Emission of Helium Nuclei in Relativistic Proton Interactions Leading to Total Break up of Ag and Br Nuclei. Z.Physik A 279, 407 (1976).

Size: px
Start display at page:

Download "Emission of Helium Nuclei in Relativistic Proton Interactions Leading to Total Break up of Ag and Br Nuclei. Z.Physik A 279, 407 (1976)."

Transcription

1 Emission of Helium Nuclei in Relativistic Proton Interactions Leading to Total Break up of Ag and Br Nuclei. Z.Physik A 279, 407 (1976).

2 Inelastic Interactions of 69.0 GeV/c Protons with Emulsion Nuclei. Egypt. J. Physics 7, 67 (1976).

3 Inelastic Interactions of 69.0 GeV/c Protons with Light (CNO) and Heavy (Ag, Br) Emulsion Nuclei. Egypt. J. Physics 8, No.1, 31 (1977).

4 Angular Distributions of Charged Secondaries Emitted in Inelastic Interactions of Relativistic Protons with Emulsion Nuclei. Egypt. J. Physics 8, No.1, 47 (1977).

5 Inelastic Interactions of 69.0 GeV/c Protons with Emulsion Nucleons. Acta Physica Academica Scientiarum Hungaricae, Tomas 43 (1), 3 (1977).

6 Topological Cross Section and Angular Distribution of Charged Secondaries in 69.0 GeV/c Nucleon-Nucleon Scattering. Bulg. J. Physics V. 1, 23 (1978).

7 Emission of Slow Protons and Alpha Particles in the Interactions of 69.0 GeV/c Protons with Emulsion Nuclei. Egypt. J. Physics 16, No.1, 1 (1985).

8 Inelastic Interactions of 70-GeV/c K+-Mesons in Nuclear Emulsions. Egypt. J. Physics 17, No.2, 379 (1986).

9 Hot and Cold Z=2 Projectile Fragments from 4He, 22Ne and 24Mg at 4.5 GeV/c in Nuclear Emulsion. Egypt. J. Physics 17, No.2, 395 (1986).

10 Angular Distributions of Relativistic Fragments of Charge 2

11 Scaling Behavior of Multiplicity Distribution in Annihilation Processes for 70 GeV/c Antiproton-Nucleus Interactions. Egypt. J. Physics 18, No.2, 169 (1987).

12 Coherence and Self-Induced NuclearTransparancy in 70 GeV/c P-Nuclear Collisions. Egypt. J. Physics 18, No. 1,157 (1987).

13 Fragmentation of 24Mg at 4.5 GeV/c/n. Proc. Math.Phys. Soc. Egypt. No. 65, 27 (1988).

14 Fragmentation of 22Ne Nuclei at 4.1 GeV/c/n in Nuclear Emulsion. Proc. Math. Phys. Soc. Egypt. No. 65, 1 (1988).

15 Interaction of 200 AGeV 32S Projectiles with Nuclear Emulsions. Proceedings of the XXIIIrd Rencontre De Moriond, March (1988).

16 Negative-binomial Multiplicity Distribution in the Interactions of 24 Mg ions with Light and Heavy Emultion Nuclei. Physics Letters B, 292,148 (1992).

17 Multiplicity and Rapidity Density in Central Collisions of 4.1 AGeVC-1 22Ne Nuclei in Nuclear Emulsion. J. Phys. G: Nuclear Part. Phys. 19, 2027 (1993).

18 The Anomalous Behavior of the Doubly Charged Projectile Fragments Produced from 16O Em Interaction at 60 and 200 A GeV. First Annual Scientific Research Conference of Cairo University;15 April (1993).

19 Relativistic Helium Fragments Emitted in 24Mg and 22Ne Emulsion Interactions at Nearly 4.5 A GeV. Egypt. J. Phys. 25, No. 1, 123 (1994).

20 Mean Free Paths of Nuclear Projectile Fragments Produced in 200 AGeV 16O Emulsion Nuclei. Egypt. J. Phys. 25, No. 1, 137 (1994).

21 ultiplicity Distributions of Produced Particles in 60 AGeV 16O-Emulsion Interactions and Eclipse Effect. IL Nuovo Cimento Vol. 108A, 3, 281 (1995).

22 On Slow Particle Production in 200 AGeV 16O Emulsion Interactions. IL Nuovo Cimento Vol. 108A, 1, 87 (1995).

23 Nuclear Temperature and Multiplicities of Relativistic He Fragments From 16O Emulshon Interactions at 200 AGeV. IL Nuovo Cimento Vol. 108A, 7, 809(1995).

24 Multiplicities of Charged Particles in 3.7 A GeV 23S Emulsion Interactions. IL Nuovo Cimento Vol. 108A, 7,831 (1995).

25 Characteristics of Projectile Fragments Produced in 24Mg-Em Interactions at Dubna Energy. IL Nuovo Cimento Vol. 108A, 8, 935 (1995).

26 Multiplicity Distributions of Target Fragments in 60 A GeV 16O-Emulsion Interactions. International Journal of Modern Physics E, Vol. 5, 4, 617 (1996).

27 Some Characteristics of Produced Particles in 16O-Emulsion Collisions of Different Relativistic Energies. IL Nuovo Cimento Vol. 109A, 8, 1135 (1996).

28 External Electron Pair Production in High Energy Collisions. IL Nuovo Cimento Vol. 109A, 1517 (1996).

29 Anomalous Behavior of Projectile Fragments from Interactions of 16OProjectiles with Nuclear Emulsion. Kerntechnik Carl Hanser Verlag, Vol. 61, 4 (1996).

30 Target Associated Particles Produced in the Interactions of 3.7 and 200 AGeV/c 32S with Nuclear Emulsion. International Journal of Physics E,Vol. 6, No1, 191 (1997).

31 Fragmentation of 32S Nuclie in Photo-Emulsion at 3.7A GeV. Radiation Measurements,Vol. 28, No1, 231 (1997).

32 Sulfur Dissociation in Nuclear Emulsion at 3.7 and 200 A GeV. Journal of Physics G. Nuclear Part Physics, Vol.28, No.2, 241 (2002).

33

arxiv: v1 [nucl-ex] 1 Dec 2007

arxiv: v1 [nucl-ex] 1 Dec 2007 Multiplicity and angular distribution of particles emitted in relativistic nuclear-nuclear interactions M. K. Suleymanov1, 2, E. U. Khan 1, A Kravchakova 3, Mahnaz Q. Haseeb 1,S. M. Saleem 1, Y. H. Huseynaliyev

More information

Scaling of multiplicity distribution in high energy hadron-nucleus interactions

Scaling of multiplicity distribution in high energy hadron-nucleus interactions IOSR Journal of Applied Physics (IOSR-JAP) e-issn: 2278-4861.Volume 6, Issue 5 Ver. II (Sep.-Oct. 2014), PP 15-19 Scaling of multiplicity distribution in high energy hadron-nucleus interactions Tufail

More information

Comparison of experimental and theoretical results to define centrality of heavy ion collisions. 1. Introduction.

Comparison of experimental and theoretical results to define centrality of heavy ion collisions. 1. Introduction. Oral talk for the 24 th International Conference on Nuclear Tracks in Solids (ICNTS) Bologna, Italy, 0-05 September 2008 and submitted in Radiation Measurements with Manuscript Number: RADMEAS-D-08-00227R

More information

NJCTL.org 2015 AP Physics 2 Nuclear Physics

NJCTL.org 2015 AP Physics 2 Nuclear Physics AP Physics 2 Questions 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of? 2. What is the definition of the atomic number? What is its symbol?

More information

Interaction of 28 Si Ions with Emulsion Nuclei at Momentum 4.5 AGeV/c

Interaction of 28 Si Ions with Emulsion Nuclei at Momentum 4.5 AGeV/c Journal of Nuclear and Particle Physics 2015, 5(1: 10-14 DOI: 10.5923/j.jnpp.20150501.02 Interaction of 28 Si Ions with Emulsion Nuclei at Momentum 4.5 AGeV/c A. Abd EL-Daiem Physics Department, Faculty

More information

Characteristics study of projectile s lightest fragment for

Characteristics study of projectile s lightest fragment for 1 Characteristics study of projectile s lightest fragment for 84 Kr 36 - emulsion interaction at around 1 A GeV N. Marimuthu 1, 2, V. Singh 1 *, S. S. R. Inbanathan 2 1 High Energy Physics laboratory,

More information

CHARACTERISTICS OF THE SECONDARY PARTICLES FROM INTERACTIONS AT 40 GeV/c IN DIFFERENT NUCLEAR MATTER PHASES

CHARACTERISTICS OF THE SECONDARY PARTICLES FROM INTERACTIONS AT 40 GeV/c IN DIFFERENT NUCLEAR MATTER PHASES DOI: http://dx.doi.org/10.5564/pmas.v54i4.619 CHARACTERISTICS OF THE SECONDARY PARTICLES FROM INTERACTIONS AT 40 GeV/c IN DIFFERENT NUCLEAR MATTER PHASES Ts.Baatar, R.Togoo, G.Sharkhuu, B.Otgongerel Institute

More information

Two Source Emission Behavior of Helium Projectile Fragments in 84 Kr Interactions at Around 1 GeV per nucleon

Two Source Emission Behavior of Helium Projectile Fragments in 84 Kr Interactions at Around 1 GeV per nucleon Physics International 1 (): 109-115, 010 ISSN 1948-9803 010 Science Publications Two Source Emission Behavior of Helium Projectile Fragments in 84 Kr Interactions at Around 1 GeV per nucleon 1, Manoj Kumar

More information

Multiplicity Characteristics of Fragments Produced in 4.5A GeV/c

Multiplicity Characteristics of Fragments Produced in 4.5A GeV/c Multiplicity Characteristics of Fragments Produced in 4.5A GeV/c Mg Emulsion Interaction A. Adelsalam, E. A. Shaat, Z. Aou Moussa, B. M. Badawy (1), and Z. S. Mater Physics Department, Faculty of Science,

More information

PoS(Baldin ISHEPP XXII)042

PoS(Baldin ISHEPP XXII)042 Multifragmentation of nuclei by photons: new approaches and results Institute for Nuclear Research RAS Prospect 60-let Octabra, 7A, 117312 Moscow, Russia E-mail: vladimir@cpc.inr.ac.ru A review on multifragmentation

More information

Heavy Ion Interactions. Beginners FLUKA Course

Heavy Ion Interactions. Beginners FLUKA Course Heavy Ion Interactions Beginners FLUKA Course 1 Overview The models DPMJET RQMD BME Input options Beam definition Transport thresholds 2 Heavy ion interaction models in FLUKA - 1 E > 5 GeV/n Dual Parton

More information

STUDY OF SOME CHARACTERISTICS OF PROTONS USING INTERACTIONS OF LIGHT NUCLEI

STUDY OF SOME CHARACTERISTICS OF PROTONS USING INTERACTIONS OF LIGHT NUCLEI STUDY OF SOME CHARACTERISTICS OF PROTONS USING INTERACTIONS OF LIGHT NUCLEI M. Ajaz 1, 2, M. K. Suleymanov 2, 3, K. H. Khan 2, A. Zaman 2, H. Younis 2, A. Rahman 4 1 Department of Physics, Abdul Wali Khan

More information

Characteristics of compound multiplicity in hadron-nucleus collisions

Characteristics of compound multiplicity in hadron-nucleus collisions Indian Journal of Pure & Applied Physics Vol. 48, December 2010, pp. 855-859 Characteristics of compound multiplicity in hadron-nucleus collisions Tufail Ahmad 1 *, Nazeer Ahmad 2, Shaeel Ahmad 2 & M Zafar

More information

RADIOACTIVITY. An atom consists of protons, neutrons and electrons.

RADIOACTIVITY. An atom consists of protons, neutrons and electrons. RADIOACTIVITY An atom consists of protons, neutrons and electrons. - Protons and neutrons are inside the nucleus - Electrons revolve around the nucleus in specific orbits ATOMIC NUMBER: - Total number

More information

Nuclear Physics Questions. 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of?

Nuclear Physics Questions. 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of? Nuclear Physics Questions 1. What particles make up the nucleus? What is the general term for them? What are those particles composed of? 2. What is the definition of the atomic number? What is its symbol?

More information

Research Article Shower and Slow Particle Productions in Nucleus-Nucleus Collisions at High Energy

Research Article Shower and Slow Particle Productions in Nucleus-Nucleus Collisions at High Energy Advances in High Energy Physics, Article ID 4354, 12 pages http://dx.doi.org/1.1155/214/4354 Research Article Shower and Slow Particle Productions in Nucleus-Nucleus Collisions at High Energy S. Fakhraddin,

More information

AZIMUTHAL CORRELATION FUNCTIONS AS A PROBE FOR COLLECTIVE MOTION. A.Kravcakova, S.Vokal. and. the Kr Collaboration

AZIMUTHAL CORRELATION FUNCTIONS AS A PROBE FOR COLLECTIVE MOTION. A.Kravcakova, S.Vokal. and. the Kr Collaboration AZIMUTHAL CORRELATION FUNCTIONS AS A PROBE FOR COLLECTIVE MOTION A.Kravcakova, S.Vokal and the Kr Collaboration (Dubna, Kosice, Lund, Moscow, Tashkent, Varanasi) Faculty of Science, P.J. Safarik University,

More information

Multiple Choice Questions

Multiple Choice Questions Nuclear Physics & Nuclear Reactions Practice Problems PSI AP Physics B 1. The atomic nucleus consists of: (A) Electrons (B) Protons (C)Protons and electrons (D) Protons and neutrons (E) Neutrons and electrons

More information

Chapter V: Interactions of neutrons with matter

Chapter V: Interactions of neutrons with matter Chapter V: Interactions of neutrons with matter 1 Content of the chapter Introduction Interaction processes Interaction cross sections Moderation and neutrons path For more details see «Physique des Réacteurs

More information

At this time the quark model consisted of three particles, the properties of which are given in the table.

At this time the quark model consisted of three particles, the properties of which are given in the table. *1 In 1961 Murray Gell-Mann predicted the existence of a new particle called an omega (Ω) minus. It was subsequently discovered in 1964. At this time the quark model consisted of three particles, the properties

More information

SHOWER PARTICLE MULTIPLICITY DISTRIBUTIONS FOR COLLISIONS OF GEV/C PROTONS WITH EMULSION UDC S. Drndarević, G. Škoro, D.

SHOWER PARTICLE MULTIPLICITY DISTRIBUTIONS FOR COLLISIONS OF GEV/C PROTONS WITH EMULSION UDC S. Drndarević, G. Škoro, D. UNIVERSITY OF NIŠ The scientific journal FACTA UNIVERSITATIS Series: Physics, Chemistry and Technology Vol. 2, No 1, 1999 pp. 39-45 Editor of series: Momčilo Pejović, e-mail: pejovic@elfak.ni.ac.yu Address:

More information

What is Spallation???

What is Spallation??? What is Spallation??? Definition found in Nuclear Physics Academic press: projectile (p, n, π,...) target Spallation---a type of nuclear reaction in which the high-energy level of incident particles causes

More information

Physics 3204 UNIT 3 Test Matter Energy Interface

Physics 3204 UNIT 3 Test Matter Energy Interface Physics 3204 UNIT 3 Test Matter Energy Interface 2005 2006 Time: 60 minutes Total Value: 33 Marks Formulae and Constants v = f λ E = hf h f = E k + W 0 E = m c 2 p = h λ 1 A= A T 0 2 t 1 2 E k = ½ mv 2

More information

Unit 2 Exam - Atomic Structure and Nuclear

Unit 2 Exam - Atomic Structure and Nuclear 1. The atomic number of an atom is always equal to the total number of. neutrons in the nucleus. protons in the nucleus 5. The mass number of an atom is equal to the number of. neutrons, only. protons,

More information

Chapter 25. Nuclear Chemistry. Types of Radiation

Chapter 25. Nuclear Chemistry. Types of Radiation Chapter 25 Nuclear Chemistry Chemical Reactions 1. Bonds are broken and formed 2. Atoms may rearrange, but remain unchanged 3. Involve only valence electrons 4. Small energy changes 5. Reaction rate is

More information

CHIARA OPPEDISANO ELENCO PUBBLICAZIONI SCIENTIFICHE

CHIARA OPPEDISANO ELENCO PUBBLICAZIONI SCIENTIFICHE CHIARA OPPEDISANO ELENCO PUBBLICAZIONI SCIENTIFICHE PUBBLICAZIONI SU RIVISTE SCIENTIFICHE INTERNAZIONALI (1) NA60 Collaboration, Precision study of the η µµγ and ω µ+µµπ0 electromagnetic transition form-factors

More information

The discovery of the antiproton and other antimatter,

The discovery of the antiproton and other antimatter, 4 Antibaryons The discovery of the antiproton and other antimatter, 1955 1959 While the existence of antiparticles was established with Anderson s discovery of the positron in 1932, it was not clear in

More information

acta physica slovaca vol. 54 No. 4, August 2004 STUDIES OF LIGHT NUCLEUS CLUSTERING IN RELATIVISTIC MULTIFRAGMENTATION PROCESSES

acta physica slovaca vol. 54 No. 4, August 2004 STUDIES OF LIGHT NUCLEUS CLUSTERING IN RELATIVISTIC MULTIFRAGMENTATION PROCESSES acta physica slovaca vol. 54 No. 4, 351 365 August 2004 STUDIES OF LIGHT NUCLEUS CLUSTERING IN RELATIVISTIC MULTIFRAGMENTATION PROCESSES V. Bradnová a, M.M. Chernyavsky b, A.Sh. Gaitinov c, L.A. Goncharova

More information

A Comparative Study of Multiplicity Scaling in Nuclear Collisions at High Energies

A Comparative Study of Multiplicity Scaling in Nuclear Collisions at High Energies A Comparative Study of Multiplicity Scaling in Nuclear Collisions at High Energies N. AHMAD S. S. ALI M. MOHSIN KHAN Department of Applied Physics Z.H. College of Engineering & Technology, S. A. DAR Abstract:

More information

Slide 1 / 57. Nuclear Physics & Nuclear Reactions Practice Problems

Slide 1 / 57. Nuclear Physics & Nuclear Reactions Practice Problems Slide 1 / 57 Nuclear Physics & Nuclear Reactions Practice Problems Slide 2 / 57 Multiple Choice Slide 3 / 57 1 The atomic nucleus consists of: A B C D E Electrons Protons Protons and electrons Protons

More information

Collaborators: Prof. W. Sandhas and members of his group (Bonn),

Collaborators: Prof. W. Sandhas and members of his group (Bonn), Few Body Systems A1 Integral Equations (AGS) A2 Integro-differential equations (Hyperspherical Harmonics) A3 Time evolution methods A4 Supersymmetric Quantum Mechanics (SUSY) and Few-Body systems A5 Astrophysics

More information

PoS(Baldin ISHEPP XXII)072

PoS(Baldin ISHEPP XXII)072 Cumulative protons in hadron-nucleus and nucleus-nucleus interactions E-mail: yuldashev@jinr.ru E.Kh. Bazarov S.L. Lutpullaev K. Olimov E-mail: olimov@uzsci.net V.I. Petrov New experimental data on the

More information

Nuclear Reactions and Astrophysics: a (Mostly) Qualitative Introduction

Nuclear Reactions and Astrophysics: a (Mostly) Qualitative Introduction Nuclear Reactions and Astrophysics: a (Mostly) Qualitative Introduction Barry Davids, TRIUMF Key Concepts Lecture 2013 Introduction To observe the nucleus, we must use radiation with a (de Broglie) wavelength

More information

Spec Content Before Revision After 1st Revision After 2nd Revision

Spec Content Before Revision After 1st Revision After 2nd Revision Use the expression p = mv. Investigate and apply the principle of conservation of linear momentum to problems in one dimension. Investigate and relate net force to rate of change of momentum in situations

More information

Chapter Four (Interaction of Radiation with Matter)

Chapter Four (Interaction of Radiation with Matter) Al-Mustansiriyah University College of Science Physics Department Fourth Grade Nuclear Physics Dr. Ali A. Ridha Chapter Four (Interaction of Radiation with Matter) Different types of radiation interact

More information

The interaction of radiation with matter

The interaction of radiation with matter Basic Detection Techniques 2009-2010 http://www.astro.rug.nl/~peletier/detectiontechniques.html Detection of energetic particles and gamma rays The interaction of radiation with matter Peter Dendooven

More information

CHEM 312: Lecture 9 Part 1 Nuclear Reactions

CHEM 312: Lecture 9 Part 1 Nuclear Reactions CHEM 312: Lecture 9 Part 1 Nuclear Reactions Readings: Modern Nuclear Chemistry, Chapter 10; Nuclear and Radiochemistry, Chapter 4 Notation Energetics of Nuclear Reactions Reaction Types and Mechanisms

More information

Projectile Fragmentation of relativistic nuclei in peripheral Collisions

Projectile Fragmentation of relativistic nuclei in peripheral Collisions Projectile Fragmentation of relativistic nuclei in peripheral Collisions Swarnapratim Bhattacharyya 1, Maria Haiduc 2, Alina Tania Neagu 2 and Elena Firu 2 1 Department of Physics, New Alipore College,

More information

SOURCES of RADIOACTIVITY

SOURCES of RADIOACTIVITY Section 9: SOURCES of RADIOACTIVITY This section briefly describes various sources of radioactive nuclei, both naturally occurring and those produced artificially (man-made) in, for example, reactors or

More information

Simulated nucleon nucleon and nucleon nucleus reactions in the frame of the cascade exciton model at high and intermediate energies

Simulated nucleon nucleon and nucleon nucleus reactions in the frame of the cascade exciton model at high and intermediate energies PRAMANA c Indian Academy of Sciences Vol. 84, No. 4 journal of April 2015 physics pp. 581 590 Simulated nucleon nucleon and nucleon nucleus reactions in the frame of the cascade exciton model at high and

More information

Improvements and developments of physics models in PHITS for radiotherapy and space applications

Improvements and developments of physics models in PHITS for radiotherapy and space applications Improvements and developments of physics models in PHITS for radiotherapy and space applications L. Sihver 1-9, T. Sato 10, S. Hashimoto 10, T. Ogawa 10, K. Niita 11 1 Atominstitut, TU Wien, Austria, 2

More information

Physics with Exotic Nuclei

Physics with Exotic Nuclei Physics with Exotic Nuclei Hans-Jürgen Wollersheim NUclear STructure, Astrophysics and Reaction Outline Projectile Fragmentation A Route to Exotic Nuclei Fragmentation Cross Sections Nuclear Reaction Rates

More information

Heavy Ion Interactions. Beginners FLUKA Course

Heavy Ion Interactions. Beginners FLUKA Course Heavy Ion Interactions Beginners FLUKA Course Overview The models DPMJET RQMD BME Input options Beam definition Transport thresholds 2 Heavy ion interaction models in FLUKA - 1 E > 5 GeV/n Dual Parton

More information

Heavy Ions Interactions. FLUKA Beginner s Course

Heavy Ions Interactions. FLUKA Beginner s Course Heavy Ions Interactions FLUKA Beginner s Course Overview The models DPMJET RQMD BME Input options Beam definition Transport thresholds 2 Heavy ion interaction models in FLUKA - 1 E > 5 GeV/n Dual Parton

More information

Outline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect

Outline. Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter. Photon interactions. Photoelectric effect Chapter 6 The Basic Interactions between Photons and Charged Particles with Matter Radiation Dosimetry I Text: H.E Johns and J.R. Cunningham, The physics of radiology, 4 th ed. http://www.utoledo.edu/med/depts/radther

More information

1 Geant4 to simulate Photoelectric, Compton, and Pair production Events

1 Geant4 to simulate Photoelectric, Compton, and Pair production Events Syed F. Naeem, hw-12, Phy 599 1 Geant4 to simulate Photoelectric, Compton, and Pair production Events 1.1 Introduction An Aluminum (Al) target of 20cm was used in this simulation to see the eect of incoming

More information

An Analysis of Energy Dependence Parameter as Mean Charged Multiplicity for Proton-Antiproton Interactions

An Analysis of Energy Dependence Parameter as Mean Charged Multiplicity for Proton-Antiproton Interactions ISSN: 2347-3215 Volume 2 Number 6 (June-2014) pp. 132-140 www.ijcrar.com An Analysis of Energy Dependence Parameter as Mean Charged Multiplicity for Proton-Antiproton Interactions Hardik P.Trivedi 1 and

More information

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics Nuclear Physics and Astrophysics PHY-30 Dr. E. Rizvi Lecture 4 - Detectors Binding Energy Nuclear mass MN less than sum of nucleon masses Shows nucleus is a bound (lower energy) state for this configuration

More information

The experiment at JINR: status and physics program

The experiment at JINR: status and physics program The 3rd International Conference on Particle Physics and Astrophysics Volume 2018 Conference Paper The BM@N experiment at JINR: status and physics program D. Baranov, M. Kapishin, T. Mamontova, G. Pokatashkin,

More information

Publications of Francesco Arneodo: journal articles

Publications of Francesco Arneodo: journal articles Publications of Francesco Arneodo: journal articles Figure 1: Citation report from ISI Web of Science (IF=31.0) [1] E. Aprile et al., First Axion Results from the XENON100 Experiment, arxiv.org (submitted

More information

FRAGMENTATION OF RELATIVISTIC NUCLEI IN PERIPHERAL INTERACTIONS IN NUCLEAR TRACK EMULSION

FRAGMENTATION OF RELATIVISTIC NUCLEI IN PERIPHERAL INTERACTIONS IN NUCLEAR TRACK EMULSION ЯДЕРНАЯ ФИЗИКА, 2008, том 71, 9, с. 1595 1601 ЭЛЕМЕНТАРНЫЕ ЧАСТИЦЫ И ПОЛЯ FRAGMENTATION OF RELATISTIC NUCLEI IN PERIPERAL INTERACTIONS IN NUCLEAR TRACK EMULSION c 2008 D. A. Artemenkov 1)*, V. Bradnova

More information

Isospin influence on Fragments production in. G. Politi for NEWCHIM/ISODEC collaboration

Isospin influence on Fragments production in. G. Politi for NEWCHIM/ISODEC collaboration Isospin influence on Fragments production in 78 Kr + 40 Ca and 86 Kr + 48 Ca collisions at 10 MeV/nucleon G. Politi for NEWCHIM/ISODEC collaboration Dipartimento di Fisica e Astronomia Sezione INFN - Catania,

More information

State the main interaction when an alpha particle is scattered by a gold nucleus

State the main interaction when an alpha particle is scattered by a gold nucleus Q1.(a) Scattering experiments are used to investigate the nuclei of gold atoms. In one experiment, alpha particles, all of the same energy (monoenergetic), are incident on a foil made from a single isotope

More information

Nuclear contribution into single-event upset in 3D on-board electronics at moderate energy cosmic proton impact

Nuclear contribution into single-event upset in 3D on-board electronics at moderate energy cosmic proton impact Nuclear contribution into single-event upset in 3D on-board electronics at moderate energy cosmic proton impact N. G. Chechenin, T. V. Chuvilskaya and A. A. Shirokova Skobeltsyn Institute of Nuclear Physics,

More information

Heavy-ion collisions in a fixed target mode at the LHC beams

Heavy-ion collisions in a fixed target mode at the LHC beams Heavy-ion collisions in a fixed target mode at the LHC beams Alexey Kurepin 1, and Nataliya Topilskaya 1, 1 Institute for Nuclear Research, RAS, Moscow, Russia Abstract. The interaction of high-energy

More information

Photo-production of vector mesons in 2.76 TeV ultra-peripheral Pb+Pb collisions at ALICE. Daniel Tapia Takaki. On behalf of the ALICE Collaboration

Photo-production of vector mesons in 2.76 TeV ultra-peripheral Pb+Pb collisions at ALICE. Daniel Tapia Takaki. On behalf of the ALICE Collaboration Photo-production of vector mesons in 2.76 TeV ultra-peripheral Pb+Pb collisions at ALICE On behalf of the ALICE Collaboration Rencontres du Viet Nam: 14th Workshop on Elastic and Diffractive Scattering

More information

Stars Nuclei Baryons Quarks. STRANGENESS IN NUCLEI UNIQUE OPPORTUNITIES at FAIR Josef Pochodzalla

Stars Nuclei Baryons Quarks. STRANGENESS IN NUCLEI UNIQUE OPPORTUNITIES at FAIR Josef Pochodzalla Stars Nuclei Baryons Quarks STRANGENESS IN NUCLEI UNIQUE OPPORTUNITIES at FAIR Josef Pochodzalla Facility for Antiproton and Ion Research GSI, Darmstadt heavy ion physics nuclear structure atomic and plasma

More information

On the true nature of transfer reactions. leading to the complete fusion of projectile and target. G. Mouze and C. Ythier

On the true nature of transfer reactions. leading to the complete fusion of projectile and target. G. Mouze and C. Ythier 1 On the true nature of transfer reactions leading to the complete fusion of projectile and target G. Mouze and C. Ythier Université de Nice, Faculté des Sciences, 06 108 Nice cedex 2, France. mouze@unice.fr

More information

Nuclear Transparency in A(e,e π/k)x Status and Prospects

Nuclear Transparency in A(e,e π/k)x Status and Prospects Nuclear Transparency in A(e,e π/k)x Status and Prospects Tanja Horn Small size configurations at high-t workshop 26 March 2011 1 Nuclear Transparency Color transparency (CT) is a phenomenon predicted by

More information

Recent results from the STAR experiment on Vector Meson production in ultra peripheral AuAu collisions at RHIC.

Recent results from the STAR experiment on Vector Meson production in ultra peripheral AuAu collisions at RHIC. Recent results from the STAR experiment on Vector Meson production in ultra peripheral AuAu collisions at RHIC. Leszek Adamczyk On behalf of STAR Collaboration September 7, 2016 RHIC AA: Au+Au, Cu+Cu,

More information

PHASE TRANSITIONS. A. Budzanowski

PHASE TRANSITIONS. A. Budzanowski PHASE TRANSITIONS A. Budzanowski The H. Niewodniczański Institute of Nuclear Physics, Polish Academy of Sciences Radzikowskiego 152, 31-342 Kraków, Poland and V.A. Karnaukhov, H. Oeschler S.P. Avdeyev,

More information

PROTON AND LIGHT ION INTERACTIONS IN COSMIC RAY EXPERIMENT STRATOSPHERE IN THE COMPARISON WITH THE RECENT COLLIDER RESULTS

PROTON AND LIGHT ION INTERACTIONS IN COSMIC RAY EXPERIMENT STRATOSPHERE IN THE COMPARISON WITH THE RECENT COLLIDER RESULTS PROTON AND LIGHT ION INTERACTIONS IN IN THE COMPARISON WITH THE RECENT COLLIDER RESULTS A.Kh. Argynova a, N.I. Kochelev b, T.N. Kvochkina c, A.A. Loktionov a,t.kh. Sadykov a, N.N. Zastrozhnova a, a, S.Zh.

More information

CHARGED PARTICLE INTERACTIONS

CHARGED PARTICLE INTERACTIONS CHARGED PARTICLE INTERACTIONS Background Charged Particles Heavy charged particles Charged particles with Mass > m e α, proton, deuteron, heavy ion (e.g., C +, Fe + ), fission fragment, muon, etc. α is

More information

Benchmarking the CEM03.03 event generator

Benchmarking the CEM03.03 event generator Vienna meeting on inter-comparison of spallation reactions models Benchmarking the CEM03.03 event generator K. K. Gudima 1, M. I. Baznat 1 S. G. Mashnik 2, and A. J. Sierk 2 1 Institute of Applied Physics,

More information

Centrality Dependence of Rapidity Spectra of Negative Pions in 12 C+ 12 C and

Centrality Dependence of Rapidity Spectra of Negative Pions in 12 C+ 12 C and Centrality Dependence of Rapidity Spectra of Negative Pions in 12 C+ 12 C and 12 C+ 181 Ta Collisions at 4.2 GeV/c per Nucleon* Kh. K. Olimov 1),2) **, Sayyed A. Hadi 3) 1) *** and Mahnaz Q. Haseeb Abstract

More information

Experimental results on nucleon structure Lecture I. National Nuclear Physics Summer School 2013

Experimental results on nucleon structure Lecture I. National Nuclear Physics Summer School 2013 Experimental results on nucleon structure Lecture I Barbara Badelek University of Warsaw National Nuclear Physics Summer School 2013 Stony Brook University, July 15 26, 2013 Barbara Badelek (Univ. of Warsaw

More information

Geant4 Hadronic Physics - II

Geant4 Hadronic Physics - II Geant4 Hadronic Physics - II Geant4 Tutorial, Marshall Space Flight Center April 2012 Daniel Brandt (based on slides by T. Koi) based on Geant4 v9.5-p01 Overview Low energy neutron physics High-precision

More information

Dedicated Arrays: MEDEA GDR studies (E γ = MeV) Highly excited CN E*~ MeV, 4 T 8 MeV

Dedicated Arrays: MEDEA GDR studies (E γ = MeV) Highly excited CN E*~ MeV, 4 T 8 MeV Dedicated Arrays: MEDEA GDR studies (E γ = 10-25 MeV) Highly excited CN E*~ 250-350 MeV, 4 T 8 MeV γ-ray spectrum intermediate energy region 10 MeV/A E beam 100 MeV/A - large variety of emitted particles

More information

Emission Characteristics of the Projectile Fragments at Relativistic Energy

Emission Characteristics of the Projectile Fragments at Relativistic Energy Emission Characteristics of the Projectile Fragments at Relativistic Energy M. K. Singh* 1, A. K. Soma 2, Ramji Pathak 1 and V. Singh 2 1. Department of physics, Tilakdhari Postgraduate College, Jaunpur

More information

HIGHER ORDER THERMAL CORRECTIONS TO PHOTON SELF ENERGY

HIGHER ORDER THERMAL CORRECTIONS TO PHOTON SELF ENERGY HIGHER ORDER THERMAL CORRECTIONS TO PHOTON SELF ENERGY Mahnaz Q. Haseeb Physics Department COMSATS Institute of Information Technology Islamabad Outline Relevance Finite Temperature Effects One Loop Corrections

More information

Chapter 12: Nuclear Reaction

Chapter 12: Nuclear Reaction Chapter 12: Nuclear Reaction A nuclear reaction occurs when a nucleus is unstable or is being bombarded by a nuclear particle. The product of a nuclear reaction is a new nuclide with an emission of a nuclear

More information

Analysis of various projectile interactions with Nuclear Emulsion Detector nuclei at ~ 1 GeV per nucleon using Coulomb modified Glauber model

Analysis of various projectile interactions with Nuclear Emulsion Detector nuclei at ~ 1 GeV per nucleon using Coulomb modified Glauber model Analysis of various projectile interactions with Nuclear Emulsion Detector nuclei at ~ 1 GeV per nucleon using Coulomb modified Glauber model N. Marimuthu 1,, V. Singh 1 *, S. S. R. Inbanathan * 1 Department

More information

Noncentral collisions

Noncentral collisions Noncentral collisions Projectile Target QT E* MRS QP E* MRS: L. Gingras et al., Phys. Rev. C 65, 061604(2002) Noncentral collisions The IVS source Velocity distributions (LAB) for the 40 Ca + 40 Ca reaction

More information

Introduction to Ionizing Radiation

Introduction to Ionizing Radiation Introduction to Ionizing Radiation Bob Curtis OSHA Salt Lake Technical Center Supplement to Lecture Outline V. 10.02 Basic Model of a Neutral Atom Electrons(-) orbiting nucleus of protons(+) and neutrons.

More information

Analysis of fixed target collisions with the STAR detector

Analysis of fixed target collisions with the STAR detector Analysis of fixed target collisions with the STAR detector Brooke Haag for the STAR Collaboration Hartnell College / University of California, Davis Presented at the Meeting of the California Section of

More information

Radiation Physics PHYS /251. Prof. Gocha Khelashvili

Radiation Physics PHYS /251. Prof. Gocha Khelashvili Radiation Physics PHYS 571-051/251 Prof. Gocha Khelashvili Interaction of Radiation with Matter: Heavy Charged Particles Directly and Indirectly Ionizing Radiation Classification of Indirectly Ionizing

More information

LIST OF PUBLICATIONS

LIST OF PUBLICATIONS LIST OF PUBLICATIONS 1. F. Ehlotzky,Klein-Winkel Delbrück-Streuung, Acta Physica Austriaca 16, 374 (1963). 2. F. Ehlotzky,Small-Angle Delbrück Scattering, Nuovo Cimento 31, 1037 (1964). 3. F. Ehlotzky,

More information

3 Radioactivity - Spontaneous Nuclear Processes

3 Radioactivity - Spontaneous Nuclear Processes 3 Radioactivity - Spontaneous Nuclear Processes Becquerel was the first to detect radioactivity. In 1896 he was carrying out experiments with fluorescent salts (which contained uranium) and found that

More information

NOTES: 25.2 Nuclear Stability and Radioactive Decay

NOTES: 25.2 Nuclear Stability and Radioactive Decay NOTES: 25.2 Nuclear Stability and Radioactive Decay Why does the nucleus stay together? STRONG NUCLEAR FORCE Short range, attractive force that acts among nuclear particles Nuclear particles attract one

More information

Lecture 3. lecture slides are at:

Lecture 3. lecture slides are at: Lecture 3 lecture slides are at: http://www.physics.smu.edu/ryszard/5380fa17/ Proton mass m p = 938.28 MeV/c 2 Electron mass m e = 0.511 MeV/c 2 Neutron mass m n = 939.56 MeV/c 2 Helium nucleus α: 2 protons+2

More information

Interaction of Ionizing Radiation with Matter

Interaction of Ionizing Radiation with Matter Type of radiation charged particles photonen neutronen Uncharged particles Charged particles electrons (β - ) He 2+ (α), H + (p) D + (d) Recoil nuclides Fission fragments Interaction of ionizing radiation

More information

Nuclear Physics 2. D. atomic energy levels. (1) D. scattered back along the original direction. (1)

Nuclear Physics 2. D. atomic energy levels. (1) D. scattered back along the original direction. (1) Name: Date: Nuclear Physics 2. Which of the following gives the correct number of protons and number of neutrons in the nucleus of B? 5 Number of protons Number of neutrons A. 5 6 B. 5 C. 6 5 D. 5 2. The

More information

Nuclear Chemistry Bravo 15,000 kilotons

Nuclear Chemistry Bravo 15,000 kilotons Nuclear Chemistry Nuclear Chemistry Bravo 15,000 kilotons Radioactive elements Radioactive elements Elements with atomic numbers greater than 83 are radioactive Why? These elements have too many protons

More information

Geant4 version 10.0.p01. Hadronic Physics I. Geant4 Tutorial: version 10.0.p01. Michael Kelsey, Wed 5 Mar 2014

Geant4 version 10.0.p01. Hadronic Physics I. Geant4 Tutorial: version 10.0.p01. Michael Kelsey, Wed 5 Mar 2014 Michael Kelsey, Wed 5 Mar 2014 Hadronic Physics I Geant4 Tutorial: version 10.0.p01 Hadronic Physics I What is Hadronic Physics? The Hadronic Framework - Processes vs. Models - Cross sections and process

More information

PHY357 Lecture 14. Applications of QCD. Varying coupling constant. Jets and Gluons. Quark-Gluon plasma. Colour counting

PHY357 Lecture 14. Applications of QCD. Varying coupling constant. Jets and Gluons. Quark-Gluon plasma. Colour counting PHY357 Lecture 14 Applications of QCD Varying coupling constant Jets and Gluons Quark-Gluon plasma Colour counting The proton structure function (not all of section 5.8!) Variable Coupling Constants! At

More information

Threshold Photo-production of J/5 Mesons J. Dunne Jefferson Lab

Threshold Photo-production of J/5 Mesons J. Dunne Jefferson Lab hreshold Photo-production of J/5 Mesons J. Dunne Jefferson Lab Introduction With the advent of higher energies at Jefferson Lab, the study of charmonium becomes possible. he threshold production of J/5

More information

EEE4101F / EEE4103F Radiation Interactions & Detection

EEE4101F / EEE4103F Radiation Interactions & Detection EEE4101F / EEE4103F Radiation Interactions & Detection 1. Interaction of Radiation with Matter Dr. Steve Peterson 5.14 RW James Department of Physics University of Cape Town steve.peterson@uct.ac.za March

More information

Formation of strangeness-nuclei at PANDA

Formation of strangeness-nuclei at PANDA Formation of strangeness-nuclei at PANDA T. Gaitanos Introduction Theoretical background RBUU+SMM hybrid model Testing strangeness & fragmentation Strangeness production & fragment yields/spectra for p+x,

More information

MCRT L8: Neutron Transport

MCRT L8: Neutron Transport MCRT L8: Neutron Transport Recap fission, absorption, scattering, cross sections Fission products and secondary neutrons Slow and fast neutrons Energy spectrum of fission neutrons Nuclear reactor safety

More information

Transport Theoretical Studies of Hadron Attenuation in Nuclear DIS. Model Results Summary & Outlook

Transport Theoretical Studies of Hadron Attenuation in Nuclear DIS. Model Results Summary & Outlook Transport Theoretical Studies of Hadron Attenuation in Nuclear DIS T. Falter, W. Cassing,, K. Gallmeister,, U. Mosel Contents: Motivation Model Results Summary & Outlook Motivation elementary en reaction

More information

High Energy Frontier Recent Results from the LHC: Heavy Ions I

High Energy Frontier Recent Results from the LHC: Heavy Ions I High Energy Frontier Recent Results from the LHC: Heavy Ions I Ralf Averbeck ExtreMe Matter Institute EMMI and Research Division GSI Helmholtzzentrum für Schwerionenforschung Darmstadt, Germany Winter

More information

Radioactive Decay What is Radioactivity? http://explorecuriocity.org/explore/articleid/3033 http://explorecuriocity.org/explore/articleid/3035 http://explorecuriocity.org/explore/articleid/2160 Quick Review

More information

Alpha Particle: or Beta Particle: or Neutron: or n 0. Positron: Proton: or p + Gamma Ray:

Alpha Particle: or Beta Particle: or Neutron: or n 0. Positron: Proton: or p + Gamma Ray: Key Worksheet 21 Nuclear Chemistry Objectives To be able to write and use a nuclear chemical equation. To be able to predict the missing reactants or products in a nuclear chemical reaction. To be able

More information

Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons

Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na. Ellen Simmons Radiation Detection for the Beta- Delayed Alpha and Gamma Decay of 20 Na Ellen Simmons 1 Contents Introduction Review of the Types of Radiation Charged Particle Radiation Detection Review of Semiconductor

More information

Atomic Theory. Contribution to Modern Atomic Theory

Atomic Theory. Contribution to Modern Atomic Theory Alief High School Chemistry STAAR Review Reporting Category 2: Atomic Structure and Nuclear Chemistry C.6.A Understand the experimental design and conclusions used in the development of modern atomic theory,

More information

PHYSICS CET-2014 MODEL QUESTIONS AND ANSWERS NUCLEAR PHYSICS

PHYSICS CET-2014 MODEL QUESTIONS AND ANSWERS NUCLEAR PHYSICS PHYSICS CET-2014 MODEL QUESTIONS AND ANSWERS NUCLEAR PHYSICS IMPORTANT FORMULE TO BE REMEMBERED IMPORTANT FORMULE TO BE REMEMBERED 1. Identify the correct statement with regards to nuclear density a) It

More information

At the conclusion of this lesson the trainee will be able to: a) Write a typical equation for the production of each type of radiation.

At the conclusion of this lesson the trainee will be able to: a) Write a typical equation for the production of each type of radiation. RADIOACTIVITY - SPONTANEOUS NUCLEAR PROCESSES OBJECTIVES At the conclusion of this lesson the trainee will be able to: 1. For~, p and 7 decays a) Write a typical equation for the production of each type

More information

A Comparison between Channel Selections in Heavy Ion Reactions

A Comparison between Channel Selections in Heavy Ion Reactions Brazilian Journal of Physics, vol. 39, no. 1, March, 2009 55 A Comparison between Channel Selections in Heavy Ion Reactions S. Mohammadi Physics Department, Payame Noor University, Mashad 91735, IRAN (Received

More information

[2] State in what form the energy is released in such a reaction.... [1]

[2] State in what form the energy is released in such a reaction.... [1] (a) The following nuclear reaction occurs when a slow-moving neutron is absorbed by an isotope of uranium-35. 0n + 35 9 U 4 56 Ba + 9 36Kr + 3 0 n Explain how this reaction is able to produce energy....

More information

Anti-Nuclei in Relativistic Nuclear Collisions: Results and Expectations

Anti-Nuclei in Relativistic Nuclear Collisions: Results and Expectations Makutsi-Symposium, Nov. 20 Anti-Nuclei in Relativistic Nuclear Collisions: Results and Expectations Reinhard Stock, Goethe University Frankfurt Content Nuclei and Anti-Nuclei in A+A collisions - - Early

More information