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Advances in High Energy Physics | 2014

The MAJORANA DEMONSTRATOR Neutrinoless Double-Beta Decay Experiment

N. Abgrall; E. Aguayo; Frank T. Avignone; A. S. Barabash; F. E. Bertrand; Melissa Boswell; V. Brudanin; M. Busch; A. S. Caldwell; Y.D. Chan; C. D. Christofferson; D. C. Combs; J. A. Detwiler; P. J. Doe; Y. V. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; J. Esterline; J. E. Fast; P. Finnerty; F. M. Fraenkle; A. Galindo-Uribarri; G. K. Giovanetti; J. Goett; M. P. Green; J. Gruszko; V. E. Guiseppe; K. Gusev; A. L. Hallin

The MAJORANA DEMONSTRATOR will search for the neutrinoless double-beta decay of the isotope Ge with a mixed array of enriched and natural germanium detectors. The observation of this rare decay would indicate that the neutrino is its own antiparticle, demonstrate that lepton number is not conserved, and provide information on the absolute mass scale of the neutrino. The DEMONSTRATOR is being assembled at the 4850-foot level of the Sanford Underground Research Facility in Lead, South Dakota. The array will be situated in a low-background environment and surrounded by passive and active shielding. Here we describe the science goals of the DEMONSTRATOR and the details of its design.


arXiv: Nuclear Experiment | 2012

The MAJORANA demonstrator: A search for neutrinoless double-beta decay of germanium-76

J. F. Wilkerson; E. Aguayo; Frank T. Avignone; H. O. Back; A. S. Barabash; James R. Beene; M. Bergevin; F. E. Bertrand; Melissa Boswell; V. Brudanin; M. Busch; Y.D. Chan; C. D. Christofferson; J. I. Collar; D. C. Combs; R. J. Cooper; J. A. Detwiler; P. J. Doe; Yu. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; J. Esterline; J. E. Fast; N. Fields; P. Finnerty; F. M. Fraenkle; V. M. Gehman; G K Giovanetti; M. P. Green

The observation of neutrinoless double-beta decay would determine whether the neutrino is a Majorana particle and provide information on the absolute scale of neutrino mass. The MAJORANA Collaboration is constructing the DEMONSTRATOR, an array of germanium detectors, to search for neutrinoless double-beta decay of 76-Ge. The DEMONSTRATOR will contain 40 kg of germanium; up to 30 kg will be enriched to 86% in 76-Ge. The DEMONSTRATOR will be deployed deep underground in an ultra-low-background shielded environment. Operation of the DEMONSTRATOR aims to determine whether a future tonne-scale germanium experiment can achieve a background goal of one count per tonne-year in a 4-keV region of interest around the 76-Ge neutrinoless double-beta decay Q-value of 2039 keV.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016

The Majorana Demonstrator radioassay program

N. Abgrall; I. J. Arnquist; F. T. Avignone; H. O. Back; A. S. Barabash; F. E. Bertrand; Melissa Boswell; A. W. Bradley; V. Brudanin; M. Busch; M. Buuck; D. Byram; A. S. Caldwell; Y.D. Chan; C. D. Christofferson; Pinghan Chu; C. Cuesta; J. A. Detwiler; J. A. Dunmore; Yu. Efremenko; H. Ejiri; S. R. Elliott; P. Finnerty; A. Galindo-Uribarri; V. M. Gehman; T. Gilliss; G. K. Giovanetti; J. Goett; M. P. Green; J. Gruszko

Abstract The Majorana collaboration is constructing the Majorana Demonstrator at the Sanford Underground Research Facility at the Homestake gold mine, in Lead, SD. The apparatus will use Ge detectors, enriched in isotope 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. The radioassay program conducted by the collaboration to ensure that the materials comprising the apparatus are sufficiently pure is described. The resulting measurements from gamma-ray counting, neutron activation and mass spectroscopy of the radioactive-isotope contamination for the materials studied for use in the detector are reported. We interpret these numbers in the context of the expected background for the experiment.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015

Focal-plane detector system for the KATRIN experiment

J.F. Amsbaugh; J. Barrett; A. Beglarian; Till Bergmann; H. Bichsel; L. I. Bodine; J. Bonn; N.M. Boyd; T.H. Burritt; Z. Chaoui; Suren Chilingaryan; T.J. Corona; P. J. Doe; J.A. Dunmore; S. Enomoto; Joseph A. Formaggio; F.M. Fränkle; D. Furse; H. Gemmeke; F. Glück; F. Harms; G. Harper; J. Hartmann; M. A. Howe; A. Kaboth; J. Kelsey; M. Knauer; Andreas Kopmann; M. Leber; E.L. Martin

Abstract The focal-plane detector system for the KArlsruhe TRItium Neutrino (KATRIN) experiment consists of a multi-pixel silicon p-i-n-diode array, custom readout electronics, two superconducting solenoid magnets, an ultra high-vacuum system, a high-vacuum system, calibration and monitoring devices, a scintillating veto, and a custom data-acquisition system. It is designed to detect the low-energy electrons selected by the KATRIN main spectrometer. We describe the system and summarize its performance after its final installation.


arXiv: Instrumentation and Detectors | 2017

The Large Enriched Germanium Experiment for Neutrinoless Double Beta Decay (LEGEND)

N. Abgrall; A. Abramov; N. Abrosimov; I. Abt; M. Agostini; M. Agartioglu; A. Ajjaq; S. I. Alvis; F. T. Avignone; X. Bai; M. Balata; I. Barabanov; A. S. Barabash; P. J. Barton; L. Baudis; L. Bezrukov; T. Bode; A. Bolozdynya; D. Borowicz; A. J. Boston; H. Boston; S. T.P. Boyd; R. Breier; V. Brudanin; R. Brugnera; M. Busch; M. Buuck; A. Caldwell; T. S. Caldwell; T. Camellato

The observation of neutrinoless double-beta decay (0νββ) would show that lepton number is violated, reveal that neu-trinos are Majorana particles, and provide information on neutrino mass. A discovery-capable experiment covering the inverted ordering region, with effective Majorana neutrino masses of 15 - 50 meV, will require a tonne-scale experiment with excellent energy resolution and extremely low backgrounds, at the level of ∼0.1 count /(FWHM·t·yr) in the region of the signal. The current generation 76Ge experiments GERDA and the Majorana Demonstrator, utilizing high purity Germanium detectors with an intrinsic energy resolution of 0.12%, have achieved the lowest backgrounds by over an order of magnitude in the 0νββ signal region of all 0νββ experiments. Building on this success, the LEGEND collaboration has been formed to pursue a tonne-scale 76Ge experiment. The collaboration aims to develop a phased 0νββ experimental program with discovery potential at a half-life approaching or at 1028 years, using existing resources as appropriate to expedite physics results.


arXiv: Nuclear Experiment | 2009

The MAJORANA DEMONSTRATOR: An R&D project towards a tonne-scale germanium neutrinoless double-beta decay search

Mark Amman; J. F. Amsbaugh; Frank T. Avignone; H. O. Back; A. S. Barabash; P.S. Barbeau; James R. Beene; M. Bergevin; F. E. Bertrand; M. Boswell; V. Brudanin; W. Bugg; T. H. Burritt; Y.D. Chan; J. I. Collar; R. J. Cooper; Richard J. Creswick; J. A. Detwiler; P. J. Doe; Yu. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; James H. Ely; J. Esterline; Horacio A. Farach; J. E. Fast; N. Fields; P. Finnerty; B. K. Fujikawa

The MAJORANA collaboration is pursuing the development of the so‐called MAJORANA DEMONSTRATOR. The DEMONSTRATOR is intended to perform research and development towards a tonne‐scale germanium‐based experiment to search for the neutrinoless double‐beta decay of 76Ge. The DEMONSTRATOR can also perform a competitive direct dark matter search for light WIMPs in the 1–10 GeV/c2 mass range. It will consist of approximately 60 kg of germanium detectors in an ultra‐low background shield located deep underground at the Sanford Underground Laboratory in Lead, SD. The DEMONSTRATOR will also perform background and technology studies, and half of the detector mass will be enriched germanium. This talk will review the motivation, design, technology and status of the Demonstrator.


ieee nuclear science symposium | 2008

FPGA-based DAQ system for multi-channel detectors

Andreas Kopmann; Till Bergmann; Hartmut Gemmeke; M. A. Howe; M. Kleifges; A. Menshikov; D. Tcherniakhovski; J. F. Wilkerson; Sascha Wüstling

In this article a data acquisition (DAQ) system is presented consisting of FPGA-based electronics and an object-oriented readout software that has been developed for the needs of multi-channel detectors. The design goal of the DAQ electronics was to develop an affordable and scalable multi-channel system that is flexible enough to be easily adapted to the experiment requirements. The analog circuitry is integrated on separate analog boards for easy adaptation to different experiments. The heart of the electronics is a hierarchical system of up to 81 FPGAs organized in three layers. It digitizes up to 480 channels with 12 bit ADCs at 10 to 40MHz sampling rate. The electronics are interfaced by a PCI-bridge to a commercial Processor PMC board.


ieee nuclear science symposium | 2008

Integration of embedded single board computers into an object-oriented software bus DAQ application

M. A. Howe; M. G. Marino; J. F. Wilkerson

The integration of Linux-based single board computers (SBC) into data acquisition systems is often complex and requires large amounts of custom software resulting in non-reusable applications. Extending the concepts of the ‘object-oriented software bus’ to include single board computers results in a system where the SBC code is dynamically managed, loaded, compiled, and launched by a remote application (ORCA - Object-oriented Real-time Control and Acquisition) that makes it easy to support diverse sets of hardware (i.e. VME, compact-PCI, etc.). In ORCA, the SBC code is separated into two parts. One part is general and implements the low-level communication protocol, the socket connection, and data transfer via circular buffer. The other part is specific and contains small amounts of custom code for each type of hardware. At run-time the SBC code is dynamically assembled into a download package that is transferred to the SBC, compiled, and started. A data structure defining the hardware readout order is also downloaded. The use of SBCs with VME and CompactPCI hardware is discussed. It is shown how the combination of an SBC and ORCA results in a dynamically configurable data acquisition system.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2015

The Majorana Parts Tracking Database

N. Abgrall; E. Aguayo; F. T. Avignone; A. S. Barabash; F. E. Bertrand; V. Brudanin; M. Busch; D. Byram; A. S. Caldwell; Y-D. Chan; C. D. Christofferson; D. C. Combs; C. Cuesta; J. A. Detwiler; P. J. Doe; Yu. Efremenko; V. Egorov; H. Ejiri; S. R. Elliott; J. Esterline; J. E. Fast; P. Finnerty; F. M. Fraenkle; A. Galindo-Uribarri; G. K. Giovanetti; J. Goett; M. P. Green; J. Gruszko; V. E. Guiseppe; K. Gusev

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. Transportation, storage, and processes undergone by parts such as machining or cleaning are linked to part records. Tracking parts provides a great logistics benefit and an important quality a ssurance reference during construction. In addition, the l ocation history of parts provides an estimate of their exposure to cosmic radiation. A web application for data entry and a radiation exposure calculator have been developed as tools for achieving the extreme radio-purity required for this rare decay search.


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2014

Dead layer on silicon p–i–n diode charged-particle detectors

B. L. Wall; J.F. Amsbaugh; A. Beglarian; T. Bergmann; H. Bichsel; L. I. Bodine; N.M. Boyd; T.H. Burritt; Z. Chaoui; T.J. Corona; P. J. Doe; S. Enomoto; F. Harms; G. Harper; M. A. Howe; E.L. Martin; D. Parno; D.A. Peterson; L. Petzold; P. Renschler; R. G. H. Robertson; J. Schwarz; M. Steidl; T.D. Van Wechel; Brent A. VanDevender; S. Wüstling; K. J. Wierman; J. F. Wilkerson

Semiconductor detectors in general have a dead layer at their surfaces that is either a result of natural or induced passivation, or is formed during the process of making a contact. Charged particles passing through this region produce ionization that is incompletely collected and recorded, which leads to departures from the ideal in both energy deposition and resolution. The silicon p–i–n diode used in the KATRIN neutrino-mass experiment has such a dead layer. We have constructed a detailed Monte Carlo model for the passage of electrons from vacuum into a silicon detector, and compared the measured energy spectra to the predicted ones for a range of energies from 12 to 20 keV. The comparison provides experimental evidence that a substantial fraction of the ionization produced in the “dead” layer evidently escapes by diffusion, with 46% being collected in the depletion zone and the balance being neutralized at the contact or by bulk recombination. The most elementary model of a thinner dead layer from which no charge is collected is strongly disfavored.

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F. E. Bertrand

Oak Ridge National Laboratory

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C. D. Christofferson

South Dakota School of Mines and Technology

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J. A. Detwiler

University of Washington

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S. R. Elliott

Los Alamos National Laboratory

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V. Brudanin

Joint Institute for Nuclear Research

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G. K. Giovanetti

University of North Carolina at Chapel Hill

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V. E. Guiseppe

University of South Dakota

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