E906 Spectrometer Upgrade Overview Paul E. Reimer Experimental Approach Impact on Fermilab Magnet Coil Fabrication Spectrometer Upgrades.

Slides:



Advertisements
Similar presentations
First results from the ATLAS experiment at the LHC
Advertisements

Introduction of trigger system: E906 as an example Shiuan-Hal,Shiu 05/02/
MTest Facility Low Energy Beam Erik Ramberg AEM 15 October, 2007.
Fermilab E906 Schedule Paul E. Reimer 20 June 2008.
NA60 results on charm and intermediate mass dimuon production in In-In 158 GeV/A collisions R. Shahoyan, IST (Lisbon) on behalf of the NA60 collaboration.
Experimental Status of Deuteron F L Structure Function and Extractions of the Deuteron and Non-Singlet Moments Ibrahim H. Albayrak Hampton University.
Ultra Peripheral Collisions at RHIC Coherent Coupling Coherent Coupling to both nuclei: photon~Z 2, Pomeron~A 4/3 Small transverse momentum p t ~ 2h 
20 June 2008E906 Collaboration Meeting1 Tracking Chambers for FNAL E906 Edward R. Kinney University of Colorado, Boulder, USA Overview of Station 1 Status.
Hall D Photon Beam Simulation and Rates Part 1: photon beam line Part 2: tagger Richard Jones, University of Connecticut Hall D Beam Line and Tagger Review.
Upcoming Review of the Hall D Photon Beam and Tagger Richard Jones, University of Connecticut, for the GlueX collaboration GlueX Collaboration Meeting.
F ERMILAB T EST B EAM F ACILITY Aria Soha March 17, 2011.
An accelerator beam of muon neutrinos is manufactured at the Fermi Laboratory in Illinois, USA. The neutrino beam spectrum is sampled by two detectors:
DPF Victor Pavlunin on behalf of the CLEO Collaboration DPF-2006 Results from four CLEO Y (5S) analyses:  Exclusive B s and B Reconstruction at.
Basic Measurements: What do we want to measure? Prof. Robin D. Erbacher University of California, Davis References: R. Fernow, Introduction to Experimental.
MICE: The International Muon Ionization Cooling Experiment Diagnostic Systems Tracker Cherenkov Detector Time of Flight Counters Calorimeter Terry Hart.
Study of two pion channel from photoproduction on the deuteron Lewis Graham Proposal Phys 745 Class May 6, 2009.
July 19, 2003 HEP03, Aachen P. Shanahan MINOS Collaboration 1 STATUS of the MINOS Experiment Argonne Athens Brookhaven Caltech Cambridge Campinas Dubna.
E906 Physics in 5? minutes Paul E. Reimer 8 December 2006 d-bar/u-bar in the proton Nuclear effects in the sea quark distributions High-x valence distributions.
E906 Changes Paul E. Reimer 8 December 2006 Spectrometer Location Spectrometer’s 2 nd magnet Hodoscopes –Scintillator for Station 1 and 2 –Photomultiplier.
Jornadas LIP, Dez P. Martins - CFTP-IST The NA60 Silicon Vertex Telescopes Dimuon measurements Dimuon measurements Vertex telescope used in: Vertex.
 A GEANT4-based simulation was performed of the production target, solenoid, selection channel, and spectrometer.  The acceptance was found to be 8.3x10.
NuMI NuMI Overview NBI 2002 S. Childress (FNAL) 14 March ‘02 NuMI / MINOS Overview.
E906/Drell-Yan: Monte Carlo, Data Acquisition and Data Analysis Paul E. Reimer Expected Rates and Monte Carlo (WBS 2.5.1) Data Acquisition (WBS 2.4) –CODA.
Jornadas LIP 2008 – Pedro Ramalhete. 17 m hadron absorber vertex region 8 MWPCs 4 trigger hodoscopes toroidal magnet dipole magnet hadron absorber targets.
PV-DIS Toroid Detector: outline and costs Paul E. Reimer 12 GeV PV-DIS detector meeting August 1.Introduction to Toroid Concept (presenting work.
NanoPHYS’12 – December 17-19, 2012 K. Nakano, S. Miyasaka, K. Nagai and S. Obata (Department of Physics, Tokyo Institute of Technology) Drift Chambers.
Measuring the Position Resolution of a COMPASS Drift Chamber Prototype Rojae Wright 1, Ihnjea Choi 2, Caroline Riedl 2, Matthias Grosse Perdekamp 2 (1)
CASA Collider Design Review Retreat HERA The Only Lepton-Hadron Collider Ever Been Built Worldwide Yuhong Zhang February 24, 2010.
NEUTRINO PHYSICS 1. Historical milestones 2. Neutrinos at accelerators 3. Solar and atmospheric neutrinos 4. Neutrino oscillations 5. Neutrino astronomy.
Opportunities with Drell-Yan Scattering at Fermilab Paul E. Reimer Physics Division Argonne National Laboratory 1.The Drell-Yan Process—A Laboratory for.
G-2 accelerator and cryo needs Mary Convery Muon Campus Review 1/23/13.
Hadron Spectroscopy with high momentum beam line at J-PARC K. Ozawa (KEK) Contents Charmed baryon spectroscopy New experiment at J-PARC.
F ERMILAB T EST B EAM F ACILITY Aria Soha March 22, 2011.
Improved Measurement of d/u Asymmetry in the Nucleon Sea
E906 Spectrometer Upgrade Overview Paul E. Reimer Magnet Concept Design Estimates (Money & Time)
Latifa Elouadrhiri Jefferson Lab Hall B 12 GeV Upgrade Drift Chamber Review Jefferson Lab March 6- 8, 2007 CLAS12 Drift Chambers Simulation and Event Reconstruction.
Vina Punjabi Norfolk State University Hall A Collaboration Meeting June 10-11, 2010 GEp-V Experiment to Measure G Ep /G Mp.
Lecture 9: Inelastic Scattering and Excited States 2/10/2003 Inelastic scattering refers to the process in which energy is transferred to the target,
1 Methods of Experimental Particle Physics Alexei Safonov Lecture #15.
DPF2000, 8/9-12/00 p. 1Richard E. Hughes, The Ohio State UniversityHiggs Searches in Run II at CDF Prospects for Higgs Searches at CDF in Run II DPF2000.
Dual Target Design for CLAS12 Omair Alam and Gerard Gilfoyle Department of Physics, University of Richmond Introduction One of the fundamental goals of.
Muon detection in NA60  Experiment setup and operation principle  Coping with background R.Shahoyan, IST (Lisbon)
 production in p-A and In-In collisions Motivation Apparatus Collected data Results for     Ongoing work for    KK Alessandro De Falco – University.
11 December 2006DOE Review at ANL1 Tracking Chambers for FNAL E906 Edward R. Kinney University of Colorado, Boulder, USA Overview of Tracking Plan Station.
Status of facility design Activities of the IPNS Nuclear/Particle Physics group Basic information for the working sessions Activities of Nuclear and Particle.
L/T separation in the 3 He(e,e’p) reaction at parallel kinematics Freija Descamps Supervisors: Ron Gilman Eric Voutier Co-supervisor: Jean Mougey.
Spin Physics from COMPASS G. Mallot/CERN On Behalf of the Compass Collaboration Spin 2003, Seattle 4-7 August, 2003.
Susan Burke DØ/University of Arizona DPF 2006 Measurement of the top pair production cross section at DØ using dilepton and lepton + track events Susan.
Ibrahim H. Albayrak, Hampton University Group Meeting Experiment Rosen07: Measurement of R =  L /  T on Deuterium in the Nucleon Resonance Region. 
Experiment Rosen07: Measurement of R =  L /  T on Deuterium in the Nucleon Resonance Region.  Physics  Data Analysis  Cross Section calculation 
1 Experimental Particle Physics PHYS6011 Fergus Wilson, RAL 1.Introduction & Accelerators 2.Particle Interactions and Detectors (2) 3.Collider Experiments.
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
P.F.Ermolov SVD-2 status and experimental program VHMP 16 April 2005 SVD-2 status and experimental program 1.SVD history 2.SVD-2 setup 3.Experiment characteristics.
E-906/SeaQuest: Parton Energy Loss and Antishadowing Benjamin W. Miller of Abilene Christian University For E-906/SeaQuest Abstract In addition to measuring.
Monte Carlo simulation of the particle identification (PID) system of the Muon Ionization Cooling Experiment (MICE) Mice is mainly an accelerator physics.
Vahe Mamyan, Hall-C collaboration meeting, January Data Analysis of F2 and R in Deuterium and Nuclei  Physics  Experiment Setup  HMS Detectors.
Feasibility studies for DVCS and first results on exclusive  at COMPASS DVCS studies Physics impact Experimental issues Recoil detector prototype Exclusive.
Open and Hidden Beauty Production in 920 GeV p-N interactions Presented by Mauro Villa for the Hera-B collaboration 2002/3 data taking:
Lecture 18 - Detectors Detector systems
G. Arnison et al., UA1 Collaboration
Chris Smith California Institute of Technology EPS Conference 2003
Trang Hoang Florida State University - Dzero
Precision Measurement of η Radiative Decay Width via Primakoff Effect
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 6th May 2009 Fergus Wilson, RAL.
Geant4 in HARP V.Ivanchenko For the HARP Collaboration
Experimental Particle Physics PHYS6011 Putting it all together Lecture 4 28th April 2008 Fergus Wilson. RAL.
Experimental Particle Physics PHYS6011 Joel Goldstein, RAL
What is the CNI experiment
Susan Burke, University of Arizona
Determination of the gluon polarisation
Presentation transcript:

E906 Spectrometer Upgrade Overview Paul E. Reimer Experimental Approach Impact on Fermilab Magnet Coil Fabrication Spectrometer Upgrades

2 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview x target x beam Detector acceptance chooses x target and x beam. Fixed target ) high x F = x beam – x target Valence Beam quarks at high-x. Sea Target quarks at low/intermediate-x. Drell-Yan scattering: A laboratory for sea quarks E906 Spect. Monte Carlo

3 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Physics Requirements Fundamentally want to measure and compare cross sections from a variety of targets as functions of di-muon Mass, x 1, x 2 Identify muons—hadron absorber and muon id wall Wide acceptance for desired muon kinematics Resolve kinematics: –Measure momentum of muons, reconstruct M, p L, x 1, x 2 –Depends on muon track reconstruction (through magnets) –Momentum measurement (2 nd magnet strength) Minimize background—muons from hadron decays –Absorber hadrons in dump and absorber before leptonic decay –Separate muon vertex—target vs. dump

4 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview E906 Spectrometer: Non-bend plane view Trigger electronics Scintillator Hodoscopes

5 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Detector Resolution Triggered Drell-Yan events 240 MeV Mass Res x 2 Res.

6 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Basic Approach to Measuring Drell-Yan Scattering Follow lead of pervious experiments: Proton beam on frequently interchanged targets 2 magnet spectrometer –1 st magnet focuses muons into spectrometer –2 nd magnet provides momentum measurement Beam dump within 1 st magnet –Graded hadron absorber within 1 st magnet to prevent interact hadrons before decay Target 1 st magnet 2 nd magnet Final  identification Tracking/Triggering Stations

7 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Spectrometer upgrade Smaller Boost at 120 GeV than 800 GeV –Lorentz contract detector from 60 m to 25 m E866 E906 –Requires new focusing magnet Largest (non-Fermilab) part of upgrade New Station tracking chambers for higher background rates New Hodoscopes (material aging) New trigger (rates and flexibility)

8 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview M1 Magnet New coils Reuse whole pieces of SM12 magnet yoke (SM12 was the 14.4 m dipole used by E866)

9 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview M1 Magnet Coil Fabrication Budget Cost dominated by cost of conductor and coil ($1.3M of $1.6M)

10 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Magnet Gantt Chart

11 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Spectrometer Upgrade—Increased Rates Significantly higher instantaneous luminosity in E906 (10£beam intensity) Smaller boost ) larger chance for mesons to decay before interaction in beam dump Solutions: Replace Station 1 Drift Chambers with MWPC’s (WBS 2.2.1— Colorado) More flexible trigger (still modeled after E866, but in FPGA rather than LeCroy units) (WBS 2.3—Rutgers) Double ended readout and mean timers on Station 3 and 4 hodoscopes (for single rf “bucket” resolution—19 ns) (WBS and 2.1.3—Abilene)

12 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Spectrometer Upgrades—Aging Equipment E866 Station 3 and 4 scintillator dates from E605 in 1982 E866 Station 2 scintillator from 1989 upgrade—surplus material shows significant crazing Large trigger efficiency corrections for some individual hodoscope elements observed in E866 E866 Station1 of insufficient size for E906 Solution : Replace Scintillator with newer material –Stations 1 and 2 recovered from HERMES muon hodoscope (WBS 2.1.2, Illinois) –Station 3 and 4 new material (WBS 2.1.3, Abilene)

13 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Spectrometer Elements Upgrade Budget Primarily DOE/Office of Nuclear Physics with significant funds from NSF Key NSF contribution on Trigger Key NSF contribution on Trigger

14 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Spectrometer Upgrade Gantt

15 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Spectrometer Upgrade (cont.)

16 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Contingency Overall contingency ¼20% –Very standard techniques held in common Considered based on each WBS item, but held in common –Technical—Existing design () Completely new design –Construction—Standard Techniques () New techniques/materials Relatively standard techniques for all items –Schedule—Subsystem only () Critical Path Schedule had minimal impact on contingency since delays were built into schedule. –Additional contingency from outside factors (e.g. fluctuation of base aluminum conductor price, hydrocarbon price in scintillator)

17 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Location Fermilab Original Meson East now used as Superconducting Cryo-Module Test Facility (SCMTF) Alternatives Meson West –Vertical bend spectro.—bends  + into earth. –2 nd magnet (SM3) must be assembled (but is available) NM4 (KTeV) –Beam lime below grade allows a horizontal bending spectrometer— bends  + and  - into earth –2 nd magnet (KTeV) in hall –Nicer facility for physicists Meson West NM4 (KTeV) Either location is acceptable to the collaboration Fermilab is considering the impact of the experiment at both locations In these talks, a vertical bend is assumed for historic reasons (i.e. E866/NuSea was that way)

18 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Impact of E906 on Fermilab Proton Impact: –5 s slow extraction of 2£10 12 protons/s each minute (possible scheme) delivers requested protons within 2 yrs –Approx. 10% impact on neutrino production Major Cost Drivers: –Beam Line –Cryogenics for liquid 1 H and 2 H targets –Assembly of Analysis Magnets Lesser (but still significant) Items: –Detector Gas System –Electrical and Water Utilities for Magnets –Shielding –Magnetic Field Mapping Equipment –Utilities for electronics –Area Preparation

19 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Summary of Overview Experimental approach has been proven by previous Drell-Yan experiments (E866, E789, E772). –E906 Expects higher rates, but appropriate modifications (e.g. Station 1 MWPC, double ended readout, trigger upgrade) have been made M1 Magnet is the major construction cost driver on the part of DOE/Nuclear Physics –Economical reuse of SM12 yoke –Design underway w/budgetary estimates Spectrometer upgrade requires only very conventional techniques –No technological show stoppers—uses well proven technology Requires commitment from DOE/NP, Fermilab (DOE/HEP), NSF Realistic schedule could start data collection in 2 ½ years

20 11 December 2006Paul Reimer E906 Sepctrometer Upgrade Overview Drell-Yan Acceptance Programmable trigger removes likely J/  events Transverse momentum acceptance to above 2 GeV Spectrometer could also be used for J/ ,  0 studies