Beamline improvement during g2p experiment. Pengjia Zhu

Similar documents
Instrumentation and analysis progress for g2p experiment

arxiv: v2 [physics.ins-det] 26 Jun 2016

Hall-B Beamline Commissioning Plan for CLAS12

Digital BPMs and Orbit Feedback Systems

DAQ Systems in Hall A

Beam Loss Detection for MPS at FRIB

ATF Energy Spectrometer Experiments

Update on DAQ for 12 GeV Hall C. Brad Sawatzky

Online Monitoring of L1CT in Run IIa. bonus: experience from Run I

Bunch-by-bunch feedback and LLRF at ELSA

Polarized Source Development Run Results

G0 Laser Status Parity Controls Injector Diagnostics

Update on DAQ for 12 GeV Hall C

Dark current and multipacting trajectories simulations for the RF Photo Gun at PITZ

The FLASH objective: SASE between 60 and 13 nm

Status of the Jefferson Lab Polarized Beam Physics Program and Preparations for Upcoming Parity Experiments

Non-Invasive Energy Spread Monitoring for the JLAB Experimental Program via Synchrotron Light Interferometers

LHC Beam Instrumentation Further Discussion

PHGN 480 Laser Physics Lab 4: HeNe resonator mode properties 1. Observation of higher-order modes:

BCM Calibration for E Abstract

A flexible FPGA based QDC and TDC for the HADES and the CBM calorimeters TWEPP 2016, Karlsruhe HADES CBM

An Operational Diagnostic Complement for Positrons at CEBAF/JLab

A fast and precise COME & KISS* QDC and TDC for diamond detectors and further applications

Parity Quality Beam (PQB) Study

Quad-to-quad correlated motion in FLASH

An Overview of Beam Diagnostic and Control Systems for AREAL Linac

LIGHT PROTON THERAPY PROJECT

R-1550A Tempest Wide Range Receiver

9th ESLS RF Meeting September ALBA RF System. F. Perez. RF System 1/20

PQB Meeting. Caryn Palatchi 02/15/2018

New Filling Pattern for SLS-FEMTO

Sensor Development for the imote2 Smart Sensor Platform

Chapter 6: Real-Time Image Formation

5 MeV Mott Polarization Measurement Procedure--DRAFT

HD Review March 30, 2011 Franz Klein

PEP-II longitudinal feedback and the low groupdelay. Dmitry Teytelman

CM-392-Video to HDMI Scaler Box ID#481

New gas detectors for the PRISMA spectrometer focal plane

Extraction/Separator Setup. Michael Spata Operations Stay Treat July 16, 2015

Sérgio Rodrigo Marques

HAPD and Electronics Updates

BRITE-VIEW BLS-2000 Professional Progressive Scan Video Converter

The CMS Detector Status and Prospects

Production of quasi-monochromatic MeV photon in a synchrotron radiation facility

Status of SOLARIS Arkadiusz Kisiel

Front End Electronics

Fast Orbit Feedback at the SLS. Outline

DT9857E. Key Features: Dynamic Signal Analyzer for Sound and Vibration Analysis Expandable to 64 Channels

Effects of the cryogenics operational conditions on the mechanical stability of the FLASH linac modules

Log-detector. Sweeper setup using oscilloscope as XY display

There are many ham radio related activities

Beam Position Monitor Developments at PSI

LLRF at SSRF. Yubin Zhao

The Elettra Storage Ring and Top-Up Operation

SPEAR 3: Operations Update and Impact of Top-Off Injection

Development of beam-collision feedback systems for future lepton colliders. John Adams Institute for Accelerator Science, Oxford University

First Simultaneous Top-up Operation of Three Different Rings in KEK Injector Linac

SPECIFICATION NO Model 207 Automatic GTAW Welding System

A SQUID-BASED BEAM CURRENT MONITOR FOR FAIR / CRYRING

CS2401-COMPUTER GRAPHICS QUESTION BANK

Screen investigations for low energetic electron beams at PITZ

P. Emma, et al. LCLS Operations Lectures

Photo cathode RF gun -

Summary report on synchronization, diagnostics and instrumentation

Terahertz focal plane arrays for astrophysics and remote sensing

Recent APS Storage Ring Instrumentation Developments. Glenn Decker Advanced Photon Source Beam Diagnostics March 1, 2010

Hardware Verification after Installation. D0 Run IIB L1Cal Technical Readiness Review. Presented by Dan Edmunds August 2005

Requirements for the Beam Abort Magnet and Dump

SSRF Beam Diagnostics Commissioning. LENG Yongbin on behalf of SSRF BI group

Open Rack Specification 2.1 Update

Digital Lock-In Amplifiers SR850 DSP lock-in amplifier with graphical display

Owner s Manual PRE1. v1.2. Triode Class A Line Preamplifier

Spatial Response of Photon Detectors used in the Focusing DIRC prototype

Drift Tubes as Muon Detectors for ILC

Status of the CUORE Electronics and the LHCb RICH Upgrade photodetector chain

Progress Update FDC Prototype Test Stand Development Upcoming Work

Development of an Abort Gap Monitor for High-Energy Proton Rings *

Andrei Seryi, Toshiaki Tauchi. December 15-18, 2008

LCLS RF Reference and Control R. Akre Last Update Sector 0 RF and Timing Systems

Real Time Control for KAGRA covered by EPICS

INTEGRATED ASSEMBLIES MICROWAVE SOLUTIONS FROM TELEDYNE COUGAR

with - < n < +. There are two types of approximations associated with the sampling process. finite precision of the ADC finite sampling frequency.

CSC Data Rates, Formats and Calibration Methods

ANKA Status Report. N.Smale, A.-S. Müller, E. Huttel, M.Schuh Slides courtesy of A.-S. Müller and C.Heske.

NSLS2 Diagnostic System Commissioning and Measurements

Commissioning and Initial Performance of the Belle II itop PID Subdetector

Beam Instrumentation for X-ray FELs

ILC Damping Ring Lattice Status Report. Louis Emery and Aimin Xiao Argonne National Laboratory Presented at KEK workshop Dec 18th, 2007

User manual for Bluetooth module (Model: MY-DJAP-BD)

Commissioning and Performance of the ATLAS Transition Radiation Tracker with High Energy Collisions at LHC

The PEFP 20-MeV Proton Linear Accelerator

Video to HDMI Scaler Box

Solid State Logic S O U N D V I S I O N

Engineering Specification

Types of CRT Display Devices. DVST-Direct View Storage Tube

Magnetic Sensor - Incremental EHP

TWO BUNCHES WITH NS-SEPARATION WITH LCLS*

FRONT-END AND READ-OUT ELECTRONICS FOR THE NUMEN FPD

Phase (deg) Phase (deg) Positive feedback, 317 ma. Negative feedback, 330 ma. jan2898/1638: beam pseudospectrum around 770*frev.

Libera Hadron: demonstration at SPS (CERN)

Transcription:

Beamline improvement during g2p experiment Pengjia Zhu

Review for g2p Q2 0.02 0.20 GeV2 o 6 forward angle detection

Review for g2p Polarized NH3 target 1K Refrigerator 2.5/5T Transverse target field Polarization influencing factors: Temperature Radiation damage Low Current ~ 50nA 1 inch

g2p Beamline Super Harp Tungsten Calorimeter Chicane Fast Raster NH3 Target BPM Slow Raster Septum,local dump BCM New for g2p: Slow Raster Chicane New BPM,BCM Receiver Super Harp Local Beam Dump Used before, added back: Tungsten Calorimeter Septum

Raster System + 1 inch AM 1/t 30Hz Sin 100Hz Triangle ~ 17KHz Fast Raster ~2mm Slow Raster ~2cm minimize depolarization reduce radiation damage less systematic error for target polarization measurement

Beam Position Monitor Space limit: <1m from FZ2 chicane magnet to target, Can not use cavity beam position monitor 2 M15 Antenna BPM and 1 superharp installed between target and FZ2 Cavity M15 Antenna BPM Target FZ1 Chicane Magnet FZ2 Chicane Magnet BPM harp

New BPM Receiver Y+ R = I 2+ Q 2 Q φ =tan 1 ( ) I X+ 15 M Cascaded integrator-comb filter dt Harmonic sampling Sample Rate:36MSPS Y X d dt Noise limit exclude out-of band signal Epics 1 1 sin θ sin ϕ= cos(θ ϕ) cos (θ+ ϕ) 2 2 X+ XY+ Y- LNA Multiply Mixer Filter 45MHz ADC IF Amp CIC Filter IIR Filter CORDIC Div >n DAQ 0~10V DAC 1497MHz Infinite impulse response filter BW=175Hz Local Oscillator 1452MHz Calculate R and φ Analog Part Digital Part We can not see fast raster signal Thanks John Musson,Trent Allison, Keith Cole

Harp 1H04 BPM Resolution BPMA BPMB Resolution: ~0.18mm in 50nA chicane BPM Harp BPM 1H05A 1H05A 1H05B Target BPMA is always good BPMB is worse than BPMA, more noise Using fake signal to test, the problem is not from BPM receiver Radiation damage and Magnet field(400gaus in BPMB, and 200gaus in BPMA) will affect it.

Super Harp ----------> Calibrate 2 BPMs 50um wires Works in pulser beam mode Did the harp scan in ~5uA pulser beam At the same position took run in 100~50nA CW beam Calibrate in Straight Through Configuration Harp 1H04 Slow raster shape in Calibrated BPM Signal length Wire position(mm) chicane BPM Harp BPM 1H05A 1H05A 1H05B

Super Harp problem during experiment 1H04 Noise from wire motion High wire speed 1~6mm/s Low wire speed 0.5~1 mm/s 1H05A

New BCM Receiver Signal LNA Multiply Mixer Filter 45MHz IF Amp CIC Filter ADC IIR Filter Local Oscillator 1497MHz 1452MHz Analog Part Digital Part Calibration: Low current ~50nA Faraday Cup and Unser not working Use Tungsten Calorimeter Calorimeter BCM CORDIC Div >n DAC 0~10V DAQ

Tungsten Calorimeter -------> Calibrate BCM Use Temperature To Calibrate Charge Scaler Count Charge calculated charge with scaler count, Current using 25,50,75,100nA

Chicane Magnet 2.5/5T Transverse Target Magnet Field Used for banding beam to hall A dump Or minimize out of plane angle

Local beam dump Used for dumping the unscattered beam during 5T run Works good, The radiation is not very huge.

Summary New BPM and BCM receiver for low current Added slow raster,chicane,local beam dump, super harp etc for g2p BCM and tungsten calorimeter works stable Need to fix the harp noise BPMA works good, but BPMB is more noisy

Thanks! Thanks for Alexandre's help for beamline study Thanks for John Musson,Trent Allison, Keith Cole's help for BPM and BCM receiver's maintenance,optimize Thanks for Tony,Chad's hard work for harp Thanks for Arny, Ahamad's help for tungsten calorimeter Thanks for Bob,David Abbott,Ed Jastrzembski's help for happex DAQ improvement Thanks for Toby,Chao,Min,Jie,Ryan,Mellisa's help