Small group Mott meeting

Slides:



Advertisements
Similar presentations
Linear Equations Review. Find the slope and y intercept: y + x = -1.
Advertisements

Excel Notes Phys244/246 © 2007, B.J. Lieb. Calculating Velocity The velocity is calculated by entering the following: =(B3-B2) / (A3-A2). Then drag the.
Chapter 3 Section 4 Copyright © 2008 Pearson Education, Inc. Publishing as Pearson Addison-Wesley.
1 Scintillating Fibre Cosmic Ray Test Results Malcolm Ellis Imperial College London Monday 29 th March 2004.
Chapter Eighteen MEASURES OF ASSOCIATION
Original image: 512 pixels by 512 pixels. Probe is the size of 1 pixel. Picture is sampled at every pixel ( samples taken)
CSE 326 Hashing Richard Anderson (instead of Martin Tompa)
CXC CUC September SDS Page 1 CUC Sep 2007 Science Data Systems – Jonathan McDowell.
TOPLHCWG. Introduction The ATLAS+CMS combination of single-top production cross-section measurements in the t channel was performed using the BLUE (Best.
Chi-squared distribution  2 N N = number of degrees of freedom Computed using incomplete gamma function: Moments of  2 distribution:
$100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300 $400 $500 $100 $200 $300.
Criteria to choose target foils for 1 st experiment Choose foils to test target thickness extrapolation vs. model => one Z maximizes number of points (we’ll.
Linear Regression Handbook Chapter. Experimental Testing Data are collected, in scientific experiments, to test the relationship between various measurable.
FE-SEM foil thickness measurements. Process Mount sister foils to Si wafers – Static for thinner foils – “glue” with aerodag carbon suspension for thicker.
ILC BDS Static Beam-Based Alignment and Tuning Glen White SLAC 1.Aims. 2.Error parameters and other assumptions. 3.Overview of alignment and tuning procedure.
Uncertainty in Measurement
Systematic error and double Gaussian fitting Toshi Gogami 3Apr2014.
Human vs. Dog Hair 50 µm scan
7 May 2009Paul Dauncey1 Tracker alignment issues Paul Dauncey.
WRITING REPORTS Introduction Section 0 Lecture 1 Slide 1 Lecture 6 Slide 1 INTRODUCTION TO Modern Physics PHYX 2710 Fall 2004 Intermediate 3870 Fall 2015.
. 5.1 write linear equation in slope intercept form..5.2 use linear equations in slope –intercept form..5.3 write linear equation in point slope form..5.4.
04/06/07I.Larin pi0 systematic error 1  0 error budget Completed items (review) Updated and new items (not reported yet) Items to be completed.
DN/d  and dN/dp T analysis status Gabor Veres for the working group QCD meeting, Jan 12, 2010.
Here are the IB Physics student requirements for dealing with uncertainties:  Describe and give examples of random and systematic errors. Dealing With.
Beam Studies December 2014 Runs: 7821, 7822, and 7860 December 29, 2014.
OMR Scanner vs. Image Scanner + OMR Software. Data Collection Systems OMR Scanners OMR Software.
CNI polarizations in Run09: Summary A.Bazilevsky For the RHIC CNI Group March 26, 2010 RSC meeting.
FIELD MAPPING V. Blackmore CM38 23rd February /70.
Exclusive |Vcb| at Belle
Alphington Photographic Club
Section 1.3 Lines.
Tilecal Pion Response and Energy Resolution
Computer Architecture Experimental Design
February 12 – 19, 2018.
Objective- To use slope and y-intercept to
Chapter 3 Section 4.
Stat 112 Notes 4 Today: Review of p-values for one-sided tests
Identifying Graphs of Linear Equations
Rate vs. Thickness Jan 18, 2017.
Mathematica fits vs. Root
PARENT GRAPH FOR LINEAR EQUATIONS
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
PrimEx Preliminary Result (short status)
Proton Beam Diagnostics
Summary of Ao extrapolation
Section 3.3 Linear Regression
Foil thickness measurements
Fitting different functional forms
ERROR BARS IN LOGGER PRO
Your Lecture you only have 8 minutes MAX 8 slides Start off with title Then give a 1 or 2 sentence introduction and conclusion Give me a topic/research.
Graphing Techniques.
Measurement and Significant Figures
  30 A 30 B 30 C 30 D 30 E 77 TOTALS ORIGINAL COUNT CURRENT COUNT
Studies of EPR-type flavor entangled states in Y(4s)->B0B0
Status of Instrumental Beam Studies and Technical Description of Detectors and DAQ February 24, 2017.
Pade order investigation Re-run of functional forms
Energy Calibration with Compton Data
(Re)Intro to Linear Equations
Looking at the 500 nm data point
Soothing Massage of HMI Magnetic Field Data
The Image The pixels in the image The mask The resulting image 255 X
Find the y-intercept and slope
Graphing with Uncertainties
Lecture 7 Spatial filtering.
Precision & Uncertainties
Types of Errors And Error Analysis.
Graph Info for Labs: In your lab book: For Lab Report:
° status report analysis details: overview; “where we are”; plans: before finalizing result.. I.Larin 02/13/2009.
L2036H1 grid6 First cut x x x x x x x x x x x x x x x x x x x x x x x
106.13: A Makeover for HMI Magnetic Field Data
Presentation transcript:

Small group Mott meeting 4 February 2016

Recent work First, write up thickness measurement section, refine error bars on data very slightly to avoid double counting Second, the small χ2 imply overestimated error bars. Do we really need the 2% foil uniformity and 5% batch uniformity specs? Third, churn through the Run 2 data vs. thickness using original error bars. Fourth, do we need to talk about the linear fit lopping off points at the end?

  Au_5385_B Au_3057_C Au_5134_B Au_7028_B Au_5275_C Au_5613_D Au_7029_B Au_6809_B nominal thickness (nm) 1000 870 750 625 500 355 225 50 mean thickness (all data, nm) 943.7 836.8 774.6 561.2 482.0 389.4 215.2 52.0 Stat. Stdev, nom. identical data (nm) 29.0 7.1 9.1 8.0 9.7 4.5 1.9 2.3 stdev image reanalysis (nm) 22.5 7.7 9.4 7.5 4.0 2.7 1.8 2.1 Syst. Image analysis: ± 4 Pixel 20.0 10.0 2.6 Resolution (1.2 nm inherent) 1.2 Tilt (0.4%) 4.6 4.2 3.9 2.8 2.5 1.1 0.3 Focus (1%) 8.4 5.6 4.8 2.2 0.5 Different spots (Lebow: 2%) 18.9 16.7 15.5 11.2 9.6 7.8 4.3 1.0 Sibling difference (Lebow:5%) 47.2 41.8 38.7 28.1 24.1 19.5 10.8 Totals stat uncertainty (nm) 36.7 10.5 13.1 11.0 5.2 3.1 syst uncertainty (nm) 55.6 46.7 43.8 31.9 27.7 22.9 12.2 4.1 total uncertainty (nm) 66.6 47.9 45.7 33.7 29.6 23.5 12.5 5.1

Pade(n,m) orders: Asy vs. Thick With both Lebow Uncertainties intercept dA R2 red. χ2 d.o.f. Conf Ftest (1,0) 43.8025 0.1169 0.991 1.28 9 <50? -- (2,0) 44.0176 0.1018 0.997 0.594 8 >70 11.45 (3,0) 44.1777 0.128 0.546 7 ~80 3.15 (rej F test) (0,1) 44.0382 0.0786 .554 >80 11.23 (0,2) 44.0484 0.1057 0.737 >60 0.022 (rej ftest) (1,1) 44.049 0.1061 9.67 (1,2) 44.0295 0.0986 0.870 6 >50 0.083 (rej. Ftest) (2,1) 45.0432 4.014 0.9977 0.6104 2.25 (rej. Ftest)

Both 5% batch and 2% uniformity Lebow uncertainties not included

Pade(n,m) orders: Asy vs. Thick, both systematic Lebow removed intercept dA R2 red. χ2 d.o.f. Conf. Ftest (1,0) 43.645 .155 0.993 3.55 9 -- (2,0) 43.95 .172 0.997 2.23 8 6.35 (3,0) 44.1523 .215 1.97 7 2.05 (0,1) 44.022 0.127 2.16 6.79 (0,2) 43.987 0.181 .997 2.44 .07 (1,1) 43.9854 0.180 2.85 5.22 (1,2) 43.9778 0.173 3.29 6 .198 (2,1) 49.1791 104 .998 2.49 1.85

Only 2% uniformity spec from Lebow included

Pade(n,m) orders: Asy vs. Thick With both only 2% Lebow Uncertainty intercept dA R2 red. χ2 d.o.f. Conf Ftest (1,0) 43.68 .147 .993 2.87 9 -- (2,0) 43.97 .997 1.56 8 8.60 (3,0) 44.156 .179 1.32 7 2.43 (0,1) 44.027 0.110 1.48 9.47 (0,2) 44.009 .153 1.68 0.027 (1,1) 44.008 1.96 7.15 (1,2) 3e10 5e10 2.26 6 .205 (2,1) 46.21 17.2 .998 1.64 2.18

Run two data: Pade terms

Run 1 Pade(n,m) orders: Asy vs. Thick intercept dA R2 red. χ2 d.o.f. Ftest (1,0) 43.8025 0.1169 0.991 1.28 9 -- (2,0) 44.0176 0.1018 0.997 0.594 8 11.45 (0,1) 44.0382 0.0786 .554 11.23 (1,1) 44.049 0.1061 0.737 7 9.67 Run 2 Pade(n,m) orders: Asy vs. Thick Pade(n,m) intercept dA R2 red. χ2 d.o.f. Ftest (1,0) 43.8437 0.1475 .984 2.28 9 -- (2,0) 44.1131 0.125 .993 1.01 8 12.21 (0,1) 44.0759 0.102 .994 1.04 11.61 (1,1) 44.1735 0.132 1.19 7 9.67

Linear fit: how many points? Points kept (of 11) Asym dA 5 43.9754 0.115 6 43.916 0.147 7 43.915 0.128 8 43.853 0.137 9 43.833 all 43.803 0.117