Optics Simulations. Dustin McNulty UMass July 10, 2009
|
|
- Imogene Lambert
- 5 years ago
- Views:
Transcription
1 Optics Simulations Dustin McNulty UMass July, 9
2 Outline Optics Simulations New HRS Optics Tune for PREx A T Hole Studies Be X, FoM and Detector Size HAPPEX-III Focal Plane Distribution PREx Optics/detector beamtest during H-III Commissioning at pass Summary and Future Work Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
3 z y x Spectrometer Coord. Sys. NOT TO SCALE Transport Coord. Sys. y z x 4 o Nominal Central Ray TOP of VDC BOX VDC s PMT PMT 6cm Transport z at det location VDC v u Transport z= Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
4 Standard (Old) and PREx (New) HRS Optics Tune RHRS xy (Standard Optics Tune) HAMC Simulation (Pb, deg,.gev) RHRS xy (PREx Optics Tune) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 3
5 PREx: Transport Plane Rates RHRS x (PREx Optics Tune) RHRS y (PREx Optics Tune) A/.cm) Event Rate (Hz/µ 7 6 HAMC Simulation (Pb, deg,.gev) ±4MeV x cut: Tot Rate =.9 MHz/µA Event Rate (Hz/ µa/.cm) 7 6 ±4MeV x cut: -6.4 < x <.8cm Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 4
6 PREx Collimator and A T Hole with 9 Be Plug Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
7 A T Hole Event Distributions (PREx Tune) RHRS x (PREx Optics Tune) RHRS y (PREx Optics Tune) A/.cm) Event Rate (Hz/µ 7 6 HAMC Simulation (Pb, deg,.gev).86χ o Be Plug ±4MeV x cut: Tot Rate =.9 MHz/µA Event Rate (Hz/ µa/.cm) 7 6 ±4MeV x cut: -6.4 < x <.8cm Bkgd from 8.6% Be 74.7 Hz/ µa Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 6
8 Paul s A T Correction Figure of Merit M = E + B R S () E is the enhancement in A T sensitivity for the hole events (estimated to be ) R is the ratio of rates of the detected hole events relative to the main detector events (Additional factor of reduction to account for radiative tail in hole events) B/S is the ratio of background to A T hole signal The error inflation due to the correction is +M For example, if M =.64, error inflation =.9 Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 7
9 A T Hole Figure of Merit Study B/S Rate Ratio Detector x size (m) A T Detector x size (m) A T Figure of Merit. Error Inflation Detector x size (m) A T Detector x size (m) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 8 A T
10 $ ' AT Hole Detector (PREx Tune) RHRS xy (PREx Optics Tune) ±4MeV x cut: sig:noise =.37-4 Tot Rate =. MHz/µA & Det Size: 7.6cm by.8cm (x by y) -6 RHRS xy (PREx Optics Tune) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting % 9
11 HAPPEX-III Focal Plane Distributions Focal Plane y (m) RHRS xy (Standard Optics Tune) 8 HAMC Simulation 6 4 (cm H, 4deg, 3.484GeV) Focal Plane x (m) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
12 HAPPEX-III Transport Plane Distributions RHRS xy (Standard Optics Tune) 8 HAMC Simulation (cm H, 4deg, 3.484GeV) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
13 HAPPEX-III Transport Plane Distributions Event Rate (arb. units/.cm)..8.6 RHRS x (Standard Optics Tune). HAMC Simulation (cm H, 4deg, 3.484GeV) Event Rate (arb. units/.cm) RHRS y (Standard Optics Tune) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
14 PREX beamtest during HAPPEX-III Commissioning RHRS xy (PREx Optics Tune) RHRS xy (PREx Optics Tune) ±4MeV x cut: Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 3
15 Summary and Future Work Based on HAMC simulation of new PREX HRS optics, optimal prex detector size is roughly cm dispersive (x) by 4cm transverse (y) For A T measurment/correction FoM studies, A T detector size is optimized at 7.6cm in x and.8cm in y with estimated error inflation of % Examine sieve slit distributions using new PREX optics tune? Determine roll and pitch angles for HAPPEX-III detector positioning? Determine Rates for HAPPEX-III running Examine thick Ta spectra for H-III commissioning at pass? Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 4
16 EXTRA SLIDES Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
17 A T Hole Event Distributions (Standard Tune) RHRS x (Standard Optics Tune) RHRS y (Standard Optics Tune) A/.cm) Event Rate (Hz/µ 7 6 HAMC Simulation (Pb, deg,.gev).86χ o Be Plug ±4MeV x cut: Tot Rate = 3. MHz/µA Event Rate (Hz/ µa/.cm) 6 ±4MeV x cut: -6.4 < x <.8cm 4 Bkgd from 8.6% Be Hz/µA Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 6
18 A T Hole Figure of Merit Study B/S Rate Ratio Detector y size (m) A T Detector y size (m) A T Figure of Merit. Error Inflation Detector y size (m) A T Detector y size (m) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 7 A T
19 $ ' AT Hole xy Distributions (Standard Tune) RHRS xy (Standard Optics Tune) 8 HAMC Simulation 6 (Pb, deg,.gev) RHRS xy (Standard Optics Tune) ±4MeV x cut: & Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting % 8
20 HAPPEX-III Transport Plane Distributions Event Rate (arb. units/.cm)..8.6 RHRS x (Standard Optics Tune).4 HAMC Simulation (cm H, 4deg, 3.484GeV). Event Rate (arb. units/.cm) RHRS y (Standard Optics Tune) Focal Plane x (m) Focal Plane x (m) - - Focal Plane y (m) Focal Plane y (m) Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting 9
21 PREX beamtest during HAPPEX-III Commissioning A/.97cm) Event Rate (Hz/µ 3 RHRS x (PREx Optics Tune) HAMC Simulation (Pb, 4deg,.4GeV) ±4MeV x cut: Tot Rate =.4 khz/µa Event Rate (Hz/µA/.67cm) ± 4MeV x cut: RHRS y (PREx Optics Tune) -7.7 < x < 6.cm Optics Simulations, July 9 -, 9, Hall A Parity Collaboration Meeting
PREX / CREX Status. Jan 25, 2018 Bob Michaels, on behalf of the PREX collaboration. docdb
PREX / CREX Status Jan 25, 2018 Bob Michaels, on behalf of the PREX collaboration. Wiki https://prex.jlab.org/wiki/index.php/main_page docdb http://prex.jlab.org/cgi-bin/docdb/public/documentdatabase (
More informationE05-009:HAPPEx-III Status Report. Dustin McNulty UMass December 5, 2008
E05-009:HAPPEx-III Status Report Dustin McNulty UMass mcnulty@jlab.org December 5, 2008 E05-009:HAPPEx-III Status Report Outline Quick Review: Parity Violation and Strange FFs Worldwide Experimental Programs
More informationThe Lead Radius Experiment PREX. Dustin McNulty Idaho State University for the PREx Collaboration July 28, 2011
The Lead Radius Experiment PREX Dustin McNulty Idaho State University for the PREx Collaboration mcnulty@jlab.org July 28, 2011 The Lead Radius Experiment PREX Outline Motivation Parity Violation at JLab
More informationC-REX : Parity-Violating Measurement of the Weak Charge of
C-REX : Parity-Violating Measurement of the Weak Charge of 48 Ca to an accuracy of 0.02 fm Spokespersons: Juliette Mammei Dustin McNulty Robert Michaels that s me Kent Paschke Seamus Riordan (contact person)
More informationGMp Experiment (E ): An update
GMp Experiment (E12-07-108): An update Kalyan Allada MIT Hall A/C Summer Meeting, Jefferson Lab 17th July 2015 Motivation Accurately measure e-p elastic cross section in kinematics similar to other JLab
More informationMeasurement of Nucleon Strange Form Factors at High Q 2
Measurement of Nucleon Strange Form Factors at High Q 2 (HAPPEX III Collaboration) Rupesh Silwal 22 March, 2011 At very low Q2, GsE/M relates to the strange matrix elements of the nucleon (strange radius
More informationCross-section Measurements with HRS and Septum
Cross-section Measurements with HRS and Septum Vincent Sulkosky The College of William and Mary Hall A Analysis Workshop January 6 th, 27 Hall A Analysis Workshop p.1/16 Overview of Experiment E97-11 Precise
More informationStatus of GEp III high Q form factor ratio analysis. Andrew Puckett, MIT on behalf of the GEp III Collaboration
Status of GEp III high Q form factor ratio 2 analysis Andrew Puckett, MIT on behalf of the GEp III Collaboration Experiments E04 108 and E04 019 e' e p Analysis Method Two primary tasks for form factor
More informationGMp Experiment. M. Eric Christy. Hall A/C Summer Meeting For the GMp Collaboration
GMp Experiment M. Eric Christy For the GMp Collaboration Hall A/C Summer Meeting 2017 Overview of GMp Experiment Performed measurements of elastic e-p cross section over a Q2 range of 2-16 GeV2 Improve
More informationAPEX: Goals and Strategy
APEX: Goals and Strategy Natalia Toro (Perimeter Institute) e 2 10-4 10-5 10-6 10-7 10-8 E141 A' Æ Standard Model a m, 5 s E774 a m,±2 s favored a e DarkLight WASA Phenix HPS 2015 KLOE MAMI APEX BaBar
More informationTritium Runplan 2017/18. Florian Hauenstein Old Dominion University Hall A collaboration meeting
Tritium Runplan 2017/18 Florian Hauenstein Old Dominion University Hall A collaboration meeting 18.01.17 Tritium Experiments E12-010-103 (MARATHON) Deep Inelastic Scattering to measure F 2n to F 2p ratio,
More informationPREX Overview Extracting the Neutron Radius from 208 Pb
PREX Overview Extracting the Neutron Radius from 208 Pb Seamus Riordan University of Massachusetts, Amherst sriordan@physics.umass.edu March 17, 2013 Seamus Riordan CREX 2013 PREX 1/19 Outline Motivation
More informationApplications of Parity Violation
Applications of Parity Violation Dustin McNulty Idaho State University mcnudust@isu.edu Thanks to: Carlos Bula, Brady Lowe, Kevin Rhine, Will Gorman, and Rhys Borchert December 8, 2014 Applications of
More informationParity-Violating Measurements of the Weak Charge of. Pb (PREX) & Ca (CREX) . and possible future measurements. R. Michaels, ICNT / MSU, Aug /26
Parity-Violating Measurements of the Weak Charge of 208 Pb (PREX) & 48 Ca (CREX) 208 Pb 48 Ca. and possible future measurements R. Michaels, ICNT / MSU, Aug 2013 1/26 Hall A at Jefferson Lab Hall A High
More informationE (GMp) Precision Measurement of the Proton Elastic Cross Section at High Q 2. Thir Gautam Hampton University
E12-07-108 (GMp) Precision Measurement of the Proton Elastic Cross Section at High Q 2 Thir Gautam Hampton University On behalf of the GMp Collaboration Hall A Collaboration Meeting January 18, 2017 GMp
More informationStatus of the PREX Experiment R n through PVeS at JLab
Status of the PREX Experiment R n through PVeS at JLab Seamus Riordan University of Massachusetts, Amherst sriordan@physics.umass.edu for the PREX Collaboration June 18, 2011 Seamus Riordan NuSym11 PREX
More informationBeam Instrumentation Challenges for Parity-Violation Experiments
Beam Instrumentation Challenges for Parity-Violation Experiments Manolis Kargiantoulakis Intense Electron Beams Workshop 2015 Cornell University Many thanks to Mark Pitt, Kent Paschke, Mark Dalton, for
More informationCoulomb Sum Rule. Huan Yao Advisor: Zein-Eddine Meziani Work support DOE Grant: DE-FG02-94ER40844
Coulomb Sum Rule Huan Yao hyao@jlab.org Advisor: Zein-Eddine Meziani Work support DOE Grant: DE-FG02-94ER40844 Oct 12,2009 1 / 30 Outline 1 Physics 2 Experiment 3 Data Analysis General Analysis BPM VDC
More informationThe SOS Quad in the Right-HRS (RHRS)
The SOS Quad in the Right-HRS (RHRS) Barak Schmookler Apex- Apr. 19, 2015 1 Current Status of the RHRS The HRSs (RHRS and LHRS) are QQDQ spectrometers. Quadrupole 1 (Q1) focuses in the dispersive (i.e.
More informationThe neutron skin in neutronrich nuclei at Jefferson Lab
The neutron skin in neutronrich nuclei at Jefferson Lab Mark Dalton, University of Virginia For the PREX and CREX Collaborations Low Energy Workshop Boston 15 March 2013 1 Weak Charge Distribution of Heavy
More informationarxiv: v1 [nucl-ex] 15 Apr 2016
arxiv:1604.04602v1 [nucl-ex] 15 Apr 2016 Beam Normal Single Spin Asymmetry Measurements from Q weak Buddhini P. Waidyawansa for the Q weak Collaboration C122, 12000 Jefferson Avenue, Newport News, VA 23602
More informationAcknowledgements: D. Armstrong, M. Dalton, K. Paschke, J. Mammei, M. Pitt, B. Waidyawansa and all my theory colleagues
Acknowledgements: D. Armstrong, M. Dalton, K. Paschke, J. Mammei, M. Pitt, B. Waidyawansa and all my theory colleagues An Experiments Krishna Kumar Stony Brook University The Electroweak Box Workshop at
More informationPREX Background Simulation Update
PREX Background Simulation Update Rakitha Beminiwattha Syracuse University rakithab@jlab.org 1 Outline PREX-II Collimator Plastic Shielding for Neutrons PREX-II Background Radiation Activation Studies
More informationParity-violating Electron Scattering and Strangeness in the Nucleon: Results from HAPPEX-II
Parity-violating Electron Scattering and Strangeness in the Nucleon: Results from HAPPEX-II L. J. Kaufman University of Massachusetts The HAPPEX Collaboration Thomas Jefferson National Accelerator Facility
More informationPREX and CREX. R N from Electroweak Asymmetry in Elastic Electron-Nucleus Scattering. Neutron Skin.
http://hallaweb.jlab.org/parity/prex PREX and CREX 08 Pb Horowitz 48 Ca Neutron Skin R N from Electroweak Asymmetry in Elastic Electron-Nucleus Scattering R L 4 6 A ~ 10 PV Q ~ 10 R L PRL 108 (01) 1150
More informationRadiological Issues at JLab
Radiological Issues at JLab Lessons Learned from the PREX-I and Preparation for PREX-II/CREX (and MOLLER) Rakitha S. Beminiwattha Louisiana Tech University College of Science and Engineering Outline Radiation
More informationThe MOLLER experiment - testing the Standard Model at Jefferson Lab
The MOLLER experiment - testing the Standard Model at Jefferson Lab Dustin McNulty Idaho State University mcnulty@jlab.org for the May 30, 2012 The MOLLER experiment - testing the Standard Model at Jefferson
More informationPREX Simulation Update
PREX Simulation Update Rakitha Beminiwattha Syracuse University rakithab@jlab.org 1 Outline PREX-II Collimator Plastic Shielding for Neutrons PREX-II Background Radiation Effects of Septum Magnet Fringe
More informationCoulomb Sum Rule. Huan Yao Feb 16,2010. Physics Experiment Data Analysis Summary Collaboration APS April Meeting
Coulomb Sum Rule 2010 APS April Meeting Huan Yao hyao@jlab.org Feb 16,2010 1 / 17 Physics Motivation The test of Coulomb Sum Rule is to shed light on the question of whether or not the properties of nucleons
More informationTransverse momentum spectra using the Inner Tracking System of the ALICE experiment at LHC
- 1 - Transverse momentum spectra using the Inner Tracking System of the ALICE experiment at LHC Seminario di fine secondo anno di dottorato Torino, 3 Febbraio 2010 Outline - 2-1 2 3 4 5 A Large Ion Collider
More informationLucite Hodoscope for SANE
Lucite Hodoscope for SANE A. Ahmidouch, S. Danagoulian NC A&T State University Outline Cosmic Ray test of a lucite prototype bar The old result from Monte Carlo Geometry consideration Trigger Electronics
More informationA Precision Measurement of Elastic e+p Beam Normal Single Spin Asymmetry and Other Transverse Spin Measurements from Qweak
A Precision Measurement of Elastic e+p Beam Normal Single Spin Asymmetry and Other Transverse Spin Measurements from Qweak Buddhini P. Waidyawansa For the Qweak Collaboration JLab Users Group Meeting June
More informationNeutron stars at JLAB and the Pb Radius Experiment
Neutron stars at JLAB and the Pb Radius Experiment PREX uses parity violating electron scattering to accurately measure the neutron radius of 208 Pb. 208 Pb This has many implications for nuclear structure,
More informationQuarkonium LHCb
Quarkonium Studies @ LHCb Giacomo Graziani (INFN Firenze) on behalf of the LHCb Collaboration December 5th, 2008 QWG08, Nara G. Graziani slide 1 QWG08 The LHCb Experiment dedicated to CP violation and
More informationBeam Polarimetry (for Future Experiments at JLab)
Outline E.Chudakov June 24, 2009, PAVI-09 Beam Polarimetry 1 Beam Polarimetry (for Future Experiments at JLab) E.Chudakov 1 1 JLab PAVI-09 Outline E.Chudakov June 24, 2009, PAVI-09 Beam Polarimetry 2 Outline
More informationP.M. King Ohio University for the MOLLER Collaboration
Parity violating electron scattering at JLab: the MOLLER experiment P.M. King Ohio University for the MOLLER Collaboration SESAPS, 10 November 2016; University of Virginia, Charlottesville, VA The Standard
More informationTransversity experiment update
Transversity experiment update Hall A collaboration meeting, Jan 20 2016 Xuefei Yan Duke University E06-010 Collaboration Hall A collaboration The Incomplete Nucleon: Spin Puzzle 1 2 = 1 2 ΔΣ + L q + J
More informationApplications of Parity Violation
Applications of Parity Violation Dustin McNulty Idaho State University mcnudust@isu.edu Thanks to: Carlos Bula, Brady Lowe, Kevin Rhine, Blake French, and Max Sturgeon April 7, 2015 Applications of Parity
More informationDirect Measurement of the W Total Decay Width at DØ. Outline
Direct Measurement of the W Total Decay Width at DØ Introduction Junjie Zhu University of Maryland On behalf of the DØ Collaboration Monte Carlo Simulation Event Selection Outline Determination of the
More informationPolarimetry in Hall A
Outline E.Chudakov Moller-12 Workshop, Aug 2008 Polarimetry in Hall A 1 Polarimetry in Hall A E.Chudakov 1 1 Hall A, JLab Moller-12 Workshop, Aug 2008 Outline E.Chudakov Moller-12 Workshop, Aug 2008 Polarimetry
More informationLarge Acceptance High Luminosity Detector at 12 GeV
Outline Large Acceptance High Luminosity Detector at 12 GeV E.Chudakov 1 1 Hall A, JLab For June 2006 Hall A Meeting Outline Outline 1 Motivation for a Large Acceptance at High Luminosity DIS Parity Violation
More informationParity Violation Experiments & Beam Requirements
Parity Violation Experiments & Beam Requirements Riad Suleiman Center for Injectors and Sources MCC Ops Training August 05, 2009 Outline Fundamental Interactions and Conservation Rules Parity Reversal
More informationSta$s$cs, Systema$cs and Run Phases
Sta$s$cs, Systema$cs and Run Phases DOE Nuclear Physics MOLLER Science Review UMass, Amherst! September, 2014 Kent Paschke University of Virginia α Rates, Noise Budget, and Sta$s$cal Precision 0.4 0.35
More informationPhotopion photoproduction and neutron radii
Photopion photoproduction and neutron radii Dan Watts, Claire Tarbert University of Edinburgh Crystal Ball and A2 collaboration at MAMI Jefferson Lab PREX workshop, August 2008 Talk Outline Nuclear (π
More informationStatus Report on the Precision Measurement of d n 2
Status Report on the Precision Measurement of d n 2 Experiment E06-014 Diana Parno (Carnegie Mellon University) David Flay, Matthew Posik (Temple University) December 15, 2009 Diana Parno (Carnegie Mellon)
More informationMin Huang Duke University, TUNL On behalf of the E (g2p) collaboration
Min Huang Duke University, TUNL On behalf of the E08-027 (g2p) collaboration Hall A Collaboration Meeting, June 13th, 2013 E08 027 g 2p & the LT Spin Polarizability Spokespeople Alexandre Camsonne (JLab)
More informationToward 0.5% Electron Beam Polarimetry. Kent Paschke University of Virginia
Toward 0.5% Electron Beam Polarimetry Kent Paschke University of Virginia Needs for 0.5% The proposed PV-DIS experiments may be systematics limited, with fractional errors approaching 0.5%. No
More informationE Analysis status Mass and cross section evaluation Comments on physics interpretation
E01-011 Analysis status Mass and cross section evaluation Comments on physics interpretation Based on Ph.D presentation of A. Matsumura Y.Fujii Tohoku University HKS-HES collaboration meeting at JLab,
More informationParity Violating Electron Scattering at Jefferson Lab. Rakitha S. Beminiwattha Syracuse University
Parity Violating Electron Scattering at Jefferson Lab Rakitha S. Beminiwattha Syracuse University 1 Outline Parity Violating Electron Scattering (PVES) overview Testing the Standard Model (SM) with PVES
More informationRecent results and future direction of the parity-violating electron scattering program in Hall A at Jefferson Lab
Recent results and future direction of the parity-violating electron scattering program in Hall A at Jefferson Lab, University of Virginia For the HAPPEX, PREX, PVDIS, MOLLER and SOLID Collaborations SPIN,
More informationA Pure Photon Source for use with Solid Polarized Targets Progress Report UVa Option
A Pure Photon Source for use with Solid Polarized Targets Progress Report UVa Option Donal Day, Dustin Keller, Darshana Perera, Jixie Zhang and friends NPS Collaboration Meeting January 19, 2017 Jefferson
More informationPrecision High Field Møller Polarimetry in Hall A Status Report
Precision High Field Møller Polarimetry in Hall A Status Report Jim Napolitano, Temple University Work Carried Out by Ted Berger, Ben LeRose (RPI) John LeRose (JJL Magnet Optics) and James Wilhelmi and
More informationParity Violation Experiments
Parity Violation Experiments Krishna Kumar University of Massachusetts thanks to the HAPPEX, G0 and Qweak Collaborations, D. Armstrong, E. Beise, G. Cates, E. Chudakov, D. Gaskell, C. Furget, J. Grames,
More informationMøller Polarimetry in Hall A and Beyond
Outline E.Chudakov EIC, Ann Arbor, Aug 2007 Møller Polarimetry: Hall A and beyond 1 Møller Polarimetry in Hall A and Beyond E.Chudakov 1 1 Hall A, JLab EIC Polarimetry Workshop, Ann Arbor, Aug 23-24, 2007
More information6 Bunch Compressor and Transfer to Main Linac
II-159 6 Bunch Compressor and Transfer to Main Linac 6.1 Introduction The equilibrium bunch length in the damping ring (DR) is 6 mm, too long by an order of magnitude for optimum collider performance (σ
More informationEM Energy Spectrum from 17.6 MeV photons. Eduardo do Couto e Silva and Xin Chen Feb 13, 2002
EM Energy Spectrum from 17.6 MeV photons Eduardo do Couto e Silva and Xin Chen Feb 13, 2002 Event display of a muon passing through EM Using GLEAM V3 the official version for EM Mechanical support structure
More informationThe π 0 Lifetime: Experimental Probe of. Dustin E. McNulty MIT/UMass for the PrimEx Collaboration April 16, 2008
The π Lifetime: Experimental Probe of the QCD Axial Anomaly Dustin E. McNulty MIT/UMass for the mcnulty@jlab.org April 16, 28 The π Lifetime: Experimental Probe of the QCD Axial Anomaly Outline Physics
More informationIPBI-TN June 30, 2004
Spray Electron Beam for Tests of Linear Collider Forward Calorimeter Detectors in SLAC End Station A R. Arnold UMass Amherst, Amherst MA 01003 T. Fieguth Stanford Linear Accelerator Center Menlo Park,
More informationDelta undulator magnet: concept and project status
Delta undulator magnet: concept and project status Part I: concept and model construction* Alexander Temnykh, CLASSE, Cornell University, Ithaca, New York, USA Part - II: beam test at ATF in BNL + M. Babzien,
More informationTechnical Status Update on PA Lifetime Spectroscopy Experiments and Results
Technical Status Update on PA Lifetime Spectroscopy Experiments and Results Dustin McNulty Idaho State University mcnudust@isu.edu October 9, 2012 Technical Status Update on PA Lifetime Spectroscopy Experiments
More informationAPEX: A Prime EXperiment at Jefferson Lab
APEX: A Prime EXperiment at Jefferson Lab e + e A e γ APEX Test Run Data, ~770K evts Z Events / ( 0.05 ) 1000 800 600 400 James Beacham New York University for the APEX Collaboration 200 0 180 190 200
More informationMøller Polarimetry for PV Experiments at 12 GeV
Outline E.Chudakov Jan 15, 2010, MOLLER Review Møller Polarimetry 1 Møller Polarimetry for PV Experiments at 12 GeV E.Chudakov 1 1 JLab MOLLER Review Outline E.Chudakov Jan 15, 2010, MOLLER Review Møller
More informationCross section measurements of the elastic electron - deuteron scattering
Cross section measurements of the elastic electron - deuteron scattering for the A1 Collaboration Institut für Kernphysik, Johannes Gutenberg-Universität Mainz Johann-Joachim-Becher-Weg 45, 55128 Mainz
More informationQweak Transverse Asymmetry Measurements
Qweak Transverse Asymmetry Measurements Buddhini Waidyawansa For the Qweak Collaboration Hall C Collaboration Meeting 02-21-2014 Outline Physics of transverse asymmetries Qweak transverse data set Analysis
More informationIntroduction Polarimeters at MAMI Analysis Future Conclusion. Polarimetry at MAMI. V. Tyukin, Inst. of Nuclear Physics, Mainz, Germany
Polarimetry at MAMI V. Tyukin, Inst. of Nuclear Physics, Mainz, Germany Workshop to Explore Physics Opportunities with Intense, Polarized Electron Beams up to 3 MeV MIT 213 15 March 213 Contents Introduction
More informationElectron Beam Polarimetry at JLab Hall C Dave Gaskell PST 2009 September 7, 2009
Electron Beam Polarimetry at JLab Hall C Dave Gaskell PST 2009 September 7, 2009 1. Møller Polarimeter 2. Compton Polarimeter 3. Summary JLab Polarimetry Techniques Three different processes used to measure
More informationAIRFLY: Measurement of the Air Fluorescence induced by electrons
AIRFLY: Measurement of the Air Fluorescence induced by electrons Valerio Verzi INFN Sezione di Roma II For the Airfly collaboration 9 th Topical Seminar on Innovative Particle and Radiation Detectors 23-26
More informationLow slice emittance preservation during bunch compression
Low slice emittance preservation during bunch compression S. Bettoni M. Aiba, B. Beutner, M. Pedrozzi, E. Prat, S. Reiche, T. Schietinger Outline. Introduction. Experimental studies a. Measurement procedure
More information1. Polarimetry Strategy 2. Møller Polarimeter 3. Compton Polarimeter 4. Summary
Vladas Tvaskis (University of Manitoba) Hall C Users Meeting January 202. Polarimetry Strategy 2. Møller Polarimeter 3. Compton Polarimeter 4. Summary Q Weak requires measurement of the beam polarization
More informationDark Matter Searches with AMS-02. AMS: Alpha Magnetic Spectrometer
Dark Matter Searches with AMS-02 AMS: Alpha Magnetic Spectrometer 2007/2008 Wim de Boer on behalf of the AMS collaboration University of Karlsruhe July, 20. 2004 COSPAR, Paris, W. de Boer, Univ. Karlsruhe
More informationMøller Polarimetry for PV Experiments at 12 GeV
Outline E.Chudakov Jan 15, 2010, MOLLER Review Møller Polarimetry 1 Møller Polarimetry for PV Experiments at 12 GeV E.Chudakov 1 1 JLab MOLLER Review Outline E.Chudakov Jan 15, 2010, MOLLER Review Møller
More informationThe DAΦNE Beam Test Facility
The DAΦNE Beam Test Facility Giovanni Mazzitelli & Paolo Valente Laboratori Nazionali di Frascati Overview BTF Parameters BTF operation mode Commissioning results First users experience Future plans Introduction
More informationThe APEX Experiment and Test Run
The APEX Experiment and Test Run Natalia Toro (Perimeter Institute) for the APEX Collaboration S. Abrahamyan, A. Afanasev, Z. Ahmed, E. Aliotta, K. Allada, D. Anez, D. Armstrong, T. Averett, A. Barbieri,
More informationSimulation for Proton Charge Radius (PRad) Experiment at Jefferson Lab1 Li Ye Mississippi State University For the PRad Collaboration The Proton Charg
Simulation for Proton Charge Radius (PRad) Experiment at Jefferson Lab1 Li Ye Mississippi State University For the PRad Collaboration The Proton Charge Radius Puzzle refers to 7 σ discrepancy between the
More informationObservation of UHECRs in horizontal flux
Observation of UHECRs in horizontal flux Igor Yashin - Moscow Engineering Physics Institute for DECOR Collaboration DECOR Collaboration M.B.Amelchakov 1, N.S.Barbashina 1, A.G.Bogdanov 1, D.V.Chernov 1,
More informationCoherent and incoherent nuclear pion photoproduction
Coherent and incoherent nuclear pion photoproduction Dan Watts, Claire Tarbert University of Edinburgh Crystal Ball and A2 collaboration at MAMI Gordon Conference on photonuclear reactions, August 2008
More informationRare B decays in ATLAS and CMS
Rare B decays in ATLAS and CMS University Dec. 14 th 2006 Makoto Tomoto Nagoya University on behalf of CMS and ATLAS collaborations Makoto Tomoto (Nagoya University) Outline B physics in ATLAS and CMS
More informationSPPS: The SLAC Linac Bunch Compressor and Its Relevance to LCLS
LCLS Technical Advisory Committee December 10-11, 2001. SPPS: The SLAC Linac Bunch Compressor and Its Relevance to LCLS Patrick Krejcik LCLS Technical Advisory Committee Report 1: July 14-15, 1999 The
More informationHall A Compton Calorimeter G. B. Franklin Carnegie Mellon University
Hall A Compton Calorimeter G. B. Franklin Carnegie Mellon University 1. Compton Scattering Polarimetry General Considerations Complications and Systematic Errors 2. CMU Integrating DAQ Content of Data
More informationThe Aʹ Experiment (APEX)
The Aʹ Experiment (APEX) Searching for New Gauge Bosons in the Aʹ Experiment at Jefferson Laboratory Natalia Toro (Perimeter Institute) for the APEX Collaboration S. Abrahamyan, Z. Ahmed, K. Allada, D.
More informationDevelopment of a Time Projection Chamber with GEM technology in IMP. Herun yang Gas detector group
Development of a Time Projection Chamber with GEM technology in IMP Herun yang Gas detector group Outline Introduction TPC prototype based on GEM performance test based cosmic ray Beam test Summary Gas
More informationMINOS. Physics Program and Construction Status. Karol Lang The University of Texas at Austin. YITP: Neutrinos and Implications for Physics Beyond
MINOS Physics Program and Construction Status Karol Lang The University of Texas at Austin YITP: Neutrinos and Implications for Physics Beyond YITP Conference: Neutrinos and Implications The Standard for
More informationA Search for Point Sources of High Energy Neutrinos with AMANDA-B10
A Search for Point Sources of High Energy Neutrinos with AMANDA-B10 Scott Young, for the AMANDA collaboration UC-Irvine PhD Thesis: http://area51.berkeley.edu/manuscripts Goals! Perform an all-sky search
More informationLAB 10: OPTICAL MATERIALS AND DISPERSION I
OPTI 202L - Geometrical and Instrumental Optics Lab LAB 10: OPTICAL MATERIALS AND DISPERSION I 10-1 Measuring the refractive index of a material is one of the most fundamental optical measurements, and
More informationMeasurement of the lifetime and of weak decay partial widths of mirror p-shell Λ-hypernuclei
Measurement of the lifetime and of weak decay partial widths of mirror p-shell -hypernuclei International Workshop on Physics at the extended Hadron Experimental Facility of J-PARC March 5-6, 2016, J-PARC,
More informationBeam Dump Experiments with Photon and Electron Beams
Beam Dump Experiments with Photon and Electron Beams Electron beams BDX at Jefferson Lab Signal and backgrounds Muon flux measurements Status Elton S. Smith, Jefferson Lab On behalf of the BDX Collaboration
More informationA model of the Earth's gamma-ray emission for GLAST derived from EGRET data. Dirk Petry (UMBC, NASA/GSFC) DC2 Meeting GSFC June 27-29, 2005
A model of the Earth's gamma-ray emission for GLAST derived from EGRET data (UMBC, NASA/GSFC) DC2 Meeting GSFC June 27-29, 2005 1 Gamma-ray emission from the Earth's atmosphere Incoming cosmic rays Cosmic
More information!"#"$%&!"'()%'&*$&+,-*%./0*1),2$3& 4)"#%-1$&5#,6"-*$3&,%&7"8"-'1$&9,:;& A"$%&+,'#BC"
!"#"$%&!"'()%'&*$&+,-*%./0*1),2$3& 4)"#%-1$&5#,6"-*$3&,%&7"8"-'1$&9,:;& +!4?++4?++4
More informationDevelopment of a Dedicated Hard X-Ray Polarimeter Mark L. McConnell, James R. Ledoux, John R. Macri, and James M. Ryan
Development of a Dedicated Hard X-Ray Polarimeter Mark L. McConnell, James R. Ledoux, John R. Macri, and James M. Ryan Space Science Center University of New Hampshire Durham, NH AAS-HEAD Mt. Tremblant,
More information2.24 Simulation Study of K L Beam: K L Rates and Background Ilya Larin Department of Physics Old Dominion University Norfolk, VA 23529, U.S.A.
2.24 Simulation Study of K L Beam: K L Rates and Background Ilya Larin Department of Physics Old Dominion University Norfolk, VA 23529, U.S.A. Abstract We report our simulation results for K L -beam and
More informationPrimary CR Energy Spectrum and Mass Composition by the Data of Tunka-133 Array. by the Tunka-133 Collaboration
Primary CR Energy Spectrum and Mass Composition by the Data of Tunka-133 Array by the Tunka-133 Collaboration Tunka-HiSCORE: First results on all-particle spectrum by the Tunka-HiSCORE Collaboration combined
More informationElectron Beam Polarimetry at Jefferson Lab Dave Gaskell Jefferson Lab (Hall C)
Electron Beam Polarimetry at Jefferson Lab Dave Gaskell Jefferson Lab (Hall C) CASA Beam Physics Seminar February 14, 2008 1. Motivation: Why do we care so much about polarimetry? 2. Overview of JLab polarimeters
More informationHall-D Update. Eric Pooser. Joint Hall A/C Summer Collaboration Meeting 07/18/2015
1 Hall-D Update Joint Hall A/C Summer Collaboration Meeting 07/18/2015 Current Hall-D Physics Program 2 Slide Courtesy of E. Chudakov Hybrid & Exotic Hybrid Mesons 3 Conventional light mesons (π, K, η,
More informationCW POSITRON SOURCE AT CEBAF
CW POSITRON SOURCE AT CEBAF by Serkan Golge B.S. July 2002, Fatih University M.S. December 2005, Old Dominion University A Dissertation Submitted to the Faculty of Old Dominion University in Partial Fulfillment
More informationLHC State of the Art and News
LHC State of the Art and News ATL-GEN-SLIDE-2010-139 16 June 2010 Arno Straessner TU Dresden on behalf of the ATLAS Collaboration FSP 101 ATLAS Vulcano Workshop 2010 Frontier Objects in Astrophysics and
More informationThe QWeak Experiment: A measurement of the proton weak charge and up-down quark weak couplings.
The QWeak xperiment: A measurement of the proton weak charge and up-down quark weak couplings. University of Manitoba -mail: mgericke@physics.umanitoba.ca In May 2012, the Q p Weak collaboration completed
More informationBari Osmanov, University of Florida. OscSNS - proposal for neutrino experiment at ORNL SNS facility
, University of Florida OscSNS - proposal for neutrino experiment at ORNL SNS facility 1 of 19 Outline ORNL SNS facility Neutrino production at SNS Neutrino detection at SNS Event reconstruction and particle
More information* * TASCA in Small Image Mode Spectroscopy
TAS ISpec TASCA in Small Image Mode Spectroscopy * * * * * Introducing the set up TASCA SIM settings Commissioning experiments Characteristics Future: Missing parts / preparations Experiments Why TAS ISpec?
More information7th IPAC, May 8-13, 2016, Busan, Korea
7th IPAC, May 8-13, 2016, Busan, Korea ER@CEBAF A High-Energy, Multiple-Pass, Energy Recovery Experiment at CEBAF On behalf of the JLab-BNL ER@CEBAF collaboration : I. Ben-Zvi, Y. Hao, P. Korysko, C. Liu,
More informationMOLLER Experiment. Many slides courtesy of K. Kumar, K. Paschke, J. Mammei, M. Dalton, etc.
MOLLER Experiment D.S. Armstrong Nov. 9 2010 Precision Tests of the Standard Model ECT* Workshop Moller scattering: intro Previous measurement: SLAC E158 MOLLER: new physics reach Experimental Concept
More information