APS April Meeting 20011 Detector Construction of the Forward Proton Detector at D0 Michael Strang University of Texas at Arlington Diffractive Events FPD.

Slides:



Advertisements
Similar presentations
MICE Collaboration MTG IIT – Feb 2002 The Fiber Tracker Option for MICE Spectrometers The D0 Central Fiber Tracker – Experience and Implications for MICE.
Advertisements

Quartz Plate Calorimeter Prototype Ugur Akgun The University of Iowa APS April 2006 Meeting Dallas, Texas.
Status of the MICE SciFi Simulation Edward McKigney Imperial College London.
Abstract At the Thomas Jefferson National Accelerator Facility in Newport News, Virginia, a team of nuclear physicists has come up with a way to probe.
Super-B Factory Workshop April 20-23, 2005 Super-B IR design M. Sullivan 1 Status on an IR Design for a Super-B Factory M. Sullivan for the Super-B Factory.
Beam Position Monitors MICE CM Harbin January, 2009.
MICE Video MTG 9/25/2002 MICE Fiber Tracker Design Update Requirements and Proposed Detector Implementations A. Bross Fermilab.
G.Barber Tracker Update, Berkeley 10 Feb Tracker Progress Contents:- Station Space Frame Patch Panel / Vacuum Seal Light Guide Map Position of Degrader/Support.
Photon Tagging in the Hall D Beamline James McIntyre University of Connecticut 13 May GlueX Graduate Student Workshop Newport News, VA.
Clear Fiber and Wave Guide Fab. Makoto YOSHIDA (Osaka Univ.) July MICE FT
The Tagger Microscope Richard Jones, University of Connecticut Hall D Tagger - Photon Beamline ReviewJan , 2005, Newport News presented by GlueX.
June 2003 M.Mulders - Fermilab 1 Diffractive results from DØ and prospects for Run II Martijn Mulders Fermilab for the DØ collaboration (with special thanks.
M.Gallinaro, ``Innovative Particle and Radiation Detectors’’, Siena, October slide 1 The CDF MiniPlug Calorimeter Forward Physics Conceptual.
Forward Detectors and Measurement of Proton-Antiproton Collision Rates by Zachary Einzig, Mentor Michele Gallinaro INTRODUCTION THE DETECTORS EXPERIMENTAL.
Elastic Scattering at s=1.96 TeV Using the DØ Forward Proton Detector
Proton Form Factor ratio GEp/GMp with polarization method --on behalf of Jefferson lab GEp3 collaboration Wei Luo Lanzhou University, China April
TOF for ATLAS Forward Proton Upgrade AFP concept: adds new ATLAS sub-detectors at 220 and 420 m upstream and downstream of central detector to precisely.
U.T. Arlington High Energy Physics Research Summary of Activities August 1, 2001.
High Energy Physics at UTA UTA faculty Andrew Brandt, Kaushik De, Andrew White, Jae Yu along with many post-docs, graduate and undergraduate students investigate.
FPD Status and Data Quality Andrew Brandt UTA Q4 D S Q3S A1A2 P 1 UP p p Z(m) D1 Detector Bellows Roman Pot P 2 OUT Q2 P 1 DN P 2 IN D2.
Jorge Barreto Low_x Prague1 Status of Diffractive Physics at DØ Run II Jorge Barreto Instituto de Física - UFRJ Rio de Janeiro – RJ - Brazil Outline.
Status of the NO ν A Near Detector Prototype Timothy Kutnink Iowa State University For the NOvA Collaboration.
THE FORWARD PROTON DETECTOR AT DZERO Gilvan Alves Lafex/CBPF 1) MOTIVATION 2) DETECTOR OPTIONS 3) FPD R&D 4) OUTLOOK Lishep 98 Lafex/CBPF Feb 17, 1998.
FPD FPD STATUS JORGE MOLINA CBPF February FPD  10 detector cartridges have been installed: 8 in the vertical plane, 2 at Dipole locations  We.
ATLAS Forward Detector Trigger ATLAS is presently planning to install forward detectors (Roman Pot system) in the LHC tunnel with prime goal to measure.
Forward Proton Detector Update  9 momentum spectrometers comprised of 18 Roman Pots  Scintillating fiber detectors can be brought close (~6 mm) to the.
ECAL LED monitoring system upgrade Pavel Shatalov ITEP, Moscow, Russia Yuri Guz IHEP Protvino, Russia.
Lishep06 Gilvan Alves1 Overview of Diffraction from DØ Gilvan Alves Lafex/Brazil  Introduction  DØ RunI x RunII  Special Runs  Outlook.
1 PID & FPD Software Gilvan Alves (Lafex/CBPF) Q4Q4 D S Q2Q2 Q2Q2 Q3Q3 Q3Q3 Q4Q4 S A 1Q A1SA1S A 2Q A 2S P 1Q P 2S P 1S P 2Q p p Z(m) A D1 Detector Roman.
Elastic Scattering and Diffraction at DØ Tamsin Edwards for the DØ collaboration 14 th - 18 th April, 2004 XII International Workshop on Deep Inelastic.
Small_X / 09/17 – 09/20Jorge Barreto – UFRJ The D0 Forward Proton Detector (FPD) Status Jorge Barreto IF – UFRJ/CBPF D1 TDC D2 TDC pbar p.
Forward Muon Installation and Commissioning Dmitri Denisov Fermilab Director’s review 7/12/1999 Plan Forward muon detectors Mini-drift tubes installation.
BES-III Workshop Oct.2001,Beijing The BESIII Luminosity Monitor High Energy Physics Group Dept. of Modern Physics,USTC P.O.Box 4 Hefei,
Small_X / 09/17 – 09/20Jorge Barreto – UFRJ The D0 Forward Proton Detector (FPD) Status Jorge Barreto UFRJ/CBPF - Brazil D1 TDC D2 TDC pbar p.
DØ Forward Proton Detector Andrew Brandt UTA Q4 D S Q3S A1A2 P 1 UP p p Z(m) D1 Detector Bellows Roman Pot P 2 OUT Q2 P 1 DN P 2 IN D2.
Time of Flight Detectors at RHIC Time of Flight Measurements at RHIC  TOF detector as a PID devices  PHENIX-TOF and BRAHMS-TOF PHENIX Time-of-Flight.
Why study Diffractive W Boson?. Data Samples Z boson sample: Start with Run1b Z ee candidate sample Central and forward electron W boson sample: Start.
G.Barber/Peter Cooke: Mechanical Design Update Imperial 22 July Mechanical Update for Tracker workshop Contents:- New Station Layout Light Guide.
Magnetized hadronic calorimeter and muon veto for the K +   +  experiment L. DiLella, May 25, 2004 Purpose:  Provide pion – muon separation (muon veto)
Andrew Brandt FPD Rio Workshop Mar Forward Proton Detector Overview Andrew Brandt University of Texas at Arlington.
DIS 2001 Bologna Hard Diffraction at DØ Run I and Run II Christophe Royon DØ Collaboration / DAPNIA-SPP Saclay, UT Arlington, Brookhaven.
Michael Strang Physics 5391, 22/July/02 Diffraction and the Forward Proton Detector at DØ Michael Strang Physics 5391.
UPDATE ON THE FORWARD PROTON DETECTOR Gilvan Alves Lafex/CBPF Introduction Accelerator Roman Pots Detector Future Plans April 1, 1998 (no kidding)
FPD Status and Plans Andrew Brandt UTA Q4 D S Q3S A1A2 P 1 UP p p Z(m) D1 Detector Bellows Roman Pot P 2 OUT Q2 P 1 DN P 2 IN D2 Q4Q3Q2.
FPD STATUS Carlos Avila Uniandes/UTA 1. FPD overview 2. Roman pot and detector status 3. FPD readout integration status 4. Software status 5. Stand-alone.
J-PARC でのハイパー核ガンマ線分光実験用 散乱粒子磁気スペクトロメータ検出器の準備 状況 東北大理, 岐阜大教 A, KEK B 白鳥昂太郎, 田村裕和, 鵜養美冬 A, 石元茂 B, 大谷友和, 小池武志, 佐藤美沙子, 千賀信幸, 細見健二, 馬越, 三輪浩司, 山本剛史, 他 Hyperball-J.
SEQUENCER DELAY PLD By ANTON H.C. SMITH ELECTRICAL ENGINEERING UNIVERSITY OF SOUTH CAROLINA.
T. Matsushita 1 Scintillating fibre tracker The scintillating fibre tracker reconstructs muon tracks before and after the MICE cooling section in 4 T magnetic.
FPD Status and Data Quality Andrew Brandt UTA Q4 D S Q3S A1A2 P 1 UP p p Z(m) D1 Detector Bellows Roman Pot P 2 OUT Q2 P 1 DN P 2 IN D2.
Convergence in Proton Reconstruction Algorithm and final reference tests of Roman pots before installation in LHC Ayah Massoud Penn State University Supervisor:
Diffraction at DØ Andrew Brandt University of Texas at Arlington E   Run IRun II Low-x Workshop June 6, 2003 Nafplion, Greece.
DØ Beauty Physics in Run II Rick Jesik Imperial College BEACH 2002 V International Conference on Hyperons, Charm and Beauty Hadrons Vancouver, BC, June.
SL/BI 16/05/1999DIPAC’99 -- JJ Gras -- CERN SL/BI -- Adaptive Optics for the LEP 2 SR Monitors G. Burtin, R.J. Colchester, G. Ferioli, J.J. Gras, R. Jung,
Roman Pots and Microstations based on talk by Jaak Lippmaa Helsinki CERN 2005.
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.
MINER A at the Triple Point: Three Phases at once Deborah Harris AEM August 31, 2009.
FTOF Status Anton A. Izotov, Frascati
FORWARD ATLAS {major contributions from Per Grafstrom (CERN), Michael Rijssenbeek (Stonybrook), Brian Cox (Manchester} Andrew Brandt Luminosity measurement.
Open and Hidden Beauty Production in 920 GeV p-N interactions Presented by Mauro Villa for the Hera-B collaboration 2002/3 data taking:
An FPD quadrupole castle Elastic Scattering and High Mass Exclusive Dijets at DØ (  s=1.96 TeV) Andrew Brandt University of Texas, Arlington on behalf.
The Ring Imaging Cherenkov Detectors for LHCb Antonis Papanestis CCLRC – RAL On behalf of the LHCb RICH group.
DØ Hard Diffraction in Run I and Prospects for Run II Andrew Brandt DØ / University of Texas, Arlington Intro and Run I Hard Diffraction Results Forward.
y x Vincenzo Monaco, University of Torino HERA-LHC workshop 18/1/2005
Andrew Brandt University of Texas at Arlington
First data from TOTEM experiment at LHC
Results of dN/dt Elastic
FPD Status and Data Quality Andrew Brandt
The E835 SCI-FI Detector In Ferrara It has been built a scintillating fibers detector for the tracking system of exp. E835 (Charmonium spectroscopy) a.
FPD Motivation Andrew Brandt UTA
The D0 Forward Proton Detector (FPD) Status
Presentation transcript:

APS April Meeting Detector Construction of the Forward Proton Detector at D0 Michael Strang University of Texas at Arlington Diffractive Events FPD Layout Detector Construction Status

APS April Meeting Diffractive Event Topologies Cross section for elastic scattering can be written as: This has the same form as light diffracting from a small disk

APS April Meeting FPD Layout Series of 18 Roman Pots forms 9 independent momentum spectrometers allowing measurement of proton momentum and angle. 1 Dipole Spectrometer ( p )  min 8 Quadrupole Spectrometers (p or p, up or down, left or right) t > t min Q4Q4 D S Q2Q2 Q2Q2 Q3Q3 Q3Q3 Q4Q4 S A 1Q A1SA1S A 2Q A 2S P 1Q P 2S P 1S P 2Q p p Z(m) A D2 A D1 Detector Bellows Roman Pot p Beam pFpF P

APS April Meeting Detector Needs Position resolution of 100µm –Beam dispersion and uncertainty in beam position make better resolution unnecessary Efficiency close to 100% Modest Radiation Hardness -Operates at 8  from beam axis, 0.03 MRad yearly dose expected High Rate capability -Active at every beam crossing Low background rate -Insensitive to particles showering along beam pipe Small dead area close to the beam -Protons are scattered at very low angles, acceptance is very dependent on position relative to beam Scintillating Fiber detector meets these needs

APS April Meeting Detector Setup 4 fiber bundle fits well the pixel size of H Ch. MAPMT 7 PMT’s/detector mm active area U U’ Six planes (u,u’,x,x’,v,v’) of 800  m scintillating fibers (’) planes offset by 2/3 fiber 20 channels/plane(U,V)(’) 16 channels/plane(X,X’) 112 channels/detector 18 detectors 2016 total channels 4 fibers/channel 8064 fibers  m LMB fiber/channel 8 LMB fibers / bundle 252 LMB bundles 80  m theoretical resolution

APS April Meeting Detector Components Fibers Scintillating fiber is spliced to clear fiber - Increased halo background with scintillating only - Light output improved due to longer attenuation length of clear fiber - Cross talk is reduced Fibers produced by Bicron mm square multiclad fiber emitting in blue Square fiber can only be polished using ice polishing method at FermiLab Lab 7 After polishing fibers are inspected for deformity and cladding damage and repolished if needed Scint Fibers 800  m Clear fiber Mirrored side 4fibers  PMT

APS April Meeting Detector Components (II) Frames Cast at FermiLab Lab 5 plastics shop Original aluminum machined piece is molded and production pieces are cast in polyurethane

APS April Meeting Splicing Splicing being completed at UTA Fibers spliced using a version of the MSU splicing machine modified for square fibers With proper setup, light transmission through splice point of over 90% possible Afterwards, splice point is sensitive to bending stresses so care must be taken - Shrink tubing cannot be used to strengthen splice due to space constraints

APS April Meeting Construction Being completed at UTA Four fibers are aligned together in the frame to make a channel X frame also includes trigger scintillating rod Bicron optical epoxy is used to secure the fibers into the frame once completely assembled After curing, channels are mapped to appropriate location in cookie, PMT calibration fibers are included, lengths are measured and final gluing with optical epoxy is done

APS April Meeting Hit Reconstruction This event (from Engineering Run data) represents a hit in our detector at the location: x d = 5.6 ± 0.4 mm y d = 3.8 ± 0.4 mm

APS April Meeting Status All fibers and frames have been delivered Currently have 7 complete detectors –Working on 8th –Expect to complete 10 by mid-May 10 detectors will be installed this Summer