Radio & Gamma-ray correlation of the blazar PKS 1424-418 during it's flaring state
←
→
Page content transcription
If your browser does not render page correctly, please read the page content below
Radio & Gamma-ray correlation of the blazar PKS 1424-418 during it's flaring state 44TH YOUNG EUROPEAN RADIO ASTRONOMY CONFERENCE (YERAC 2014) BY: PFESESANI VAN ZYL Dr Michael Gaylard (The late), Prof Sergio Colafrancesco & Dr Alet deWit HARTEBEESTHOEK RADIO ASTRONOMY OBSERVATORY (HARTRAO)
Outline Introduction to blazars Why are we interested in blazars? Introduction to my research topic Observations & Data reduction Results Conclusion Future work
Introduction to blazars BLAZARS AGN UNIFICATION SCHEME Subclass of AGN sources Harbor black hole (SMBH) at core (M > 10^6 Msol) More than 1000 times brighter than MW, E > 10^40 erg s^-1 Fuel – accretion of ISM matter SPECIAL CHARACTERISTICS Show strong polarizations in both the optical and radio λ's Radiate their energy at all λ's across the EM spectrum Viewed when radio jet Image credit: http://www.nasa.gov/centers/goddard/images/content/182566main2_1agn_LO.jpg is along observers line of sight Highly variable at all λ's, compact
Introduction to blazars SPECTRAL ENERGY DISTRIBUTION (SED) BLAZAR SED SED characterised by 2 broad peaks LBL – low energy peaking blazars known as FSRQ sources Emission spectra HBL – High energy peaking blazars known as BL Lac objects Feature less spectrum ENERGY EMISSION Two main sources: Sync IC Synchtrotron (Sync) emission Peaking in (IR-Opt) LBL Image credit: Giommi P, Colafrancesco S, Cavazzuti E, Perri M and Pittori C, 2006. Peaking in (UV-X-rays) HBL Inverse Compton (IC) emission Peaking in Gamma-rays (GeV) LBL Peaking in Gamma-rays (TeV) HBL
Introduction to blazars Two main sources: Synchtrotron (Sync) emission (RADIO EMISSION) e- spiralling around B-field Inverse Compton (IC) emission (GAMMA_RAY EMISSION) Low energy photons boosted to relativistic energies
Introduction to blazars Two main sources: Synchtrotron (Sync) emission (RADIO EMISSION) e- spiralling around B-field Not the only sources! Hadronic models Protons and e- main particles for Gamma-ray generation Bottcher et al. 2013 Inverse Compton (IC) emission (GAMMA_RAY EMISSION) Low energy photons boosted to relativistic energies
Why are we interested in blazars? Blazars: the only sources that JET GEOMETRY OF QUASAR 3C345 allow us to study the emission jets in detail Jets: find both high & low energy particles Blazar variability: helps constrain emission regions (establish physical Parameters e.g distance core to jet base) and Lets us study the behavior of the region around the BH Blazar multifrequency: Still many things we do not yet understand, e.g. Where the VLBI flux density plots of 3C345. HE gamma-ray particles originate Image credit: Kudryavtseva N A, Gabudza D C, Aller M F and Aller H D, 2011 from
Introduction to research AIM: RECENT VLBI IMAGE OF PKS 1424-418 Conduct a long-term (1 year) multi-wavelength study on PKS 1424-418 during its flaring state (Oct '12 – Sep '13) - Flat spectrum radio quasar (FSRQ) - z = 1.522 - highly compact core on VLBI scales - good positional stability – used as ICRF calibration source Interests: Correlation between Radio & Gamma-rays Time-lags METHOD: Conducted flux density observations of the Image credit: Mr Sayan Basu, HartRAO PHD student source Used the Discrete correlation function (DCF) (Edelson & Krolik 1988) to estimate possible correlations and time-lags between Gamma-rays & radio waves, and also between the radio waves themselves
Observations & Data Reductions Study based on Gamma-rays and radio waves: Gamma-rays: Short wavelengths 10^-12 m Do not penetrate atmosphere Require space based telescopes Radio waves: Long wavelength (mm - m) Penetrate Earth's atmosphere Can observe from Earth
Observations & Data Reductions OBSERVATIONS: FERMI-LAT OBSERVATIONS: HartRAO 26m dish On board the Fermi-GST 26m radio telescope at Hartebeesthoek Observed Gamma-rays since June 2008 Freq: 2.3 GHz, 4.8 GHz, 8.4 GHz and 12.2 GHz 20 MeV < E < +300 GeV On average 2 scans per day Entire sky every 3 hrs in all sky mode Used Drift-scan technique
Observations & Data Reductions DATA REDUCTIONS: HartRAO 26m DRIFT SCAN OF HYDRA A (3C218) Ran quality checks on scans: Outliers, RFI, baseline drifts Data fitting: parabolic fits to top 20% Source calibrated against a known calibrator source Hydra A (3C218) using equations from Ott et al. 1994 to estimate flux density of Hydra A Made plots of the flux density of PKS 1424-418 vs time to evaluate the source behavior
Results: Flux density PKS 1424-418 FERMI GAMMA-RAY DATA MULTIWAVELENGTH FLUX DENSITY PLOTS Results of the gamma-ray observations conducted by Fermi-LAT as they appear On the Fermi website, Results of the multiwavelength observations. The top level is the Fermi-LAT data http://fermi.gsfc.nasa.gov/FTP/glast/data/lat/catalogs/asp/current and levels 2, 3, 4 & 5 are HartRAO data @ 12.2, 8.4, 4.8 & 2.3 GHz respectively. /lightcurves/PKS1424-41_86400.png
Results: Flux density PKS 1424-418 FERMI GAMMA-RAY DATA MULTIWAVELENGTH FLUX DENSITY PLOTS Freq (GHz) ~Min Flux (Jy) ~Max Flux (Jy) ~% Change 12.2 6.4 9.5 67.4 8.4 5.4 8.0 67.5 4.8 3.2 6.3 51.0 2.3 2.5 4.8 52.1 Results of the gamma-ray observations conducted by Fermi-LAT as they appear On the Fermi website, Results of the multiwavelength observations. The top level is the Fermi-LAT data http://fermi.gsfc.nasa.gov/FTP/glast/data/lat/catalogs/asp/current and levels 2, 3, 4 & 5 are HartRAO data @ 12.2, 8.4, 4.8 & 2.3 GHz respectively. /lightcurves/PKS1424-41_86400.png
Results: Flux density
Results: Flux density Intensity over long term trend - 26.1% Intensity over observing period – 60.9%
Other Results: Flux density Image ref: Buson et al. 2014
Other results: Astrogeo (VLBI) Source structure changing over long term on VLBI scales - Each peak accompanied by matter ejection (compact at lower Flux) - Need more data and imaging to follow trend - Images on astrogeo website http://astrogeo.org/cgi-bin/imdb_get_source.csh?source=J1427-4206
Results : Data correlation - Gamma-ray/radio correlations have been found (Pushkarev et al. 2010, Fan et al. 2012, Kovalev et al. 2009, Richards et al. 2011) - can't be confirmed – too little data - most use - VLBI radio data, very little single dish - non-quasi simultaneous data - Consensus - if high Gamma-ray, radio exists - flares due to shock in jet model (Sokolov & Marscher 2004) producing both +ve and -ve lags
Results: Periodogram Found flare period! PERIODOGRAM OF PKS 1424-418 86.2 days for the flares Agrees with data but cannot conclude on this too few cycles, need more data Image credit: Mr Jabulani Maswanganye, HartRAO PHD student
Conclusion Both the Radio & Gamma-rays show some variability over the observing period. Found Gamma-rays & Radio waves were correlated − Gamma-rays leading Radio Found Radio waves were correlated − Most cases, higher frequencies were leading lower counterparts Found 86.2 day period between Gamma-ray flares All results show we need more data, and the importance of continuing with multi- wavelength observations.
Future work - Continue single dish monitoring on source PKS 1424-418 - Perform (O-C) analysis on gamma-ray data to see if periodicity is real - Include other southern hemisphere AGN flaring sources for Phd - Include VLBI data observations and imaging for these sources with the TANAMI group (Dr Roopesh Ojha – NASA JPL) to monitor stuctrural variability on milliarcsecond scales - Conduct spectral index studies on VLBI scales
Thank you
You can also read