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30 TH I NT E R N AT I ON AL C OSMIC R AY C O N F ER EN C E Search for global asymmetry of UHECR arrival directions with the TUS space detector P. K LI M OV 1 ,O. K AL ASHE V 2 , B . ... Introduction Space-based ultra-high-energy cosmic-ray detectors such as TUS or JEM/EUSO are best suited for searches of the global anisotropies in the distribution of arrival directions of cosmic-ray particles because they provide full-sky coverage with a single experiment. ... Phys. 12, 25 (1999). ... Phys. Lett. ...
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Ссылки http://cosrad.sinp.msu.ru/experiments/tus/doc/global2007.pdf -- 136.8 Кб -- 19.03.2008 Похожие документы
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Anisotropy of Cosmic Rays. Origins, experiments, data analysis problems & methods. ... ANTARES problems and methods. ... 2D» experiments Name Tibet Air Shower Array Position 90.522o E, 30.102o N; 4300 m above sea level 30.11 N, 4300m a.s.l. Gran Sasso, 2000m Caucasus, 1700m (40deg N, 113 deg W), atmospheric depth of 860 gm/cm2 Energy 4,6.2,12,50, 300 TeV Gamma /CR mix Time 1997-1999 TibetII, 1999-2001 TibetIII (bigger HD array). 4 years 1 year Statistics 7x109 in ~1000 days Rate Ang. ...
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Ссылки http://antares.sinp.msu.ru/docs/Anisotropy_2011Bamberg.pdf -- 1353.8 Кб -- 16.12.2013 Похожие документы
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Ссылки http://new.math.msu.su/content_root/programs/kaf/special/terver/2bystr-sokol.doc -- 294.5 Кб -- 10.11.2008 Похожие документы
... 0208, 043 (2002); § S.Alexeyev, D.Starodubtseva, JETP 138, (2010), accepted for October issue Randal-Sundrum 2 Cosmology solutions Black hole solutions 5D bulk equations G AB g 2 AB ( ) A B g A B T 4D brane equations with extra dimensions contribution G g T S 2 4 Black hole solution on the brane dr 2 2 2 ds ( r ) dt r d sin d (r) 2 2 2 2 where ( r ) 1 , н constants, r r 2 2 M / M q/M 2 pl 2 pl q ... Perhaps, the indirect consequences of "tidal charge" could be established in high energy physics....
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