PIXEL SCANS. Measuring Data Measure last point before graphs cuts off at 1/10³. Measure last point before graphs cuts off at 1/10³. For spread of data,

Slides:



Advertisements
Similar presentations
PS wirescanner calibration Student Meeting 10/03/2014 Carolina Bianchini BE-BI-BL.
Advertisements

LHC Collimation Working Group – 19 December 2011 Modeling and Simulation of Beam Losses during Collimator Alignment (Preliminary Work) G. Valentino With.
Laser scans Feb 25 th -29 th Jamie & Marcel. Orientation: Laser Targets Event display: 13 QPONQPON HGFEHGFE PGCK 24 DCBADCBA LKJILKJI Region 0Region.
AN UPDATE ON ABSORPTION LENGTH MEASUREMENT WITH THE OB SYSTEM ANTARES Collaboration Meeting Paris (France), September 20th-24th H Yepes, J Barrios IFIC.
Status Report For Threshold Scans. Shaper/Sampler Drop Trims As promised new and improved trimming techniques have been developed. As suggested, we will.
AN UPDATE ON ABSORPTION LENGTH MEASUREMENT WITH THE OB SYSTEM ANTARES Collaboration Meeting Paris (France), September 20th-24th H Yepes, J Barrios IFIC.
Digital Cameras (Basics) CCD (charge coupled device): image sensor Resolution: amount of detail the camera can capture Capturing Color: filters go on.
The “zero” of a function is just the value at which a function touches the x-axis.
Chapter 11 Adjusting Colors. Chapter Lessons Correct and adjust color Enhance colors by altering saturation Modify color channels using levels Create.
7 Nov 2007Paul Dauncey1 Test results from Imperial Basic tests Source tests Firmware status Jamie Ballin, Paul Dauncey, Anne-Marie Magnan, Matt Noy Imperial.
1.1 EXPLORING STATISTICAL QUESTIONS Unit 1 Data Displays and Number Systems.
 The image that the digital camera sensor captures is based on the light reflected or emitted from a subject and how much the sensor is exposed to that.
Digital Image Processing Part 1 Introduction. The eye.
TPAC1.1 Testing JC/Feb 6th. Laser Scan: Test Pixel Test pixels were mounted specially in centre of pcb hole 2um spot 4um steps 50 measurements/pt  Before:
11 Sep 2009Paul Dauncey1 TPAC test beam analysis tasks Paul Dauncey.
Image Manipulation CSC361/661 – Digital Media Spring 2002 Burg/Wong.
A. Research the photo electric effect and provide a written explanation of the effect and its importance to modern physics B. Write down the equation for.
MPPC status M.Taguchi(kyoto) T2K ND /7/7.
1 A first look at the KEK tracker data with G4MICE Malcolm Ellis 2 nd December 2005.
26 Apr 2009Paul Dauncey1 Digital ECAL: Lecture 2 Paul Dauncey Imperial College London.
A MAPS-based readout for a Tera-Pixel electromagnetic calorimeter at the ILC Marcel Stanitzki STFC-Rutherford Appleton Laboratory Y. Mikami, O. Miller,
Introduction to Nanoscan
1 Oct 2009Paul Dauncey1 Status of 2D efficiency study Paul Dauncey.
, Dan Peterson Apparent inconsistencies and other issues in the xBSM measurements of IBS Scans We have studied the pinhole and CodedAperture.
IPBSM Operation 11th ATF2 Project Meeting Jan. 14, 2011 SLAC National Accelerator Laboratory Menlo Park, California Y. Yamaguchi, M.Oroku, Jacqueline Yan.
4 Jun 2008Paul Dauncey1 Crosstalk and laser results Paul Dauncey, Anne-Marie Magnan, Matt Noy.
Fits to consec data In what follows the black line shows the mean and the rms of the double gaussian fit The green line (usually too small to be visible)
Development of a pad interpolation algorithm using charge-sharing.
Program Design for REMPI Jingming Long 08/02/2010.
Irradiated 3D sensor testbeam results Alex Krzywda On behalf of CMS 3D collaboration Purdue University March 15, 2012.
1 James N. Bellinger Robert Handler University of Wisconsin-Madison 11-Monday-2009 Laser fan non-linearity James N. Bellinger 20-March-2009.
What is wave? A wave is a disturbance that moves from one place to another through a medium.
1 Edge Operators a kind of filtering that leads to useful features.
Equations of Straight Line Graphs. Graphs parallel to the y -axis All graphs of the form x = c, where c is any number, will be parallel to the y -axis.
1 Setting Laser Power and PMT Gain Begin with laser power at 20% Set PMT gain to 6.00.
28/11/02Guy Dewhirst1 Ultra Light Weights Method Guy Dewhirst Imperial College London.
A quadratic function always contains a term in x 2. It can also contain terms in x or a constant. Here are examples of three quadratic functions: The.
INTRODUCTION TO STATISTICS
EZDC spectra reconstruction and calibration
Lasers for the polarimeter
Solution of Nonlinear Equations
Figure 1. Whisker-evoked intrinsic signal in S1
Determining a Detector’s Saturation Threshold
Introduction to Summary Statistics
Introduction to Summary Statistics
The Coordinate Plane Chapter 2 Integers pg. 88.
Beam-beam R&D for eRHIC Linac-Ring Option
9 Graphs and Graphing.
Introduction to Summary Statistics
Introduction to Summary Statistics
Finding the Zeros of a Polynomial Function
Results of HyCal Analyses
a kind of filtering that leads to useful features
a kind of filtering that leads to useful features
Polynomial Functions of Higher Degree
Finding the Zeros of a Polynomial Function
Finding the Zeros of a Polynomial Function
3.3 Polynomial Functions and Models
Joseph M. Johnson, William J. Betz  Biophysical Journal 
Pixel Non-Uniformity Study
Section 2.3 Pictures of Data
What do you think will be the values of y?
Laser oscillation Laser is oscillator
Distance and the coordinate plane
Volume 107, Issue 6, Pages (September 2014)
3.3 Polynomial Functions and Models
Imperial laser system and analysis
Finding the Zeros of a Polynomial Function
GRAPHING.
Plotting quadratic graphs
Presentation transcript:

PIXEL SCANS

Measuring Data Measure last point before graphs cuts off at 1/10³. Measure last point before graphs cuts off at 1/10³. For spread of data, imagine fitting curve and take point where it would cross X axis. For spread of data, imagine fitting curve and take point where it would cross X axis. For larger spreads of data (see opposite), fit cubic polynomial. For larger spreads of data (see opposite), fit cubic polynomial.

Mask Scanning 9 x 9 Mask Scanned 9 x 9 Mask Scanned 3 x 3 Aperture 3 x 3 Aperture 60% Intensity 60% Intensity 50μm step size 50μm step size 1064nm Wavelength 1064nm Wavelength 25Hz Firing Frequency 25Hz Firing Frequency Continuous Firing Continuous Firing Scan Type: mpsAnalysis Threshold 149 Scan Type: mpsAnalysis Threshold 149 Scanned Between 50 and 350 units. Scanned Between 50 and 350 units.

Mask Scanning – 3D Data Plotted In 3D for aesthetics. Data Plotted In 3D for aesthetics. Cut Off Point Measured By Eye, defined as when no hits are recorded with more than 1/10³ frequency. Cut Off Point Measured By Eye, defined as when no hits are recorded with more than 1/10³ frequency.

Mask Scanning: Histogram Gaussian Fitted Ignoring Saturated Data Points. Gaussian Fitted Ignoring Saturated Data Points. Fitted by eye so may not be optimum Fitted by eye so may not be optimum

Mask Scans Other Region Another region was also scanned, 6mm down on sensor. Another region was also scanned, 6mm down on sensor. Prob statistic for green histogram is Prob statistic for green histogram is Mean = ± 4.3. Sigma = ± 4.11

Pedestal Adjustment Pedestals For each Pixel Subtracted And Data Replotted Pedestals For each Pixel Subtracted And Data Replotted

Pedestal Adjusted Histogram Gaussian Again Fitted By Eye. Gaussian Again Fitted By Eye. Histogram Does Not Include Saturated Pixels - 72 points. Histogram Does Not Include Saturated Pixels - 72 points.

Pedestal Adjustment In Other Region

Intensity Automate d Scans of Intensity For Several Pixels Automate d Scans of Intensity For Several Pixels % Alternatin g Steps of 2% and 3% % Alternatin g Steps of 2% and 3%. Scanned between 0 and 500 units. Scanned between 0 and 500 units.

Does Turning Laser Off and On Make A Difference? NO SIGNIFICANT DIFFERENCE

Alignment Data Scanned In Alternating 5 and 6 micron steps, over whole of Pixel (28,143). Scanned In Alternating 5 and 6 micron steps, over whole of Pixel (28,143). 2 x 2 Aperture 2 x 2 Aperture 1 x 1 Mask over chosen pixel 1 x 1 Mask over chosen pixel 60% Intensity 60% Intensity (All other settings same as for Mask Scanning) (All other settings same as for Mask Scanning) Coordinates arbitrary to allow ROOT plots. Coordinates arbitrary to allow ROOT plots.

Alignment Plots Looks As Though Laser Is Out of Focus!!!

Focused Alignment Scans Scanned Along X Axis Through Centre of Four Pixels (Separate 1 x 1 Mask for each) Scanned Along X Axis Through Centre of Four Pixels (Separate 1 x 1 Mask for each) 2 μm steps. 2 μm steps. Pixel (29,143) best displayed twin peaks. Pixel (29,143) best displayed twin peaks.

Pixel (29,143) Alignment Scanned along Y axis (through maximum point from earlier scan) to find Diode. Scanned along Y axis (through maximum point from earlier scan) to find Diode. Then along X axis, through maximum Point from Y Axis Scan. Then along X axis, through maximum Point from Y Axis Scan.

END More data is at SpiderWiki