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UID:E1C486FF-B489-474E-A5FF-D0ECC6F0D003
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DESCRIPTION:When studying the properties of the Vavilov-Cherenkov radiation
  (VChR) arising from the arbitrary motion of a charged particle in the tra
 nsparent medium\, using the catastrophe theory\, the existence of a new ty
 pe of radiation\, the cuspoid VChR\, was predicted. This radiation is a re
 alisation of cuspoid catastrophes in electromagnetic radiation. The radiat
 ion can be generated at the non-constant motion of a charged particle in a
  transparent medium and is emitted at a very narrow solid angle. The radia
 tion is more intensive than ordinary VChR and is generated only at specifi
 c angles\, that depend uniquely on the particle&#39;s motion in the medium. Fo
 r this reason\, it could be used to measure particle parameters that deter
 mine the motion of a charged particle\, such as momentum and charge. The m
 omenta of charged particles are usually determined in magnetic spectromete
 rs. The Lorentz force causes the particles to follow circular or helical t
 rajectories around the direction of the magnetic field. The bending radius
  R of particle tracks is related to the magnetic field strength and the mo
 mentum component of the particle perpendicular to the magnetic field ptran
 s. With a suitably focusing optical system\, this allows the reconstructio
 n arc of a ring. In a focusing detector\, the photons can be collected by 
 a spherical mirror with focal length f and focused onto the photon detecto
 r placed at the focal plane. The result is an arc of the circle with a rad
 ius r\, independent of the emission point along the particle&#39;s track. The 
 main goal of this work is to study the cuspoid radiation emitted by a char
 ge when it moves in a magnetic field and its application in high-energy ph
 ysics and neutrino physics. If we use the ring-imaging detection technique
 \, then we can measure the following parameters using cuspoid radiation: r
 adius r of the arc of the ring (r is directly related to ptrans)\, deflect
 ion angle ψ\, azimuthal angle φ\, polar angle θ and the number of emitt
 ed photons Ncusp. With the help of these parameters\, it is\, in principle
 \, also possible to determine the position of the vertex\, the origin of p
 article track in the magnetic field. Cuspoid radiation could be an alterna
 tive for measuring the momentum of relativistic particles and improve the 
 possibilities of their identification. In many cases\, measuring only elec
 tromagnetic radiation (Cherenkov\, cuspoid) will be sufficient to identify
  a charged particle. Due to the large penetrating power of muons in materi
 als\, the influence of multiple scattering on its trajectory in a transpar
 ent medium placed in a magnetic field can be neglected. Muon detection is 
 an important aspect of neutrino physics and\, therefore\, in our opinion\,
  measuring the muon momentum using the cuspoid radiation method can be of 
 significant help in experiments aimed at investigating the properties of n
 eutrino. The advantage is that the same Ring Imaging Cherenkov detectors u
 sed in neutrino experiments can be used to determine the muon momentum and
  thus their kinetic energy.\n\nĽuboš Krupa\n\nIEAP\, CTU in Prague\, Hus
 ova 240/5\, Prague\, Czech Republic\, Czech Republic
LOCATION:IEAP\, CTU in Prague\, Husova 240/5\, Prague\, Czech Republic\, Cz
 ech Republic
ORGANIZER:andre.sopczak@cern.ch
SEQUENCE:4
SUMMARY:Cuspoid Vavilov-Cherenkov Radiation and Its Application in High-Ene
 rgy and Neutrino Physics
URL;VALUE=URI:https://events.vtools.ieee.org/m/522187
X-ALT-DESC:Description: &lt;br /&gt;&lt;p&gt;When studying the properties of the Vavilo
 v-Cherenkov radiation (VChR) arising from the arbitrary motion of a charge
 d particle in the transparent medium\, using the catastrophe theory\, the 
 existence of a new type of radiation\, the cuspoid VChR\, was predicted. T
 his radiation is a realisation of cuspoid catastrophes in electromagnetic 
 radiation. The radiation can be generated at the non-constant motion of a 
 charged particle in a transparent medium and is emitted at a very narrow s
 olid angle. The radiation is more intensive than ordinary VChR and is gene
 rated only at specific angles\, that depend uniquely on the particle&#39;s mot
 ion in the medium. For this reason\, it could be used to measure particle 
 parameters that determine the motion of a charged particle\, such as momen
 tum and charge. The momenta of charged particles are usually determined in
  magnetic spectrometers. The Lorentz force causes the particles to follow 
 circular or helical trajectories around the direction of the magnetic fiel
 d. The bending radius &lt;em&gt;R&lt;/em&gt; of particle tracks is related to the magn
 etic field strength and the momentum component of the particle perpendicul
 ar to the magnetic field &lt;em&gt;p&lt;/em&gt;&lt;em&gt;trans&lt;/em&gt;. With a suitably focusin
 g optical system\, this allows the reconstruction arc of a ring. In a focu
 sing detector\, the photons can be collected by a spherical mirror with fo
 cal length &lt;em&gt;f&lt;/em&gt; and focused onto the photon detector placed at the f
 ocal plane. The result is an arc of the circle with a radius &lt;em&gt;r&lt;/em&gt;\, 
 independent of the emission point along the particle&#39;s track. The main goa
 l of this work is to study the cuspoid radiation emitted by a charge when 
 it moves in a magnetic field and its application in high-energy physics an
 d neutrino physics. If we use the ring-imaging detection technique\, then 
 we can measure the following parameters using cuspoid radiation: radius &lt;e
 m&gt;r&lt;/em&gt; of the arc of the ring (&lt;em&gt;r &lt;/em&gt;is directly related to &lt;em&gt;p&lt;/
 em&gt;&lt;em&gt;trans&lt;/em&gt;)\, deflection angle &lt;em&gt;&amp;psi\;&lt;/em&gt;\, azimuthal angle &lt;e
 m&gt;&amp;phi\;&lt;/em&gt;\, polar angle &lt;em&gt;&amp;theta\;&lt;/em&gt; and the number of emitted ph
 otons &lt;em&gt;N&lt;/em&gt;&lt;em&gt;cusp&lt;/em&gt;. With the help of these parameters\, it is\,
  in principle\, also possible to determine the position of the vertex\, th
 e origin of particle track in the magnetic field. Cuspoid radiation could 
 be an alternative for measuring the momentum of relativistic particles and
  improve the possibilities of their identification. In many cases\, measur
 ing only electromagnetic radiation (Cherenkov\, cuspoid) will be sufficien
 t to identify a charged particle. Due to the large penetrating power of mu
 ons in materials\, the influence of multiple scattering on its trajectory 
 in a transparent medium placed in a magnetic field can be neglected. Muon 
 detection is an important aspect of neutrino physics and\, therefore\, in 
 our opinion\, measuring the muon momentum using the cuspoid radiation meth
 od can be of significant help in experiments aimed at investigating the pr
 operties of neutrino. The advantage is that the same Ring Imaging Cherenko
 v detectors used in neutrino experiments can be used to determine the muon
  momentum and thus their kinetic energy.&lt;/p&gt;\n&lt;p&gt;Ľubo&amp;scaron\; Krupa&lt;/p&gt;\
 n&lt;p&gt;&amp;nbsp\;&lt;/p&gt;
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