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Featured researches published by R. Acciarri.


Journal of Instrumentation | 2010

Oxygen contamination in liquid Argon: combined effects on ionization electron charge and scintillation light

R. Acciarri; M Antonello; B. Baibussinov; M. Baldo-Ceolin; P. Benetti; F. Calaprice; E. Calligarich; M. Cambiaghi; N Canci; F. Carbonara; F. Cavanna; S. Centro; A. G. Cocco; F Di Pompeo; G. Fiorillo; C. Galbiati; V. Gallo; L. Grandi; G. Meng; I. Modena; C. Montanari; O. Palamara; L. Pandola; G B Piano Mortari; F. Pietropaolo; G.L. Raselli; M. Roncadelli; M. Rossella; C. Rubbia; E. Segreto

A dedicated test of the effects of Oxygen contamination in liquid Argon has been performed at the INFN-Gran Sasso Laboratory (LNGS, Italy) within the WArP R&D program. Two detectors have been used: the WArP2.3 lt prototype and a small (0.7 lt) dedicated detector, coupled with a system for the injection of controlled amounts of gaseous Oxygen. O2 contamination in LAr leads to depletion of both the free electron charge (via attachment process) and the scintillation light (via quenching and absorption mechanisms) available for ionization signal detection. Purpose of the test with the 0.7 lt detector was to detect the reduction of the long-lived component lifetime of the Argon scintillation light emission and of the overall light yield at increasing O2 concentration. Data from the WArP prototype were used for determining the behavior of both the ionization electron lifetime and the scintillation long-lived component lifetime at decreasing O2 concentration by the purification process activated in closed loop during the acquisition run. The electron lifetime measurements allowed to infer the O2 content of the Argon and correlate it with the long-lived scintillation lifetime data. The effects of Oxygen contamination on the scintillation light have been thus extensively measured over a wide range of O2 concentration, spanning from ~ 10−3 ppm up to ~ 10 ppm.


Journal of Instrumentation | 2012

Demonstration and comparison of photomultiplier tubes at liquid Argon temperature

R. Acciarri; M Antonello; F. Boffelli; M. Cambiaghi; N Canci; F. Cavanna; A. G. Cocco; N Deniskina; F Di Pompeo; G. Fiorillo; C. Galbiati; L. Grandi; P. Kryczynski; G. Meng; C. Montanari; O. Palamara; L. Pandola; F Perfetto; G B Piano Mortari; F. Pietropaolo; G.L. Raselli; C. Rubbia; E. Segreto; A.M. Szelc; A. Triossi; S. Ventura; C. Vignoli; A. Zani

Liquified noble gases are widely used as a target in direct Dark Matter searches. Signals from scintillation in the liquid, following energy deposition from the recoil nuclei scattered by Dark Matter particles (e.g. WIMPs), should be recorded down to very low energies by photosensors suitably designed to operate at cryogenic temperatures. Liquid Argon based detectors for Dark Matter searches currently implement photo multiplier tubes for signal read-out. In the last few years PMTs with photocathodes operating down to liquid Argon temperatures (87 K) have been specially developed with increasing Quantum Efficiency characteristics. The most recent of these, Hamamatsu Photonics Mod. R11065 with peak QE up to about 35%, has been extensively tested within the R&D program of the WArP Collaboration. During these testes the Hamamatsu PMTs showed superb performance and allowed obtaining a light yield around 7 phel/keVee in a Liquid Argon detector with a photocathodic coverage in the 12% range, sufficient for detection of events down to few keVee of energy deposition. This shows that this new type of PMT is suited for experimental applications, in particular for new direct Dark Matter searches with LAr-based experiments.


Journal of Physics: Conference Series | 2010

The WArP experiment

R. Acciarri; M. Antonello; B. Baibussinov; P. Benetti; F. Calaprice; E. Calligarich; M. Cambiaghi; N Canci; C Cao; F. Carbonara; F. Cavanna; S. Centro; M B Ceolin; A Chavarria; A. G. Cocco; F Di Pompeo; G. Fiorillo; C. Galbiati; L Grandi; B Loer; G. Mangano; A Menegolli; G. Meng; C. Montanari; O. Palamara; L. Pandola; F. Pietropaolo; G.L. Raselli; M. Roncadelli; M. Rossella

Cryogenic noble liquid detectors are presently considered one of the best options for WIMP Dark Matter searches, especially when extensions to multi ton scale sensitive masses are foreseen. The WArP experiment is the first one that exploits the unique characteristics of liquid Argon to make a highly sensitive search for WIMP Dark Matter candidates. In 2008, a double phase detector has been assembled in the Gran Sasso National Laboratory with 140 kg sensitive mass and a discovery potential in the range of 5 × 10−45 cm2 in the spin-independent WIMP-nucleon cross-section. In addition to standard neutrons and gamma-rays passive shields, WArP implements an 8 ton liquid Argon active shield with 4π coverage. The detector was commissioned and put into operation during the first half of 2009 for a first technical run. This first run lasted about three months and then it was stopped for some detector repairs and modifications in the summer of 2009. A second run was started at the beginning of 2010. Detector design, construction and assembly are described, together with the results of the technical run and the very first results of the 2010 run.


Journal of Physics: Conference Series | 2008

Discovery of underground argon with a low level of radioactive 39Ar and possible applications to WIMP dark matter detectors

C. Galbiati; D. Acosta-Kane; R. Acciarri; O Amaize; M. Antonello; B. Baibussinov; Mb Ceolin; Cj Ballentine; R. Bansal; L. Basgall; A. O. Bazarko; P. Benetti; J. Benziger; A. Burgers; F. Calaprice; E. Calligarich; M. Cambiaghi; N. Canci; F. Carbonara; M. Cassidy; F. Cavanna; S. Centro; A. Chavarria; D. Cheng; Ag Cocco; Philippe Collon; F. Dalnoki-Veress; E. de Haas; F Di Pompeo; G. Fiorillo

We report on the first measurement of 39Ar in argon from underground natural gas reservoirs. The gas stored in the US National Helium Reserve was found to contain a low level of 39Ar. The ratio of 39Ar to stable argon was found to be ≤4×10-17 (84% C.L.), less than 5% the value in atmospheric argon (39Ar/Ar=8×10-16). The total quantity of argon currently stored in the National Helium Reserve is estimated at 1000 tons. 39Ar represents one of the most important backgrounds in argon detectors for WIMP dark matter searches. The findings reported demonstrate the possibility of constructing large multi-ton argon detectors with low radioactivity suitable for WIMP dark matter searches.


Journal of Instrumentation | 2012

Tests of PMT signal read-out of liquid argon scintillation with a new fast waveform digitizer

R. Acciarri; N Canci; F. Cavanna; A. Cortopassi; M. D'Incecco; G. Mini; F. Pietropaolo; A. Romboli; E. Segreto; A.M. Szelc

The CAEN V1751 is a new generation of Waveform Digitizer recently introduced by CAEN SpA. It features 8 Channels per board, 10 bit, 1 GS/s using Flash ADCs Waveform Digitizers (or 4 channels at 2 GS/s in Dual Edge Sampling mode) with threshold and Auto-Trigger capabilities. This provides a good basis for data acquisition in Dark Matter searches using PMTs to detect scintillation light in liquid argon, as it matches the requirements for measuring the fast scintillation component. The board was tested by operating it in real experimental conditions and by comparing it with a state of the art digital oscilloscope. We find that the sampling at 1 or 2 GS/s is appropriate for the reconstruction of the fast component of the scintillation light in argon (characteristic time of about 6-7 ns) and the extended dynamic range, after a small customization, allows for the detection of signals in the range of energy needed. The bandwidth is found to be adequate and the intrinsic noise is very low.


Astroparticle Physics | 2008

First results from a dark matter search with liquid argon at 87 K in the Gran Sasso underground laboratory

P. Benetti; R. Acciarri; F. Adamo; B. Baibussinov; M. Baldo-Ceolin; M. Belluco; F. Calaprice; E. Calligarich; M. Cambiaghi; F. Carbonara; F. Cavanna; S. Centro; A. G. Cocco; F Di Pompeo; N. Ferrari; G. Fiorillo; C. Galbiati; V. Gallo; L. Grandi; Andrea Ianni; G. Mangano; G. Meng; C. Montanari; O. Palamara; L. Pandola; F. Pietropaolo; G.L. Raselli; M. Rossella; C. Rubbia; A.M. Szelc


Nuclear Physics B - Proceedings Supplements | 2009

Effects of Nitrogen and Oxygen contamination in liquid Argon

R. Acciarri; M. Antonello; B. Baibussinov; M. Baldo-Ceolin; P. Benetti; F. Calaprice; E. Calligarich; M. Cambiaghi; N. Canci; F. Carbonara; F. Cavanna; S. Centro; A. G. Cocco; F Di Pompeo; G. Fiorillo; C. Galbiati; V. Gallo; L. Grandi; G. Meng; I. Modena; C. Montanari; O. Palamara; L. Pandola; F. Pietropaolo; G.L. Raselli; M. Roncadelli; M. Rossella; C. Rubbia; E. Segreto; A.M. Szelc


NUCL PHYS B-PROC SUPPL | 2008

Effects of Nitrogen contamination in liquid Argon

R. Acciarri; M. Antonello; B. Baibussinov; Massimilla Baldo-Ceolin; P. Benetti; Frank Calaprice; E. Calligarich; Mario Cambiaghi; N. Canci; F. Carbonara; F. Cavanna; S. Centro; A. G. Cocco; F. Di Pompeo; G. Fiorillo; C. Galbiati; Vittorio Gallo; L. Grandi; G. Meng; I. Modena; Carlos Alberto Montanari; O. Palamara; L. Pandola; F. Pietropaolo; G.L. Raselli; Marco Roncadelli; M. Rossella; Carlo Rubbia; E. Segreto; A.M. Szelc


Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2009

Effects of Nitrogen and Oxygen contaminations in liquid Argon

R. Acciarri; M Antonello; B. Baibussinov; M. Baldo-Ceolin; P. Benetti; F. Calaprice; E. Calligarich; M. Cambiaghi; N Canci; F. Carbonara; F. Cavanna; S. Centro; A. G. Cocco; F Di Pompeo; G. Fiorillo; C. Galbiati; V. Gallo; L. Grandi; G. Meng; I. Modena; C. Montanari; O. Palamara; L. Pandola; F. Pietropaolo; G.L. Raselli; M. Roncadelli; M. Rossella; Carlo Rubbia; E. Segreto; A.M. Szelc


Physics Procedia | 2012

Neutron to Gamma Pulse Shape Discrimination in Liquid Argon Detectors with High Quantum Effciency Photomultiplier Tubes

R. Acciarri; N Canci; F. Cavanna; P. Kryczynski; L. Pandola; E. Segreto; A.M. Szelc

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F. Cavanna

University of L'Aquila

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G. Fiorillo

University of Naples Federico II

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F Di Pompeo

University of L'Aquila

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L. Pandola

Istituto Nazionale di Fisica Nucleare

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A. G. Cocco

Istituto Nazionale di Fisica Nucleare

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