A Staged approach to the Super Bigbite Project The Super Bigbite Project is designed to provide precision measurements of the nucleon form factors G E.

Slides:



Advertisements
Similar presentations
E05-102: Measurement of A x and A z asymmetries in the quasi-elastic 3 He(e,e'd) reaction Hall A Collaboration Meeting Xiaohui Zhan MIT prsented by Measurement.
Advertisements

Super BigBite concepts Bogdan Wojtsekhowski, JLab
April 06, 2005 JLab 12 GeV upgrade DOE Science Review 1 Fundamental Structure of Hadrons Zein-Eddine Meziani April 06, 2005 DOE Science Review for JLab.
Target Fragmentation studies at JLab M.Osipenko in collaboration with L. Trentadue and F. Ceccopieri, May 20,SIR2005, JLab, Newport News, VA CLAS Collaboration.
Jin Huang PhD Candidate, MIT For MENU 2010 May 31, Williamsburg.
Ozgur Ates Hampton University TREK Experiment “Tracking and Baseline Design” And OLYMPUS Experiment “Study of Systematics” 1.
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.
SBS Budget A Staged Approach John J. LeRose Hall A Collaboration Meeting December 10, 2010.
The Size and Shape of the Deuteron The deuteron is not a spherical nucleus. In the standard proton-neutron picture of this simplest nucleus, its shape.
SBS Program Management John J. LeRose SBS Collaboration Meeting October 18,
Jefferson Lab Status Hall A collaboration Dec. 16, 2013 R. D. McKeown Deputy Director For Science.
1 SBS Spectrometer / GEP5 Conf.. 2 Tracking Requirements Requirements Tracking Technology DriftMPGDSilicon High Rate: MHz/cm 2 (Front Tracker)
THE DEEP INELASTIC SCATTERING ON THE POLARIZED NUCLEONS AT EIC E.S.Timoshin, S.I.Timoshin.
Future Opportunities at an Electron-Ion Collider Oleg Eyser Brookhaven National Laboratory.
AM Software Review. Hall C after 12 GeV Upgrade Beam Energy: 2 – 11 GeV/c Super High Momentum Spectrometer (SHMS) –Horizontal Bender, 3 Quads, Dipole.
12 GeV Science Program R. D. McKeown JSA Science Council January 7, 2011 Thanks to A. Lung, L. Cardman, others.
UK Hadron Physics D. G. Ireland 10 October 2014 NuPECC Meeting, Edinburgh.
A High Precision Measurement of the Deuteron Spin-Structure Function Ratio g 1 /F 1  Motivation  Proposed Experiment  Expeced Results Co:spokespersons:
Possibility for Double DVCS measurement in Hall A Alexandre Camsonne SBS Meeting June 4 th 2013.
Xiaodong Jiang Gluon spin with longitudinal asymmetries at RHIC. Parton angular motion - transverse spin asymmetries. Spin at RHIC : p+p. Spin at JLab:
John LeRose March 12, A Program of three “projects” to assemble the Super BigBite Spectrometer for a series of experiments in Hall A There is a.
Spin-Flavor Decomposition J. P. Chen, Jefferson Lab PVSA Workshop, April 26-27, 2007, Brookhaven National Lab  Polarized Inclusive DIS,  u/u and  d/d.
The Bigbite second GEM tracker. SBS GEM Trackers Front Tracker Geometry x6 18 modules In Italy  50 cm x 40 cm Modules are assembled to form larger chambers.
Particle Physics Chris Parkes Experimental QCD Kinematics Deep Inelastic Scattering Structure Functions Observation of Partons Scaling Violations Jets.
HallA/SBS – Front Tracker PARAMETERDESIGN VALUE Microstrip Silicon Detector Number of tiles/plane and size2 Number of planes2 Size of the single
Future Physics at JLab Andrew Puckett LANL medium energy physics internal review 12/14/
GEM chambers for SoLID Nilanga Liyanage University of Virginia.
GEM chambers for SoLID Nilanga Liyanage University of Virginia.
Large acceptance magnetic spectrometer for the 12 GeV 2 GEp experiment (at Jefferson Lab) E. Cisbani INFN Rome – Sanità Group and Italian National Institute.
GEM Trackers for Super BigBite Spectrometer (SBS) in Hall JLab The Super Big Bite Spectrometer (SBS) is one of the major new equipment in hall A in.
General Discussion some general remarks some questions.
G E p -2γ experiment and the new JLab Hall-C Focal Plane Polarimeter Mehdi Meziane The College of William & Mary - APS Meeting April 14, On behalf.
Vina Punjabi Norfolk State University Hall A Collaboration Meeting June 10-11, 2010 GEp-V Experiment to Measure G Ep /G Mp.
The Quark Structure of the Nucleon Inti Lehmann & Ralf Kaiser University of Glasgow Cosener’s House Meeting 23/05/2007 Nucleon Structure Generalised Parton.
Proton Charge Form Factor Measurement E. Cisbani INFN Rome – Sanità Group and Italian National Institute of Health 113/Oct/2011E. Cisbani / Proton FF.
MOLLER Collaboration Meeting May 2014 Hall A Update Thia Keppel 1.
Jefferson Laboratory Hall A SuperBigBite Spectrometer Data Acquisition System Alexandre Camsonne APS DNP 2013 October 24 th 2013 Hall A Jefferson Laboratory.
E Precision Measurement of the Neutron Magnetic Form Factor up to Q 2 =13.5 (GeV/c) 2 by the Ratio Method B. Quinn, J. Annand, R. Gilman, B. Wojtsekhowski.
Transverse Momentum Dependence of Semi-Inclusive Pion and Kaon Production E : Spokespersons Peter Bosted, Rolf Ent, Hamlet Mkrtchyan 25.5 days.
Test of the GEM Front Tracker for the SBS Spectrometer at Jefferson Lab F. Mammoliti, V. Bellini, M. Capogni, E. Cisbani, E. Jensen, P. Musico, F. Noto,
The 12 GeV Physics Program at Jefferson Lab R. D. McKeown Jefferson Lab College of William and Mary PTSP 2013 – Charlottesville, VA September 9, 2013.
GEp-III in Hall C Andrew Puckett, MIT On behalf of the Jefferson Lab Hall C GEp-III Collaboration April 15, 2008.
Transverse Single-Spin Asymmetries Understanding the Proton: One of the fundamental building blocks of ordinary matter! Spin decomposition of proton still.
Daniel S. Carman Page 1 Hadron Sep , 2015 Daniel S. Carman Jefferson Laboratory N* Spectrum & Structure Analysis of CLAS Data  CLAS12 N*
Dual Target Design for CLAS12 Omair Alam and Gerard Gilfoyle Department of Physics, University of Richmond Introduction One of the fundamental goals of.
Modifying the PMP (remove some GEM’s add a scintillator coordinate detector) -JJL (8/29/2012)
MPC-EX hardware design and capability The MPC-EX detector system is an extension of the existing Muon Piston Calorimeters (MPCs) of the PHENIX experiment.
The 12 GeV equipment Hall D – Hall D – GLUEx detector for photoproduction experiments Hall B – Large acceptance detector CLAS12 for high luminosity measurements.
Front Tracker: main technical solutions 40x50 cm 2 module Front Tracker Chamber: 40x150 cm 2  Use COMPASS approach: 3xGEM, 2D readout - one significant.
 0 life time analysis updates, preliminary results from Primex experiment 08/13/2007 I.Larin, Hall-B meeting.
JLab, October 31, 2008 WACS in 12 GeV era 1 GPDs Wide-Angle Compton Scattering pi-0 photo-production in 12 GeV era B. Wojtsekhowski Outline WACS and other.
1 Melynda Brooks, “Understanding the Origin of the Nucleon Spin” Understanding the Origin of the Nucleon Spin Andi Klein, P-23, Melynda Brooks P-25, Pat.
RHIC-PV, April 27, 2007 M. Rijssenbeek 1 The Measurement of W ’s at the CERN and FNAL hadron colliders W ’s at RHIC ! W ’s at CERN – UA2 W ’s at FNAL -
Relativistic Nuclear Collisions (RNC) Group Nuclear Science Division (NSD), Lawrence Berkeley National Lab Large Hadron Collider (LHC) Spin physics program.
Transverse Spin Physics with an Electron Ion Collider Oleg Eyser 4 th International Workshop on Transverse Polarisation Phenomena in Hard Processes Chia,
Hall A Update Thia Keppel User Group Board of Directors January 2015.
18 Oct 2010 / PSHP / Frascati E. Cisbani: JLab/Hall A April Frascati Probing Strangeness in Hard Processes Kaon SIDIS experiments.
Understanding the 3 He Nuclei: Asymmetry Measurements in Quasi- Elastic Ge Jin University of Virginia For the E Collaboration.
Jefferson Lab PAC 30 1 August 23, 2006 PR (Hall A) ● PR (Hall C) Measuring the Neutron g 2 and d 2 at 12 GeV PR (Hall A) ● PR
Timelike Compton Scattering at JLab
Structure and Dynamics of the Nucleon Spin on the Light-Cone
Hadron Form Factors Rolf Ent Jefferson Lab
Neutron (e,e’π±) Target Single-Spin Asymmetry in Semi-inclusive DIS on a Transversely Polarized 3He Target - Kalyan Allada, Chiranjib Dutta, Mitra Shabestari,
A Precision Measurement of GEp/GMp with BLAST
Special Considerations for SIDIS
Introduction and Workshop Charge
GEANT Simulations and Track Reconstruction
Physics program in Hall A for the CEBAF 12 GeV era
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.
PHYS 3446 – Lecture #23 Standard Model Wednesday, Apr 25, 2012
Presentation transcript:

A Staged approach to the Super Bigbite Project The Super Bigbite Project is designed to provide precision measurements of the nucleon form factors G E n, G M n and G E p to unprecedented values of Q 2, and to enable a greatly expanded program of DIS experiments. The first stage, for 1.8M, will be comprised of:  Fully approved: G E n (50 days) and G M n (25 days). The second stage is for 2.3M. The second stage will open the door to a large group of Super Bigbite experiments including:  Fully approved: G E p to 15 GeV 2 (45days),  Conditionally approved: SIDIS: Transversity for 3 He(e,e’π/K), high-x u/d ratio using T & 3 He  In planning stages: A 1 n (high Q 2 ), DIS(e,e’ ϕ ), Transversity in (e,e’π o ), PVDIS w 70 msr,, and G E n and F π using a neutron polarimeter. 1

In this presentation we discuss: The excellent quality of the physics that will come out of Stage I. The structure of the project and its budget. The reasons it is so important to move forward quickly 2

The first Hall A gEn experiment First GEn data in the high Q 2 regime where unexpected results were seen for G E p /G M p. Fairly consistent with theoretical explanations of G E p /G M p, thus supporting the importance of quark orbital angular momentum in nucleon structure. Closest agreement is with the Argonne DSE that incorporates dynamic generation of mass, and contains diquark degrees of freedom. 3

Flavor separated dependence for F 1 & F 2 4 With the Hall A results for G E n, the assumption of isospin symmetry, and existing proton results, it is possible to determine F 1 and F 2 separately for u quarks d quarks to high values of Q 2. What is clearly evident is that the ratio drops off markedly for higher values of Q 2, indicating that the d quark is more spatially diffuse than are the u quarks. Shown at left is the ratio of F 1 d and F 1 u for the d and u quarks as they exist in the proton.

The first Hall A g E n experiment enables a more detailed visualization of the neutron 5 Core is positive and “proton like” Core is surrounded by negative pion cloud Naive charge density representing the Fourier transform of the neutron electric form factor Covariant light-front transverse “charge” density in impact- parameter space. After the charge, spin and magnetic moment, the elastic form factors are among the nucleon’s most fundamental properties, telling us their “size and shape”.

Intriguing observation that the ratio F2/F1 is roughly constant over 1 < Q 2 < 3.4 GeV 2  diquark configuration?  An effect of orbital motion? Accurate data at higher Q 2 could reshape our thinking of valence quark structure The first Hall A GEn experiment enabled the flavor decomposition of F 1 and F 2 at high Q F 1,2 u = 2F 1,2 p + F 1,2 n F 1,2 d = F 1,2 p + 2F 1,2 n κ d -1 F 2d / F 1d κ u -1 F 2u / F 1u 6

Stage I of The Super Bigbite program following the 12 GeV upgrade 7

Hall A G E n (E ) will provide dramatic new insight into nucleon structure The dramatic turnover of the Argonne DSE model would be clearly visible. If the turnover is seen, it would provide strong evidence for the importance of diquark degrees of freedom in the nucleon form factors. 8

Hall A G M n (E ) will provide superb accuracy WILL GREATLY IMPROVE THE ACCURACY WITH WHICH G M n KNOWN, AND IS ESSENTIAL FOR EXTRACTING G E n, F 1, F 2 AND DOING FLAVOR DECOMPOSITIONS. WILL GREATLY IMPROVE THE ACCURACY WITH WHICH G M n KNOWN, AND IS ESSENTIAL FOR EXTRACTING G E n, F 1, F 2 AND DOING FLAVOR DECOMPOSITIONS. COMPARED TO HALL B, WILL ACHIEVE superior accuracy IN half the time, WITH INDEPENDENT SYSTEMATIC ERRORS. COMPARED TO HALL B, WILL ACHIEVE superior accuracy IN half the time, WITH INDEPENDENT SYSTEMATIC ERRORS. 9

Projected flavor decomposition using the E data The flavor decomposition of F 1 using G M n /G M p represents a unique opportunity to see deep inside the nucleon. GPD’s will need to be seriously modified to accommodate F 1 d /F 1 u going through zero. 10 Two highest points in planning stage.

The layout of the Super Bigbite apparatus with all components for GEp(5) Scatterin g chamber Vacuu m snout Magnetic shield First tracke r Second tracker Hadron calorimet er Beam line Pb shield 48D48 magn et Third tracker CH2 analyzer Bea m 11

The layout of the Super Bigbite apparatus necessary for the Neutron FFs 48D48 magnet Hadron calorimete r GEM-based “First trackers” Single-axis GEM tracker Magnetic:  beam-line cut, power, support platform  but without new coils, lead shielding Hadron calorimeter GEM-based veto in front of hadron calorimeter. INFN funded GEM-based “First tracker” from SBS BigBite 12

The layout of the Super Bigbite apparatus necessary for the Neutron FFs 48D48 magnet Hadron calorimete r GEM-based “First trackers” Single-axis GEM tracker TOSCA calculation was performed and showed that single coil solution is quite adequate for both G E n and G M n 13

All amounts are in $ k stage I budget for Super Bigbite 14 ItemInstitution Total Magnet, DC power, Beam line and university contracts overhead Jlab Hadron CalorimeterCMU Coordinate detectorUVa Total ,797 ItemSourceAmount SBS Front GEM TrackerINFN1,050 (720 k Euro) Clean room and DAQ electronicsUVa match 50 Readout ChipsUVa on hand 10 Total non-DOE contributions1,110 Non-DOE contributions DOE contributions Jlab Contribution1,797 Non-DOE contributions1,110 Total Stage I Budget2,907

ItemQuantityUnit costContingencyOverheadTotal GEM foil86$1,55020%--$160,000 Readout Boards26$ 38530%--$13,000 Supplies1$ 10,00020%--$ 12,000 Tooling1$ 5,00020%--$6,000 Gas plumbing1$ 2,00020%--$ 2,400 HV distribution1$ 2,75020%--$ 3,300 Support frames2$ 2,50020%--$ 6,000 Readout electronics1$ 129,00020%--$ 154,800 Technician (FTE)2$ 59, %$ 180,000 Total$537,500 ItemCostContingencyTotalNotes Clean room and supplies$14,60020%$17,520Proposed UVa match VME electronics$ 27,00020%$ 32,500Proposed UVa match Readout chips$ 10,000--$ 10,000In hand the coordinate detector at Uva Support from other sources: 15

hadron calorimeter at Carnegie mellon 16 ItemQuantityUnit costContingencyOverheadTotal Shower modules250$ 68030%--$ 221,000 LED Monitoring1$ %--$ 6,630 Tooling1$ 18,00030%--$ 23,400 Transportation1$ 40,00030%--$ 52,000 Total$ 303,030

STage I DOE funds spent at jlab 17 All amounts are in $ k Item Total Magnet DC Power Beam Line Detector Supports0750 university contracts overhead Total

Stage II of The Super Bigbite program following the 12 GeV upgrade 18 The second stage comprising a measurement of G E p and more can be completed for an additional 2.3M USD. The second stage will open the door to a large group of Super Bigbite experiments including:  Fully approved: G E p to 15 GeV 2 (45days)  Conditionally approved: SIDIS: Transversity for 3 He(e,e’π/K), high-x u/d ratio using T & 3 He  In planning stages: A 1 n (high Q 2 ), DIS(e,e’ ϕ ), Transversity in (e,e’π o ), PVDIS w 70 msr,, and G E n and F π using a neutron polarimeter.

The 12 GeV G E p /G M p Experiment The proton form factor, according to the most recent NSAC LRP, “... remains the only source of information about quark distributions at small transverse distance scales." Super Bigbite is the only way to obtain good accuracy at the necessary Q 2 scaling with existing equipment and roughly half the time

Key goals of the 12 GeV program Super Bigbite, together with Bigbite, is the only way to push A1n to x=0.8. Super Bigbite is currently conditionally approved as the basis for the tritium expt.

The 12 GeV A1n Experiment E GeV 8.8 GeV 11 GeV

All amounts are in $ k stage II budget for super bigbite 22 ProjectProject Execution Total New coils for magnet, Beam line, detector supports, and university contracts overhead Jlab Polarimeter GEM chambersUVa GEM ReadoutNSU GEM mechanicsW&M0720 TriggerRutgers Total Jlab contribution5991, ,345

All amounts are in $ k 23 STAGE II DOE FUNDS SPENT AT JLAB Item Total Magnet02120 DC Power0000 Beam Line03050 Detector Supports university contracts overhead Total

All amounts are in $ k Time line of DOE expenditures Stage I + Stage II Total cost to DOE : $ 4,142 k Total non-DOE contributions: $ 1,110 k + Labor

Why it is important to start the Super Bigbite Project now It is important to produce first-rate physics soon after establishing the upgraded beam. To be ready on time, work on the Super Bigbite project must begin now. Of the approved 12 GeV experiments for Hall A, 6 out of 12 require the Super Bigbite apparatus in one form or another. INFN is already moving at full speed to construct their GEM trackers. Delay of Super Bigbite could jeopardize our collaboration. Dubna proposed to build a calorimeter for $0.3M, which is very efficient. UVa has already accumulated experience with small GEM chambers, and has manpower assembled and ready to proceed. 25

26