K. Scholberg
Duke University
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Featured researches published by K. Scholberg.
Physical Review Letters | 2003
M. H. Ahn; S. Aoki; Hyoung Chan Bhang; S. Boyd; David William Casper; Jin-Oh Choi; Satoru Fukuda; Y. Fukuda; W. Gajewski; T. Hara; M. Hasegawa; T. Hasegawa; Y. Hayato; J. Hill; Atsushi Ichikawa; A. Ikeda; T. Inagaki; T. Ishida; T. Ishii; M. Ishitsuka; Y. Itow; T. Iwashita; H.I. Jang; J. S. Jang; E. J. Jeon; C. K. Jung; T. Kajita; J. Kameda; K. Kaneyuki; I. Kato
The K2K experiment observes indications of neutrino oscillation: a reduction of nu(mu) flux together with a distortion of the energy spectrum. Fifty-six beam neutrino events are observed in Super-Kamiokande (SK), 250 km from the neutrino production point, with an expectation of 80.1(+6.2)(-5.4). Twenty-nine one ring mu-like events are used to reconstruct the neutrino energy spectrum, which is better matched to the expected spectrum with neutrino oscillation than without. The probability that the observed flux at SK is explained by statistical fluctuation without neutrino oscillation is less than 1%.
New Journal of Physics | 2004
Pietro Antonioli; Richard Tresch Fienberg; F. Fleurot; Y. Fukuda; W. Fulgione; A. Habig; Jaret Heise; A.B. McDonald; C. Mills; T. Namba; Leif J Robinson; K. Scholberg; Michael Schwendener; Roger W. Sinnott; Blake Stacey; Y. Suzuki; Reda Tafirout; C. Vigorito; B. Viren; C.J. Virtue; A. Zichichi
This paper provides a technical description of the SuperNova Early Warning System (SNEWS), an international network of experiments with the goal of providing an early warning of a galactic supernova.
Physical Review D | 2006
K. Scholberg
Rates of coherent neutrino-nucleus elastic scattering at a high-intensity stopped-pion neutrino source in various detector materials (relevant for novel low-threshold detectors) are calculated. Sensitivity of a coherent neutrino-nucleus elastic scattering experiment to new physics is also explored.
Science | 2017
D. Akimov; J. B. Albert; P. An; C. Awe; P.S. Barbeau; B. Becker; V. Belov; A. Brown; A. Bolozdynya; B. Cabrera-Palmer; M. Cervantes; J. I. Collar; R. J. Cooper; R.L. Cooper; C. Cuesta; D.J. Dean; J. A. Detwiler; A. Eberhardt; Y. V. Efremenko; S. R. Elliott; E. M. Erkela; L. Fabris; M. Febbraro; N. Fields; W. Fox; Z. Fu; A. Galindo-Uribarri; M. P. Green; M. Hai; M.R. Heath
A 14.6-kilogram sodium-doped CsI scintillator is used to detect a neutrino scattering process with a 6.7σ confidence level. Nailing down an elusive process Detecting neutrinos—elementary particles that barely interact with other matter—usually requires detectors of enormous size. A particular interaction of neutrinos with atomic nuclei, called the coherent elastic neutrino-nucleus scattering (CEνNS), is predicted to occur with relatively high probability, and it could be used to drastically reduce the size of neutrino detectors. However, observing this interaction requires a source of low-energy neutrinos and detectors that contain nuclei of optimal mass. Akimov et al. observed CEνNS with a 6.7σ confidence by using a comparatively tiny, 14.6-kg sodium-doped CsI scintillator exposed to neutrinos from a spallation neutron facility (see the Perspective by Link). The discovery places tighter bounds on exotic, beyond-the-standard-model interactions involving neutrinos. Science, this issue p. 1123; see also p. 1098 The coherent elastic scattering of neutrinos off nuclei has eluded detection for four decades, even though its predicted cross section is by far the largest of all low-energy neutrino couplings. This mode of interaction offers new opportunities to study neutrino properties and leads to a miniaturization of detector size, with potential technological applications. We observed this process at a 6.7σ confidence level, using a low-background, 14.6-kilogram CsI[Na] scintillator exposed to the neutrino emissions from the Spallation Neutron Source at Oak Ridge National Laboratory. Characteristic signatures in energy and time, predicted by the standard model for this process, were observed in high signal-to-background conditions. Improved constraints on nonstandard neutrino interactions with quarks are derived from this initial data set.
Rivista Del Nuovo Cimento | 2016
Alessandro Mirizzi; Irene Tamborra; H.-Th. Janka; N. Saviano; K. Scholberg; Robert Bollig; Lorenz Hüdepohl; Sovan Chakraborty
Neutrinos play a crucial role in the collapse and explosion of massive stars, governing the infall dynamics of the stellar core, triggering and fueling the explosion and driving the cooling and deleptonization of the newly formed neutron star. Due to their role neutrinos carry information from the heart of the explosion and, due to their weakly interacting nature, offer the only direct probe of the dynamics and thermodynamics at the center of a supernova. In this paper, we review the present status of modelling the neutrino physics and signal formation in collapsing and exploding stars. We assess the capability of current and planned large underground neutrino detectors to yield faithful information of the time and flavor dependent neutrino signal from a future Galactic supernova. We show how the observable neutrino burst would provide a benchmark for fundamental supernova physics with unprecedented richness of detail. Exploiting the treasure of the measured neutrino events requires a careful discrimination of source-generated properties from signal features that originate on the way to the detector. As for the latter, we discuss self-induced flavor conversions associated with neutrino-neutrino interactions that occur in the deepest stellar regions; matter effects that modify the pattern of flavor conversions in the dynamical stellar envelope; neutrino-oscillation signatures that result from structural features associated with the shock-wave propagation as well as turbulent mass motions in post-shock layers. Finally, we highlight our current understanding of the formation of the diffuse supernova neutrino background and we analyse the perspectives for a detection of this relic signal that integrates the contributions from all past core-collapse supernovae in the Universe.
Physical Review D | 2011
Alexander John Anderson; J. M. Conrad; E. Figueroa-Feliciano; K. Scholberg; J. Spitz
Coherent elastic neutrino- and WIMP-nucleus interaction signatures are expected to be quite similar. This paper discusses how a next generation ton-scale dark matter detector could discover neutrino-nucleus coherent scattering, a precisely-predicted Standard Model process. A high intensity pion- and muon- decay-at-rest neutrino source recently proposed for oscillation physics at underground laboratories would provide the neutrinos for these measurements. In this paper, we calculate raw rates for various target materials commonly used in dark matter detectors and show that discovery of this interaction is possible with a 2 ton
Physical Review D | 2012
A. J. Anderson; J. M. Conrad; E. Figueroa-Feliciano; C. Ignarra; G. Karagiorgi; K. Scholberg; M. H. Shaevitz; J. Spitz
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Classical and Quantum Gravity | 2010
I. Leonor; L. Cadonati; E. Coccia; S. D'Antonio; A. Di Credico; V. Fafone; R. Frey; W Fulgione; E. Katsavounidis; Christian D. Ott; G. Pagliaroli; K. Scholberg; E. Thrane; F Vissani
year GEODM exposure in an optimistic energy threshold and efficiency scenario. We also study the effects of the neutrino source on WIMP sensitivity and discuss the modulated neutrino signal as a sensitivity/consistency check between different dark matter experiments at DUSEL. Furthermore, we consider the possibility of coherent neutrino physics with a GEODM module placed within tens of meters of the neutrino source.
Astronomische Nachrichten | 2008
K. Scholberg
Light sterile neutrinos have been introduced as an explanation for a number of oscillation signals at
Nuclear Physics B - Proceedings Supplements | 2002
Th. Siedenburg; C.H. Chung; S. Fopp; M.Fernández García; W. Karpinski; Th. Kirn; K. Lübelsmeyer; J. Orboeck; S. Schael; A. Schultz von Dratzig; G. Schwering; R. Siedling; W. Wallraft; U. Becker; P. Berges; J.D. Burger; P. Fischer; R. Henning; A. Kounine; V. Koutsenko; K. Scholberg; W. De Boer; F. Hauler; L. Jungermann
\Delta m^2 \sim 1