First analysis results of EXT MW0-4 X,Y,- 10,-10 wire-size measurements to reconstruct the 4D betatron phase-space.

Slides:



Advertisements
Similar presentations
Linear Inverse Problems
Advertisements

Emittance Reconstruction from measured Beam Sizes A.Faus-Golfe and Jesus Navarro Faus IFIC Valencia.
A circle is tangent to the x-axis at (-2, 0) and the y-axis at (0, 2). What is the equation of this circle?
Sha Bai, Philip Bambade, Glen White FJPPL – FKPPL ATF2 workshop LAL, 11~13 February, 2013 Orthogonality of beam waist corrections in the presence of IPBSM.
Denavit-Hartenberg Convention
Coupling Correction in ATF2 EXT 7 th ATF2 Project Meeting, december 2008 C.Rimbault, LAL Orsay.
EXT Beam Measurements & Corrections Dispersion, Coupling, Beta Matching 10th ATF2 Project Meeting, June M. Woodley1/31.
Emittance Measurement Simulations in the ATF Extraction Line Anthony Scarfe The Cockcroft Institute.
ATF2 FB/FF layout Javier Resta Lopez (JAI, Oxford University) for the FONT project group FONT meeting January 11, 2007.
Tracking using the Kalman Filter. Point Tracking Estimate the location of a given point along a sequence of images. (x 0,y 0 ) (x n,y n )
Wilson Lab Tour Guide Orientation 11 December 2006 CLASSE 1 Focusing and Bending Wilson Lab Tour Guide Orientation M. Forster Mike Forster 11 December.
Status Report: Emittance and IP Sizes from Synchrotron Light Alan Fisher
Mon 03 July 06Laserwire Mini-Workshop1 Using Laserwires to Measure Emittance at the ILC Leo Jenner, Daresbury Labs.
Optics for Skew Correction and Emittance Measurement Leo Jenner This talk is going to look familiar if you were at the recent LC-ABD meeting in Manchester…
Screw Rotation and Other Rotational Forms
1 Topic The Substitution Method. 2 Topic The Substitution Method California Standard: 9.0 Students solve a system of two linear equations.
2IV60 Computer Graphics Basic Math for CG
Eigenvectors and Eigenvalues
Status of very high priority beam tuning software Special ATF2 project meeting, Korea, 1 st October 2008 Cécile Rimbault, on behalf of High Priority task.
Basic Mathematics for Accelerators
ATF2 Javier Resta Lopez (JAI, Oxford University) for the FONT project group 5th ATF2 project meeting, KEK December 19-21, 2007.
Relative Error on Parameter Pessimistic Estimate Optimistic Estimate β function at the LW 3% 1% LW readout error 2% 1% Laser spot waist 10% Laser Pointing.
ATF2 optics … 1 3 rd Mini-Workshop on Nano Project at ATF ATF2 optics, tuning method and tolerances of initial alignment, magnets, power supplies etc.
FFS Issues in the 2011 autumn continuous operation Toshiyuki OKUGI (KEK) 1/13/2011 The 11 th ATF2 project meeting SLAC, USA.
6. betatron coupling sources: skew quadrupoles, solenoid fields concerns: reduction in dynamic (& effective physical) aperture; increase of intrinsic &
Fifth ATF2 Project Meeting, dec. 2007, KEK, Japan Emittance measurements with multiple wire-scanners and quadrupole scans in ATF EXT C. Rimbault,
Geometric Camera Models
1 IR with elliptical compensated solenoids in FCC-ee S. Sinyatkin Budker Institute of Nuclear Physics 13 July 2015, CERN.
Computer Graphics 2D Transformations. 2 of 74 Contents In today’s lecture we’ll cover the following: –Why transformations –Transformations Translation.
ATF1/2 laser-wires Stewart T. Boogert on behalf of UK Extraction line laserwire collaboration A. Aryshev, G. Blair, S. Boogert, A. Bosco, L. Corner, L.
Summary of Commissioning and Tuning session Philip Bambade LAL-Orsay 5 th ATF2 project meeting KEK, 21 December 2007.
Wire scanner controls at SLAC. Subgroup for one emittance measurement station Wire to select Scan range Park position Selection x,y,u Single scan Start.
Vectors (9) Lines in 3D Lines in 3D Angle between skew lines Angle between skew lines.
Mark Woodley, SLACATF2 Project March 20-21, Summary of Tuning, Corrections, and Commissioning.
27 MAY 2008NANOBEAM A laser-wire scanner for the ATF extraction line Alexander Aryshev, Stewart Boogert, Grahame Blair, Gary Boorman a Lawrence.
EXAMPLE 2 Write an equation given a vertex and a co-vertex Write an equation of the ellipse that has a vertex at (0, 4), a co-vertex at (– 3, 0), and center.
Low emittance tuning in ATF Damping Ring - Experience and plan Sendai GDE Meeting Kiyoshi Kubo.
EXT: Summary of activities, software development, and tuning performance 11th ATF2 Project Meeting, January M. Woodley1/29.
1 H. Hayano for the ATF collaboration Low Emittance Beam Generation in ATF H. Hayano for the ATF collaboration BPM electronics improvement emittance tuning.
WARM UP SOLVE USING THE QUADRATIC EQUATION, WHAT IS THE EXACT ANSWER. DON’T ROUND.
J. Brossard, C. Rimbault a P. Bambade LAL / / 8-9 nov LAL 1 Exercising emittance measurements in the ATF EXT line Upgrade.
Fall 2004CS-321 Dr. Mark L. Hornick 1 2-D Transformations World Coordinates Local/Modelling Coordinates x y Object descriptions Often defined in model.
Design options for emittance measurement systems for the CLIC RTML R Apsimon.
ATF2 Tuning Summary Nov & Dec 2010 Glen White, SLAC 11 th ATF2 Project Meeting, SLAC Jan
Linear Imperfections equations of motion with imperfections: smooth approximation orbit correction for the un-coupled case transfer matrices with coupling:
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.
Recent MIA Results Yiton T. Yan Stanford Linear Accelerator Center Acknowledgement: Y. Cai, F-J. Decker, S. Ecklund, J. Irwin, J. Seeman, M. Sullivan,
Emittance measurements with multiple wire-scanners and quadrupole scans in ATF EXT C. Rimbault, Brossard, P. Bambade (LAL) Main goal : - Try to improve.
Summary of Tuning, Corrections, and Commissioning ( Short summary of ATF2 meeting at SLAC in March 2007 ) and Hardware Issues for beam Tuning Toshiyuki.
ATF2 Software Review LAL June 2008 Philip Bambade & Glen White ATF2 weekly meeting June
Simulation of the α, dispersion, coupling and β multiknobs in large β optics Sha Bai, Philip Bambade, Benoit Bolzon, Javier Resta Lopez
Status of EXT coupling measurement analysis 9 th ATF2 project meeting C.Rimbault (LAL) S. Kuroda, T. Tauchi, N. Terunuma (KEK), G. White, M. Woodley (SLAC)
1 RTML Emittance Measurement Station Yuri Kubyshin (1), Robert Apsimon (2), Hector García (1,2) (1) Technical University of Catalonia (UPC) (2) CERN CLIC.
Status and plan of Beta-matching in Extraction line Kiyoshi Kubo.
2nd ATF2 Project Meeting (May 30, 2006)M. Woodley [SLAC]1 ATF2 Layout/Optics (v3.3) nBPM (SLAC) nBPM (KEK) FONT Compton / laserwire ODR Existing ATF Extraction.
Measurements and analysis of beam parameters at post-IP wire-scanner
at Royal Holloway Univ. London
Get out Ellipse: Notes Worksheet and complete #2 & #3 (Notes Sheet From Yesterday)
Let s be the 3x3 stress matrix and let n be a 3x1 unit vector
Beam Optics Set-Up at SLAC End Station A
3rd ATF2 Project Meeting, December 18-20, 2006
foci {image} None of these choices
Tilt Correction to Geometric Hourglass Effect
Geometric Camera Models
Find the focus of the parabola
Emittance Diagnostics
Beam-Based Alignment Results
Emittance Diagnostics
IR Lattice with Detector Solenoid
Expressions and Equations
Presentation transcript:

First analysis results of EXT MW0-4 X,Y,- 10,-10 wire-size measurements to reconstruct the 4D betatron phase-space

Questions opened by the First analysis results of EXT MW0-4 X,Y,- 10,-10 wire-size measurements to reconstruct the 4D betatron phase-space

1-Principle

Coupling Measurements: waist scan method - 1 Transfer Matrix: normal quad: R tot = RQ skew quad: R tot = RQ K Coupling terms Measurable terms The squares of the measured beam sizes,  11 M,  13 M,  33 M, at a wire scanner position can be expressed as a parabolic function of the strength of the scanned quad, described by 3 fit parameters A, B, C:  ij =A ij (k-B ij ) 2 +C ij  13 M can be measured using a tilted wire scanner, u (10 o ), applying method described in I. Agapov, G. Blair, M. Woodley, PRST-AB (2007) P. Emma, M. Woodley, ATF-99-04: where  is the angle between x and tilted wires

Coupling Measurements: waist scan method - 2 With normal quad scan: With skew quad scan:

2-Measurements

- Measurements performed on 28th May 2009 by G.W., Y.R., M.W., F.Z. - Dispersion measurements and corrections - QK1X scans: at -20, -10, 0, 10, and 20 A, 3 measurements each time - MW0X: y, +10 o, -10 o - MW1X-MW4X: x, y, +10 o, -10 o MW1X_xMW2X_xMW3X_xMW4X_x /-1596+/-3163+/-784+/ /-8103+/-3167+/-881+/ /-9102+/ /-379+/ / /-5163+/-779+/ /-5108+/ /-1084+/-2 MW0X_+10MW1X_+10MW2X_+10MW3X_+10MW4X_ / / / / / / / / / / / / / / / / / / / / / / / / /-0.6 MW0X_yMW1X_yMW2X_yMW3X_yMW4X_y / / / / / / / / / / / / / / / / / / / / / / / / /-1.2 MW0X_-10MW1X_-10MW2X_-10MW3X_-10MW4X_ / / / / / / / / / / / / / / / / / / / / / / / / /-2.6

3-First "difficulty"

The measurements we get from x and y are corrected from the moving 45 o axis, but not for +10 o and -10 o. Question: -How are oriented wire on each wire-scanners? Answer: the same for all the WS Beam direction Correction to apply to -10 o : cos(35 o ) With  =80 o Correction to apply to +10 o : cos(55 o ) With  =100 o

4- Graphical representation

x +10 o -10 o y MW0X MW1X MW2X MW3X MW4X

5- Coupling

From I. Agapov, G. Blair, M. Woodley, PRST-AB (2007), pp 8-9 Simple deductions - If the major axis of the beam lies along the horizontal axis  =0 - if ≠0, then =cste with  - if  (80 o )=  (100 o ) then =0

Coupling reconstruction applying MW1X MW2X MW4XMW3X from +10 o (  100) and -10 o  =80) measurements

Coupling reconstruction applying MW1X MW2X MW4XMW3X abs(1- + / - )

6- Questions 1 - Stupid mistakes from me... (after several verifications, no major bugs found) 2 - Are the named and wires invert / Was there an error in the positionning of the wires for the scan of the beam? 3 - Several other errors during data acquisition? other  Test of 2

Coupling reconstruction applying from +10 o (  100) and -10 o  =80) measurements with inversion of named +10/-10 wires MW1X MW2X MW4X MW3X

7- Interpretations Coupling reconstruction applying inversion of +10/-10 wires Results should look like b1: 2 options: 1 - Consider b1 is true:  +10 and -10 are invert + half of the data are "wrong" but what I mean by "true"?  2 - Should I believe this equation? fig. a fig. b

8- A bit of geometry

Are you agree with this? The tranverse profile of a gaussian beam can be represent by an ellipse of major axis  x and minor axis  y  x =5  y =1

From I. Agapov, G. Blair, M. Woodley, PRST-AB (2007), pp 8-9 From P. Emma, M. Woodley, ATF-99-04

If no coupling, =0 o B A C 

From P. Emma, M. Woodley, ATF If no coupling, =0 o B A C  A’ B’

From P. Emma, M. Woodley, ATF If no coupling, =0 o B A C’  A’ B’  !!!??? C

What I know about an ellipse general equation: reduce equation: o xx r  yy

But what do the wire scanners measure?: projections the tilted wires don’t measure the beam sizes, but the projection of r, such as: is maximal  

But what do the wire scanners measure: projections

From P. Emma, M. Woodley, ATF Is it the philosophy of this?

The measurements MW1X MW2XMW3X MW4X -20A -10A 0A 10A 20A