BAYESIAN STUDY OF UHECRS Wooram Cho Institute of Physics and Applied Physics Yonsei University, Seoul, Korea [email protected] Feb. 21th, 2012 @ YongPyong Resort. YongPyong2012 Feb. 21st, 2011 1 CONTENTS Introduction Ultra High Energy Cosmic Rays(UHECRs) Telescope Array(TA) Experiment Bayesian Study of UHECRs Bayesian Analysis and Likelihood Function Density distribution and UHECR AGNs(VCV catalogue) and 27 Highest Energy PAO UHECRs. REFERENCE: Summary ARXIV:1010.0911V1 A BAYESIAN ANALYSIS OF THE 27 HIGHEST ENERGY COSMIC RAYS DETECTED BY THE PIERRE AUGER OBSERVATORY WATSON ET AL. YongPyong2012 Feb. 21st, 2011 2 INTRODUCTION TO COSMIC RAY Primary particle Extensive Air Shower Ground Detector Array Experiment EAS can be detected by ground detectors, Detected signals are correlated with the Primary energy, type of primary particle and the arrival direction. YongPyong2012 Feb. 21st, 2011 3 INTRODUCTION TO COSMIC RAY Energy spectrum Mass composition Source of cosmic ray EAS can be detected by ground detectors, Detected signals are correlated with the Primary energy, type of primary particle and the arrival direction. YongPyong2012 Feb. 21st, 2011 4 TELESCOPE ARRAY EXPERIMENT 109~1010 eV 1012 eV 1015 eV Telescope Array Experiment( Utah, USA) ◆: Surface Detector HOT ISSUE!! GZK cutoff 1019 eV 1020 eV YongPyong2012 Feb. 21st, 2011 5 Bayesian Study of UHECRs Bayesian Analysis and Likelihood Function Bayesian approach Full likelihood function in watson’s paper. Simple likelihood function Density distribution and UHECR AGNs(VCV catalogue) and 27 Highest Energy PAO UHECRs. YongPyong2012 Feb. 21st, 2011 6 BAYESIAN ANALYSIS r_src : emission rate from src R_bkg : emission rate from bkg Posterior Probability Distribution(LEFT) is proportional to Likelihood function(RIGHT), when prior probability can be approximated to step function. Celestial sphere model of 180(dec)*360(ra) pixels Ref. arXiv:1010.0911v1 watson et al. YongPyong2012 Feb. 21st, 2011 7 CELESTIAL SPHERE MODEL Violet : random events Red and Blue : PAO events Science,318,938, Abraham J., et al. Black : VCV AGN YongPyong2012 Feb. 21st, 2011 8 SIMPLE LIKELIHOOD FUNCTION Ref. arXiv:1010.0911v1 Watson et al. Nc,p : counted number of events in each pixel YongPyong2012 Feb. 21st, 2011 9 SIMPLE LIKELIHOOD FUNCTION Ref. arXiv:1010.0911v1 Watson et al. Nc,p : counted number of events in each pixel Poisson distribution YongPyong2012 Feb. 21st, 2011 10 SIMPLE LIKELIHOOD FUNCTION Ref. arXiv:1010.0911v1 Watson et al. Nc,p : counted number of events in each pixel Poisson distribution Area of each pixel YongPyong2012 Feb. 21st, 2011 11 SIMPLE LIKELIHOOD FUNCTION Ref. arXiv:1010.0911v1 Watson et al. Nc,p : counted number of events in each pixel Poisson distribution Area of each pixel YongPyong2012 Refraction of arrival direction Feb. 21st, 2011 12 SIMPLE LIKELIHOOD FUNCTION Ref. arXiv:1010.0911v1 Watson et al. Nc,p : counted number of events in each pixel Poisson distribution Area of each pixel Refraction of arrival direction GZK effect YongPyong2012 Feb. 21st, 2011 13 SIMPLE LIKELIHOOD FUNCTION Ref. arXiv:1010.0911v1 Watson et al. Nc,p : counted number of events in each pixel Poisson distribution Area of each pixel Refraction of arrival direction GZK effect YongPyong2012 Feb. 21st, 2011 14 SIMPLE LIKELIHOOD FUNCTION Remove effect of Energy, Pixel area, arrival angle error. SRC or BKG fills one pixel completely UHECR emission rate/each pixel : Constant YongPyong2012 Feb. 21st, 2011 15 SIMPLE LIKELIHOOD FUNCTION All events from AGN YongPyong2012 All events from BKG 27 PAO events Feb. 21st, 2011 16 SIMPLE LIKELIHOOD FUNCTION F_AGN=1 F_AGN=0 F_AGN=4/27 FAGN= (UHECR from AGN)/(detected UHECR) YongPyong2012 Feb. 21st, 2011 17 Bayesian Study of UHECRs Bayesian Analysis and Likelihood Function Density distribution and UHECR Matter can be the source of UHECR Density distribution and TA data AGNs(VCV catalogue) and 27 Highest Energy PAO UHECRs. YongPyong2012 Feb. 21st, 2011 18 DENSITY DISTRIBUTION AND UHECR Z:Y:X Dec:z:ra:delta(color), (z<0.03) Binned dec:ra density distribution is reconstructed from SDSS Mon. Not. R. Astron. Soc. 409, Jens Jasche et al. UHECRs can be generated in dotted pixels YongPyong2012 Feb. 21st, 2011 19 DENSITY DISTRIBUTION AND UHECR r -> 1 YongPyong2012 Feb. 21st, 2011 20 DENSITY DISTRIBUTION AND UHECR TA 12 -1 Y : F_src 2 Random 12 1 0 0 YongPyong2012 1 2 X : F_bkg – Fraction of cosmic ray from BKG Feb. 21st, 2011 21 DENSITY DISTRIBUTION AND UHECR TA 12 0 Random 12 YongPyong2012 Feb. 21st, 2011 22 DENSITY DISTRIBUTION AND UHECR TA 12 1 Random 12 YongPyong2012 Feb. 21st, 2011 23 DENSITY DISTRIBUTION AND UHECR TA 12 2 Random 12 YongPyong2012 Feb. 21st, 2011 24 Bayesian Study of UHECRs Bayesian Analysis and Likelihood Function Density distribution and UHECR AGNs(VCV catalogue) and 27 Highest Energy PAO UHECRs. My likelihood function Linearity test YongPyong2012 Feb. 21st, 2011 25 AGN AND UHECR Violet : random events Red and Blue : PAO events Science,318,938, Abraham J., et al. Black : VCV AGN YongPyong2012 Feb. 21st, 2011 26 AGN AND UHECR Nc,p : counted number of events in each pixel except Energy spectrum and GZK effect (because energy of each event can be reconstructed) YongPyong2012 Feb. 21st, 2011 27 AGN AND UHECR Red : VCV AGN Black : Probability of arriving of cosmic ray emitted from AGN YongPyong2012 Feb. 21st, 2011 28 AGN AND UHECR Y : F_AGN 2 Events observed by PAO 1 0 0 1 2 Likelihood functions and its contour plots Y axis : Events from source / X axis : Events from background YongPyong2012 Feb. 21st, 2011 29 AGN AND UHECR All events are from AGN Random events Expected figure of AGN events Expected figure of Random events Likelihood functions and its contour plots Y axis : Events from source / X axis : Events from background YongPyong2012 Feb. 21st, 2011 30 LINEARITY TEST Likelihood functions and its contour plots Y axis : Events from source / X axis : Events from background Z=0.003 , F_AGN=0 ~ F_AGN=1 YongPyong2012 Feb. 21st, 2011 31 MAX. LIKELIHOOD VS F_AGN PAO case : 1.80E-01 YongPyong2012 Prelim. +1.34E-01 -9.41E-02 Feb. 21st, 2011 32 MAX. LIKELIHOOD VS F_AGN Prelim. Sources should be selected by applying PAO case : 1.80E-01 YongPyong2012 +1.34E-01 -9.41E-02 Feb. 21st, 2011 33 SUMMARY Summary By Applying Bayesian statistics, correlation between AGN and UHECR can be estimated using Maximum likelihood estimator. Plan Linearity test will be done. This study will be applied to TA data. Density distribution will be applied to this study. Large Scale Structure study. YongPyong2012 Feb. 21st, 2011 34 THANK YOU VERY MUCH. Mr W.R.Cho with Al profiles on the top (2008). YongPyong2012 Feb. 21st, 2011 35 .bak YongPyong2012 Feb. 21st, 2011 36 RE-PRODUCING Ref. arXiv:1010.0911v1 Watson et al. Nc,p : counted number of events in each pixel YongPyong2012 Feb. 21st, 2011 37 RE-PRODUCING Smearing angle=3deg sa=5 sa=6 F_AGN=9% sa=10 F_AGN=11% sa=20 sa=12 F_AGN=15% Likelihood functions and its contour plots Y axis : Events from source / X axis : Events from background 27 PAO events, gamma = 3.6 , various sigma_angle/2(sa) YongPyong2012 Feb. 21st, 2011 38 REPRODUCING sigma_angle/2 Y_maximum Sum(prob. point ) F_AGN F_AGN(wats on) 1.5 5.00E-02 1.71E+06 22.65 3 5.05E-03 6.85E+06 9.17 5 1.96E-03 1.92E+07 9.94 6 1.50E-03 2.78E+07 11.01 22 10 7.19E-04 8.02E+07 15.29 31 YongPyong2012 Feb. 21st, 2011 18 39 Neutrino fluxes from AGN YongPyong2012 Feb. 21st, 2011 40 BAYESIAN ANALYSIS Ref. arXiv:1010.0911v1 Watson et al. r_src : emission rate from src R_bkg : emission rate from bkg Events observed by PAO Expected figure of Random events Likelihood functions and its contour plots Y axis : Events from source / X axis : Events from background YongPyong2012 Feb. 21st, 2011 41
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