Hall A BCM Infrastructure Dave Mack July 21, 2015.

Slides:



Advertisements
Similar presentations
EPOCH 1000 Series Procedure Conventional Straight Beam Calibration
Advertisements

EPOCH 1000 Series Procedure Conventional Angle Beam Calibration
Beam Monitors Info from John Musson on new cavity receivers Other monitor issues.
CAVITY LOCK ELECTRONICS Dan Sexton, Sirish Nanda, and Abdurahim Rakhman.
DAM-Île de France Département Analyse, Surveillance, Environnement 06/06/2014 DIF/DASE/B.ALCOVERRO 1 INFRASOUND SENSOR CALIBRATION DEVICE 13/11/2001 Infrasound.
Novocontrol Alpha Analyzers Fundamentals
EPOCH 1000 Series Procedure Phase Array Straight Beam Calibration
Cold Sky Calibration Aquarius: D. M. Le Vine MWR: J. C. Gallo.
Beam position monitors LCABD Plenary meeting Bristol, 24th March 2009 A. Aryshev, S. T. Boogert, G. Boorman, S. Molloy, N. Joshi JAI at Royal Holloway.
C and S band BPM system update A. Aryshev, S. T. Boogert, S. Molloy, C. Swinson 5/25/20151ATF2 Software meeting.
Isaac Vasserman Magnetic Measurements and Tuning 10/14/ I. Vasserman LCLS Magnetic Measurements and Tuning.
The concept Provide a small (2 K) difference signal to allow continuous receiver gain measurement to 1% Alternate between three loads: 300K, 400K, sky.
Beam Loss Analysis Tool for the CTF3 PETS Tank M. Velasco, T. Lefevre, R. Scheidegger, M. Wood, J. Hebden, G. Simpson Northwestern University, Evanston,
Scanning apparatus. Final tune ups Repeatability: move in a given steps and see if we can get the same amounts. Calibration: mainly to convert any given.
Fundamentals of Power Electronics 1 Chapter 19: Resonant Conversion Outline of discussion DIRECT MODELING APPROACH 1.How small-signal variations in the.
Precision Power Measurement Solutions from Bird Precision Power Measurement Solutions from Bird.
Hall A Beam Current Monitors (J.G. for Sasha, Roman and Vadym)
WP06_AntennaIF. WP06_AntennaIF 3 principal modules switch amplifier (= ATA ‘PAM’) –includes attenuators (0-60 dB), power detector, and bias tee for the.
GMPS Transductor Upgrades And Realtime B Field Measurement for Reference Magnet Kent Triplett, Xiaolong Zhang.
19 Nov 08,ILC08Cherrill Spencer Rotating Coil System Description 1 Short description of the SLAC rotating coil system used to measure the CIEMAT-made prototype.
Black Box Electronics An Introduction to Applied Electronics for Physicists 2. Analog Electronics: BJTs to opamps University of Toronto Quantum Optics.
ATF2 Q-BPM System 19 Dec Fifth ATF2 Project Meeting J. May, D. McCormick, T. Smith (SLAC) S. Boogert (RH) B. Meller (Cornell) Y. Honda (KEK)
1 Digital Voltage Transducer family DV from 1200 to 4200 V RMS DVL from 50 to 2000 V RMS.
FEL Beam Dynami cs FEL Beam Dynamics T. Limberg FEL driver linac operation with very short electron bunches.
Interferometer Control Matt Evans …talk mostly taken from…
LLRF-05 Oct.10,20051 Digital LLRF feedback control system for the J-PARC linac Shin MICHIZONO KEK, High Energy Accelerator Research Organization (JAPAN)
The Cavity Beam Position Monitor (BPM) Massimo Dal Forno Paolo Craievich, Raffaele De Monte, Thomas Borden, Andrea Borga, Mauro Predonzani, Mario Ferianis,
1 ATF2 Q BPM electronics Specification (Y. Honda, ) Design System –Hardware layout –Software –Calibration Testing Production schedule ATF2 electronics.
March 2004 Charles A. DiMarzio, Northeastern University ECEG287 Optical Detection Course Notes Part 15: Introduction to Array Detectors Profs.
Requirements concerning the interface linking the BPM to the quadrupole M. Wendt, S. Zorzetti.
Production and Installation Policy of IP-BPM ATF2 Project Meeting, 2006/12/18 Y. Honda, Y. Inoue, T. Hino, T. Nakamura.
PSD upgrade: concept and plans - Why the PSD upgrade is necessary? - Concept and status of the PSD temperature control - Concept of the PSD analog part.
ECE 4710: Lecture #37 1 Link Budget Analysis  BER baseband performance determined by signal to noise ratio ( S / N ) at input to detector (product, envelope,
Femtosecond phase measurement Alexandra Andersson CLIC Beam Instrumentation workshop.
Paolo La Penna ILIAS N5-WP1 meeting Commissioning Progress Hannover, July 2004 VIRGO commissioning progress report.
Marc Ross T9 – Snowmass 2001 Closing Plenary T9 – Diagnostics M. Ross/R. Pasquinelli Thursday, July 19 RD: 1) determine mixing between z and x/y 2) determine.
Magnetic Field Stability Measurements Joe DiMarco 23Oct07.
Contents: 1. Introduction 2. Gyroscope specifications 3. Drift rate compensation 4. Orientation error correction 5. Results 6. Gyroscope and odometers.
PSD upgrade: concept and plans - Why the PSD upgrade is necessary? - Concept of the PSD temperature stabilization and control - Upgrade of HV control system.
Eric Prebys, FNAL.  We consider motion of particles either through a linear structure or in a circular ring USPAS, Hampton, VA, Jan , 2015 Longitudinal.
Beam Position Reconstruction Pengjia Zhu 02/15/2012.
Development of a High Resolution Cavity BPM for the CLIC Main Beam
High precision phase monitoring Alexandra Andersson, CERN Jonathan Sladen, CERN This work is supported by the Commission of the European Communities under.
SiW ECAL: the status before Fermilab Marcel Reinhard LLR – Ecole Polytechnique CALICE caollaboration meeting 18/03/08, Argonne.
Instrumentation at ATF / TTF Accelerator Test Facility (KEK) Tesla Test Facility – FLASH (DESY) ESA / LCLS (SLAC) Marc Ross, SLAC.
Progress report of the tilt monitor Daisuke OKAMOTO Tohoku University.
MO/LO Performance Summary and Maintenance Plans Tomasz Plawski Jefferson Lab OPS Stay Retreat, July 15th, 2015.
R. Michaels, JLab PREX Mtg, July 2008 Recent Cavity Monitor Tests Credit: John Musson, Anna Boehle, Vince Sulkosky Good position & current for 10 nA to.
An X-band system for phase space linearisation on CLARA
Andrei Shishlo ORNL SNS Project Florence, Italy November 2015
CLIC Workshop 2016: Main Beam Cavity BPM
Studies of Padova Perugia 16 June 2009 Flavio Dal Corso INFN-Padova.
STF Wire Position Monitor
Electric Current & Electrical Energy brainpop
DC Injector and Space Charge Simulation Status
High speed LWL connections for WP02
Irradiation test of Pressure Transducers for the LHC machine
Upcoming longitudinal MDs
BEPCII RF POWER SOURCE AND INPUT COUPLER
Muhammad Amir Yousaf.
Bunch Tiltmeter Steve Smith SLAC Snowmass July 16, 2001 Update date
BESIII EMC electronics
Readout units and the calibration of loadcells.
Beam Current Monitoring with ICT and BPM Electronics
BCM test in low current for g2p
LCLS Undulator Tuning And Fiducialization
KFPA CDR R. Norrod Feb 27, 2008.
Breakout Session SC3 – Undulator
Analysis of the Phase Drift in the Main Drive Line and L2 Reference Lines along the LCLS Using MATLAB By: Guy Grubbs II.
Update on MPPC frontend electronics development at IU
Presentation transcript:

Hall A BCM Infrastructure Dave Mack July 21, 2015

2 Hallaweb.jlab.org/github/halla-osp/version/Standard-Equipment-Manual.pdf

Big Picture Two key types of non-intercepting transducers: 1. Resonant cavity monitors (pill-box, TM 010, Q value ~ 1500??) – very high S/N, but unfeasible to dead-reckon an accurate calibration with RF at 1497 MHz 2. Unser monitor (Parametric Current Transformer) – extremely stable gain, but low S/N, and offset has poor long term stability TargetFast Raster 3 The cavities and Unser are sensitive to temperature change, so are located inside an insulating box regulated at 110F. With beam threading both cavities and Unser, an absolute calibration can be transferred from the Unser to the cavities. The Unser signal is then generally ignored until the next calibration, but is available for backup.

Unser Determines absolute current for calibration of cavities The Unser gain is stable and accurate to 0.1% out of the box (4 mV/muA). We check the gain of the Unser+V/F+gated electronics chain by passing an accurate current thru a wire. The current reference is a TargetFast Raster Wire Current 4

Current Monitors The RF cavities monitors have high S/N and can be very linear, but have to be calibrated. The Unser monitor has a stable gain which can be verified with wire current calibrations, but it is noisy and the offset tends to drift. It is only used for calibration. Same beam current threads all three devices. TargetFast Raster Wire Current 5

Charge 6 We integrate the current to get charge. It is convenient to use

To Do 7 Firm up knowledge of the system: Cavity stability factors: What Q value do the cavities have? Temperature variations inside insulated box Change Unser gain to 40 mV/muA.

Upgrades for Hall A 8 UPS on Unser

Upgrades for Hall C 9 Thermal box Current source

Acknowledgements 10