Coupling Beam Transfer Function (BTF) Measurement Y. Luo, M. Minty - PowerPoint PPT Presentation

Dec 22, 2022 •41 likes •91 views

Coupling Beam Transfer Function (BTF) Measurement Y. Luo, M. Minty March 28, 2018 APEX session General Beam condition: ~ 1 hour at store with Ru+, 12*12 bunched, re-bucketed, Blue ring Procedure: set up experiment condition

Coupling Beam Transfer Function (BTF) Measurement Y. Luo, M. Minty March 28, 2018 APEX session
General ● Beam condition: ~ 1 hour at store with Ru+, 12*12 bunched, re-bucketed, Blue ring ● Procedure: → set up experiment condition → scan blue skewQ F2, F13 in steps measure eignmode projections, BTF Note: no time to fine tune the operational coupling angles
Examples Eigenmode projections WCM monitor BTF with coupling
Preliminary data processing Setting r1 r2 F2: +0.1 1.0 0.6 F2: +0.2 1.25 0.3 F2: +0.3 1.4 0.4 F13: +0.1 0.8 0.3 F13: +0.2 1.4 0.5 F13: +0.3 1.6 0.6 Note: simulations to be done to compare these measurements.
Summary ● Taken a full set of data with different skewQ settings as planned. ● Will do BTF simulations to compare the results. ● If time allows in future, would like to repeat without re-bucked beam: 1) Why there are side peaks on both sides of main peak? Is it related to re-bucketed or not? 2) How rebucketed beam affect BTF measurment

Download Presentation

Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend

Coupling Beam Transfer Function Measurement Yun, Al, Henry 2018 May 09, APEX Session General

Coupling Beam Transfer Function Measurement Yun, Al, Henry 2018 May 09, APEX Session General We had 2 hours as planned. Ramped up 12*12 Ru+ ion bunches. Fill 21660. Experiment done at store stone of energy ramp. Scan family 2s

176 views • 5 slides

Measure Twiss and Coupling at IP IP Q 1 Q 2 Q 2 Q 1 IP T B T R T E Beam Figure 1: Schematic

Measure Twiss and Coupling at IP IP Q 1 Q 2 Q 2 Q 1 IP T B T R T E Beam Figure 1: Schematic of the synchrotron from an IP through two of the triplet quadrupoles and back to the IP. Thus the beam transfer matrix is: T = T E T R T B . T = T E T

577 views • 8 slides

Coupling and Optics Measurement at Store Al, Guillaume, Yun APEX Session: Feb. 25, 2015 , p-p

Coupling and Optics Measurement at Store Al, Guillaume, Yun APEX Session: Feb. 25, 2015 , p-p run General Beam Time : used 3 hours Ramps : 2 , non-collisional pattern 12*12 What had been done : measured coupling angles at store /

102 views • 8 slides

Measure Twiss and Coupling Q1 QS Rest IP Q2 Varied 6 quadrupoles for each measurement Got 21

Measure Twiss and Coupling Q1 QS Rest IP Q2 Varied 6 quadrupoles for each measurement Got 21 tune/coupling measurements Solve for 10 unknowns for the twiss and coupling matrix [ x , x , x , y , y , y , a , b ,c ,d ]

111 views • 7 slides

Coupling 3D radiative transfer models with soil vegetation transfer models for sparse vegetation

Coupling 3D radiative transfer models with soil vegetation transfer models for sparse vegetation and validating with hyperspectral remote sensing and eddy covariance flux data Hideki Kobayashi Japan Agency for Marine-Earth Science and Technology

585 views • 29 slides

Measurement of the top-Higgs Measurement of the top-Higgs Yukawa coupling in ttH(bb) events at

Measurement of the top-Higgs Measurement of the top-Higgs Yukawa coupling in ttH(bb) events at Yukawa coupling in ttH(bb) events at the LHC in the ATLAS experiment the LHC in the ATLAS experiment New trends in High Energy Physics 06/11/2014

579 views • 21 slides

Overview of Bode Plots Transfer Function Review Transfer function review x ( t ) H ( s ) y ( t

Overview of Bode Plots Transfer Function Review Transfer function review x ( t ) H ( s ) y ( t ) Piece-wise linear approximations First-order terms Recall that if H ( s ) is known and Second-order terms (complex poles & zeros) x

235 views • 19 slides

s to Z-Domain Transfer Function 1. s to Z-Domain Transfer Function 1. Discrete ZOH Signals s

s to Z-Domain Transfer Function 1. s to Z-Domain Transfer Function 1. Discrete ZOH Signals s to Z-Domain Transfer Function 1. Discrete ZOH Signals 1. Get step response of continuous transfer function y s ( t ) . s to Z-Domain

3.01k views • 178 slides

Measurement of the top Yukawa coupling near ttbar threshold Yuichiro Kiyo, KEK LCWS2010, 2010

Measurement of the top Yukawa coupling near ttbar threshold Yuichiro Kiyo, KEK LCWS2010, 2010 Mar. 29@Beijing Aim of this talk Set up a goal of theory calculations to measure top Yukawa coupling near top threshold SM case Susy

796 views • 14 slides

First Measurement of the Beam Normal Single Spin Asymmetry in

First Measurement of the Beam Normal Single Spin Asymmetry in Resonance Produc=on by Q-weak Nuruzzaman (https://userweb.jlab.org/~nur) for the Q-weak Collaboration Beam

1k views • 38 slides

Measurement of the strong coupling constant by CMS Juska Pekkanen on behalf of the CMS

QCD@LHC 2019 Measurement of the strong coupling constant by CMS Juska Pekkanen on behalf of the CMS Collaboration juska@cern.ch SUNY Buffalo July 16, 2019 The strong coupling constant S Not a constant but running wildly Leads to

401 views • 14 slides

Cone Beam CT: imaging beams have gained interest following Dose Measurement, Calculation, and

Introduction Measurement and calculation of the dose from Cone Beam CT: imaging beams have gained interest following Dose Measurement, Calculation, and development of cone beam CT systems Inclusion in the Treatment Plan Various

344 views • 8 slides

Beam Energy Measurement: SLC-style Energy Spectrometer (WISRD in extraction line) Stan

NLC - The Next Linear Collider Project Beam Energy Measurement: SLC-style Energy Spectrometer (WISRD in extraction line) Stan Hertzbach University of Massachusetts Not here... IP Beam Instrumentation Study Marc Ross, SLAC, 26 June 2002

676 views • 11 slides

Simulation of a Conjugate Heat Transfer using a preCICE Coupling Library Dehee Kim a , Jongtae

Transactions of the Korean Nuclear Society Virtual Spring Meeting July 9-10, 2020 Simulation of a Conjugate Heat Transfer using a preCICE Coupling Library Dehee Kim a , Jongtae Kim a a Korea Atomic Energy Research Institute, 111 Daedeok-daero

400 views • 4 slides

Coolant Transfer Coupling with Integrated Dynamo for Rotor with HTS Windings Swarn Kalsi 1 , R.

M2Or4A-03 [Invited] Coolant Transfer Coupling with Integrated Dynamo for Rotor with HTS Windings Swarn Kalsi 1 , R. A. Badcock 2 and K. Hamilton 2 1 Kalsi Green Power Systems, LLC, Princeton, NJ 08540 2 Robinson Research Institute, Victoria

321 views • 16 slides

In general, the lead block of the transfer function speeds up the process. A pure lead block as

Department of Chemical Engineering I.I.T. Bombay, India Lead Lag Systems If a transfer function is of the form , s 1 G ( s ) K s 1 In general, the lead block of the transfer function speeds up the process. A

602 views • 9 slides

260 Beacon Street Rear Facade Inc. #2918 Architects Landscape Architects 36 BromfieldStreet

260 Beacon 7th floor unit existing window to be replaced to match window of unit below 1.Existing Condition View of Rear Elevation 2.Existing Condition View of Rear Elevation Hresko Associates, 260 Beacon Street Rear Facade Inc. #2918

194 views • 3 slides

EDDYSTONE BEACONS: An application for Earthquake Survivors Identification By Jaylen Gregory

EDDYSTONE BEACONS: An application for Earthquake Survivors Identification By Jaylen Gregory Eddystone Beacons: Results Though we were unable to perform the experiment, we created viable webpage and server that will activate when a survivor

204 views • 8 slides

Beacon City School District Budget 2018-19 Additions to the Budget for 2018-19 Three Elementary

Beacon City School District Budget 2018-19 Additions to the Budget for 2018-19 Three Elementary Teachers for further class size reductions Two Elementary Physical Education Teachers Special Education teacher or COTA Security Major Factor that

200 views • 8 slides

I ts not the documents; its the DATA! Tom Johnson Managing Director Inst. for Analytic

I ts not the documents; its the DATA! Tom Johnson Managing Director Inst. for Analytic Journalism Santa Fe, New Mexico USA t o m @ j t j o h n s o n . c o m 1 I ts not the documents, its the DATA! Presentation at 2011 Open

572 views • 40 slides

Laser Interferometric Searches for Ultralight Dark Matter

Ando Lab Seminar July 3, 2020 Laser Interferometric Searches for Ultralight Dark Matter Yuta Michimura Department of Physics, University of Tokyo Contents Background - Dark matter models -

1.03k views • 47 slides

Progress Towards Coherent Multibeam Arrays Doug Henke NRC Herzberg Astronomy and Astrophysics,

Progress Towards Coherent Multibeam Arrays Doug Henke NRC Herzberg Astronomy and Astrophysics, Victoria, Canada August 2016 ALMA Band 3 Receiver (84116 GHz) Dual linear, 2SB Feed horn OMT (two linear polarisations) Each

613 views • 29 slides

a force of .0059 nN/volt2 per comb-finger height (ym)

A High Force Low Area MEMS Thermal Actuator Michael J. Sinclair Microsoft Research Microsoft Corporation ABSTRACT zyxwvutsrqponmlkjihgfedcbaZYXWVUTSRQPONMLKJIHGFEDCBA One Microsoft Way, Redmond, WA 98052 Phone: (425) 703-8343 Fax: (425) 936-7329

180 views • 6 slides

INVESTOR PRESENTATION August 2019 Safe Harbor Statement The statements in this presentation

INVESTOR PRESENTATION August 2019 Safe Harbor Statement The statements in this presentation that relate to future plans, market forecasts, events or performance are forward-looking statements. These statements involve risks and uncertainties,

359 views • 23 slides