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A reconstruction algorithm for unfolding the neutron energy spectrum has been developed based on the potential reduction interior point. This algorithm can be easily applied to the neutron energy spectrum reconstruction in the recoil proton…

Instrumentation and Detectors · Physics 2017-05-24 Guanying Wang , Ran Han , Xiaoping Ouyang , Jincheng He , Junyao Yan

A neutron monitor (NM) is, since the 1950s, a standard ground-based detector whose count rate reflects cosmic-ray variability. The worldwide network of NMs forms a rough spectrometer for cosmic rays. Recently, a brand-new data acquisition…

Instrumentation and Methods for Astrophysics · Physics 2021-04-13 Markus Similä , Ilya Usoskin , Stepan Poluianov , Alexander Mishev , Gennady A. Kovaltsov , Du Toit Strauss

The accuracy of neutronics simulations of actual or future reactor cores is nowadays driven by the precision of the nuclear data used as input. Among the most important neutron-induced fission cross sections to understand well are the…

There is considerable experimental effort dedicated to the directional detection of particle dark matter. Gaseous mu-TPC detectors present the privileged features of being able to reconstruct the track and the energy of the recoil nucleus…

Instrumentation and Detectors · Physics 2015-05-30 O. Guillaudin , J. Billard , G. Bosson , O. Bourrion , T. Lamy , F. Mayet , D. Santos , P. Sortais

Active Target Time Projection Chambers (AT-TPCs) are state-of-the-art tools in the field of low-energy nuclear physics, particularly suitable for experiments using low-intensity radioactive ion beams or gamma rays. The Fudan Multi-purpose…

By correlating nuclear recoil directions with the Earth's direction of motion through the Galaxy, a directional dark matter detector can unambiguously detect Weakly Interacting Massive Particles (WIMPs), even in the presence of backgrounds.…

We have developed a prototype time-resolved neutron imaging detector employing the micro-pixel chamber (muPIC), a micro-pattern gaseous detector, coupled with a field programmable gate array-based data acquisition system for applications in…

Directional detection can provide unambiguous observation of Dark Matter interactions even in presence of insidious backgrounds. The DM-TPC collaboration is developing a detector with the goal of measuring the direction and sense of nuclear…

A novel large volume spherical proportional counter, recently developed, is used for neutron measurements. Gas mixtures of $N_{2}$ with $C_{2}H_{6}$ and pure $N_{2}$ are studied for thermal and fast neutron detection, providing a new way…

We provide a quantitative description of a method to measure neutron-induced fission cross sections in ratio to elastic hydrogen scattering in a white-source neutron beam with the fission Time Projection Chamber. This detector has measured…

A new method for directional fast neutron detection is proposed based on a neutron time projection chamber (TPC) and position-sensitive plastic scintillation detectors. The detection system can efficiently locate the approximate location of…

Instrumentation and Detectors · Physics 2019-07-11 Yidong Fu , Yang Tian , Yulan Li , Jian Yang , Jin Li

A new Radio-frequency quadrupole (RFQ), which operates at 800 MHz high frequency and will enable to accelerate of the proton beam efficiently was designed at KAHVELab (Kandilli Detector, Accelerator and Instrumentation Laboratory) at…

The GammaTPC is an MeV-scale single-phase liquid argon time-projection-chamber gamma-ray telescope concept with a novel dual-scale pixel-based charge-readout system. It promises to enable a significant improvement in sensitivity to…

Instrumentation and Methods for Astrophysics · Physics 2023-01-25 M. Buuck , A. Mishra , E. Charles , N. Di Lalla , O. Hitchcock , M. E. Monzani , N. Omodei , T. Shutt

A fast neutron spectrometer consisting of segmented plastic scintillator and He-3 proportional counters was constructed for the measurement of neutrons in the energy range 1 MeV to 200 MeV. We discuss its design, principles of operation,…

Instrumentation and Detectors · Physics 2014-11-24 T. J. Langford , C. D. Bass , E. J. Beise , H. Breuer , D. K. Erwin , C. R. Heimbach , J. S. Nico

The available experimental information on the Range-Energy relation for protons stopped in hydrogen gas is summarized in the SRIM software package. The estimated precision of this data is several percents. Here we describe a possibility to…

Instrumentation and Detectors · Physics 2019-12-13 A. Vorobyev , N. Sagidova

We present work on the detection of neutral particles via nuclear recoils in gas-filled Time Projection Chambers (TPCs). We employ Gas Electron Multipliers (GEMs) to amplify the signal and silicon pixel electronics to detect the avalanche…

A large area plastic scintillator detector array(~ 1 m x1m) has been set up for fast neutron spectroscopy at the BARC-TIFR Pelletron laboratory, Mumbai. The energy, time and position response has been measured for electrons using…

Nuclear Experiment · Physics 2009-01-16 P. C. Rout , D. R. Chakrabarty , V. M. Datar , Suresh Kumar , E. T. Mirgule , A. Mitra , V. Nanal , R. Kujur

The neutron lifetime, $\tau$ = 880.2 $\pm$ 1.0 sec , is an important parameter for particle physics and cosmology. There is, however, an 8.4 sec (4.0$\,\sigma$) deviation between the measured value of the neutron lifetime using two methods…

Instrumentation and Detectors · Physics 2018-12-26 Naoyuki Sumi , Hidetoshi Otono , Tamaki Yoshioka , Kenji Mishima , Yasuhiro Makida

The direct search for dark matter in the form of weakly interacting massive particles (WIMP) is performed by detecting nuclear recoils (NR) produced in a target material from the WIMP elastic scattering. A promising experimental strategy…

Instrumentation and Detectors · Physics 2024-01-12 20k Collaboration , P. Agnes , I. Ahmad , S. Albergo , I. F. M. Albuquerque , T. Alexander , A. K. Alton , P. Amaudruz , M. Atzori Corona , M. Ave , I. Ch. Avetisov , O. Azzolini , H. O. Back , Z. Balmforth , A. Barrado-Olmedo , P. Barrillon , A. Basco , G. Batignani , V. Bocci , W. M. Bonivento , B. Bottino , M. G. Boulay , J. Busto , M. Cadeddu , A. Caminata , N. Canci , G. Cappello , A. Capra , S. Caprioli , M. Caravati , N. Cargioli , M. Carlini , P. Castello , V. Cataudella , P. Cavalcante , S. Cavuoti , S. Cebrian , J. M. Cela Ruiz , S. Chashin , A. Chepurnov , E. Chyhyrynets , L. Cifarelli , D. Cintas , M. Citterio , B. Cleveland , V. Cocco , E. Conde Vilda , L. Consiglio , S. Copello , G. Covone , M. Czubak , M. D'Aniello , S. D'Auria , M. D. Da Rocha Rolo , S. Davini , A. de Candia , S. De Cecco , D. De Gruttola , G. De Filippis , D. Dell'Aquila , S. De Pasquale , G. De Rosa , G. Dellacasa , A. V. Derbin , A. Devoto , F. Di Capua , L. Di Noto , C. Dionisi , P. Di Stefano , G. Dolganov , F. Dordei , A. Elersich , E. Ellingwood , T. Erjavec , M. Fernandez Diaz , G. Fiorillo , P. Franchini , D. Franco , N. Funicello , F. Gabriele , D. Gahan , C. Galbiati , G. Gallina , G. Gallus , M. Garbini , P. Garcia Abia , A. Gendotti , C. Ghiano , C. Giganti , G. K. Giovanetti , V. Goicoechea Casanueva , A. Gola , G. Grauso , G. Grilli di Cortona , A. Grobov , M. Gromov , M. Guan , M. Guerzoni , M. Gulino , C. Guo , B. R. Hackett , A. L. Hallin , A. Hamer , M. Haranczyk , T. Hessel , S. Hill , S. Horikawa , F. Hubaut , J. Hucker , T. Hugues , An. Ianni , V. Ippolito , C. Jillings , S. Jois , P. Kachru , N. Kemmerich , A. A. Kemp , C. L. Kendziora , M. Kimura , I. Kochanek , K. Kondo , G. Korga , S. Koulosousas , A. Kubankin , M. Kuss , M. Kuzniak , M. La Commara , M. Lai , E. Le Guirriec , E. Leason , A. Leoni , X. Li , L. Lidey , M. Lissia , L. Luzzi , O. Lychagina , O. Macfadyen , I. N. Machulin , S. Manecki , I. Manthos , L. Mapelli , A. Margotti , S. M. Marik , C. Mariani , J. Maricic , A. Marini , M. Martínez , C. J. Martoff , G. Matteucci , K. Mavrokoridis , A. B. McDonald , A. Messina , R. Milincic , A. Mitra , A. Moharana , J. Monroe , E. Moretti , M. Morrocchi , T. Mróz , V. N. Muratova , C. Muscas , P. Musico , R. Nania , M. Nessi , G. Nieradka , K. Nikolopoulos , J. Nowak , K. Olchansky , A. Oleinik , V. Oleynikov , P. Organtini , A. Ortiz de Solórzano , L. Pagani , M. Pallavicini , L. Pandola , E. Pantic , E. Paoloni , G. Paternoster , P. A. Pegoraro , K. Pelczar , V. Pesudo , S. Piacentini , N. Pino , A. Pocar , D. M. Poehlmann , S. Pordes , P. Pralavorio , D. Price , F. Ragusa , Y. Ramachers , M. Razeti , A. L. Renshaw , M. Rescigno , F. Retiere , L. P. Rignanese , C. Ripoli , A. Rivetti , A. Roberts , C. Roberts , J. Rode , G. Rogers , L. Romero , M. Rossi , A. Rubbia , M. A. Sabia , P. Salomone , E. Sandford , S. Sanfilippo , D. Santone , R. Santorelli , C. Savarese , E. Scapparone , G. Schillaci , F. G. Schuckman , G. Scioli , M. Simeone , P. Skensved , M. D. Skorokhvatov , O. Smirnov , T. Smirnova , B. Smith , A. Sosa , F. Spadoni , M. Spangenberg , R. Stefanizzi , A. Steri , V. Stornelli , S. Stracka , M. Stringer , S. Sulis , A. Sung , Y. Suvorov , A. M. Szelc , R. Tartaglia , A. Taylor , J. Taylor , S. Tedesco , G. Testera , K. Thieme , T. N. Thorpe , A. Tonazzo , A. Tricomi , E. V. Unzhakov , T. Vallivilayil John , M. Van Uffelen , T. Viant , S. Viel , R. B. Vogelaar , J. Vossebeld , M. Wada , M. B. Walczak , H. Wang , Y. Wang , S. Westerdale , L. Williams , I. Wingerter-Seez , R. Wojaczynski , Ma. M. Wojcik , T. Wright , Y. Xie , C. Yang , A. Zabihi , P. Zakhary , A. Zani , A. Zichichi , G. Zuzel , M. P. Zykova