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Synthesis of Element 113 in the Reaction 209 Bi( 70 Zn, n) 278 113

Synthesis of Element 113 in the Reaction 209 Bi( 70 Zn, n) 278 113

Synthesis of Element 113 in the Reaction 209 Bi( 70 Zn, n) 278 113 Morita Kosuke, Morimoto Kouji, Kaji Daiya*, Yoshida Atsushi, Suda Toshimi, Yoneda Akira, Haba Hiromitsu*, Ohnishi Tetsuya, Kanungo Rituparna, Katori Kenji, Akiyama Takahiro, Ideguchi Eiji,

By jereni
(78 views)

Adam Maj IFJ PAN Krakow

Adam Maj IFJ PAN Krakow

Adam Maj IFJ PAN Krakow. Search for Pigmy Dipole Resonance in 68 Ni RISING experiment in GSI. EWON Meeting Prague, 10-12 May, 2007. RISING R are IS otope IN vestigation at G SI. The Accelerators: UNILAC ( injector) E<11.5 MeV/n SIS 18Tm corr. U 1 GeV/n

By jam
(103 views)

Multi-Strangeness Dibaryon

Multi-Strangeness Dibaryon

Multi-Strangeness Dibaryon. T.Goldman, TD, LANL Y.X.Liu, Peking Univ. X.F.Lu, Sichuan Univ. J.L.Ping, Nanjing Normal Univ. Fan Wang, Nanjing Univ. Contents. “Discovery” of multi-quark states. Candidates of multi-strangeness dibaryons. RHIC is a factory of multi-quark.

By garnet
(81 views)

Nuclear Technology

Nuclear Technology

Nuclear Technology. Radioactivity Calculations. Example 1. α – particles ionise 95 000 atoms per cm of air. α – particles lose 42 eV per ionised atom Q1.How much energy (Joules) will α – particles lose per cm of air ?

By rex
(88 views)

Nilsson Model 50 years

Nilsson Model 50 years

Nilsson Model 50 years. Low-Lying resonant states in the 9 Be continuum. María José García Borge Århus-Göteborg-ISOLDE-Madrid-York Collaborations. Outline: Motivation Experimental Tools & Analysis Methods Excited states in 9 Be E < 9 MeV Summary and Outlook.

By tudor
(167 views)

Double Chooz

Double Chooz

Double Chooz. Daya bay. Reno. Reactor Neutrino Experiments. SNO+. Borexino. KamLAND. Thierry Lasserre CEA/Saclay/DSM/IRFU SPP & APC. European Strategy for Future Neutrino Physics October 1 st 2009. MeV Reactor Neutrinos.

By jalen
(170 views)

PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter

PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter

PANDA: Experiments to Study the Properties of Charm in Dense Hadronic Matter. Overview of the PANDA Pbar-A Program The Pbar Facility The PANDA Detector Selected Simulation Results. Why Are Hadrons So Heavy?. Hadron Masses. 2M u + M d ~ 15 MeV/c 2 M p = 938 MeV/c 2.

By maylin
(79 views)

Status of the MEG experiment

Status of the MEG experiment

Status of the MEG experiment. A. M. Baldini INFN Pisa. http://meg.pi.infn.it. Physics motivations General description of the experiment Detectors R&D Sensitivity of the experiment Time schedule. Layout of this talk. SUSY SU(5) predictions BR ( m e g )  10 -14  10 -13

By felix
(127 views)

Energy Loss

Energy Loss

Energy Loss. Graduate School of Scienc e, Tohoku University Toshi Gogami 22/May/2013. GEANT4 Simulation. Energy Loss 12 C 100mg/cm 2 208 Pb 100mg/cm 2. Setup. Virtual Detector. Target. Generate 2344 M eV/c electrons at the center of target. e. Simulation code : POSI

By amity
(146 views)

Chasing  13 with new experiments at nuclear reactors

Chasing  13 with new experiments at nuclear reactors

Chasing  13 with new experiments at nuclear reactors. Thierry Lasserre Saclay NuFact04, Osaka July 26 2004. solar  + KamLAND + reactor  ?. atmospheric  + K2K + MINOS – Superbeams …. superbeam  + reactor . sin 2 (2  13 )<0.20 (CHOOZ)   13 ? (small angle)

By benard
(115 views)

 Mass Measurement at BESIII

 Mass Measurement at BESIII

 Mass Measurement at BESIII. X.H.MO. Workshop on Future PRC-U.S. Cooperation in High Energy Physics Beijing, China, Jun 11-18. Content Introduction Statistical optimization of  mass measurement Systematic uncertainty study Summary. Introduction. Pseudomass method ARGUS CLEO

By stian
(122 views)

Polarizability of the Nucleon*

Polarizability of the Nucleon*

Polarizability of the Nucleon*. Olena Yevetska. Motivation Experimental setup Experiments and results Summary and outlook. SFB 634. *Supported by the DFG within SFB 634. E. B. Motivation. a , b - electric and magnetic polarizabilities. m = b B. d = a E.

By palma
(106 views)

Neutron Imaging of Fuel Cells at NIST: Present and Future Plans

Neutron Imaging of Fuel Cells at NIST: Present and Future Plans

Neutron Imaging of Fuel Cells at NIST: Present and Future Plans. Converts neutrons to light 6 LiF/ZnS:Cu,Al,Au Note that ZnS was used by Rutherford over 100 years ago to image alpha particles backscattered from the gold nucleus

By gerek
(97 views)

Special Theory of Relativity

Special Theory of Relativity

Special Theory of Relativity. In ~1895, used simple Galilean Transformations x’ = x - vt t’ = t But observed that the speed of light, c, is always measured to travel at the same speed even if seen from different, moving frames

By leane
(171 views)

MEG – эксперимент по поиску распада  e 

MEG – эксперимент по поиску распада  e 

MEG – эксперимент по поиску распада  e . Б.И.Хазин Институт ядерной физики им.Г.И. Будкера Новосибирск. Outline. Physics motivation Experimental technique The MEG detector and performances Analysis Summary and prospects. Quarks. Quark mixing (CKM ). t. c. b. s. u. t.

By donal
(190 views)

Alpha and Beta Interactions

Alpha and Beta Interactions

Alpha and Beta Interactions. Rad Pro III NUCP 2331. Interactions. How radiation interacts with matter depends on Energy Mass Charge Charged particles interact differently than uncharged. Attenuation.

By rex
(207 views)

University of California, Los Angeles Department of Physics and Astronomy arisaka@physics.ucla

University of California, Los Angeles Department of Physics and Astronomy arisaka@physics.ucla

Detection of SN Neutrino-Nucleus Elastic Scattering by Multi-ton Liquid Xe/Ar Detectors MAX and XAX. Katsushi Arisaka Michael (Chi Wai ) Lam. University of California, Los Angeles Department of Physics and Astronomy arisaka@physics.ucla.edu. XAX (Xenon-Argon-Xenon). Water Tank Veto.

By linnea
(142 views)

Heavy Quarkonia cc, bb

Heavy Quarkonia cc, bb

Heavy Quarkonia cc, bb. Tomasz Skwarnicki Syracuse University. Use bb as an example. Long and Short-lived Quarkonia. Laboratory of strong interactions. Factory of weakly decaying heavy flavors. Strong int. physics. G ¡( 3S ) ~ 24 keV. G ¡( 4S ) ~ 24 000 keV. W. g. p. p. e +. e +.

By roddy
(85 views)

Introduction to Hypernuclear Physics

Introduction to Hypernuclear Physics

Introduction to Hypernuclear Physics. K. Tanida (RIKEN) CNS summer school, Aug. 21, 2002. Outline: What is hypernucleus? BB interaction and structure of hypernuclei Hyperons in nuclei Weak decay of hypernuclei Results from recent experiments Future prospects. 4. He. S.

By zona
(149 views)

March 23, 1989

March 23, 1989

“Nuclear Reactions in Micro/Nano-Scale Metal Particles” Yeong E. Kim Department of Physics, Purdue University West Lafayette, Indiana 47907, USA August 22, 2011 BACKGROUD.

By elvin
(123 views)

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