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: http://www.iki.rssi.ru/galeev/english/future.htm Дата изменения: Thu Dec 5 20:16:18 2013 Дата индексирования: Fri Feb 28 01:09:03 2014 Кодировка: Windows-1251 Поисковые слова: redshift survey | 
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 | FUTURE SEMINARS,  2013 December, 2 Vladimir Rakov (University
  of Florida, Institute of Applied Physics of the RAS) "Compact Intracloud
  Lightning Discharges" Abstract: Compact Intracloud Lightning Discharges
  (CIDs), which were first reported by Le Vine (1980), received their name
  (Smith et al. 1999) due to their relatively small (hundreds of meters)
  spatial extent. They November, 19 Leopold Lobkovsky (P.P.Shirshov
  Institute of Oceanology RAS) "Geological
  evolution and present lithosphere state of Arctic: field investigations,
  theoretical models and practical applications" September, 20 N. Vedenkin, S. Ivanov (Dauria
  Aerospace) "Dauria Aerospace microsatellites" September, 17 Joerg Buechner (Max
  Planck Institute for Solar System Research) "Magnetic
  reconnection at the Sun" September, 10 Irina Kitiashvili (Stanford
  University, Kazan University) "Turbulent MHD
  processes at the Sun " June, 27 Carl Gwinn (University
  of California, Santa Barbara) "RadioAstron Pulsar
  Early Science Results" Abstract: The early science program for the
  RadioAstron mission has produced remarkable results for pulsars. Using
  baselines as long as 220,00 km, we locate the material that scatters nearby
  pulsars, only 2-8 pc from Earth. 
  Observations of more distant, highly-scattered pulsars show fringes on
  baselines of tens of Earth diameters, where scattering should lead to zero
  average visibility. We discuss possible interpretations of this result. June, 17 Salvatore Capozziello (University
  of Napoli 'Federico II') "Scaling Relations
  from Gamma Ray Bursts to constrain Cosmography" Abstract: Relations connecting gamma ray burst
  quantities can be used to constrain cosmographic parameters of the Hubble law
  at medium-high redshifts. We consider a sample of gamma ray bursts to
  construct the luminosity distance to redshift relation and derive the values
  of the parameters q_0, j_0, and s_0. The analysis is compared with other
  methods in the literature. Gamma ray bursts, if calibrated by SNeIa, seem
  reliable as distance indicators and give cosmographic parameters in good
  agreement with some Dark Energy models. June, 13 Michael S. Briggs (The
  Center for Space Plasma and Aeronomic Research, Huntsville, USA) "Observations of
  Terrestrial Gamma-ray Flashes (TGFs) by the Fermi Gamma-ray Burst Monitor
  (GBM)" Abstract with references: Observations of Terrestrial Gamma-ray
  Flashes (TGFs) by the Fermi Gamma-ray Burst Monitor (GBM) TGFs have were discovered in the early 1990s
  and since then have been observed with several astrophysical instruments,
  most recently with the Gamma-ray Burst Monitor (GBM) on Fermi. With the large
  effective area of GBM new properties of the pulses have been found: in
  addition to the previously known muliple pulses with ms separations, very
  close pulses are observed [1,4]. The GBM sample has two pulse types; also,
  the rise time is aways equal to or shorter than the fall time [1]. A new GBM
  datatype and TGF search method has been implemented, making GBM the
  instrument with the highest TGF detection rate [7]. In addition to fainter
  TGFs, GBM is detecting TGFs shorter than ever before detected, with durations
  as short as 50 microseconds [7]. Some TGFs are observed at great distances
  from the source when electrons follow the Earth's magnetic field in a
  beam.  GBM found these Terrestrial
  Electron Beams (TEBs) to also contain positrons [2]. Correlation of GBM TGFs
  with ground-based radio observations has revealed new features [3,5,6]. A
  strong correlation between radio detection probabilty and gamma-ray duration
  changed our interpretation of the VLF radio detections, showing that they are
  of the current of the TGF itself [6]. preprints: http://gammaray.nsstc.nasa.gov/publications/tgf_journal.html [1] First Results on Terrestrial Gamma-ray
  Flashes from the Fermi Gamma-ray Burst Monitor, M. S. Briggs, G. J. Fishman,
  V. Connaughton, et al., J. Geophys. Res. (2010). [2] Electron-Positron Beams from Terrestrial
  Lightning Observed with Fermi GBM, M. S. Briggs, V. Connaughton, C. A.
  Wilson-Hodge, et al., Geophys. Res. Lett (2010). [3] Associations between Fermi GBM
  Terrestrial Gamma-ray Flashes and sferics from the WWLLN, V. Connaughton, M.
  S. Briggs, R. H. Holzworth, et al., J. Geophys. Res. (2010). [4] Temporal properties of the terrestrial
  gamma-ray flashes from the Gamma-Ray Burst Monitor on the Fermi Observatory,
  G. J. Fishman,, M. S. Briggs, V. Connaughton, et al., J. Geophys. Res.
  (2011). [5] The lightning-TGF relationship on
  microsecond timescales, S. Cummer, G. Lu, M. S. Briggs, et al., Geophys. Res.
  Lett (2011). [6] Radio signals from electron beams in
  Terrestrial Gamma-ray Flashes, V. Connaughton, M. S. Briggs, S. Xiong, et al.,
  J. Geophys. Res. (2012). [7] Terrestrial Gamma-ray Flashes in the
  Fermi era: Improved Observations and Analysis Methods, M. S. Briggs, S.
  Xiong, V. Connaughton, et al., J. Geophys. Res. (2013). Michael S. Briggs National Space Science & Technology Center Principal Research Scientist University of Alabama in Huntsville Gamma-Ray Astronomy Group 320 Sparkman Drive The Center for Space Plasma and Aeronomic
  Research (CSPAR)      Huntsville, AL 35805 Michael.Briggs@uah.edu or
  Michael.S.Briggs@nasa.gov 256-961-7667 April, 30 A.P. Itin (Institut für Laser-Physik,
  Hamburg, Germany; Zentrum für Optische Quantentechnologien (ZOQ), Hamburg, Germany; Space Research Institute (IKI), Moscow) "Bose-Einstein condensates:
  fundamental applications on the Earth and in space. Projects QUANTUS,
  PRIMUS, MAIUS, ZARM" April, 26 1.
  Weiqun Gan (the Purple Mountain Observatory, Nanjing, China) 2. Li Feng (the Purple Mountain Observatory, Nanjing, China) 1.
  Before the formal talk, I would like to take a few minutes to give a brief introduction
  of solar community in China and PMO. Then I will focus on our recent work on
  frequency distribution of solar flares: the scaled peak distribution of GOES
  flares; the thermal energy distribution of flares; a fitting study of the
  flare distribution.  2. On 2011 September 6, an X-class flare and a halo
  coronal mass ejection (CME) were observed from Earth erupting from the same
  active region AR 11283. The magnetic energy partition between them has been
  investigated. SDO/HMI vector magnetograms were used to obtain the coronal
  magnetic field using the nonlinear force-free field (NLFFF) extrapolation
  method. The free magnetic energies before and after the flare were calculated
  to estimate the released energy available to power the flare and the CME. For
  the flare energetics, thermal and nonthermal energies were derived using the
  RHESSI and GOES data. To obtain the radiative output, SDO/EVE data in the
  0.1-37 nm waveband were utilized. We have reconstructed the three-dimensional
  (3D) periphery of the CME from the coronagraph images observed by STEREO-A,
  B, and SOHO. The mass calculations were then based on a more precise
  Thomson-scattering geometry. The subsequent estimate of the kinetic and
  potential energies of the CME took advantage of the more accurate mass, and
  the height and speed in a 3D frame. The released free magnetic energy
  resulting from the NLFFF model is about 6.4 × 1031 erg, which has a
  possible upper limit of 1.8 × 1032 erg. The thermal and nonthermal
  energies are lower than the radiative output of 2.2 × 1031 erg from
  SDO/EVE for this event. The total radiation covering the whole solar spectrum
  is probably a few times larger. The sum of the kinetic and potential energy
  of the CME could go up to 6.5 × 1031 erg. Therefore, the free energy is
  able to power the flare and the CME in AR 11283. Within the uncertainty, the
  flare and the CME may consume a similar amount of free energy. April, 18 L. Rykhlova (INASAN) "Chelyabinsk
  meteorite and asteroid and cometary hazard" Abstract: Chelyabinsk meteorite entered Earth' s atmosphere at
  about 9-20 YEKT with estimated speed of 18 km/s. The total kinetic energy
  before atmospheric impact equivalent to approximately 450-500 kilotons of
  TNT. The object had not been detected before atmospheric entry. |