Structure of RIPL discrete level library files

R. Capote and M. Verpelli (December 7, 2020)

The description of how the files are generated can be found in
INDC-NDS(0702) and in INDC-NDS(0626).
See also the 2002 and 2015 description of the RIPL discrete levels.
Content:     Changes 2015     File Structure     Identification Record     Level Record     Gamma Record     Changes 2012     +X energy assignment
Major changes from the 2015 release
Ground State (GS) properties are taken from
Nubase2016, and separation values from AME2016

In this release, The FORTRAN format of the GAMMA record has one additional digit for the energy
((39x,i4,1x,f10.4,3(1x,e10.3)))

File Structure
Data are stored in files containing a full isotopic chain of a given element. File names indicate an element by referring to its atomic number (e.g., z026.dat).
Each Isotope has three types of records:
(i) identification,
(ii) level,
(iii) gamma.

Each isotope begins with an identification record, which is followed by the level record, which in turn is followed by the pertinent gamma records if decay of the level is known. This combination is repeated for all levels in a given isotope.
Identification Record
Each isotope begins with an identification record such as the one shown below for the case of Mg-22 (heading has been introduced to facilitate reading but does not show up in the actual file):

  SYMB    A     Z     Nol    Nog    Nmax    Nc     Sn[MeV]     Sp[MeV]
  22Mg    22    12    17     18      9      4     19.382000    5.497000

The corresponding FORTRAN format is (a5,6i5,2f12.6)
  
  
SYMB   : mass number with symbol of the element
A      : mass number
Z      : atomic number
Nol    : number of levels in the decay scheme
Nog    : number of gamma rays in the decay scheme
Nmax   : maximum number of levels up to which the level scheme is
         complete
Nc     : number of a level up to which spins and parities are unique
Sn     : neutron separation energy in MeV
Sp     : proton separation energy in MeV


Level Record
Each level record may contain the following quantities:
N1  Elv[MeV]  s   p   T1/2    Ng  J  unc  spins   nd  m  percent  mode      m   percent   mode    /.../ shift     band

1  0.000000  0.0  1  3.86E+00  0           0+      2  =  8.2000E+01 %IT     =  1.8000E+01 %B-     /.../ 0.031100  2    
2  1.246300  2.0  1  2.10E12   1           2+      0

(i3,1x,f10.6,1x,f5.1,i3,1x,(e10.3),i3,1x,a1,1x,a4,1x,a18,i3,10(1x,a2,1x,e10.4,1x,a7),f10.6,1x,3(2i))
 

Nl    :  sequential number of a level
Elv   :  energy of the level in MeV
s     :  level spin (unique). Whenever possible unknown spins up to
         Umax were inferred. Unknown and undetermined spins are entered as -1.0
p     :  parity (unique). If the parity of the level was unknown, positive or
         negative was chosen with equal probability. Parities were determined up
         to Umax as in the case of spins. The method of choice is not coded.
             The possible values are: 0 for unknown, +1 for positive and -1 for negative.
T1/2  :  half-life of the level (if known). All known half-lives or level widths
         were converted into seconds. Half-lives of stable nuclei are
         represented as -1.0E+0.
Ng    :  number of gamma rays de-exciting the level.
J     :  flag for spin estimation method (see below the list of possible flags).
unc   :  flag for an uncertain level energy. When impossible to determine, the
         relative energy of the band, the energy of these band heads were set to
         0.0 keV or, if the level order is known, to the preceding level energy
         with a note that an unknown energy X should be added. The notation uses
         X+, Y+, Z+ etc. for different bands.
spins :  original spins from the ENSDF file.
nd    :  number of decay modes of the level (if known). Values from 0 through 10
         are possible; 0 means that the level may decay via gamma-emission,
         and other decay modes are not known.
m     :  decay percentage modifier; informs a user about major uncertainties. 
         The modifiers are copied out of ENSDF with no modification, and can 
         have the following values: =, <, >, ? (unknown, but expected), 
         AP (approximate), GE (greater or equal), LE (less or equal), 
         LT (less then), SY  (value from systematics).
percent: percentage decay of different decay modes. As a general rule  the
         various decay modes add up 100%. There are, however, two exceptions:
         (i) when a small percentage decay is present, the sum may be slightly
         more then 100% due to rounding error, (ii) when beta -decay is
         followed by a heavier particle emission, the percentage of the
         beta-delayed particle emission is given as a portion of the beta-decay
         and the sum can be substantially larger then 100%. Naturally, when the
         modifier is "?" the sum is indefinite.
mode   : short indication of decay modes of a level (see Table below).
shift  : value assigned to the unknown "X", in MeV.
band   : integer assigned to band(s) to which the level is part

Spin estimation method flags
The spin values were determined in the following way. First it was checked whether a limited set of spin values could be assigned to a level based on gamma-transitions to known spin levels. In the second step, if there were 10 or more levels with known spins (they did not need to be unique); a spin distribution was determined from the experimentally known spins, plus the spins assigned in the first step. To do this the usual form of the spin distribution [Eri60,GIL65] is utilized. The experimental spin cut-off parameter s was determined from the average value of (J+1/2)2. In the case of the continuous normalized spin distribution this average yields 2s2 +1/4. Assuming that the average yields the same result in the discrete case, the experimental spin cut-off parameter sexp can easily be obtained. Levels up to the Emax value were used in this procedure. If less then 10 levels had spin assignments, then no spins were inferred; otherwise spins up to Emax were determined uniquely as described below.

Four cases were distinguished. Let Ni designate the number of spins, which are compatible with the experimental data for the ith level.
  1. Ni =0. A unique spin was determined using the spin distribution with sexp. This method is flagged as 'n'.
  2. Ni =1. In spite of uncertainties (like (1)+ ), this case was considered to be unique and the flag is 'u'.
  3. Ni >1. The spin was chosen from the limited set (eg. (1,3,4)-) using the spin continuous normalized distribution and the flag is 'c'.
  4. Above Emax the flag is left ' ' (blank).

Decay modes notation
The decay code is taken from the ENSDF format, the following table explains the meaning of the main decay modes
%B- β- decay
%EC electron capture
%EC+%B+ electron capture and β+ decay
%N neutron decay
%A α decay
%IT isomeric transition
%P proton decay
%3HE 3He decay
%B+P β+ delayed proton decay
%B-N β- delayed neutron decay
%SF spontaneous fission
%ECP electron capture delayed proton decay
%ECA electron capture delayed alpha decay
%G gamma decay
%B-2N β- delayed double neutron decay
%B+2P β+ delayed double proton decay
Gamma Record
Two examples of the gamma records are given below:
  Nf    Eg[MeV]       Pg          Pe          ICC
  3      0.055     2.790E-01   2.870E-01    5.130E-03
  1      0.113     5.330E-01   5.330E-01    0.000E+00

The corresponding FORTRAN format is (39x,i4,1x,f10.4,3(1x,e10.3))

Nf    : sequential number of the final state
Eg    : gamma-ray energy in MeV
Pg    : Probability that the level decays through photon (gamma ray) emission. 
        If no branching ratio is given in the ENSDF file, Pg=0.
Pe    : Probability of the electromagnetic transition (photon, conversion electron, pair creation). 
        The sum of the Pe gives the IT (electromagnetic transition) branching ratio of the level. 
        This is 1 unless other decay modes are listed in the level record (see example below). 
ICC   : Internal conversion coefficient of the transition.
Pe, Pg, and ICC are in the following relation:
Pe = Pg * (1 + ICC)
In the first gamma line Pe ≠ Pg since ICC ≠ 0
The sum of the Pe is 0.82, indeed the level record reports two decay modes: IT (82%) and beta- (18%)
N1  Elv[MeV]  s   p   T1/2       Ng  J  unc  spins   nd  m  percent    mode    m  percent    mode    
2   0.643400  4.0  1  2.200E-03  1            (4+)    2  =  8.2000E+01 %IT     =  1.8000E+01 %B-      
Major changes from the 2012 release

Treatment of the unknown "+X" energies


All levels having the same energy are splitted by 0.1 keV.

The internal conversion factor are calculated using BRICC

In the FORTRAN format of the LEVEL record, the half-life format is e10.3 and the decay branching is e10.4.
The two new fields at the end - in red here below
(i3,1x,f10.6,1x,f5.1,i3,1x,(e10.3),,i3,1x,a1,1x,a4,1x,a18,i3,10(1x,a2,1x,e10.4,1x,a7),f10.6,1x,3(2i))
have the following content:


"+X" energies summary

Nuclides where one or
more "+X" energies were assigned
using Nubase 2016.
# Nuclide Band Energy
021-Sc-56X100
123-V-44X270
223-V-60X0
323-V-60Y150
424-Cr-45X107
525-Mn-62X0
625-Mn-62Y343
727-Co-68X150
827-Co-68Y146.6
927-Co-70X200
1029-Cu-76Y200
1135-Br-92X662
1239-Y-78X500
1339-Y-92X807
1439-Y-102X200
1539-Y-102Y0
1641-Nb-85Y81
1741-Nb-86Y250
1841-Nb-88X130
1941-Nb-93X24.7
2041-Nb-100X313
2141-Nb-102X94
2242-Mo-93X25
2342-Mo-111X100
2443-Tc-87X0
2543-Tc-88W5
2643-Tc-88X0
2743-Tc-88Y300
2843-Tc-102X20
2943-Tc-114X160
3043-Tc-114Y0
3144-Ru-91X150
3244-Ru-113X130
3344-Ru-115X158.3
3445-Rh-92X50
3545-Rh-94X300
3645-Rh-98X60
3745-Rh-108X115
3845-Rh-110Y220
3945-Rh-112Y340
4045-Rh-114X200
4146-Pd-124X0
4247-Ag-94X1350
4347-Ag-96X0
4447-Ag-96Y50
4547-Ag-119X20
4647-Ag-119Y0
4747-Ag-122X80
4847-Ag-123X20
4947-Ag-123Y34.8
5047-Ag-124X0
5147-Ag-124Y100
5247-Ag-125X20.1
5347-Ag-126X0
5447-Ag-126Y100
5547-Ag-129X20
5648-Cd-125X186
5748-Cd-127X276
5848-Cd-129X150
5949-In-98X0
6049-In-98Y500
6149-In-120X300
6249-In-121Y1
6350-Sn-102Y48
6450-Sn-131X65.1
6551-Sb-119X10.3
6651-Sb-120X50
6751-Sb-121X19.5
6851-Sb-128X10
6951-Sb-132X200
7051-Sb-140X31.8
7152-Te-130X18.6
7255-Cs-117X50
7355-Cs-117Y0
7455-Cs-117Z150
7555-Cs-118X100
7655-Cs-119X50
7755-Cs-120X100
7855-Cs-123X20.37
7955-Cs-144Y300
8056-Ba-125X42.3
8157-La-124V100
8257-La-126X0
8357-La-126Z210
8457-La-128X100
8557-La-134X103.56
8657-La-146X130
8759-Pr-127X600
8859-Pr-130X0
8959-Pr-132X30
9059-Pr-134X0
9159-Pr-134Y68
9260-Nd-129Z50
9361-Pm-134X0
9461-Pm-134Y120
9561-Pm-135X0
9661-Pm-135Y151.3
9761-Pm-136X100
9861-Pm-136Y0
9961-Pm-138X30
10061-Pm-140X431
10161-Pm-152X100
10261-Pm-154X20
10361-Pm-158X29
10462-Sm-133Y120
10563-Eu-136X0
10663-Eu-136Y500
10763-Eu-140X210
10863-Eu-142X460
10964-Gd-139X250
11065-Tb-141X200
11165-Tb-145X850
11265-Tb-145Y0
11365-Tb-146X150
11465-Tb-154V8000
11565-Tb-154X12
11665-Tb-154Y200
11765-Tb-156X4.73
11867-Ho-148X250
11967-Ho-150X50
12067-Ho-154X243
12167-Ho-156X117.63
12267-Ho-160X27.4
12368-Er-147X100
12468-Er-149X29.3
12569-Tm-151X94
12669-Tm-152X100
12769-Tm-154X70
12869-Tm-156X196.4
12969-Tm-158X50
13069-Tm-160X7.8
13169-Tm-162X130
13269-Tm-164X10
13369-Tm-166X7.662
13469-Tm-174X252.4
13570-Yb-151X750
13670-Yb-151Y658.8
13770-Yb-151Z92
13870-Yb-153X121.8
13971-Lu-154X60
14071-Lu-154Y2569.6
14171-Lu-156X20
14271-Lu-159X100
14371-Lu-160X100
14471-Lu-161X7.5
14571-Lu-162X120
14671-Lu-162Y300
14771-Lu-167X30
14872-Hf-154X39
14973-Ta-161X61
15073-Ta-163X140
15173-Ta-173X7.22
15273-Ta-176W103
15373-Ta-178X0
15473-Ta-180X2.3
15573-Ta-183X25.84
15673-Ta-185X14.9
15773-Ta-189X1600
15873-Ta-190X25
15975-Re-159X210
16075-Re-164X50
16175-Re-166Y150
16275-Re-167X0
16375-Re-169X175
16475-Re-172X0
16575-Re-172Y100
16675-Re-179X49.8
16775-Re-180X89.2
16875-Re-182X60
16975-Re-192X-1.1
17075-Re-193X0
17175-Re-194X1100
17275-Re-196X120
17377-Ir-164X260
17477-Ir-168X50
17577-Ir-170X160
17677-Ir-171X167
17777-Ir-172X0
17877-Ir-172Y139
17977-Ir-185X39.8
18077-Ir-186X0.8
18177-Ir-188X46.47
18277-Ir-191X54.3
18377-Ir-194X180
18477-Ir-199X130
18578-Pt-204X0.1
18679-Au-172X160
18779-Au-175X167
18879-Au-176X0
18979-Au-176Y139
19079-Au-185X100
19179-Au-190X200
19279-Au-195X39.16
19379-Au-204X2839.4
19480-Hg-181Y210
19580-Hg-187X59
19680-Hg-189X80
19780-Hg-191X128
19880-Hg-208X41.1
19980-Hg-210X40
20081-Tl-179X825
20181-Tl-186X20
20281-Tl-186Y0
20381-Tl-187X46.77
20481-Tl-190X0
20581-Tl-190Y83
20681-Tl-191X297
20781-Tl-193X6.8
20881-Tl-194X260
20981-Tl-203X50.4
21081-Tl-204X0.2
21182-Pb-185X70
21282-Pb-190X3
21382-Pb-191X50
21482-Pb-193X130
21582-Pb-201X218.4
21682-Pb-202X23
21782-Pb-203X46.6
21882-Pb-211X24.9
21982-Pb-212X1335
22082-Pb-214X55
22182-Pb-216X55
22283-Bi-184X150
22383-Bi-184Y0
22483-Bi-186X170
22583-Bi-188X153
22683-Bi-190X0
22783-Bi-190Y130
22883-Bi-191X49.9
22983-Bi-194X180
23083-Bi-194Y150
23183-Bi-197X42.6
23283-Bi-198X280
23383-Bi-199X24.7
23483-Bi-200X100
23583-Bi-201X39.7
23683-Bi-202X20
23783-Bi-215X19.5
23883-Bi-216X24
23983-Bi-217X44
24084-Po-198X48.14
24184-Po-200X12.5
24284-Po-202X20.5
24385-At-192X40
24485-At-192Y0
24585-At-194X0
24685-At-194Y40
24785-At-198X82
24885-At-199X244
24985-At-202X190
25085-At-213X51.9
25185-At-213Y54
25286-Rn-197X199
25386-Rn-200X19.5
25486-Rn-201X280
25586-Rn-205X657.1
25686-Rn-210X45.4
25786-Rn-211X25.2
25886-Rn-212X6.6
25986-Rn-213X46
26086-Rn-213Y51
26187-Fr-198X0
26287-Fr-198Y50
26387-Fr-201X127
26487-Fr-202X274
26587-Fr-206X190
26687-Fr-214Y103
26787-Fr-216X219
26888-Ra-201X263
26988-Ra-203X190
27088-Ra-205X300
27188-Ra-215X53.4
27289-Ac-206X220
27389-Ac-215X52
27489-Ac-216X98
27589-Ac-218Y145.51
27689-Ac-222X200
27790-Th-209X470
27890-Th-215X48.7
27990-Th-217X55.09
28091-Pa-234X5.08
28192-U-239X20
28293-Np-236X60
28393-Np-240X18
28493-Np-242Y50
28595-Am-236X50
28695-Am-244X200
28795-Am-244Y201
28895-Am-246X30
28996-Cm-244X1100
29097-Bk-242Y200
29197-Bk-244X500
29297-Bk-245X50
29397-Bk-248X30
29497-Bk-248Y50
29597-Bk-248Z0
29699-Es-245X330
29799-Es-246X0
29899-Es-250X200
29999-Es-256X100
300100-Fm-250X1199.2
301100-Fm-253X140
302101-Md-246X0
303101-Md-246Y60
304101-Md-247X260
305101-Md-249X100
306101-Md-254X50
307101-Md-258X200
308102-No-251X50.3
309102-No-253X1200
310102-No-254Y905.2
311102-No-257X300
312103-Lr-253Y30
313103-Lr-255Y54
314104-Rf-253X0
315104-Rf-253Y200
316104-Rf-254X1300
317104-Rf-254Y2000
318104-Rf-259X60
319105-Db-258X60
320105-Db-262X50
321107-Bh-262X0
322107-Bh-262Y210
323109-Mt-276X250
324110-Ds-271X68
325110-Ds-279X0
326110-Ds-281X0
327111-Rg-279X0
328112-Cn-285X0
329114-Fl-289X0
Nuclides where one or
more "+X" bands were removed.
# Nuclide Band
010-Ne-28X
112-Mg-35Y
212-Mg-35X
313-Al-38X
414-Si-39X
518-Ar-36X
618-Ar-43X
719-K-48X
821-Sc-52X
926-Fe-63X
1027-Co-70Y
1128-Ni-58X
1228-Ni-59Y
1328-Ni-59X
1428-Ni-59Z
1529-Cu-59X
1629-Cu-61Y
1729-Cu-61X
1830-Zn-60X
1930-Zn-60Y
2030-Zn-65X
2130-Zn-65Z
2230-Zn-65Y
2330-Zn-68X
2431-Ga-84X
2532-Ge-65X
2632-Ge-68X
2735-Br-69X
2835-Br-76X
2937-Rb-76X
3037-Rb-100X
3138-Sr-80Y
3238-Sr-80U
3338-Sr-80X
3438-Sr-80Z
3538-Sr-81Z
3638-Sr-81X
3738-Sr-81Y
3838-Sr-82X
3938-Sr-83X
4039-Y-81X
4139-Y-82X
4239-Y-83U
4339-Y-83X
4439-Y-83Y
4539-Y-83Z
4639-Y-84V
4739-Y-84Z
4839-Y-84U
4940-Zr-81X
5040-Zr-83Z
5140-Zr-83X
5240-Zr-83Y
5340-Zr-86Y
5440-Zr-86X
5540-Zr-86U
5640-Zr-86Z
5741-Nb-85X
5841-Nb-85Z
5941-Nb-86X
6041-Nb-87X
6141-Nb-87Z
6241-Nb-87Y
6341-Nb-100Y
6441-Nb-102Z
6541-Nb-102Y
6642-Mo-85Y
6742-Mo-85X
6842-Mo-88Z
6942-Mo-88Y
7042-Mo-88X
7142-Mo-88U
7243-Tc-88Z
7343-Tc-89X
7443-Tc-90Y
7543-Tc-91X
7643-Tc-106X
7743-Tc-107X
7843-Tc-108X
7945-Rh-102X
8045-Rh-102Y
8145-Rh-118X
8246-Pd-103X
8346-Pd-104X
8446-Pd-105X
8547-Ag-96Z
8647-Ag-105X
8747-Ag-110X
8847-Ag-112Y
8947-Ag-112X
9047-Ag-114X
9147-Ag-114Y
9247-Ag-116X
9347-Ag-126Z
9448-Cd-104X
9548-Cd-106X
9648-Cd-107X
9748-Cd-108Y
9848-Cd-108X
9948-Cd-109X
10048-Cd-125Y
10148-Cd-127Y
10249-In-100X
10349-In-109X
10449-In-111Y
10549-In-111X
10649-In-113Y
10749-In-113X
10849-In-121X
10950-Sn-102X
11050-Sn-106X
11150-Sn-106Y
11250-Sn-106Z
11350-Sn-108X
11450-Sn-115X
11551-Sb-107Y
11651-Sb-107X
11751-Sb-109Z
11851-Sb-109Y
11951-Sb-109W
12051-Sb-109X
12151-Sb-110X
12251-Sb-110Y
12351-Sb-111X
12451-Sb-111Y
12551-Sb-112Y
12651-Sb-112X
12751-Sb-114Y
12851-Sb-114X
12951-Sb-122X
13051-Sb-125X
13152-Te-110U
13252-Te-110Z
13352-Te-110X
13452-Te-110Y
13552-Te-110V
13652-Te-112X
13752-Te-112Z
13852-Te-112Y
13952-Te-113X
14052-Te-125X
14153-I-109X
14253-I-110X
14353-I-112X
14453-I-113X
14553-I-113Y
14653-I-113U
14753-I-113W
14853-I-113V
14953-I-113Z
15053-I-114X
15153-I-115W
15253-I-115V
15353-I-115Z
15453-I-115Y
15553-I-115X
15653-I-116X
15753-I-118X
15853-I-119X
15953-I-120X
16053-I-121X
16153-I-130X
16253-I-140X
16354-Xe-116Y
16454-Xe-116Z
16554-Xe-116X
16654-Xe-117Y
16754-Xe-117X
16854-Xe-123X
16954-Xe-125X
17054-Xe-125Z
17154-Xe-125Y
17254-Xe-125U
17354-Xe-126X
17455-Cs-112X
17555-Cs-114X
17655-Cs-116X
17755-Cs-119Y
17855-Cs-121X
17955-Cs-125X
18055-Cs-128X
18155-Cs-140X
18255-Cs-142X
18355-Cs-144X
18456-Ba-119X
18556-Ba-119Y
18656-Ba-122X
18756-Ba-126X
18857-La-121X
18957-La-121Y
19057-La-123Y
19157-La-123X
19257-La-124X
19357-La-124Y
19457-La-125Y
19557-La-125X
19657-La-126Y
19757-La-129X
19857-La-130Z
19957-La-130Y
20057-La-130X
20157-La-134Y
20258-Ce-123Z
20358-Ce-123Y
20458-Ce-123X
20558-Ce-125Y
20658-Ce-125X
20758-Ce-129X
20858-Ce-129Y
20958-Ce-130Z
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