Systematical Analysis of Fast Neutron Induced Alpha Particle Emission Reaction Cross Sections Jigmeddorj Badamsambuu, Nuclear Research Center, National.

Slides:



Advertisements
Similar presentations
Neutron-induced Reactions
Advertisements

Compound Nucleus Reactions
? Nuclear Reactions Categorization of Nuclear Reactions
Accelerator Physics, JU, First Semester, (Saed Dababneh).
CHAPTER 22 Nuclear Chemistry
Measurements of Angular and Energy Distributions of Prompt Neutron Emission from Thermal Induced Fission Vorobyev A.S., Shcherbakov O.A., Gagarski A.M.,
M3.1 JYFL fission model Department of Physics, University of Jyväskylä, FIN-40351, Finland V.G. Khlopin Radium Institute, , St. Petersburg, Russia.
NUCLEAR REACTION MODELS FOR SYSTEMATIC ANALYSIS OF FAST NEUTRON INDUCED (n,p) REACTION CROSS SECTIONS M.Odsuren, J.Badamsambuu, G.Khuukhenkhuu Nuclear.
Microscopic time-dependent analysis of neutrons transfers at low-energy nuclear reactions with spherical and deformed nuclei V.V. Samarin.
Kazimierz What is the best way to synthesize the element Z=120 ? K. Siwek-Wilczyńska, J. Wilczyński, T. Cap.
Course Title: Nuclear Physics Course Code: EEE-202
RFSS: Lecture 9 Nuclear Reactions
Nuclear / Subatomic Physics Physics – Chapter 25 (Holt)
Direct Reactions. Optical model Represent the target nucleus by a potential -- Attenuation length.
 -decay theory.  -particle penetration through Coulomb Barrier Goal: estimate the parent lifetime for  -decay Assume an  -particle is formed in the.
Nuclear models. Models we will consider… Independent particle shell model Look at data that motivates the model Construct a model Make and test predictions.

Nuclear and Radiation Physics, BAU, 1 st Semester, (Saed Dababneh). 1 Nuclear Reactions Categorization of Nuclear Reactions According to: bombarding.
A. Dokhane, PHYS487, KSU, 2008 Chapter2- Nuclear Fission 1 Lecture 3 Nuclear Fission.
25 9. Direct reactions - for example direct capture: Direct transition from initial state |a+A> to final state B +  geometrical.
Lecture 10 Energy production. Summary We have now established three important equations: Hydrostatic equilibrium: Mass conservation: Equation of state:
Nuclear and Radiation Physics, BAU, 1 st Semester, (Saed Dababneh). 1 Nuclear Binding Energy B tot (A,Z) = [ Zm H + Nm n - m(A,Z) ] c 2 B  m.
6.1 The Atomic Models of Thomson and Rutherford 6.2 Definition of Cross Section 6.2 Rutherford Scattering 6.3 Structure of the Nucleus Rutherford Scattering.
Oslo, May 21-24, Systematics of Level Density Parameters Till von Egidy, Hans-Friedrich Wirth Physik Department, Technische Universität München,
The study of fission dynamics in fusion-fission reactions within a stochastic approach Theoretical model for description of fission process Results of.
Aim  to compare our model predictions with the measured (Dubna and GSI) evaporation cross sections for the 48 Ca Pb reactions. Calculations.
Α - capture reactions using the 4π γ-summing technique Α. Lagoyannis Institute of Nuclear Physics, N.C.S.R. “Demokritos”
Transmutation of Spent Nuclear Fuel utilizing Spallation Reactions John Freiderich NCSS 07/27/2006.
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.
Nuclear and Radiation Physics, BAU, First Semester, (Saed Dababneh). 1 Nuclear Reactions Sample.
Cross Sections One of the most important quantities we measure in nuclear physics is the cross section. Cross sections always have units of area and in.
1 New horizons for MCAS: heavier masses and α-particle scattering Juris P. Svenne, University of Manitoba, and collaborators CAP 15/6/2015.
Nuclear Level Density 1.What we know, what we do not know, and what we want to know 2.Experimental techniques to study level densities, what has been done.
Kazimierz 2011 T. Cap, M. Kowal, K. Siwek-Wilczyńska, A. Sobiczewski, J. Wilczyński Predictions of the FBD model for the synthesis cross sections of Z.
Breakup reaction for polarimetry of tensor polarized deuteron beams 1 A.P. Kobushkin Bogolyubov Institute for Theoretical Physics Metrologicheskaya str.
Pygmy Dipole Resonance in 64Fe
NUCLEAR LEVEL DENSITIES NEAR Z=50 FROM NEUTRON EVAPORATION SPECTRA IN (p,n) REACTION B.V.Zhuravlev, A.A.Lychagin, N.N.Titarenko State Scientific Center.
C. Johannesson CHAPTER 22 Nuclear Chemistry II. Radioactive Decay (p ) II. Radioactive Decay (p ) I IV III II.
3/2003 Rev 1 I.2.9 – slide 1 of 35 Session I.2.9 Part I Review of Fundamentals Module 2Basic Physics and Mathematics Used in Radiation Protection Session.
NUCLEAR CHEMISTRY OBJECTIVE: TO EXPLAIN THE PROCESS OF RADIOACTIVE DECAY USING NUCLEAR EQUATIONS AND HALF LIFE Essential Question: How do unstable (radioactive)
Types of Radioactive Decay Kinetics of Decay Nuclear Transmutations
Improving systematic predictions of  -delayed neutron emission probabilities E. A. McCutchan A.A. Sonzogni T.D. Johnson NNDC D. Abriola IAEA M. Birch,
With S. Mavrodiev (INRNE, BAS, Sofia, Bulgaria D. Vlasenko (NPU, Odessa, Ukraine) M. Deliyergiyev (NPU, Odessa, Ukraine) Kramers Diffusive Mechanism of.
Pion-Induced Fission- A Review Zafar Yasin Pakistan Institute of Engineering and Applied Sciences (PIEAS) Islamabad, Pakistan.
A.Yu. Chirkov1), S.V. Ryzhkov1), P.A. Bagryansky2), A.V. Anikeev2)
Nuclear and Radiation Physics, BAU, First Semester, (Saed Dababneh). 1.
Time dependent GCM+GOA method applied to the fission process ESNT janvier / 316 H. Goutte, J.-F. Berger, D. Gogny CEA/DAM Ile de France.
The experimental evidence of t+t configuration for 6 He School of Physics, Peking University G.L.Zhang Y.L.Ye.
© 2003 By Default! A Free sample background from Slide 1 JINR SCIENTIFIC COUNCIL 102 nd Session, September 2007, Dubna.
Nuclear Stability and Decay 1500 different nuclei are known. Only 264 are stable and do not decay. The stability of a nucleus depends on its neutron-to-
Improvements of microscopic transport models stimulated by spallation data for incident energies from 113 to MeV Umm Al-Qura University and King.
1 Alushta 2016 CROSS SECTION OF THE 66 Zn(n,α) 63 Ni REACTION at CROSS SECTION OF THE 66 Zn(n, α) 63 Ni REACTION at E n = 4.0, 5.0 and 6.0 MeV I. Chuprakov,
Rotational energy term in the empirical formula for the yrast energies in even-even nuclei Eunja Ha and S. W. Hong Department of Physics, Sungkyunkwan.
Transmutation of 129 I with high energy neutrons produced in spallation reactions induced by protons in massive target V.HENZL Nuclear Physics Institute.
Absorption of Nuclear Radiation & Radiation Effects on Matter: Atomic and Nuclear Physics Dr. David Roelant.
Nuclear Transformations
Aim # 47: How can we obtain energy from the nucleus of an atom?
JOINT INSTITUTE FOR NUCLEAR RESEARCH
Resonance Reactions HW 34 In the 19F(p,) reaction:
Section III: A World of Particles
CHAPTER 24 Nuclear Energy
Intermediate-mass-fragment Production in Spallation Reactions
Nuclear Transformations
Chapter 4 Mechanisms and Models of Nuclear Reactions
Performed experiments Nuclotron – set up ENERGY PLUS TRANSMUTATION
Elastic alpha scattering experiments
CHAPTER 22 Nuclear Chemistry
Unit 4 – Nuclear Reactions
Effects of Deformation Parameter on Reaction Cross Section
Catalin Borcea IFIN-HH INPC 2019, Glasgow, United Kingdom
Presentation transcript:

Systematical Analysis of Fast Neutron Induced Alpha Particle Emission Reaction Cross Sections Jigmeddorj Badamsambuu, Nuclear Research Center, National University of Mongolia, Ulaanbaatar, Mongolia G.Khuukhenkhuu, M.Odsuren.

Overview Introduction Formula for the reaction cross sections The Comparison of Theoretical and Experimental (n,a) Cross Sections Systematic analysis Conclusion

Introduction Investigation of the fast neutron induced alpha particle emission reaction is important for both: nuclear reactor technology the understanding of nuclear reaction mechanisms. Systematic study of reaction cross sections is important: to estimate radiation damage due to helium production nuclear heating and transmutations in the structural materials of reactors. in practice to evaluate the neutron cross sections of the nuclides, for which no experimental data are available.

Formula for The Reaction Cross Section G.Khuukhenkhuu, G.Unenbat Scientific Transactions, National University of Mongolia, 7(159), 2000, p.72 For fast neutrons using the evaporation and constant nuclear temperature models and semi-classical approach for an inverse reaction cross section we can obtain the following general formula: where: R – radius of target nuclei - wavelength of incident neutrons Q n  – reaction energy V  - coulomb potential for alpha particle  - thermodynamic temperature of nuclei

Coulomb potential D.G.Gardner and Yu-Wen Yu Nucl. Phys., v.60, N1, 1964, p.49 Thermodynamic temperature J.M.Blatt and V.F.Weisskopf Theoretical Nuclear Physics, John Wiley and Sons, New York, where: E n – neutron energy A – mass number of target nuclei where: Z – proton number of target nuclei

Reaction energy (used Weizsacker formula) Where: B  – the binding energy of alpha particle, N – neutron number of target nuclei,  =15.7 MeV,  =17.8 MeV,  =0.71 MeV,  =23.7 MeV and for even-even nuclei  =11.8 MeV, for odd-odd nuclei  MeV, for even-odd or o-even nuclei  0. Rohlf: Modern Physics from a to Z0, James William Rohlf, Wiley, 1994

Simple Formula for the (n,a) cross section:

The Comparison of Theoretical and Experinmental (n,a) Cross Sections The comparisons of the absolute values for theoretical cross sections calculated by statistical model with known experimental data at neutron energies En=14.5 MeV is shown here. It was observed that statistical model formulae give overestimated values for (n,a) cross sections at the 14,5 MeV energy of neutrons. Our hypothesis: the difference is caused by the alpha-clusterization effect ( alpha-particle formation probability) on the surface of nuclei.

Yu.P.Popov and W.I.Furman III School on Neutron Physics, JINR, D , 1978, Dubna, p.390 The ratio of neutron emission probability to alpha emission one from compound nucleus is 4.5 In this case theoretical (n,a) cross sections are in agreement with experimental data

Systematic Analysis E n (MeV)KC The values of parameters C and K fitted to experimental data are given in here. And It is seen that theoretical line fitted to experimental data is in agreement with known experimental cross section data The same as, C and K parameters for different neutron energies are fitted, and are given in Table.

Conclusion Using the statistical model formula we performed the systematic analysis of fast neutron induced (n,a) reaction cross sections data. We have fitted the values of parameters C and K to experimental data for some energy of neutrons. When we take into account alpha particle emission probability the theoretical results agree well with the experimental data

Thank you for your kind attention!