Beam Studies December 2014 Runs: 7820 – 7860 December 27, 2014.

Slides:



Advertisements
Similar presentations
Robert Michaels HAMC Hall A Analysis Workshop 09 C HAMC = Hall A Monte Carlo ROOT / C++ Design Somewhat like SAMC & genercone For HRS only. Uses LeRose.
Advertisements

CAVITY RING DOWN SPECTROSCOPY
Microsoft ® Word 2010 Core Skills Lesson 4: Working with Tabs Courseware #: 3240 Microsoft Office Word 2010.
Feedback on phase adjustment with BPTX Using scope and LHCb BPIM boards to readout BPTX signal BPIM only used for triggering, phase measurements (BPTX1-BC1,
CSC Timers Since this is a microcontroller it mainly finds itself in embedded devices Quite often embedded devices need to synchronize events The.
MICO Alain Blondel 17 March MICO Alain Blondel 17 March MICE target test-run March 2008 Friday 14/03/2008 6:00-> 18:00 Saturday 15/03/2008.
Linda R. Coney – 24th April 2009 MOM Update Linda R. Coney 21 September, 2009.
E166 Collaboration J.C. Sheppard SLAC, October, 2003 E166 Background Test Simulations: Overview-what do we need J. C. Sheppard.
UK 8-12 Dec 2007 Alignment and Calibrations K. Goulianos1 Alignment and Calibrations Konstantin Goulianos The Rockefeller University Forward Physics.
Linda R. Coney – 24th April 2009 MOM Update Linda R. Coney 14 September, 2009.
MICE CM Berkeley 9-12 Feb February 2005 Edda Gschwendtner 1 Control/Monitoring and DAQ for PIDs Edda Gschwendtner.
Y. Karadzhov MICE Video Conference Thu April 9 Slide 1 Absolute Time Calibration Method General description of the TOF DAQ setup For the TOF Data Acquisition.
Background Subtraction Fitting technique: Fit mass with G 1 + G 2 + a + b/x Background is G 1 + a + b/x Use 3  cut Goal: put limit on systematic error.
MOM - M.ApollonioAccel. R&D/Physics and IADR - RAL - 19/3/ Summary of MICE operations – 14/15 March 2008 AIMS - establish MICE beamline in ISIS synchrotron.
14/1/20097 January 2009MICE CM23 - Harbin - Beamline Session1 MICE Beamloss Data Adam Dobbs.
Laser Tracking System (LTS) Son Nguyen Jassim Alshamali Aja ArmstrongMatt Aamold.
Conducting a Test Beam Experiment - Page 1 To begin with, elect an experimental spokesman, who can act as a coordinator. Survey the area to understand.
Range Measurement Unit Messenger Mercury Laser Altimeter Basic Familiarization.
Mott DAQ Speed December 18, How to speedup DAQ I.Reject low-energy electrons before reaching DAQ: 1.Increase E-detector hardware threshold 2.Vetoing.
UNRELIABLE DATA, SEE FIRST SLIDE WARNING!!! Data taken on these shifts had attenuation factors set incorrectly and problems with faraday cup bunch charge.
Prototype Test of SPring-8 FADC Module Da-Shung Su Wen-Chen Chang 02/07/2002.
SODA: Synchronization Of Data Acquisition I.Konorov  Requirements  Architecture  System components  Performance  Conclusions and outlook PANDA FE-DAQ.
Diana Parno – July 22, 2008 January PREx Test Run: Compton Photon Analysis Diana Parno Carnegie Mellon University HAPPEX Collaboration Meeting.
Analogue BPM data analysis Calibration & resolution results.
#3205 Summary Studying beam instabilities along bunch train 3 observables – INJ-BPM-01 fast bunch electronics – INJ FCUP-01 – Laser pulse power. Laser.
Xiao-Yan Zhao Beam Instrumentation Group Accelerator Center, IHEP BEPCII Background Issues: Beam Loss Measurement.
Features of the new Alibava firmware: 1. Universal for laboratory use (readout of stand-alone detector via USB interface) and for the telescope readout.
Linda R. Coney – 24th September 2009 MOM Update Linda R. Coney 24 September, 2009.
A. Fabich, CERN MERIT collaboration meeting, CERN, 7-8 February 2008 MERIT beam intensities, Feb 08A. Fabich, CERN1.
3243 Fri 23 Nov Summary INJ-BPM-01: took 1 shot of data, just a reference to compare with previous recent shifts – Did not see a strong dominant 100 kHz.
TELL-1 and TDC board: present status and future plans B. Angelucci, A. Burato, S. Venditti.
IP BPM Shift Report FONT Meeting: 22 December 2014 Talitha Bromwich.
TELL1 high rate Birmingham Karim Massri University of Birmingham CEDAR WG Meeting – CERN – 26/03/2012.
DAQ Map of Electronic Components R. Suleiman February 12,
Target tests 1 st – 2 nd Nov. Chris Booth Sheffield 7 th December 2006.
VULCAN Handshake June Purpose Control system tracks – Proton charge on target – # of neutrons received by detector – # of neutrons..
K0 meeting 2007/10/17 Taito Kawasaki. ~ 10/8 (Mon) : Prepare for experiment 10/9 (Tue) : Beam on (1.0 GeV mode) | 9 days, 18 shifts | Normal run : 31.
The Q Weak Experiment Event tracking, luminosity monitors, and backgrounds John Leacock Virginia Tech on behalf of the Q Weak collaboration Hall C Users.
ILD/ECAL MEETING 2014, 東京大学, JAPAN
MICE Target Failure UKNFIC Meeting Adam Dobbs - when and why 4 th July 2008.
#3205 Summary 6 th Nov 2012 Studying beam instabilities along bunch train 3 observables – INJ-BPM-01 fast bunch electronics – INJ FCUP-01 – Laser pulse.
Status of E14 G.Y.Lim IPNS, KEK. E14 Experiment Step-by-step approach to precise measurement of Br( K L    ) KEK-PS E391a J-PARC E14 (Step-1) J-PARC.
1 Fast kicker study Machine Time 2011/10/18~10/29(2 weeks) TB meeting 2011/01/14 T.Naito.
CALO Meeting–September 2 nd 2015 Calorimeter Upgrade Electronics: June 2015 Test Beam E. Picatoste Universitat de Barcelona, Institut de Ciències del Cosmos.
#3205 Summary Studying beam instabilities along bunch train 3 observables – INJ-BPM-01 fast bunch electronics – INJ FCUP-01 – Laser pulse power. Laser.
Beam Studies December 2014 Runs: 7821, 7822, and 7860 December 29, 2014.
DAQ Speed and Run2 Estimates April 3, Summary of FADC Development for Faster Performance NameReadoutTrigger ScalersScaler S1 (helicity gated), S2.
ApEx needs for CeC PoP Experiment December 11, 2015.
1 Report on analysis of PoGO Beam Test at Spring-8 Tsunefumi Mizuno July 15, 2003 July 21, 2003 revised.
TOF Emittance Emittance measurements with the TOFs Mark Rayner 4 December 2008.
Moving Wire, Pulsed Wire and Long Coil Measurements on the SSRL Beam Line 5 EPU Scott Anderson SLAC Magnetic Measurements.
Name: Abdullah ALghamdi
OMEGA3 & COOP The New Pixel Detector of WA97
Physics Case of the Day - Sunday
AHCAL Beam Interface (BIF)
Gated Mode - System Aspects
Gated Mode - System Aspects
Iwaki System Readout Board User’s Guide
Timer Source: under
Mott DAQ Speed February 16, 2015.
MERIT beam intensities
Flip-Flop Applications
CLAS12 Timing Calibration
ECE 554 HW Tutorial Spring Good afternoon everyone.
Mott DAQ Timing R. Suleiman February 12, 2014.
Transition Radiation Studies with Xe GlueX Collaboration Meeting
The New Trigger/GPS Module for the EEE Project
Beam Halo Considerations for Back Angle Running
Thursday 22nd March 00:20 – 02:40 on longer squeeze function, orbit and chroma correction at 4 TeV 2:40 – 5:30 second cycle with long squeeze 5:46 – 7:00.
Tuesday
Presentation transcript:

Beam Studies December 2014 Runs: 7820 – 7860 December 27, 2014

Outline FADC and TDC Data Synchronization: – Mott_SemiInt Mode: good (only one run was taken – 7860) – Mott_Sample Mode: TDC data is off by one event (except first four runs: 7820, 7821, 7822, and 7823*) * After Run 7823, TDC stop signal offset (NIM740) was adjusted before going to DISC (NIM708) but nothing obvious on scope Beam Rep = 31 MHz (C Laser) Beam Rep = 62 MHz (C Laser) Beam Rep = 499 MHz (A Laser) Background 2

Mott_SemiInt – Run

Mott_Sample – Run TDC Shift =0 TDC Shift =1 TDC Shift =2 Run from May 2014

5 Extra TDC stripes because four detectors have slightly different time offsets

Mott_Sample – Run 7859 – 31 MHz 6 TDC Shift =0 TDC Shift =1 TDC Shift =2 TDC is off by one event

Run 7858 – Thru Hole 7 TDC Shift =1

Run 7824 – 62 MHz 8 TDC Shift =1

Run 7839 – 499 MHz 9 TDC Shift =1

Solution B. Moffit thinks it's possible that loss of synchronization was actually coming from fadc250, instead of TDC. With prescription that was in current readout-lists may have left data on fadc250 that was not cleared before next run. This would explain why changing configuration, or resetting and downloading again would clear it up. Added a faClear(..) into start-of-run to see if this should help. 10

Background Rep Rate = 499 MHz (A Laser) : – Runs: 7821, 7822, → yes background – Runs: , → no background Rep Rate = 62 MHz (C Laser) : – Runs: 7820, → yes background – Run: 7824* → no background * C Laser, amp=2.0W, A-slit = 60mm Rep Rate = 31 MHz (C Laser) : – Runs: 7831, 7832, 7833 → yes background – Runs: 7851, 7858, 7859 → no background 11 All runs before 7839 (except for Run 7824) have background All runs before 7839 (except for Run 7824) have background

BPM0L02 x-position 12 Before Run 7839, BPM0L02X was changed from 1.5 to -4.5 mm Before Run 7839, BPM0L02X was changed from 1.5 to -4.5 mm

Beam Current 13

Mott Events 14

Detector Events 15

E Events 16

dE Events 17

Run 7838 – 499 MHz 18 TDC Shift =1

Run 7830 – 31 MHz 19 TDC Shift =1 Background events from beam scraping apertures upstream of target

Run 7825 – 62 MHz 20 TDC Shift =1