F Tevatron Software Digital Receiver Beam Line Tuner Vic Scarpine Instrumentation Instrumentation Meeting July 13, 2005.

Slides:



Advertisements
Similar presentations
1 Coherent Synchro-Betatron Resonance in the FNAL Booster A. Burov, V. Lebedev HB 2008.
Advertisements

M.Gasior, CERN-AB-BIBase-Band Tune (BBQ) Measurement System 1 Base-Band Tune (BBQ) Measurement System Marek Gasior Beam Instrumentation Group, CERN.
Development of a Chromaticity measurement application using Head-Tail phase shift technique.
Low Emittance Program David Rubin Cornell Laboratory for Accelerator-Based Sciences and Education CesrTA.
ALPHA Storage Ring Indiana University Xiaoying Pang.
Paul Derwent 30 Nov 00 1 The Fermilab Accelerator Complex o Series of presentations  Overview of FNAL Accelerator Complex  Antiprotons: Stochastic Cooling.
Key Specifications for Tevatron BPM Hardware Architecture Choices Jim Steimel.
3/7/05A. Semenov Batch-by-Batch Intensity Monitor 1 Two-Channel Batch by Batch Intensity Monitor for Main Injector BBI.
Beam Instrumentation for Orbit Stability I. Pinayev.
1 Plans for KEK/ATF 1. Introduction 2. Related Instrumentations at ATF 3. Experimental Plans for Fast Kicker R&D at ATF Junji Urakawa (KEK) at ILC Damping.
Digital Signal Processing and Generation for a DC Current Transformer for Particle Accelerators Silvia Zorzetti.
INTRODUCTION  RECYCLER BPM – Original system not adequate to measure beam position precisely. It is being upgraded to meet the required physics precision.
Tevatron BPM System Upgrade Technical Update Bob Webber Run II Luminosity Upgrade Review February 2004.
S. De Santis “Measurement of the Beam Longitudinal Profile in a Storage Ring by Non-Linear Laser Mixing” - BIW 2004 May, 5th Measurement of the Beam Longitudinal.
Basic BPM Hardware Theory Jim Steimel. Wall Current Charge in a cylindrical perfectly conducting pipe produces an equal and opposite image charge at the.
Figure 2 gives an overview of the hardware components of the upgraded Main Injector BPM system. The figure shows 2 signal channels which produce one position.
Details of space charge calculations for J-PARC rings.
Beam dynamics on damping rings and beam-beam interaction Dec 포항 가속기 연구소 김 은 산.
F 19 August 2002 All Experimenters Meeting Beams Week in Review Continued to work on providing Luminosity L  N p N a /  –Stacking rate –Coalescing efficiency.
BPM Signal Processing: A Cartoon View Rob Kutschke Oct 13, 2003.
Measurement opportunities with the LHC transverse damper W. Hofle, D. Valuch.
RHIC Status: Startup Run 12 V. Schoefer RHIC Spin Collaboration Meeting 1/13/12.
Digital Phase Control System for SSRF LINAC C.X. Yin, D.K. Liu, L.Y. Yu SINAP, China
Digital Phase Control System for SSRF LINAC C.X. Yin, D.K. Liu, L.Y. Yu SINAP, China
The Main Injector Beam Position Monitor Front-End Software Luciano Piccoli, Stephen Foulkes, Margaret Votava and Charles Briegel Fermi National Accelerator.
Electron Model for a 3-10 GeV, NFFAG Proton Driver G H Rees, RAL.
Proposal for LHC Microwave Schottky Pickups Ralph J. Pasquinelli 3/9/2005.
F Beam Line Tuners Vic Scarpine Instrumentation DoE Review Oct 28-31, 2002.
Fast feedback, studies and possible collaborations Alessandro Drago INFN-LNF ILCDR07 Damping Rings R&D Meeting 5-7 March 2007.
The Quadrupole Pick-up in the CPS -intro and progress report PPC 3 Dec 1999 A. Jansson.
F Fermilab July 6, 2005Recycler Damper Stability1 Recycler Damper High Frequency Stability Jim Crisp
Beam Line BPM Filter Module Nathan Eddy May 31, 2005.
BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing.
Multibunch beam stability in damping ring (Proposal of multibunch operation week in October) K. Kubo.
Beam stability in damping ring - for stable extracted beam for ATF K. Kubo.
BIC Issues Alan Fisher PEP-II Run-4 Post-Mortem Workshop 2004 August 4–5.
Damping ring oscillation simulation R. Apsimon. Assumptions Synchrotron oscillation causes revolution period to oscillate around a nominal value. –This.
F All Experimenters' Mtg - 2 Jun 03 Weeks in Review: 05/19/03 –06/02/03 Keith Gollwitzer – FNAL Stores and Operations Summary Standard Plots.
First Collision of BEPCII C.H. Yu May 10, Methods of collision tuning Procedures and data analysis Luminosity and background Summary.
Bunch by bunch feedback systems for KEKB Makoto Tobiyama KEK Accelerator Laboratory.
R.SREEDHARAN  SOLEIL main parameters  Booster and storage ring low level RF system  New digital Booster LLRF system under development  Digital LLRF.
Updated Overview of Run II Upgrade Plan Beam Instrumentation Bob Webber Run II Luminosity Upgrade Review February 2004.
Simultaneous Position Measurements of Protons and Anti-Protons in the Tevatron R. K. Kutschke †, J. Steimel, R.Webber, S. Wolbers, Fermilab*, Batavia,
Andreas Jansson, "Quadrupole Pick-ups", LHC BI-Review, November 19-20, Quadrupole Pick-ups  What is a quadrupole pick-up?  PS pick-ups and experimental.
TeV BPM Review 12/16/2003 Summary Status, Motivation, and Directions.
 A model of beam line built with G4Beamline (scripting tool for GEANT4)  Simulated performance downstream of the AC Dipole for core of beam using  x.
By Verena Kain CERN BE-OP. In the next three lectures we will have a look at the different components of a synchrotron. Today: Controlling particle trajectories.
Specifications of Tevatron BPM Upgrade Jim Steimel.
Plan for Beam Extraction using strip-line kicker with pulse bump orbit Present extraction kicker system Strip-line kicker system for ILC Beam extraction.
9/2/2003Tev BPM requirements1 Tevatron BPM and BLM requirements Mike Martens.
9/25/2006All experimenters meetingA. Jansson 1 Tevatron Ionization Profile Monitors Andreas Jansson.
SPS 200 MHz LLRF upgrade Part 2: Implementation Philippe Baudrenghien, Grégoire Hagmann,
Robert R. Wilson Prize Talk John Peoples April APS Meeting: February 14,
U. Raich CERN Accelerator School on Digital Signal Processing Sigtuna Digital Signal processing in Beam Diagnostics Lecture 1 Ulrich Raich CERN.
12/16/03Tev BPM requirements1 Tevatron BPM requirements Mike Martens.
Tevatron Beam Position Monitor Upgrade Stephen Wolbers (for the Tevatron BPM Upgrade Project) PAC05, Knoxville, TN May 16-20, 2005.
Beam Diagnostics Seminar, Nov.05, 2009 Das Tune-Meßverfahren für das neue POSI am SIS-18 U. Rauch GSI - Strahldiagnose.
Summary of ions measurements in 2015 and priorities for 2016 studies E. Shaposhnikova 3/02/2016 Based on input from H. Bartosik, T. Bohl, B. Goddard, V.
8/10/04N. Michelotti1 Study of Main Injector BLT.
10/3/2003Andreas Jansson - Tevatron IPM review1 Tevatron IPM Proposed design.
A Survey of TBT Capabilities of the Upgraded TeV BPMs Rob Kutschke, CD/EXP Tevatron Department Meeting February 18, 2005 Beams-doc-1583-v2.
A Survey of the Capabilities of the Upgraded TeV BPMs Rob Kutschke, CD/EXP Run II Meeting March 24, 2005 Beams-doc-1752-v2.
Bunch by bunch feedback systems for KEKB Makoto Tobiyama KEK Accelerator Laboratory.
SDA- Shot Data Analysis Jean Slaughter DOE Review July 21, 2003.
Multi-bunch Feedback System Review and Challenges for 1-2GHz Japan Synchrotron Radiation Research Institute (JASRI) SPring-8 T. Nakamura CFA Beam Dynamics.
RF acceleration and transverse damper systems
Fill-pattern Control System for KEKB
Limits on damping times
LHC (SSC) Byung Yunn CASA.
Feedforward correction to injection bump error in the SPring-8
Presentation transcript:

f Tevatron Software Digital Receiver Beam Line Tuner Vic Scarpine Instrumentation Instrumentation Meeting July 13, 2005

f Instrumentation Meeting - TeV BLT2 Introduction Primary function of a Beam Line Tuner (BLT) is to measure turn-by-turn transverse beam positions for all bunches during transfers from one accelerator ring to another –Can measure betatron oscillations, fractional tune, coupling, time- of-arrival, synchrotron oscillations, emittance growth, etc Focus has been on betatron measurements for improved closing –Feed-forward correction system – correct magnets for next transfer BLT is a key component for reducing transverse emittances and increase luminosity

f July 13, 2005Instrumentation Meeting - TeV BLT3 Tevatron BLT Measure all proton and pbar transfers from Main Injector to Tevatron Requirements: 1.Measure initial injection oscillations for every proton and pbar bunch 2.Measure tunes, emittance growth, synchrotron frequency 3.Measure bunch time-of-arrival relative to RF Beam formats: –Pbar: Four 53 MHz bunches separated by 392 ns at 150 GeV –Protons: Single 53 MHz bunch at 150 GeV

f July 13, 2005Instrumentation Meeting - TeV BLT4 Basic BLT System

f July 13, 2005Instrumentation Meeting - TeV BLT5 Analog Signals - Striplines and Fanout TeV Stripline Parameters: –~ 30 dB directionality –1 meter long (< 1/4 ) –D = 83 mm –0.65 dB/mm Sensitivity –Located at near F0 Optimally separated proton and pbars Fanout Box –M/A-Com H-9 Junction Hybrid generates A+B and A-B

f July 13, 2005Instrumentation Meeting - TeV BLT6 Tevatron Scope BLT Use Tektronix TDS7104 as fast waveform digitizer –2.5 GSample/sec/channel –Segmented memory –Embedded PC/Windows Samples pbar bunches each transfer Signal processing analysis of waveform in Scope PC Decimate data to single position per bunch –Pbars – 64 turns –Too slow for protons Only used for closing pbars

f July 13, 2005Instrumentation Meeting - TeV BLT7 Tevatron Software Digital Receiver BLT Software Digital Receiver system for pbars (similar for protons) 30 MHz LP to ring single 53 MHz bunch Digitize bunches at 2*RF Transfer digital data to PC Down convert at 30 MHz Correlate with window function –Correlation max gives A and B Generate position and time-of- arrival for ~ 1000 turns

f July 13, 2005Instrumentation Meeting - TeV BLT8 Tev BLT Trigger UCD VXI trigger module –Use TCLK and BSCLK to trigger pattern generator turn-by-turn at injection –Use pattern generator to gate Struck digitizing card for injected proton or pbar bunches

f July 13, 2005Instrumentation Meeting - TeV BLT9 Tev BLT Digitizer Struck SIS3300 Digitizing card –8 ADC channels per board –12 bit ADCs –Digitizing clock at 106 MHz (2*RF) –128K samples per channel –128 sample per turn for 1024 turns 4 x 32 sample per pbar bunch (~ 320 ns window for each pbar bunch) 30 MHz signal damps out in ~150 ns

f July 13, 2005Instrumentation Meeting - TeV BLT10 Analog Signals 53 MHz signal too short for 106 MHz digitizer Stretch signal using 30 MHz low-pass filter

f July 13, 2005Instrumentation Meeting - TeV BLT11 Down Conversion Down convert digitized signal

f July 13, 2005Instrumentation Meeting - TeV BLT12 Windows for Convolution

f July 13, 2005Instrumentation Meeting - TeV BLT13 Convolution Use peak of each convolution bump for A and B values

f July 13, 2005Instrumentation Meeting - TeV BLT14 Store 4175 Proton Vertical Oscillations

f July 13, 2005Instrumentation Meeting - TeV BLT15 Store 4175 Proton Horizontal Oscillations

f July 13, 2005Instrumentation Meeting - TeV BLT16 Store 4175 Injections Oscillations

f July 13, 2005Instrumentation Meeting - TeV BLT17 Store 4210 Pbar Injections Why is 4 th bunch different closed orbit than first three bunches? (Of course it can’t be!)

f July 13, 2005Instrumentation Meeting - TeV BLT18 Proton Contamination on Pbars Two effects: 1.Proton reflection 600 ns later falls on pbar bunch (except for last pbar) 2.Proton signal generates some sort of structured reflection in pbar signal Fix: Add 10 db attenuators at stripline on proton signal cables

f July 13, 2005Instrumentation Meeting - TeV BLT19 Pbar Oscillations after Attenuators

f July 13, 2005Instrumentation Meeting - TeV BLT20 Pbar Fractional Tunes

f July 13, 2005Instrumentation Meeting - TeV BLT21 Pbar Time of Arrival Relative to RF Use real and imaginary portions of convolution to determine phase of bunch relative to RF T = 1/(2  f)*atan(Imag/Real)

f July 13, 2005Instrumentation Meeting - TeV BLT22 Summary Tevatron software Digital Receiver BLT measuring turn- by-turn transverse positions for all proton and pbar bunches for each shot for 1000 turns –Position information being used for emittance growth estimates BLT also determining bunch time-of-arrival relative to RF Presently system only used for time-of-arrival information Want to use system to close on protons (and possible close on pbars)

f July 13, 2005Instrumentation Meeting - TeV BLT23