English
Related papers

Related papers: Track Reconstruction and Performance of DRIFT Dire…

200 papers

Precise radial velocity measurements (delta v/c ~ 10^{-7}) of FeII lines in damped Ly-alpha systems from very high quality VLT/UVES spectra of quasars HE0515-4414 and Q1101-264 are used to probe cosmological time dependence of the fine…

The possibility of nuclear reactions within a low voltage DC deuterium discharge with palladium electrodes is addressed. The solid-state nuclear track detector known as CR-39 was chosen to investigate the emission of energetic charged…

Nuclear Experiment · Physics 2024-02-09 Erik P. Ziehm , George H. Miley

We present two examples of velocity distributions for light dark matter particles that reconcile the annual modulation signal observed by DAMA with all other negative results from dark matter searches. They are: (1) a conventional…

High Energy Physics - Phenomenology · Physics 2009-11-11 Paolo Gondolo , Graciela Gelmini

Tracking by Deblatting stands for solving an inverse problem of deblurring and image matting for tracking motion-blurred objects. We propose non-causal Tracking by Deblatting which estimates continuous, complete and accurate object…

Computer Vision and Pattern Recognition · Computer Science 2019-11-27 Denys Rozumnyi , Jan Kotera , Filip Šroubek , Jiří Matas

DEAP-1 is a 7 kg liquid argon dark matter detector used to prototype the tonne scale DEAP-3600 detector at SNOLAB.We present an analysis of the alpha particle backgrounds in DEAP-1 and isolate the radiations from various 222Rn daughters at…

High Energy Physics - Experiment · Physics 2009-06-02 Kevin S. Olsen

The measurement of the direction of WIMP-induced nuclear recoils is a compelling but technologically challenging strategy to provide an unambiguous signature of the detection of Galactic dark matter. Most directional detectors aim to…

The CRESST-II experiment uses cryogenic detectors to search for nuclear recoil events induced by the elastic scattering of dark matter particles in CaWO$_4$ crystals. Given the low energy threshold of our detectors in combination with light…

The Time Projection method is an ideal candidate to track low energy release particles. Large volumes can be readout by means of a moderate number of channels providing a complete 3D reconstruction of the charged tracks within the sensitive…

Instrumentation and Detectors · Physics 2019-01-15 G. Mazzitelli , E. Baracchini , G. Cavoto , E. Di Marco , M. Marafini , C. Mancini , D. Pinci , F. Renga , S. Tomassini

The ALICE detector was designed to track and identify particles in a wide transverse momentum range, from more than 100 GeV/c down to ~100 MeV/c. The innermost barrel-like detector, the Inner Tracking System (ITS), is dedicated to precise…

Instrumentation and Detectors · Physics 2019-08-13 Andrea Rossi

This text describes a method to simultaneously reconstruct flow states and determine particle properties from Lagrangian particle tracking (LPT) data. LPT is a popular measurement strategy for fluids in which particles in a flow are…

Fluid Dynamics · Physics 2023-11-16 Ke Zhou , Samuel J. Grauer

We present a measurement of the charged particle reconstruction inefficiency inside of jet cores, using data collected by the ATLAS experiment in 2015 of $pp$ collisions produced at the LHC, at a center-of-mass energy of 13 TeV. The…

High Energy Physics - Experiment · Physics 2017-01-04 Jason D. Mansour

The Dark Matter Time Projection Chamber (DMTPC) experiment uses CF_4 gas at low pressure (0.1 atm) to search for the directional signature of Galactic WIMP dark matter. We describe the DMTPC apparatus and summarize recent results from a…

We study the capabilities of the MAJORANA DEMONSTRATOR, a neutrinoless double-beta decay experiment currently under construction at the Sanford Underground Laboratory, as a light WIMP detector. For a cross section near the current…

High Energy Physics - Phenomenology · Physics 2013-07-17 Alexander Friedland , Ian M. Shoemaker

In Phase 2 of CRESST-II 18 detector modules were operated for about two years (July 2013 - August 2015). Together with this document we are publishing data from two detector modules which have been used for direct dark-matter searches. With…

Directional detection of non-baryonic Dark Matter requires 3D reconstruction of low energy nuclear recoils tracks. A gaseous micro-TPC matrix, filled with either 3He, CF4 or C4H10 has been developed within the MIMAC project. A dedicated…

Instrumentation and Methods for Astrophysics · Physics 2011-11-14 O. Bourrion , G. Bosson , C. Grignon , J. L. Bouly , J. P. Richer , O. Guillaudin , F. Mayet , J. Billard , D. Santos

We present here a search for WIMP dark matter using 790.8 live-days of data collected with 3269 kg of liquid argon (1266 kg fiducial) by the DEAP-3600 detector at SNOLAB, using the Profile Likelihood Ratio method. The likelihood model is…

High Energy Physics - Experiment · Physics 2026-03-17 DEAP Collaboration , P. Adhikari , R. Ajaj , M. Alpízar-Venegas , P. -A. Amaudruz , J. Anstey , D. J. Auty , M. Baldwin , M. Batygov , B. Beltran , A. Bigentini , C. E. Bina , W. Bonivento , M. G. Boulay , J. F. Bueno , P. M. Burghardt , A. Butcher , M. Cadeddu , B. Cai , M. Cárdenas-Montes , S. Cavuoti , Y. Chen , S. Choudhary , B. T. Cleveland , R. Crampton , S. Daugherty , P. DelGobbo , P. Di Stefano , G. Dolganov , L. Doria , F. A. Duncan , M. Dunford , E. Ellingwood , A. Erlandson , S. S. Farahani , N. Fatemighomi , G. Fiorillo , R. J. Ford , D. Gahan , D. Gallacher , A. Garai , P. García Abia , S. Garg , P. Giampa , A. Giménez-Alcázar , D. Goeldi , P. Gorel , K. Graham , A. Grobov , A. L. Hallin , M. Hamstra , S. Haskins , J. Hu , J. Hucker , D. Huff , T. Hugues , A. Ilyasov , B. Jigmeddorj , C. J. Jillings , A. Joy , G. Kaur , A. Kemp , M. Khoshraftar Yazdi , M. Kuźniak , F. La Zia , M. Lai , S. Langrock , B. Lehnert , J. LePage-Bourbonnais , M. Lissia , L. Luzzi , I. Machulin , P. Majewski , A. Maru , J. Mason , A. B. McDonald , T. McElroy , J. B. McLaughlin , C. Mielnichuk , L. Mirasola , A. Moharana , J. Monroe , A. Murray , M. Needs , C. Ng , G. Oliviéro , M. Olszewski , S. Pal , D. Papi , B. Park , M. Perry , V. Pesudo , T. R. Pollmann , F. Rad , C. Rethmeier , F. Retière , I. Rodríguez García , L. Roszkowski , R. Santorelli , F. G. Schuckman , N. Seeburn , S. Seth , V. Shalamova , P. Skensved , T. Smirnova , N. J. T. Smith , K. Sobotkiewich , T. Sonley , J. Sosiak , J. Soukup , R. Stainforth , M. Stringer , J. Tang , P. Taylor , R. Turcotte-Tardif , E. Vázquez-Jáuregui , G. Vera Díaz , S. Viel , B. Vyas , M. Walczak , J. Walding , M. Ward , S. Westerdale , R. Wormington , A. Zuñiga-Reyes

Dark matter detectors with directional sensitivity have the capability to distinguish dark matter induced nuclear recoils from isotropic backgrounds, thus providing a smoking gun signature for dark matter in the Galactic halo. Motivated by…

Instrumentation and Detectors · Physics 2019-07-05 Shang-Yung Wang

The Cryogenic Dark Matter Search (CDMS II) experiment aims to detect dark matter particles that elastically scatter from nuclei in semiconductor detectors. The resulting nuclear-recoil energy depositions are detected by ionization and…

Instrumentation and Detectors · Physics 2018-07-31 R. Agnese , A. J. Anderson , T. Aramaki , W. Baker , D. Balakishiyeva , S. Banik , D. Barker , R. Basu Thakur , D. A. Bauer , T. Binder , A. Borgland , M. A. Bowles , P. L. Brink , R. Bunker , B. Cabrera , D. O. Caldwell , R. Calkins , C. Cartaro , D. G. Cerdeno , H. Chagani , Y. -Y. Chang , Y. Chen , J. Cooley , B. Cornell , P. Cushman , M. Daal , T. Doughty , E. M. Dragowsky , L. Esteban , S. Fallows , E. Fascione , E. Figueroa-Feliciano , M. Fritts , G. Gerbier , R. Germond , M. Ghaith , G. L. Godfrey , S. R. Golwala , J. Hall , H. R. Harris , D. Holmgren , Z. Hong , L. Hsu , M. E. Huber , V. Iyer , D. Jardin , A. Jastram , C. Jena , M. H. Kelsey , A. Kennedy , A. Kubik , N. A. Kurinsky , A. Leder , E. Lopez Asamar , P. Lukens , D. MacDonell , R. Mahapatra , V. Mandic , N. Mast , K. A. McCarthy , E. H. Miller , N. Mirabolfathi , R. A. Moffatt , B. Mohanty , D. Moore , J. D. Morales Mendoza , J. Nelson , S. M. Oser , K. Page , W. A. Page , R. Partridge , M. Penalver Martinez , M. Pepin , A. Phipps , S. Poudel , M. Pyle , H. Qiu , W. Rau , P. Redl , A. Reisetter , A. Roberts , H. E. Rogers , A. E. Robinson , T. Saab , B. Sadoulet , J. Sander , K. Schneck , R. W. Schnee , S. Scorza , K. Senapati , B. Serfass , D. Speller , P. C. F. Di Stefano , M. Stein , J. Street , H. A. Tanaka , D. Toback , R. Underwood , A. N. Villano , B. von Krosigk , B. Welliver , J. S. Wilson , M. J. Wilson , D. H. Wright , S. Yellin , J. J. Yen , B. A. Young , X. Zhang , X. Zhao

An important issue for rare-event-search experiments, such as the search for dark matter or neutrinoless double beta decay, is to reduce radioactivity of the detector materials and the experimental environment. The selection of materials…

Instrumentation and Detectors · Physics 2020-01-29 H. Ito , T. Hashimoto , K. Miuchi , K. Kobayashi , Y. Takeuchi , K. D. Nakamura , T. Ikeda , H. Ishiura

The Nab (Neutron a b) experiment is designed to measure the beta-antineutrino angular correlation in free neutron $\beta$ decay with an ultimate precision goal of 0.1%, providing input for tests of Cabibbo-Kobayashi-Maskawa (CKM) matrix…