Challenges in Nuclear Data Program Evaluation and Remedies

 
Texas A&M University
US Nuclear Data Program
 
 
TAMU NSDD CENTER
 Evaluation Issues
 
N. Nica
 
1. Case study for typical EC decay cases
 
Typical case of a beta decay to an
isomer of unknown energy
Favored 11/2- to 11/2- 
ε
+
 decay,
Q(
ε
)=10630 keV
Other two lower levels known, of which one
is the g.s., unfavored for the 
ε
+
 decay
The decay goes to a level 5000 ± 5000 keV
The decay drawing is not drawing the range,
so it is confusing!
Remedies ???
1. Case study for typical EC decay cases
 
Typical case of a beta decay to an isomer of
unknown energy
Favored 11/2- to 11/2- 
ε
+
 decay, Q(
ε
)=10630
keV
Other two lower levels known, of which one is
the g.s., unfavored for the 
ε
+
 decay
The decay goes to a level 5000 ± 5000 keV
The decay drawing is not drawing the range, so
it is confusing!
Remedy 1
: 
Remove the 
ε
+
 table
The 
ε
+
 decay does exist and so the 11/2-
level, even if its energy is not known
Not shown the level it would be more
confusing, even wrong
 
1. Case study for typical EC decay cases
 
Typical case of a beta decay to an isomer of
unknown energy
Favored 11/2- to 11/-2 
ε
 decay fot Q(
ε
)=10630
keV
Other two lower levels known, of which one is
the g.s. unfavored for the 
ε
 decay
The decay goes to a level 5000 ± 5000 keV
The decay drawing is not drawing the range, so
it is confusing!
Remedy 2:
 Redesignate 
(5
10
3 
 
5
) 
level
Maintain the 
ε
+
 table
Rename the level as:
      147ER  E 10630-X
That would restore the correctness and good
sense
However, it should be checked:
Whether it can be implemented in JAVA-NDS
(also fmtchk should be modified to accept the
change)
Whether other unwanted effects are propagated
on other codes
 
 
 
 
2. A beta-delayed particle decay ambiguity
 
Remedy 1
Following publications notations 
P
1n
, P
2n
%
 
-
1n, 
%
 
-
2n
can be acceptable form for the respective probabilities (as for evaluator in
example 2)
This in turn would made available the notation
%
 
-
n
to be used for indicating the 
“total delayed-neutron decay”.
However, that would consequently demand the systematic
replacement of all 
%
 
-
n 
of with 
%
 
-
1n.
That would be a greater problem than the one here scrutinized
Remedy 2
Fortunately, there is a simple solution for the ambiguity:
Keep
 
%
 
-
n, 
%
 
-
2n 
unchanged for beta-delayed –one and –two
neutrom decays
For the 
“total delayed-neutron decay” 
use instead the new notation:
 
%
 
-
n
        that would need to replace only the fewer cases of such occurrences
For the beta-delayed proton emission use the corresponding notations
       %
 
+
p, 
%
 
+
2p, 
%
 
+
p
Example 1
Example 2
 
 
 
 
%
 
+
p
 
%
 
+
1p
 
%
 
-
n
 
%
 
-
1n
 
%
 
-
1n
3. The S(n)+x, S(2n)+y range situation
 
 
L 3759.6    9  (1/2+,3/2+,5/2+)                                         ?
 
L 2312+X                                                                      R
 
L 8652+Y                                                                      R
4. Extend the capability of JAVA_RULER
 
PROPOSAL, 
based on JAVA-RULER’s the key
feature 
“calculate ICC by BrIcc”
“calculate ICC by BrIcc”
Design a new button (unless is already done
but I ignored its existence) to analyze each 
γ
transition with incomplete information and
get the RUL comparisons for these situations:
If 
γ
 rays are assigned  D, or Q, or higher
multipoles, 
JAVA-RULER can run the possible
case scenarios, e.g., E2 vs. M2, E1 vs. M1, etc.,
combining 
’s if known
If no 
 is assigned, JAVA-RULER can calculate
RUL comparisons for 
=0
If no 
multipoles are assigned, 
JAVA-RULER
can calculate all combinations for 
Δ
J=1 to 4.
If BR is not known, JAVA-RULER can
calculate
 RUL comparisons for BR=1
The corresponding JAVA-RULER output will
contain only the 
γ 
transition with incomplete
information.
 
 
 
 
RULER can be used to discriminate
between different gamma-ray multipolarities
when T
1/2 
is known as value or limit
However, RULER is able to output the
“Recommended Upper Limits (RUL)
comparisons with calculated B(XL)(W.u.)”
only if all needed parameters are known
(T
1/2 
, A, E
γ
, BR, 
, 
).
Tom Burrows recommended to rerun
RULER for a given transition by varying the
different E
’s / M
’s
However, changing parameters and
rerunning the code especially when looking
to test for multiple 
γ
’s is tedious and time
consuming
 
 
 
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Exploring evaluation challenges in a nuclear data program, including issues with decay cases and ambiguous notations. Remedies such as redesignating levels and clarifying decay probabilities are discussed to address these challenges.

  • Nuclear Data
  • Evaluation Issues
  • Remedies
  • Decay Cases
  • Notation Ambiguity

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  1. Texas A&M University US Nuclear Data Program TAMU NSDD CENTER Evaluation Issues N. Nica

  2. 1. Case study for typical EC decay cases Typical case of a beta decay to an isomer of unknown energy Favored 11/2- to 11/2- + +decay, Q( )=10630 keV Other two lower levels known, of which one is the g.s., unfavored for the + +decay The decay goes to a level 5000 5000 keV The decay drawing is not drawing the range, so it is confusing! Remedies ???

  3. 1. Case study for typical EC decay cases Typical case of a beta decay to an isomer of unknown energy Favored 11/2- to 11/2- + +decay, Q( )=10630 keV Other two lower levels known, of which one is the g.s., unfavored for the + +decay The decay goes to a level 5000 5000 keV The decay drawing is not drawing the range, so it is confusing! Remedy 1: Remove the , +table The + +decay does exist and so the 11/2- level, even if its energy is not known Not shown the level it would be more confusing, even wrong

  4. 1. Case study for typical EC decay cases Typical case of a beta decay to an isomer of unknown energy Favored 11/2- to 11/-2 decay fot Q( )=10630 keV Other two lower levels known, of which one is the g.s. unfavored for the decay The decay goes to a level 5000 5000 keV The decay drawing is not drawing the range, so it is confusing! Remedy 2: Redesignate (5 103 5) level Maintain the + +table Rename the level as: 147ER E 10630-X That would restore the correctness and good sense However, it should be checked: Whether it can be implemented in JAVA-NDS (also fmtchk should be modified to accept the change) Whether other unwanted effects are propagated on other codes

  5. 2. A beta-delayed particle decay ambiguity Remedy 1 Example 1 Following publications notations P1n, P2n % -1n, % -2n % +1p can be acceptable form for the respective probabilities (as for evaluator in example 2) This in turn would made available the notation % -n % +p to be used for indicating the total delayed-neutron decay . Example 2 However, that would consequently demand the systematic replacement of all % -n of with % -1n. That would be a greater problem than the one here scrutinized Remedy 2 Fortunately, there is a simple solution for the ambiguity: Keep % -n, % -2n unchanged for beta-delayed one and two neutrom decays For the total delayed-neutron decay use instead the new notation: % - n that would need to replace only the fewer cases of such occurrences % -1n For the beta-delayed proton emission use the corresponding notations % +p, % +2p, % + p % -1n % -n

  6. 3. The S(n)+x, S(2n)+y range situation L 3759.6 9 (1/2+,3/2+,5/2+) ? L 2312+X R L 8652+Y R

  7. 4. Extend the capability of JAVA_RULER PROPOSAL, based on JAVA-RULER s the key feature calculate ICC by BrIcc Design a new button (unless is already done but I ignored its existence) to analyze each transition with incomplete information and get the RUL comparisons for these situations: If rays are assigned D, or Q, or higher multipoles, JAVA-RULER can run the possible case scenarios, e.g., E2 vs. M2, E1 vs. M1, etc., combining s if known If no is assigned, JAVA-RULER can calculate RUL comparisons for =0 If no multipoles are assigned, JAVA-RULER can calculate all combinations for J=1 to 4. If BR is not known, JAVA-RULER can calculate RUL comparisons for BR=1 The corresponding JAVA-RULER output will contain only the transition with incomplete information. RULER can be used to discriminate between different gamma-ray multipolarities when T1/2 is known as value or limit However, RULER is able to output the Recommended Upper Limits (RUL) comparisons with calculated B(XL)(W.u.) only if all needed parameters are known (T1/2 , A, E , BR, , ). Tom Burrows recommended to rerun RULER for a given transition by varying the different E s / M s However, changing parameters and rerunning the code especially when looking to test for multiple s is tedious and time consuming

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