LIGO-G020332-00-W The knownpulsardemod DSO August 2002 LSC Update PULG Session 08/23/02 Gregory Mendell LIGO Hanford Observatory.

Slides:



Advertisements
Similar presentations
Estimating a Population Variance
Advertisements

LIGO-G Z Beating the spin-down limit on gravitational wave emission from the Crab pulsar Michael Landry LIGO Hanford Observatory for the LIGO.
LIGO-G W Gregory Mendell and Mike Landry LIGO Hanford Observatory The StackSlide Search Summary: November 2003.
LIGO-G W Gregory Mendell, LIGO Hanford Observatory on behalf of the LIGO Scientific Collaboration StackSlide Summary LSC Meeting, August 2005.
Searching for pulsars using the Hough transform Badri Krishnan AEI, Golm (for the pulsar group) LSC meeting, Hanford November 2003 LIGO-G Z.
Chapter 26: Comparing Counts. To analyze categorical data, we construct two-way tables and examine the counts of percents of the explanatory and response.
BCOR 1020 Business Statistics
Introduction To Signal Processing & Data Analysis
Goodness of Fit Test for Proportions of Multinomial Population Chi-square distribution Hypotheses test/Goodness of fit test.
1 1 Slide © 2014 Cengage Learning. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole.
LIGO-G W Gregory Mendell, LIGO Hanford Observatory on behalf of the LIGO Scientific Collaboration Stackslide search for continuous gravitational.
SECTION 6.4 Confidence Intervals for Variance and Standard Deviation Larson/Farber 4th ed 1.
The Demodulation Code The Demodulation Code For the 1 st and 3 rd stage of hierarchical searches and for targeted searches of known objects. LIGO-G Z.
1 1 Slide IS 310 – Business Statistics IS 310 Business Statistics CSU Long Beach.
1 1 Slide © 2005 Thomson/South-Western Chapter 12 Tests of Goodness of Fit and Independence n Goodness of Fit Test: A Multinomial Population Goodness of.
For testing significance of patterns in qualitative data Test statistic is based on counts that represent the number of items that fall in each category.
LIGO- XXX Bruce Allen, LSC Talk LIGO Scientific Collaboration - U. Wisconsin - Milwaukee 1 Effects of Timing Errors and Timing Offsets in Pulsar.
Physics 114: Exam 2 Review Lectures 11-16
The Continuous Waves UL Group: status report. LSC Meeting LIGO Hanford Observatory August 2002 M.Alessandra Papa LIGO-G Z.
Status of Standalone Inspiral Code Duncan Brown University of Wisconsin-Milwaukee LIGO Scientific Collaboration Inspiral Working Group LIGO-G Z.
Analysis of Two-Way Tables Moore IPS Chapter 9 © 2012 W.H. Freeman and Company.
Data Analysis for Two-Way Tables. The Basics Two-way table of counts Organizes data about 2 categorical variables Row variables run across the table Column.
Selecting Input Probability Distribution. Simulation Machine Simulation can be considered as an Engine with input and output as follows: Simulation Engine.
Yousuke Itoh GWDAW8 UW Milwaukee USA December 2003 A large value of the detection statistic indicates a candidate signal at the frequency and.
G030XXX-00-Z Excess power trigger generator Patrick Brady and Saikat Ray-Majumder University of Wisconsin-Milwaukee LIGO Scientific Collaboration.
NSF Review, 18 Nov 2003 Peter Shawhan (LIGO/Caltech)1 How to Develop a LIGO Search Peter Shawhan (LIGO / Caltech) NSF Review November 18, 2003 LIGO-G E.
15-18 December 2004 GWDAW-9 Annecy 1 All-Sky broad band search for continuous waves using LIGO S2 data Yousuke Itoh 1 for the LIGO Scientific Collaboration.
Chi Square Test for Goodness of Fit Determining if our sample fits the way it should be.
GW pulsars in binary systems Sco X-1 C Messenger and A Vecchio LSC General Meeting LIGO Livingston Observatory 17 th – 20 th March, 2003 LIGO-G Z.
LIGO-G9900XX-00-M DMT Monitor Verification with Simulated Data John Zweizig LIGO/Caltech.
Scientific data storage: How are computers involved in the following?
AP Stats Check In Where we’ve been… Chapter 7…Chapter 8… Where we are going… Significance Tests!! –Ch 9 Tests about a population proportion –Ch 9Tests.
Report on the FCT MDC Stuart Anderson, Kent Blackburn, Philip Charlton, Jeffrey Edlund, Rick Jenet, Albert Lazzarini, Tom Prince, Massimo Tinto, Linqing.
SC03 failed results delayed FDS: parameter space searches
Inference concerning two population variances
Unit 9 White Noise FFT.
National Mathematics Day
Hypotheses and test procedures
Searching for pulsars using the Hough transform
Chapter 4. Inference about Process Quality
Vocoders.
The Q Pipeline search for gravitational-wave bursts with LIGO
Coherent wide parameter space searches for gravitational waves from neutron stars using LIGO S2 data Xavier Siemens, for the LIGO Scientific Collaboration.
LIGO Scientific Collaboration meeting
(Y. Itoh, M.A.Papa,B.Krishnan-AEI, X. Siemens –UWM
Active Learning Lecture Slides
A.M. Sintes for the pulgroup
Estimating a Population Variance
John Loucks St. Edward’s University . SLIDES . BY.
1 Vocoders. 2 The Channel Vocoder (analyzer) : The channel vocoder employs a bank of bandpass filters,  Each having a bandwidth between 100 HZ and 300.
Linear Regression Models
Physics 114: Exam 2 Review Material from Weeks 7-11
Data Analysis for Two-Way Tables
Statistical Methods For Engineers
CHAPTER 29: Multiple Regression*
Targeted Searches using Q Pipeline
Broad-band CW searches in LIGO and GEO S2 and S3 data
AP Stats Check In Where we’ve been… Chapter 7…Chapter 8…
Econ 3790: Business and Economics Statistics
University of Wisconsin-Milwaukee
Broad-band CW searches in LIGO and GEO S2 and S3 data
Chapter 11: Inference for Distributions of Categorical Data
Excess power trigger generator
Line tracking methods used in LineMon
Multiple Regression Chapter 14.
Environmental Monitoring: Coupling Function Calculator
The STACK-SLIDE Search Initial Report: PULG F2F UWM June 2003
Replicated Binary Designs
CW Search Group Efforts – overview Michael Landry LIGO Hanford Observatory on behalf of the CW Search Group LSC Meeting June 6, 2004 Tufts University,
The Search For Periodic Gravitational Waves
Presentation transcript:

LIGO-G W The knownpulsardemod DSO August 2002 LSC Update PULG Session 08/23/02 Gregory Mendell LIGO Hanford Observatory

LIGO-G W The knownpulsardemod DSO Runs under LDAS. Code is in LALWrapper CVS. Generates Short-time Fourier Transforms (SFTs). NEW: inputs SFTs, and ephemeris data from ilwd. NEW: wrote LALWRAPPERInitBarycenter to transfer ephemeris data from LDAS to LAL. Uses the LALDemod function to generate JKS F statistic for one set of source parameters. Writes to the SIGNAL_DPERIOD database table. NEW: also writes to the search summary and search summary variables tables; outputs F statistic in frame or ilwd format for a specified frequency band.

LIGO-G W The JKS F Statistic Jaranowski, Krolak, and Schutz gr-qc/ ; Schutz & Papa gr- qc/ ; Williams and Schutz gr-qc/ ; Berukoff and Papa LAL Pulsar Package Documentation 0T

LIGO-G W E7 Update Loop scripts drove knownpulsardemod to generated SFTs for L1, H1, and H2. Scripts are checked into MDC CVS. NEW: E7 SFTs data are available from LDAS using getsftdata.tclsh script. (Need ligotools LDAS job package and LDAS password.) NEW: LDAS can read SFT data very quickly (1 days worth of data in 1 Hz band in < 60 seconds.) NEW: knownpulsardemod test jobs that produce the JKS F statistic have been run on E7 data.

LIGO-G W Goals before S1 (from last LSC conf.). Update knownpulsardemod DSO to work with latest LAL and LDAS code. (DONE.) Understand distribution of SNR and F statistic in Jaranowski, Krolak, and Schutz gr-qc/ (Understand the case of pure gaussian noise.) Understand how to set upper limits. (Have thought very briefly about this.) Design and run knownpulardemod MDC tests for LALDemod. (SURF Student Brian Cameron worked on LALapps test code.)

LIGO-G W Test Code Progress SURF student Brian Cameron wrote LAL-apps code to aid testing this summer. We worked on four basic tests:  Compared Brian’s code vs. LALDemod.  Generated synthetic data sets to study the distribution of the F statistic.  Studied: “Is F the best estimator?”  Studied effective of windowing and side lobes on SNR. Much more work is needed.

LIGO-G W Simple Test of LALDemod Brian Cameron’s test code vs. LALDemod.

LIGO-G W Distribution of the F Statistic. Note that F depends on a(t)exp[i  (t)] and b(t)exp[i  (t)]. Note that a(t) and b(t) are proportional to sin(2  f r t) and cos(2  f r t), where f r is the frequency of the Earth’s rotation. Thus F depends on amplitudes of sin(  (t)  2  f r t) and cos(  (t)  2  f r t). For white noise this corresponds to 4 gaussian distributed random amplitudes; F can be written as the sum of the squares of linear combinations of these and thus follows a chi-squared distribution for 4 degrees of freedom.

LIGO-G W Special Case If  (t) = 2  f c t, where f c is the Nyquist frequency, the F statistic comes from f c  f r bins which are aliased to each other. For this case and white noise, F depends on only 2 independent gaussian distributed random variables, not 4. Thus F follows a chi- squared distribution for 2 degrees of freedom.

LIGO-G W Special Case Nyquist Frequency, Distribution of F For pure noise we get the usual chi-squared with 2 degrees of freedom:  (F) dF = 1/2  2 exp(-F/2  2 )dF Courtesy Brian Cameron

LIGO-G W Special Case Nyquist Frequency, Distribution of A =  F For pure noise we get the usual Rayleigh distribution  (A) dA = A/  2 exp(-A 2 /2  2 ) dA Courtesy Brian Cameron

LIGO-G W General Case, Distribution of F For pure noise we get a chi-squared with 4 degrees of freedom:  (F) dF = 1/4  4 F exp(-F/2  2 ) dF, as predicted. Courtesy Brian Cameron fit is * F^ * exp(-F/ )

LIGO-G W General Case, Distribution of A =  F For pure noise we get the expected distribution  (A) dA = A 3 /2  4 exp(-A 2 /2  2 ) dA Courtesy Brian Cameron fit is * A^ * exp(-A^2/ )

LIGO-G W Is JKS F stat the best estimator? Should we track the amplitude and phase or just the phase? Generated signal at ¼ Nyquist frequency with large spindown and equiv of 10 days of data; SNR = max(A) with signal present divided by mean(A) when only noise is present. solid curve = no tracking, dot-dashed = track phase only, dotted = F stat tracks amp & phase = best. SNR ~  T for latter two, though this is not obvious from the graph. Differences are due to leakage into side lobes. Courtesy Brian Cameron

LIGO-G W Side lobes in JKS F Statistic Courtesy Brian Cameron

LIGO-G W Special case without amplitude tracking Courtesy Brian Cameron

LIGO-G W General case with amplitude tracking = F statistic Courtesy Brian Cameron

LIGO-G W General case without amplitude tracking Courtesy Brian Cameron

LIGO-G W Effective Windowing of Data

LIGO-G W Leakage Due to Windowing

LIGO-G W Sample Result from E7 Produced by knownpulsardemod LDAS job in less than 2 minutes. Anyone with LDAS password can run jobs to get data like this. Warning: code is untested!

LIGO-G W Data Quality and Dropout Clean locks are used to generate a quality channel. Poor quality data is “padded” (replaced) with the mean of the good quality data. The percent of the data padded is stored in the SFT history structure. NEW: percent clean lock for S1 SFTs will be stored in search summary vars database table. Data dropout code is not yet working. SFTs are missing for drop outs during E7. SAME will be true for S1.

LIGO-G W knownpulsardemod MDC Held November at LHO. In DCC: LIGO-T W Primarly Tested SFT generation. MDC scripts and documentation are in UWM mdc CVS repository. NEW: need another MDC to test new code, before S1 data can be analyzed with confidence. Code needs to be debugged first.

LIGO-G W Example Test TEST 2a Correctness of SFT output Purpose: Test that the SFTs output by the KPD DSO are indeed the DFT of the input data for input data with known results. Tester: ______________. Date & Time: __________. Tester Location: ___________. Job Site: _______________________. Job Database: __________________________. Job Channel: ___________________. Job Log File: ____________________________. Instructions: (See the “How to run the test scripts” section if you need help.) Use RunJob.tclsh to run the jobs below, perform the task indicated, and record the results. 1. Impulse tests. These test run on KPDTEST-ImpulseN32I gwf, which contains 32 data points sampled at 32 Hz, with an impulse in the 16 th data point (index = 15).. a. Run kpdImpulseTest.job. The output will be an xml file. Ftp the result to the KPD MDC output URL. Append test.2a.1a to the name. Check that the results agree with that in ASCII_ImpN32I16Output.txt. LDAS Job #: Pass/Fail