نتایج جستجو برای: neutrino detection

تعداد نتایج: 586258  

2009
Michele Maltoni Walter Winter

We discuss the interplay of neutrino oscillation and decay properties at neutrino telescopes. Motivated by recent unparticle scenarios, which open the possibility of new neutrino decay modes over astrophysical distances, we perform a complete classification of possible decay schemes, and we illustrate how different scenarios can be identified. Moreover, we show that the sensitivity of neutrino ...

2008
G. M. A. Lim

Relic neutralinos produced after the Big Bang are favoured candidates for Dark Matter. They can accumulate at the centre of massive celestial objects like our Sun. Their annihilation can result in a high-energy neutrino flux that could be detectable as a localised emission with earthbased neutrino telescopes like ANTARES. In this paper a brief overview of the prospects of the indirect search fo...

2007
F. Boehm J. Hanson H. Henrikson D. Michael V. M. Novikov A. Piepke P. Vogel S. Yang G. Gratta L. Miller D. Tracy Y. F. Wang

Our collaboration has installed a long baseline neutrino oscillation experiment at the Palo Verde Nuclear Generating Station in Arizona. 12 tons of Gd loaded liquid scintillator, in a segmented detector, are used to search for e $ x oscillations at 740 m distance to three reactors. The anti-neutrino capture on the proton serves as detection reaction. The experiment is expected reach a sensitivi...

2011
B Beltran H Bichsel B Cai G A Cox H Deng J Detwiler J A Formaggio S Habib A L Hallin A Hime M Huang C Kraus H R Leslie J C Loach R Martin S McGee M L Miller B Monreal J Monroe N S Oblath S J M Peeters A W P Poon G Prior K Rielage R G H Robertson M W E Smith L C Stonehill N Tolich T Van Wechel H Wan Chan Tseung J Wendland J F Wilkerson

The third phase of the Sudbury Neutrino Observatory (SNO) experiment added an array of 3He proportional counters to the detector. The purpose of this neutral-current detection (NCD) array was to observe neutrons resulting from neutral-current solar-neutrino–deuteron interactions. We have developed a detailed simulation of current pulses from NCD array proportional counters, from the primary neu...

2006
S. Mikheyev

The Baikal Neutrino Telescope has been operating in its NT200 configuration since April, 1998. The telescope has been upgraded in April, 2005 to the 10Mton scale detector NT200+. It’s main physics goal is the detection of signals from high energy neutrino cascades. NT200+ reaches a 3-year sensitivity of 2 × 10cmssrGeV for an all-flavor diffuse cosmic E neutrino flux for energies 10 TeV ÷ 10 TeV...

Journal: :Physical review. C, Nuclear physics 1996
Kim Schramm Horowitz

Neutrino-nucleus cross sections for the detection of atmospheric neutrinos are calculated in relativistic impulse and random phase approximations. Pion production is estimated via inclusive ∆hole nuclear excitations. The number of pion events can confuse the identification of the neutrino flavor. As a further source of pions we calculate coherent pion production (where the nucleus remains in th...

2003
Carlo Giunti

We review critically the main assumptions on which the standard theory of neutrino oscillations is based. We show that all assumptions are realistic, except the so-called “equal momentum assumption”, which however is irrelevant. We briefly review the covariant plane-wave derivation of neutrino oscillations and a quantum field theoretical wave packet model of neutrino oscillations. We show that ...

2000
A. Cervera

The precision and discovery potential of a neutrino factory based on muon storage rings is summarized. For three-family neutrino oscillations, we analyze how to measure or severely constraint the angle θ13, CP violation, MSW effects and the sign of the atmospheric mass difference ∆m223. The appearance of “wrong-sign muons” at three reference baselines is considered: 732 km, 3500 km and 7332 km....

2003
Alexander Kusenko

Two astrophysical puzzles, the origin of pulsar velocities and that of dark matter, may have a simultaneous explanation if there exists a sterile neutrino with a mass in the 1–20 keV range and a small mixing (sin θ ∼ 10) with the electron neutrino. Although the mixing is too small for direct detection, future observations of the X-ray telescopes, as well as the gravity waves detectors, such as ...

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