Jixie Zhang Javier Gomez Oleksandr Glamazdin Roman Pomatsalyuk Vadym Vereshchaka Hall A Collabortion Meeting, Dec 2012 Hall A Moller Polarimeter 12 GeV.

Slides:



Advertisements
Similar presentations
Super BigBite concepts Bogdan Wojtsekhowski, JLab
Advertisements

Optics and magnetic field calculation for the Hall D Tagger Guangliang Yang Glasgow University.
G2p Hall Infrastructure Alan Gavalya May Overall g2p Target on Pivot in Hall A.
Y. R. Roblin, G2P review, 1/17/ HALLA G2P readiness review Yves Roblin, CASA.
1/22 MOLLER Juliette M. Mammei. 2/22 Working Groups Polarized Source Hydrogen Target Spectrometer Integrating Detectors Tracking Detectors Polarized Beam.
G2P Target installation and Beyond. Schedule Pivot before.
Tagger and Vacuum Chamber Design. Outline. Design considerations. Stresses and deformations. Mechanical assembly.
LINACs Michael Bevins May 17, GeV Upgrade - Beam Transport Injection, Linac, Extraction, & Correctors Preliminary Design and Safety Review.
Tagger and Vacuum Chamber Design. Outline. Design considerations. Stresses and deformations. Mechanical assembly.
Update on the Gas Ring Imaging Cherenkov (GRINCH) Detector for A 1 n using BigBite Todd Averett Department of Physics The College of William and Mary Williamsburg,
AWAKE Electron Spectrometer Design Simon Jolly 4 th September 2012.
HPS Test Run Setup Takashi Maruyama SLAC Heavy Photon Search Collaboration Meeting Thomas Jefferson National Accelerator Facility, May 26-27,
Report of the NTPC Test Experiment in 2007Sep and Others Yohei Nakatsugawa.
Improved beam line for Hall A layouts, present and proposed optics in altered region benefits of proposed layout costs of proposed layout conclusions.
New Methods for Precision M ø ller Polarimetry Dave Mack Jefferson Lab ( for Dave Gaskell ) May 20, 2006 PAVI06 Precision M ø ller polarimetry Beam kicker.
05/30/08J. Dunne -- SANE Collaboration Meeting 1 Beamline Status Upstream beamline –Chicane –SEM –Rasters –Girder Downstream beamline –Helium bag –Extension.
SHMS Optics and Background Studies Tanja Horn Hall C Summer Meeting 5 August 2008.
WBS1 SBS Basic: Magnet and Infrastructure Robin Wines 11/4/ SBS DOE Review.
Hall C Meeting SHMS Magnets and Support Structure Design and Procurement Status Paul Brindza January 26, 2009.
October 31, BDS Group1 ILC Beam Delivery System “Hybrid” Layout 2006e Release Preliminary M. Woodley.
Question and Answer 1) A weighted Monte-Carlo ray trace of particles exiting the target/magnet assembly for all primary beam energies showing: a) Where.
HPS Collaboration Meeting JLAB, May Tracker Design Status M.Oriunno, SLAC.
Orbit Control For Diamond Light Source Ian Martin Joint Accelerator Workshop Rutherford Appleton Laboratory28 th -29 th April 2004.
F Antiproton Source Apertures Steve Werkema DOE Tevatron Operations Review March 22, 2006.
LCLS-II Magnet Error Sensitivities. Sensitivities of dipole magnets, from injector output (95 MeV) to SXR undulator input (4 GeV), where each plotted.
Accelerator and NuMI Upgrades Shutdown Update Cons Gattuso July 02, 2012 July 2, 2012 Cons Gattuso1.
ILC Beam Delivery System / MDI Issues for LCC-phase (~
Beam Line Layout – Cooling Section There seems to be two options for energy measurement: at the 180 dipole and/or in a diagnostic branch at the end of.
GlueX Collaboration Meeting. Jefferson Lab. September 9 – 11, Review of Tagger System.
Overview of the GlueX Tagger and Photon Beamline..
1 G9a -FROST. 2 Experiments FROST New generation of CLAS photoproduction experiments with FROzen Spin Polarized Target (FROST) E02-112: γp→KY (K + Λ,
Lecture 9: Inelastic Scattering and Excited States 2/10/2003 Inelastic scattering refers to the process in which energy is transferred to the target,
Managed by UT-Battelle for the Department of Energy SNS Injection and Extraction Systems Issues and Solutions by M. Plum for the SNS team and our BNL collaborators.
Proton Charge Form Factor Measurement E. Cisbani INFN Rome – Sanità Group and Italian National Institute of Health 113/Oct/2011E. Cisbani / Proton FF.
UK Neutrino Factory Meeting Front End Test Stand (F.E.T.S.) Engineering Status by P. Savage 22nd April 2009.
PREX Mtg, July 2008R. Michaels, JLAB Warm Septum : Status Septum Team: Kees deJager, Paul Brindza, Javier Gomez, John Lerose, Al Gavalya, & me New Design.
Kiyoshi Kubo Electron beam in undulators of e+ source - Emittance and orbit angle with quad misalignment and corrections - Effect of beam pipe.
Hall A Installation Review John J. LeRose 2/25/2009.
Hall C - 12 GeV pCDR Max. Central Momentum 11 GeV/c 9 GeV/c Min. Scattering Angle 5.5 deg 10 deg Momentum Resolution.15% -.2% Solid Angle 2.1 msr 4.4 msr.
Forward Tagger Simulations Implementation in GEMC Moller Shield Tracking Studies R. De Vita INFN –Genova Forward Tagger Meeting, CLAS12 Workshop, June.
Moller Polarimeter Upgrading for PREx in 1)Mollar Analysis & Upgrading Works during/after 2009 PVDIS 2)Flash ADC based DAQ dead-time measurement.
Overall Layout 1 IP2 64 m LEReC-I (1.6-2MeV): Gun to dump SRF gun used as a booster cavity Booster Cavity and Gun move (next slide)
Beam collimation in the transfer line from 8 GeV linac to the Main Injector A. Drozhdin The beam transfer line from 8 GeV Linac to the Main Injector is.
Booster bpm’s Jim Crisp 3/29/06. Plate width and linearity with the response linearized along the axis 60 and 20 degree plates become nonlinear in the.
DAQ Speed and Run2 Estimates April 3, Summary of FADC Development for Faster Performance NameReadoutTrigger ScalersScaler S1 (helicity gated), S2.
Thomas Jefferson National Accelerator Facility Operated by the Southeastern Universities Research Association for the U.S. Depart. Of Energy The Department.
Tagger and Vacuum Chamber Design Jim Kellie Glasgow University.
Status of Polarimeters and Polarized Targets: what are the plans for development of polarized targets to meet the needs of the Day 1 and future experimental.
Extraction/Separator Setup Michael Spata Operations Stay Treat July 16, 2015.
ATF2 Status N.Terunuma, KEK
12-GeV Upgrade of Hall-C: Project Scope and Status
Arun Saini, N. Solyak Fermi National Accelerator Laboratory
Interaction Region and Detector
Orbit Control For Diamond Light Source
eRHIC FFAG Lattice Design
Main magnets for PERLE Test Facility
ILC BDS Emittance Diagnostics: Design and Requirements
Hall A Infrastructure and the Moller Parity Experiment “AMPEX”
Specifications for the JLEIC IR Magnets
Hall “12 GeV” May 27, 2003 NAPP 2003: J.J. LeRose.
OLYMPUS Collaboration Meeting Luminosity Monitor Calorimeter
Hall C Beamline Upgrade
Polarimeter Detectors for 12 GeV Hall C GEn measurements
MEIC Shifting Magnet Tim Michalski August 6, 2015.
IR Beam Transport Status
Feasibility of Reusing PEP-II Hardware for MEIC Electron Ring
Feasibility of Recuperation of Magnets in Decommissioned Storage Rings
Main Design Parameters RHIC Magnets for MEIC Ion Collider Ring
Alternative Ion Injector Design
Possibility of MEIC Arc Cell Using PEP-II Dipole
Presentation transcript:

Jixie Zhang Javier Gomez Oleksandr Glamazdin Roman Pomatsalyuk Vadym Vereshchaka Hall A Collabortion Meeting, Dec 2012 Hall A Moller Polarimeter 12 GeV Upgrade

Jixie ZhangHall A collaboration Meeting, Dec Hall A Moller Polarimeter for 6 GeV Side View Top View P beam = Asym x P target / AnaPower Designed to detect electrons of GeV, E’ = E beam /2

Jixie ZhangHall A collaboration Meeting, Dec Sys error ~1.7% 5 target foils of15x3 cm 2 Supermendur and iron foils, 7-30μm thick 20 deg tilted The Low Field Target

Jixie ZhangHall A collaboration Meeting, Dec The High Field Target Sys error ~0.9% 4 Tesla maximum field To use this target, we should: a. Improve the target holder for better alignment b. Build Cryogenic line to feed the magnet c. Change target foils

Jixie Zhang5Hall A collaboration Meeting, Dec 2012 Upgrade for 12 GeV Add the 4th quadruple magnet to cover electron energy range 0.8~11GeV. Need to shift Q1 and a new bench for Q1 and Q4 Add a shielding pipe into the dipole magnet to shield the beam from high dipole field Møller electrons bending angle changes from 10 ⁰ to 7.3 ⁰ in order to use the same dipole power supply Rearrange the beam line shielding downstream of the dipole for 7.3 ⁰ angle Lift up the detector shielding box by 10cm to match 7.3 o Need a new detector shielding house (can not cut from the old one) New correctors and new BPM downstream of the Møller dipole

Changes to the Quadrupole Magnets Quad #1 is moved 40 cm downstream New quad #4 New girder for Q1 & Q4 Jixie Zhang6Hall A collaboration Meeting, Dec 2012 beam

Jixie ZhangHall A collaboration Meeting, Dec The new quadrupole magnet (Q4) has already been designed and manufactured New bench for Q1 qnd Q4 has also been designed and manufactured The magnetic field of Q4 was mapped by magnetic group in the summer of 2012 Q4 and the bench has already been installed in the beam line Status of the New Quadrupole Magnet (Q4)

Beam line Shielding pipe inserted into dipole magnet to increase to the field attenuation. Rearrange for 7.3 degrees Overall length of the pipe is cm. Maximum beam shift in vertical is less than 2 mm at the pivot or 9 mm at the beam dump with 11 GeV beam. Changes to the Dipole Magnet Jixie Zhang8Hall A collaboration Meeting, Dec 2012

Top of outer box extended to safely contain lead shielding bricks. Clearance in doors for upside down girder components. Detector shielding box lifted 7 cm above 6 GeV position. (Designed to be lifted by 10 cm if needed.) Changes to the Detector Shielding Box Jixie Zhang9Hall A collaboration Meeting, Dec 2012

Added a sheet metal enclosure around the opening of the box. Changed the mounting angle of the detector package from 10 deg to 7.3 deg. Internal Changes to the Detector Shielding Box Jixie Zhang10Hall A collaboration Meeting, Dec 2012

Removed one quad Move the remaining quad to a central location Added vertical corrector magnet Added a BPM Changes to the Upside Down Girder Jixie Zhang11Hall A collaboration Meeting, Dec 2012

Jixie ZhangHall A collaboration Meeting, Dec Discrepancy is about %, using scaler triggers. Comparison between old and FADC DAQs Old DAQ FADC DAQ

Jixie ZhangHall A collaboration Meeting, Dec Systematic Errors for Current System

1)Increase detector bandwidth up to 200MHz Programmable Logical Unit(PLU) module LeCroy-2365, bandwidth <75 MHz, CAMAC (out of market now)  replaced by PLU module based on CAEN V1495 board (bandwidth 200MHz, VME, FPGA) Discriminator Ortec-TD8000, input rate <150 MHz, CAMAC  replaced by P/S 706 (300 MHz, NIM), modified for remote threshold setup with DAC type of VMIC4140 2)Reduce readout time from ADC and TDC modules ADC LeCroy 2249A, 12 channels, CAMAC  replaced by QDC CAEN V792 (32 channels, VME) TDC LeCroy 2229, CAMAC  replaced by TDC V1190B (64 channels, 0.1ns, VME)  We also consider to implement some new triggers unit (for ADC, TDC trigger and gate). Electronics Upgrade Goals Jixie Zhang14Hall A collaboration Meeting, Dec 2012

1. Some electronic modules have been installed to VME and NIM crates for testing. 2. Firmware for PLU module is under developing and testing. 3. Software: Library to control DAC for remote threshold setup is ready. Library for configuring and controlling of PLU module is ready ( Logical Unit and Scalers). Readout list for TDC and PLU Scalers is ready. Coda for testing TDC and PLU modules is running. ToDo List. Code to analyzing Data Trigger of FADC DAQ PLU Firmware optimization Continue testing of PLU+TDC+QDC with CODA and Analyzer (modify from old DAQ). Migrate both old DAQ and FADC DAQ to CODA 3 ( configuration files, mSQL DB, CRL code) Electronics Upgrades Status Jixie Zhang15Hall A collaboration Meeting, Dec 2012

Jixie ZhangHall A collaboration Meeting, Dec Current Moller polarimeter working very well. Discrepancy between old and FADC DAQ is %. The systematic uncertianty of moller measurement with low field target is ~1.7% and 0.9% for high field target. Engineerging designs has been finished. New Q4 has been mapped. Q4, Q1 and their new bench have been installed. Changes to the Dipole, the detector house and the upside down girder have been done in the hall. Electronics module test is in progress. Software upgrade is going well. Summary

Jixie ZhangHall A collaboration Meeting, Dec Back Up

Jixie ZhangHall A collaboration Meeting, Dec TOSCA calculations for the electron beam shift after the Møller dipole with shielding insertion and additional shielding pipe Vertical Beam Position Shifted Due to the Moller Dipole Magnet