A.P. Colijn
University of Amsterdam
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Featured researches published by A.P. Colijn.
Physical Review Letters | 2013
E. Aprile; M. Alfonsi; K. Arisaka; F. Arneodo; C. Balan; L. Baudis; B. Bauermeister; A. Behrens; P. Beltrame; K. Bokeloh; Abbe Brown; E. Brown; G. Bruno; R. Budnik; João Cardoso; W. T. Chen; B. Choi; 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. Ghag; Karl-Ludwig Giboni; L. W. Goetzke
We present new experimental constraints on the elastic, spin-dependent WIMP-nucleon cross section using recent data from the XENON100 experiment, operated in the Laboratori Nazionali del Gran Sasso in Italy. An analysis of 224.6 live days×34 kg of exposure acquired during 2011 and 2012 revealed no excess signal due to axial-vector WIMP interactions with 129Xe and 131Xe nuclei. This leads to the most stringent upper limits on WIMP-neutron cross sections for WIMP masses above 6 GeV/c², with a minimum cross section of 3.5×10(-40) cm² at a WIMP mass of 45 GeV/c², at 90% confidence level.
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.
Journal of Physics G | 2013
E. Aprile; M. Alfonsi; K. Arisaka; F. Arneodo; C. Balan; L. Baudis; B. Bauermeister; A. Behrens; P. Beltrame; K. Bokeloh; Abbe Brown; E. Brown; G. Bruno; R. Budnik; João Cardoso; W. T. Chen; B. Choi; 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. Ghag; Karl-Ludwig Giboni; L. W. Goetzke
The XENON100 experiment, installed underground at the Laboratori Nazionali del Gran Sasso, aims to directly detect dark matter in the form of weakly interacting massive particles (WIMPs) via their elastic scattering off xenon nuclei. This paper presents a study on the nuclear recoil background of the experiment, taking into account neutron backgrounds from (α, n) reactions and spontaneous fission due to natural radioactivity in the detector and shield materials, as well as muon-induced neutrons. Based on Monte Carlo simulations and using measured radioactive contaminations of all detector components, we predict the nuclear recoil backgrounds for the WIMP search results published by the XENON100 experiment in 2011 and 2012, 0.11 events and 0.17 events, respectively, and conclude that they do not limit the sensitivity of the experiment.TheXENON100 experiment, installed underground at the LaboratoriNazionali del Gran Sasso, aims to directly detect dark matter in the form of weakly interacting massive particles (WIMPs) via their elastic scattering off xenon nuclei. This paper presents a study on the nuclear recoil background of the experiment, taking into account neutron backgrounds from (alpha, n) reactions and spontaneous fission due to natural radioactivity in the detector and shield materials, as well as muon-induced neutrons. Based on MonteCarlo simulations and using measured radioactive contaminations of all detector components, we predict the nuclear recoil backgrounds for the WIMP search results published by theXENON100 experiment in 2011 and 2012, 0.11(-0.04)(+0.08) events and 0.17(-0.07)(+0.12) events, respectively, and conclude that they do not limit the sensitivity of the experiment.
Nuclear Physics B - Proceedings Supplements | 1999
A.P. Colijn
Abstract The tau lepton lifetime is measurd with the L3 detector at LEP. For the analysis presented here tau pairs produced during 1994 and 1995 around the Z pole are used. The measurement is done by a decay length method for the 3-prong tau decays and by an impact parameter analysis for the 1-prong decays. From the data 6 620 3-prong decays are selected, from which a lifetime of ττ = 291.4 ± 3.9 (stat) ± 2.0 (syst) fs is determined. The impact parameter analysis on 58 656 1-prong decays results in a lifetime of ττ = 290.5 ± 2.7 (stat) ± 2.9 (syst) fs. Combination with our previous results gives ττ = 291.7 ± 2.0 (stat) ±1.8 (syst) fs. These numbers are preliminary.
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
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2004
P. Colas; A.P. Colijn; A. Fornaini; Y. Giomataris; H. van der Graaf; E.H.M. Heijne; X. Llopart; Jurriaan Schmitz; J. Timmermans; J.L. Visschers
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
Journal of Physical Chemistry C | 2010
A.P. Colijn; B. Verlaat
Archive | 2011
B. Verlaat; A.P. Colijn; H. Postema