RADIATIVE RECOMBINATION OF BARE NUCLEI AND IONS IN ELECTRON COOLING SYSTEM. A.V. Philippov, A.B. Kuznetsov, I.N. Meshkov
|
|
|
- Shon Jacobs
- 5 years ago
- Views:
Transcription
1 RADIATIVE RECOMBINATION OF BARE NUCLEI AND IONS IN ELECTRON COOLING SYSTEM A.V. Philippov A.B. Kuznetsov I.N. Meshkov Veksler and Baldin Laboratory of High Energy Physics Joint Institute for Nuclear Research Dubna Russia Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine
2 OUTLINE Introduction Analysis of experimental data of radiative recombination (RR) rates for bare nuclei Analysis of experimental data of RR rates for intermediate charge state of ions 3 RR beam lifetime and cooling time Conclusion A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine /
3 INTRODUCTION Review of experimental results and their comparison with theoretical approaches is presented in this talk. We consider two essential cases for NICA: Recombination of bare gold nuclei in the NICA cooling system Recombination of intermediate charge state of gold ions in the Booster cooling system. Based on these comparisons we evaluated the contribution of the RR losses of intermediate charge state of gold ions: Au 3+ Au 33+ Au 43+ Au 5+ Au 6+ Au 68+ and Au 69+ during their acceleration in the Booster and the beam lifetime of the gold bare nuclei Au 79+ in NICA. A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 3/
4 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI RR rates vs. the electron relative energy ΔE experiments: TSR CRYRING ESR. Red solid line theoretical models of H.A. Kramers [Phil. Mag. V P. 836.] black solid line R. Schuch [Phys. Rev. А. V. 45. N P ]. Fitted 50.0 Z Z Z Z E f E Recombination rate 0-8 cm 3 s e - +He + ØHe + + ÿz U Z He e - +C 6+ ØC 5+ + ÿz U Z C e - +N 7+ ØN 6+ + ÿz U Z N e - +Ne 0 + ØNe 9+ + ÿz U Z Ne e - +U 9 + ØU e - +U 9 + ØU Black dashed line is the fit of the formula above DE ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 4/ f E a Eb Ry E. Fitted 3 8 ZZ 8
5 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI (Contnd) RR rates vs. the electron relative energy ΔE experiments: TSR CRYRING ESR. Red solid line theoretical models of H.A. Kramers [Phil. Mag. V P. 836.] black solid line R. Schuch [Phys. Rev. А. V. 45. N P ]. Fitted 50.0 Z Z Z Z E f E Recombination rate 0-8 cm 3 s e - +Si 4 + ØSi ÿz U Z Si e - +Cl 7 + ØCl ÿz U Z Cl e - +Ar 8 + ØAr ÿz U Z Ar e - +Bi 83 + ØBi ÿz U Z Bi e - +U 9 + ØU e - +U 9 + ØU Black dashed line is the fit of the formula above DE ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 5/ f E a Eb Ry E. Fitted 3 8 ZZ 8
6 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI (Contnd) RR rates vs. magnetic field strength B experiment: ESR. [M. Steck et al. EPJ D P ] Recombination rate 0-8 cm 3 s mt 84 mt 94 mt 04. mt a=.0 a=0.7 a=0.4 a=0. Fitted ZZ RR spectra of U 9+ measured at 4 different magnetic guiding field strengths DE ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 6/ Z Z E f E f E a Eb Ry E. Fitted 3 8 ZZ 8
7 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI (Contnd) RR rates vs. transverse electron temperature T experiment: ESR. [M. Steck. NIM A V. 53. P ] EVcm Vd cm s B Gs l T E d U clearing voltage Vcm k 0 cm kb.6 0 Erg ev cathode cm cathode V me g V cm s d ev Erg ev d B T T T T l 0. ev. A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 7/
8 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI (Contnd) RR rates vs. transverse electron temperature T experiment: ESR. [M. Steck. NIM A V. 53. P ]. Case B=96 mt. Recombination rate 0 - s - Recombination rate 0 - s - Recombination rate 0 - s T ev 96 mt R NICA T ev Recombination rate 0 - s b T0. ESR a T ev ESR U NICA enica 0.4 NICAZAu ESR neesr Recombination rate 0 - s T ev a R Ry b Z n Top curve (right slope) Bottom curve (left slope) T ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 8/ R ESR.
9 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI [M. Bell and J.S. Bell. Particle Accelerators. 98. V.. P ] [M. Steck. NIM A V. 53. P ] (Contnd) RR rates vs. transverse electron temperature T experiment: ESR (Bell & Bell comparison). RR spectra of U 9+ measured for a different drift temperature T d e mred dashed line Maxwell blue dashed line flattened..000 T T d Tcathode T cathode 0.eV Recombination rate 0 - s MaxwellRR 3 3 8k B Z Ry 4 T 3 ZZ a0 Z Ry ln 3 3 mt e T 3 Z Ry FlattenedRR 3 3 k B Z Ry 5 T 3 ZZ a0 Z Ry ln ln. 3 3 mt e T 6 Z Ry 96 mt 98. mt 00.5 mt 0.8 mt 05 mt Bell & Bell Maxwell Bell & Bell Flattened T ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 9/
10 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI [M. Bell and J.S. Bell. Particle Accelerators. 98. V.. P ] [M. Steck. NIM A V. 53. P ] (Contnd) RR rates vs. transverse electron temperature T experiment: ESR (Bell & Bell comparison). RR spectra of U 9+ measured for a different drift temperature T d e mred dashed line Maxwell blue dashed line flattened..000 T T d Tcathode T cathode 0.eV Recombination rate 0 - s MaxwellRR 3 3 8k B Z Ry 4 T 3 ZZ a0 Z Ry ln 3 3 mt e T 3 Z Ry FlattenedRR 3 3 k B Z Ry 5 T 3 ZZ a0 Z Ry ln ln. 3 3 mt e T 6 Z Ry 96 mt 98. mt 00.5 mt Bell & Bell Maxwell Bell & Bell Flattened T ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 0/
11 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR BARE NUCLEI [M. Bell and J.S. Bell. Particle Accelerators. 98. V.. P ] [M. Steck. NIM A V. 53. P ] (Contnd) RR rates vs. transverse electron temperature T experiment: ESR (Bell & Bell comparison). RR spectra of U 9+ measured for a different drift temperature T d e mred dashed line Maxwell blue dashed line flattened..000 T T d Tcathode T cathode 0.eV Recombination rate 0 - s MaxwellRR 3 3 8k B Z Ry 4 T 3 ZZ a0 Z Ry ln 3 3 mt e T 3 Z Ry FlattenedRR 3 3 k B Z Ry 5 T 3 ZZ a0 Z Ry ln ln. 3 3 mt e T 6 Z Ry 98. mt 0.8 mt 05 mt Bell & Bell Maxwell Bell & Bell Flattened T ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine /
12 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR INTERMEDIATE CHARGE STATE OF IONS RR spectra of U 8+ measured at ESR. [A. Müller et al. Phys. Scr. 99. V. T37. P ] Recombination rate 0-8 cm 3 s e - +U 8 + ØU e - +U 9 + ØU Fitted ZZ Black line is the fit of the formula above DE ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine / Z Z E f E f E a Eb Ry E. Fitted 3 8 ZZ 8
13 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR INTERMEDIATE CHARGE STATE OF IONS (Contnd) RR rates vs. electron shell structure experiments: ESR LEAR SIS8. Recombination rate 0-8 cm 3 s Complete shell Au 63+ [Ne]3s 3p 4 U 76+ [Ne]3s 3p 4 Bi 67+ [Ne]3s 3p 4 Pb 66+ [Ne]3s 3p 4 One electron missing Bi 64+ [Ar]4s Au 60+ [Ar]4s Pb 63+ [Ar]4s One electron missing Pb 65+ [Ne]3s 3p 5 Bi 66+ [Ne]3s 3p 5 Au 6+ [Ne]3s 3p 5 U 75+ [Ne]3s 3p 5 Au ESR Pb ESR Pb LEAR Bi SIS8 U ESR Complete shell 30 Pb Electron number in ion N 54+ [Ar]4s 3d 8 e One electron missing Pb 53+ [Ar]4s 3d 0 Complete shell Pb 5+ [Ar]4s 3d 0 A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 3/
14 ANALYSIS OF EXPERIMENTAL DATA OF RR RATES FOR INTERMEDIATE CHARGE STATE OF IONS (Contnd) RR rates vs. electron shell structure experiments: LEAR (Pb ) ESR (Au 5+ ) TSR (Au ). Au 49+ and Pb 5+ [Ar]4s 3d 0 Au 50+ and Pb 53+ [Ar]4s 3d 0 Au 5+ and Pb 54+ [Ar]4s 3d 8. Recombination rate 0-8 cm 3 s e - +Au 50 + ØAu e - +Au 79 + ØAu e - +Pb 5 + ØPb ÿz Au Z Pb e - +Pb 53 + ØPb ÿz Au Z Pb e - +Pb 54 + ØPb ÿz Au Fitted e - +Au 5 Z + Z ØAu 4 Z + Z E f E + e - +Au 49 + ØAu Eb f Ea e - +Au 50 + ØAu Ry e - +Au 5 + ØAuFitte 50 + d+ 3 8 E. ZZ Black solid and dashed lines are the fit of the formula above. 0.0 Z Pb DE ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 4/
15 3 RR BEAM LIFETIME AND COOLING TIME RR beam lifetime in lab frame: RR RR dn Z dnz ZZ necool RR Fitted ZZ ZZ ZZ nz dt nz dt. We use well known Parkhomchuk formula for cooling time in lab frame: cool cool Zene cool cool 4m e ez Ze Ze Ze 3 Ze Ze Am u me V V Veff ln l e m c k T Ze max min L cool e B max V V min L min L V0 me kbe V qb me me V c V c V 0 c V 3 B 0 eff BV0. me All the units in CGS; q Z ion charge and nuclear number; m u m e unit of mass electron mass; γ β Lorenz factor beta; max min impact parameter; L electron Larmor radius; V V ion velocity; V eff electron effective velocity; B magnetic field angular spread; B magnetic field in Gs; ΔE electron energy shift in ev; beta-function emittance; l cool cool length relative length of cooling section; k B =.6 0 Erg/eV Boltzmann constant; e electron charge; c speed of light. k E A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 5/
16 3 RR BEAM LIFETIME AND COOLING TIME (Contnd) Estimation of gold ions beam losses in Booster. Recombination rate losses % Au 5 + Au 3 + Au 50 + Au 5 + Au 5 + Au 79 + Fitted ZZ Black solid and dashed lines are the fit of the formula above DE ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 6/ Z Z E f E f E a Eb Ry E. Fitted 3 8 ZZ 8
17 3 RR BEAM LIFETIME AND COOLING TIME (Contnd) Estimation of bare gold nucleus beam lifetime at NICA: I e = A r e = cm T /T =0./5 0 3 ev B=0. T. Intrabeam scattering (IBS) time (τ IBS ) black dashed line. Beam lifetime 0 4 s RR cool ü GeVu RR cool ü 3.5 GeVu RR cool ü 4.5 GeVu τ IBS ( GeV/u)=300 s DE ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 7/
18 3 RR BEAM LIFETIME AND COOLING TIME (Contnd) Estimation of bare gold nucleus beam lifetime at NICA vs. transverse temperature: I e = A r e = cm B=0. T. Beam lifetime 0 4 s RR cool Bell & Bell ü GeVu RR cool Bell & Bell ü 3.5 GeVu RR cool Bell & Bell ü 4.5 GeVu τ IBS ( GeV/u)=300 s T ev A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 8/
19 CONCLUSION The RR process of gold bare nuclei in NICA cooling system can be suppressed in two methods: by choosing of optimal relative electron energy shift between ions and electrons beam and by an artificial increase the transverse temperature of the electron beam (more preferable). In order to suppress the RR process of intermediate gold ions charge state in the Booster cooling system during ions accumulation is required to avoided when using the ions with electron shell configuration which have one electron missing. A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 9/
20 CONCLUSION (Contnd) Beam lifetime 0 4 s RR cool Bell & Bell ü GeVu RR cool Bell & Bell ü 3.5 GeVu RR cool Bell & Bell ü 4.5 GeVu T ev Beam lifetime 0 4 s RR cool ü GeVu RR cool ü 3.5 GeVu RR cool ü 4.5 GeVu DEeV A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine 0/
21 REFERENCES [] I.N. Meshkov et al. Status of NICA Project These Proceedings. MOIO0. [] H.A. Kramers. Phil. Mag. V P [3] М. Pajek and R. Schuch. Phys. Rev. А. V. 45. N P [4] M. Bell and J.S. Bell. Particle Accelerators. 98. V.. P (and references therein for table). [5] W. Shi et al. Euro. Phys. J. D P [6] A. Hoffknecht et al. Phys. Rev. А V [7] O. Uwira et al. Hyperfine Interaction V. 08. P [8] A. Hoffknecht et al. Phys. Scr. 00. V. T9. P [9] W. Spies et al. Hyperfine Interactions V. 4. P [0] R. Schuch et al. Acta Physica Polonica B V. 7. N. -. P [] L. Andersen et al. Phys. Rev. Lett V. 64. P [] A. Müller et al. Phys. Scr. 99. V. T37. P [3] A. Wolf et al. NIMA V. 44. P / A. Hoffknecht et al. HYINT V. 4. P [4] S. Baird et al. Phys. Lett. B. V. 36. Iss P [5] I. Meshkov. Ion Recombination in Electron Coolers. Working meeting. 4 March 0. CERN. Geneva. Private communication. [6] P. Beller et al. NIM A V. 53. P [7] V.V. Parkhomchuk A.N. Skrinskii. Phys. Usp V. 43. Num. 5. P A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine /
22 Thank you for your attention! A.V. Philippov Workshop on Beam Cooling and Related Topics (COOL ) September 6 0 Alushta Ukraine /
Theory of electron cooling
Theory of electron cooling Daria Astapovych 03/12/2014 HSC Meeting Outline Motivation and idea of the particle beam cooling Cooler Low energy, high energy beam Electron beam Kinetics of electron cooling
RECENT STATUS OF BEAM COOLING AT S-LSR*
Proceedings of COOL 11, Alushta, Ukraine MOIO06 RECENT STATUS OF BEAM COOLING AT S-LSR* A. Noda, M. Nakao, H. Souda, H. Tongu, ICR, Kyoto U., Kyoto, Japan, K. Jimbo, IAE, Kyoto U., Kyoto, Japan, T. Fujimoto,
Application of cooling methods at NICA project. G.Trubnikov JINR, Dubna
Application of cooling methods at NICA project G.Trubnikov JINR, Dubna Outline 1. NICA scheme, modes of operation, working cycles;. Booster scheme, parameters, beam requirements; 3. Status of the electron
BEAM COOLING AT NICA COLLIDER
BEAM COOLING AT NICA COLLIDER T. Katayama, GSI, Darmstadt, Germany I. Meshkov, A. Sidorin and G. Trubnikov, JINR, Dubna, Russia. Abstract At the heavy ion collider NICA presently promoted at the JINR,
ELECTRON COOLING EXPERIMENTS AT S-LSR
ELECTRON COOLING EXPERIMENTS AT S-LSR T. Shirai #, S. Fujimoto, M. Ikegami, H. Tongu, M. Tanabe, H. Souda, A. Noda ICR, Kyoto-U, Uji, Kyoto, Japan, K. Noda, NIRS, Anagawa, Inage, Chiba, Japan, T. Fujimoto,
free electron plus He-like ion
free electron plus He-like ion E e I p,n E 2 E 1 ΔE=E e +I p,n aber: ΔE=E 2 -E 1 n n n n n n=1 n=2 n=3 AAMOP 2011-2012 2011-11-16 1 dielectronic recombination E 2 E 1 n n n n n n=1 n=2 n=3 AAMOP 2011-2012
Beam Cooling. Beam Cooling. M. Steck, GSI, Darmstadt CERN Accelerator School Chios, Greece September 18 30, Introduction. 1.
Beam Cooling, GSI, Darmstadt CERN Accelerator School, September 18 30, 2011 Beam Cooling Introduction 1.Electron Cooling 2.Ionization Cooling 3.Laser Cooling 4.Stochastic Cooling Beam Cooling Beam cooling
National Institute of Radiological Sciences (NIRS), Anagawa, Inage-ku, Chiba
A. Noda 1, K. Noda 1, Е. М. Syresin 2, 1 National Institute of Radiological Sciences (NIRS), 4-9-1 Anagawa, Inage-ku, Chiba 263-8555 2 Joint Institute for Nuclear Research, Dubna, Moscow region,141980
SIMULATION STUDY FOR MEIC ELECTRON COOLING*
SIMULATION STUDY FOR MEIC ELECTRON COOLING* He Zhang #, Yuhong Zhang, JLab, Newport News, VA 23606, USA Abstract Electron cooling of the ion beams is one critical R&D to achieve high luminosities in JLab
Beam Cooling. M. Steck, GSI, Darmstadt. JUAS, Archamps, France March 9, 2015
Beam Cooling M. Steck, GSI, Darmstadt JUAS, Archamps, France March 9, 2015 time longitudinal (momentum) cooling Cooling injection into storage ring transverse cooling Xe 54+ 50 MeV/u p/p cooling off with
High-energy collision processes involving intense laser fields
High-energy collision processes involving intense laser fields Carsten Müller Max Planck Institute for Nuclear Physics, Theory Division (Christoph H. Keitel), Heidelberg, Germany EMMI Workshop: Particle
NICA Project at JINR Nuclotron-based Ion Collider facility I.Meshkov for NICA team
Workshop on Beam Cooling and Related Topics COOL 11 NICA Project at JINR Nuclotron-based Ion Collider facility I.Meshkov for NICA team, Ukraine hosted by JINR, Dubna 1 Contents Introduction: The goal of
Longitudinal stacking and electron cooling of ion beams in the ESR as a proof of principle for FAIR. C. Dimopoulou
Longitudinal stacking and electron cooling of ion beams in the ESR as a proof of principle for FAIR C. Dimopoulou B. Franzke, T. Katayama, D. Möhl, G. Schreiber, M. Steck DESY Seminar, 20 November 2007
Development of Electron Coolers in Novosibirsk
Development of Electron Coolers in Novosibirsk on behalf of Vasily Parkhomchuk (Budker INP SB RAS, Novosibirsk) May 23, 2012, IPAC12, New Orleans What is beam cooling? Cooling is reduction of the phase
[Published in Russian: V.V.Ammosov et al. Yadernaya Fizika I Inzhiniring 4 (2013) ] Received:
![[Published in Russian: V.V.Ammosov et al. Yadernaya Fizika I Inzhiniring 4 (2013) ] Received:](/thumbs/88/115132660.jpg "[Published in Russian: V.V.Ammosov et al. Yadernaya Fizika I Inzhiniring 4 (2013) ] Received:")
[Published in Russian: V.V.Ammosov et al. Yadernaya Fizika I Inzhiniring 4 (01)77 778] Received:.09.01 PRODUCION OF HIGH-P CUMULAIVE PARICLES IN PROON- NUCLEUS INERACIONS A 50 GeV. V.V.Ammosov 1, N.N.Antonov
DEVELOPMENT OF ELECTRON COOLERS IN NOVOSIBIRSK
DEVELOPMENT OF ELECTRON COOLERS IN NOVOSIBIRSK V.V. Parkhomchuk, BINP, Novosibirsk, 630090, Russia Abstract An electron cooling method was proposed by G. Budker almost 50 years ago. Since the first demonstrations
Analysis of Slice Transverse Emittance Evolution in a Photocathode RF Gun. Abstract
SLAC PUB 868 October 7 Analysis of Slice Transverse Emittance Evolution in a Photocathode RF Gun Z. Huang, Y. Ding Stanford Linear Accelerator Center, Stanford, CA 9439 J. Qiang Lawrence Berkeley National
DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS
DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS TSOKOS LESSON 6-6 NUCLEAR PHYSICS IB Assessment Statements Topic 13.2, Nuclear Physics 13.2.1. Explain how the radii of nuclei may be estimated from
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
ELECTRON COOLING EXPERIMENTS IN CSR*
ELECTRON COOLING EXPERIMENTS IN CSR* Xiaodong Yang #, Guohong Li, Jie Li, Xiaoming Ma, Lijun Mao, Ruishi Mao, Tailai Yan, Jiancheng Yang, Youjin Yuan, IMP, Lanzhou, 730000, China Vasily V. Parkhomchuk,
A new storage ring for ISOLDE
A new storage ring for ISOLDE Manfred Grieser Max Planck Institut für Kernphysik, Heidelberg ISOLDE facility at CERN NARRS workshop, GSI, Darmstadt, 13 th -15 th March 2018 1 Proposed TSR@ISOLDE project
SPIN2010. I.Meshkov 1, Yu.Filatov 1,2. Forschungszentrum Juelich GmbH. 19th International Spin Physics Symposium September 27 October 2, 2010
Forschungszentrum Juelich GmbH SPIN200 9th International Spin Physics Symposium September 27 October 2, 200 Jülich, Germany Polarized Hadron Beams in NICA Project I.Meshkov, Yu.Filatov,2 JINR, Dubna 2
HIGH-ENERGY HEAVY-ION ACCELERATORS
HIGH-ENERGY HEAVY-ION ACCELERATORS D. DINEV Bulgarian Academy of Sciences Institute for Nuclear Research and Nuclear Energy Why heavy ions accelerated to high energies? QCD phase diagram (Artist s view)
TAMU-TRAP facility for Weak Interaction Physics. P.D. Shidling Cyclotron Institute, Texas A&M University
TAMU-TRAP facility for Weak Interaction Physics P.D. Shidling Cyclotron Institute, Texas A&M University Outline of the talk Low energy test of Standard Model T =2 Superallowed transition Facility T-REX
Status of the Source of Polarized Ions project for the JINR accelerator complex (September 2013)
Status of the Source of Polarized Ions project for the JINR accelerator complex (September 2013) V.V. Fimushkin, A.D. Kovalenko, L.V. Kutuzova, Yu.V. Prokofichev Joint Institute for Nuclear Research, Dubna
PHYS 5012 Radiation Physics and Dosimetry
Radiative PHYS 5012 Radiation Physics and Dosimetry Mean Tuesday 24 March 2009 Radiative Mean Radiative Mean Collisions between two particles involve a projectile and a target. Types of targets: whole
Acceleration of Heavy Ions generated by ECR and EBIS
Acceleration of Heavy Ions generated by ECR and EBIS R.Becker, Goethe-Universität, Frankfurt, Germany O. Kester, NSCL, MSU, USA OUTLINE Ion production in ECR and EBIS is governed by the same collision
FIRST STEPS IN PHYSICAL TREATING OF THE COLLINEAR CLUSTER TRI-PARTITION MECHANISM
FIRST STEPS IN PHYSICAL TREATING OF THE COLLINEAR CLUSTER TRI-PARTITION MECHANISM Yu.V. Pyatkov 1,2, D.V. Kamanin 1, W. von Oertzen 3, A.A. Alexandrov 1, I.A. Alexandrova 1, N.A. Kondratyev 1, E.A. Kuznetsova
The FAIR Accelerator Facility
The FAIR Accelerator Facility SIS300 existing GSI proton linac SIS18 UNILAC SIS100 HESR pbar target SuperFRS goals: higher intensity (low charge states) higher energy (high charge states) production of
Issues of Electron Cooling
Issues of Electron Cooling Yaroslav Derbenev derbenev@jlab.org JLEIC Spring 2016 Collaboration Meeting JLab, March 29-31, 2016 Outline Friction force Magnetized cooling Misalignment impact Cooling rates
The KATRIN experiment
The KATRIN experiment Status and SDS comissioning Philipp Chung-On Ranitzsch for the KATRIN collaboration Insitute for Nuclear Physics, Westfälische Wilhelms-Universität, Münster The KATRIN experiment
Physics with stopped beams at TRIP-TRAP Facility. P.D. Shidling Cyclotron Institute, Texas A&M University
Physics with stopped beams at TRIP-TRAP Facility P.D. Shidling Cyclotron Institute, Texas A&M University Physics with stopped beams Experiments require high purity low energy ions for studying various
Development of the Positron Injector for LEPTA Facility
Development of the Positron Injector for LEPTA Facility V.Bykovsky, M.Eseev *, A.Kobets, I.Meshkov, V.Pavlov, R. Pivin, A.Rudakov, G.Trubnikov, S.Yakovenko * - Lomonosov Pomor State Universitet, Arkhangelsk
F. Zimmermann and M.-P. Zorzano, CERN, Geneva, Switzerland
LHC Project Note 244 11.12.2000 Touschek Scattering in HERA and LHC F. Zimmermann and M.-P. Zorzano, CERN, Geneva, Switzerland Keywords: Touschek effect, beam loss, coasting beam Summary We estimate the
3. Gas Detectors General introduction
3. Gas Detectors 3.1. General introduction principle ionizing particle creates primary and secondary charges via energy loss by ionization (Bethe Bloch, chapter 2) N0 electrons and ions charges drift in
Feasibility of measuring the magnetic dipole moments of the charm baryons at the LHC using bent crystals
Feasibility of measuring the magnetic dipole moments of the charm baryons at the LHC using bent crystals Alex Fomin Laboratoire de l Accélérateur Linéaire Université Paris-Sud/IN2P3, Orsay, France NSC
Magnetic field simulation in the central region of the VINCY Cyclotron
NUKLEONIKA 2003;48(Supplement 2):S39 S44 PROCEEDINGS Magnetic field simulation in the central region of the VINCY Cyclotron Sergei B. Vorojtsov, Aleksei S. Vorozhtsov, Nebojsa Nešković, Jasna Ristić-Ðurović,
Continuous electron cooling for high-luminosity colliders
Nuclear Instruments and Methods in Physics Research A 441 (2000) 286}293 Continuous electron cooling for high-luminosity colliders A. Skrinsky* Budker Institute for Nuclear Physics, 630090 Novosibirsk,
Laser Spectroscopy on Bunched Radioactive Ion Beams
Laser Spectroscopy on Bunched Radioactive Ion Beams Jon Billowes University of Manchester Balkan School on Nuclear Physics, Bodrum 2004 Lecture 1. 1.1 Nuclear moments 1.2 Hyperfine interaction in free
Nuclear Spin and Stability. PHY 3101 D. Acosta
Nuclear Spin and Stability PHY 3101 D. Acosta Nuclear Spin neutrons and protons have s = ½ (m s = ± ½) so they are fermions and obey the Pauli- Exclusion Principle The nuclear magneton is eh m µ e eh 1
Electromagnetic modulation of monochromatic neutrino beams
Journal of Physics: Conference Series PAPER OPEN ACCESS Electromagnetic modulation of monochromatic neutrino beams To cite this article: A L Barabanov and O A Titov 2016 J. Phys.: Conf. Ser. 675 012009
Atomic Structure and Atomic Spectra
Atomic Structure and Atomic Spectra Atomic Structure: Hydrogenic Atom Reading: Atkins, Ch. 10 (7 판 Ch. 13) The principles of quantum mechanics internal structure of atoms 1. Hydrogenic atom: one electron
TeV energy physics at LHC and in cosmic rays
Vulcano 2016 TeV energy physics at LHC and in cosmic rays Anatoly Petrukhin National Research Nuclear University MEPhI (Moscow Engineering Physics Institute), Russia Many physicists dream and hope to find
Nuclear Effects in Electron Capture into Highly Charged Heavy Ions
Nuclear Effects in Electron Capture into Highly Charged Heavy Ions W. Scheid 1,A.Pálffy 2,Z.Harman 2, C. Kozhuharov 3, and C. Brandau 3 1 Institut für Theoretische Physik der Justus-Liebig-Universität
Measurements of liquid xenon s response to low-energy particle interactions
Measurements of liquid xenon s response to low-energy particle interactions Payam Pakarha Supervised by: Prof. L. Baudis May 5, 2013 1 / 37 Outline introduction Direct Dark Matter searches XENON experiment
RFSS: Lecture 2 Nuclear Properties
RFSS: Lecture 2 Nuclear Properties Readings: Modern Nuclear Chemistry: Chapter 2 Nuclear Properties Nuclear and Radiochemistry: Chapter 1 Introduction, Chapter 2 Atomic Nuclei Nuclear properties Masses
Electron spins in nonmagnetic semiconductors
Electron spins in nonmagnetic semiconductors Yuichiro K. Kato Institute of Engineering Innovation, The University of Tokyo Physics of non-interacting spins Optical spin injection and detection Spin manipulation
High-resolution Study of Gamow-Teller Transitions
High-resolution Study of Gamow-Teller Transitions Yoshitaka Fujita, Osaka Univ. @CNS-SS, 04.Aug.17-20 Nucleus : 3 active interactions out of 4 Strong, Weak, EM Comparison of Analogous Transitions High
ELECTRON COOLING PERFORMANCE AT IMP FACILITY*
ELECTRON COOLING PERFORMANCE AT IMP FACILITY* Xiaodong Yang #, Jie Li, Lijun Mao, Guohong Li, Xiaoming Ma, Tailai Yan, Mingtao Song, Youjin Yuan, Jiancheng Yang, Ruishi Mao, Tiecheng Zhao, Peng Li, Wei
Accelerator Physics Final Exam pts.
Accelerator Physics Final Exam - 170 pts. S. M. Lund and Y. Hao Graders: C. Richard and C. Y. Wong June 14, 2018 Problem 1 P052 Emittance Evolution 40 pts. a) 5 pts: Consider a coasting beam composed of
IB Physics SL Y2 Option B (Quantum and Nuclear Physics) Exam Study Guide Practice Problem Solutions
IB Physics SL Y2 Option B (Quantum and Nuclear Physics) Exam Study Guide Practice Problem Solutions Objectives: 1. Describe the photoelectric effect. (B.1.1) 2. Describe the concept of the photon and use
Experimental Storage Ring - ESR E max = 420 MeV/u, 10 Tm, electron-, stochastic- and laser cooling. Indian Institute of Technology Ropar
Experimental Storage Ring - ESR E max = 420 MeV/u, 10 Tm, electron-, stochastic- and laser cooling Specification of the ESR Particle detectors Re-injection to SIS Two 5 kv rf-cavities Fast Injection Schottky
Two-body weak decay of highly charged ions, a tool to study neutrino properties?
Two-body weak decay of highly charged ions, a tool to study neutrino properties? The detector: ESR Experimental Storage Ring cooling: electron-, stochastic ion detection: Schottky-noise, particle detector
H/He burning reactions on unstable nuclei for Nuclear Astrophysics
H/He burning reactions on unstable nuclei for Nuclear Astrophysics PJ Woods University of Edinburgh H T O F E E U D N I I N V E B R U S I R T Y H G Explosive H/He burning in Binary Stars Isaac Newton,
Chapter 44. Nuclear Structure
Chapter 44 Nuclear Structure Milestones in the Development of Nuclear Physics 1896: the birth of nuclear physics Becquerel discovered radioactivity in uranium compounds Rutherford showed the radiation
Methods for optimization of the dynamics of positrons storage in the Surko trap
Workshop on Beam Cooling and Related Topics COOL 11 1 16 September 011, Alushta, Ukraine Methods for optimization of the dynamics of positrons storage in the Surko trap *М. Есеев, A. Kobets, I. Meshkov,
Superconducting Magnets for Future Electron-Ion Collider. Yuhong Zhang Thomas Jefferson National Accelerator Facility, USA
Superconducting Magnets for Future Electron-Ion Collider Yuhong Zhang Thomas Jefferson National Accelerator Facility, USA Mini-workshop on Accelerator, IAS, HKUST, Hong Kong, January 18-19, 2018 1 Outline
Ionization Detectors. Mostly Gaseous Detectors
Ionization Detectors Mostly Gaseous Detectors Introduction Ionization detectors were the first electrical devices developed for radiation detection During the first half of the century: 3 basic types of
ELECTRON COOLING OF PB54+ IONS IN LEIR
ELECTRON COOLING OF PB+ IONS IN LEIR G. Tranquille, CERN, Geneva, Switzerland Abstract Electron cooling is central in the preparation of dense bunches of lead beams for the LHC. Ion beam pulses from the
13.2 NUCLEAR PHYSICS HW/Study Packet
13.2 NUCLEAR PHYSICS HW/Study Packet Required: READ Tsokos, pp 407-412 SL/HL Supplemental: Cutnell and Johnson, pp 652-652, 970-973 DO Questions pp 412-414 #1,3,11 REMEMBER TO. Work through all of the
Heavy ion fusion energy program in Russia
Nuclear Instruments and Methods in Physics Research A 464 (2001) 1 5 Heavy ion fusion energy program in Russia B.Yu. Sharkov*, N.N. Alexeev, M.D. Churazov, A.A. Golubev, D.G. Koshkarev, P.R. Zenkevich
The Electronic Structure of Atoms
The Electronic Structure of Atoms Classical Hydrogen-like atoms: Atomic Scale: 10-10 m or 1 Å + - Proton mass : Electron mass 1836 : 1 Problems with classical interpretation: - Should not be stable (electron
Past searches for kev neutrinos in beta-ray spectra
Past searches for kev neutrinos in beta-ray spectra Otokar Dragoun Nuclear Physics Institute of the ASCR Rez near Prague dragoun@ujf.cas.cz supported by GAČR, P203/12/1896 The ν-dark 2015 Workshop TUM
KEK isotope separation system for β-decay spectroscopy of r-process nuclei
2 nd Workshop on Inelastic Reaction Isotope Separator for Heavy Elements Nov. 19, 2010 KEK isotope separation system for β-decay spectroscopy of r-process nuclei Y.X. Watanabe, RNB group (KEK) 1. Outline
Experiments in Ion Storage Rings: mass and lifetime measurements
Leuven, 2-6 June 2003, FANTOM Study week on Trapping and Manipulating Atomic and Subatomic Particles Experiments in Ion Storage Rings: mass and lifetime measurements Fritz Bosch, GSI Darmstadt, Germany
Laser wakefield electron acceleration to multi-gev energies
Laser wakefield electron acceleration to multi-gev energies N.E. Andreev Joint Institute for High Temperatures, Russian Academy of Sciences, Moscow, Russia Moscow Institute of Physics and Technology, Russia
On-axis injection into small dynamic aperture
On-axis injection into small dynamic aperture L. Emery Accelerator Systems Division Argonne National Laboratory Future Light Source Workshop 2010 Tuesday March 2nd, 2010 On-Axis (Swap-Out) injection for
Beam halo formation in high-intensity beams
Beam halo formation in high-intensity beams Alexei V. Fedotov,1,2 Brookhaven National Laboratory, Upton, NY 11973, USA Abstract Studies of beam halo became an unavoidable feature of high-intensity machines
Synchrotron Power Cosmic rays are astrophysical particles (electrons, protons, and heavier nuclei) with extremely high energies. Cosmic-ray electrons in the galactic magnetic field emit the synchrotron
for the production of lepton pairs and photons in collisions of relativistic nuclei
Strong-field effects for the production of lepton pairs and photons in collisions of relativistic nuclei Valery G. Serbo and Ulrich D. Jentschura Novosibirsk State University, Novosibirsk, Russia Institut
Department of Natural Sciences Clayton State University. Physics 3650 Quiz 1
Physics 3650 Quiz 1 October 1, 009 Name SOLUTION 1. If the displacement of the object, x, is related to velocity, v, according to the relation x = A v, the constant, A, has the dimension of which of the
THE THEORY AND EXPERIMENTAL INVESTIGATION OF CONTROLLED SPONTANEOUS CONVERSION NUCLEAR DECAY OF RADIOACTIVE ISOTOPES
THE THEORY AND EXPERIMENTAL INVESTIGATION OF CONTROLLED SPONTANEOUS CONVERSION NUCLEAR DECAY OF RADIOACTIVE ISOTOPES V.I. VYSOTSKII Kiev Shevchenko University, Kiev, Ukraine A.A. KORNILOVA, YU. D. PERFILIEV
STATUS OF HIRFL-CSR PROJECT *
STATUS OF HIRFL-CSR PROJECT * Y.J. Yuan #, H.W. Zhao, J.W. Xia, X.D. Yang, H.S. Xu and CSR Group Institute of Modern Physics(IMP), CAS, Lanzhou, 730000, P.R. China. Abstract The HIRFL-CSR project is a
V.G. Baryshevsky. Institute for Nuclear Problems, Belarusian State University, Minsk, Belarus
The phenomena of spin rotation and depolarization of highenergy particles in bent and straight crystals at Large Hadron Collider (LHC) and Future Circular Collider (FCC) energies and the possibility to
FUNDAMENTAL SHORT TIME-SCALE RELATIVISTIC PHYSICS: COLLECTIVE PHENOMENA. PARTICLE ACCELERATION AND PRODUCTION IN FEMTOSECOND LASER-MATTER INTERACTION
FUNDAMENTAL SHORT TIME-SCALE RELATIVISTIC PHYSICS: COLLECTIVE PHENOMENA. PARTICLE ACCELERATION AND PRODUCTION IN FEMTOSECOND LASER-MATTER INTERACTION Anton Baldin Institute for Advanced Studies, Dubna
Conclusion. 109m Ag isomer showed that there is no such broadening. Because one can hardly
Conclusion This small book presents a description of the results of studies performed over many years by our research group, which, in the best period, included 15 physicists and laboratory assistants
Radiation and Radioactivity. PHYS 0219 Radiation and Radioactivity
Radiation and Radioactivity 1 Radiation and Radioactivity This experiment has four parts: 1. Counting Statistics 2. Gamma (g) Ray Absorption Half-length and shielding 3. 137 Ba Decay Half-life 4. Dosimetry
High-resolution study of Gamow- Teller transitions in pf-shell nuclei. Tatsuya ADACHI
High-resolution study of Gamow- Teller transitions in pf-shell nuclei Tatsuya ADACHI Type II supernova Electron Capture (EC) & β decay Neutrino induced reaction A Z-1X N+1 daughter EC β A ZX N parent (A,Z)
Final Exam Practice Solutions
Physics 390 Final Exam Practice Solutions These are a few problems comparable to those you will see on the exam. They were picked from previous exams. I will provide a sheet with useful constants and equations
How Electronics Started! And JLab Hits the Wall!
How Electronics Started! And JLab Hits the Wall! In electronics, a vacuum diode or tube is a device used to amplify, switch, otherwise modify, or create an electrical signal by controlling the movement
PHY492: Nuclear & Particle Physics. Lecture 4 Nature of the nuclear force. Reminder: Investigate
PHY49: Nuclear & Particle Physics Lecture 4 Nature of the nuclear force Reminder: Investigate www.nndc.bnl.gov Topics to be covered size and shape mass and binding energy charge distribution angular momentum
Two-stage Rydberg charge exchange in a strong magnetic field
Two-stage Rydberg charge exchange in a strong magnetic field M. L. Wall, C. S. Norton, and F. Robicheaux Department of Physics, Auburn University, Auburn, Alabama 36849-5311, USA Received 21 June 2005;
CHAPTER 12 TEST REVIEW
IB PHYSICS Name: Period: Date: # Marks: 76 Raw Score: IB Curve: DEVIL PHYSICS BADDEST CLASS ON CAMPUS CHAPTER 12 TEST REVIEW 1. An alpha particle is accelerated through a potential difference of 10 kv.
PHL424: Nuclear fusion
PHL424: Nuclear fusion Hot Fusion 5 10 15 5 10 8 projectiles on target compound nuclei 1 atom Hot fusion (1961 1974) successful up to element 106 (Seaborgium) Coulomb barrier V C between projectile and
Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia
Commun. Theor. Phys. (Beijing, China) 43 (005) pp. 709 718 c International Academic Publishers Vol. 43, No. 4, April 15, 005 Spin Cut-off Parameter of Nuclear Level Density and Effective Moment of Inertia
Chapter 2 Bremsstrahlung and Black Body
Chapter 2 Bremsstrahlung and Black Body 2.1 Bremsstrahlung We will follow an approximate derivation. For a more complete treatment see [2] and [1]. We will consider an electron proton plasma. Definitions:
Cross-section Measurements of Relativistic Deuteron Reactions on Copper by Activation Method
Nuclear Physics Institute, Academy of Sciences of the Czech Republic Department of Nuclear Reactors, Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague Cross-section
Nuclear Spectroscopy: Radioactivity and Half Life
Particle and Spectroscopy: and Half Life 02/08/2018 My Office Hours: Thursday 1:00-3:00 PM 212 Keen Building Outline 1 2 3 4 5 Some nuclei are unstable and decay spontaneously into two or more particles.
Atomic Structure, Periodic Table, and Other Effects: Chapter 8 of Rex and T. Modern Physics
Atomic Structure, Periodic Table, and Other Effects: Chapter 8 of Rex and T Modern Physics 11/16 and 11/19/2018 1 Introduction In Chapter 7, we studied the hydrogen atom. What about other elements, e.g.,
NMR Dynamics and Relaxation
NMR Dynamics and Relaxation Günter Hempel MLU Halle, Institut für Physik, FG Festkörper-NMR 1 Introduction: Relaxation Two basic magnetic relaxation processes: Longitudinal relaxation: T 1 Relaxation Return
P627/Chem 542 Surface/Interface Science Spring 2013 Rutherford Backscattering Lab: Answers to Questions
Intro Questions: 1) How is a tandem ion accelerator different from a so-called van der Graaf accelerator, and what are some of the advantages (and drawbacks) of the tandem design? A tandem ion accelerator
Opportunities with collinear laser spectroscopy at DESIR:
Opportunities with collinear laser spectroscopy at DESIR: the LUMIERE facility GOALS of LUMIERE experiments: Gerda Neyens, K.U. Leuven, Belgium (1) measure ground state properties of exotic isotopes: (see
Colliding Crystalline Beams
BNL-65137 Colliding Crystalline Beams J. Wei BNL A.M. Sessler LBNL June 1998 RHIC Project Brookhaven National Laboratory Operated by Brookhaven Science Associates Upton NY 11973 Under Contract with the
Selected Topics in Physics a lecture course for 1st year students by W.B. von Schlippe Spring Semester 2007
Selected Topics in Physics a lecture course for 1st year students by W.B. von Schlippe Spring Semester 2007 Lecture 11 1.) Determination of parameters of the SEMF 2.) α decay 3.) Nuclear energy levels
The Windowless Gaseous Tritium Source of KATRIN
The Windowless Gaseous Tritium Source of KATRIN W. Käfer, for the KATRIN Collaboration Karlsruhe Institute of Technology International School for Nuclear Physics: Neutrinos in Astro- Particle- and Nuclear
Cold Metastable Neon Atoms Towards Degenerated Ne*- Ensembles
Cold Metastable Neon Atoms Towards Degenerated Ne*- Ensembles Supported by the DFG Schwerpunktprogramm SPP 1116 and the European Research Training Network Cold Quantum Gases Peter Spoden, Martin Zinner,
ª 10 KeV. In 2XIIB and the tandem mirrors built to date, in which the plug radius R p. ª r Li
Axisymmetric Tandem Mirrors: Stabilization and Confinement Studies R. F. Post, T. K. Fowler*, R. Bulmer, J. Byers, D. Hua, L. Tung Lawrence Livermore National Laboratory *Consultant, Presenter This talk
NMR: Formalism & Techniques
NMR: Formalism & Techniques Vesna Mitrović, Brown University Boulder Summer School, 2008 Why NMR? - Local microscopic & bulk probe - Can be performed on relatively small samples (~1 mg +) & no contacts
LEAP, Kanazawa, Japan 2016
Klaus.blaum@mpi-hd.mpg.de LEAP, Kanazawa, Japan 2016 Precision atomic and nuclear masses and their importance for nuclear structure, astrophysics and fundamental studies Motivation for precision mass data
Nonstatistical fluctuations for deep inelastic processes
Nonstatistical fluctuations for deep inelastic processes in 27 Al + 27 Al collision Introduction Experimental procedures Cross section excitation functions (EFs) 1. Statistical analysis (a) Energy autocorrelation