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Discovery of Relativistic Positrons in Solar Flares with Microwave Imaging and Polarimetry

Discovery of Relativistic Positrons in Solar Flares with Microwave Imaging and Polarimetry. Gregory D. Fleishman, Alexander T. Altyntsev, Natalia S. Meshalkina NJIT 05 Nov. 2013. HAPPY BIRTHDAY, DALE!. Dale Gary, Research Highlights I. Instrumentation. Owens Valley Solar Array (OVSA)

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Discovery of Relativistic Positrons in Solar Flares with Microwave Imaging and Polarimetry

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  1. Discovery of Relativistic Positrons in Solar Flares with Microwave Imaging and Polarimetry Gregory D. Fleishman, Alexander T. Altyntsev, Natalia S. Meshalkina NJIT 05 Nov. 2013

  2. HAPPY BIRTHDAY, DALE!

  3. Dale Gary, Research HighlightsI. Instrumentation • Owens Valley Solar Array (OVSA) • Korean Solar Radio Burst Locator (KSRBL) • FASR Subsystem Testbed (FST) • EOVSA Subsystem Testbed (EST) • Expanded OVSA (EOVSA )

  4. Dale Gary, Research HighlightsII. Research

  5. Dale Gary, Research HighlightsII. Research

  6. Dale Gary, Research HighlightsII. Research 276 Citations

  7. HAPPY BIRTHDAY, DALE!

  8. BEST WISHES, DALE! $60 Million NSF Grant Will Upgrade EOVSA to FASR NEWARK, Nov 5 2013 $60

  9. Discovery of Relativistic Positrons in Solar Flares with Microwave Imaging and Polarimetry Gregory D. Fleishman, Alexander T. Altyntsev, Natalia S. Meshalkina NJIT 05 Nov. 2013

  10. Plan of the talk • Where relativistic positrons come from in flares? • What is the positron contribution to the microwave emission? • How emission by positrons can be distinguished from that by electrons? • Can this be done with existing microwave databases? • Data analysis • Discussion and conclusions

  11. Origin of Relativistic Positrons in Flares

  12. Acceleration of Ions

  13. Polarimetry – a key to positron detection

  14. Nobeyama Radioheliograph (NoRH) is well suited for our study: NoRH produces images of intensity (I = R+L) and polarization (V = R – L) at 17 GHz while of the intensity only at 34 GHz. In addition, Nobeyama Polarimeters (NoRP) (Nakajima 1985) observe total power data (both I and V) at a number of single frequencies including 17 and 35 GHz. This set of observational tools suggests the following strategy of identifying properties of solar bursts with unambiguous positron contribution: • single, spatially coinciding, sources at both 17 and 34 GHz; • the 34 GHz emission must come from an area where the 17 GHz V displays a unipolar distribution (i.e., the polarization of 17 GHz emission has a definite sense throughout the region of 34 GHz emission); and • the total power V must have opposite signs at 17 and 34 GHz.

  15. 13 Mar 2000 Yohkoh NoRP Gan et al (2001).

  16. Gan et al (2001). Bz, photosphere V, 17 GHz, RCP

  17. Spectra X-ray Gan et al (2001). MW

  18. Polarization

  19. >90 MeV 24 Aug 2002 70-150 keV 0.7-2 MeV V.Kurt. Pr. Com.

  20. 17 May 1999

  21. 15 Jul 2004 Kawate et al. 2012

  22. 03 Mar 2000

  23. 02 Sep 2001

  24. 23 Apr 1998

  25. 24 Oct 2003 ?

  26. 9 Jul 2012 NO

  27. Summary • High-frequency microwave imaging spectropolarimetry offers a new way of detecting and studying relativistic positrons from solar flares. • Analysis of the Nobeyama database augmented by other context data reveals around 10 events-candidates with the relativistic positron signature; a few of them unambiguously show all expected evidence, so the conclusion that the positrons dominated in producing high-frequency microwave emission in those events seems inescapable. • New generation of the radio imaging instruments observing at many high frequencies, such as JVLA and ALMA, promises that the positron contribution to the GS emission can be routinely observed in many events. • Being observed at many frequencies the relativistic positron energy spectrum and spatial distribution can be measured in great detail as a function of time.

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