Alpha-Decay Hindrance Factors. Program ALPHAD. Edgardo Browne Decay Data Evaluation Project Workshop May 12 - PowerPoint PPT Presentation

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Alpha-Decay Hindrance Factors. Program ALPHAD. Edgardo Browne Decay Data Evaluation Project Workshop May 12

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The probability of a decay depends on the: Energy of the a particle ... is from 'The Theory of Alpha Radioactivity,' M.A. Preston, Phys. Rev. 71, 865 (1947! ... – PowerPoint PPT presentation

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Title: Alpha-Decay Hindrance Factors. Program ALPHAD. Edgardo Browne Decay Data Evaluation Project Workshop May 12


1
Alpha-Decay Hindrance Factors.Program
ALPHAD.Edgardo BrowneDecay Data Evaluation
Project WorkshopMay 12 14, 2008Bucharest,
Romania
2
  • The probability of a decay depends on the
  • Energy of the a particle
  • Parent and daughter nuclear structure
    configurations
  • A useful definition of hindrance factor is
  • HF T1/2(a) exp./T1/2(a) theor.
  • Notice that T1/2(a) T1/2/ a branching.
  • HF depends only on the nuclear structure
    configurations. The energy dependence has been
    removed.
  • T1/2(a) theor. is from The Theory of Alpha
    Radioactivity, M.A. Preston, Phys. Rev. 71, 865
    (1947!!)

3
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4
HF(0 to 0, even-even nucleus) 1by
definition. All other hindrance factors are
relative to this value.Hindrance factors for
odd-A and odd-odd nuclei are relative to HF
values for the 0 to 0 a transitions in the
neighboring even-even nuclei
5
The Radius Parameter r0
  • This parameter is roughly equivalent to the
    nuclear radius, and it may be determine for each
    nucleus from the 0 to 0 a transition in
    even-even nuclei, and assuming HF1.
  • See Review of Alpha-Decay Data from Doubly-Even
    Nuclei, Y.A. Akovali, Nucl. Data Sheets 84, 1
    (1998).

6
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7
Favored alpha-particle transition in odd-A nuclei
  • If HF lt 4 then initial and final levels have the
    same spin (J) and parity (p).

8
The radius parameter r0(Y. Akovali, Oak Ridge)
  • Odd-N nucleus (Z, A)
  • r0(Z, N) r0(Z, N-1) r0(Z, N1)/2
  • Odd-Z nucleus (Z, A)
  • r0(Z, N) r0(Z-1, N) r0(Z1, N)/2
  • Odd-Odd nucleus (Z, A)
  • r0(Z, N) r0(Z, N-1) r0(Z, N1)/2
  • r0(Z-1, N1)r0(Z-1, N-1)r0(Z1, N1) r0(Z1,
    N-1)/4

9
Example
219Rn ?215Po (Odd-N) r0 (Z84, N131)
r0(84, 130) r0(84, 132) /2 From
1998Ak04 r0(84,214) 1.559 8 r0(84,216)
1.5555 2, therefore
r0 (Z84, N131) 1.557 Use Table 1
Calculated r0 for even-even nuclei (1998Ak04).
Insert R0 in comment record
CA HF R0 Run program ALPHAD to
calculate hindrance factors. HF(401 keV) 3.4
(Favored a decay).
10
Estimating an a-decay branching
0
9 ms
210Th
a
90
?
2
474
0
0
100 HF1
206Ra
88
11
HF Systematic for Even-even Thorium Nuclei
  • Parent nucleus Jp Daughter nucleus Jp
    HF
  • 210Th 0 206Ra
    2 ?
  • 228Th 0 224Ra
    2 0.92
  • 230Th 0 226Ra
    2 1.1
  • 232Th 0 228Ra
    2 1.0
  • We expect HF(210Th) 1

12
Computer Program ALPHAD

Z A
90. 210.
Q ALPHA E TOTAL ALPHA HALF
LIFE RADIUS RZERO TOTAL HALF LIFE
ALPHA BRANCH 8.0530 8.0881 1.042E-07
D 9.0867E-13 1.5386 9.000E-03 S
1.000E00
ENERGY LEVEL
ABUNDANCE CALC. HALF LIFE HINDRANCE FACTOR
0.00 1.00E00 1.04E-07
1.00E00 474.00 1.00E-01 3.35E-06
3.11E-01 474.00 5.00E-02
3.35E-06 6.22E-01 474.00 3.00E-02
3.35E-06 1.04E00 474.00
1.00E-02 3.35E-06 3.11E00 474.00
5.00E-03 3.35E-06 6.22E00
474.00 3.00E-03 3.35E-06
1.04E01 474.00 1.00E-03 3.35E-06
3.11E01 474.00 1.00E-04
3.35E-06 3.11E02
So a(474) 3
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