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Showing papers by "V. M. Gehman published in 2012"


Posted Content
TL;DR: The 2011 Workshop on Fundamental Physics at the Intensity Frontier as discussed by the authors identified and described opportunities at the intensity frontier in the areas of heavy quarks, charged leptons, neutrinos, proton decay, new light weakly-coupled particles, and nucleons, nuclei, and atoms.
Abstract: The Proceedings of the 2011 workshop on Fundamental Physics at the Intensity Frontier. Science opportunities at the intensity frontier are identified and described in the areas of heavy quarks, charged leptons, neutrinos, proton decay, new light weakly-coupled particles, and nucleons, nuclei, and atoms.

157 citations


Journal ArticleDOI
TL;DR: The Next-100 detector as discussed by the authors was designed to search for neutrinoless double beta decay (ββ0ν) in 136XE at the Laboratorio Subterraneo de Canfranc (LSC) in Spain.
Abstract: In this Technical Design Report (TDR) we describe the NEXT-100 detector that will search for neutrinoless double beta decay (ββ0ν) in 136XE at the Laboratorio Subterraneo de Canfranc (LSC), in Spain. The document formalizes the design presented in our Conceptual Design Report (CDR): an electroluminescence time projection chamber, with separate readout planes for calorimetry and tracking, located, respectively, behind cathode and anode. The detector is designed to hold a maximum of about 150 kg of xenon at 15 bar, or 100 kg at 10 bar. This option builds in the capability to increase the total isotope mass by 50% while keeping the operating pressure at a manageable level. The readout plane performing the energy measurement is composed of Hamamatsu R11410-10 photomultipliers, specially designed for operation in low-background, xenon-based detectors. Each individual PMT will be isolated from the gas by an individual, pressure resistant enclosure and will be coupled to the sensitive volume through a sapphire window. The tracking plane consists in an array of Hamamatsu S10362-11-050P MPPCs used as tracking pixels. They will be arranged in square boards holding 64 sensors (8 × 8) with a 1-cm pitch. The inner walls of the TPC, the sapphire windows and the boards holding the MPPCs will be coated with tetraphenyl butadiene (TPB), a wavelength shifter, to improve the light collection.

120 citations


Posted Content
TL;DR: The Next prototype for Double Beta and Dark Matter (NEXT-DBDM) detector was constructed at the Lawrence Berkeley National Laboratory (LBNL) and achieved energy resolution of 0.5% FWHM for the 2,459 keV hypothetical neutrino-less double beta decay peak as mentioned in this paper.
Abstract: We present the design, data and results from the NEXT prototype for Double Beta and Dark Matter (NEXT-DBDM) detector, a high-pressure gaseous natural xenon electroluminescent time projection chamber (TPC) that was built at the Lawrence Berkeley National Laboratory. It is a prototype of the planned NEXT-100 $^{136}$Xe neutrino-less double beta decay ($0 u\beta\beta$) experiment with the main objectives of demonstrating near-intrinsic energy resolution at energies up to 662 keV and of optimizing the NEXT-100 detector design and operating parameters. Energy resolutions of $\sim$1% FWHM for 662 keV gamma rays were obtained at 10 and 15 atm and $\sim$5% FWHM for 30 keV fluorescence xenon X-rays. These results demonstrate that 0.5% FWHM resolutions for the 2,459 keV hypothetical neutrino-less double beta decay peak are realizable. This energy resolution is a factor 7 to 20 better than that of the current leading $0 u\beta\beta$ experiments using liquid xenon and thus represents a significant advancement. We present also first results from a track imaging system consisting of 64 silicon photo-multipliers recently installed in NEXT-DBDM that, along with the excellent energy resolution, demonstrates the key functionalities required for the NEXT-100 $0 u\beta\beta$ search.

62 citations


Journal ArticleDOI
TL;DR: The Next-100 detector as mentioned in this paper was designed to search for neutrinoless double beta decay (bbonu) in Xe-136 at the Laboratorio Subterraneo de Canfranc (LSC) in Spain.
Abstract: In this Technical Design Report (TDR) we describe the NEXT-100 detector that will search for neutrinoless double beta decay (bbonu) in Xe-136 at the Laboratorio Subterraneo de Canfranc (LSC), in Spain. The document formalizes the design presented in our Conceptual Design Report (CDR): an electroluminescence time projection chamber, with separate readout planes for calorimetry and tracking, located, respectively, behind cathode and anode. The detector is designed to hold a maximum of about 150 kg of xenon at 15 bar, or 100 kg at 10 bar. This option builds in the capability to increase the total isotope mass by 50% while keeping the operating pressure at a manageable level. The readout plane performing the energy measurement is composed of Hamamatsu R11410-10 photomultipliers, specially designed for operation in low-background, xenon-based detectors. Each individual PMT will be isolated from the gas by an individual, pressure resistant enclosure and will be coupled to the sensitive volume through a sapphire window. The tracking plane consists in an array of Hamamatsu S10362-11-050P MPPCs used as tracking pixels. They will be arranged in square boards holding 64 sensors (8 times8) with a 1-cm pitch. The inner walls of the TPC, the sapphire windows and the boards holding the MPPCs will be coated with tetraphenyl butadiene (TPB), a wavelength shifter, to improve the light collection.

60 citations


Journal ArticleDOI
TL;DR: In this article, the ionization and scintillation detection properties of xenon gas at 10 bar pressure were investigated using a source of alpha particles in the NEXT-DEMO time projection chamber, in three different drift electric field configurations.
Abstract: High-pressure xenon gas is an attractive detection medium for a variety of applications in fundamental and applied physics. In this paper we study the ionization and scintillation detection properties of xenon gas at 10 bar pressure. For this purpose, we use a source of alpha particles in the NEXT-DEMO time projection chamber, the large scale prototype of the NEXT-100 neutrinoless double beta decay experiment, in three different drift electric field configurations. We measure the ionization electron drift velocity and longitudinal diffusion, and compare our results to expectations based on available electron scattering cross sections on pure xenon. In addition, two types of measurements addressing the connection between the ionization and scintillation yields are performed. On the one hand we observe, for the first time in xenon gas, large event-by-event correlated fluctuations between the ionization and scintillation signals, similar to that already observed in liquid xenon. On the other hand, we study the field dependence of the average scintillation and ionization yields. Both types of measurements may shed light on the mechanism of electron-ion recombination in xenon gas for highly-ionizing particles. Finally, by comparing the response of alpha particles and electrons in NEXT-DEMO, we find no evidence for quenching of the primary scintillation light produced by alpha particles in the xenon gas.

41 citations


Journal ArticleDOI
TL;DR: NEXT-DEMO as discussed by the authors is a large-scale prototype of the NEXT-100 detector, an electroluminescent time projection chamber that will search for the neutrinoless double beta decay of Xe-136 using 100 to 150 kg of enriched xenon gas.
Abstract: NEXT-DEMO is a large-scale prototype of the NEXT-100 detector, an electroluminescent time projection chamber that will search for the neutrinoless double beta decay of Xe-136 using 100 to 150 kg of enriched xenon gas. NEXT-DEMO was built to prove the expected performance of NEXT-100, namely, energy resolution better than 1% FWHM at 2.5 MeV and event topological reconstruction. In this paper we describe the prototype and its initial results. A resolution of 1.75% FWHM at 511 keV (which extrapolates to 0.8% FWHM at 2.5 MeV) was obtained at 10 bar pressure using a gamma-ray calibration source. Also, a basic study of the event topology along the longitudinal coordinate is presented, proving that it is possible to identify the distinct dE/dx of electron tracks in high-pressure xenon using an electroluminescence TPC.

40 citations


Journal ArticleDOI
TL;DR: In this paper, the authors examined the atomic theory behind recent constraints on the violation of the Pauli Exclusion Principle derived from experiments that look for X-rays emitted from conductors while a large current is present.
Abstract: We have examined the atomic theory behind recent constraints on the violation of the Pauli Exclusion Principle derived from experiments that look for X-rays emitted from conductors while a large current is present. We also re-examine the assumptions underlying such experiments. We use the results of these studies to assess pilot measurements to develop an improved test of the Principle. We present an improved limit of $\frac{1}{2}\beta^{2} < 2.6\times10^{-39}$ on the Pauli Exclusion Principle. This limit is the best to date for interactions between a system of fermions and a fermion that has not previously interacted with that given system. That is, for systems that do not obviously violate the Messiah-Greenberg symmetrization-postulate selection rule.

38 citations


Journal ArticleDOI
J. F. Wilkerson1, J. F. Wilkerson2, J. F. Wilkerson3, E. Aguayo4, F. T. Avignone3, F. T. Avignone5, Henning O. Back2, Henning O. Back6, A. S. Barabash, J. R. Beene3, M. Bergevin7, F. E. Bertrand3, M. Boswell8, V. B. Brudanin9, Matthew Busch10, Yuen-Dat Chan7, C. D. Christofferson11, J. I. Collar12, D. C. Combs2, D. C. Combs6, Reynold J. Cooper3, J. A. Detwiler7, P. J. Doe13, Yu. Efremenko14, V. G. Egorov9, H. Ejiri15, S. R. Elliott8, J. Esterline2, J. Esterline10, James E. Fast4, N. Fields12, P. Finnerty1, P. Finnerty2, F. M. Fraenkle1, F. M. Fraenkle2, V. M. Gehman8, G. K. Giovanetti10, G. K. Giovanetti16, M. P. Green2, M. P. Green1, V. E. Guiseppe17, K. Gusey9, A. L. Hallin18, Ryuta Hazama15, Reyco Henning2, Reyco Henning1, Eric W. Hoppe4, M. Horton11, Stanley M. Howard11, M. A. Howe2, M. A. Howe1, R. A. Johnson13, K. J. Keeter16, C. Keller17, M. F. Kidd8, A. Knecht13, O.I. Kochetov9, S. I. Konovalov, Richard T. Kouzes4, Brian D. LaFerriere4, B. H. LaRoque8, Jonathan D. Leon13, L. E. Leviner2, L. E. Leviner6, J. C. Loach7, S. MacMullin1, S. MacMullin2, Michael G. Marino13, R. D. Martin7, Dongming Mei17, J. H. Merriman4, M. L. Miller13, L. Mizouni5, L. Mizouni4, Masaharu Nomachi15, John L. Orrell4, Nicole R. Overman4, D. G. Phillips1, D. G. Phillips2, A. W. P. Poon7, G. Perumpilly17, G. Prior7, D. C. Radford3, Keith Rielage8, R. G. H. Robertson13, M. C. Ronquest8, Alexis G. Schubert13, Tatsushi Shima15, M. Shirchenko9, K. J. Snavely1, K. J. Snavely2, D. Steele8, J. Strain2, J. Strain1, Keenan Thomas17, V. V. Timkin9, Werner Tornow2, Werner Tornow10, I. Vanyushin, R. L. Varner3, Kai Vetter7, K. Vorren2, K. Vorren8, E. Yakushev9, A. R. Young2, A. R. Young6, C.-H. Yu3, Vladimir Yumatov, Chao Zhang17 
30 Jul 2012
TL;DR: The MAJORANA collaboration is constructing the DEMONSTRATOR, an array consisting of 40 kg of p-type point contact germanium detectors, at least half of which will be enriched to 86% in 76Ge.
Abstract: The observation of neutrino less double-beta decay would show that neutrinos are Majorana particles and provide information on neutrino mass. Attaining sensitivities for neutrino masses in the inverted hierarchy region requires large, tonne scale detectors with extremely low backgrounds, at the level of 10−3 counts keV−1 t−1 y−1 or lower in the region of the signal. The MAJORANA collaboration is constructing the DEMONSTRATOR, an array consisting of 40 kg of p-type point contact germanium detectors, at least half of which will be enriched to 86% in 76Ge. The primary aim is to show the feasibility for a future tonne scale measurement. With a sub-keV energy threshold, the array should also be able to search for light WIMP dark matter. This paper presents a brief update on the status of constructing the DEMONSTRATOR including an electroforming facility that is now operating underground at the Sanford Underground Research Facility.

24 citations


Journal ArticleDOI
TL;DR: The Neutrino Experiment with a Xenon TPC (NEXT) as mentioned in this paper is intended to investigate the neutrinoless double beta decay of 136Xe, which requires a severe suppression of potential backgrounds.
Abstract: The Neutrino Experiment with a Xenon TPC (NEXT) is intended to investigate the neutrinoless double beta decay of 136Xe, which requires a severe suppression of potential backgrounds. An extensive screening and material selection process is underway for NEXT since the control of the radiopurity levels of the materials to be used in the experimental set-up is a must for rare event searches. First measurements based on Glow Discharge Mass Spectrometry and gamma-ray spectroscopy using ultra-low background germanium detectors at the Laboratorio Subterraneo de Canfranc (Spain) are described here. Activity results for natural radioactive chains and other common radionuclides are summarized, being the values obtained for some materials like copper and stainless steel very competitive. The implications of these results for the NEXT experiment are also discussed.

20 citations


Journal ArticleDOI
D. G. Phillips1, D. G. Phillips2, E. Aguayo3, F. T. Avignone4, F. T. Avignone5, Henning O. Back6, Henning O. Back1, A. S. Barabash, M. Bergevin7, F. E. Bertrand5, M. Boswell8, V. B. Brudanin9, Matthew Busch1, Matthew Busch10, Yuen-Dat Chan7, C. D. Christofferson11, J. I. Collar12, D. C. Combs6, D. C. Combs1, Reynold J. Cooper5, J. A. Detwiler7, P. J. Doe13, V. Efremenko14, V. G. Egorov9, H. Ejiri15, S. R. Elliott8, J. Esterline10, J. Esterline1, James E. Fast3, N. Fields12, P. Finnerty2, P. Finnerty1, F. M. Fraenkle1, F. M. Fraenkle2, V. M. Gehman8, G. K. Giovanetti2, G. K. Giovanetti1, M. P. Green2, M. P. Green1, V. E. Guiseppe16, K. Gusey9, A. L. Hallin17, Ryuta Hazama15, Reyco Henning2, Reyco Henning1, Andrew Hime8, Eric W. Hoppe3, M. Horton11, Stanley M. Howard11, M. A. Howe1, M. A. Howe2, R. A. Johnson13, K. J. Keeter18, C. Keller16, M. F. Kidd8, A. Knecht13, O.I. Kochetov9, S. I. Konovalov, Richard T. Kouzes3, Brian D. LaFerriere3, B. H. LaRoque8, Jonathan D. Leon13, L. E. Leviner1, L. E. Leviner6, J. C. Loach7, S. MacMullin2, S. MacMullin1, Michael G. Marino13, R. D. Martin7, Dongming Mei16, J. H. Merriman3, M. L. Miller13, L. Mizouni4, L. Mizouni3, Masaharu Nomachi15, John L. Orrell3, Nicole R. Overman3, A. W. P. Poon7, G. Perumpilly16, G. Prior7, D. C. Radford5, Keith Rielage8, R. G. H. Robertson13, M. C. Ronquest8, Alexis G. Schubert13, Tatsushi Shima15, M. Shirchenko9, K. J. Snavely2, K. J. Snavely1, D. Steele8, J. Strain1, J. Strain2, Keenan Thomas16, V. V. Timkin9, Werner Tornow10, Werner Tornow1, I. Vanyushin, R. L. Varner5, Kai Vetter7, Kai Vetter19, K. Vorren2, K. Vorren1, J. F. Wilkerson2, J. F. Wilkerson1, J. F. Wilkerson5, B. A. Wolfe13, E. Yakushev9, A. R. Young6, A. R. Young1, C.-H. Yu5, Vladimir Yumatov, Chao Zhang16 
18 Sep 2012
TL;DR: The initial phase of the MAJORANA experiment, known as the DEMONSTRATOR, will house 40 kg of Ge in an ultra-low background shielded environment at the 4850' level of the Sanford Underground Laboratory in Lead, SD as mentioned in this paper.
Abstract: The observation of neutrinoless double-beta decay would resolve the Majorana nature of the neutrino and could provide information on the absolute scale of the neutrino mass. The initial phase of the MAJORANA experiment, known as the DEMONSTRATOR, will house 40 kg of Ge in an ultra-low background shielded environment at the 4850' level of the Sanford Underground Laboratory in Lead, SD. The objective of the DEMONSTRATOR is to determine whether a future 1-tonne experiment can achieve a background goal of one count per tonne-year in a narrow region of interest around the 76Ge neutrinoless double-beta decay peak.

17 citations


Journal ArticleDOI
G. K. Giovanetti1, G. K. Giovanetti2, E. Aguayo3, F. T. Avignone4, F. T. Avignone5, Henning O. Back6, Henning O. Back7, A. S. Barabash, J. R. Beene4, M. Bergevin8, F. E. Bertrand4, M. Boswell9, V. B. Brudanin10, Matthew Busch6, Matthew Busch1, Yuen-Dat Chan8, C. D. Christofferson11, J. I. Collar12, D. C. Combs7, D. C. Combs6, Reynold J. Cooper4, J. A. Detwiler8, P. J. Doe13, Yu. Efremenko14, V. G. Egorov10, H. Ejiri15, S. R. Elliott9, J. Esterline6, J. Esterline1, James E. Fast3, N. Fields12, P. Finnerty6, P. Finnerty16, F. M. Fraenkle6, F. M. Fraenkle16, V. M. Gehman9, M. P. Green16, M. P. Green6, V. E. Guiseppe17, K. Gusey10, A. L. Hallin18, Ryuta Hazama15, Reyco Henning16, Reyco Henning6, Eric W. Hoppe3, M. Horton11, Stanley M. Howard11, M. A. Howe6, M. A. Howe16, R. A. Johnson13, K. J. Keeter2, C. Keller17, M. F. Kidd9, A. Knecht13, O.I. Kochetov10, S. I. Konovalov, Richard T. Kouzes3, Brian D. LaFerriere3, B. H. LaRoque9, Jonathan D. Leon13, L. E. Leviner7, L. E. Leviner6, J. C. Loach8, S. MacMullin6, S. MacMullin16, Michael G. Marino13, R. D. Martin8, Dongming Mei17, J. H. Merriman3, M. L. Miller13, L. Mizouni3, L. Mizouni5, Masaharu Nomachi15, John L. Orrell3, Nicole R. Overman3, D. G. Phillips16, D. G. Phillips6, Alan Poon8, G. Perumpilly17, G. Prior8, D. C. Radford4, Keith Rielage9, R. G. H. Robertson13, M. C. Ronquest9, Alexis G. Schubert13, Tatsushi Shima15, M. Shirchenko10, K. J. Snavely6, K. J. Snavely16, D. Steele9, J. Strain6, J. Strain16, Keenan Thomas17, V. V. Timkin10, Werner Tornow6, Werner Tornow1, I. Vanyushin, R. L. Varner4, Kai Vetter8, K. Vorren6, K. Vorren9, J. F. Wilkerson16, J. F. Wilkerson6, J. F. Wilkerson4, E. Yakushev10, A. R. Young7, A. R. Young6, C.-H. Yu4, Vladimir Yumatov, Chao Zhang17 
30 Jul 2012
TL;DR: The Majorana Demonstrator as mentioned in this paper is an array of natural and enriched high purity germanium detectors that will search for the neutrinoless double-beta decay of Germanium-76 and perform a search for weakly interacting massive particles with masses below 10 GeV.
Abstract: The Majorana Demonstrator is an array of natural and enriched high purity germanium detectors that will search for the neutrinoless double-beta decay of Germanium-76 and perform a search for weakly interacting massive particles with masses below 10 GeV. To reach the background rate goal in the neutrinoless double-beta decay region of interest of 4 counts/keV/t/y, the DEMONSTRATOR will utilize a number of background reduction strategies, including a time-correlated event cut for 68Ge that requires a sub-keV energy threshold. This low energy threshold allows the DEMONSTRATOR to extend its physics reach to include a search for light WIMPs. We will discuss the detector systems and data analysis techniques required to achieve sub-keV thresholds as well as present the projected dark matter sensitivities of the Majorana Demonstrator.


Posted Content
TL;DR: In this article, a novel 3D imaging concept using SiPMs coated with tetraphenyl butadiene (TPB) for the EL read out and its first implementation in NEXT-DEMO, a large-scale prototype of the NEXT-100 experiment is presented.
Abstract: NEXT-100 experiment aims at searching the neutrinoless double-beta decay of the Xe-136 isotope using a TPC filled with a 100 kg of high-pressure gaseous xenon, with 90% isotopic enrichment. The experiment will take place at the Laboratorio Subterraneo de Canfranc (LSC), Spain. NEXT-100 uses electroluminescence (EL) technology for energy measurement with a resolution better than 1% FWHM. The gaseous xenon in the TPC additionally allows the tracks of the two beta particles to be recorded, which are expected to have a length of up to 30 cm at 10 bar pressure. The ability to record the topological signature of the neutrinoless double-beta events provides a powerful background rejection factor for the double-beta experiment. In this paper, we present a novel 3D imaging concept using SiPMs coated with tetraphenyl butadiene (TPB) for the EL read out and its first implementation in NEXT-DEMO, a large-scale prototype of the NEXT-100 experiment. The design and the first characterization measurements of the NEXT-DEMO SiPM tracking system are presented. The SiPM response uniformity over the tracking plane drawn from its gain map is shown to be better than 4%. An automated active control system for the stabilization of the SiPMs gain was developed, based on the voltage supply compensation of the gain drifts. The gain is shown to be stabilized within 0.2% relative variation around its nominal value, provided by Hamamatsu, in a temperature range of 10 degree C. The noise level from the electronics and the SiPM dark noise is shown to lay typically below the level of 10 photoelectrons (pe) in the ADC. Hence, a detection threshold at 10 pe is set for the acquisition of the tracking signals. The ADC full dynamic range (4096 channels) is shown to be adequate for signal levels of up to 200 pe/microsecond, which enables recording most of the tracking signals.

Journal ArticleDOI
TL;DR: In this paper, the Majorana Experiment was used to search for the neutrinoless double-beta decay of 76Ge using arrays of enriched HPGe detectors, and measurements were performed to quantitatively assess this background.
Abstract: The Majorana Experiment will use arrays of enriched HPGe detectors to search for the neutrinoless double-beta decay of 76Ge. Such a decay, if found, would show lepton-number violation and confirm the Majorana nature of the neutrino. Searches for such rare events are hindered by obscuring backgrounds which must be understood and mitigated as much as possible. A potentially important background contribution to this and other double-beta decay experiments could come from decays of alpha-emitting isotopes in the 232Th and 238U decay chains on or near the surfaces of the detectors. An alpha particle emitted external to an HPGe crystal can lose energy before entering the active region of the detector, either in some external-bulk material or within the dead region of the crystal. The measured energy of the event will only correspond to a partial amount of the total kinetic energy of the alpha and might obscure the signal from neutrinoless double-beta decay. A test stand was built and measurements were performed to quantitatively assess this background. We present results from these measurements and compare them to simulations using Geant4. These results are then used to measure the alpha backgrounds in an underground detector in situ. We also make estimates of surface contamination tolerances for double-beta decay experiments using solid-state detectors.

Posted Content
TL;DR: In this article, the authors used the primary scintillation produced by X-rays to induce a single photoelectron response of the PMT and determined the peak position of such response relative to the pedestal peak.
Abstract: We have investigated the possibility of calibrating the PMTs of scintillation detectors, using the primary scintillation produced by X-rays to induce single photoelectron response of the PMT. The high-energy tail of this response, can be approximated to an exponential function, under some conditions. In these cases, it is possible to determine the average gain for each PMT biasing voltage from the inverse of the exponent of the exponential fit to the tail, which can be done even if the background and/or noise cover-up most of the distribution. We have compared our results with those obtained by the commonly used single electron response (SER) method, which uses a LED to induce a single photoelectron response of the PMT and determines the peak position of such response, relative to the pedestal peak (the electronic noise peak, which corresponds to 0 photoelectrons). The results of the exponential fit method agree with those obtained by the SER method when the average number of photoelectrons reaching the first dynode per light/scintillation pulse is around 1.0. The SER method has higher precision, while the exponential fit method has the advantage of being useful in situations where the PMT is already in situ, being difficult or even impossible to apply the SER method, e.g. in sealed scintillator/PMT devices.