(Positron Annihilation Lifetime Spectroscopy; PALS) 1) 4) PALS

Size: px
Start display at page:

Download "(Positron Annihilation Lifetime Spectroscopy; PALS) 1) 4) PALS"

Transcription

1 A positron probe micro analyzer (PPMA) has been developed in AIST. When a positron microbeam is injected into a specimen, radiations including secondary electrons, back scattered positrons, and annihilation gamma-rays are emitted from the beam injected point. In the PPMA, these radiations are detected to characterize small area of specimens. We report on details of designs and specifications of the PPMA. Key words: positron probe micro analyzer, positron microscope, positron microbeam, positron annihilation lifetime spectroscopy 1. g Development of a Positron Probe Micro Analyzer with a High Intensity Positron Beam Nagayasu OH=>B6, Ryoichi SJOJ@>, Toshiyuki O=96>G6, and Atsushi K>CDBJG6 (Research Institute of Instrumentation Frontier (RIIF), National Institute for Advanced Industrial Science and Technology (AIST)) Takamitsu N6GJB> and Akira U:9DCD (Graduate School of Pure and Applied Science, University of Tsukuba) Masanori FJ?>C6B> (Department of Applied Chemistry, Chiba University) TEX: (45203) FAX: nagayasu-oshima@aist.go.jp (Positron Annihilation Lifetime Spectroscopy; PALS) 1)4) PALS PALS 1mm mm 5)7) (Positron Probe Micro Analyzer; PPMA) PPMA PALS (2008) 39

2 PPMA (RI) 12 PPMA PPMA 57) 8) 9) PPMA 2. PALS PALS PALS b RI 1) 1MBq 22 Na Na g (1.3 MeV) g (0.5 MeV) 200 ps PALS RI 23 mm (110 mm 2 ) RI b 0 E max b 17E max (MeV) 1.43 (cm 2 /g) 10) E max RI 1 MeV 22 Na 0.5 MeV r110 g/cm mm RI PALS mm 3 RI PALS 1mm 0.1 mm ev RI 200 ps 200 ps RI 40 (0.530 kev) PALS 40 E(keV) 1.6 /r (g/cm 3 )nm E0.530 kev 10 nm 1 mm 11) RI (0.11 GBq) 510 mm kev 10 3 mm 3 PALS ( 100 mm 2 ) RI 10 mm PALS 1 mm 2 3. PPMA PPMA (Electron Probe Micro Analyzer; EPMA) 12) PPMA EPMA 2 PPMA 2 g g PALS EPMA 2 PPMA MeV 100 pps 3 ma 1 mm X 13) ev 10 7 e /s RI 12

3 1 PPMA 2 1 ms 100 pps ms 1 ms ms 10 mm 0.1 mt 10 ev 1 ms ms 13) ns 2ns 150 MHz 300 ps 14), 15) mm 1mm 1mm 200 nm 200 ps 2 XY 2 MCPBaF 2 3 MCP 2 MCP BaF 2 g MCP PC 85 (2008) 41

4 5 (1) 3 PPMA 2 4(b) 10 16) 10 d2r d min 2r min r 2 min 2 E r a E e 2 /8mBr 2 2 a E (1) 4 2 (a) (b) (L 2 /L 1 ) PPMA 11) 4(a) (1/10) e m a E E B 5 5 E B E 0.11 ev E (in situ) B 1 1 1mT 6 PPMA (1) (E 0.1 ev, E10 kev, B1 mt, a0.1) d min 30 mm 5. PPMA MCP 1 7 MCP 1mm 1mm

5 6 1 1mT mm 7 1 MCP 1mm 9 PPMA Ta SiO ps 500 cps 2 Ta SiO ) Ta/SiO 2 8 E5 kev 100 mm PPMA 0.01 mm 2 PALS 100 mm kev 10 7 mm 3 10 mm RI PALS PPMA ps PALS 500 cps RI ps ) 10 ps 20/ 1,024 (32 pixel32 pixel) 6 6. PPMA 200 ps 500 cps PALS 85 (2008) 43

6 100 mm mm SiO 2 1,600 (40 pixel40 pixel) 2 PPMA Cao Xingzhong He Chunqing 1) (1993). 2) 84, 3(2007). 3) 83, 2(2007). 4) 82, 2(2007). 5) H. Greif, M. Haaks, U. Holzwarth, U. Männig, M. Tongbhoyai, T. Wider, K. Maier, J. Bihr, and B. Huber, Appl. Phys. Lett., 71, 2115 (1997). 6) A. David, G. Kögel, P. Sperr, and W. Triftshäuser, Phys. Rev. Lett., 87, (2001). 7) /press2007/p /index.html 8) Cao Xingzhong p. 971 (2007). 9) p. 162 (2007). 10) ). 11) P. J. Schultz and K. G. Lynn, Rev. Mod. Phys., 60, 701 (1988). 12) EPMA 2001). 13) T. Akahane, T. Chiba, N. Shiotani, S. Tanigawa, T. Mikado, R. Suzuki, M. Chiwaki, T. Yamazaki, and T. Tomimasu, Appl. Phys. A, 51, 146 (1990). 14) R. Suzuki, Y. Kobayashi, T. Mikado, H. Ohgaki, M. Chiwaki, T. Yamazaki, and T. Tomimasu, Jpn. J. Appl. Phys., 30, L532 (1991). 15) R. Suzuki, T. Ohdaira, and T. Mikado, Rad. Phys. Chem., 48, 603 (2000). 16) D. M. Chen, K. G. Lynn, R. Pareja, and Bent Nielsen, Phys. Rev. B, 31, 4123 (1985). 17) R. Suzuki, T. Mikado, H. Ohgaki, M. Chiwaki, and T. Yamazaki, Material Science Forum, , 217 (1995). 44

Positron Probe Microanalyzer (PPMA) facilities at AIST

Positron Probe Microanalyzer (PPMA) facilities at AIST Positron Probe Microanalyzer (PPMA) and other accelerator based slow positron facilities at AIST B. E. O Rourke, N. Oshima, A. Kinomura, T. Ohdaira and R. Suzuki National Institute of Advanced Industrial

More information

Determination of the timing properties of a pulsed positron lifetime beam by the application of an electron gun and a fast microchannel plate

Determination of the timing properties of a pulsed positron lifetime beam by the application of an electron gun and a fast microchannel plate Applied Surface Science 252 (2006) 3148 3153 www.elsevier.com/locate/apsusc Determination of the timing properties of a pulsed positron lifetime beam by the application of an electron gun and a fast microchannel

More information

Positron Beam Lifetime Spectroscopy at

Positron Beam Lifetime Spectroscopy at UCRL-JC-124616 PREPRINT Positron Beam Lifetime Spectroscopy at Lawrence Livermore National Laboratory R. Howell T. Cowan J. Hartley P. Stern This paper was prepared for submittal to the 14th International

More information

Outlook: Application of Positron Annihilation for defects investigations in thin films. Introduction to Positron Annihilation Methods

Outlook: Application of Positron Annihilation for defects investigations in thin films. Introduction to Positron Annihilation Methods Application of Positron Annihilation for defects investigations in thin films V. Bondarenko, R. Krause-Rehberg Martin-Luther-University Halle-Wittenberg, Halle, Germany Outlook: Introduction to Positron

More information

Positron and Positronium Annihilation in Polymers Studied by Age-Momentum Correlation Spectroscopy

Positron and Positronium Annihilation in Polymers Studied by Age-Momentum Correlation Spectroscopy Vol. 113 (2008) ACTA PHYSICA POLONICA A No. 5 Proceedings of the 37th Polish Seminar on Positron Annihilation, L adek-zdrój 2007 Positron and Positronium Annihilation in Polymers Studied by Age-Momentum

More information

Positron Annihilation Spectroscopy - A non-destructive method for material testing -

Positron Annihilation Spectroscopy - A non-destructive method for material testing - Maik Butterling Institute of Radiation Physics http://www.hzdr.de Positron Annihilation Spectroscopy - A non-destructive method for material testing - Maik Butterling Positron Annihilation Spectroscopy

More information

David B. Cassidy. Department of Physics and Astronomy, University of California, Riverside, USA. Varenna, July 09

David B. Cassidy. Department of Physics and Astronomy, University of California, Riverside, USA. Varenna, July 09 Experimental production of many- positron systems: L2, techniques David B. Cassidy Department of Physics and Astronomy, University of California, Riverside, USA cassidy@physics.ucr.edu Varenna, July 09

More information

Study on Bose-Einstein Condensation of Positronium

Study on Bose-Einstein Condensation of Positronium Study on Bose-Einstein Condensation of Positronium K. Shu 1, T. Murayoshi 1, X. Fan 1, A. Ishida 1, T. Yamazaki 1,T. Namba 1,S. Asai 1, K. Yoshioka 2, M. Kuwata-Gonokami 1, N. Oshima 3, B. E. O Rourke

More information

Application of positrons in materials research

Application of positrons in materials research Application of positrons in materials research Trapping of positrons at vacancy defects Using positrons, one can get defect information. R. Krause-Rehberg and H. S. Leipner, Positron annihilation in Semiconductors,

More information

Identification of Getter Defects in high-energy self-implanted Silicon at Rp/2

Identification of Getter Defects in high-energy self-implanted Silicon at Rp/2 Identification of Getter Defects in high-energy self-implanted Silicon at Rp R. Krause-Rehberg 1, F. Börner 1, F. Redmann 1, J. Gebauer 1, R. Kögler 2, R. Kliemann 2, W. Skorupa 2, W. Egger 3, G. Kögel

More information

in Si by means of Positron Annihilation

in Si by means of Positron Annihilation Investigation of the Rp/2 /2-effect in Si by means of Positron Annihilation R. Krause-Rehberg, F. Börner, F. Redmann Universität Halle Martin-Luther-Universität R. Kögler, W. Skorupa Forschungszentrum

More information

Positron Annihilation Lifetime Spectroscopy (PALS)

Positron Annihilation Lifetime Spectroscopy (PALS) Positron Annihilation Lifetime Spectroscopy (PALS) Javier Puertas 12/12/12 Contents 1. Introduction. 1.1. General idea of the process. 3. PALS: Experimental results. 1.2. What is a positron? 3.1. Math.

More information

DEVELOPMENT OF A NEW POSITRON LIFETIME SPECTROSCOPY TECHNIQUE FOR DEFECT CHARACTERIZATION IN THICK MATERIALS

DEVELOPMENT OF A NEW POSITRON LIFETIME SPECTROSCOPY TECHNIQUE FOR DEFECT CHARACTERIZATION IN THICK MATERIALS Copyright JCPDS - International Centre for Diffraction Data 2004, Advances in X-ray Analysis, Volume 47. 59 DEVELOPMENT OF A NEW POSITRON LIFETIME SPECTROSCOPY TECHNIQUE FOR DEFECT CHARACTERIZATION IN

More information

POSITRON AND POSITRONIUM INTERACTIONS WITH CONDENSED MATTER. Paul Coleman University of Bath

POSITRON AND POSITRONIUM INTERACTIONS WITH CONDENSED MATTER. Paul Coleman University of Bath POSITRON AND POSITRONIUM INTERACTIONS WITH CONDENSED MATTER Paul Coleman University of Bath THE FATE OF POSITRONS IN CONDENSED MATTER POSITRON-SURFACE INTERACTIONS positron backscattering BACKSCATTERED

More information

Research Center Dresden Rossendorf

Research Center Dresden Rossendorf News of the EPOS Project at the ELBE Radiation Source in the Research Center Dresden Rossendorf EPOS-Team & R. Krause-Rehberg Extended Concept of EPOS Progress of the mono-energetic Positron Beam (MePS)

More information

PHYS 3650L - Modern Physics Laboratory

PHYS 3650L - Modern Physics Laboratory PHYS 3650L - Modern Physics Laboratory Laboratory Advanced Sheet Photon Attenuation 1. Objectives. The objectives of this laboratory exercise are: a. To measure the mass attenuation coefficient at a gamma

More information

Positronium Formation at Low Temperatures in Polymers and Other Molecular Solids

Positronium Formation at Low Temperatures in Polymers and Other Molecular Solids Vol. 107 (2005) ACTA PHYSICA POLONICA A No. 4 Proceedings of the 35th Polish Seminar on Positron Annihilation, Turawa, Poland 2004 Positronium Formation at Low Temperatures in Polymers and Other Molecular

More information

Laboratory of Nuclear Solid State Physics, USTC

Laboratory of Nuclear Solid State Physics, USTC IV Laboratory of Nuclear Solid State Physics, USTC 5. e+e e+e- 2 180 180 e+e e+e- 2 CDB CDB, 2D 2D-ACAR ACAR e+ e+-e- CDB CDB 2D 2D-ACAR 1 = x y ρ 2γ z N ( p, p ) ( p) dp γ D ( p ) ρ ( p) dp z = 2 y dp

More information

MT Electron microscopy Scanning electron microscopy and electron probe microanalysis

MT Electron microscopy Scanning electron microscopy and electron probe microanalysis MT-0.6026 Electron microscopy Scanning electron microscopy and electron probe microanalysis Eero Haimi Research Manager Outline 1. Introduction Basics of scanning electron microscopy (SEM) and electron

More information

Hierarchical Dynamics of Soft Matters & Prospects of Japanese Future Light Sources

Hierarchical Dynamics of Soft Matters & Prospects of Japanese Future Light Sources XDL Workshop 6 @ Cornell Univ. Hierarchical Dynamics of Soft Matters & Prospects of Japanese Future Light Sources Yuya Shinohara Department of Advanced Materials Science, Graduate School of Frontier Sciences,

More information

Study on Positronium Bose-Einstein Condensation

Study on Positronium Bose-Einstein Condensation 3rd China-Japan Joint Workshop on Positron Science (JWPS2017) https://doi.org/10.7567/jjapcp.7.011001 Study on Positronium Bose-Einstein Condensation Akira Ishida 1, Kenji Shu 1, Tomoyuki Murayoshi 1,XingFan

More information

Positron Annihilation in Material Research

Positron Annihilation in Material Research Positron Annihilation in Material Research Introduction Positron sources, positron beams Interaction of positrons with matter Annihilation channels: Emission of 1, 2 or 3 γ-quanta Annihilation spectroscopies:

More information

Study on positronium Bose-Einstein condensation

Study on positronium Bose-Einstein condensation Study on positronium Bose-Einstein condensation Akira Ishida a,*, K. Shu a, T. Murayoshi a, X. Fan a, T. Namba a,s. Asai a, K. Yoshioka b, M. Kuwata-Gonokami a, N. Oshima c, B. E. O Rourke c, R. Suzuki

More information

STRESS ANALYSIS USING BREMSSTRAHLUNG RADIATION

STRESS ANALYSIS USING BREMSSTRAHLUNG RADIATION Copyright JCPDS - International Centre for Diffraction Data 2003, Advances in X-ray Analysis, Volume 46. 106 STRESS ANALYSIS USING BREMSSTRAHLUNG RADIATION F. A. Selim 1, D.P. Wells 1, J. F. Harmon 1,

More information

Trap-based positron beams

Trap-based positron beams Applied Surface Science 194 (2002) 56 60 Trap-based positron beams R.G. Greaves a,*, S.J. Gilbert b, C.M. Surko b a First Point Scientific Inc., 5330 Derry Avenue, Suite J, Agoura Hills, CA 91301, USA

More information

New Concept of EPOS Progress of the Mono-energetic Positron Beam (MePS) Gamma-induced Positron Spectroscopy (GiPS)

New Concept of EPOS Progress of the Mono-energetic Positron Beam (MePS) Gamma-induced Positron Spectroscopy (GiPS) Progress of the EPOS Project: Gamma Induced Positron Spectroscopy (GiPS) R. Krause-Rehberg 1,*,W.Anwand 2,G.Brauer 2, M. Butterling 1,T.Cowan 2,M. Jungmann 1, A. Krille 1, R. Schwengner 2, A. Wagner 2

More information

Measurement and Analysis of the Positron Annihilation Lifetime Spectra for Mesoporous Silica

Measurement and Analysis of the Positron Annihilation Lifetime Spectra for Mesoporous Silica Vol. 110 (2006) ACTA PHYSICA POLONICA A No. 5 Proceedings of the 36th Polish Seminar on Positron Annihilation, Turawa, Poland, 2006 Measurement and Analysis of the Positron Annihilation Lifetime Spectra

More information

The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf

The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf The intense, pulsed positron source EPOS at the Research Centre Dresden-Rossendorf The EPOS Team and R. Krause-Rehberg Martin-Luther University, Halle-Wittenberg, Dept. of Physics, 06099 Halle / Germany

More information

Introduction into Positron Annihilation

Introduction into Positron Annihilation Introduction into Positron Annihilation Introduction (How to get positrons? What is special about positron annihilation?) The methods of positron annihilation (positron lifetime, Doppler broadening, ACAR...)

More information

Slow-Positron-Beam Techniques

Slow-Positron-Beam Techniques Slow-Positron-Beam Techniques 1 Slow-Positron-Beam Techniques The main advantage of the conventional sample source sandwich arrangement is that the emitted positrons immediately penetrate the sample. A

More information

Study of semiconductors with positrons. Outlook:

Study of semiconductors with positrons. Outlook: Study of semiconductors with positrons V. Bondarenko, R. Krause-Rehberg Martin-Luther-University Halle-Wittenberg, Halle, Germany Introduction Positron trapping into defects Methods of positron annihilation

More information

Application of laser Compton photon beam to nondestructive tests

Application of laser Compton photon beam to nondestructive tests Research paper Application of laser Compton photon beam to nondestructive tests - A spin-off technology from nuclear physics- Hiroyuki Toyokawa [Translation from Synthesiology, Vol.8, No.2, p.89-96 (2015)]

More information

13th International Workshop on Slow Positron Beam Techniques and Applications

13th International Workshop on Slow Positron Beam Techniques and Applications Positronium and positronium negative ion emission from alkali-metal coated tungsten surfaces Y Nagashima 1, K Michishio 1, H Terabe 1, R H Suzuki 1, S Iida 1, T Yamashita 1, R Kimura 1, T Tachibana 2,

More information

Investigation of SiC by Positrons

Investigation of SiC by Positrons nd/march/000/erlangen Investigation of SiC by Positrons Atsuo KAWASUSO Martin-Luther-Universität Halle-Wittenberg (Humboldt Research Fellow) Japan Atomic Energy Research Institute Takasaki Establishment

More information

Department of Physics, Techno India Batanagar (Techno India Group), Kolkata , West Bengal, India.

Department of Physics, Techno India Batanagar (Techno India Group), Kolkata , West Bengal, India. Department of Physics, Techno India Batanagar (Techno India Group), Kolkata 700141, West Bengal, India. Visiting Scientists @ SINP, @VECC, @ IIEST Kolkata, India. nn.mondal2011@gmail.com, nagendra.n.mondal@biemsindia.org

More information

Effects of Si doping on optical properties of GaN epitaxial layers

Effects of Si doping on optical properties of GaN epitaxial layers (123) 31 Effects of Si doping on optical properties of GaN epitaxial layers Chiharu SASAKI (Department of Electrical and Electronic Engineering) Tatsuya YAMASHITA (Department of Electrical and Electronic

More information

Positron Annihilation Spectroscopy

Positron Annihilation Spectroscopy Positron Annihilation Spectroscopy (1) Angular Correlation θ N x, y = p x, y m C θ γ-ray (511keV ± E) 0 (2) Doppler Broadening Cp E = z 2 θ N p ~100µm 22 Na (e + Source) e - e + ~ 10-12 s Sample γ-ray

More information

Repeatability of Spectral Intensity Using an Auger Electron Spectroscopy Instrument Equipped with a Cylindrical Mirror Analyzer

Repeatability of Spectral Intensity Using an Auger Electron Spectroscopy Instrument Equipped with a Cylindrical Mirror Analyzer A. Kurokawa et al. Repeatability of Spectral Intensity Using an Auger lectron Spectroscopy Instrument quipped with a Cylindrical Mirror Analyzer Paper Repeatability of Spectral Intensity Using an Auger

More information

ATHENA / AD-1. First production and detection of cold antihydrogen atoms. ATHENA Collaboration. Rolf Landua CERN

ATHENA / AD-1. First production and detection of cold antihydrogen atoms. ATHENA Collaboration. Rolf Landua CERN ATHENA / AD-1 First production and detection of cold antihydrogen atoms ATHENA Collaboration Rolf Landua CERN 1 LONG TERM PHYSICS GOALS Antihydrogen = Hydrogen? CPT Gravity But... 2 FIRST GOAL PRODUCTION

More information

ABNORMAL X-RAY EMISSION FROM INSULATORS BOMBARDED WITH LOW ENERGY IONS

ABNORMAL X-RAY EMISSION FROM INSULATORS BOMBARDED WITH LOW ENERGY IONS 302 ABNORMAL X-RAY EMISSION FROM INSULATORS BOMBARDED WITH LOW ENERGY IONS M. Song 1, K. Mitsuishi 1, M. Takeguchi 1, K. Furuya 1, R. C. Birtcher 2 1 High Voltage Electron Microscopy Station, National

More information

CPT ALPHA CPT 2.1 CPT , CERN. TRIUMF Canada s National Laboratory for Particle and Nuclear Physics

CPT ALPHA CPT 2.1 CPT , CERN. TRIUMF Canada s National Laboratory for Particle and Nuclear Physics 258 501 ALPHA (CERN) CPT, CERN ishida@icepp.s.u-tokyo.ac.jp TRIUMF Canada s National Laboratory for Particle and Nuclear Physics Makoto.Fujiwara@triumf.ca 2015 2 26 ( H ) (p ) ( e + ) CPT ( ) CERN (AD;

More information

In Situ Observation of Damage Evolution in Polycarbonate under Ion Irradiation with Positrons

In Situ Observation of Damage Evolution in Polycarbonate under Ion Irradiation with Positrons Proc. 2nd Japan-China Joint Workshop on Positron Science JJAP Conf. Proc. 2 (2014) 011103 2014 The Japan Society of Applied Physics In Situ Observation of Damage Evolution in Polycarbonate under Ion Irradiation

More information

The MePS System at Helmholtz-Zentrum Dresden-Rossendorf and its special Capability for Positronium Lifetime Spectroscopy

The MePS System at Helmholtz-Zentrum Dresden-Rossendorf and its special Capability for Positronium Lifetime Spectroscopy The MePS System at Helmholtz-Zentrum Dresden-Rossendorf and its special Capability for Positronium Lifetime Spectroscopy R. Krause-Rehberg and many colleagues of Univ. Halle and HZDR Martin-Luther University

More information

Positron Facilities in Europe

Positron Facilities in Europe Positron Facilities in Europe W. Triftshäuser To cite this version: W. Triftshäuser. Positron Facilities in Europe. Journal de Physique IV Colloque, 1995, 05 (C1), pp.c1-217-c1-226. .

More information

Measurements of the Deuterium-Tritium Branching Ratio Using ICF Implosions

Measurements of the Deuterium-Tritium Branching Ratio Using ICF Implosions 1 IFE/P6-11 Measurements of the Deuterium-Tritium Branching Ratio Using ICF Implosions Y. Kim 1), H.W. Herrmann 1), J.M. Mack 1), C.S. Young 1), J.R. Langenbrunner 1), S. Evans 1), T. Sedillo 1), A.M.

More information

GBAR Project Gravitational Behavior of Antihydrogen at Rest

GBAR Project Gravitational Behavior of Antihydrogen at Rest GBAR Project Gravitational Behavior of Antihydrogen at Rest Pierre Dupré CEA Saclay, FRANCE 1 Contents Motivation Scheme Schedule 2 Motivation A direct test of the Equivalence Principle with antimatter

More information

Motivation. g-spectroscopy deals with g-ray detection and is one of the most relevant methods to investigate excited states in nuclei.

Motivation. g-spectroscopy deals with g-ray detection and is one of the most relevant methods to investigate excited states in nuclei. Motivation Spins and excited states of double-magic nucleus 16 O Decay spectra are caused by electro-magnetic transitions. g-spectroscopy deals with g-ray detection and is one of the most relevant methods

More information

ASPECTS OF THE MCMASTER INTENSE POSITRON BEAM FACILITY

ASPECTS OF THE MCMASTER INTENSE POSITRON BEAM FACILITY ASPECTS OF THE MCMASTER INTENSE POSITRON BEAM FACILITY ASPECTS OF THE MCMASTER INTENSE POSITRON BEAM FACILITY (MIPBF) By PEIHAI LI M.Eng., B.Sc. A Thesis Submitted to the School of Graduate Studies in

More information

High-temperature In-situ Measurements of Thermal Vacancies in a TiAl Intermetallic Compound using a Desktop Positron Beam

High-temperature In-situ Measurements of Thermal Vacancies in a TiAl Intermetallic Compound using a Desktop Positron Beam 3rd China-Japan Joint Workshop on Positron Science (JWPS217) JJAP Conf. Proc. 7, https://doi.org/1.7567/jjapcp.7.1112 High-temperature In-situ Measurements of Thermal Vacancies in a TiAl Intermetallic

More information

High energy X-ray vortex generation using inverse Compton scattering

High energy X-ray vortex generation using inverse Compton scattering 22nd International Spin Symposium 9/28/216 High energy X-ray vortex generation using inverse Compton scattering Yoshitaka Taira National Institute of Advanced Industrial Science and Technology (AIST),

More information

1. Introduction Zhe Chen 1,2,, Zhi Wang 1,2,QiumingFu 1,2, Zhibin Ma 1,2, Pengfei Fang 3, and Chunqing He 3. (Received March 10, 2014)

1. Introduction Zhe Chen 1,2,, Zhi Wang 1,2,QiumingFu 1,2, Zhibin Ma 1,2, Pengfei Fang 3, and Chunqing He 3. (Received March 10, 2014) Proc. 2nd Japan-China Joint Workshop on Positron Science JJAP Conf. Proc. 2 (2014) 011202 2014 The Japan Society of Applied Physics Microstructure and Surface State of Plasma-treated High-density Polyethylene

More information

CHAPTER-II Experimental Techniques and Data Analysis (Positron annihilation spectroscopy)

CHAPTER-II Experimental Techniques and Data Analysis (Positron annihilation spectroscopy) CHAPTER-II Experimental Techniques and Data Analysis (Positron annihilation spectroscopy) 64 Techniques in Positron annihilation spectroscopy PAS comprises of different techniques which provide information

More information

on basis of the Geant4 simulations

on basis of the Geant4 simulations Optimization of BaF 2 PAL-spectrometer geometry on basis of the Geant4 simulations L.Yu. Dubov 2, V.I. Grafutin 1, Yu.V. Funtikov 1, Yu.V. Shtotsky 2, L.V. Elnikova 1 1 FSBI RF SSC Institute for Theoretical

More information

Supplementary Information for. Effect of Interface on Surface Morphology and Proton Conduction of Polymer Electrolyte Thin Films

Supplementary Information for. Effect of Interface on Surface Morphology and Proton Conduction of Polymer Electrolyte Thin Films Supplementary Information for Effect of Interface on Surface Morphology and Proton Conduction of Polymer Electrolyte Thin Films Akihiro Ohira* a,b, Seiichi. Kuroda* b, Hamdy F. M. Mohamed b,c, and Bruno

More information

Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL

Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL Development of Cs 2 Te photocathode RF gun system for compact THz SASE-FEL R. Kuroda, H. Ogawa, N. Sei, H. Toyokawa, K. Yagi-Watanabe, M. Yasumoto, M. Koike, K. Yamada, T. Yanagida*, T. Nakajyo*, F. Sakai*

More information

Progress in using prompt gammas for ion range monitoring during hadrontherapy

Progress in using prompt gammas for ion range monitoring during hadrontherapy Progress in using prompt gammas for ion range monitoring during hadrontherapy J. Krimmer 1, M. Chevallier 1, J. Constanzo 1, M. Dahoumane 1, D. Dauvergne 1, M. De Rydt 1,2, G. Dedes 1, N. Freud 3, J.M.

More information

OBSERVATION OF TRANSVERSE- LONGITUDINAL COUPLING EFFECT AT UVSOR-II

OBSERVATION OF TRANSVERSE- LONGITUDINAL COUPLING EFFECT AT UVSOR-II OBSERVATION OF TRANSVERSE- LONGITUDINAL COUPLING EFFECT AT UVSOR-II The 1st International Particle Accelerator Conference, IPAC 10 Kyoto International Conference Center, May 23-28, 2010 M. Shimada (KEK),

More information

Laser heating of noble gas droplet sprays: EUV source efficiency considerations

Laser heating of noble gas droplet sprays: EUV source efficiency considerations Laser heating of noble gas droplet sprays: EUV source efficiency considerations S.J. McNaught, J. Fan, E. Parra and H.M. Milchberg Institute for Physical Science and Technology University of Maryland College

More information

positron source EPOS - general concept - timing system - digital lifetime measurement

positron source EPOS - general concept - timing system - digital lifetime measurement The pulsed high-brightness positron source EPOS R. Krause-Rehberg 1, G. Brauer 2, A. Krille 1, M. Jungmann 1, S. Sachert 1, A. Rogov 2, K. Nowak 2 1 Martin-Luther-University Halle, Germany 2 Research Center

More information

Basics and Means of Positron Annihilation

Basics and Means of Positron Annihilation Basics and Means of Positron Annihilation Positron history Means of positron annihilation positron lifetime spectroscopy angular correlation Doppler-broadening spectroscopy Near-surface positron experiments:

More information

Physics of Radioactive Decay. Purpose. Return to our patient

Physics of Radioactive Decay. Purpose. Return to our patient Physics of Radioactive Decay George Starkschall, Ph.D. Department of Radiation Physics U.T. M.D. Anderson Cancer Center Purpose To demonstrate qualitatively the various processes by which unstable nuclides

More information

Modeling Electron Emission From Diamond-Amplified Cathodes

Modeling Electron Emission From Diamond-Amplified Cathodes Modeling Electron Emission From Diamond-Amplified Cathodes D. A. Dimitrov Tech-X Corporation, Boulder, CO I. Ben-Zvi, T. Rao, J. Smedley, E. Wang, X. Chang Brookhaven National Lab, NY This work is funded

More information

Quantum Condensed Matter Physics Lecture 12

Quantum Condensed Matter Physics Lecture 12 Quantum Condensed Matter Physics Lecture 12 David Ritchie QCMP Lent/Easter 2016 http://www.sp.phy.cam.ac.uk/drp2/home 12.1 QCMP Course Contents 1. Classical models for electrons in solids 2. Sommerfeld

More information

Possibilities for a Bose-Einstein Condensed Positronium Annihilation Gamma Ray Laser

Possibilities for a Bose-Einstein Condensed Positronium Annihilation Gamma Ray Laser Possibilities for a Bose-Einstein Condensed Positronium Annihilation Gamma Ray Laser Allen Mills, Jr., University of California Riverside in collaboration with David Cassidy and Harry Tom (UCR) Rod Greaves

More information

Positron theoretical prediction

Positron theoretical prediction Positron theoretical prediction Schrödinger equation: ˆ 2 p x, t Vx, t x, t i 22 m tt non-relativistic equation of motion for electron Erwin Schrödinger 1933 Nobel prize Positron theoretical prediction

More information

Intense Slow Positron Source

Intense Slow Positron Source Intense Slow Positron Source Introduction Science & Frontier Technology Production of e + Competition Proposal Request to EPAC ~ 14 m 10 MeV rhodotron target - collector moderator - buffer gas - trap e+

More information

Material Science using Positron Annihilation

Material Science using Positron Annihilation Material Science using Positron Annihilation R. Krause-Rehberg Universität Halle, Inst. für Physik 9.3.2018 Some historical remarks Techniques of Positron Annihilation Study of Defects in Semiconductors

More information

MT Electron microscopy Scanning electron microscopy and electron probe microanalysis

MT Electron microscopy Scanning electron microscopy and electron probe microanalysis MT-0.6026 Electron microscopy Scanning electron microscopy and electron probe microanalysis Eero Haimi Research Manager Outline 1. Introduction Basics of scanning electron microscopy (SEM) and electron

More information

Coulomb crystal extraction from an ion trap for application to nano-beam source"

Coulomb crystal extraction from an ion trap for application to nano-beam source Coulomb crystal extraction from an ion trap for application to nano-beam source" K. Ito, K. Izawa, H. Higaki and H. Okamoto,! Aadvanced Sciences of Matter, Hiroshima University,! 1-3-1 Kagamiyama, Higashi-Hiroshima,

More information

Nuclear Physics and Astrophysics

Nuclear Physics and Astrophysics Nuclear Physics and Astrophysics PHY-302 Dr. E. Rizvi Lecture 13 - Gamma Radiation Material For This Lecture Gamma decay: Definition Quantum interpretation Uses of gamma spectroscopy 2 Turn to γ decay

More information

The Standard Auger Electron Spectra in The AIST DIO-DB(111); Ge(111)

The Standard Auger Electron Spectra in The AIST DIO-DB(111); Ge(111) Paper The Standard Auger Electron Spectra in The AIST DIO-DB(111); Ge(111) K. Goto, a,* Adel Alkafri, b Y. Ichikawa, b A.Kurokawa, c and Y. Yamauchi a a AIST-Chubu Center, Anagahora 2266, Moriyama-ku,

More information

Reduced preferential sputtering of TiO 2 (and Ta 2 O 5 ) thin films through argon cluster ion bombardment.

Reduced preferential sputtering of TiO 2 (and Ta 2 O 5 ) thin films through argon cluster ion bombardment. NATIOMEM Reduced preferential sputtering of TiO 2 (and Ta 2 O 5 ) thin films through argon cluster ion bombardment. R. Grilli *, P. Mack, M.A. Baker * * University of Surrey, UK ThermoFisher Scientific

More information

The EPOS System (ELBE Positron Source) at Helmholtz Centre Dresden- Rossendorf and first experiments at photovoltaic CIGS layers

The EPOS System (ELBE Positron Source) at Helmholtz Centre Dresden- Rossendorf and first experiments at photovoltaic CIGS layers The EPOS System (ELBE Positron Source) at Helmholtz Centre Dresden- Rossendorf and first experiments at photovoltaic CIGS layers R. Krause-Rehberg 1, A. Wagner 2 and many colleagues of Univ. Halle and

More information

Formation of High-b ECH Plasma and Inward Particle Diffusion in RT-1

Formation of High-b ECH Plasma and Inward Particle Diffusion in RT-1 J Fusion Energ (2010) 29:553 557 DOI 10.1007/s10894-010-9327-6 ORIGINAL RESEARCH Formation of High-b ECH Plasma and Inward Particle Diffusion in RT-1 H. Saitoh Z. Yoshida J. Morikawa Y. Yano T. Mizushima

More information

New source of ultra-cold positron and electron beams

New source of ultra-cold positron and electron beams Nuclear Instruments and Methods in Physics Research B 143 (1998) 188±194 New source of ultra-cold positron and electron beams C. Kurz, S.J. Gilbert, R.G. Greaves, C.M. Surko * Dept. of Physics, University

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Detection of gamma photons using solution-grown single crystals of hybrid lead halide perovskites Sergii Yakunin, 1, 2 Dmitry N. Dirin, 1, 2 Yevhen Shynkarenko 1,3, Viktoriia Morad, 1 Ihor Cherniukh, 1

More information

Modeling of the secondary electron emission in rf photocathode guns

Modeling of the secondary electron emission in rf photocathode guns Modeling of the secondary electron emission in rf photocathode guns J.-H. Han, DESY Zeuthen 8 June 2004 Joint Uni. Hamburg and DESY Accelerator Physics Seminar Contents 1. Necessity of secondary electron

More information

Investigations on warm dense plasma with PHELIX facility

Investigations on warm dense plasma with PHELIX facility 2 nd EMMI Workshop on Plasma Physics with Intense Laser and Heavy Ion Beams, May 14-15, Moscow Investigations on warm dense plasma with PHELIX facility S.A. Pikuz Jr., I.Yu. Skobelev, A.Ya. Faenov, T.A.

More information

Supplementary Figures

Supplementary Figures Supplementary Figures Supplementary Figure. X-ray diffraction pattern of CH 3 NH 3 PbI 3 film. Strong reflections of the () family of planes is characteristics of the preferred orientation of the perovskite

More information

Medical Applications of Compact Laser-Compton Light Source

Medical Applications of Compact Laser-Compton Light Source Medical Applications of Compact Laser-Compton Light Source Y. Hwang 1, D. J. Gibson 2, R. A. Marsh 2, G. G. Anderson 2, T. Tajima 1, C. P. J. Barty 2 1 University of California, Irvine 2 Lawrence Livermore

More information

Interaction of Electrons with Matter and Comparison of the Obtained Results with Experimental Measurements

Interaction of Electrons with Matter and Comparison of the Obtained Results with Experimental Measurements Australian Journal of Basic and Applied Sciences, 5(): 83-80, 0 ISSN 99-878 Interaction of Electrons with Matter and Comparison of the Obtained Results with Experimental Measurements Somayeh Almasi Bigdelo,

More information

Digital Gamma-ray Spectroscopy & Imaging with Semiconductor detectors Frontiers of gamma-ray spectroscopy

Digital Gamma-ray Spectroscopy & Imaging with Semiconductor detectors Frontiers of gamma-ray spectroscopy Digital Gamma-ray Spectroscopy & Imaging with Semiconductor detectors Frontiers of gamma-ray spectroscopy AGATA GRETA Dr Andy Boston ajboston@liv.ac.uk And its applications The AGATA Concept Without Compton

More information

Exercise 1 Atomic line spectra 1/9

Exercise 1 Atomic line spectra 1/9 Exercise 1 Atomic line spectra 1/9 The energy-level scheme for the hypothetical one-electron element Juliettium is shown in the figure on the left. The potential energy is taken to be zero for an electron

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

Status of A Positron-Electron Experiment (APEX) towards the formation of pair plasmas

Status of A Positron-Electron Experiment (APEX) towards the formation of pair plasmas Status of A Positron-Electron Experiment (APEX) towards the formation of pair plasmas H. Saitoh 1,5, J. Stanja 1, T. Sunn Pedersen 1,3, U. Hergenhahn 1, E. V. Stenson 1, H. Niemann 1,3, N. Paschkowski

More information

Gamma-ray shielding of concretes including magnetite in different rate

Gamma-ray shielding of concretes including magnetite in different rate Vol. 8(8), pp. 310-314, 28 February, 2013 DOI: 10.5897/IJPS2013.3854 ISSN 1992-1950 2013 Academic Journals http://www.academicjournals.org/ijps International Journal of Physical Sciences Full Length Research

More information

? Physics with many Positrons

? Physics with many Positrons Varenna Summer School July 2009? Physics with many Positrons Positron Sources & Positron Beams Christoph Hugenschmidt Technische Universität München What is many? Galaxy: 1.5 10 43 e + /s! = 1 lake + 1

More information

A CdTe detector with a Gd converter for thermal neutron detection

A CdTe detector with a Gd converter for thermal neutron detection A CdTe detector with a Gd converter for thermal neutron detection Aki Miyake, Takahiro Nishika, Shailendra Singh, Hisashi Morii, Hidenori Minura, Toru Aoki. Nuclear Instruments and Methods in Physics Research

More information

Chapter 16 Basic Precautions

Chapter 16 Basic Precautions Chapter 16 Basic Precautions 16.1 Basic Principles of Radiation Protection The four basic methods used to control radiation exposure are time, distance, shielding, and contamination control. The first

More information

Travels with a Cyclotron. David Parker University of Birmingham

Travels with a Cyclotron. David Parker University of Birmingham Travels with a Cyclotron David Parker University of Birmingham Quick history Current uses of the cyclotron Transfer from Minneapolis 2 History of accelerators at Birmingham 60 Nuffield cyclotron (1948-1999)

More information

Inorganic Scintillators

Inorganic Scintillators Inorganic Scintillators Inorganic scintillators are inorganic materials (usually crystals) that emit light in response to ionizing radiation NaI is the protypical example Scintillation mechanism is different

More information

Thermal Radiation Studies for an Electron-Positron Annihilation Propulsion System

Thermal Radiation Studies for an Electron-Positron Annihilation Propulsion System Thermal Radiation Studies for an Electron-Positron Annihilation Propulsion System Jonathan A. Webb Embry Riddle Aeronautical University Prescott, AZ 8631 Recent studies have shown the potential of antimatter

More information

Passage of particles through matter

Passage of particles through matter Passage of particles through matter Alexander Khanov PHYS6260: Experimental Methods is HEP Oklahoma State University September 11, 2017 Delta rays During ionization, the energy is transferred to electrons

More information

Gamma ray coincidence and angular correlation

Gamma ray coincidence and angular correlation University of Cape Town Department of Physics Course III laboratory Gamma ray coincidence and angular correlation Introduction Medical imaging based on positron emission tomography (PET) continues to have

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

Depth Distribution Functions of Secondary Electron Production and Emission

Depth Distribution Functions of Secondary Electron Production and Emission Depth Distribution Functions of Secondary Electron Production and Emission Z.J. Ding*, Y.G. Li, R.G. Zeng, S.F. Mao, P. Zhang and Z.M. Zhang Hefei National Laboratory for Physical Sciences at Microscale

More information

Controllable Atomic Scale Patterning of Freestanding Monolayer. Graphene at Elevated Temperature

Controllable Atomic Scale Patterning of Freestanding Monolayer. Graphene at Elevated Temperature Controllable Atomic Scale Patterning of Freestanding Monolayer Graphene at Elevated Temperature AUTHOR NAMES Qiang Xu 1, Meng-Yue Wu 1, Grégory F. Schneider 1, Lothar Houben 2, Sairam K. Malladi 1, Cees

More information

β and γ decays, Radiation Therapies and Diagnostic, Fusion and Fission Final Exam Surveys New material Example of β-decay Beta decay Y + e # Y'+e +

β and γ decays, Radiation Therapies and Diagnostic, Fusion and Fission Final Exam Surveys New material Example of β-decay Beta decay Y + e # Y'+e + β and γ decays, Radiation Therapies and Diagnostic, Fusion and Fission Last Lecture: Radioactivity, Nuclear decay Radiation damage This lecture: nuclear physics in medicine and fusion and fission Final

More information

Scaling Hot-Electron Generation to High-Power, Kilojoule-Class Lasers

Scaling Hot-Electron Generation to High-Power, Kilojoule-Class Lasers Scaling Hot-Electron Generation to High-Power, Kilojoule-Class Lasers 75 nm 75 75 5 nm 3 copper target Normalized K b /K a 1.2 1.0 0.8 0.6 0.4 Cold material 1 ps 10 ps 0.2 10 3 10 4 Heating 2.1 kj, 10

More information

PRINCIPLES OF POSITRON ANNIHILATION

PRINCIPLES OF POSITRON ANNIHILATION 1.1. Introduction The phenomenon of positron annihilation spectroscopy (PAS) has been utilized as nuclear method to probe a variety of material properties as well as to research problems in solid state

More information