Fits for Pinhole and FresnelZonePlate

Slides:



Advertisements
Similar presentations
Richard Young Optronic Laboratories Kathleen Muray INPHORA
Advertisements

A Crash Course in Radio Astronomy and Interferometry: 4
xBSM meeting, Dan Peterson, Coded Aperture 1 1 A new Coded Aperture design In this talk, I will discuss a means to evaluated different coded.
Effect of b-tagging Scale Factors on M bb invariant mass distribution Ricardo Gonçalo.
05/03/2004 Measurement of Bunch Length Using Spectral Analysis of Incoherent Fluctuations Vadim Sajaev Advanced Photon Source Argonne National Laboratory.
Some answers to the questions/comments at the Heavy/Light presentation of March 17, Outline : 1) Addition of the id quadrant cut (slides 2-3); 2)
Multiple comparison correction Methods & models for fMRI data analysis 29 October 2008 Klaas Enno Stephan Branco Weiss Laboratory (BWL) Institute for Empirical.
Comp 665 Convolution. Questions? Ask here first. Likely someone else has the same question.
Matlab Tutorial Continued Files, functions and images.
Linear Filtering About modifying pixels based on neighborhood. Local methods simplest. Linear means linear combination of neighbors. Linear methods simplest.
02/12/02 (c) 2002 University of Wisconsin, CS 559 Filters A filter is something that attenuates or enhances particular frequencies Easiest to visualize.
Extension of the Excel-based Numerical Integration Calculation of the Coded Aperture Image to include mask partial-transmission and phase shift.
07/27/2004XFEL 2004 Measurement of Incoherent Radiation Fluctuations and Bunch Profile Recovery Vadim Sajaev Advanced Photon Source Argonne National Laboratory.
Outrigger Timing Calibration & Reconstruction Milagro – 11/17/03 Shoup – 1 Purpose: To incorporate outrigger hits in event angle fitting Additionally incorporated.
Signals CY2G2/SE2A2 Information Theory and Signals Aims: To discuss further concepts in information theory and to introduce signal theory. Outcomes:
Eusoballoon optics test Baptiste Mot, Gilles Roudil, Camille Catalano, Peter von Ballmoos Test configuration Calibration of the light beam Exploration.
XBSM Analysis - Dan Peterson Review of the optics elements: Pinhole (“GAP”), FZP, Coded Aperture Extracting information from the GAP what is the GAP width?
3/2003 Rev 1 II.3.15b – slide 1 of 19 IAEA Post Graduate Educational Course Radiation Protection and Safe Use of Radiation Sources Part IIQuantities and.
Simulation of direct space charge in Booster by using MAD program Y.Alexahin, A.Drozhdin, N.Kazarinov.
CSC508 Convolution Operators. CSC508 Convolution Arguably the most fundamental operation of computer vision It’s a neighborhood operator –Similar to the.
PSF in-flight calibration - PN IFC/CNRRingberg, April 2-4, 2002 PSF in-flight calibration for PN camera Simona Ghizzardi Silvano Molendi.
CS 691B Computational Photography
(c) 2002 University of Wisconsin, CS 559
 Measurement of  x E  (Fig. 4) Assorted correlations between a fixed high-p T trigger hadron (  p Ttrig  =4.7GeV/c) and lower p T associated hadrons.
Peterson xBSM Optics, Beam Size Calibration1 xBSM Beam Size Calibration Dan Peterson CesrTA general meeting introduction to the optics.
1 Oct 2009Paul Dauncey1 Status of 2D efficiency study Paul Dauncey.
Jeffery T. Mitchell (BNL) – Quark Matter The Evolution of Correlation Functions from Low to High p T : From HBT to Jets Quark Matter 2005 Jeffery.
UM PPS Lab Activities Mid-size Panel Tests PPS meeting January 15, 2012 Claudio, Curtis, Dan, Ethan, Riley.
Design of a New Coded Aperture Dan Peterson, Design study by DPP, John Flanagan and Brian Heltsley.
, Dan Peterson Apparent inconsistencies and other issues in the xBSM measurements of IBS Scans We have studied the pinhole and CodedAperture.
Calculation of the Coded Aperture zero-beam-size image (the “image”). The CA fitting procedure: The image is parameterized as a Sum-Of-Gaussians.
Grauman Today: Image Filters Smooth/Sharpen Images... Find edges... Find waldo…
XBSM Analysis - Dan Peterson Review of the optics elements: Pinhole (“GAP”), FZP, Coded Aperture Extracting information from the GAP what is the GAP width?
G. Eigen, Paris, Introduction The SiPM response is non-linear and depends on operating voltage (V-V bd ) and temperature  SiPMs need monitoring.
Charm Mixing and D Dalitz analysis at BESIII SUN Shengsen Institute of High Energy Physics, Beijing (for BESIII Collaboration) 37 th International Conference.
23 Jan 2012 Background shape estimates using sidebands Paul Dauncey G. Davies, D. Futyan, J. Hays, M. Jarvis, M. Kenzie, C. Seez, J. Virdee, N. Wardle.
Progress on Excel-based Numerical Integration Calculation
Momentum and Momentum Spread Measurements
New TRD (&TOF) tracking algorithm
Fabio, Francesco, Francesco and Nicola INFN and University Bari
C-Line Windowless Operation:
l 66TH MEETING OF THE ESRF l May 2014 l Author
Benchmarking MAD, SAD and PLACET Characterization and performance of the CLIC Beam Delivery System with MAD, SAD and PLACET T. Asaka† and J. Resta López‡
Signal processing.
Spread Spectrum Audio Steganography using Sub-band Phase Shifting
Tracking System at CERN 06 and 07 test beams
Beam-beam R&D for eRHIC Linac-Ring Option
Design of a New Coded Aperture
Progress on Excel-based Numerical Integration Calculation
OptiSystem-MATLAB data interchange model and features
Simplifying the Problem Tests of Self-Similarity
xBSM Analysis - Dan Peterson
EMCal Recalibration Check
a kind of filtering that leads to useful features
a kind of filtering that leads to useful features
EMCal Recalibration Check
Beam Instrumentation Meeting – Dan Peterson
Soft X-Ray pulse length measurement
Apparent Subdiffusion Inherent to Single Particle Tracking
Design of a New Coded Aperture
Problems with the Run4 Preliminary Phi->KK Analysis
Meeting 02/11/2016 – Andreas Christou
How we do Spectroscopy An Overview
Dan Peterson Comments on changing the C-line low-energy optics
Optics Measurements in the PSB
Filtering Images Work in the spatial domain
Imperial laser system and analysis
Slope measurements from test-beam irradiations
Dilepton Mass. Progress report.
Modern Observational/Instrumentation Techniques Astronomy 500
Presentation transcript:

Notes for xBSM meeting, 2012-01-05 Fits for Pinhole and FresnelZonePlate have been standardized to each call the same “TwoGaussFit”. There are 4 free parameters: Beam Size, Position Fraction of Image Area in SIGNAL Fraction of Image Area in Flat Background Each has a “signal” or “line shape” defined by 2 Gaussians, hence 6 fixed parameters : PinHole FresnelZonePlate Narrow Gaussian Locate 0 0 Fraction of SIGNAL 0.8 0.1284 Intrinsic Width 0 † 0.288 pixel =1/sqrt(12) Wide Gaussian Locate 0 0 Fraction of SIGNAL (1-0.8) (1-0.1284) Intrinsic Width 2 pixel 3.925 pixel † (subtracting(quad) 18 microns, 0.9 pixel at the image)

Coded Aperture: Implemented the DanP parameterization of the DanP calculated image from January 2011. The “line shape” is 12 gaussians, 36 fixed parameters. There are, AGAIN, 4 free parameters: Beam Size, Position Fraction of Image Area in SIGNAL Fraction of Image Area in Flat Background Well, OK, there is a 5th free parameter: Background slope, but this is constrained to 0 ± 2% . Also, implemented the DanP parametization of the JohnF calculated image for zero beam size, zero offset, some standard area. ~All information from John’s calculation is in this image. Brian templates in beam size. The MatLab code convolutes the beam size by describing the image as a linear sum of Gaussians.

DanP parameterization of the DanP calculated image DanP parameterization of the JohnF calculated image

Study of IBS data taken night of 2011-12-14 Conditions as described: PinHole subtractor: 18 microns CodedAperture: DanP January 2011 Systematic issues: PinHole result will increase with smaller subtractor. CodedAperture result will increase with decreased background level (slide) with decreased Gaussian widths (slide) . Will the agreement remain intact? I don’t know.

Extending to Left and Right sides of Coded Aperture image Fitted beam size in Coded Aperture is highly correlated with the background. Investigate the background level and slope. We did this 2 times: 2011-12-07 004018, 20, 21 2011-12-15 021428, 29, 30 . It could be done more often. Better to analyze this with averaged images. Learn that the background level should be lower, and the background is slightly higher (~4% ?) on the Left, and can be locked.

Intrinsic Gaussian widths: an error from January 2011 (This is kind-of technical.) The parameterization to 12 Gaussians starts with a smoothed image. [smoothed bin value] = (self + ½ NearestNeighbors) /2 This introduces a FWHM of 2 bins (=1 pixel) . A new parameterization matches the smoothed images with an equally smoothed Gaussian parameterization but with reduced intrinsic widths. With a value of 1 in the center, and ½ in the side bins, the RMS of this thing is 2-1/2 bins, or 0.3536 pixel. Optimum was found at 0.3735 pixel, 7.5 micron referred to the source. The line shape was too wide; ADD this subtractor.

Thinking about adding the semi-transparency of the mask. ( JohnF knows all about this. ) Increased the optics integration range beyond the 310 micron height Coded Aperture. 500 microns is still not enough. 500 microns * (projection =3.3) = 1.65 mm This causes those bumps on the sides. We can read off the semi-transparency from slide 5. 50% amplitude transmission (25% intensity) , -0.2λ phase shift ( vphase/c > 1 ) may have some nice features. (BLUE line) deaper central valley , w.r.t. the background level, more defined side peak on main peak. Must install transmission based on observed and phase shift based on material.