Some thoughts on the pointing measurement Nilanga Liyanage.

Slides:



Advertisements
Similar presentations
The 26g Al(p, ) 27 Si Reaction at DRAGON Heather Crawford Simon Fraser University TRIUMF Student Symposium July 27, 2005.
Advertisements

Accelerator Physics, JU, First Semester, (Saed Dababneh).
Robert Michaels HAMC Hall A Analysis Workshop 09 C HAMC = Hall A Monte Carlo ROOT / C++ Design Somewhat like SAMC & genercone For HRS only. Uses LeRose.
Measuring the Neutron and 3 He Spin Structure at Low Q 2 Vincent Sulkosky College of William and Mary, Williamsburg VA Experimental Overview The.
Hall C SHMS Fringe Field Analysis Michael Moore Hall C Winter Meeting
Alpha Stucture of 12 B Studied by Elastic Scattering of 8 Li Excyt Beam on 4 He Thick Target M.G. Pellegriti Laboratori Nazionali del Sud – INFN Dipartimento.
Ion Beam Analysis techniques:
Rutherford Backscattering Spectrometry
E : HRS Cross Section Analyses Vincent Sulkosky Massachusetts Institute of Technology GMp Collaboration Meeting September 24 th, 2012.
Navaphon Muangma (Tai) “SRC Weekly Meeting”, June 19, 2011 SRC Weekly Meeting June 19, 2012  Revisit Optics for LHRS,  LHRS Timing, RHRS Timing  BigBite.
Jin Huang & Vincent Sulkosky Massachusetts Institute of Technology Boson 2010 Workshop Sept 20, JLab.
Outline: 1) Experiment Setup 2) HES Geant4 Simulation 3) Missing Mass Spectra Calibration 4) Experiment status Zhihong Ye, March 16 th 2009 HU Group Meeting.
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.
XPS and SIMS MSN 506 Notes.
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:
Rutherford Backscattering Spectrometry
Particle Interactions
Cross section measurements for analysis of D and T in thicker films Liqun Shi Institute of Modern Physics, Fudan University, Shanghai, , People’s.
ANASEN - Array for Nuclear Astrophysics Studies with Exotic Nuclei Silicon-strip detector array backed with 2-cm-thick CsI Gas proportional counter for.
Zhihong Ye Hampton University Feb. 16 th 2010, APS Meeting, Washington DC Data Analysis Strategy to Obtain High Precision Missing Mass Spectra For E
Bogdan Wojtsekhowski, Jefferson Lab Experimental search for A’ for APEX collaboration 1.
Min Huang Duke University, TUNL On Behalf of the E g2p collaboration Hall A Analysis Workshop, 12/12/12.
Spectroscopic Investigation of P-shell Λ hypernuclei by the (e,e'K + ) Reaction - Analysis Update of the Jlab Experiment E Chunhua Chen Hampton.
Medium heavy Λ hyper nuclear spectroscopic experiment by the (e,e’K + ) reaction Graduate school of science, Tohoku University Toshiyuki Gogami for HES-HKS.
Measurements of F 2 and R=σ L /σ T on Deuteron and Nuclei in the Nucleon Resonance Region Ya Li January 31, 2009 Jlab E02-109/E (Jan05)
The Inverse Kinematics Resonance Elastic Scattering Reaction of 10,11,12 Be+p Liu Yingdu( 刘应都 ) PHD candidate Advisor : Wang Hongwei, Ma Yugang
HAPPEX-III, PVDIS, PREx targets D.S. Armstrong April 17 ‘09 1)Cryotargets – what we requested: new 25 cm racetrack cells – status 2) Solid Targets for.
Polarimetry at the LC Source Which type of polarimetry, at which energies for LC ? Sabine Riemann (DESY), LEPOL Group International Workshop on Linear.
Rosen07 Two-Photon Exchange Status Update James Johnson Northwestern University & Argonne National Lab For the Rosen07 Collaboration.
After last meeting Matt, Riad and I discussed January energy choice…  Focus on Physics paper measurements  Focus on 5 MeV systematics  Pick “final”
1 Polarimeter for dEDM experiment G. Venanzoni Laboratori Nazionali di Frascati for the dEDM collaboration Workshop on Flavour in the era of LHC – Cern.
Exclusive π 0 electroproduction in the resonance region. Nikolay Markov, Maurizio Ungaro, Kyungseon Joo University of Connecticut Hadron spectroscopy meeting.
 -capture measurements with the Recoil-Separator ERNA Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum HRIBF Workshop – Nuclear.
HAPPEX-III and PVDIS targets D.S. Armstrong July 22 ‘08 1)Pointing angle measurements – water cell target some old-style nuclear physics… 2) Cryotargets.
2. RUTHERFORD BACKSCATTERING SPECTROMETRY Basic Principles.
E. Penel-NottarisLaboratoire de Physique Subatomique et de Cosmologie de Grenoble 1 July, 7 th, 2004 Quasi-elastic 3 He(e,e’p) experiment (E89-044) at.
Hypernuclei Production Experiment E05115 at Jefferson Laboratory by the (e,e’K + ) Reaction Chunhua Chen March 31, 2012  Introduction  Experimental Setup.
Systematic error and double Gaussian fitting Toshi Gogami 3Apr2014.
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.
Chapter 5 Interactions of Ionizing Radiation. Ionization The process by which a neutral atom acquires a positive or a negative charge Directly ionizing.
Lecture 9: Inelastic Scattering and Excited States 2/10/2003 Inelastic scattering refers to the process in which energy is transferred to the target,
Proton Charge Form Factor Measurement E. Cisbani INFN Rome – Sanità Group and Italian National Institute of Health 113/Oct/2011E. Cisbani / Proton FF.
SLAC, September 25, 2009 Searching for a U -boson with a positron beam Bogdan Wojtsekhowski Thomas Jefferson National Accelerator Facility  The light.
Calorimetry for Deeply Virtual Compton Scattering in Hall A Alexandre Camsonne Hall A Jefferson Laboratory Workshop on General Purpose High Resolution.
Status of Compton Scattering at ATF ATF Users Meeting April 2012 Oliver Williams.
1 Design of active-target TPC. Contents I.Physics requirements II.Basic structure III.Gas property IV.Electric field Distortion by ground Distortion of.
E97-110: Small Angle GDH Experimental Status Report E97-110: Small Angle GDH Experimental Status Report Vincent Sulkosky Massachusetts Institute of Technology.
(F.Cusanno, M.Iodice et al,Phys. Rev. Lett (2009). 670 keV FWHM  M. Iodice,F.Cusanno et al. Phys.Rev.Lett. 99, (2007) 12 C ( e,e’K )
CERF simulation Mitsu 14th Feb Simulation components Production Transportation Detector response
Jan. 18, 2008 Hall C Meeting L. Yuan/Hampton U.. Outline HKS experimental goals HKS experimental setup Issues on spectrometer system calibration Calibration.
04/06/07I.Larin pi0 systematic error 1  0 error budget Completed items (review) Updated and new items (not reported yet) Items to be completed.
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.
Absolute Polarization Measurement at RHIC in the Coulomb Nuclear Interference Region September 30, 2006 RHIC Spin Collaboration Meeting RIKEN, Wako, Japan.
E97-110: Small Angle GDH Experimental Status Report E97-110: Small Angle GDH Experimental Status Report Vincent Sulkosky Massachusetts Institute of Technology.
Spectrometer optics studies and target development for the 208Pb(e,e’p) experiment in Hall A at Jefferson Lab, GUIDO M. URCIUOLI, INFN, Roma, Italy, JUAN.
Simulation of Heavy Hypernuclear Lifetime Measurement For E Zhihong Ye Hampton University HKS/HES, Hall C Outline: 1,Physics 2,Detectors 3,Events.
Jin Huang Brookhaven National Lab ● Optics General ● Test Run Calibration ● Comment on Full Runs Trying to collect materials from three years ago. May.
Exploring the alpha cluster structure of nuclei using the thick target inverse kinematics technique for multiple alpha decays. Marina Barbui June, 23 rd,
Shuya Ota: Japan Atomic Energy Agency, Rutgers University H. Makii, T. Ishii, K. Nishio, S. Mitsuoka, I. Nishinaka : Japan Atomic Energy Agency M. Matos,
E.C. AschenauerEIC INT Program, Seattle Week 81.
ISR Experiment at MAMI Miha Mihovilovic JGU Mainz and JSI LEPP Workshop, Mainz 2016.
 -capture measurements with a Recoil-Separator Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum Int. Workshop on Gross Properties.
Spin Asymmetries of the Nucleon Experiment ( E07-003) Anusha Liyanage Advisor : Dr. Michael Kohl  Introduction  Physics Motivation  Detector Setup &
Target Effect, Beam correction and T0 Adjustment
MAGIX Detectors Overview
Elastic Scattering in Electromagnetism
Searching for states analogous to the 12C Hoyle state in heavier nuclei using the thick target inverse kinematics technique. Marina Barbui 5/17/2018, Galveston,
HRS at small angles for e+/ e- pair for APEX
Design of active-target TPC
What is the CNI experiment
Presentation transcript:

Some thoughts on the pointing measurement Nilanga Liyanage

2 Q 2 Measurements RHRS LHRS Beam Dump Point of reference for spectrometer angle Center of the spectrometer or Central sieve slit hole Target e-e- e-e- θ0θ0 θ tg

Spectrometer Angle Measurement – Survey: accuracy ~ 0.8 mrad (1% for PREX) – Pointing Measurement: – Use watercell target (with several central momentum settings), find the separation in elastic scattered energies of 16 O and 1 H. – Find the spectrometer angle using the least squared method 3/28/133 Q 2 Measurements Nuclear Recoil Energy

Pointing measurement with H and a heavy nucleus in the same target Most systematics cancel in the difference: Energy loss in target Bean energy shifts Beam position shifts

Challenges For the kinematics of PREX the separation between the two elastic peaks is only about 4 MeV; a 1% measurement of angle requires measuring this separation to < 40 keV accuracy Small H peak sitting on the sloping radiative tail of Oxygen; need a simulation and a careful peak fit to get the separation right.

Pointing Measurement 6 Q 2 Measurements LHRS88.4±0.35 mrad RHRS86.1±0.35 mrad LHRS RHRS

In general the absolute momentum accuracy of the HRS ~ : 100 keV But we can measure momentum differences with better accuracy over small momentum ranges. Luckily we can verify this in the 4-10 MeV range using the elastic states of 12 C Achieved the required < 40 keV accuracy for PREX-I

Issues with different targets Water-foil: – Small H peak – Fe elastic peak next to oxygen, need to separate. LiH powder sandwiched between steel foils : – H, Li and Fe peaks well separated – 3 foils for calculation instead of 2 – optimize the amount of power to window thickness Mixed gas target: H and Ar (?) or Xe – Can mix gas so that the two peaks are about the same. – But effects due to extended target (range of angles): different angular variations for the two nuclei – average angle is different for the two, need to simulate carefully. – Can use a software cut to make a “thin” target: 1 cm (?) – But how long we need to run to get enough stats. with this cut ?