RF Pick-Up Measurements in the 2004 SPS Testbeam Before installation of silicon detector assemblies in the Roman Pot: Antenna insertions for measurement.

Slides:



Advertisements
Similar presentations
Measurements of adiabatic dual rf capture in the SIS 18 O. Chorniy.
Advertisements

CLIC drive beam accelerating (DBA) structure Rolf Wegner.
Simultaneous Four-Hall Operation for 12 GeV CEBAF Reza Kazimi November 2012.
RF test of the GEM detector prototipe Detector description RF test area (LINAC3) detector working conditions RF field measurement Detector measurements.
MuCool RF Status MICE Collaboration Meeting June 7-10, 2006, Fermilab A. Moretti June 9, 2006.
DESY MHF-p 1 Layout of the Synchronisation System for the VUV-FEL Dipl. Ing. Henning Christof Weddig DESY Hamburg.
Alessandro Cappelletti for CTF3 collaboration 5 th May 2010 RESULTS OF BEAM BASED RF POWER PRODUCTION IN CTF3.
F Tevatron Software Digital Receiver Beam Line Tuner Vic Scarpine Instrumentation Instrumentation Meeting July 13, 2005.
Microwave diagnostics for electron cloud detection on the SPS F. Caspers, E. Mahner, T. Kroyer B. Henrist, J.M. Jimenez Thanks to the SPSU study team members.
Front-end amplifiers for the beam phase loops in the CERN PS Alessandro Meoli (CERN BE/RF/FB) Supervised by Heiko Damerau 21 April CERN.
Strategy for SPS 200 MHz LLRF upgrade (1)  Each of the four cavities (2x 5 sections, 2x 4 sections):  1-T Feedback (loop around cavity and amplifier)
CLIC Drive Beam Linac Rolf Wegner. Outline Introduction: CLIC Drive Beam Concept Drive Beam Modules (modulator, klystron, accelerating structure) Optimisation.
AMY Meeting. 24 Mar 2011 status Auger Lecce Meeting,
1 Electron Cloud Measurements at the Fermilab Main Injector Bob Zwaska Fermilab ECloud07 Workshop April 9, 2007.
, WP1 Meeting, RAL J. Pasternak Status and Recent Progress in the Muon FFAG Designs for the NF J. Pasternak, Imperial College, London / RAL STFC.
7.8GHz Dielectric Loaded High Power Generation And Extraction F. Gao, M. E. Conde, W. Gai, C. Jing, R. Konecny, W. Liu, J. G. Power, T. Wong and Z. Yusof.
The 2008 SPS electron cloud transmission experiment: first results F. Caspers, E. Mahner, T. Kroyer B. Henrist, J.M. Jimenez Thanks to the SPSU study team.
TE Wave Measurements Of Electron Cloud At CesrTA J. Byrd, M. Billing, S. De Santis,M. Palmer, J. Sikora ILC08 November 17 th, 2008.
F. Caspers, S. Federmann, E. Mahner SPSU meeting, 27 th October 2009.
BEPCII Transverse Feedback System Yue Junhui IHEP , Beijing Sep 17 th, 08IMAC.
Bits (0s and 1s) need to be transmitted from one host to another. Each bit is placed on the cable as an electrical signal or pulse. On copper cable the.
Construction and Installation Readiness of TOTEM Roman Pots Detectors Federico Ravotti (PH/TOT) Gennaro Ruggiero (PH/TOT) LHCC minireview – 06 May 2009.
Status of the NO ν A Near Detector Prototype Timothy Kutnink Iowa State University For the NOvA Collaboration.
BI day 2011 T Bogey CERN BE/BI. Overview to the TTpos system Proposed technical solution Performance of the system Lab test Beam test Planning for 2012.
Acknowledgements F. Caspers, H. Damerau, M. Hourican, S.Gilardoni, M. Giovannozzi, E. Métral, M. Migliorati, B. Salvant Dummy septum impedance measurements.
Mathilde FAVIER Fellow in BE/BI/QP Mathilde FAVIER BE/BI-QPSCHOTTKY STATUS - BI DAY - December 6th
IP-BPM status Siwon Jang KNU. Contents The electronics repair status –Repair work status –Electronics RF test (by using Oscilloscope) –Electronics shipment.
Preliminary Results of the Beetle Readout for the MaPMTs  Part 1: as presented on  Achievements since last LHCb week  Common Mode correction.
The 2008 SPS electron cloud transmission experiment: first results F. Caspers, E. Mahner, T.Kroyer Acknowledgements to B. Henrist, J.M. Jimenez, J.M. Laurent,
Magnet Motion Produces Luminosity Loss. NLC Feedback Operation Kicker Gain Bunch Charge Measure deflected bunches with BPM and kick other beam to eliminate.
Steve Smith - May ‘05 Estimate Beam RF Effects in ILC Detector May 4, 2005 Steve Smith SLAC.
F. Caspers, S. Federmann. Contents  Further observations and confirmation on intermodulation effects  Analysis and explanation of the gain variation.
The ISIS Dual Harmonic Upgrade The Council for the Central Laboratory of the Research Councils Andy Seville Joint Accelerator WorkshopMarch 28th, 2006.
Shashlyk FE-DAQ requirements Pavel Semenov IHEP, Protvino on behalf of the IHEP PANDA group PANDA FE-DAQ workshop, Bodenmais April 2009.
00:15: Stable beams fill 1883, 1.1E33 cm-2s-1.  Seems the 144 bunches beam 1 doe not fit properly on the injection kicker waveform. Systematically the.
BEPCII Transverse Feedback System Yue Junhui Beam Instrumentation Group IHEP , Beijing.
Schottky Summary of status and plans for YETS 15/16.
1 P.Rebecchi (CERN) “Monitoring of radiation damage of PbWO 4 crystals under strong Cs 137  irradiation in GIF-ECAL” “Advanced Technology and Particle.
BEPC II TIMING SYSTEM EPICS Seminar Presented by Ma zhenhan IHEP 20.August 2002.
Beam Test status and Plans of the ILC Main LINAC BPM
Receive Antenna Performance Comparison. Receive Antenna Monitoring The receive antenna was installed in its permanent location inside the chamber A spectrum.
RF improvements over the weekend Giulia on behalf of Delphine, Philippe, Andy and many other people in the RF team LHC Beam Commissioning Working Group,
An Inductive Pick-Up (IPU) for Beam Position and Current Measurement
Bunch Separation with RF Deflectors D. Rubin,R.Helms Cornell University.
Dec
ON/OFF news. Reflected Transmitted Stroke 8.0 mm RF power, dB Piston position (gap width), mm ON OFF Compact design of the high RF power variable (mechanically)
SPS coating studies 28 February, 2016TE-VSC1 Present situation of the development of e-cloud mitigation methods -MD 2011 results -Carbon coating of dipoles.
Pressure data from SPS MDw35 H.Neupert, M.Taborelli For SPSU, 23/09/2010.
Measurement of the neutrino velocity with the MINOS detectors and NuMI neutrino beam GdR Saclay – 11/04/08 Magali Besnier hep-ex – v3.
F. Caspers, S. Federmann, E. Mahner, B. Salvant, D. Seebacher 1.
NUMI NUMI/MINOS Status J. Musser for the MINOS Collatoration 2002 FNAL Users Meeting.
Oleksiy Kononenko CERN and JINR
 NICA is being constructed  For heavy ions we need very highluminosity level – 10 cm s  For keeping up such level we inevitably need cooling  Stochastic.
AWAKE synchronization with SPS Andy Butterworth, Thomas Bohl (BE/RF) Thanks to: Urs Wehrle (BE/RF), Ioan Kozsar, Jean-Claude Bau (BE/CO)
CLIC Workshop 2008 TBTS status. PETS testing program and installation status. Igor Syratchev & Germana Riddone for the CLIC team.
Update on the RHIC Stochastic Cooling J.M. Brennan M.M. Blaskiewicz and K. Mernick COOL Workshop 2015 Thomas Jefferson National Accelerator Facility September.
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.
LONGITUDINAL COUPLED-BUNCH OSCILLATIONS IN THE RECYCLER RING PRESENTED BY: MUHED RANA UNIVERSITY OF MARYLAND, BALTIMORE COUNTY (UMBC), BALTIMORE, MD SUPERVISOR:
CLIC Workshop 18 th -22 nd January 2016, CERN 1 Alfonso Benot Morell Manfred Wendt.
RF manipulations in SIS 18 and SIS 100 O. Chorniy.
What they are What they do How to apply
The ISIS Dual Harmonic Upgrade
A 2.3 GHz BANDWIDTH STRUCTURE FOR CLIC_DDS
Ubaldo Iriso Many thanks to:
Beam-induced EMI and detector electronics
Upcoming longitudinal MDs
Non-ideal property – crosstalk
Bunch Separation with RF Deflectors
T2K Run8 MUMON Summary.
SPS-DQW HOM Measurements
Presentation transcript:

RF Pick-Up Measurements in the 2004 SPS Testbeam Before installation of silicon detector assemblies in the Roman Pot: Antenna insertions for measurement of RF background 1 wire loop in the pot (  B-field) 1 pin in the pot (  E-field) For comparison: 1 open coax cable outside near the beam pipe 1 terminated coax cable outside near the beam pipe Read-out with spectrum analyser sometimes replaced by a 2 nd antenna insertion lying on the ground

Antenna Measurements: Examples CNGS (Gran Sasso) beam: 200 MHz bunch frequency during spill Higher harmonics visible: 400, 600, 800 MHz 80, 120, 160, 200, 240, 280, 320, 520, 680 MHz Spectra measured from 0 to 3 GHz. 25 ns beam: 40 MHz bunch frequency during spill

Spectrum Evolution during an SPS Cycle 1 st half ring filling 2 nd half ring filling, after acceleration after extraction time 200 MHz

Analysis Status Spectra give us pick-up in mW at the end of the coax cable (surface building). Problem: Where was the signal picked up? Solution: Compare with the signal induced in the cables ending blind outside the beam pipe. Different cable lengths and types  correct each spectrum for cable attenuation (data from pool catalogue).

25ns Beam: Comparison inside/outside Pot Natel = 956 MHz Typical error bar: ~ 2 dB

Loops Pins inside outside inside outside 25ns Beam: Comparison inside/outside Pot (low frequencies) No clear quantitative conclusion about inside/outside comparison. Similar situations for Gran Sasso beam and for 400 GeV beam.

A Hint at Pick-Up by VFAT ? 25ns Beam: big fraction of VFAT signals 1.6  s too late TOTEM Beam: ~ ~ ~ 0.8  s ~ ~ Cannot be: Cable length difference (Would need 400 m! In-time signals also exist.) Delay in chip or motherboard (  Walter) What is it ???

Future RF Tests in the Lab Suggestions from F. Caspers: Remount the antenna pieces on the Roman Pot, add pieces of beam pipe on both arms (planned for end of this week) Inject pulse with network analyser Generate spark with a spark pistol (or even just a bricolage solution)