Improving systematic predictions of  -delayed neutron emission probabilities E. A. McCutchan A.A. Sonzogni T.D. Johnson NNDC D. Abriola IAEA M. Birch,

Slides:



Advertisements
Similar presentations
NUCLEAR REACTION MODELS FOR SYSTEMATIC ANALYSIS OF FAST NEUTRON INDUCED (n,p) REACTION CROSS SECTIONS M.Odsuren, J.Badamsambuu, G.Khuukhenkhuu Nuclear.
Advertisements

 -Ray Emission Probabilities Edgardo Browne Decay Data Evaluation Project Workshop May 12 – 14, 2008 Bucharest, Romania.
The r-Process Nearly four decades have passed since the r-process was postulated. The nature of the distribution of heavy elements in the solar system.
International Atomic Energy Agency The IAEA’s Commitment to Nuclear Structure and Decay Data Paraskevi (Vivian) Demetriou Nuclear Data Section, Division.
ROGER CABALLERO FOLCH, Barcelona, 9 th November 2011.
ISOLDE workshop, CERN, November 2008 Correlations between nuclear masses, radii and E0 transitions P. Van Isacker, GANIL, France Simple nuclear mass formulas.
Nuclear equation of state in form suitable for quantum molecular dynamics model 1.Brief indroduction of the EOS prescription 2.New form for bullk and surface.
Neurons layered ANNs are structures, inspired from the corresponding biological neural systems, that consist of interconnected processing units (called.
The Atomic Mass Evaluation: Present and Future WANG Meng Institute of Modern Physics, CAS ARIS2014, Tokyo, June 2.
9/28/ :01 (00) PAIRING PROPERTIES OF SUPERHEAVY NUCLEI A. Staszczak, J. Dobaczewski and W. Nazarewicz (KFT UMCS) (IFT UW) (ORNL & UT)
THE BIG DIP experimental and systematic discussions of neutron binding in very neutron-rich nuclides William B. Walters Department of Chemistry University.
 What are the appropriate degrees of freedom for describing fission of heavy nuclei (171 ≤ A ≤ 330)?  Fission barrier heights for 5239 nuclides between.
Recycling NuDat Programs A.A. Sonzogni, T.D. Johnson, E.A. McCutchan, National Nuclear Data Center Brookhaven National Laboratory Building 817 Upton, NY.
Proton and Two-Proton Decay of a High-Spin Isomer in 94 Ag Ernst ROECKL GSI Darmstadt and Warsaw University.
Compilation and Evaluation of Beta-Delayed Neutron emission probabilities and half-lives of precursors in the Non-Fission Region (A ≤ 72) M. Birch and.
International Atomic Energy Agency Nuclear Data Development and Dissemination at IAEA Paraskevi (Vivian) Dimitriou Nuclear Data Section, Division of Physical.
Boris Pritychenko Nuclear Physics Data Compilation for Nucleosynthesis Modeling, Trento, May 29 – June 1, 2007 MACS and Astrophysical Reaction Rates from.
Role of mass asymmetry in fusion of super-heavy nuclei
Reactor Antineutrino Anomaly
1 TCP06 Parksville 8/5/06 Electron capture branching ratios for the nuclear matrix elements in double-beta decay using TITAN ◆ Nuclear matrix elements.
Stats for Engineers Lecture 9. Summary From Last Time Confidence Intervals for the mean t-tables Q Student t-distribution.
Futoshi Minato JAEA Nuclear Data Center, Tokai Theoretical calculations of beta-delayed neutrons and sensitivity analyses 1.
Oslo, May 21-24, Systematics of Level Density Parameters Till von Egidy, Hans-Friedrich Wirth Physik Department, Technische Universität München,
Nuclear Data and Applications
Aim  to compare our model predictions with the measured (Dubna and GSI) evaporation cross sections for the 48 Ca Pb reactions. Calculations.
D.Bucurescu, T. von Egidy, Level density, spin distribution-Ohio, July Nuclear Level Densities and Spin Distributions Dorel Bucurescu National Institute.
Α - capture reactions using the 4π γ-summing technique Α. Lagoyannis Institute of Nuclear Physics, N.C.S.R. “Demokritos”
International Atomic Energy Agency D. Abriola Nuclear Data Section Department of Nuclear Sciences and Applications 20 th NSDD Meeting, Kuwait, Jan
Beatriz Jurado, Karl-Heinz Schmidt CENBG, Bordeaux, France Supported by EFNUDAT, ERINDA and NEA The GEneral Fission code (GEF) Motivation: Accurate and.
A=193 Mass Chain evaluation: A summary IAEA-ICTP Workshop on Nuclear Structure and Decay Data: Theory and Evaluation, Trieste, Italy November
Structures of Exotic 131,133 Sn Isotopes for r-process nucleosynthesis Shisheng Zhang 1,2 ( 张时声 ) 1. School of Physics and Nuclear Energy Engineering,
Status Report: McMaster University Feb 1, 2013 to April 17, 2015 Balraj Singh Department of Physics and Astronomy McMaster University (Retired June 30,
Agenda Structure Group Discussions NSDD/ENSDF Long Range Planning: (Monday Afternoon) – Priorities and characterization of user base What is the.
Completed compilation and evaluation of experimental Pn and half-lives for nuclei in Z=2-28 region Balraj Singh (McMaster University, Canada) 2 nd RCM.
Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.
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.
Beta Delayed Neutron Covariances Tim Johnson, Libby McCutchan, Alejandro Sonzogni National Nuclear Data Center.
B. Singh and M. Birch 02/05/2013Beta-Delayed Neutron Data Evaluation Compilation and Evaluation of %P n and T 1/2 Data for β-delayed Neutron Emitters Balraj.
JAVA-GAMUT and V.AveLib Update Michael Birch – Presented by Balraj Singh McMaster University, Canada IAEA-NSDD Meeting, Vienna April 20-24, 2015.
Incomplete fusion studies near Coulomb barrier Pragya Das Indian Institute of Technology Bombay Powai, Mumbai , India.
Anti-neutrinos Spectra from Nuclear Reactors Alejandro Sonzogni National Nuclear Data Center.
International Atomic Energy Agency D. Abriola Nuclear Data Section Department of Nuclear Sciences and Applications 20 th NSDD Meeting, Kuwait, Jan
Korea Atomic Energy Research Institute (KAERI) Jounghwa Lee 21st NSDD Meeting, Vienna, Austria, April 2015.
Application Nuclear Data Needs
Fundamental Interactions Physics & Instrumentation Conclusions Conveners: P. Mueller, J. Clark G. Savard, N. Scielzo.
R-process experiments at the National Superconducting Cyclotron Laboratory Giuseppe Lorusso NSCL at Michigan State university.
Alejandro SonzogniNSDD 2007 Decay Data Library In ENDF/B-VII Alejandro Sonzogni National Nuclear Data Center Brookhaven National Laboratory
International Atomic Energy Agency IAEA Nuclear Data Section ENSDF Activities D. Abriola International Atomic Energy Agency, Vienna, Austria 17 th Meeting.
Ning Wang An improved nuclear mass formula Guangxi Normal University, Guilin, China KITPC , Beijing.
Nuclear Structure SnSn P,n p n (  )‏ ( ,Xn)‏ M1E1 p,nn X λ ?E1 ExEx  Study of the pygmy dipole resonance as a function of deformation.
Production and beta decay lifetimes of heavy neutron-rich nuclei approaching the r-process path Teresa Kurtukian-Nieto Universidad de Santiago de Compostela.
Structure of Super-Heavy Elements Andreas Heinz A. W. Wright Nuclear Structure Laboratory Yale University ATLAS Workshop, August 8-9, 2009.
July 29-30, 2010, Dresden 1 Forbidden Beta Transitions in Neutrinoless Double Beta Decay Kazuo Muto Department of Physics, Tokyo Institute of Technology.
TAGS data in ENDF/B-VII.1 and ENDF/B-VII.1.1 A.A. Sonzogni, T.D. Johnson, E.A. McCutchan, National Nuclear Data Center.
Shape evolution of highly deformed 75 Kr and projected shell model description Yang Yingchun Shanghai Jiao Tong University Shanghai, August 24, 2009.
First Gogny conference, TGCC December 2015 DAM, DIF, S. Péru QRPA with the Gogny force applied to spherical and deformed nuclei M. Dupuis, S. Goriely,
Nuclear Structure Data Needs Filip G. Kondev Collaborative meeting, Trento, May 28 –June 1, 2007 Outline  What kind of nuclear structure.
The i 13/2 Proton and j 15/2 Neutron Orbital and the SD Band in A~190 Region Xiao-tao He En-guang Zhao En-guang Zhao Institute of Theoretical Physics,
Global fitting of pairing density functional; the isoscalar-density dependence revisited Masayuki YAMAGAMI (University of Aizu) Motivation Construction.
Multi-particle emission H.O.U. Fynbo Department of Physics, University ofAarhus, Denmark Symposium on Approaching the Drip-line for Unstable Nuclei Budapest.
Present Status of AME and NUBASE Meng WANG CSNSM, Orsay, France IMP,Lanzhou,China April 6, 2011, Vienna.
Example of Evaluation: Decay of 177 Lu (6.647 d) Filip G. Kondev 2 nd Workshop for DDEP Evaluators, Bucharest, Romania May 12-15,2008.
Systematical Analysis of Fast Neutron Induced Alpha Particle Emission Reaction Cross Sections Jigmeddorj Badamsambuu, Nuclear Research Center, National.
1 Atomic Mass Evaluation Meng WANG (王猛) CSNSM-CNRS, France MPIK-Heidelberg, Germany IMP-CAS, China 5 th FCPPL workshop.
超重原子核的结构 孙 扬 上海交通大学 合作者:清华大学 龙桂鲁, F. Al-Khudair 中国原子能研究院 陈永寿,高早春 济南,山东大学, 2008 年 9 月 20 日.
NNDC Services B. Pritychenko National Nuclear Data Center, Brookhaven National Laboratory, Upton, NY , USA.
Unblocking of the Gamow-Teller Strength for Stellar Electron Capture
Nuclear Data for Reactor Fluxes
Symmetry energy coefficients and shell gaps from nuclear masses
Kazuo MUTO Tokyo Institute of Technology
Presentation transcript:

Improving systematic predictions of  -delayed neutron emission probabilities E. A. McCutchan A.A. Sonzogni T.D. Johnson NNDC D. Abriola IAEA M. Birch, B. Singh McMaster

Beta-delayed neutron emission A Z+1 QQ AZAZ SnSn A-1 Z+1 QnQn  n What is it ? P n : the probability to emit a neutron following  decay

214 nuclei with measured P n values Beta-delayed neutron emission Where is it ?

Beta-delayed neutron emission Why do we care? Reactor control and post-processing of fuel r-process nucleosynthesis and abundances Basic structure physics

5 Kratz -Herrmann Formula (KHF) Cut off parameter C (MeV) 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 line with slope=b

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

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)

A better parameterization? Strength function Fermi integral Applying same concept as KHF

With this approach a = (9) b = 4.87(7) red  2 = 35 a = 119(42) b = 5.45(48) red  2 = 146

A surprising correlation a = 45(6) b = 4.4(4) red  2 = 280 a = 0.037(9) b = 4.11(9) red  2 = 87

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, (2003).

Summary New prescription for systematics of P n values Ratio of P n to T 1/2 More compact trajectory Seems to work across nuclear chart

Relevance to ENSDF Some evaluators give Pfeiffer KHF results (2002Pf04) for cases where P n has not been measured Should we replace with values from new systematics ?

Another surprising correlation P. Moller et al., Phys. Rev. C 67, (2003).