Neutrino Physics 1988
DOI: 10.1007/978-3-642-73679-7_29
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Detection of the Neutrino Signal from SN1987A Using the INR Baksan Underground Scintillation Telescope

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Cited by 29 publications
(34 citation statements)
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“…One possibility for producing a massive dark core without accreting DM from the halo arises if DM particles are produced via bremsstrahlung in a new-born hot neutron star [22,23]. The upper limit on the total mass of exotic particles produced this way arises from the measured neutrino burst of SN 1987A [75][76][77][78][79]. Adopting the 'Raffelt criterion' [80] that χ production should not reduce the duration of the neutrino burst from SN 1987A by more than 50%, we require that the instantaneous χ luminosity should be L χ ≤ 3 × 10 52 ergs s −1 .…”
Section: Constraints On Dark Core Production In Supernovaementioning
confidence: 99%
“…One possibility for producing a massive dark core without accreting DM from the halo arises if DM particles are produced via bremsstrahlung in a new-born hot neutron star [22,23]. The upper limit on the total mass of exotic particles produced this way arises from the measured neutrino burst of SN 1987A [75][76][77][78][79]. Adopting the 'Raffelt criterion' [80] that χ production should not reduce the duration of the neutrino burst from SN 1987A by more than 50%, we require that the instantaneous χ luminosity should be L χ ≤ 3 × 10 52 ergs s −1 .…”
Section: Constraints On Dark Core Production In Supernovaementioning
confidence: 99%
“…The dependence of the final results on the different models of progenitor stars, neutrino flavor conversions and the relevant backgrounds is also discussed.In the paradigm of the delayed neutrino-driven supernova (SN) explosions, massive stars heavier than (8 · · · 10) solar masses will end their lives as core-collapse SNe by emitting a huge number of neutrinos of tens of MeV energies, which carry away most of the released gravitational binding energy of 3 × 10 53 erg [1,2]. The successful detection of neutrinos from SN 1987A in Kamiokande-II [3], IMB [4] and Baksan [5] experiments has provided a strong support for this overall picture of core-collapse SNe.Even prior to the core collapse, the evolved massive stars are experiencing significant neutrino emission, which is actually the most efficient mechanism of cooling after the phase of helium burning [6,7]. In the stellar environment, where both the matter density and the temperature may span quite a wide range, neutrinos are primarily produced in pairs by the plasma process γ * → ν + ν, the photo process γ + e − → e − + ν + ν, the pair process e + + e − → ν + ν and the bremsstrahlung e − + Ze → e − + Ze + ν + ν, where Ze stands for the heavy nuclei with the atomic number Z and ν (ν) denotes neutrinos (antineutrinos) of all three flavors [8][9][10][11][12][13][14].…”
mentioning
confidence: 99%
“…The facility has been operating under the program of search for collapse neutrinos since the mid-1980 [7]. The observation time is T = 24.7 years.…”
Section: Resultsmentioning
confidence: 99%