R3B p,A scattering at intermediate energies : 700 MeV/u Low momentum transfer : -t < 0.05 (GeV/c) ̂ 2 Exotic nuclei with T(1/2) < 1 sec. Example:

Slides:

Advertisements

Similar presentations

Accelerator Physics, JU, First Semester, (Saed Dababneh).

Advertisements

PPR Meeting - May 16, 2003 Andrea Dainese 1 Measurement of D 0 production in pp Andrea Dainese University of Padova.

NDVCS measurement with BoNuS RTPC M. Osipenko December 2, 2009, CLAS12 Central Detector Collaboration meeting.

Ion Beam Analysis techniques:

Neutron interaction with matter 1) Introduction 2) Elastic scattering of neutrons 3) Inelastic scattering of neutrons 4) Neutron capture 5) Other nuclear.

10-1 CHEM 312 Lecture 10: Part 1 Radiation Reactions: Dosimetry and Hot Atom Chemistry Readings: §Reading: Modern Nuclear Chemistry, Chap. 17; Nuclear.

Pion yield studies for proton drive beams of 2-8 GeV kinetic energy for stopped muon and low-energy muon decay experiments Sergei Striganov Fermilab Workshop.

GAMMA-PARTICLE ARRAY FOR DIRECT REACTION STUDIES SIMULATIONS.

DESY PRC May 10, Beyond the One Photon Approximation in Lepton Scattering: A Definitive Experiment at DESY for J. Arrington (Argonne) D. Hasell,

Final state study Jaewon Park University of Rochester MINERvA/Jupiter Group Meeting, Jan 31, 2007.

Transfer reactions Resonant Elastic scattering Inelastic scattering: GR.

GAMMA-PARTICLE ARRAY FOR DIRECT REACTION STUDIES SIMULATIONS.

TIME-LIKE BARYON FORM FACTORS: EXPERIMENTAL SITUATION AND POSSIBILITIES FOR PEP-N Roberto Calabrese Dipartimento di Fisica and I.N.F.N. Ferrara, Italy.

Particle Interactions

Count rate estimates from TDR Assuming beam intenisties from previous slide and acc *rec from SIM LH2 case [counts/24h] p [GeV/c] beam momentum Solid.

03/07/2015radiation safety - level 51 Radiation safety level 5 Frits Pleiter.

Cross section measurements for analysis of D and T in thicker films Liqun Shi Institute of Modern Physics, Fudan University, Shanghai, , People’s.

Bogdan Wojtsekhowski, Jefferson Lab Experimental search for A’ for APEX collaboration 1.

APS Meeting April 5-8, 2003 at Philadelphia Chunhui Luo 1 Chunhui Luo Inclusive J/ψ Production at DØ.

FFAG-ERIT R&D 06/11/06 Kota Okabe (Kyoto Univ.) for FFAG-DDS group.

Tools for Nuclear & Particle Physics Experimental Background.

SHMS Optics and Background Studies Tanja Horn Hall C Summer Meeting 5 August 2008.

SQM2004, Cape Town, Sept. 16, 2004 STAR 1 Cronin Effect for the identified particles from 200 GeV d+Au collisions Xiangzhou Cai Shanghai INstitute of Applied.

DE/dx measurement with Phobos Si-pad detectors - very first impressions (H.P Oct )

BNL/ Tatsuya CHUJO CNS workshop, Tokyo Univ. Identified Charged Single Particle Spectra at RHIC-PHENIX Tatsuya Chujo (BNL) for the PHENIX.

Kinematics of  + n   p   0  p reaction Susumu Oda 2007/04/10-19.

ACTAR meeting - Dec 10th 2008Hervé Savajols (GANIL) Tracking Algorithms Hervé Savajols & Thomas Roger (GANIL) Wolfgang Mittig (MSU) …

A search for deeply-bound kaonic nuclear states in (in-flight K -, N) reaction Hiroaki Ohnishi RIKEN.

Mitglied der Helmholtz-Gemeinschaft Calibration of the COSY-TOF STT & pp Elastic Analysis Sedigheh Jowzaee IKP Group Talk 11 July 2013.

Development of solid hydrogen target in RIKEN RIKEN T. Ohnishi, H. Takeda, T. Suda KEK S. Ishimoto, S. Suzuki RCNP Y. Takahashi ANL I. Tanihata  Introduction.

Accelerator Physics, JU, First Semester, (Saed Dababneh). 1 Electron pick-up. ~1/E What about fission fragments????? Bragg curve stochastic energy.

Neutral Current Deep Inelastic Scattering in ZEUS The HERA collider NC Deep Inelastic Scattering at HERA The ZEUS detector Neutral current cross section.

Difference between Roman Pots and VELO Very forward tracking is typically done using detectors located in Roman pots. They are far away from the interaction.

Proton Charge Form Factor Measurement E. Cisbani INFN Rome – Sanità Group and Italian National Institute of Health 113/Oct/2011E. Cisbani / Proton FF.

Charged Particle Multiplicity and Transverse Energy in √s nn = 130 GeV Au+Au Collisions Klaus Reygers University of Münster, Germany for the PHENIX Collaboration.

Jet Physics at CDF Sally Seidel University of New Mexico APS’99 24 March 1999.

Resolution and radiative corrections A first order estimate for pbar p  e + e - T. H. IPN Orsay 05/10/2011 GDR PH-QCD meeting on « The nucleon structure.

1 Design of active-target TPC. Contents I.Physics requirements II.Basic structure III.Gas property IV.Electric field Distortion by ground Distortion of.

J-PARC でのハイパー核ガンマ線分光実験用散乱粒子磁気スペクトロメータ検出器の準備状況東北大理, 岐阜大教 A, KEK B 白鳥昂太郎, 田村裕和, 鵜養美冬 A, 石元茂 B, 大谷友和, 小池武志, 佐藤美沙子, 千賀信幸, 細見健二, 馬越, 三輪浩司, 山本剛史, 他 Hyperball-J.

D 0 reconstruction: 15 AGeV – 25 AGeV – 35 AGeV M.Deveaux, C.Dritsa, F.Rami IPHC Strasbourg / GSI Darmstadt Outline Motivation Simulation Tools Results.

Current estimation of the background level Ken Sakashita ( Osaka University ) for the E391a collaboration 1.Overview/Motivation 2.4  data analysis 3.2.

Open and Hidden Charm production in 920 GeV Proton-Nucleus Collisions Presented by Marko Starič for the Hera-B collaboration The.

ЭКСПЕРИМЕНТ R3B РЕАКЦИИ С РЕЛЯТИВИСТКИМИ РАДИОАКТИВНЫМИ ПУЧКАМИ НА УСКОРИТЕЛЬНОМ КОМПЛЕКСЕ FAIR (GSI, DARMSTADT, GERMANY) Е.М. МАЕВ.

J-PARC でのシグマ陽子散乱実験の提案 Koji Miwa Tohoku Univ.. Contents Physics Motivation of YN scattering Understanding Baryon-Baryon interaction SU(3) framework Nature.

Kalanand Mishra June 29, Branching Ratio Measurements of Decays D 0  π - π + π 0, D 0  K - K + π 0 Relative to D 0  K - π + π 0 Giampiero Mancinelli,

J-PARC における 4  He の生成と構造の研究東北大学大学院理学研究科白鳥昂太郎 for the Hyperball-J Collaboration.

Particle identification by energy loss measurement in the NA61 (SHINE) experiment Magdalena Posiadala University of Warsaw.

Masashi Kaneta, RBRC, BNL 2003 Fall Meeting of the Division of Nuclear Physics (2003/10/31) 1 KANETA, Masashi for the PHENIX Collaboration RIKEN-BNL Research.

RP Software Collaboration Meeting 7 Mars 2007 Hubert Niewiadomski TOTEM, CERN Brunel University.

Compton Data Analysis Liping Gan University of North Carolina Wilmington.

The Active Target for R 3 FAIR Peter Egelhof GSI Darmstadt, Germany ACTAR Workshop Bordeaux, France June 16 – June 18, 2008 FAIR.

E.C. AschenauerEIC INT Program, Seattle Week 81.

Quarkonia production with the HERA-B experiment J. Spengler, MPI Heidelberg.

INFN - PadovaBeauty Measurements in pp with the Central Detector 1 Beauty Measurements in p-p with the Central Detector F. Antinori, C. Bombonati, A. Dainese,

First data from TOTEM experiment at LHC

A.Smirnov, A.Sidorin, D.Krestnikov

Event Reconstruction and Data Analysis in R3BRoot Framework

SBS Magnet, Optics, and Spin Transport

Beam-Gas Inelastic scattering in CEPC partial double ring

Elastic Scattering in Electromagnetism

How to detect protons from exclusive processes

Charged Particle Multiplicity in DIS

Charged Particle Multiplicity in DIS

Feasibility of   γγ study with ECAL

MINOS: a new vertex tracker for in-flight γ-ray spectroscopy

Proposal for high precision measuremens of

Compton Data Analysis Jing Feng China Atomic Institute Liping Gan

GEANT Simulations and Track Reconstruction

Design of active-target TPC

What is the CNI experiment

Presentation transcript:

R3B p,A scattering at intermediate energies : 700 MeV/u Low momentum transfer : -t < 0.05 (GeV/c) ̂ 2 Exotic nuclei with T(1/2) < 1 sec. Example: 132Sn (39.7 sec.)

p,A elastic scattering scheme Cylinder with Be windows 500 um Beam shield d = 2 cm Beam tracking + vertex reconstruction Pressure P in the range 10 to 20 bar

p,A scattering : measurement p(132Sn,132Sn) – 700 MeV/u Glauber differential cross sections < -t < (GeV/c) ̂ ° < theta < 7.18° in the CM frame First diffraction minimum With a 5000 beam pps, we achieve < 1% statistical errors

Sensitivity to RMS matter distribution

Energy resolution for spectroscopic studies

Beam E loss and straggling Scattering at 0, 50 cm and 1 m Contribution from the Be windows => thinner ? Large signal from the beam => Shielding Straggling still acceptable at 20 bar E loss correction => Vertex reconstruction

Protons Maximum energy stopped in 50 cm : 9.1 MeV (10 bar) and 13.3 MeV (20 bar) Energy lost in the central dead region (2 cm) : 200 keV (10 bar) and 291 keV (20 bar) => Necessary to correct with vertex reconstruction Low energy (2.7 MeV) will lose 602 keV (10 bar) and 1.4 MeV (20 bar)