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Featured researches published by B. Hill.


Physical Review D | 2016

Performance of two Askaryan Radio Array stations and first results in the search for ultrahigh energy neutrinos

P. Allison; R. Bard; J. J. Beatty; David Z. Besson; C. Bora; Chih-Ching Chen; C.-H. Chen; Pisin Chen; A. Christenson; A. Connolly; Jonathan Davies; M. A. DuVernois; B. Fox; R. Gaior; P. Gorham; K. Hanson; J. Haugen; B. Hill; Kara Dion Hoffman; E. Hong; S.-Y. Hsu; L. Hu; J.-J. Huang; M.-H. A. Huang; A. Ishihara; A. Karle; J. L. Kelley; D. Kennedy; Ilya Kravchenko; T. Kuwabara

Ultrahigh energy neutrinos are interesting messenger particles since, if detected, they can transmit exclusive information about ultrahigh energy processes in the Universe. These particles, with energies above 1016 eV, interact very rarely. Therefore, detectors that instrument several gigatons of matter are needed to discover them. The ARA detector is currently being constructed at the South Pole. It is designed to use the Askaryan effect, the emission of radio waves from neutrino-induced cascades in the South Pole ice, to detect neutrino interactions at very high energies. With antennas distributed among 37 widely separated stations in the ice, such interactions can be observed in a volume of several hundred cubic kilometers. Currently three deep ARA stations are deployed in the ice, of which two have been taking data since the beginning of 2013. In this article, the ARA detector “as built” and calibrations are described. Data reduction methods used to distinguish the rare radio signals from overwhelming backgrounds of thermal and anthropogenic origin are presented. Using data from only two stations over a short exposure time of 10 months, a neutrino flux limit of 1.5 × 10−6 GeV=cm2=s=sr is calculated for a particle energy of 1018 eV, which offers promise for the full ARA detector.


Physical Review D | 2011

Ultra-Relativistic Magnetic Monopole Search with the ANITA-II Balloon-borne Radio Interferometer

M. Detrixhe; D. Besson; P. Gorham; P. Allison; B. Baughmann; J. J. Beatty; K. Belov; Simon Bevan; W. R. Binns; Chun Hsiung Chen; Pisin Chen; J. Clem; A. Connolly; D. De Marco; P. F. Dowkontt; M. A. DuVernois; C. Frankenfeld; E. Grashorn; D. P. Hogan; N. Griffith; B. Hill; S. Hoover; M. H. Israel; A. Javaid; Kurt Liewer; S. Matsuno; B. C. Mercurio; C. Miki; M. Mottram; J. W. Nam

We have conducted a search for extended energy deposition trails left by ultrarelativistic magnetic monopoles interacting in Antarctic ice. The nonobservation of any satisfactory candidates in the 31 days of accumulated ANITA-II (Antarctic Impulsive Transient Antenna) flight data results in an upper limit on the diffuse flux of relativistic monopoles. We obtain a 90% C.L. limit of order 10{sup -19} (cm{sup 2} s sr){sup -1} for values of Lorentz factor, {gamma}, 10{sup 10{<=}{gamma}} at the anticipated energy E{sub tot}=10{sup 16} GeV. This bound is stronger than all previously published experimental limits for this kinematic range.


The Astrophysical Journal | 2011

THE FIRST LIMITS ON THE ULTRA-HIGH ENERGY NEUTRINO FLUENCE FROM GAMMA-RAY BURSTS

A. G. Vieregg; K. Palladino; P. Allison; B. M. Baughman; J. J. Beatty; K. Belov; D. Besson; S. Bevan; W. R. Binns; C.T. Chen; Pisin Chen; J. Clem; A. Connolly; M. Detrixhe; D. De Marco; P. F. Dowkontt; M. DuVernois; P. Gorham; Grashorn E; B. Hill; S. Hoover; M.A. Huang; M. H. Israel; A. Javaid; Kurt Liewer; S. Matsuno; B. C. Mercurio; C. Miki; M. Mottram; J. W. Nam

We set the first limits on the ultra-high energy (UHE) neutrino fluence at energies greater than 10{sup 9} GeV from gamma-ray bursts (GRBs) based on data from the second flight of the Antarctic Impulsive Transient Antenna (ANITA). During the 31 day flight of ANITA-II, 26 GRBs were recorded by Swift or Fermi. Of these, we analyzed the 12 GRBs which occurred during quiet periods when the payload was away from anthropogenic activity. In a blind analysis, we observe 0 events on a total background of 0.0044 events in the combined prompt window for all 12 low-background bursts. We also observe 0 events from the remaining 14 bursts. We place a 90% confidence level limit on the E{sup -4} prompt neutrino fluence between 10{sup 8} GeV < E < 10{sup 12} GeV of E{sup 4}{Phi} = 2.5 x 10{sup 17} GeV{sup 3} cm{sup -2} from GRB090107A. This is the first reported limit on the UHE neutrino fluence from GRBs above 10{sup 9} GeV, and the strongest limit above 10{sup 8} GeV.


arXiv: Instrumentation and Methods for Astrophysics | 2017

Antarctic Surface Reflectivity Measurements from the ANITA-3 and HiCal-1 Experiments

P. Gorham; P. Allison; O. Banerjee; J. J. Beatty; K. Belov; D. Besson; W. R. Binns; V. Bugaev; P. Cao; Chun Hsiung Chen; P. Chen; J. Clem; A. Connolly; B. Dailey; P. Dasgupta; C. Deaconu; L. Cremonesi; P. F. Dowkontt; B. Fox; J. Gordon; B. Hill; R. Hupe; M. H. Israel; P. Jain; J. Kowalski; J. Lam; J. G. Learned; Kurt Liewer; T.-C. Liu; S. Matsuno

The primary science goal of the NASA-sponsored ANITA project is measurement of ultra-high energy neutrinos and cosmic rays, observed via radio-frequency signals resulting from a neutrino or cosmic ray interaction with terrestrial matter (e.g. atmospheric or ice molecules). Accurate inference of the energies of these cosmic rays requires understanding the transmission/reflection of radio wave signals across the ice–air boundary. Satellite-based measurements of Antarctic surface reflectivity, using a co-located transmitter and receiver, have been performed more-or-less continuously for the last few decades. Our comparison of four different reflectivity surveys, at frequencies ranging from 2 to 45GHz and at near-normal incidence, yield generally consistent maps of high versus low reflectivity, as a function of location, across Antarctica. Using the Sun as an RF source, and the ANITA-3 balloon borne radio-frequency antenna array as the RF receiver, we have also measured the surface reflectivity over the interval 200–1000MHz, at elevation angles of 12–30∘. Consistent with our previous measurement using ANITA-2, we find good agreement, within systematic errors (dominated by antenna beam width uncertainties) and across Antarctica, with the expected reflectivity as prescribed by the Fresnel equations. To probe low incidence angles, inaccessible to the Antarctic Solar technique and not probed by previous satellite surveys, a novel experimental approach (“HiCal-1”) was devised. Unlike previous measurements, HiCal-ANITA constitute a bi-static transmitter–receiver pair separated by hundreds of kilometers. Data taken with HiCal, between 200 and 600MHz shows a significant departure from the Fresnel equations, constant with frequency over that band, with the deficit increasing with obliquity of incidence, which we attribute to the combined effects of possible surface roughness, surface grain effects, radar clutter and/or shadowing of the reflection zone due to Earth curvature effects. We discuss the science implications of the HiCal results, as well as improvements planned for HiCal-2, preparing for launch in December 2016.


arXiv: High Energy Astrophysical Phenomena | 2017

Upward-Pointing Cosmic-Ray-like Events Observed with ANITA

A. Romero-Wolf; J. W. Nam; S. Hoover; P. Gorham; P. Allison; L. Batten; J. J. Beatty; K. Belov; D. Besson; W. R. Binns; P. Cao; Chun Hsiung Chen; P. Chen; J. Clem; A. Connolly; B. Dailey; C. Deaconu; L. Cremonesi; P. F. Dowkontt; M. A. DuVernois; R. C. Field; D. Goldstein; J. Gordon; C. Hast; C. L. Hebert; B. Hill; K. Hughes; R. Hupe; M. H. Israel; A. Javaid

These proceedings address a recent publication by the ANITA collaboration of four upward- pointing cosmic-ray-like events observed in the first flight of ANITA. Three of these events were consistent with stratospheric cosmic-ray air showers where the axis of propagation does not inter- sect the surface of the Earth. The fourth event was consistent with a primary particle that emerges from the surface of the ice suggesting a possible {\tau}-lepton decay as the origin of this event. These proceedings follow-up on the modeling and testing of the hypothesis that this event was of {\tau} neutrino origin.


Physical Review D | 2018

Antarctic surface reflectivity calculations and measurements from the ANITA-4 and HiCal-2 experiments

S. Prohira; A. Novikov; P. Dasgupta; P. Jain; S. Nande; P. Allison; O. Banerjee; L. Batten; J. J. Beatty; K. Belov; D. Besson; W. R. Binns; V. Bugaev; P. Cao; C.-H. Chen; P. Chen; J. Clem; A. Connolly; L. Cremonesi; B. Dailey; C. Deaconu; P. F. Dowkontt; B. Fox; J. Gordon; P. Gorham; C. Hast; B. Hill; R. Hupe; M. H. Israel; J. Lam

The balloon-borne HiCal radio-frequency (RF) transmitter, in concert with the ANITA radio-frequency receiver array, is designed to measure the Antarctic surface reflectivity in the RF wavelength regime. The amplitude of surface-reflected transmissions from HiCal, registered as triggered events by ANITA, can be compared with the direct transmissions preceding them by O ( 10 ) microseconds, to infer the surface power reflection coefficient R . The first HiCal mission (HiCal-1, Jan. 2015) yielded a sample of 100 such pairs, resulting in estimates of R at highly glancing angles (i.e., zenith angles approaching 90°), with measured reflectivity for those events which exceeded extant calculations [P. W. Gorham et al., Journal of Astronomical Instrumentation, 1740002 (2017)]. The HiCal-2 experiment, flying from December 2016–January 2017, provided an improvement by nearly 2 orders of magnitude in our event statistics, allowing a considerably more precise mapping of the reflectivity over a wider range of incidence angles. We find general agreement between the HiCal-2 reflectivity results and those obtained with the earlier HiCal-1 mission, as well as estimates from Solar reflections in the radio-frequency regime [D. Z. Besson et al., Radio Sci. 50, 1 (2015)]. In parallel, our calculations of expected reflectivity have matured; herein, we use a plane-wave expansion to estimate the reflectivity R from both a flat, smooth surface (and, in so doing, recover the Fresnel reflectivity equations) and also a curved surface. Multiplying our flat-smooth reflectivity by improved Earth curvature and surface roughness corrections now provides significantly better agreement between theory and the HiCal-2 measurements.


Astroparticle Physics | 2017

Constraints on the ultra-high-energy neutrino flux from Gamma-Ray bursts from a prototype station of the Askaryan radio array

P. Allison; J. Auffenberg; R. Bard; J. J. Beatty; D. Besson; C. Bora; Chih-Ching Chen; Pisin Chen; A. Connolly; Jonathan Davies; M. A. DuVernois; B. Fox; P. Gorham; K. Hanson; B. Hill; Kara Dion Hoffman; E. Hong; L. Hu; A. Ishihara; A. Karle; J. L. Kelley; Ilya Kravchenko; H. Landsman; A. Laundrie; C.-J. Li; T.-C. Liu; M.-Y. Lu; R. Maunu; K. Mase; T. Meures

Abstract We report on a search for ultra-high-energy (UHE) neutrinos from gamma-ray bursts (GRBs) in the data set collected by the Testbed station of the Askaryan Radio Array (ARA) in 2011 and 2012. From 57 selected GRBs, we observed no events that survive our cuts, which is consistent with 0.12 expected background events. Using NeuCosmA as a numerical GRB reference emission model, we estimate upper limits on the prompt UHE GRB neutrino fluence and quasi-diffuse flux from 10 7 to 10 10 GeV. This is the first limit on the prompt UHE GRB neutrino quasi-diffuse flux above 10 7 GeV.


united states national committee of ursi national radio science meeting | 2014

The Exa Volt Antenna

P. Gorham; H. Schoorlemmer; F.E. Baginski; P. Allison; K. M. Liewer; C. Miki; B. Hill; G. Varner

Summary form only given. The Exa Volt Antenna is an ultra-high energy (UHE) particle observatory under development for NASAs suborbital super-pressure balloon program in Antarctica. Radio impulses are emitted via the Askaryan effect when UHE neutrinos interact in the ice, and from geomagnetic emission from UHE cosmic ray interactions in the atmosphere above Antarctica. The design utilized part of the balloons surfaces as a reflector which collimates the incoming radiation to a feed-array mounted on a surface inside the balloon. In this way, an ultra-large radio antenna system with a synoptic view on the Antarctic ice sheet below is created. The instantaneous aperture is estimated to be several hundred m2 within the frequency range between 150-600MHz. For standard models of cosmogenic UHE neutrino productions, EVAs sensitivity should result in the order of 30 events per flight. This is a 1-2 orders improvement over ANITAs integrated totals, which is the current state-of-the-art UHE particle observatory for cosmogenic neutrinos. The estimated total amount of UHE cosmic rays is in the order of 15,000, of which we expect several hundred above 10 EeV, and of order 60 above the GZK cutoff energy. Using a the surface of a suborbital supper-pressure balloon as a toroidal reflector is a novel technique of which thorough validation with scale models and simulations is ongoing. The focus of this talk will be the scientific motivation for the mission and recent results from ongoing design studies.


Astroparticle Physics | 2012

Design and Initial Performance of the Askaryan Radio Array Prototype EeV Neutrino Detector at the South Pole

P. Allison; J. Auffenberg; Robert Bard; J. J. Beatty; David Dzb Besson; Sybille Böser; Chih-Ching Chen; Pisin Chen; A. Connolly; Jonathan Davies; M. A. DuVernois; B. Fox; P. Gorham; E. Grashorn; K. Hanson; James Haugen; Klaus Helbing; B. Hill; Kara Hoffman; E. Hong; M.A. Huang; Ming-Huey A. Huang; A. Ishihara; A. Karle; Daniel Kennedy; H. Landsman; T.-C. Liu; Luca Macchiarulo; K. Mase; T. Meures


Physical Review D | 2010

Observational constraints on the ultrahigh energy cosmic neutrino flux from the second flight of the ANITA experiment

P. Gorham; P. Allison; M. DuVernois; B. Hill; S. Matsuno; C. Miki; A. Romero-Wolf; L. Ruckman; G. Varner; B. M. Baughman; J. J. Beatty; E. Grashorn; B. C. Mercurio; K. Palladino; K. Belov; S. Hoover; D. Saltzberg; Vieregg Ag; D. Besson; M. Detrixhe

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P. Allison

Jet Propulsion Laboratory

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J. Clem

University of Delaware

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P. F. Dowkontt

Washington University in St. Louis

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B. Fox

University of Hawaii at Manoa

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C. Miki

University of Hawaii at Manoa

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K. Belov

University of California

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