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A new approach to estimating the probability for delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven National Laboratory, NY USA

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Page 1: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

A new approach to estimating the probability for delayed neutron emission

E. A. McCutchanA.A. SonzogniT.D. Johnson

National Nuclear Data CenterBrookhaven National Laboratory, NY USA

Page 2: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

Outline

• Motivation

• Traditional systematics

• A new parameterization

• A closer look

Page 3: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

-delayed neutrons and their use

• Reactor control and post-processing of fuel

• r-process nucleosynthesis and abundances

• Basic structure physics

Page 4: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

214 nuclei with measured Pn values

http://www.nndc.bnl.gov/nudat2

Relevance of reliable systematics

Page 5: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

Some terminology

AZ+1

Q

AZ

Sn

A-1Z+1

Qn

n

Pn : the probability to emit a neutron following decay

Page 6: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

6

Kratz -Herrmann Formula (KHF)

𝑃𝑛≈𝑎 [𝑄 𝛽−𝑆𝑛

𝑄𝛽−𝐶 ]𝑏

Cut off parameter C (MeV)

𝐶=0𝐶=

13

√𝐴𝐶=

26

√𝐴

even-even

even-odd

odd-odd

Traditional systematic studies

K.-L. Kratz and G. Herrmann, Z. Phys. A 263, 435 (1973)

Two parameter fit with ‘a’ and ‘b’

Log-log plot gives straight linewith slope=b

Page 7: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

B. Pfeiffer et al., Prog. Nucl. Energy 41, 39 (2002).

The standard for systematic studies

Linear regression

Weighted least-squares

a = 106(38)b = 5.5(6)

red 2 = 81

Page 8: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

a = 119(42)b = 5.45(48)red 2 = 146

Audi and Meng (2011)

Effect of improved Q values

a = 106(38)b = 5.5(6)

red 2 = 81

Masses from :Audi and Wapstra (1995)

Page 9: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

A better parameterization?

Strength function Fermi integral

𝑃𝑛

𝑇1 /2𝑎(𝑄 𝛽𝑛)

𝑏

Applying same concept as KHF

Page 10: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

A more compact trajectory

a = 0.0097(9)b = 4.87(7)red 2 = 35

a = 119(42)b = 5.45(48)red 2 = 146

Light fission fragment region

Page 11: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

Heavy fission fragment region

a = 141(48)b = 5.08(37)red 2 = 78

a = 0.016(2)b = 4.55(13)red 2 = 55

A more compact trajectory

Page 12: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

A surprising correlation

a = 45(6)b = 4.4(4)

red 2 = 280

a = 0.037(9)b = 4.11(9)red 2 = 87

Light nuclei, Z <26

Page 13: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

A closer lookLight fission fragment region

• Very linear trend• Few outliers

100Rb102Rb

Page 14: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

A closer lookHeavy fission fragment region

• Few outliers• Less linear trend• Possible shell

effects?

Page 15: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

How do we do ??

KHF-2002: B. Pfeiffer et al., Prog. Nucl. Energy 41, 39 (2002).QRPA-1: P. Moller et al., Phys. Rev. C 67, 055802 (2003).

Page 16: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

Another surprising correlation

P. Moller et al., Phys. Rev. C 67, 055802 (2003).

Page 17: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

Summary

• New prescription for systematics of Pn values

• Ratio of Pn to T1/2

• More compact trajectory

• Works across nuclear chart

• For the future

• Extract information about strength function from slope ??

Page 18: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

Relevance to ENSDF

• Some evaluators give Pfeiffer KHF results (2002Pf04) for cases where Pn has not been measured

• Should we replace with values from new systematics ?

Page 19: A new approach to estimating the probability for  delayed neutron emission E. A. McCutchan A.A. Sonzogni T.D. Johnson National Nuclear Data Center Brookhaven

Another surprising correlation

P. Moller et al., Phys. Rev. C 67, 055802 (2003).