(27/2+)
  5097   D (31/2+)     1126.9 5 
  100
Q
  3969.8
(27/2+)
  5100   D (29/2-)      252.9 5 
   720.7 5 
  <86
  100 14 

M1
  4847
  4379.7
(27/2-)
(27/2-)
  5108.8AB D (33/2+)      957.4 5 
  100
E2
  4151.6
(29/2+)
  5961.7AB   (35/2+)      852.9
  100
D
  5108.8
(33/2+)
  5996.4AB D (33/2-)     1004.7 5 
  100
E2
  4991.9
(29/2-)
  6085.0AB   (37/2+)      123.3
   976.2
   75 11 
  100 16 


  5961.7
  5108.8
(35/2+)
(33/2+)
  6313.8AB   (35/2-)      317.4
  100
D
  5996.4
(33/2-)
  6922.3AB   (37/2-)      608.5
  100

  6313.8
(35/2-)
  7515.2AB   (41/2+)     1430.2
  100
Q
  6085.0
(37/2+)
  7516.8AB   (39/2-)     1203.0
  100
Q
  6313.8
(35/2-)
  8149AB   (41/2-)     1226.7
  100

  6922.3
(37/2-)
  9630 B   (43/2-,45/2-)     1481.2
  100

  8149
(41/2-)

E(level): From least-squares fit to Eγ, allowing 1 keV uncertainty (the maximum specified by authors) for data from (40Ca,α2pnγ) and (36Ar,2pnγ): E=149 MeV.

Jπ(level): Based on γ deexcitation data given in comments and/or on systematics of (HI,xnγ)-type reactions, unless noted otherwise.

E(γ): From (36Ar,2pnγ): E=111 MeV, unless noted otherwise. These data are in excellent agreement with those from (36Ar,2pnγ): E=149 MeV, for which ΔEγ=0.1-1.0 keV, depending on energy and Iγ, and with those from (40Ca,α2pnγ) for which the stated precision is 0.2-1.0 keV.

I(γ): From (36Ar,2pnγ): E=111 MeV, unless noted otherwise.

M(γ): From measured DCO ratio in (36Ar,2pnγ): E=149 MeV, except as noted.

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Band Transitions:

E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 1 - π=-, SENIORITY ≥ 3 STATES.
  1893.0 (13/2-)        
  2200.0 (17/2-)        
  2253.8 (15/2-)      360.6 5 
  1280.7 5 
  100 3 
   36 14 
M1
E1
  1893.0
   973.5
(13/2-)
(13/2+)
  2409.3 (17/2-)      155.4 5 
   209.4 5 
   516.4 5 
   67 4 
  100 4 
   24.4 22 
D

E2
  2253.8
  2200.0
  1893.0
(15/2-)
(17/2-)
(13/2-)
  2709.3 (19/2-)      299.9 5 
   509.4
  100 14 
   57 29 
M1

  2409.3
  2200.0
(17/2-)
(17/2-)
  2927.6 (19/2-)      218
   727.5 5 
   33 17 
  100 17 

M1
  2709.3
  2200.0
(19/2-)
(17/2-)
  3004.9 (19/2-)      296.3
   804
  100 33 
   67 33 


  2709.3
  2200.0
(19/2-)
(17/2-)
  3164.3 (21/2-)      236.8 5 
   455.0 5 
   754.5 5 
   964.5 5 
   16.8 17 
    5.8 6 
    9.8 12 
  100.0 17 

D

E2
  2927.6
  2709.3
  2409.3
  2200.0
(19/2-)
(19/2-)
(17/2-)
(17/2-)
  3554.6 (23/2-)      296.0 5 
   390.5 5 
   549.3 5 
   845.3 5 
   59 7 
  100 7 
   25 8 
   74 4 

M1

E2
  3258
  3164.3
  3004.9
  2709.3
(21/2-)
(21/2-)
(19/2-)
(19/2-)
  3893.9 (23/2-)      339
   889.4
   29 14 
  100 14 


  3554.6
  3004.9
(23/2-)
(19/2-)
  4035.8 (25/2-)      142
   871.2 5 
   11 6 
  100 11 

E2
  3893.9
  3164.3
(23/2-)
(21/2-)
  4379.7 (27/2-)      343.8 5 
   824.7 5 
  100.0 19 
   69 4 
M1
Q
  4035.8
  3554.6
(25/2-)
(23/2-)
  4991.9 (29/2-)      612.3 5 
  1022
  100 9 
    9 4 
M1

  4379.7
  3969.8
(27/2-)
(27/2+)
  5996.4 (33/2-)     1004.7 5 
  100
E2
  4991.9
(29/2-)
E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
  6313.8 (35/2-)      317.4
  100
D
  5996.4
(33/2-)
  6922.3 (37/2-)      608.5
  100

  6313.8
(35/2-)
  7516.8 (39/2-)     1203.0
  100
Q
  6313.8
(35/2-)
  8149 (41/2-)     1226.7
  100

  6922.3
(37/2-)
E(level)
(keV)		Jπ(level) T1/2(level)E(γ)I(γ)M(γ)Final Levels
Band 2 - π=+, SENIORITY ≥ 3 STATES.
   973.5 (13/2+)        
  1872.0 (17/2+)        
  2369.4 (21/2+)      497.2 5 
  100
E2
  1872.0
(17/2+)
  2985.3 (23/2+)      615.8 5 
  100
M1
  2369.4
(21/2+)
  3192.5 (25/2+)      206.9 5 
   823.0 5 
  100.0 25 
   42.5 13 
D
E2
  2985.3
  2369.4
(23/2+)
(21/2+)
  3633.6 (25/2+)      648.0 5 
  1263.9 5 
   57 4 
  100 21 

E2
  2985.3
  2369.4
(23/2+)
(21/2+)
  3969.8 (27/2+)      336.5 5 
   777.5 5 
   67 4 
  100.0 21 

M1
  3633.6
  3192.5
(25/2+)
(25/2+)
  4151.6 (29/2+)      181.6 5 
   959.4 5 
   28.1 10 
  100 3 
D
E2
  3969.8
  3192.5
(27/2+)
(25/2+)
  5108.8 (33/2+)      957.4 5 
  100
E2
  4151.6
(29/2+)
  5961.7 (35/2+)      852.9
  100
D
  5108.8
(33/2+)
  6085.0 (37/2+)      123.3
   976.2
   75 11 
  100 16 


  5961.7
  5108.8
(35/2+)
(33/2+)
  7515.2 (41/2+)     1430.2
  100
Q
  6085.0
(37/2+)

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Additional Gamma Data:











E(level)
(keV)		Jπ(level)T1/2(level)E(γ)
(keV)		MultipolarityAdditional Data
  2369.4 (21/2+)      497.2 5 E2B(E2)(W.u.)>0.038

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
     0.0(9/2+) 8.0 s 4 
% ε = 100
E(level): From systematics of n=47 isotones, it is concluded that the 1/2- state (rather than the 9/2+ state) is the isomeric one (1983Ha06).
     0.0+X(1/2-) 7.6 s 8 
% IT = ?
% β+p > 0
% ε > 0
Jπ(level): Although the T1/2 observed in ε-delayed p decay is similar to that measured in (9/2+) 91Ru ε decay, it is presumed that two isomers exist since the spin difference between 91Ru (9/2+) and 90Mo g.s. (0+) is too large to allow sizeable ε-delayed p decay. Also, from systematics for n=47 isotones, 9/2+ and 1/2- states are expected at low excitation and, among these Jπ possibilities, the statistical-model calculations of 1983Ha06 favor 1/2- for the delayed p precursor. Dominant configuration=(ν p1/2)-1 (1994He09).
   973.5(13/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  1872.0(17/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  1893.0(13/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  2200.0(17/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  2253.8(15/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  2369.4(21/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  2409.3(17/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): configuration includes major contribution from ((ν p1/2)-1(ν g9/2)-2)17/2 or ((π g9/2)2(ν p1/2)-1(ν g9/2)-2) (see 1994He09).
  2709.3(19/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  2927.6(19/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
  2985.3(23/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  3004.9(19/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
  3164.3(21/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  3192.5(25/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  3554.6(23/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  3633.6(25/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  3893.9(23/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
  3969.8(27/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  4035.8(25/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  4151.6(29/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  4379.7(27/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  4991.9(29/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  5108.8(33/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  5961.7(35/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
E(level)Jπ(level)T1/2(level)Comments
  5996.4(33/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): configuration includes major contribution from ((ν p1/2)-1(ν g9/2)-2)17/2 or ((π g9/2)2(ν p1/2)-1(ν g9/2)-2) (see 1994He09).
  6085.0(37/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  6313.8(35/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  6922.3(37/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  7515.2(41/2+)   E(level): π=+, SENIORITY ≥ 3 STATES.
  7516.8(39/2-)   XREF: B(7197).
E(level): π=-, SENIORITY ≥ 3 STATES.
Jπ(level): Major configuration=((π p1/2)(π g9/2)n(ν g9/2)-m), with seniority=3, 5, 7 and/or 9 components; see 1994He09 for more detailed discussion of likely configurations.
  8149(41/2-)   E(level): π=-, SENIORITY ≥ 3 STATES.

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Additional Gamma Comments:

E(level)E(gamma)Comments
    46    46E(γ): from level energy difference. γ shown in fig. 7 of 2013Zh10 but details not yet available.
   889.8   889.8E(γ): from ε decay.
   973.5   538.0M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   973.1E(γ): from ε decay; 973.5 5 from (36Ar,2pnγ): E=111 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  1872.0   898.5M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  1893.0   919.8M(γ): interpreted as ΔJ=0 transition in (40Ca,α2pnγ).. From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2200.0   306.8I(γ): 11 3 from (40Ca,α2pnγ), 34 7 from (36Ar,2pnγ): E=149 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   328.0I(γ): From 58Ni(36Ar,2pnγ): E=149 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2253.8   360.6M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  1280.7M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2363   491.4M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2369.4   497.2M(γ): Q from DCO ratio in (36Ar,2pnγ): E=149 MeV; not M2 from RUL, based on |<20 ns γγ-coincidence resolving time.. From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2409.3   155.4M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   209.4M(γ): interpreted as d, ΔJ=0 in (36Ar,2pnγ): E=111 MeV.
   516.4M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2709.3   299.9I(γ): from (36Ar,p2nγ): E=149 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   509.4I(γ): from (36Ar,p2nγ): E=149 MeV; unobserved at E=111 MeV.
  2799   436.0M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2927.6   218I(γ): from (36Ar,p2nγ): E=149 MeV only.
   727.5I(γ): from (36Ar,p2nγ): E=149 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  2985.3   615.8M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  3004.9   296.3I(γ): from (36Sr,p2nγ): E=149 MeV.
   804I(γ): from (36Sr,p2nγ): E=149 MeV.
  3164.3   964.5M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  3192.5   206.9M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   823.0M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
E(level)E(gamma)Comments
  3258   549.3M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.. From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  3554.6   390.5M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   845.3M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  3633.6  1263.9M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  3969.8   336.5I(γ): weighted average of 60 10 from (36Ar,2pnγ): E=149 MeV and 63 18 from (40Ca,α2pnγ).
   777.5M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  4035.8   871.2M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  4151.6   181.6I(γ): other Iγ: 43 4 from (40Ca,α2pnγ); 20 6 in (36Ar,2pnγ): E=149 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   959.4M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  4379.7   343.8M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
   824.7E(γ): From systematics of n=47 isotones, it is concluded that the 1/2- state (rather than the 9/2+ state) is the isomeric one (1983Ha06).
M(γ): Based on measured γ anisotropy ratio in (40Ca,α2pnγ).
  4847   811.6M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  4991.9   612.3M(γ): DCO ratio in (36Ar,2pnγ) not consistent with pure Q (as proposed based on γ anisotropy data in (40Ca,α2pnγ)).. From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  5097  1126.9I(γ): From 58Ni(36Ar,2pnγ): E=149 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  5100   252.9I(γ): From 58Ni(36Ar,2pnγ): E=149 MeV.
   720.7I(γ): From 58Ni(36Ar,2pnγ): E=149 MeV.
M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  5108.8   957.4M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  5961.7   852.9E(γ): from (36Ar,2pnγ): E=149 MeV.. From systematics of n=47 isotones, it is concluded that the 1/2- state (rather than the 9/2+ state) is the isomeric one (1983Ha06).
M(γ): Based on measured γ anisotropy ratio in (40Ca,α2pnγ).
  5996.4  1004.7M(γ): From DCO and/or polarization in (36Ar,2pnγ): E=111 MeV.
  6085.0   123.3I(γ): from (40Ca,α2pnγ); 44 22 from (36Ar,2pnγ): E=149 MeV.
  6313.8   317.4E(γ): From systematics of n=47 isotones, it is concluded that the 1/2- state (rather than the 9/2+ state) is the isomeric one (1983Ha06).
M(γ): Based on measured γ anisotropy ratio in (40Ca,α2pnγ).
  6922.3   608.5M(γ): Q from γ-anisotropy ratio in (40Ca,α2pnγ); however, Eγ is atypically low for a crossover transition, and γ is placed as a ΔJ=1, Δπ=no transition in (36Ar,2pnγ): E=149 MeV.
  7515.2  1430.2E(γ): from (40Ca,α2pnγ).. From systematics of n=47 isotones, it is concluded that the 1/2- state (rather than the 9/2+ state) is the isomeric one (1983Ha06).
M(γ): Based on measured γ anisotropy ratio in (40Ca,α2pnγ).
  7516.8  1203.0E(γ): from (40Ca,α2pnγ).. From systematics of n=47 isotones, it is concluded that the 1/2- state (rather than the 9/2+ state) is the isomeric one (1983Ha06).
M(γ): Based on measured γ anisotropy ratio in (40Ca,α2pnγ).
  8149  1226.7E(γ): from (40Ca,α2pnγ).
E(level)E(gamma)Comments
  9630  1481.2E(γ): from (40Ca,α2pnγ).

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