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  3. Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
  4. 2014
Showing papers in "Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment in 2014"
Journal Article•10.1016/J.NIMA.2014.07.029•
Mantid - Data Analysis and Visualization Package for Neutron Scattering and $μ SR$ Experiments

[...]

Owen Arnold1, Jean-Christophe Bilheux2, Jose M. Borreguero2, A. Buts1, Stuart I. Campbell2, Laurent Chapon1, Mathieu Doucet2, Nick Draper1, R. Ferraz Leal, M. Gigg1, Vickie E. Lynch2, Anders J. Markvardsen1, D.J. Mikkelson2, D.J. Mikkelson3, R.L. Mikkelson3, R.L. Mikkelson2, Ross Miller2, K. Palmen1, Peter G. Parker1, G. Passos1, Toby Perring1, Peter F. Peterson2, Shelly Ren2, Michael A. Reuter2, Andrei T. Savici2, Jon W. Taylor1, R.J. Taylor2, R. Tolchenov1, Wenduo Zhou2, Janik L. Zikovsky2 •
Rutherford Appleton Laboratory1, Oak Ridge National Laboratory2, University of Wisconsin–Stout3
11 Nov 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: The Mantid framework as discussed by the authors is a software solution developed for the analysis and visualization of neutron scattering and muon spin measurements, which is jointly developed by software engineers and scientists at the ISIS Neutron and Muon Facility and the Oak Ridge National Laboratory.
Abstract: The Mantid framework is a software solution developed for the analysis and visualization of neutron scattering and muon spin measurements. The framework is jointly developed by software engineers and scientists at the ISIS Neutron and Muon Facility and the Oak Ridge National Laboratory. The objectives, functionality and novel design aspects of Mantid are described.

1,607 citations

Journal Article•10.1016/J.NIMA.2014.06.008•
Technology developments and first measurements of Low Gain Avalanche Detectors (LGAD) for high energy physics applications

[...]

Giulio Pellegrini1, Pablo Fernandez-Martinez1, M. Baselga1, C. Fleta1, David Flores1, V. Greco1, Salvador Hidalgo1, Igor Mandić2, Gregor Kramberger2, David Quirion1, Miguel Ullan1 •
Spanish National Research Council1, Jožef Stefan Institute2
21 Nov 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, the authors introduce a new concept of silicon radiation detector with intrinsic multiplication of the charge, called Low Gain Avalanche Detector (LGAD), which is based on the standard Avalanche Photo Diodes (APD) normally used for optical and X-ray detection applications.
Abstract: This paper introduces a new concept of silicon radiation detector with intrinsic multiplication of the charge, called Low Gain Avalanche Detector (LGAD). These new devices are based on the standard Avalanche Photo Diodes (APD) normally used for optical and X-ray detection applications. The main differences to standard APD detectors are the low gain requested to detect high energy charged particles, and the possibility to have fine segmentation pitches: this allows fabrication of microstrip or pixel devices which do not suffer from the limitations normally found [1] in avalanche detectors. In addition, a moderate multiplication value will allow the fabrication of thinner devices with the same output signal of standard thick substrates. The investigation of these detectors provides important indications on the ability of such modified electrode geometry to control and optimize the charge multiplication effect, in order to fully recover the collection efficiency of heavily irradiated silicon detectors, at reasonable bias voltage, compatible with the voltage feed limitation of the CERN High Luminosity Large Hadron Collider (HL-LHC) experiments [2] . For instance, the inner most pixel detector layers of the ATLAS tracker will be exposed to fluences up to 2×10 16 1 MeV n eq /cm 2 , while for the inner strip detector region fluences of 1×10 15 n eq /cm 2 are expected. The gain implemented in the non-irradiated devices must retain some effect also after irradiation, with a higher multiplication factor with respect to standard structures, in order to be used in harsh environments such those expected at collider experiments.

421 citations

Journal Article•10.1016/J.NIMA.2013.12.053•
Design, calibration, and performance of the MINERvA detector

[...]

L. Aliaga1, L. Aliaga2, L. Bagby3, B. Baldin3, A. Baumbaugh2, Arie Bodek4, R. Bradford4, William Brooks5, D. J. Boehnlein3, S. Boyd6, H. S. Budd4, Anatoly Butkevich7, D. A. Martinez Caicedo8, C. M. Castromonte8, M.E. Christy9, J. Chvojka4, H. da Motta, D.S. Damiani1, I. Z. Danko6, Mousumi Datta8, R. DeMaat3, J. Devan1, E. Draeger9, S. A. Dytman6, G. A. Díaz2, B. Eberly6, D.A. Edmondson1, Julián Félix10, L. Fields11, G. A. Fiorentini, R. Flight4, A. M. Gago2, H. R. Gallagher12, C.A. George6, J.A. Gielata4, C. Gingu3, B. Gobbi11, R. Gran8, J. Grange13, N. Grossman3, D. A. Harris3, J. Heaton9, A. Higuera10, Jennifer Hobbs11, I.J. Howley1, K. Hurtado14, M. Jerkins15, T. Kafka12, M.O. Kantner1, C. E. Keppel8, J. Kilmer3, M. Kordosky1, A.H. Krajeski1, G. J. Kumbartzki16, H. Lee4, A.G. Leister1, George Locke16, G. Maggi5, E. Maher17, S. Manly4, W. A. Mann12, C. M. Marshall4, K. S. McFarland4, C.L. McGivern5, A. M. McGowan4, A. Mislivec4, Jorge G. Morfin3, J. Mousseau13, D. Naples6, J. K. Nelson1, G. Niculescu18, I. Niculescu18, C.D. O'Connor1, N. Ochoa2, J. Olsen3, B. Osmanov13, J. Osta3, J. L. Palomino, V. Paolone6, J. Park4, Gabriel Perdue4, C. Peña5, Anna Pla-Dalmau3, L. Rakotondravohitra3, Ronald Ransome16, H. Ray13, L. Ren6, P. Rubinov3, Cody Rude9, K.E. Sassin1, H. Schellman11, D. W. Schmitz19, D. W. Schmitz3, R.M. Schneider1, E. Schulte16, C. Simon20, F. D. Snider3, M.C. Snyder1, C. J. Solano Salinas14, N. Tagg21, B. G. Tice16, R. N. Tilden11, G. Tzanakos22, J.P. Velásquez2, T. Walton8, A. Westerberg9, J. Wolcott4, B.A. Wolthuis1, Natasha Woodward9, T. P. Wytock11, G. Zavala10, H.B. Zeng4, D. Zhang1, L.Y. Zhu8, B. P. Ziemer20 •
College of William & Mary1, Pontifical Catholic University of Peru2, Fermilab3, University of Rochester4, Federico Santa María Technical University5, University of Pittsburgh6, Russian Academy of Sciences7, Hampton University8, University of Minnesota9, Universidad de Guanajuato10, Northwestern University11, Tufts University12, University of Florida13, National University of Engineering14, University of Texas at Austin15, Rutgers University16, Massachusetts College of Liberal Arts17, James Madison University18, University of Chicago19, University of California, Irvine20, Otterbein University21, National and Kapodistrian University of Athens22
11 Apr 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: The MINERvA detector as mentioned in this paper is composed of a finely segmented scintillator-based inner tracking region surrounded by electromagnetic and hadronic sampling calorimetry.
Abstract: The MINERvA 6 experiment is designed to perform precision studies of neutrino-nucleus scattering using ν μ and ν ¯ μ neutrinos incident at 1–20 GeV in the NuMI beam at Fermilab. This article presents a detailed description of the MINERvA detector and describes the ex situ and in situ techniques employed to characterize the detector and monitor its performance. The detector is composed of a finely segmented scintillator-based inner tracking region surrounded by electromagnetic and hadronic sampling calorimetry. The upstream portion of the detector includes planes of graphite, iron and lead interleaved between tracking planes to facilitate the study of nuclear effects in neutrino interactions. Observations concerning the detector response over sustained periods of running are reported. The detector design and methods of operation have relevance to future neutrino experiments in which segmented scintillator tracking is utilized.

248 citations

Journal Article•10.1016/J.NIMA.2014.07.052•
Test of a single module of the J-PET scanner based on plastic scintillators

[...]

Paweł Moskal1, Sz. Niedźwiecki1, Tomasz Bednarski1, Eryk Czerwiński1, Łukasz Kapłon1, Łukasz Kapłon2, Ewelina Kubicz1, I. Moskal1, Monika Pawlik-Niedźwiecka1, Neha Gupta Sharma1, Michał Silarski1, Marcin Zieliński1, N. Zoń1, Piotr Białas1, Aleksander Gajos1, Andrzej Kochanowski1, Grzegorz Korcyl1, Janusz Kowal1, Paweł Kowalski, Tomasz Kozik1, Wojciech Krzemien1, Marcin Molenda1, Marek Palka1, Lech Raczyński, Zbigniew Rudy1, Piotr Salabura1, Artur Słomski1, Jerzy Smyrski1, Adam Strzelecki1, Anna Wieczorek1, Anna Wieczorek2, Wojciech Wiślicki •
Jagiellonian University1, Polish Academy of Sciences2
11 Nov 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, a single detection module built out from the BC-420 plastic scintillator strip (with dimensions of 5 � 19 � 300 mm 3 ) read out at two ends by Hamamatsu R5320 photomultipliers was used for low energy gamma quanta detection.
Abstract: A Time of Flight Positron Emission Tomography scanner based on plastic scintillators is being developed at the Jagiellonian University by the J-PET collaboration. The main challenge of the conducted research lies in the elaboration of a method allowing application of plastic scintillators for the detection of low energy gamma quanta. In this paper we report on tests of a single detection module built out from the BC-420 plastic scintillator strip (with dimensions of 5 � 19 � 300 mm 3 ) read out at two ends by Hamamatsu R5320 photomultipliers. The measurements were performed using collimated beam of annihilation quanta from the 68 Ge isotope and applying the Serial Data Analyzer (Lecroy SDA6000A) which enabled sampling of signals with 50 ps intervals. The time resolution of the prototype module was established to be better than 80 ps (σ) for a single level discrimination. The spatial resolution of the determination of the hit position along the strip was determined to be about 0.93 cm (σ) for the annihilation quanta. The fractional energy resolution for the energy E deposited by the annihilation quanta via the Compton scattering amounts to σðEÞ=E � 0:044= ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi EðMeVÞ p

236 citations

Journal Article•10.1016/J.NIMA.2013.11.081•
Calibration of the Super-Kamiokande detector

[...]

K. Abe1, Y. Hayato1, T. Iida1, K. Iyogi1, J. Kameda1, Yasuhiro Kishimoto1, Yusuke Koshio1, Yusuke Koshio2, Ll. Marti1, M. Miura1, S. Moriyama1, Masayuki Nakahata1, Yuuki Nakano1, S. Nakayama1, Y. Obayashi1, Hiroyuki Sekiya1, Masato Shiozawa1, Yoshihiro Suzuki1, Atsushi Takeda1, Y. Takenaga1, H. K. Tanaka1, T. Tomura1, Koh Ueno1, R. A. Wendell1, T. Yokozawa1, T. J. Irvine1, H. Kaji1, Takaaki Kajita1, K. Kaneyuki1, K. P. Lee1, Yasuhiro Nishimura1, Kimihiro Okumura1, T. McLachlan1, L. Labarga3, E. Kearns4, E. Kearns1, J. L. Raaf4, J. L. Stone4, J. L. Stone1, L. R. Sulak4, S. Berkman5, H.A. Tanaka5, S. Tobayama5, M. Goldhaber6, K. Bays7, G. Carminati7, W. R. Kropp7, S. Mine7, A. L. Renshaw7, M. B. Smy7, H. W. Sobel7, H. W. Sobel1, K. S. Ganezer8, John Hill8, W. E. Keig8, J. S. Jang9, J. Y. Kim9, I. T. Lim9, N. Hong9, T. Akiri10, Justin Albert10, A. Himmel10, Kate Scholberg10, Kate Scholberg1, C. W. Walter10, C. W. Walter1, T. Wongjirad10, T. Ishizuka11, Shigeki Tasaka12, John G. Learned, S. Matsuno, S. N. Smith, Takehisa Hasegawa, T. Ishida, T. Ishii, T. Kobayashi, T. Nakadaira, K. Nakamura1, K. Nishikawa, Yuichi Oyama, K. Sakashita, T. Sekiguchi, T. Tsukamoto, A. T. Suzuki13, Y. Takeuchi13, Y. Takeuchi1, K. Huang14, K. Ieki14, M. Ikeda14, T. Kikawa14, Hidetoshi Kubo14, A. Minamino14, A. Murakami14, Tsuyoshi Nakaya14, Tsuyoshi Nakaya1, Minoru Otani14, Kazuhiro Suzuki14, Susumu Takahashi14, Y. Fukuda15, K. Choi16, Yoshitaka Itow16, G. Mitsuka16, M. Miyake16, P. Mijakowski, R. Tacik17, Joshua Hignight18, J. Imber18, C. K. Jung18, I. Taylor18, C. Yanagisawa18, Y. Idehara2, Hirokazu Ishino2, A. Kibayashi2, Takaaki Mori2, Makoto Sakuda2, R. Yamaguchi2, T. Yano2, Y. Kuno19, S. B. Kim20, B. S. Yang20, H. Okazawa21, Y. Choi22, K. Nishijima23, M. Koshiba1, Y. Totsuka1, Masashi Yokoyama1, K. Martens1, M. R. Vagins1, M. R. Vagins7, J. F. Martin24, P. de Perio24, A. Konaka25, M. J. Wilking25, Song Chen26, Y. Heng26, H. Sui26, Zishuo Yang26, H. Zhang26, Y. Zhenwei26, K. Connolly27, M. Dziomba27, R. J. Wilkes27 •
University of Tokyo1, Okayama University2, Autonomous University of Madrid3, Boston University4, University of British Columbia5, Brookhaven National Laboratory6, University of California, Irvine7, California State University, Dominguez Hills8, Chonnam National University9, Duke University10, Fukuoka Institute of Technology11, Gifu University12, Kobe University13, Kyoto University14, Miyagi University of Education15, Nagoya University16, University of Regina17, Stony Brook University18, Osaka University19, Seoul National University20, Shizuoka University21, Sungkyunkwan University22, Tokai University23, University of Toronto24, TRIUMF25, Tsinghua University26, University of Washington27
11 Feb 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, a hardware-level detector calibration in Super-Kamiokande (SK) is presented, which can be used to obtain physical numbers such as photon counts and arrival times for each photomultiplier tube (PMT).
Abstract: Procedures and results on hardware-level detector calibration in Super-Kamiokande (SK) are presented in this paper. In particular, we report improvements made in our calibration methods for the experimental phase IV in which new readout electronics have been operating since 2008. The topics are separated into two parts. The first part describes the determination of constants needed to interpret the digitized output of our electronics so that we can obtain physical numbers such as photon counts and their arrival times for each photomultiplier tube (PMT). In this context, we developed an in situ procedure to determine high-voltage settings for PMTs in large detectors like SK, as well as a new method for measuring PMT quantum efficiency and gain in such a detector. The second part describes modeling of the detector in Monte Carlo simulations, including, in particular, the optical properties of the water target and their variability over time. Detailed studies on water quality are also presented. As a result of this work, we have achieved a precision sufficient for physics analyses over a wide energy range (from a few MeV to above 1 TeV). For example, charge determination was at the level of 1%, and the timing resolution was 2.1 ns at the one-photoelectron charge level and 0.5 ns at the 100-photoelectron charge level.

170 citations

Journal Article•10.1016/J.NIMA.2013.09.018•
Tunka-133: Results of 3 year operation

[...]

V. V. Prosin, S. F. Berezhnev, N. M. Budnev, A. Chiavassa1, O.A. Chvalaev, O. A. Gress, A. N. Dyachok, S. Epimakhov2, N. I. Karpov, N. N. Kalmykov, E. N. Konstantinov, A.V. Korobchenko, E. E. Korosteleva, V. A. Kozhin, L. A. Kuzmichev, B. K. Lubsandorzhiev, N. B. Lubsandorzhiev, R. R. Mirgazov, M. I. Panasyuk, L. V. Pankov, E.G. Popova, V. S. Ptuskin, Yu. A. Semeney, A. A. Silaev, A. V. Skurikhin, C. Spiering, L. G. Sveshnikova, I. V. Yashin, A. V. Zagorodnikov •
University of Turin1, University of Hamburg2
21 Aug 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: The EAS Cherenkov light array Tunka-133 has been taking data since 2009 as mentioned in this paper, and the array permits a detailed study of cosmic ray energy spectrum and mass composition in the PeV energy range.
Abstract: The EAS Cherenkov light array Tunka-133, with ~3 km2 geometric area, is taking data since 2009. The array permits a detailed study of cosmic ray energy spectrum and mass composition in the PeV energy range. After a short description of the methods of EAS parameter reconstruction, we present the all-particle energy spectrum and results of studying CR composition, based on 3 seasons of array operation. In the last part of the paper, we discuss possible interpretations of the obtained results.

156 citations

Journal Article•10.1016/J.NIMA.2013.11.025•
Time resolution deterioration with increasing crystal length in a TOF-PET system

[...]

Stefan Gundacker1, A. Knapitsch1, Etiennette Auffray1, Pierre Jarron1, T.I. Meyer1, Paul Lecoq1 •
CERN1
11 Feb 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, the authors used a Monte Carlo simulation tool in MATLAB incorporating the timing properties of the photodetector and electronics, the scintillation properties of crystal and the light transfer within the crystal simulated by SLITRANI, and showed that the predictions of the simulation are in good agreement with the experimental data.
Abstract: Highest time resolution in scintillator based detectors is becoming more and more important In medical detector physics L(Y)SO scintillators are commonly used for time of flight positron emission tomography (TOF-PET) Coincidence time resolutions (CTRs) smaller than 100 ps FWHM are desirable in order to improve the image signal to noise ratio and thus give benefit to the patient by shorter scanning times Also in high energy physics there is the demand to improve the timing capabilities of calorimeters down to 10 ps To achieve these goals it is important to study the whole chain, ie the high energy particle interaction in the crystal, the scintillation process itself, the scintillation light transfer in the crystal, the photodetector and the electronics Time resolution measurements for a PET like system are performed with the time-over-threshold method in a coincidence setup utilizing the ultra-fast amplifier-discriminator NINO With 2×2×3 mm3 LSO:Ce codoped 04%Ca crystals coupled to commercially available SiPMs (Hamamatsu S10931-050P MPPC) we achieve a CTR of 108±5 ps FWHM at an energy of 511 keV Under the same experimental conditions an increase in crystal length to 5 mm deteriorates the CTR to 123±7 ps FWHM, 10 mm to 143±7 ps FWHM and 20 mm to 176±7 ps FWHM This degradation in CTR is caused by the light transfer efficiency (LTE) and light transfer time spread (LTTS) in the crystal To quantitatively understand the measured values, we developed a Monte Carlo simulation tool in MATLAB incorporating the timing properties of the photodetector and electronics, the scintillation properties of the crystal and the light transfer within the crystal simulated by SLITRANI In this work, we show that the predictions of the simulation are in good agreement with the experimental data We conclude that for longer crystals the deterioration in CTR is mainly caused by the LTE, ie the ratio of photons reaching the photodetector to the total amount of photons generated by the scintillation whereas the LTTS influence is partly offset by the gamma absorption in the crystal

101 citations

Journal Article•10.1016/J.NIMA.2014.09.057•
OCELOT: A software framework for synchrotron light source and FEL studies

[...]

Ilya Agapov1, Gianluca Geloni1, Igor Zagorodnov2, Sergey Tomin3•
European XFEL1, University of Hamburg2, Kurchatov Institute3
21 Dec 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: OCELOT as mentioned in this paper is a multiphysics simulation toolkit developed at European XFEL in collaboration with NRC Kurchatov Institute and DESY since 2011, which has been used for synchrotron light sources and FELs.
Abstract: OCELOT is a novel multiphysics simulation toolkit, which has been in development at European XFEL in collaboration with NRC Kurchatov Institute and DESY since 2011. In this paper we describe its architecture, implementation, and applications in the area of synchrotron light sources and FELs.

88 citations

Journal Article•10.1016/J.NIMA.2014.04.078•
Nonlinear dynamics optimization with particle swarm and genetic algorithms for SPEAR3 emittance upgrade

[...]

Xiaobiao Huang1, James Safranek1•
SLAC National Accelerator Laboratory1
01 Sep 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: The result shows that the particle swarm algorithm converges significantly faster to similar or better solutions than the genetic algorithm and it does not require seeding of good solutions in the initial population, which may make it more suitable for many accelerator optimization applications.
Abstract: Nonlinear dynamics optimization is carried out for a low emittance upgrade lattice of SPEAR3 in order to improve its dynamic aperture and Touschek lifetime. Two multi-objective optimization algorithms, a genetic algorithm and a particle swarm algorithm, are used for this study. The performance of the two algorithms are compared. The result shows that the particle swarm algorithm converges significantly faster to similar or better solutions than the genetic algorithm and it does not require seeding of good solutions in the initial population. These advantages of the particle swarm algorithm may make it more suitable for many accelerator optimization applications.

87 citations

Journal Article•10.1016/J.NIMA.2014.04.080•
The STAR Vertex Position Detector

[...]

W. J. Llope1, J. Zhou1, T. Nussbaum1, Gerald W Hoffmann2, K. Asselta3, James Brandenburg1, J. Butterworth1, T. Camarda3, W. Christie3, H. J. Crawford4, X. Dong5, J. Engelage4, G. Eppley1, Frank Jm Geurts1, J. Hammond3, E. G. Judd4, D. L. McDonald1, C. Perkins4, L. Ruan3, J.A. Scheblein3, J. Schambach2, R. Soja3, K. Xin1, C. Yang6 •
Rice University1, University of Texas at Austin2, Brookhaven National Laboratory3, University of California, Berkeley4, Lawrence Berkeley National Laboratory5, University of Science and Technology of China6
21 Sep 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, the Vertex Position Detector (VPD) has been upgraded to a 2×19 channel detector, called the VPD detector, which is fully integrated into the STAR trigger system and provides the primary input to the minimum bias trigger in Au+Au collisions.
Abstract: The 2×3 channel pseudo Vertex Position Detector (pVPD) in the STAR experiment at RHIC has been upgraded to a 2×19 channel detector in the same acceptance, called the Vertex Position Detector (VPD). This detector is fully integrated into the STAR trigger system and provides the primary input to the minimum-bias trigger in Au+Au collisions. The information from the detector is used both in the STAR Level-0 trigger and offline to measure the location of the primary collision vertex along the beam pipe and the event “start time” needed by other fast-timing detectors in STAR. The offline timing resolution of single detector channels in full-energy Au+Au collisions is ~100 ps, resulting in a start time resolution of a few tens of picoseconds and a resolution on the primary vertex location of ~1 cm.

75 citations

Journal Article•10.1016/J.NIMA.2014.04.065•
Reactor antineutrino monitoring with a plastic scintillator array as a new safeguards method

[...]

Shugo Oguri1, Y. Kuroda2, Yoshiaki Kato2, R. Nakata2, Yoshizumi Inoue2, Chikara Ito3, M. Minowa2 •
KEK1, University of Tokyo2, Japan Atomic Energy Agency3
01 Sep 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: A segmented reactor-antineutrino detector made of plastic scintillators for application as a tool in nuclear safeguards inspection and performed mostly unmanned field operations at a commercial power plant reactor.
Abstract: We developed a segmented reactor-antineutrino detector made of plastic scintillators for application as a tool in nuclear safeguards inspection and performed mostly unmanned field operations at a commercial power plant reactor. At a position outside the reactor building, we measured the difference in reactor antineutrino flux above the ground when the reactor was active and inactive.
Journal Article•10.1016/J.NIMA.2014.03.033•
Chromium compensated gallium arsenide detectors for X-ray and γ-ray spectroscopic imaging

[...]

Matthew C. Veale1, Steven Bell2, Steven Bell1, D.D. Duarte2, D.D. Duarte1, M.J. French1, Andreas Schneider1, Paul Seller1, Matthew D. Wilson1, A. Lozinskaya3, V. A. Novikov3, O. P. Tolbanov3, A. V. Tyazhev3, A. N. Zarubin3 •
Science and Technology Facilities Council1, University of Surrey2, Tomsk State University3
11 Jul 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, the performance of three small pixel detectors with 80×80 pixels on a 250-μm pitch, fabricated with metal contacts and bonded to a spectroscopic imaging ASIC, was investigated.
Abstract: Semi-insulating GaAs material of 500 μm thickness grown using the Liquid Encapsulated Czochralski (LEC) method has been compensated with chromium to produce high resistivity single crystals suitable for spectroscopic imaging applications. Results are presented for the performance of three small pixel detectors each with 80×80 pixels on a 250 μm pitch, fabricated with metal contacts and bonded to a spectroscopic imaging ASIC. Current–voltage measurements demonstrated a material resistivity of 2.5×10 9 Ω cm at room temperature. At an optimised bias voltage, the average energy resolution at 60 keV (FWHM) was in the range 2.8–3.3 keV per pixel. An analysis of the voltage dependent X-ray spectroscopy suggests that the electron mobility lifetime ( μτ e ) for each detector is in the range 2.1–4.5×10 −5 cm 2 V −1 . The spectroscopic imaging capability of the detectors is also demonstrated in X-ray absorption spectroscopy measurements.
Journal Article•10.1016/J.NIMA.2014.03.055•
Neutron imaging options at the BOA beamline at Paul Scherrer Institut

[...]

M. Morgano1, Steven Peetermans1, Eberhard Lehmann1, Tobias Panzner1, Uwe Filges1 •
Paul Scherrer Institute1
01 Aug 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: The characterization of the BOA beamline at the Swiss spallation neutron source SINQ at Paul Scherrer Institut is presented in this article, where different techniques can be employed there as user-friendly plugins for non-standard neutron imaging experiments.
Abstract: The BOA beamline at the Swiss spallation neutron source SINQ at Paul Scherrer Institut is a flexible instrument used mainly for testing novel techniques and devices for neutron scattering and optics, but, due to the large and relatively homogeneous field of view, it can be successfully used for experiments in the field of neutron imaging. The beamline allows also for the exploitation of advanced imaging concepts such as polarized neutron imaging and diffractive neutron imaging. In this paper we present the characterization of the BOA beamline in the light of its neutron imaging capabilities. We show also the different techniques that can be employed there as user-friendly plugins for non-standard neutron imaging experiments.
Journal Article•10.1016/J.NIMA.2014.02.032•
Pulse shape discrimination with fast digitizers

[...]

D. Cester1, Marcello Lunardon1, G. Nebbia, Luca Stevanato1, Giuseppe Viesti1, S. Petrucci, Carlo Tintori •
University of Padua1
01 Jun 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, the pulse shape discrimination (PSD) between neutrons and gamma rays in liquid scintillators is studied by using the charge integration method with fast digitizers having different technical characteristics.
Abstract: The pulse shape discrimination (PSD) between neutrons and gamma rays in liquid scintillators is studied by using the charge integration method with fast digitizers having different technical characteristics. The use of the Figure of Merit (FoM) to verify the PSD capability is discussed. The dependence of the FoM on the digitizer sampling rate and resolution is experimentally determined. The effects due to the type of source and the irradiation geometry are also evidenced and discussed.
Journal Article•10.1016/J.NIMA.2013.09.027•
Photon attenuation coefficients of Heavy-Metal Oxide glasses by MCNP code, XCOM program and experimental data: A comparison study

[...]

A.M. El-Khayatt1, Atif Mossad Ali2, Vishwanath P. Singh3•
Islamic University1, Jazan University2, Karnatak University3
21 Jan 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, the mass attenuation coefficients, μ / ρ, total interaction cross-section, σ t, and mean free path (MFP) of some Heavy Metal Oxides (HMO) glasses, with potential applications as gamma ray shielding materials, have been investigated using the MCNP-4C code.
Abstract: The mass attenuation coefficients, μ / ρ , total interaction cross-section, σ t , and mean free path ( MFP ) of some Heavy Metal Oxides (HMO) glasses, with potential applications as gamma ray shielding materials, have been investigated using the MCNP-4C code. Appreciable variations are noted for all parameters by changing the photon energy and the chemical composition of HMO glasses. The numerical simulations parameters are compared with experimental data wherever possible. Comparisons are also made with predictions from the XCOM program in the energy region from 1 keV to 100 MeV. Good agreement noticed indicates that the chosen Monte Carlo method may be employed to make additional calculations on the photon attenuation characteristics of different glass systems, a capability particularly useful in cases where no analogous experimental data exist.
Journal Article•10.1016/J.NIMA.2013.10.005•
Apparatus for measurement of the electric dipole moment of the neutron using a cohabiting atomic-mercury magnetometer

[...]

C.A. Baker1, Y. Chibane2, M. Chouder2, P. Geltenbort, K. Green1, Philip Harris2, Blayne Heckel3, P. Iaydjiev1, S. N. Ivanov1, I. Kilvington1, Steve K. Lamoreaux3, D. J. R. May2, J. M. Pendlebury2, J. D. Richardson2, D. Shiers2, K. F. Smith2, M. G. D. van der Grinten1 •
Rutherford Appleton Laboratory1, University of Sussex2, University of Washington3
01 Feb 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, a description of the apparatus used to carry out an experimental search for an electric dipole moment of the neutron, at the Institut Laue-Langevin (ILL), Grenoble, is presented.
Abstract: A description is presented of apparatus used to carry out an experimental search for an electric dipole moment of the neutron, at the Institut Laue-Langevin (ILL), Grenoble. The experiment incorporated a cohabiting atomic-mercury magnetometer in order to reduce spurious signals from magnetic field fluctuations. The result has been published in an earlier letter [1]; here, the methods and equipment used are discussed in detail.
Journal Article•10.1016/J.NIMA.2014.01.002•
Calibration and performance of the AMS-02 time of flight detector in space

[...]

Veronica Bindi1, Guo-Ming Chen2, H. S. Chen2, E. Choumilov3, V. Choutko3, Andrea Contin, A. Lebedev3, Yunpeng Lu2, N. Masi, A.I. Oliva, F. Palmonari, Lucio Quadrani, Qiurong Yan2 •
University of Hawaii1, Chinese Academy of Sciences2, Massachusetts Institute of Technology3
11 Apr 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: The AMS-02 time-of-flight (TOF) detector was deployed on board of the International Space Station (ISS) where it is expected to be in operation for the ISS lifetime of at least a decade.
Abstract: AMS-02 is a high energy particle detector deployed in May 19, 2011 on board of the International Space Station (ISS) where it is expected to be in operation for the ISS lifetime of at least a decade. The main goal of AMS-02 is the detection of cosmic rays and gammas from the GeV to the TeV energy region to search for anti-matter, dark matter and understanding the origin of the cosmic rays. The AMS-02 time of flight (TOF) detector provides the trigger to experiment and allows precise measurements of the cosmic rays velocity and charge magnitude from hydrogen to iron and above. With the data set acquired during the first two and a half years of operation in space, a precise time-dependent calibration for time, velocity and charge measured by the TOF had been developed. The TOF calibration methods are described and the AMS-02 TOF performance in space is presented. (C) 2014 Elsevier B.V. All rights reserved.
Journal Article•10.1016/J.NIMA.2014.05.057•
A time projection chamber for high accuracy and precision fission cross-section measurements

[...]

M. Heffner1, David M. Asner2, Rich Baker3, J. D. Baker4, S. Barrett5, Carl R. Brune6, J. Bundgaard7, Eric Burgett8, D. Carter1, M. Cunningham1, Jenna Deaven8, D. L. Duke7, Uwe Greife7, S. M. Grimes6, U. Hager7, Nolan E. Hertel9, Tony S. Hill4, D. Isenhower10, Keith Jewell4, Jonathan B. King5, J. L. Klay3, Verena Kleinrath8, N. Kornilov6, R. Kudo3, Alexander B Laptev11, M. Leonard5, W. Loveland5, T. N. Massey6, C. McGrath8, R. Meharchand11, L. Montoya11, N. Pickle10, Hai Qu10, Vincent J. Riot1, J. Ruz1, Samuele Sangiorgio1, B. Seilhan1, S. Sharma10, L. Snyder1, Sean C. Stave2, G. Tatishvili2, R. T. Thornton10, Fredrik Tovesson11, Dwayne Towell10, R. S. Towell10, S. Watson10, B. Wendt8, Lynn Wood2, L. Yao5 •
Lawrence Livermore National Laboratory1, Pacific Northwest National Laboratory2, California Polytechnic State University3, Idaho National Laboratory4, Oregon State University5, Ohio University6, Colorado School of Mines7, Idaho State University8, Georgia Institute of Technology9, Abilene Christian University10, Los Alamos National Laboratory11
21 Sep 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: The fission Time Projection Chamber (fissionTPC) as mentioned in this paper is a two-chamber MICROMEGAS TPC designed to make precision cross-section measurements of neutron-induced fission.
Abstract: The fission Time Projection Chamber (fissionTPC) is a compact (15 cm diameter) two-chamber MICROMEGAS TPC designed to make precision cross-section measurements of neutron-induced fission. The actinide targets are placed on the central cathode and irradiated with a neutron beam that passes axially through the TPC inducing fission in the target. The 4π acceptance for fission fragments and complete charged particle track reconstruction are powerful features of the fissionTPC which will be used to measure fission cross-sections and examine the associated systematic errors. This paper provides a detailed description of the design requirements, the design solutions, and the initial performance of the fissionTPC.
Journal Article•10.1016/J.NIMA.2014.06.004•
Germanium-gated γ-γ fast timing of excited states in fission fragments using the EXILL&FATIMA spectrometer

[...]

J.-M. Régis1, G.S. Simpson2, Aurelien Blanc, Michael Jentschel, Ulli Köster, P. Mutti, V. Paziy3, N. Saed-Samii1, T. Soldner, C. A. Ur4, W. Urban5, Alison Bruce6, F. Drouet, L. M. Fraile3, S. Ilieva7, J. Jolie1, W. Korten8, T. Kröll7, S. Lalkovski9, Henryk Mach3, N. Marginean, Gheorghe Pascovici1, Zs. Podolyák10, P. H. Regan10, Oliver J. Roberts6, J. F. Smith2, C. Townsley10, A. Vancraeyenest, N. Warr1 •
University of Cologne1, University of the West of Scotland2, Complutense University of Madrid3, Istituto Nazionale di Fisica Nucleare4, University of Warsaw5, University of Brighton6, Technische Universität Darmstadt7, Commissariat à l'énergie atomique et aux énergies alternatives8, Sofia University9, University of Surrey10
01 Nov 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, a high-granularity mixed spectrometer consisting of high-resolution Ge and very fast LaBr3(Ce) detectors has been installed around a fission target at the cold-neutron guide PF1B of the high-flux reactor of the Institut Laue-Langevin.
Abstract: A high-granularity mixed spectrometer consisting of high-resolution Ge and very fast LaBr3(Ce)scintillator detectors has been installed around a fission target at the cold-neutron guide PF1B of the high-flux reactor of the Institut Laue–Langevin. Lifetimes of excited states in the range of 10 ps to 10 ns can be measured in around 100 exotic neutron-rich fission fragments using Ge-gated LaBr3(Ce)– LaBr3(Ce) or Ge–Ge–LaBr3(Ce)–LaBr3(Ce) coincidences. We report on various characteristics of the EXILL&FATIMA spectrometer for the energy range of 40 keV up to 6.8 MeV and present results of pslifetime test measurements in a fission fragment. The results are discussed with respect to possible systematic errors induced by background contributions. & 2014 Published by Elsevier B.V.
Journal Article•10.1016/J.NIMA.2013.10.074•
Improvement in Fast Particle Track Reconstruction with Robust Statistics

[...]

M. G. Aartsen1, Rasha Abbasi2, Y. Abdou3, Markus Ackermann  +279 more•Institutions (38)
01 Feb 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, the authors used data filters and robust statistical techniques to augment the detector's early reconstruction with data filters, which can be implemented at the level of online reconstruction and therefore improve all subsequent reconstructions.
Abstract: The IceCube project has transformed 1 km(3) of deep natural Antarctic ice into a Cherenkov detector Muon neutrinos are detected and their direction is inferred by mapping the light produced by the secondary muon track inside the volume instrumented with photomultipliers. Reconstructing the muon track from the observed light is challenging due to noise, light scattering in the ice medium, and the possibility of simultaneously having multiple muons inside the detector, resulting from the large flux of cosmic ray muons. This paper describes work on two problems: (1) the truck reconstruction problem, in which, given a set of observations, the goal is to recover the track of a muon; and (2) the coincident event problem, which is to determine how many muons are active in the detector during a time window. Rather than solving these problems by developing more complex physical models that are applied at later stages of the analysis, our approach is to augment the detector's early reconstruction with data filters and robust statistical techniques. These can be implemented at the level of on-line reconstruction and, therefore, improve all subsequent reconstructions. Using the metric of median angular resolution, a standard metric for track reconstruction, we improve the accuracy in the initial reconstruction direction by 13%. We also present improvements in measuring the number of muons in coincident events: we can accurately determine the number of muons 98% of the time. (C) 2013 Elsevier RV. All rights reserved.
Journal Article•10.1016/J.NIMA.2014.02.031•
Fabrication and characterization of solid-state thermal neutron detectors based on hexagonal boron nitride epilayers

[...]

T. C. Doan1, S. Majety1, S. J. Grenadier1, Jing Li1, Jingyu Lin1, Hongxing Jiang1 •
Texas Tech University1
01 Jun 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, Hexagonal boron nitride (hBN) epilayers have been synthesized by metal organic chemical vapor deposition on sapphire substrates and important material parameters including the mobility-lifetime (μτ) product and the thermal neutron absorption length (λ) have been measured.
Abstract: Solid-state thermal neutron detectors with improved detection efficiencies are highly sought after for many applications. Hexagonal boron nitride (hBN) epilayers have been synthesized by metal organic chemical vapor deposition on sapphire substrates. Important material parameters including the mobility-lifetime (μτ) product and the thermal neutron absorption length (λ) have been measured. For hBN epilayers with a room temperature resistivity of 5.3 � 10 10 Ω cm, the measured μτ product of electrons is 4.46 � 10 � 8 cm 2 /V and of holes is 7.07 � 10 � 9 cm 2 /V. The measured λ values are 277 μm and 77 μm for natural and 10 B enriched hBN epilayers, respectively. Metal–semiconductor–metal detectors incorporating 0.3 mm thick hBN epilayers were fabricated. The reaction product pulse-height spectra were measured under thermal neutron irradiation produced by a 252 Cf source moderated by high density polyethylene block. The measured pulse-height spectra revealed distinguishable peaks corresponding to the product energies of 10 B and neutron reaction with the 0.84 MeV 7 Li peak being the most prominent. The detectors exhibited negligible responses to gamma rays produced by 137 Cs decay. Our results indicate that hBN epilayers are highly promising for realizing highly sensitive solid-state thermal neutron detectors with expected advantages resulting from semiconductor technologies, including compact size, light weight, ability to integrate with other functional devices, and low cost.
Journal Article•10.1016/J.NIMA.2013.10.004•
Co-doping of CeBr3 scintillator detectors for energy resolution enhancement

[...]

Francesco Quarati1, Mikhail S. Alekhin1, Karl Krämer2, Pieter Dorenbos1•
Delft University of Technology1, University of Bern2
21 Jan 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, aliovalent co-doping techniques are used to enhance the energy resolution of the CeBr 3 gamma-ray spectrometers to at least 3.5%.
Abstract: CeBr 3 gamma-ray spectrometers are preferable to LaBr 3 :Ce ones for low-count-rate experiments because of their low intrinsic activity and consequently increased detection sensitivity. A drawback of CeBr 3 is a nonoptimum energy resolution, i.e. 4% at 662 keV. Here we demonstrate that aliovalent co-doping techniques are effective to enhance the CeBr 3 energy resolution to at least 3%. Such an enhancement is achieved because of a more proportional energy response of the scintillation.
Journal Article•10.1016/J.NIMA.2014.02.037•
A LaBr3: Ce fast-timing array for DESPEC at FAIR

[...]

Oliver J. Roberts1, Alison Bruce1, P. H. Regan2, Zsolt Podolyak2, Christopher M. Townsley2, J. F. Smith3, Kieran F. Mulholland3, Andrew M. Smith4 •
University of Brighton1, University of Surrey2, University of the West of Scotland3, University of Manchester4
01 Jun 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, the design of a fast-timing γ-ray detection array aimed at measuring sub-nanosecond half-lives using LaBr 3 :Ce scintillation crystals is presented.
Abstract: The design of a fast-timing γ-ray detection array aimed at measuring sub-nanosecond half-lives using LaBr 3 :Ce scintillation crystals is presented. This array will complement novel and existing charged particle and neutron detector arrays at the low-energy branch of a fragment separator (Super-FRS) to be built within the NuSTAR collaboration as part of the future Facility for Anti-proton and Ion Research (FAIR). The array will be used in conjunction with the Advanced Implantation Detector Array (AIDA), to measure implant-decay correlations. Monte-Carlo simulations have been performed to determine the design of the proposed fast-timing array around a localised implantation point. In particular, simulations were used to determine the full-energy peak efficiencies for single cylindrical, conical and ‘hybrid’ detector geometries, as well as complete array configurations of ‘hybrid’ and ∅1.5 in.×2 in. cylindrical crystals. Timing precision calculations were then used to determine the timing response for each configuration based on its simulated efficiency. An informed decision based on the simulated efficiencies and timing precision calculations allowed the optimum configuration for the array to be determined.
Journal Article•10.1016/J.NIMA.2013.07.061•
Development of a kinematically focused neutron source with the p(7Li,n)7Be inverse reaction

[...]

M. Lebois, J. N. Wilson, P. Halipre, B. Leniau, I. Matea, Andreas Oberstedt1, Stephan Oberstedt, D. Verney •
Chalmers University of Technology1
21 Jan 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, the authors investigated the use of the p(Li-7,n)Be-7 inverse reaction to produce kinematically focused, quasi-mono-energetic neutron beams with a view to develop such an unusual neutron source for fundamental and applied nuclear physics studies.
Abstract: Directional beams of neutrons can be produced, if a nuclear reaction, which emits neutrons, is initiated in inverse kinematics with a heavy ion projectile bombarding a light target. In this paper we investigate the use of the p(Li-7,n)Be-7 inverse reaction to produce kinematically focused, quasi-mono-energetic neutron beams with a view to develop such an unusual neutron source for fundamental and applied nuclear physics studies. An experiment was carried out to validate the concept and to test the viability of two types of hydrogen-rich solid targets: polypropylene and TiH2. Neutron time-of-flight/energy spectra at 3 m distance from the source have been measured at Li-7 bombarding energies of 13.5, 15, 15.5, 16, and 17 MeV, and neutron backgrounds from parasitic reactions have been characterized. The neutron angular distribution in the laboratory has been measured at 15 MeV. A Monte-Carlo code based on two-body relativistic kinematics has been developed and validated by comparison with the experimental data. Code-based extrapolations have then been used to deduce neutron energy spectra and maximum neutron fluxes available for future irradiation of samples placed in the neutron beam at small distances. For neutrons produced with thin (4 mu m) and thick (28 mu m) polypropylene targets the maximum available fluxes are calculated to be 10(7)n/s/sr and 7 x 10(7) n/s/sr respectively. The development of a dedicated facility to produce kinematically focused neutrons is discussed.
Journal Article•10.1016/J.NIMA.2014.05.006•
Sensors for ultra-fast silicon detectors

[...]

Hartmut Sadrozinski1, M. Baselga1, S. Ely1, Vitaliy Fadeyev1, Z. Galloway1, J. Ngo1, C. Parker1, D. Schumacher1, Abraham Seiden1, A. Zatserklyaniy1, Nicolo Cartiglia, Giulio Pellegrini2, Pablo Fernandez-Martinez2, V. Greco2, Salvador Hidalgo2, David Quirion2 •
Santa Cruz Institute for Particle Physics1, Spanish National Research Council2
21 Nov 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, the authors investigate the non-uniform doping profile of low-gain avalanche detectors (LGAD), which are n-on-p pad sensors with charge multiplication due to the presence of a thin, low resistivity diffusion layer below the junction, obtained with a highly doped implant.
Abstract: We report on electrical and charge collection tests of silicon sensors with internal gain as part of our development of ultra-fast silicon detectors. Using C–V and α TCT measurements, we investigate the non-uniform doping profile of so-called low-gain avalanche detectors (LGAD). These are n-on-p pad sensors with charge multiplication due to the presence of a thin, low-resistivity diffusion layer below the junction, obtained with a highly doped implant. We compare the bias dependence of the pulse shapes of traditional sensors and of LGAD sensors with different dopant density of the diffusion layer, and extract the internal gain.
Journal Article•10.1016/J.NIMA.2014.07.046•
Performance comparison of scintillators for alpha particle detectors

[...]

Yuki Morishita1, Yuki Morishita2, Seiichi Yamamoto2, Kenji Izaki1, Junichi Kaneko3, Kohei Toui3, Youichi Tsubota3, Mikio Higuchi3 •
Japan Atomic Energy Agency1, Nagoya University2, Hokkaido University3
11 Nov 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, a new ceramic sample, namely the cerium doped Gd 2 Si 2 O 7 (GPS) scintillator, has been tested as alpha particle detector and its performances have been compared to that one of three different scintilling materials: ZnS(Ag), GAGG and a standard plastic scintillation detector, coupled with two different photodetectors, namely a photomultiplier tube (PMT) and a Silicon Photo-multiplier (Si-PM)
Abstract: Scintillation detectors for alpha particles are often used in nuclear fuel facilities. Alpha particle detectors have also become important in the research field of radionuclide therapy using alpha emitters. ZnS(Ag) is the most often used scintillator for alpha particle detectors because its light output is high. However, the energy resolution of ZnS(Ag)-based scintillation detectors is poor because they are not transparent. A new ceramic sample, namely the cerium doped Gd 2 Si 2 O 7 (GPS) scintillator, has been tested as alpha particle detector and its performances have been compared to that one of three different scintillating materials: ZnS(Ag), GAGG and a standard plastic scintillator. The different scintillating materials have been coupled to two different photodetectors, namely a photomultiplier tube (PMT) and a Silicon Photo-multiplier (Si-PM): the performances of each detection system have been compared. Promising results as far as the energy resolution performances (10% with PMT and 14% with Si-PM) have been obtained in the case of GPS and GAGG samples. Considering the quantum efficiencies of the photodetectors under test and their relation to the emission wavelength of the different scintillators, the best results were achieved coupling the GPS with the PMT and the GAGG with the Si-PM
Journal Article•10.1016/J.NIMA.2013.12.031•
Generation of sub-fs electron beams at few-MeV energies

[...]

K. Floettmann
11 Mar 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, the question of what limits the bunch length in this parameter regime is addressed by means of numerical simulations and the limiting factors are identified as rf-curvature and nonlinear compression.
Abstract: Time resolved electron diffraction is an alternative approach to FEL based X-ray experiments for the study of structural dynamics of matter on the relevant timescales. The required electron beam parameters are demanding in terms of emittance and bunch length and require the operation at charges typically well below 1 pC. Moreover the energy is low – a few MeV only. The longitudinal compression of the bunches can be realized with a simple longitudinal focusing scheme in a drift. In this paper the question of what limits the bunch length in this parameter regime is addressed by means of numerical simulations. Beside emittance increasing space charge effects also rf-curvature and nonlinear compression are identified as limiting factors.
Journal Article•10.1016/J.NIMA.2014.06.074•
Fast neutron response of 6Li-depleted CLYC detectors up to 20 MeV

[...]

N. D׳Olympia1, P. Chowdhury1, E.G. Jackson1, C. J. Lister1•
University of Massachusetts Lowell1
01 Nov 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this paper, the response of 6Li-depleted Cs2LiYCl6 (CLYC) to high-energy neutrons has been investigated using a pair of 1.×1.in. crystals.
Abstract: The response of 6Li-depleted Cs2LiYCl6 (CLYC) to high-energy neutrons has been investigated using a pair of 1 in.×1 in. crystals. These are the first two detectors of their kind, which will comprise a 16-element array for studies in fast neutron spectroscopy. Their thermal neutron response has been compared with standard CLYC crystals with a 6Li enrichment of 95%, demonstrating excellent suppression of the overwhelming thermal neutron background. The response to mono-energetic neutrons over a range of 0.5 to 20 MeV was tested. From this, the response function, energy resolution, and pulse-shape discrimination up to 20 MeV were characterized. Detailed Monte Carlo investigations with MCNPX have been used to show that the dominant reaction mechanisms contributing to the observed response are 35Cl(n,p) and 35Cl(n,α). Preliminary investigations have also demonstrated the possibility for separating events from these two reactions.
Journal Article•10.1016/J.NIMA.2013.12.011•
Muon puzzle in cosmic ray experiments and its possible solution

[...]

A. A. Petrukhin1•
National Research Nuclear University MEPhI1
01 Apr 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, various aspects of the muon puzzle are considered, including the production of blobs of quark-gluon matter with large orbital momentum in nucleus-nucleus interactions at energies more than several PeV.
Abstract: The term “muon puzzle” was formulated at International Symposium on Future Directions in UHECR Physics in CERN 13–16 February 2012. In this paper, various aspects of muon puzzle are considered. Obtained experimental data can be divided into two types: muon bundle excess compared to simulations which is increasing with the increase of primary particle energy, and the excess of very-high-energy muons ( > 100 TeV ) in the muon energy spectrum. One of the possible (and realistic) solutions of the muon puzzle is the hypothesis about production of blobs of quark-gluon matter with large orbital momentum in nucleus–nucleus interactions at energies more than several PeV. Possibilities of the check of this hypothesis are discussed.
Journal Article•10.1016/J.NIMA.2014.03.027•
Boron-loaded plastic scintillator with neutron-γ pulse shape discrimination capability

[...]

Iwona Pawelczak1, A. Glenn1, H.P. Martinez1, M.L. Carman1, Natalia Zaitseva1, S.A. Payne1 •
Lawrence Livermore National Laboratory1
01 Jul 2014-Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment
TL;DR: In this article, a plastic scintillator with pulse shape discrimination (PSD) capability has been developed and a PSD figure-of-merit value of 1.4±0.03 has been achieved for events in a thermal neutron energy domain, 50-100 keVee, for PSD plastic loaded with 5.5% of m-carborane.
Abstract: Development of the plastic scintillator with neutron sensitivity from thermal to multi-MeV and pulse shape discrimination (PSD) has been demonstrated. Incorporation of 10B-containing compounds into the plastic scintillator with PSD capability leads to detector improvement in regard to neutron detection efficiency while preserving the discrimination between neutrons and γ-rays. Effects of boron loading on scintillation and pulse shape discrimination properties are discussed. A PSD figure-of-merit value of 1.4±0.03 has been achieved for events in a thermal neutron energy domain, 50–100 keVee, for PSD plastic loaded with 5 wt.% of m-carborane.
...

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