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Featured researches published by P. Vahle.


Journal of Instrumentation | 2016

A Convolutional Neural Network Neutrino Event Classifier

A. Aurisano; A. Radovic; D. Rocco; A. Himmel; M. D. Messier; E. Niner; G. Pawloski; F. Psihas; A. Sousa; P. Vahle

Convolutional neural networks (CNNs) have been widely applied in the computer vision community to solve complex problems in image recognition and analysis. We describe an application of the CNN technology to the problem of identifying particle interactions in sampling calorimeters used commonly in high energy physics and high energy neutrino physics in particular. Following a discussion of the core concepts of CNNs and recent innovations in CNN architectures related to the field of deep learning, we outline a specific application to the NOvA neutrino detector. This algorithm, CVN (Convolutional Visual Network) identifies neutrino interactions based on their topology without the need for detailed reconstruction and outperforms algorithms currently in use by the NOvA collaboration.


arXiv: Instrumentation and Detectors | 2013

CHerenkov detectors In mine PitS (CHIPS) Letter of Intent to FNAL

P. Adamson; A. Sousa; A. Perch; K. Lang; A. Radovic; J. J. Evans; M. L. Marshak; M. M. Pfützner; J. R. Meier; J. A B Coelho; S. V. Cao; R. J. Nichol; R. Mehdiyev; Gavin Davies; J. K. Nelson; G. Pawloski; A. Kreymer; J. S. Huang; R. B. Patterson; S. G. Wojcicki; M. Proga; L. Whitehead; V. Paolone; J. P. Thomas; S. Schreiner; Manuel Calderon De La Barca Sanchez; A. Habig; D. Naples; A. Holin; J. Hartnell

This Letter of Intent outlines a proposal to build a large, yet cost-effective, 100 kton fiducial mass water Cherenkov detector that will initially run in the NuMI beam line. The CHIPS detector (CHerenkov detector In Mine PitS) will be deployed in a flooded mine pit, removing the necessity and expense of a substantial external structure capable of supporting a large detector mass. There are a number of mine pits in northern Minnesota along the NuMI beam that could be used to deploy such a detector. In particular, the Wentworth Pit 2W is at the ideal off-axis angle to contribute to the measurement of the CP violating phase. The detector is designed so that it can be moved to a mine pit in the LBNE beam line once that becomes operational.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2001

A comprehensive characterization of Hamamatsu 16- and 64-anode PMTs

K. Lang; J. Day; S. Eilerts; S. Fuqua; M. Kordosky; P. Vahle; P.J. Dervan; R. Saakyan; J. Thomas; M. A. Barker; P. S. Miyagawa; A. De Santo; A. Weber; G. Tzanakos; H. Kim; D. Michael; M. Ignatenko; V. Makeev; A. Para; R. Lee; C. Bower; S. Mufson; P. M. Border; P. Cushman; K. Ruddick; R. Schwienhorst; P. Adamson; P. Harris; R. Webb; W. P. Oliver

We are reporting preliminary results of studies of R59000-00-M16 and M64 tubes, manufactured by Hamamatsu Photonics, to be employed by the MINOS neutrino experiment. Our tests focused on anode response uniformity, gain, cross-talk, and linearity for light illuminating PMTs through a 1.2 mm diameter fiber.


Unknown Journal | 2011

MINOS+: a Proposal to FNAL to run MINOS with the medium energy NuMI beam

G. Tzanankos; A. Weber; K. Lang; C. Escobar; J. J. Evans; E. Falk; S. G. Wojcicki; P. Vahle; M. L. Marshak; J. K. Nelson; C. White; A. Blake; J. Schneps; M. Thomson; B Pahlka; R. Mehdiyev; D. Cronin-Hennessy; J. Hartnell; G. Pawloski; Z. Isvan; G. B. Mills; S. K. Swain; A. Kreymer; J.L.: aff Texas U. Ritchie; R. B. Patterson; A. Holin; R. Plunkett; R. Nichol; P. Lucas; Z. Pavlovic

This is a proposal to continue to expose the two MINOS detectors to the NuMI muon neutrino beam for three years starting in 2013. The medium energy setting of the NuMI beam projected for NO{nu}A will deliver about 18 x 10{sup 20} protons-on-target during the first three years of operation. This will allow the MINOS Far Detector to collect more than 10,000 charged current muon neutrino events in the 4-10 GeV energy range and provide a stringent test for non-standard neutrino interactions, sterile neutrinos, extra dimensions, neutrino time-of-flight, and perhaps more. In addition there will be more than 3,000 neutral current events which will be particularly useful in extending the sterile neutrino search range.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009

Comparisons of the MINOS near and far detector readout systems at a test beam

A. Cabrera; P. Adamson; M. A. Barker; A. Belias; S. Boyd; G. Crone; G. Drake; E. Falk; P. Harris; J. Hartnell; Linda Jenner; M. Kordosky; K. Lang; R. P. Litchfield; D. G. Michael; P. S. Miyagawa; R. Morse; S. Murgia; R. Nichol; T. C. Nicholls; G. F. Pearce; D. Petyt; D. Reyna; R. Saakyan; P. Shanahan; C. Smith; P. A. Symes; N. Tagg; J. Thomas; P. Vahle

MINOS is a long baseline neutrino oscillation experiment that uses two detectors separated by 734 km. The readout systems used for the two detectors are different and have to be independently calibrated. To verify and make a direct comparison of the calibrated response of the two readout systems, test beam data were acquired using a smaller calibration detector. This detector was simultaneously instrumented with both readout systems and exposed to the CERN PS T7 test beam. Differences in the calibrated response of the two systems are shown to arise from differences in response non-linearity, photomultiplier tube crosstalk, and threshold effects at the few percent level. These differences are reproduced by the Monte Carlo (MC) simulation to better than 1% and a scheme that corrects for these differences by calibrating the MC to match the data in each detector separately is presented. The overall difference in calorimetric response between the two readout systems is shown to be consistent with zero to a precision of 1.3% in data and 0.3% in MC with no significant energy dependence.


Archive | 2008

Neutrino Oscillations: Present Status and Future Plans

Jennifer A Thomas; P. Vahle

Present Status: Super K (C Walter) K2K (J Wilkes) MINOS (T Vahle) SNO (J Wilson & S Peeters) Kamland (K Heeger) LSND/Karmen (W Louis) MiniBoone (S Brice) Future Plans: LNGS (D Autiero) T2K (D Wark) Double Chooz (G Horton-Smith & T Lassarre) Nova (G Feldman) Daya Bay (K B Luk).


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017

Measuring the attenuation length of water in the CHIPS-M water Cherenkov detector

F. Amat; P. Bizouard; J. Bryant; T. J. Carroll; S. De Rijck; S. Germani; T. Joyce; B. Kriesten; M. L. Marshak; J. R. Meier; J. K. Nelson; A. Perch; M. M. Pfützner; R. Salazar; J. Thomas; J. Trokan-Tenorio; P. Vahle; R. Wade; C. Wendt; L. Whitehead; M. Whitney

The water at the proposed site of the CHIPS water Cherenkov detector has been studied to measure its attenuation length for Cherenkov light as a function of filtering time. A scaled model of the CHIPS detector filled with water from the Wentworth 2W pit, proposed site of the CHIPS deployment, in conjunction with a 3.2 m vertical column filled with this water, was used to study the transmission of 405 nm laser light. Results consistent with attenuation lengths of up to 100 m were observed for this wavelength with filtration and UV sterilization alone.


12th International Workshop on Neutrino Factories, Superbeams, and Betabeams: NuFact10 | 2011

Summary of the Oscillation Physics Working Group

Sandhya Choubey; Thomas Schwetz; P. Vahle

This is a summary of the Oscillation Physics Working Group (WG1) activity at the NuFact10 Conference.


Physical Review Letters | 2009

First Measurement of

P. Adamson; A. A. Aguilar-Arevalo; C. E. Anderson; A. O. Bazarko; M. Bishai; S. J. Brice; B. C. Brown; L. Bugel; J. Cao; B. Choudhary; L. Coney; J. M. Conrad; D. C. Cox; A. Curioni; Z. Djurcic; D. A. Finley; B. T. Fleming; R. Ford; H. R. Gallagher; F. G. Garcia; G. T. Garvey; C. Green; J. A. Green; Deborah A. Harris; T. L. Hart; E. Hawker; J. Hylen; R. Imlay; R. A. Johnson; G. Karagiorgi

We report the first observation of off-axis neutrino interactions in the MiniBooNE detector from the NuMI beam line at Fermilab. The MiniBooNE detector is located 745 m from the NuMI production target, at 110 mrad angle (6.3 degrees) with respect to the NuMI beam axis. Samples of charged-current quasielastic numicro and nue interactions are analyzed and found to be in agreement with expectation. This provides a direct verification of the expected pion and kaon contributions to the neutrino flux and validates the modeling of the NuMI off-axis beam.


Physical Review Letters | 2009

ν_μ

P. Adamson; A. A. Aguilar-Arevalo; C. E. Anderson; A. O. Bazarko; M. Bishai; S. J. Brice; B. C. Brown; L. Bugel; J. Cao; B. Choudhary; L. Coney; J. M. Conrad; D. C. Cox; A. Curioni; Z. Djurcic; D. A. Finley; B. T. Fleming; R. Ford; H. R. Gallagher; F. G. Garcia; G. T. Garvey; C. Green; J. A. Green; D. A. Harris; T. L. Hart; E. Hawker; J. Hylen; R. Imlay; R. A. Johnson; G. Karagiorgi

We report the first observation of off-axis neutrino interactions in the MiniBooNE detector from the NuMI beam line at Fermilab. The MiniBooNE detector is located 745 m from the NuMI production target, at 110 mrad angle (6.3 degrees) with respect to the NuMI beam axis. Samples of charged-current quasielastic numicro and nue interactions are analyzed and found to be in agreement with expectation. This provides a direct verification of the expected pion and kaon contributions to the neutrino flux and validates the modeling of the NuMI off-axis beam.

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K. Lang

University of Texas at Austin

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J. Thomas

University College London

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A. Weber

University of Oxford

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R. Nichol

University College London

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