M. Green - The PROSPECT Collaboration

M. Green
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M. Green
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The PROSPECT Collaboration
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Physics - Instrumentation and Detectors (25)
 
Nuclear Experiment (23)
 
High Energy Physics - Experiment (11)
 
High Energy Physics - Theory (6)
 
Physics - Strongly Correlated Electrons (5)
 
Physics - Materials Science (4)
 
Solar and Stellar Astrophysics (3)
 
Physics - Superconductivity (3)
 
Mathematics - Mathematical Physics (2)
 
Mathematical Physics (2)
 
Mathematics - Algebraic Topology (2)
 
Physics - Other (2)
 
High Energy Physics - Phenomenology (1)
 
Physics - Mesoscopic Systems and Quantum Hall Effect (1)
 
General Relativity and Quantum Cosmology (1)
 
Mathematics - Algebraic Geometry (1)
 
Physics - Classical Physics (1)
 
Physics - Biological Physics (1)
 
Computer Science - Cryptography and Security (1)
 
Quantum Physics (1)
 
Mathematics - Rings and Algebras (1)
 
Mathematics - Quantum Algebra (1)
 
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Publications Authored By M. Green

We introduce and study ternary $f$-distributive structures, Ternary $f$-quandles and more generally their higher $n$-ary analogues. A classification of ternary $f$-quandles is provided in low dimensions. Moreover, we study extension theory and introduce a cohomology theory for ternary, and more generally $n$-ary, $f$-quandles. Read More

The Fe1+xTe phase diagram consists of two distinct magnetic structures with collinear order present at low interstitial iron concentrations and a helical phase at large values of x with these phases separated by a Lifshitz point. We use unpolarized single crystal diffraction to confirm the helical phase for large interstitial iron concentrations and polarized single crystal diffraction to demonstrate the collinear order for the iron deficient side of the Fe1+xTe phase diagram. Polarized neutron inelastic scattering show that the fluctuations associated with this collinear order are predominately transverse at low energy transfers, consistent with a localized magnetic moment picture. Read More

Attacks on the microarchitecture of modern processors have become a practical threat to security and privacy in desktop and cloud computing. Recently, cache attacks have successfully been demonstrated on ARM based mobile devices, suggesting they are as vulnerable as their desktop or server counterparts. In this work, we show that previous literature might have left an overly pessimistic conclusion of ARM's security as we unveil AutoLock: an internal performance enhancement found in inclusive cache levels of ARM processors that adversely affects Evict+Time, Prime+Probe, and Evict+Reload attacks. Read More

2017Feb
Affiliations: 1University of Warwick, UK, 2University of Warwick, UK, 3University of Warwick, UK, 4University of Warwick, UK, 5University of Warwick, UK, 6University of Warwick, UK, 7University of Warwick, UK, 8Hubble Fellow, University of North Carolina, Chapel Hill, USA, 9University of Warwick, UK, 10Universidad de Valparaíso, Chile, 11Universidad de Valparaíso, Chile, 12Universidad de Antofagasta, Chile, 13Universitat Politècnica de Catalunya, Spain

An observational constraint on the contribution of double degenerates to Type Ia supernovae requires multiple radial velocity measurements of ideally thousands of white dwarfs. This is because only a small fraction of the double degenerate population is massive enough, with orbital periods short enough, to be considered viable Type Ia progenitors. We show how the radial velocity information available from public surveys such as the Sloan Digital Sky Survey can be used to pre-select targets for variability, leading to a ten-fold reduction in observing time required compared to an unranked or random survey. Read More

The crystal and magnetic structures of stoichiometric ZnCr2Se4 have been investigated using synchrotron X-ray and neutron powder diffraction, muon spin relaxation (muSR) and inelastic neutron scattering. Synchrotron X-ray diffraction shows a spin-lattice distortion from the cubic spinel to a tetragonal I41/amd lattice below TN = 21 K, where powder neutron diffraction confirms the formation of a helical magnetic structure with magnetic moment of 3.04(3) {\mu}B at 1. Read More

2016Dec
Affiliations: 1California Institute of Technology, 2Radboud University Nijmegen, 3University of California, Santa Barbara, 4University of Tuebingen, 5University of Warwick, 6Radboud University Nijmegen, 7Radboud University Nijmegen, 8California Institute of Technology, 9California Institute of Technology, 10University of Erlangen-Nuremberg, 11University of California, Santa Barbara, 12Northwestern University, 13University of Sheffield, 14University of Sheffield, 15University of Warwick, 16National Astronomical Research Institute of Thailand, 17Spitzer Science Center, Caltech, 18University of Sheffield, 19Infrared Processing and Analysis Center, Caltech, 20California Institute of Technology, 21University of Sheffield, 22University of Cambridge

We present the discovery of the hot subdwarf B star (sdB) binary PTF1 J082340.04+081936.5. Read More

We present new limits on exotic keV-scale physics based on 478 kg d of MAJORANA DEMONSTRATOR commissioning data. Constraints at the 90% confidence level are derived on bosonic dark matter (DM) and solar axion couplings, Pauli exclusion principle violating (PEPV) decay, and electron decay using monoenergetic peak signal-limits above our background. Our most stringent DM constraints are set for 11. Read More

Confluent populations of elongated cells give rise to ordered patterns seen in nematic phase liquid crystals. We correlate cell elongation and intercellular distance with intercellular alignment using an amorphous spin glass model. We compare in vitro time-lapse imaging with Monte Carlo simulation results by framing a novel hard ellipses model in terms of Boltzmann statistics. Read More

A search for Pauli-exclusion-principle-violating K-alpha electron transitions was performed using 89.5 kg-d of data collected with a p-type point contact high-purity germanium detector operated at the Kimballton Underground Research Facility. A lower limit on the transition lifetime of 5. Read More

The Majorana Demonstrator searches for neutrinoless double-beta decay of $^{76}$Ge using arrays of high-purity germanium detectors. If observed, this process would demonstrate that lepton number is not a conserved quantity in nature, with implications for grand-unification and for explaining the predominance of matter over antimatter in the universe. A problematic background in such large granular detector arrays is posed by alpha particles. Read More

An oscillator design based on a periodic, double ladder resonant circuit is proposed. The circuit exhibits a degenerate band edge (DBE) in the dispersion diagram of its phase-frequency eigenstates, and possesses unique resonance features associated with a high Q-factor resonance, compared to a single ladder or a conventional LC tank circuit. This oscillator is shown to have an oscillation threshold that is half that of a single LC ladder circuit having the same total quality factor, and thus is more robust than an LC oscillator in the presence of losses. Read More

Neutrinoless double-beta decay searches seek to determine the nature of neutrinos, the existence of a lepton violating process, and the effective Majorana neutrino mass. The {\sc Majorana} Collaboration is assembling an array of high purity Ge detectors to search for neutrinoless double-beta decay in $^{76}$Ge. The {\sc Majorana Demonstrator} is composed of 44. Read More

The MAJORANA Collaboration is constructing a system containing 44 kg of high-purity Ge (HPGe) detectors to demonstrate the feasibility and potential of a future tonne-scale experiment capable of probing the neutrino mass scale to ~15 meV. To realize this, a major goal of the MAJORANA DEMONSTRATOR is to demonstrate a path forward to achieving a background rate at or below 1 count/(ROI-t-y) in the 4 keV region of interest (ROI) around the Q-value at 2039 keV. This goal is pursued through a combination of a significant reduction of radioactive impurities in construction materials and analytical methods for background rejection, for example using powerful pulse shape analysis techniques profiting from the p-type point contact HPGe detectors technology. Read More

The famous Stern-Gerlach experiment has played an important role in our understanding of quantum behavior. We propose a modified Stern-Gerlach experiment in which the magnetic field is in a superposition of two opposite directions. We find that incident spin-1/2 particles through the field yield a discrete target distribution with crucial differences compared to the classical Stern-Gerlach case. Read More

CaFe$_{2}$O$_{4}$ is a $S={5\over 2}$ anisotropic antiferromagnet based upon zig-zag chains having two competing magnetic structures, denoted as the A ($\uparrow \uparrow \downarrow \downarrow$) and B ($\uparrow \downarrow \uparrow \downarrow$) phases, which differ by the $c$-axis stacking of ferromagnetic stripes. We apply neutron scattering to demonstrate that the competing A and B phase order parameters results in magnetic antiphase boundaries along $c$ which freeze on the timescale of $\sim$ 1 ns at the onset of magnetic order at 200 K. Using high resolution neutron spectroscopy, we find quantized spin wave levels and measure 9 such excitations localized in regions $\sim$ 1-2 $c$-axis lattice constants in size. Read More

The purpose of this paper is to introduce and study the notions of $f$-rack and $f$-quandle which are obtained by twisting the usual equational identities by a map. We provide some key constructions, examples and classification of low order $f$-quandles. Moreover, we define modules over $f$-racks, discuss extensions and define a cohomology complex for $f$-quandles. Read More

Birnessite compounds are stable across a wide range of compositions that produces a remarkable diversity in their physical, electrochemical and functional properties. These are hydrated analogues of the magnetically frustrated, mixed-valent manganese oxide structures, with general formula, NaxMnO2. Here we demonstrate that the direct hydration of layered rock-salt type a-NaMnO2, with the geometrically frustrated triangular lattice topology, yields the birnessite type oxide, Na0. Read More

We present the first corpus annotated with preposition supersenses, unlexicalized categories for semantic functions that can be marked by English prepositions (Schneider et al., 2015). That scheme improves upon its predecessors to better facilitate comprehensive manual annotation. Read More

This paper investigates relationships between low-energy four-particle scattering amplitudes with external gauge particles and gravitons in the E_8 X E_8 and SO(32) heterotic string theories and the type I and type IA superstring theories by considering a variety of tree level and one-loop Feynman diagrams describing such amplitudes in eleven-dimensional supergravity in a Horava--Witten background compactified on a circle. This accounts for a number of perturbative and non-perturbative aspects of low order higher derivative terms in the low-energy expansion of string theory amplitudes, which are expected to be protected by half maximal supersymmetry from receiving corrections beyond one or two loops. It also suggests the manner in which type I/heterotic duality may be realised for certain higher derivative interactions that are not so obviously protected. Read More

The MAJORANA Collaboration is constructing the MAJORANA Demonstrator, an ultra-low background, 44-kg modular high-purity Ge (HPGe) detector array to search for neutrinoless double-beta decay in Ge-76. The phenomenon of surface micro-discharge induced by high-voltage has been studied in the context of the MAJORANA Demonstrator. This effect can damage the front-end electronics or mimic detector signals. Read More

This paper investigates the relations between modular graph forms, which are generalizations of the modular graph functions that were introduced in earlier papers motivated by the structure of the low energy expansion of genus-one Type II superstring amplitudes. These modular graph forms are multiple sums associated with decorated Feynman graphs on the world-sheet torus. The action of standard differential operators on these modular graph forms admits an algebraic representation on the decorations. Read More

2016Feb
Affiliations: 1The Majorana Collaboration, 2The Majorana Collaboration, 3The Majorana Collaboration, 4The Majorana Collaboration, 5The Majorana Collaboration, 6The Majorana Collaboration, 7The Majorana Collaboration, 8The Majorana Collaboration, 9The Majorana Collaboration, 10The Majorana Collaboration, 11The Majorana Collaboration, 12The Majorana Collaboration, 13The Majorana Collaboration, 14The Majorana Collaboration, 15The Majorana Collaboration, 16The Majorana Collaboration, 17The Majorana Collaboration, 18The Majorana Collaboration, 19The Majorana Collaboration, 20The Majorana Collaboration, 21The Majorana Collaboration, 22The Majorana Collaboration, 23The Majorana Collaboration, 24The Majorana Collaboration, 25The Majorana Collaboration, 26The Majorana Collaboration, 27The Majorana Collaboration, 28The Majorana Collaboration, 29The Majorana Collaboration, 30The Majorana Collaboration, 31The Majorana Collaboration, 32The Majorana Collaboration, 33The Majorana Collaboration, 34The Majorana Collaboration, 35The Majorana Collaboration, 36The Majorana Collaboration, 37The Majorana Collaboration, 38The Majorana Collaboration, 39The Majorana Collaboration, 40The Majorana Collaboration, 41The Majorana Collaboration, 42The Majorana Collaboration, 43The Majorana Collaboration, 44The Majorana Collaboration, 45The Majorana Collaboration, 46The Majorana Collaboration, 47The Majorana Collaboration, 48The Majorana Collaboration, 49The Majorana Collaboration, 50The Majorana Collaboration, 51The Majorana Collaboration, 52The Majorana Collaboration, 53The Majorana Collaboration, 54The Majorana Collaboration, 55The Majorana Collaboration, 56The Majorana Collaboration, 57The Majorana Collaboration, 58The Majorana Collaboration, 59The Majorana Collaboration, 60The Majorana Collaboration, 61The Majorana Collaboration, 62The Majorana Collaboration, 63The Majorana Collaboration, 64The Majorana Collaboration, 65The Majorana Collaboration, 66The Majorana Collaboration, 67The Majorana Collaboration, 68The Majorana Collaboration, 69The Majorana Collaboration, 70The Majorana Collaboration, 71The Majorana Collaboration, 72The Majorana Collaboration, 73The Majorana Collaboration, 74The Majorana Collaboration

We report the first measurement of the total MUON flux underground at the Davis Campus of the Sanford Underground Research Facility at the 4850 ft level. Measurements were done with the Majorana Demonstrator veto system arranged in two different configurations. The measured total flux is (5. Read More

The MAJORANA collaboration is constructing the MAJORANA DEMONSTATOR at the Sanford Underground Research Facility at the Homestake gold mine, in Lead, SD. The apparatus will use Ge detectors, enriched in isotope \nuc{76}{Ge}, to demonstrate the feasibility of a large-scale Ge detector experiment to search for neutrinoless double beta decay. The long half-life of this postulated process requires that the apparatus be extremely low in radioactive isotopes whose decays may produce backgrounds to the search. Read More

In earlier work we studied features of non-holomorphic modular functions associated with Feynman graphs for a conformal scalar field theory on a two-dimensional torus with zero external momenta at all vertices. Such functions, which we will refer to as modular graph functions, arise, for example, in the low energy expansion of genus-one Type II superstring amplitudes. We here introduce a class of single-valued elliptic multiple polylogarithms, which are defined as elliptic functions associated with Feynman graphs with vanishing external momenta at all but two vertices. Read More

The Precision Reactor Oscillation and Spectrum Experiment, PROSPECT, is designed to make a precise measurement of the antineutrino spectrum from a highly-enriched uranium reactor and probe eV-scale sterile neutrinos by searching for neutrino oscillations over meter-long distances. PROSPECT is conceived as a 2-phase experiment utilizing segmented $^6$Li-doped liquid scintillator detectors for both efficient detection of reactor antineutrinos through the inverse beta decay reaction and excellent background discrimination. PROSPECT Phase I consists of a movable 3-ton antineutrino detector at distances of 7 - 12 m from the reactor core. Read More

Neutrinoless double beta decay searches play a major role in determining neutrino properties, in particular the Majorana or Dirac nature of the neutrino and the absolute scale of the neutrino mass. The consequences of these searches go beyond neutrino physics, with implications for Grand Unification and leptogenesis. The \textsc{Majorana} Collaboration is assembling a low-background array of high purity Germanium (HPGe) detectors to search for neutrinoless double-beta decay in $^{76}$Ge. Read More

The COHERENT collaboration's primary objective is to measure coherent elastic neutrino-nucleus scattering (CEvNS) using the unique, high-quality source of tens-of-MeV neutrinos provided by the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory (ORNL). In spite of its large cross section, the CEvNS process has never been observed, due to tiny energies of the resulting nuclear recoils which are out of reach for standard neutrino detectors. The measurement of CEvNS has now become feasible, thanks to the development of ultra-sensitive technology for rare decay and weakly-interacting massive particle (dark matter) searches. Read More

The coefficients of the higher-derivative terms in the low energy expansion of genus-one graviton Type II superstring scattering amplitudes are determined by integrating sums of non-holomorphic modular functions over the complex structure modulus of a torus. In the case of the four-graviton amplitude, each of these modular functions is a multiple sum associated with a Feynman diagram for a free massless scalar field on the torus. The lines in each diagram join pairs of vertex insertion points and the number of lines defines its weight $w$, which corresponds to its order in the low energy expansion. Read More

2015Aug
Affiliations: 1The PROSPECT Collaboration, 2The PROSPECT Collaboration, 3The PROSPECT Collaboration, 4The PROSPECT Collaboration, 5The PROSPECT Collaboration, 6The PROSPECT Collaboration, 7The PROSPECT Collaboration, 8The PROSPECT Collaboration, 9The PROSPECT Collaboration, 10The PROSPECT Collaboration, 11The PROSPECT Collaboration, 12The PROSPECT Collaboration, 13The PROSPECT Collaboration, 14The PROSPECT Collaboration, 15The PROSPECT Collaboration, 16The PROSPECT Collaboration, 17The PROSPECT Collaboration, 18The PROSPECT Collaboration, 19The PROSPECT Collaboration, 20The PROSPECT Collaboration, 21The PROSPECT Collaboration, 22The PROSPECT Collaboration, 23The PROSPECT Collaboration, 24The PROSPECT Collaboration, 25The PROSPECT Collaboration, 26The PROSPECT Collaboration, 27The PROSPECT Collaboration, 28The PROSPECT Collaboration, 29The PROSPECT Collaboration, 30The PROSPECT Collaboration, 31The PROSPECT Collaboration, 32The PROSPECT Collaboration, 33The PROSPECT Collaboration, 34The PROSPECT Collaboration, 35The PROSPECT Collaboration, 36The PROSPECT Collaboration, 37The PROSPECT Collaboration, 38The PROSPECT Collaboration, 39The PROSPECT Collaboration, 40The PROSPECT Collaboration, 41The PROSPECT Collaboration, 42The PROSPECT Collaboration, 43The PROSPECT Collaboration, 44The PROSPECT Collaboration, 45The PROSPECT Collaboration, 46The PROSPECT Collaboration, 47The PROSPECT Collaboration, 48The PROSPECT Collaboration, 49The PROSPECT Collaboration, 50The PROSPECT Collaboration, 51The PROSPECT Collaboration, 52The PROSPECT Collaboration, 53The PROSPECT Collaboration, 54The PROSPECT Collaboration, 55The PROSPECT Collaboration, 56The PROSPECT Collaboration, 57The PROSPECT Collaboration, 58The PROSPECT Collaboration, 59The PROSPECT Collaboration, 60The PROSPECT Collaboration, 61The PROSPECT Collaboration, 62The PROSPECT Collaboration, 63The PROSPECT Collaboration, 64The PROSPECT Collaboration, 65The PROSPECT Collaboration, 66The PROSPECT Collaboration

A meter-long, 23-liter EJ-309 liquid scintillator detector has been constructed to study the light collection and pulse-shape discrimination performance of elongated scintillator cells for the PROSPECT reactor antineutrino experiment. The magnitude and uniformity of light collection and neutron/gamma discrimination power in the energy range of antineutrino inverse beta decay products have been studied using gamma and spontaneous fission calibration sources deployed along the cell long axis. We also study neutron-gamma discrimination and light collection abilities for differing PMT and reflector configurations. Read More

The MAJORANA Collaboration is constructing the MAJORANA DEMONSTRATOR, an ultra-low background, modular, HPGe detector array with a mass of 44-kg (29 kg 76Ge and 15 kg natGe) to search for neutrinoless double beta decay in Ge-76. The next generation of tonne-scale Ge-based neutrinoless double beta decay searches will probe the neutrino mass scale in the inverted-hierarchy region. The MAJORANA DEMONSTRATOR is envisioned to demonstrate a path forward to achieve a background rate at or below 1 count/tonne/year in the 4 keV region of interest around the Q-value of 2039 keV. Read More

The MAJORANA Collaboration will seek neutrinoless double beta decay (0nbb) in 76Ge using isotopically enriched p-type point contact (PPC) high purity Germanium (HPGe) detectors. A tonne-scale array of HPGe detectors would require background levels below 1 count/ROI-tonne-year in the 4 keV region of interest (ROI) around the 2039 keV Q-value of the decay. In order to demonstrate the feasibility of such an experiment, the MAJORANA DEMONSTRATOR, a 40 kg HPGe detector array, is being constructed with a background goal of <3 counts/ROI-tonne-year, which is expected to scale down to <1 count/ROI-tonne-year for a tonne-scale experiment. Read More

2015Jun
Affiliations: 1The PROSPECT Collaboration, 2The PROSPECT Collaboration, 3The PROSPECT Collaboration, 4The PROSPECT Collaboration, 5The PROSPECT Collaboration, 6The PROSPECT Collaboration, 7The PROSPECT Collaboration, 8The PROSPECT Collaboration, 9The PROSPECT Collaboration, 10The PROSPECT Collaboration, 11The PROSPECT Collaboration, 12The PROSPECT Collaboration, 13The PROSPECT Collaboration, 14The PROSPECT Collaboration, 15The PROSPECT Collaboration, 16The PROSPECT Collaboration, 17The PROSPECT Collaboration, 18The PROSPECT Collaboration, 19The PROSPECT Collaboration, 20The PROSPECT Collaboration, 21The PROSPECT Collaboration, 22The PROSPECT Collaboration, 23The PROSPECT Collaboration, 24The PROSPECT Collaboration, 25The PROSPECT Collaboration, 26The PROSPECT Collaboration, 27The PROSPECT Collaboration, 28The PROSPECT Collaboration, 29The PROSPECT Collaboration, 30The PROSPECT Collaboration, 31The PROSPECT Collaboration, 32The PROSPECT Collaboration, 33The PROSPECT Collaboration, 34The PROSPECT Collaboration, 35The PROSPECT Collaboration, 36The PROSPECT Collaboration, 37The PROSPECT Collaboration, 38The PROSPECT Collaboration, 39The PROSPECT Collaboration, 40The PROSPECT Collaboration, 41The PROSPECT Collaboration, 42The PROSPECT Collaboration, 43The PROSPECT Collaboration, 44The PROSPECT Collaboration, 45The PROSPECT Collaboration, 46The PROSPECT Collaboration, 47The PROSPECT Collaboration, 48The PROSPECT Collaboration, 49The PROSPECT Collaboration, 50The PROSPECT Collaboration, 51The PROSPECT Collaboration, 52The PROSPECT Collaboration, 53The PROSPECT Collaboration, 54The PROSPECT Collaboration, 55The PROSPECT Collaboration, 56The PROSPECT Collaboration, 57The PROSPECT Collaboration, 58The PROSPECT Collaboration, 59The PROSPECT Collaboration, 60The PROSPECT Collaboration, 61The PROSPECT Collaboration

Research reactors host a wide range of activities that make use of the intense neutron fluxes generated at these facilities. Recent interest in performing measurements with relatively low event rates, e.g. Read More

The MAJORANA Collaboration is constructing the MAJORANA DEMONSTRATOR, an ultra-low background, 40-kg modular HPGe detector array to search for neutrinoless double beta decay in 76Ge. In view of the next generation of tonne-scale Ge-based 0nbb-decay searches that will probe the neutrino mass scale in the inverted-hierarchy region, a major goal of the MAJORANA DEMONSTRATOR is to demonstrate a path forward to achieving a background rate at or below 1 count/tonne/year in the 4 keV region of interest around the Q-value at 2039 keV. The background rejection techniques to be applied to the data include cuts based on data reduction, pulse shape analysis, event coincidences, and time correlations. Read More

Interactions between atomic and molecular objects are to a large extent defined by the nanoscale electrostatic potentials which these objects produce. We introduce a scanning probe technique that enables three-dimensional imaging of local electrostatic potential fields with sub-nanometer resolution. Registering single electron charging events of a molecular quantum dot attached to the tip of a (qPlus tuning fork) atomic force microscope operated at 5 K, we quantitatively measure the quadrupole field of a single molecule and the dipole field of a single metal adatom, both adsorbed on a clean metal surface. Read More

2015Mar
Authors: C. Adams, J. R. Alonso, A. M. Ankowski, J. A. Asaadi, J. Ashenfelter, S. N. Axani, K. Babu, C. Backhouse, H. R. Band, P. S. Barbeau, N. Barros, A. Bernstein, M. Betancourt, M. Bishai, E. Blucher, J. Bouffard, N. Bowden, S. Brice, C. Bryan, L. Camilleri, J. Cao, J. Carlson, R. E. Carr, A. Chatterjee, M. Chen, S. Chen, M. Chiu, E. D. Church, J. I. Collar, G. Collin, J. M. Conrad, M. R. Convery, R. L. Cooper, D. Cowen, H. Davoudiasl, A. De Gouvea, D. J. Dean, G. Deichert, F. Descamps, T. DeYoung, M. V. Diwan, Z. Djurcic, M. J. Dolinski, J. Dolph, B. Donnelly, D. A. Dwyer, S. Dytman, Y. Efremenko, L. L. Everett, A. Fava, E. Figueroa-Feliciano, B. Fleming, A. Friedland, B. K. Fujikawa, T. K. Gaisser, M. Galeazzi, D. C. Galehouse, A. Galindo-Uribarri, G. T. Garvey, S. Gautam, K. E. Gilje, M. Gonzalez-Garcia, M. C. Goodman, H. Gordon, E. Gramellini, M. P. Green, A. Guglielmi, R. W. Hackenburg, A. Hackenburg, F. Halzen, K. Han, S. Hans, D. Harris, K. M. Heeger, M. Herman, R. Hill, A. Holin, P. Huber, D. E. Jaffe, R. A. Johnson, J. Joshi, G. Karagiorgi, L. J. Kaufman, B. Kayser, S. H. Kettell, B. J. Kirby, J. R. Klein, Yu. G. Kolomensky, R. M. Kriske, C. E. Lane, T. J. Langford, A. Lankford, K. Lau, J. G. Learned, J. Ling, J. M. Link, D. Lissauer, L. Littenberg, B. R. Littlejohn, S. Lockwitz, M. Lokajicek, W. C. Louis, K. Luk, J. Lykken, W. J. Marciano, J. Maricic, D. M. Markoff, D. A. Martinez Caicedo, C. Mauger, K. Mavrokoridis, E. McCluskey, D. McKeen, R. McKeown, G. Mills, I. Mocioiu, B. Monreal, M. R. Mooney, J. G. Morfin, P. Mumm, J. Napolitano, R. Neilson, J. K. Nelson, M. Nessi, D. Norcini, F. Nova, D. R. Nygren, G. D. Orebi Gann, O. Palamara, Z. Parsa, R. Patterson, P. Paul, A. Pocar, X. Qian, J. L. Raaf, R. Rameika, G. Ranucci, H. Ray, D. Reyna, G. C. Rich, P. Rodrigues, E. Romero Romero, R. Rosero, S. D. Rountree, B. Rybolt, M. C. Sanchez, G. Santucci, D. Schmitz, K. Scholberg, D. Seckel, M. Shaevitz, R. Shrock, M. B. Smy, M. Soderberg, A. Sonzogni, A. B. Sousa, J. Spitz, J. M. St. John, J. Stewart, J. B. Strait, G. Sullivan, R. Svoboda, A. M. Szelc, R. Tayloe, M. A. Thomson, M. Toups, A. Vacheret, M. Vagins, R. G. Van de Water, R. B. Vogelaar, M. Weber, W. Weng, M. Wetstein, C. White, B. R. White, L. Whitehead, D. W. Whittington, M. J. Wilking, R. J. Wilson, P. Wilson, D. Winklehner, D. R. Winn, E. Worcester, L. Yang, M. Yeh, Z. W. Yokley, J. Yoo, B. Yu, J. Yu, C. Zhang

The US neutrino community gathered at the Workshop on the Intermediate Neutrino Program (WINP) at Brookhaven National Laboratory February 4-6, 2015 to explore opportunities in neutrino physics over the next five to ten years. Scientists from particle, astroparticle and nuclear physics participated in the workshop. The workshop examined promising opportunities for neutrino physics in the intermediate term, including possible new small to mid-scale experiments, US contributions to large experiments, upgrades to existing experiments, R&D plans and theory. Read More

The analytic contribution to the low energy expansion of Type II string amplitudes at genus-one is a power series in space-time derivatives with coefficients that are determined by integrals of modular functions over the complex structure modulus of the world-sheet torus. These modular functions are associated with world-sheet vacuum Feynman diagrams and given by multiple sums over the discrete momenta on the torus. In this paper we exhibit exact differential and algebraic relations for a certain infinite class of such modular functions by showing that they satisfy Laplace eigenvalue equations with inhomogeneous terms that are polynomial in non-holomorphic Eisenstein series. Read More

The MAJORANA DEMONSTRATOR is a planned 40 kg array of Germanium detectors intended to demonstrate the feasibility of constructing a tonne-scale experiment that will seek neutrinoless double beta decay ($0\nu\beta\beta$) in $^{76}\mathrm{Ge}$. Such an experiment would require backgrounds of less than 1 count/tonne-year in the 4 keV region of interest around the 2039 keV Q-value of the $\beta\beta$ decay. Designing low-noise electronics, which must be placed in close proximity to the detectors, presents a challenge to reaching this background target. Read More

The goal of the \textsc{Majorana} \textsc{Demonstrator} project is to search for 0$\nu\beta\beta$ decay in $^{76}\mathrm{Ge}$. Of all candidate isotopes for 0$\nu\beta\beta$, $^{76}\mathrm{Ge}$ has some of the most favorable characteristics. Germanium detectors are a well established technology, and in searches for 0$\nu\beta\beta$, the high purity germanium crystal acts simultaneously as source and detector. Read More

2015Feb
Affiliations: 1Lawrence Berkeley National Laboratory, 2Pacific Northwest National Laboratory, 3University of South Carolina, 4Institute for Theoretical and Experimental Physics, 5Oak Ridge National Laboratory, 6Joint Institute for Nuclear Research, 7Duke University, 8University of South Dakota, 9South Dakota School of Mines and Technology, 10Lawrence Berkeley National Laboratory, 11South Dakota School of Mines and Technology, 12North Carolina State University, 13Center for Experimental Nuclear Physics and Astrophysics and University of Washington, 14Center for Experimental Nuclear Physics and Astrophysics and University of Washington, 15Center for Experimental Nuclear Physics and Astrophysics and University of Washington, 16University of Tennessee, 17Joint Institute for Nuclear Research, 18Osaka University, 19Los Alamos National Laboratory, 20Duke University, 21Pacific Northwest National Laboratory, 22University of North Carolina, 23University of North Carolina, 24Oak Ridge National Laboratory, 25University of North Carolina, 26Los Alamos National Laboratory, 27Oak Ridge National Laboratory, 28Center for Experimental Nuclear Physics and Astrophysics and University of Washington, 29University of South Carolina, 30Joint Institute for Nuclear Research, 31University of Alberta, 32Osaka University, 33Lawrence Berkeley National Laboratory, 34University of North Carolina, 35Pacific Northwest National Laboratory, 36South Dakota School of Mines and Technology, 37University of North Carolina, 38Black Hills State University, 39Tennessee Tech University, 40Joint Institute for Nuclear Research, 41Institute for Theoretical and Experimental Physics, 42Pacific Northwest National Laboratory, 43Osaka University, 44Center for Experimental Nuclear Physics and Astrophysics and University of Washington, 45North Carolina State University, 46Shanghai Jiao Tong University, 47University of North Carolina, 48University of South Dakota, 49University of North Carolina, 50Lawrence Berkeley National Laboratory, 51Center for Experimental Nuclear Physics and Astrophysics and University of Washington, 52University of South Carolina, 53Osaka University, 54Pacific Northwest National Laboratory, 55University of North Carolina, 56Pacific Northwest National Laboratory, 57University of North Carolina, 58North Carolina State University, 59Lawrence Berkeley National Laboratory, 60University of South Dakota, 61Oak Ridge National Laboratory, 62University of North Carolina, 63Los Alamos National Laboratory, 64Center for Experimental Nuclear Physics and Astrophysics and University of Washington, 65Oak Ridge National Laboratory, 66Los Alamos National Laboratory, 67University of North Carolina, 68Osaka University, 69Joint Institute for Nuclear Research, 70University of North Carolina, 71University of South Dakota, 72Pacific Northwest National Laboratory, 73South Dakota School of Mines and Technology, 74University of South Carolina, 75Black Hills State University, 76Joint Institute for Nuclear Research, 77Duke University, 78University of North Carolina, 79Oak Ridge National Laboratory, 80University of Tennessee, 81Lawrence Berkeley National Laboratory, 82University of North Carolina, 83Oak Ridge National Laboratory, 84University of North Carolina, 85University of South Carolina, 86Los Alamos National Laboratory, 87Joint Institute for Nuclear Research, 88North Carolina State University, 89Oak Ridge National Laboratory, 90Institute for Theoretical and Experimental Physics, 91Joint Institute for Nuclear Research

The Majorana Demonstrator is an ultra-low background physics experiment searching for the neutrinoless double beta decay of $^{76}$Ge. The Majorana Parts Tracking Database is used to record the history of components used in the construction of the Demonstrator. The tracking implementation takes a novel approach based on the schema-free database technology CouchDB. Read More

The goal of this paper is to build a foundation for, and explore the possibility of, using high overtone quasinormal modes of analog black holes to probe the small scale (microscopic) structure of a background fluid in which an analog black hole is formed. This may provide a tool to study the small scale structure of some interesting quantum systems such as Bose-Einstein condensates. In order to build this foundation, we first look into the hydrodynamic case where we calculate the high overtone quasinormal mode frequencies of a 3+1 dimensional canonical non-rotating acoustic black hole. Read More

Neutron spectroscopy is used to investigate the magnetic fluctuations in Fe_{1+x}Te - a parent compound of chalcogenide superconductors. Incommensurate "stripe-like" excitations soften with increased interstitial iron concentration. The energy crossover from incommensurate to stripy fluctuations defines an apparent hour-glass dispersion. Read More

The MAJORANA DEMONSTRATOR is an array of natural and enriched high purity germanium detectors that will search for the neutrinoless double-beta decay of 76-Ge and perform a search for weakly interacting massive particles (WIMPs) with masses below 10 GeV. As part of the MAJORANA research and development efforts, we have deployed a modified, low-background broad energy germanium detector at the Kimballton Underground Research Facility. With its sub-keV energy threshold, this detector is sensitive to potential non-Standard Model physics, including interactions with WIMPs. Read More

2014Jun
Authors: A. J. Bevan, B. Golob, Th. Mannel, S. Prell, B. D. Yabsley, K. Abe, H. Aihara, F. Anulli, N. Arnaud, T. Aushev, M. Beneke, J. Beringer, F. Bianchi, I. I. Bigi, M. Bona, N. Brambilla, J. B rodzicka, P. Chang, M. J. Charles, C. H. Cheng, H. -Y. Cheng, R. Chistov, P. Colangelo, J. P. Coleman, A. Drutskoy, V. P. Druzhinin, S. Eidelman, G. Eigen, A. M. Eisner, R. Faccini, K. T . Flood, P. Gambino, A. Gaz, W. Gradl, H. Hayashii, T. Higuchi, W. D. Hulsbergen, T. Hurth, T. Iijima, R. Itoh, P. D. Jackson, R. Kass, Yu. G. Kolomensky, E. Kou, P. Križan, A. Kronfeld, S. Kumano, Y. J. Kwon, T. E. Latham, D. W. G. S. Leith, V. Lüth, F. Martinez-Vidal, B. T. Meadows, R. Mussa, M. Nakao, S. Nishida, J. Ocariz, S. L. Olsen, P. Pakhlov, G. Pakhlova, A. Palano, A. Pich, S. Playfer, A. Poluektov, F. C. Porter, S. H. Robertson, J. M. Roney, A. Roodman, Y. Sakai, C. Schwanda, A. J. Schwartz, R. Seidl, S. J. Sekula, M. Steinhauser, K. Sumisawa, E. S. Swanson, F. Tackmann, K. Trabelsi, S. Uehara, S. Uno, R. van der Water, G. Vasseur, W. Verkerke, R. Waldi, M. Z. Wang, F. F. Wilson, J. Zupan, A. Zupanc, I. Adachi, J. Albert, Sw. Banerjee, M. Bellis, E. Ben-Haim, P. Biassoni, R. N. Cahn, C. Cartaro, J. Chauveau, C. Chen, C. C. Chiang, R. Cowan, J. Dalseno, M. Davier, C. Davies, J. C. Dingfelder, B. Eche nard, D. Epifanov, B. G. Fulsom, A. M. Gabareen, J. W. Gary, R. Godang, M. T. Graham, A. Hafner, B. Hamilton, T. Hartmann, K. Hayasaka, C. Hearty, Y. Iwasaki, A. Khodjamirian, A. Kusaka, A. Kuzmin, G. D. Lafferty, A. Lazzaro, J. Li, D. Lindemann, O. Long, A. Lusiani, G. Marchiori, M. Martinelli, K. Miyabayashi, R. Mizuk, G. B. Mohanty, D. R. Muller, H. Nakazawa, P. Ongmongkolkul, S. Pacetti, F. Palombo, T. K. Pedlar, L. E. Piilonen, A. Pilloni, V. Poireau, K. Prothmann, T. Pulliam, M. Rama, B. N. Ratcliff, P. Roudeau, S. Schrenk, T. Schroeder, K. R. Schubert, C. P. Shen, B. Shwartz, A. Soffer, E. P. Solodov, A. Somov, M. Starič, S. Stracka, A. V. Telnov, K. Yu. Todyshev, T. Tsuboyama, T. Uglov, A. Vinokurova, J. J. Walsh, Y. Watanabe, E. Won, G. Wormser, D. H. Wright, S. Ye, C. C. Zhang, S. Abachi, A. Abashian, K. Abe, K. Abe, N. Abe, R. Abe, T. Abe, T. Abe, G. S. Abrams, I. Adam, K. Adamczyk, A. Adametz, T. Adye, A. Agarwal, H. Ahmed, M. Ahmed, S. Ahmed, B. S. Ahn, H. S. Ahn, I. J. R. Aitchison, K. Akai, S. Akar, M. Akatsu, M. Akemoto, R. Akhmetshin, R. Akre, M. S. Alam, J. N. Albert, R. Aleksan, J. P. Alexander, G. Alimonti, M. T. Allen, J. Allison, T. Allmendinger, J. R. G. Alsmiller, D. Altenburg, K. E. Alwyn, Q. An, J. Anderson, R. Andreassen, D. Andreotti, M. Andreotti, J. C. Andress, C. Angelini, D. Anipko, A. Anjomshoaa, P. L. Anthony, E. A. Antillon, E. Antonioli, K. Aoki, J. F. Arguin, K. Arinstein, K. Arisaka, K. Asai, M. Asai, Y. Asano, D. J. Asgeirsson, D. M. Asner, T. Aso, M. L. Aspinwall, D. Aston, H. Atmacan, B. Aubert, V. Aulchenko, R. Ayad, T. Azemoon, T. Aziz, V. Azzolini, D. E. Azzopardi, M. A. Baak, J. J. Back, S. Bagnasco, S. Bahinipati, D. S. Bailey, S. Bailey, P. Bailly, N. van Bakel, A. M. Bakich, A. Bala, V. Balagura, R. Baldini-Ferroli, Y. Ban, E. Banas, H. R. Band, S. Banerjee, E. Baracchini, R. Barate, E. Barberio, M. Barbero, D. J. Bard, T. Barillari, N. R. Barlow, R. J. Barlow, M. Barrett, W. Bartel, J. Bartelt, R. Bartoldus, G. Batignani, M. Battaglia, J. M. Bauer, A. Bay, M. Beaulieu, P. Bechtle, T. W. Beck, J. Becker, J. Becla, I. Bedny, S. Behari, P. K. Behera, E. Behn, L. Behr, C. Beigbeder, D. Beiline, R. Bell, F. Bellini, G. Bellodi, K. Belous, M. Benayoun, G. Benelli, J. F. Benitez, M. Benkebil, N. Berger, J. Bernabeu, D. Bernard, R. Bernet, F. U. Bernlochner, J. W. Berryhill, K. Bertsche, P. Besson, D. S. Best, S. Bettarini, D. Bettoni, V. Bhardwaj, W. Bhimji, B. Bhuyan, B. Bhuyan, M. E. Biagini, M. Biasini, K. van Bibber, J. Biesiada, I. Bingham, R. M. Bionta, M. Bischofberger, U. Bitenc, I. Bizjak, F. Blanc, G. Blaylock, V. E. Blinov, E. Bloom, P. C. Bloom, N. L. Blount, J. Blouw, M. Bly, S. Blyth, C. T. Boeheim, M. Bomben, A. Bondar, M. Bondioli, G. R. Bonneaud, G. Bonvicini, M. Booke, J. Booth, C. Borean, A. W. Borgland, E. Borsato, F. Bosi, L. Bosisio, A. A. Botov, J. Bougher, K. Bouldin, P. Bourgeois, D. Boutigny, D. A. Bowerman, A. M. Boyarski, R. F. Boyce, J. T. Boyd, A. Bozek, C. Bozzi, M. Bračko, G. Brandenburg, T. Brandt, B. Brau, J. Brau, A. B. Breon, D. Breton, C. Brew, H. Briand, P. G. Bright-Thomas, V. Brigljević, D. I. Britton, F. Brochard, B. Broomer, J. Brose, T. E. Browder, C. L. Brown, C. M. Brown, D. N. Brown, D. N. Brown, M. Browne, M. Bruinsma, S. Brunet, F. Bucci, C. Buchanan, O. L. Buchmueller, C. Bünger, W. Bugg, A. D. Bukin, R. Bula, H. Bulten, P. R. Burchat, W. Burgess, J. P. Burke, J. Button-Shafer, A. R. Buzykaev, A. Buzzo, Y. Cai, R. Calabrese, A. Calcaterra, G. Calderini, B. Camanzi, E. Campagna, C. Campagnari, R. Capra, V. Carassiti, M. Carpinelli, M. Carroll, G. Casarosa, B. C. K. Casey, N. M. Cason, G. Castelli, N. Cavallo, G. Cavoto, A. Cecchi, R. Cenci, G. Cerizza, A. Cervelli, A. Ceseracciu, X. Chai, K. S. Chaisanguanthum, M. C. Chang, Y. H. Chang, Y. W. Chang, D. S. Chao, M. Chao, Y. Chao, E. Charles, C. A. Chavez, R. Cheaib, V. Chekelian, A. Chen, A. Chen, E. Chen, G. P. Chen, H. F. Chen, J. -H. Chen, J. C. Chen, K. F. Chen, P. Chen, S. Chen, W. T. Chen, X. Chen, X. R. Chen, Y. Q. Chen, B. Cheng, B. G. Cheon, N. Chevalier, Y. M. Chia, S. Chidzik, K. Chilikin, M. V. Chistiakova, R. Cizeron, I. S. Cho, K. Cho, V. Chobanova, H. H. F. Choi, K. S. Choi, S. K. Choi, Y. Choi, Y. K. Choi, S. Christ, P. H. Chu, S. Chun, A. Chuvikov, G. Cibinetto, D. Cinabro, A. R. Clark, P. J. Clark, C. K. Clarke, R. Claus, B. Claxton, Z. C. Clifton, J. Cochran, J. Cohen-Tanugi, H. Cohn, T. Colberg, S. Cole, F. Colecchia, C. Condurache, R. Contri, P. Convert, M. R. Convery, P. Cooke, N. Copty, C. M. Cormack, F. Dal Corso, L. A. Corwin, F. Cossutti, D. Cote, A. Cotta Ramusino, W. N. Cottingham, F. Couderc, D. P. Coupal, R. Covarelli, G. Cowan, W. W. Craddock, G. Crane, H. B. Crawley, L. Cremaldi, A. Crescente, M. Cristinziani, J. Crnkovic, G. Crosetti, T. Cuhadar-Donszelmann, A. Cunha, S. Curry, A. D'Orazio, S. Dû, G. Dahlinger, B. Dahmes, C. Dallapiccola, N. Danielson, M. Danilov, A. Das, M. Dash, S. Dasu, M. Datta, F. Daudo, P. D. Dauncey, P. David, C. L. Davis, C. T. Day, F. De Mori, G. De Domenico, N. De Groot, C. De la Vaissière, Ch. de la Vaissière, A. de Lesquen, G. De Nardo, R. de Sangro, A. De Silva, S. DeBarger, F. J. Decker, P. del Amo Sanchez, L. Del Buono, V. Del Gamba, D. del Re, G. Della Ricca, A. G. Denig, D. Derkach, I. M. Derrington, H. DeStaebler, J. Destree, S. Devmal, B. Dey, B. Di Girolamo, E. Di Marco, M. Dickopp, M. O. Dima, S. Dittrich, S. Dittongo, P. Dixon, L. Dneprovsky, F. Dohou, Y. Doi, Z. Doležal, D. A. Doll, M. Donald, L. Dong, L. Y. Dong, J. Dorfan, A. Dorigo, M. P. Dorsten, R. Dowd, J. Dowdell, Z. Drásal, J. Dragic, B. W. Drummond, R. S. Dubitzky, G. P. Dubois-Felsmann, M. S. Dubrovin, Y. C. Duh, Y. T. Duh, D. Dujmic, W. Dungel, W. Dunwoodie, D. Dutta, A. Dvoretskii, N. Dyce, M. Ebert, E. A. Eckhart, S. Ecklund, R. Eckmann, P. Eckstein, C. L. Edgar, A. J. Edwards, U. Egede, A. M. Eichenbaum, P. Elmer, S. Emery, Y. Enari, R. Enomoto, E. Erdos, R. Erickson, J. A. Ernst, R. J. Erwin, M. Escalier, V. Eschenburg, I. Eschrich, S. Esen, L. Esteve, F. Evangelisti, C. W. Everton, V. Eyges, C. Fabby, F. Fabozzi, S. Fahey, M. Falbo, S. Fan, F. Fang, F. Fang, C. Fanin, A. Farbin, H. Farhat, J. E. Fast, M. Feindt, A. Fella, E. Feltresi, T. Ferber, R. E. Fernholz, S. Ferrag, F. Ferrarotto, F. Ferroni, R. C. Field, A. Filippi, G. Finocchiaro, E. Fioravanti, J. Firmino da Costa, P. -A. Fischer, A. Fisher, P. H. Fisher, C. J. Flacco, R. L. Flack, H. U. Flaecher, J. Flanagan, J. M. Flanigan, K. E. Ford, W. T. Ford, I. J. Forster, A. C. Forti, F. Forti, D. Fortin, B. Foster, S. D. Foulkes, G. Fouque, J. Fox, P. Franchini, M. Franco Sevilla, B. Franek, E. D. Frank, K. B. Fransham, S. Fratina, K. Fratini, A. Frey, R. Frey, M. Friedl, M. Fritsch, J. R. Fry, H. Fujii, M. Fujikawa, Y. Fujita, Y. Fujiyama, C. Fukunaga, M. Fukushima, J. Fullwood, Y. Funahashi, Y. Funakoshi, F. Furano, M. Furman, K. Furukawa, H. Futterschneider, E. Gabathuler, T. A. Gabriel, N. Gabyshev, F. Gaede, N. Gagliardi, A. Gaidot, J. -M. Gaillard, J. R. Gaillard, S. Galagedera, F. Galeazzi, F. Gallo, D. Gamba, R. Gamet, K. K. Gan, P. Gandini, S. Ganguly, S. F. Ganzhur, Y. Y. Gao, I. Gaponenko, A. Garmash, J. Garra Tico, I. Garzia, M. Gaspero, F. Gastaldi, C. Gatto, V. Gaur, N. I. Geddes, T. L. Geld, J. -F. Genat, K. A. George, M. George, S. George, Z. Georgette, T. J. Gershon, M. S. Gill, R. Gillard, J. D. Gilman, F. Giordano, M. A. Giorgi, P. -F. Giraud, L. Gladney, T. Glanzman, R. Glattauer, A. Go, K. Goetzen, Y. M. Goh, G. Gokhroo, P. Goldenzweig, V. B. Golubev, G. P. Gopal, A. Gordon, A. Gorišek, V. I. Goriletsky, R. Gorodeisky, L. Gosset, K. Gotow, S. J. Gowdy, P. Graffin, S. Grancagnolo, E. Grauges, G. Graziani, M. G. Green, M. G. Greene, G. J. Grenier, P. Grenier, K. Griessinger, A. A. Grillo, B. V. Grinyov, A. V. Gritsan, G. Grosdidier, M. Grosse Perdekamp, P. Grosso, M. Grothe, Y. Groysman, O. Grünberg, E. Guido, H. Guler, N. J. W. Gunawardane, Q. H. Guo, R. S. Guo, Z. J. Guo, N. Guttman, H. Ha, H. C. Ha, T. Haas, J. Haba, J. Hachtel, H. K. Hadavand, T. Hadig, C. Hagner, M. Haire, F. Haitani, T. Haji, G. Haller, V. Halyo, K. Hamano, H. Hamasaki, G. Hamel de Monchenault, J. Hamilton, R. Hamilton, O. Hamon, B. Y. Han, Y. L. Han, H. Hanada, K. Hanagaki, F. Handa, J. E. Hanson, A. Hanushevsky, K. Hara, T. Hara, Y. Harada, P. F. Harrison, T. J. Harrison, B. Harrop, A. J. Hart, P. A. Hart, B. L. Hartfiel, J. L. Harton, T. Haruyama, A. Hasan, Y. Hasegawa, C. Hast, N. C. Hastings, K. Hasuko, A. Hauke, C. M. Hawkes, K. Hayashi, M. Hazumi, C. Hee, E. M. Heenan, D. Heffernan, T. Held, R. Henderson, S. W. Henderson, S. S. Hertzbach, S. Hervé, M. Heß, C. A. Heusch, A. Hicheur, Y. Higashi, Y. Higasino, I. Higuchi, S. Hikita, E. J. Hill, T. Himel, L. Hinz, T. Hirai, H. Hirano, J. F. Hirschauer, D. G. Hitlin, N. Hitomi, M. C. Hodgkinson, A. Höcker, C. T. Hoi, T. Hojo, T. Hokuue, J. J. Hollar, T. M. Hong, K. Honscheid, B. Hooberman, D. A. Hopkins, Y. Horii, Y. Hoshi, K. Hoshina, S. Hou, W. S. Hou, T. Hryn'ova, Y. B. Hsiung, C. L. Hsu, S. C. Hsu, H. Hu, T. Hu, H. C. Huang, T. J. Huang, Y. C. Huang, Z. Huard, M. E. Huffer, D. Hufnagel, T. Hung, D. E. Hutchcroft, H. J. Hyun, S. Ichizawa, T. Igaki, A. Igarashi, S. Igarashi, Y. Igarashi, O. Igonkina, K. Ikado, H. Ikeda, H. Ikeda, K. Ikeda, J. Ilic, K. Inami, W. R. Innes, Y. Inoue, A. Ishikawa, A. Ishikawa, H. Ishino, K. Itagaki, S. Itami, K. Itoh, V. N. Ivanchenko, R. Iverson, M. Iwabuchi, G. Iwai, M. Iwai, S. Iwaida, M. Iwamoto, H. Iwasaki, M. Iwasaki, M. Iwasaki, T. Iwashita, J. M. Izen, D. J. Jackson, F. Jackson, G. Jackson, P. S. Jackson, R. G. Jacobsen, C. Jacoby, I. Jaegle, V. Jain, P. Jalocha, H. K. Jang, H. Jasper, A. Jawahery, S. Jayatilleke, C. M. Jen, F. Jensen, C. P. Jessop, X. B. Ji, M. J. J. John, D. R. Johnson, J. R. Johnson, S. Jolly, M. Jones, K. K. Joo, N. Joshi, N. J. Joshi, D. Judd, T. Julius, R. W. Kadel, J. A. Kadyk, H. Kagan, R. Kagan, D. H. Kah, S. Kaiser, H. Kaji, S. Kajiwara, H. Kakuno, T. Kameshima, J. Kaminski, T. Kamitani, J. Kaneko, J. H. Kang, J. S. Kang, T. Kani, P. Kapusta, T. M. Karbach, M. Karolak, Y. Karyotakis, K. Kasami, G. Katano, S. U. Kataoka, N. Katayama, E. Kato, Y. Kato, H. Kawai, H. Kawai, M. Kawai, N. Kawamura, T. Kawasaki, J. Kay, M. Kay, M. P. Kelly, M. H. Kelsey, N. Kent, L. T. Kerth, A. Khan, H. R. Khan, D. Kharakh, A. Kibayashi, H. Kichimi, C. Kiesling, M. Kikuchi, E. Kikutani, B. H. Kim, C. H. Kim, D. W. Kim, H. Kim, H. J. Kim, H. J. Kim, H. O. Kim, H. W. Kim, J. B. Kim, J. H. Kim, K. T. Kim, M. J. Kim, P. Kim, S. K. Kim, S. M. Kim, T. H. Kim, Y. I. Kim, Y. J. Kim, G. J. King, K. Kinoshita, A. Kirk, D. Kirkby, I. Kitayama, M. Klemetti, V. Klose, J. Klucar, N. S. Knecht, K. J. Knoepfel, D. J. Knowles, B. R. Ko, N. Kobayashi, S. Kobayashi, T. Kobayashi, M. J. Kobel, S. Koblitz, H. Koch, M. L. Kocian, P. Kodyš, K. Koeneke, R. Kofler, S. Koike, S. Koishi, H. Koiso, J. A. Kolb, S. D. Kolya, Y. Kondo, H. Konishi, P. Koppenburg, V. B. Koptchev, T. M. B. Kordich, A. A. Korol, K. Korotushenko, S. Korpar, R. T. Kouzes, D. Kovalskyi, R. Kowalewski, Y. Kozakai, W. Kozanecki, J. F. Kral, A. Krasnykh, R. Krause, E. A. Kravchenko, J. Krebs, A. Kreisel, M. Kreps, M. Krishnamurthy, R. Kroeger, W. Kroeger, P. Krokovny, B. Kronenbitter, J. Kroseberg, T. Kubo, T. Kuhr, G. Kukartsev, R. Kulasiri, A. Kulikov, R. Kumar, S. Kumar, T. Kumita, T. Kuniya, M. Kunze, C. C. Kuo, T. -L. Kuo, H. Kurashiro, E. Kurihara, N. Kurita, Y. Kuroki, A. Kurup, P. E. Kutter, N. Kuznetsova, P. Kvasnička, P. Kyberd, S. H. Kyeong, H. M. Lacker, C. K. Lae, E. Lamanna, J. Lamsa, L. Lanceri, L. Landi, M. I. Lang, D. J. Lange, J. S. Lange, U. Langenegger, M. Langer, A. J. Lankford, F. Lanni, S. Laplace, E. Latour, Y. P. Lau, D. R. Lavin, J. Layter, H. Lebbolo, C. LeClerc, T. Leddig, G. Leder, F. Le Diberder, C. L. Lee, J. Lee, J. S. Lee, M. C. Lee, M. H. Lee, M. J. Lee, M. J. Lee, S. -J. Lee, S. E. Lee, S. H. Lee, Y. J. Lee, J. P. Lees, M. Legendre, M. Leitgab, R. Leitner, E. Leonardi, C. Leonidopoulos, V. Lepeltier, Ph. Leruste, T. Lesiak, M. E. Levi, S. L. Levy, B. Lewandowski, M. J. Lewczuk, P. Lewis, H. Li, H. B. Li, S. Li, X. Li, X. Li, Y. Li, Y. Li, L. Li Gioi, J. Libby, J. Lidbury, V. Lillard, C. L. Lim, A. Limosani, C. S. Lin, J. Y. Lin, S. W. Lin, Y. S. Lin, B. Lindquist, C. Lindsay, L. Lista, C. Liu, F. Liu, H. Liu, H. M. Liu, J. Liu, R. Liu, T. Liu, Y. Liu, Z. Q. Liu, D. Liventsev, M. Lo Vetere, C. B. Locke, W. S. Lockman, F. Di Lodovico, V. Lombardo, G. W. London, D. Lopes Pegna, L. Lopez, N. Lopez-March, J. Lory, J. M. LoSecco, X. C. Lou, R. Louvot, A. Lu, C. Lu, M. Lu, R. S. Lu, T. 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Zheng, Z. P. Zheng, V. Zhilich, P. Zhou, R. Y. Zhu, Y. S. Zhu, Z. M. Zhu, V. Zhulanov, T. Ziegler, V. Ziegler, G. Zioulas, M. Zisman, M. Zito, D. Zürcher, N. Zwahlen, O. Zyukova, T. Živko, D. Žontar

This work is on the Physics of the B Factories. Part A of this book contains a brief description of the SLAC and KEK B Factories as well as their detectors, BaBar and Belle, and data taking related issues. Part B discusses tools and methods used by the experiments in order to obtain results. Read More

This paper was motivated by the following question: Recall that for a smooth projective variety X whose polarized Hodge structure on H^n(X,Q)_{prim} leads to a period point ... Read More

The coefficient of the $D^6 {\cal R}^4$ interaction in the low energy expansion of the two-loop four-graviton amplitude in type II superstring theory is known to be proportional to the integral of the Zhang-Kawazumi (ZK) invariant over the moduli space of genus-two Riemann surfaces. We demonstrate that the ZK invariant is an eigenfunction with eigenvalue 5 of the Laplace-Beltrami operator in the interior of moduli space. Exploiting this result, we evaluate the integral of the ZK invariant explicitly, finding agreement with the value of the two-loop $D^6 {\cal R}^4$ interaction predicted on the basis of S-duality and supersymmetry. Read More

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