A. Tiseni
University of Amsterdam
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Featured researches published by A. Tiseni.
Physical Review D | 2014
E. Aprile; F. Agostini; M. Alfonsi; K. Arisaka; F. Arneodo; M. Auger; C. Balan; P. Barrow; L. Baudis; B. Bauermeister; A. Behrens; P. Beltrame; K. Bokeloh; A. Brown; E. Brown; Stefan Brünner; G. Bruno; R. Budnik; João Cardoso; A.P. Colijn; H. Contreras; J. P. Cussonneau; M.P. Decowski; E. Duchovni; S. Fattori; A. D. Ferella; W. Fulgione; F. Gao; M. Garbini; C. Geis
We present the first results of searches for axions and axionlike particles with the XENON100 experiment. The axion-electron coupling constant, g Ae , has been probed by exploiting the axioelectric effect in liquid xenon. A profile likelihood analysis of 224.6 live days × 34-kg exposure has shown no evidence for a signal. By rejecting g Ae larger than 7.7×10 −12 (90% C.L.) in the solar axion search, we set the best limit to date on this coupling. In the frame of the DFSZ and KSVZ models, we exclude QCD axions heavier than 0.3 and 80 eV/c 2 , respectively. For axionlike particles, under the assumption that they constitute the whole abundance of dark matter in our galaxy, we constrain g Ae to be lower than 1×10 −12 (90% C.L.) for masses between 5 and 10 keV/c 2 .
Science | 2015
E. Aprile; M. Alfonsi; A. Brown; A.P. Colijn; M.P. Decowski; A. Tiseni; C. Tunnell
Limiting unknows in the dark side Our knowledge of the inventory of stuff that makes up our universe amounts to a humbling 5%. The rest consists of either dark energy (~70%) or dark matter (~25%). Using atom interferometry, Hamilton et al. describe the results of experiments that controlled for dark energy screening mechanisms in individual atoms, not bulk matter. Aprile et al. report on an analysis of data taken with the XENON100 detectors aiming to identify dark matter particles directly by monitoring their rare interaction with ordinary matter. In this setup, a large underground tank of liquid xenon forms a target for weakly interacting m assive particles. These combined results set limits on several types of proposed dark matter and dark energy candidates (see the Perspective by Schmiedmayer and Abele). Science, this issue p. 849, p. 851; see also p. 786 Results from the XENON100 underground detector set limits on some proposed candidates for dark matter. [Also see Perspective by Schmiedmayer and Abele] Laboratory experiments searching for galactic dark matter particles scattering off nuclei have so far not been able to establish a discovery. We use data from the XENON100 experiment to search for dark matter interacting with electrons. With no evidence for a signal above the low background of our experiment, we exclude a variety of representative dark matter models that would induce electronic recoils. For axial-vector couplings to electrons, we exclude cross sections above 6 × 10–35 cm2 for particle masses of mχ = 2 GeV/c2. Independent of the dark matter halo, we exclude leptophilic models as an explanation for the long-standing DAMA/LIBRA signal, such as couplings to electrons through axial-vector interactions at a 4.4σ confidence level, mirror dark matter at 3.6σ, and luminous dark matter at 4.6σ.
European Physical Journal C | 2015
E. Aprile; F. Agostini; M. Alfonsi; L. Arazi; K. Arisaka; F. Arneodo; M. Auger; C. Balan; P. Barrow; L. Baudis; B. Bauermeister; A. Behrens; P. Beltrame; Abbe Brown; E. Brown; S. Bruenner; G. Bruno; R. Budnik; Lukas Bütikofer; João Cardoso; Daniel Coderre; A. P. Colijn; H. Contreras; J. P. Cussonneau; M.P. Decowski; A. Di Giovanni; E. Duchovni; S. Fattori; A. D. Ferella; A. Fieguth
The low-background, VUV-sensitive 3-inch diameter photomultiplier tube R11410 has been developed by Hamamatsu for dark matter direct detection experiments using liquid xenon as the target material. We present the results from the joint effort between the XENON collaboration and the Hamamatsu company to produce a highly radio-pure photosensor (version R11410-21) for the XENON1T dark matter experiment. After introducing the photosensor and its components, we show the methods and results of the radioactive contamination measurements of the individual materials employed in the photomultiplier production. We then discuss the adopted strategies to reduce the radioactivity of the various PMT versions. Finally, we detail the results from screening 286 tubes with ultra-low background germanium detectors, as well as their implications for the expected electronic and nuclear recoil background of the XENON1T experiment.
Journal of Instrumentation | 2014
E. Aprile; F. Agostini; M. Alfonsi; K. Arisaka; F. Arneodo; M. Auger; C. Balan; P. Barrow; L. Baudis; B. Bauermeister; A. Behrens; P. Beltrame; K. Bokeloh; A. Breskin; Abbe Brown; E. Brown; S. Bruenner; G. Bruno; R. Budnik; João Cardoso; A. P. Colijn; H. Contreras; J. P. Cussonneau; M.P. Decowski; E. Duchovni; S. Fattori; A. D. Ferella; W. Fulgione; M. Garbini; C. Geis
XENON is a dark matter direct detection project, consisting of a time projection chamber (TPC) filled with liquid xenon as detection medium. The construction of the next generation detector, XENON1T, is presently taking place at the Laboratori Nazionali del Gran Sasso (LNGS) in Italy. It aims at a sensitivity to spin-independent cross sections of 2 10-47 c 2 for WIMP masses around 50 GeV2, which requires a background reduction by two orders of magnitude compared to XENON100, the current generation detector. An active system that is able to tag muons and muon-induced backgrounds is critical for this goal. A water Cherenkov detector of ~ 10 m height and diameter has been therefore developed, equipped with 8 inch photomultipliers and cladded by a reflective foil. We present the design and optimization study for this detector, which has been carried out with a series of Monte Carlo simulations. The muon veto will reach very high detection efficiencies for muons (>99.5%) and showers of secondary particles from muon interactions in the rock (>70%). Similar efficiencies will be obtained for XENONnT, the upgrade of XENON1T, which will later improve the WIMP sensitivity by another order of magnitude. With the Cherenkov water shield studied here, the background from muon-induced neutrons in XENON1T is negligible.
Journal of Physics: Conference Series | 2013
M. Alfonsi; N. van Bakel; A. P. Colijn; M.P. Decowski; H. van der Graaf; R. Schön; A. Tiseni
GridPix is a gas-filled detector with an aluminium mesh stretched 50 μm above the Timepix CMOS pixel chip. This defines a high electric field where gas amplification occurs. A feasibility study is ongoing at Nikhef for the application of the GridPix technology as a charge sensitive device in a dual phase noble gas Time Projection Chamber (TPC), within the framework of the DARWIN design study for next generation dark matter experiments. The smallness of the device and well defined materials allow for high radio-purity and low outgassing. The high granularity of a pixel readout and the high detection efficiency of single electrons of GridPix bring benefits especially in terms of energy resolution for small energy deposits. This feature is interesting also for the measurement of the scintillation yield and the ionisation yield of noble liquids. The accurate measurements of such quantities have a direct impact on the data interpretation of dark matter experiments. The application in dual phase argon or xenon TPCs implies several technological challenges, such as the survival of the device at cryogenic temperature as well as the operation in a pure noble gas atmosphere without discharges. We describe here the recent developments of the project.
Physical Review Letters | 2017
E. Aprile; J. Aalbers; F. Agostini; M. Alfonsi; F. D. Amaro; M. Anthony; F. Arneodo; P. Barrow; L. Baudis; B. Bauermeister; M.L. Benabderrahmane; T. Berger; P. A. Breur; A. Brown; S. Bruenner; G. Bruno; R. Budnik; Lukas Bütikofer; J. Calvén; João Cardoso; M. Cervantes; D. Cichon; D. Coderre; A.P. Colijn; J. Conrad; J.P. Cussonneau; M.P. Decowski; P. de Perio; P. Di Gangi; A. Di Giovanni
Physical Review Letters | 2015
E. Aprile; J. Aalbers; M. Alfons; P. A. Breur; A. Brown; A.P. Colijn; M.P. Decowski; A. Tiseni; C. Tunnell
Physical Review D | 2017
E. Aprile; F. Agostini; M. Alfonsi; K. Arisaka; F. Arneodo; M. Auger; C. Balan; P. Barrow; L. Baudis; B. Bauermeister; A. Behrens; P. Beltrame; K. Bokeloh; April S. Brown; E. Brown; S. Bruenner; G. Bruno; R. Budnik; João Cardoso; A. P. Colijn; H. Contreras; J. P. Cussonneau; M.P. Decowski; E. Duchovni; S. Fattori; A. D. Ferella; W. Fulgione; F. Gao; M. Garbini; C. Geis