Overview: E (x>1) E (EMC)

Slides:



Advertisements
Similar presentations
BigBite K.Egiyan Probabilities of SRC in Nuclei Measured with A(e,e / ) Reactions K. Egiyan (Yerevan Physics Institute, Yerevan, Armenia and Jefferson.
Advertisements

PR : Precision Measurements and Studies of a Possible Nuclear Dependence of R = L / T Simona Malace - contact (JLab) Eric Christy (Hampton U.),
Ioana Niculescu James Madison University August 15, 2013.
MeAsurement of F 2 n /F 2 p, d/u RAtios and A=3 EMC Effect in Deep Inelastic Electron Scattering Off the Tritium and Helium MirrOr Nuclei J. Gomez for.
High precision study of the  decay of 42 Ti  V ud matrix element and nuclear physics  Experimental and theoretical precisions  New cases: goals and.
DNP Long Range Plan January Nuclei at Short Distance Scale Ronald Ransome Rutgers, The State University of New Jersey Piscataway, NJ.
Eli Piasetzky Tel Aviv University, ISRAEL Short Range Correlations and the EMC Effect Work done in collaboration with: L. B. Weinstein (ODU) D. Higinbotham,
Coulomb distortion in the inelastic regime Patricia Solvignon Argonne National Laboratory Work done in collaboration with Dave Gaskell (JLab) and John.
Status of Hall C 6 GeV Analysis Software Robust Fortran/CERNLIB code, “ENGINE”, for analysis of HMS/SOS coincidence and single arm experiments that has.
Experiment Rosen07: Measurement of R =  L /  T on Deuterium in the Nucleon Resonance Region. 1  Physics  Data Analysis  Cross Section calculation.
Does a nucleon appears different when inside a nucleus ? Patricia Solvignon Argonne National Laboratory Postdoctoral Research Symposium September 11-12,
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)
Status of Hall C 6 GeV Analysis Software Robust Fortran/CERNLIB code, “ENGINE”, for analysis of HMS/SOS coincidence and single arm experiments that has.
Precision measurements of the F 2 structure function at large x in the resonance region and beyond S. Malace, PAC35 January 2010, Jefferson Lab Outline.
 4 He(e,e'p)X, April 13 and April 14, 2011, 16 hours Measured P miss at to 1.0 GeV/c, x b = 1.24, Q 2 = 2 (GeV/c) 2 Extension of SRC 2 body data.
Future Physics at JLab Andrew Puckett LANL medium energy physics internal review 12/14/
Measurement of F 2 and R=σ L /σ T in Nuclei at Low Q 2 Phase I Ya Li Hampton University January 18, 2008.
EMC effect in few-body nuclei at large x Patricia Solvignon Argonne National Laboratory Elba X Workshop Electron-Nucleus Scattering X June 23-27, 2008.
Charged Kaon Production Yield Studies with Stretcher Sergei Striganov Fermilab Future of Kaon Physics at Fermilab August 21, Fermilab.
A Measurement of Two-Photon Exchange in Unpolarized Elastic Electron-Proton Scattering John Arrington and James Johnson Northwestern University & Argonne.
Transverse Momentum Dependence of Semi-Inclusive Pion and Kaon Production E : Spokespersons Peter Bosted, Rolf Ent, Hamlet Mkrtchyan 25.5 days.
Model independent extraction of neutron structure functions from deuterium data. Svyatoslav Tkachenko University of South Carolina.
Nilanga Liyanage University of Virginia For Jefferson Lab Hall A, CLAS and RSS Collaborations.
Pion-Induced Fission- A Review Zafar Yasin Pakistan Institute of Engineering and Applied Sciences (PIEAS) Islamabad, Pakistan.
 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.
New measurements of the EMC effect in few-body nuclei John Arrington, Physics Division, Argonne Second meeting of the APS Topical Group on Hadron Physics.
Experiment Rosen07: Measurement of R =  L /  T on Deuterium in the Nucleon Resonance Region.  Physics  Data Analysis  Cross Section calculation 
New Measurement of the EMC effect for Light Nuclei and Global Study of the A-Dependence Patricia Solvignon Argonne National Laboratory ECT 2008 Workshop.
New global study of the A-dependence of the EMC effect and the extrapolation to nuclear matter Patricia Solvignon Argonne National Laboratory Physics Division.
Status of Hall C 6 GeV Analysis Software Robust Fortran/CERNLIB code, “ENGINE”, for analysis of HMS/SOS coincidence and single arm experiments that has.
Comparison of GENIE with Garino Data Xin Qian BNL In collaboration with Steve Dytman 1.
Envisioned PbWO4 detector Wide-Angle Compton Scattering at JLab-12 GeV with a neutral-particle detector With much input from B. Wojtsekhowski and P. Kroll.
Non-Prompt J/ψ Measurements at STAR Zaochen Ye for the STAR Collaboration University of Illinois at Chicago The STAR Collaboration:
Bryan Moffit PAC32 Dry Run Precision Measurement of the Proton Elastic Cross Section at High Q 2 PAC32 12 GeV Proposal : PR Spokespersons:Bryan.
Nuclear structure and the flavor dependence of the EMC effect
John Arrington Argonne National Lab
x>1: Short Range Correlations and “Superfast” Quarks
Short Range NN Correlations (from Inclusive Cross Sections)
John Arrington Argonne National Lab
Probing Quark – Gluon correlations in the neutron Precision measurements of d2n and g2n Brad Sawatzky for the E Collaboration.
Kaons Propagation Through Nuclei
E Measuring the Neutron g2 and d2 at 12 GeV
Plans for nucleon structure studies at PANDA
JLab6: Cluster structure connects to high-momentum components and internal quark modification of nuclei Short-Range Correlations (SRCs) dominated by np.
Flavor dependence of the EMC effect
Nadia Fomin University of Virginia
Precision Measurement of η Radiative Decay Width via Primakoff Effect
presented by Werner Boeglin Florida International University Miami
Deep Inelastic Parity Robert Michaels, JLab Electroweak Physics
Larisa Nogach Institute of High Energy Physics, Protvino
Special Considerations for SIDIS
Large-X PDFs in the Drell-Yan Process
Duality in Pion Electroproduction (E00-108) …
how is the mass of the nucleon generated?
High-pT Identified Charged Hadrons in √sNN = 200 GeV Au+Au Collisions
University of Tennessee
Duality in 12 GeV Era: Projected Results from E
Identified Charged Hadron Production at High pT
Early running planning process
Argonne National Laboratory
Scaling Study of the L-T Separated p(e,e’π+)n Cross Section at Large Q2 Tanja Horn Jefferson Lab APS/DNP meeting 2007 DNP07 October 2007.
Duality in Nuclei: The EMC Effect
Update of RG-A Hadron Structure Analyses
New Results on the EMC Effect at Large x in Light to Heavy Nuclei
Semi-Inclusive DIS measurements at Jefferson Lab
University of Tennessee
25.5 days at 11.0 GeV & 6.5 days at 8.8 GeV = 32 days total
E (“x>1”) PAC47 Jeopardy presentation John Arrington
Deuteron Electro-Disintegration at Very High Missing Momenta PR Hall C Collaboration Experiment Probe two nucleon dynamics at short space-time distances.
E , Spokespersons: P. Bosted, R. Ent, E. Kinney, and H. Mkrtchyan
Presentation transcript:

Overview: E12-06-105 (x>1) E12-10-008 (EMC) Experimental readiness review Overview: E12-06-105 (x>1) E12-10-008 (EMC) drhgfdjhngngfmhgmghmghjmghfmf John Arrington Argonne National Laboratory June 8, 2017 Newport News, VA

Outline Addressing charge items 3 and 6 Physics Overview Emphasis on key requirements for kinematics, performance, etc… Run plan Collaboration Readiness Documentation

Physics overview Focus on experimental requirements E12-06-105 (x>1): J. Arrington, D. Day, N. Fomin QE scattering from high-momentum nucleons (>kF) arising from hard, short-range N-N interactions to study short-range correlations (SRCs) in nuclei DIS scattering at x>1: Probe distribution of super-fast quarks (SFQs) in nuclei E12-10-008 (EMC): J. Arrington, A. Daniel, N. Fomin, D. Gaskell DIS from range of nuclei to study Nuclear effects in parton distributions Combined: Examine EMC-SRC correlation as function of A and N/Z Several Common Requirements Inclusive scattering with reasonable rates, modest backgrounds Study wide range of nuclei to examine A-dependence and isospin-dependence of SRC contributions, nuclear pdfs Scan range of angles to examine Q2 dependence Most observables focus on A/2H ratios; common systematics

EMC-SRC correlation How are EMC effect, SRCs related? High-momentum vs. high-density? EMC effect as small modification in all nucleons vs. large effect limited within SRCs? JA, A. Daniel, D. Day, N. Fomin, D. Gaskell, P. Solvignon, PRC 86, 065204 (2012) N. Fomin, et al., PRL 108, 092052 (2012) L. Weinstein, et al., PRL 106, 052301 (2011) J. Seely, et al., PRL103, 202301 (2009)

Run plan: Targets 1H 2H 3He 4He 6,7Li 9Be 10,11B 12C 27Al 40*,48Ca Light nuclei: Reliable calculations of nuclear structure (e.g. clustering) Run plan: Targets Both experiments use wide range of nuclear targets to study impact of cluster structure, separate mass and isospin dependence on SRCs, nuclear PDFs Additional foil targets (dark blue) added to original proposal. No additional beam time required, no special target issues All targets measured for SRCs, EMC effect at high-rate kinematics. Select targets run at higher Q2 to study Q2 dependence or extend kinematic reach Nadia Fomin, Dave Meekins will cover technical details 1H 2H 3He 4He 6,7Li 9Be 10,11B 12C 27Al 40*,48Ca 48Ti 54Fe 58,64Ni 64*Cu 108*Ag 119*Sn 197*Au 232Th Heavier nuclei: Cover range of N/Z at ~fixed values of A

Run plan: Kinematics overview Both experiments cover range of angles (20-55º) to examine Q2 dependence of structure functions [angles shifted from proposal to increase compatibility] Main PDF measurements at 20, 33º (EMC), or x≥1: modest pion backgrounds High-x SRCs requires small angle Need SHMS for E’ ≈ 11 GeV Need ‘medium’ beam pipe HMS: 20-55º, 1.4-6.4 GeV/c SHMS: 8-33º, 1.4-10.6 GeV/c All data taking at 11 GeV Focus on target ratios Light nuclei: cluster structure Heavier nuclei: vary N/Z EMC x>1 EMC effect vs A, N/Z Larger Q2 pushes to highest x PDFs at x>1 x, Q2 dependence A-dependence of SRCs

Run plan overview Basic Run plan: 23 PAC days EMC, 32 days x>1 Assume 2 days will be completed during Hall C commissioning 7 days for EMC effect at 20º [all targets, HMS and SHMS in parallel] 6 (3) days for selected targets at 35 (40) degrees 6 days overhead, calibrations, … 4 days for x>1 at 8º [SHMS] 4 days for selected targets at 10º 17 days for high Q2 x>1 (2H,C,Cu) EMC x>1 EMC effect vs A, N/Z Larger Q2 pushes to highest x PDFs at x>1 x, Q2 dependence Notes: Proposed 80uA; assuming 60uA Single ladder with all solid targets Start with 1,2H, taking data with all targets; 1 day target changeover before running 3,4He (+C, dummy) A-dependence of SRCs

Manpower and analysis overview Charge item 3 Confirmed participation 12 institutions (JLab, UVa, ANL, UT, UNH, JMU, MSU, Ohio - key collabs.) Estimated participation of 40 Faculty/Staff, 10 Postdocs, 20 Graduate students (4 Thesis) Analysis Relatively simple analysis; key issues are similar for x>1 and EMC (inclusive scattering, rapidly varying cross sections, focus on target ratios) Follows all the same procedures as 6 GeV “XEM” rungroup Have calibration codes, cross section models, radiative corrections, etc… Arrington/Day/Gaskell spokespersons for 6 GeV run Daniel/Fomin were graduate students on EMC/x>1 Plan to treat both experiments as single analysis, with students focusing on different physics aspects Calibrations, simulations, analysis, etc… will all be tested during F2p/F2d commissioning run Expect 4 Thesis students: 2 focusing on x>1 physics, 2 on EMC physics

Experimental, analysis requirements Charge item 6 Conventional trigger and efficiency studies: high efficiency, low background, modest rates Working version of C++/ROOT analyzer exists (validated against 6 GeV code) Full simulations (realistic cross section model, detailed radiative corrections, spectrometer models, etc….) exist now SHMS spectrometer model checked during 2017 run All aspects of x>1/EMC data taking and analysis will be tested during Hall C commissioning (small subset of targets being run with F2p/F2d due to significant kinematic overlap) EMC and x>1 physics analysis will follow the same procedures as Tritium rungroup experiments. Codes and procedures will be well tested, the collaboration includes most current experts, and the Tritium rungroup and Hall C commissioning data will provide many more experts

Responsibilities for running/analysis Nadia will discuss hardware responsibilities Run plan Physics plan: Arrington, Fomin (+ Day, Gaskell, postdoc) Calibrations: Gaskell, Fomin (+ Arrington, postdoc, Thesis students) Online analysis Will assign responsibility for detector checks, calibration monitoring, data quality checks, etc… to specific postdocs/students for each subsystems Coordinated by Gaskell, local postdoc Physics Analysis Lead student will be identified for each spectrometer subsystem, other thesis students will verify quality of final calibrations, optics, etc… for their data sets PhD students will perform basic cross section extraction for full data sets Significant cross-checks Extraction of physics results separate for x>1, EMC Analysis is identical to what is required for F2p/F2d commissioning running

Documentation Charge element 6 Experiments use only standard equipment except for new targets, most of which have no additional procedures or documentation requirements Steve Wood is generating updated documentation Will use the standard Hall C COO, ESAD, ERG Greg Smith has identified the minimal additions to the Standard Equipment Manual needed for Helium targets Will get full RSAD from Radcon (have prelim. calculations) Standard OSPs, Operation manuals, etc… Physics Div. Liaison assigned: Simona Malace