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Jul 2, 2013 - Abstract: The MINOS experiment has used the world's most powerful neutrino beam to make precision neutrino oscillation measurements. By observing the disappearance of muon neutrinos, MINOS has made the world's most precise measurement o
May 30, 2008 - absorbing wafer on the left hand side and the scintillating crystal in its housing on the right hand side. ... In 2007, the experimental setup was extended to be capable of housing up to 33 detector modules. ... The data reported here
provide a tracking accuracy of 0.02â¦. Each telescope is .... tunately, we did not find DC Î³-ray signals from any one of these sources. ... of Mrk 501. In order to obtain max- imum exposure time the source was observed in tracking mode. Almost 150
Feb 7, 2013 - tems, followed by a software stage which applies a full event reconstruction. The maximum output rate of the hardware and software stages is currently limited to about. 1 MHz and 5 kHz, respectively. .... signal shape is described by a
Jan 14, 2009 - Mine in Minnesota, to make precise measurements of Î½Âµ ... the Î¸13 mixing angle by searching for Î½e appearance in the Î½Âµ beam. Key words:.
Sep 23, 2016 - UHF telephones. Satellite, SAR receiving ... The stations communicate either via long-range wifi or via satellite communication. Both allow for ... Trigger rates as function of time of all regular HRA stations. After December 31st ...
Aug 16, 2016 - ... obtained using the data recorded with the Belle detector at the KEKB asymmetric-energy e+eâ collider in KEK, Japan. 1 Introduction. The Belle detector is a large-solid-angle magnetic spec- trometer that consists of a silicon vert
Aug 18, 2004 - more use of fixed target data, and with the MRST 2001 PDF . 3 Hadronic Final States. The ZEUS collaboration has recently developed a rigorous and consistent technique for including jets in QCD fits. Figure 3 shows the effect of comb
results extracted from 2011 data produce more questions than answers; this doubles expectations for the 2012 run of LHC, which will conclusively ... particular, and for high-energy physics in general. After the start-up of the LHC at the .... imperfe
Nov 14, 2012 - In the recent decade, the measurement of the radio counterparty of EAS becomes a promising technique. Many scientific collaborations like ...
Nov 6, 2005 - a transversely polarized target to address transverse information for quarks inside the nucleon. In addition, a pilot run with incoming pions taken late 2004 will give first information on the pion polarizabilities and hadron resonances
Aug 18, 2014 - for dedicated physics measurements over a wide range of subjects, starting ... (SM) by means of forward physics, multijet and boson production, ...
Jan 27, 2014 - The OPERA (Oscillation Project with Emulsion-tRacking Apparatus) ex- periment1 ... tion in appearance mode, through the direct detection of the short-lived Ï ... Tracks found in CS are looked for in the most downstream film of the bri
Aug 18, 2014 - The recorded data un- dergoes a certification process where depending on the operationality of the various sub-detector systems and the needs for dedicated physics analyses two dataset categories are established. 85% of the data are ce
E787a measures the charged track emanating ... Princeton, TRIUMF, Alberta and British Columbia. 50 cm. K Beam ... For further rejection of Âµ+ tracks, the out-.
Dec 11, 2016 - The experiment took data at center-of-mass energies corresponding to ... where Ebeam. arXiv:1612.03493v1 [hep-ex] 11 Dec 2016 .... The world average values  are R(Dâ)=0.322 Â± 0.018 Â± 0.012 and R(D)=0.391 Â± 0.041 Â± 0.028, whic
Jan 20, 2015 - The absolute energy scale uncertainty, which is correlated among all ADs, is constrained to be less than 1% in the majority of the energy range of reactor Â¯Î½e. Daya Bay took data in the aforementioned 6-AD configuration from December
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May 30, 2014 - The Spectral Power Density (SPD) distribution is shown in fig. 5 (right). The significance of SPD peaks has been evaluated by Monte Carlo simulations of the signal and the ... certainties for most isotopes, some cases (12B, 11C, 8Li fo
Jul 25, 2016 - arXiv:1607.07324v1 [hep-ph] 25 Jul 2016. Proceedings of the Seventh Meeting on CPT and Lorentz Symmetry (CPT'16), Indiana University, Bloomington, June 20-24, 2016. 1. Results and Prospects from the. Daya Bay Reactor Neutrino Experimen
Feb 29, 2012 - The RICE array is designed to detect events in which a neutrino-nucleon scattering event initiates a compact ... frequency (RF) studies of ice properties will impact new initiatives at South Pole. Development of .... 'thermal noise hit
Association, Inc., under contract with the United States Department of Energy.  J. A. Appel, Ann. Rev. Nucl. Part. Sci. 42 367-399 (1992), and references therein;. D. J. Summers et al., Proceedings of the XXVIIth Rencontre de Moriond, Electroweak
Sep 2, 2010 - I.M. Brancusg, P. Buchholzh, S. Buitinkd, E. Cantonie,i, A. Chiavassae, K. Daumillera, V. de Souzab,o, P. Dolla, R. Engela,. H. Falcked,j, M. Fingera, ..... thermore, the prominence of a signature for radio emission sen- sitivity on the
arXiv:hep-ex/0011064v1 20 Nov 2000
The CRESST Experiment: Recent Results and Prospects P. Di Stefanoa1 , M. Bruckmayera, C. Buccic, S. Cooperb, C. Cozzinia, F. von Feilitzschd, T. Franka, D. Hauffa, T. Jagemannd, J. Jochumd, R. Keelingb, H. Krausb, J. Marcheseb, D. Pergolesia, F. Pr¨obsta, Y. Ramachersb, J. Schnagld, W. Seidela, I. Sergeyeva, M. Starkd, L. Stodolskya, S. Uchaikina, H. Wulandarid a
Max-Planck-Institut f¨ ur Physik, F¨ ohringer Ring 6, D-80805 Munich, Germany b University of Oxford, Department of Physics, Oxford OX1 3RH, UK c Laboratori Nazionali del Gran Sasso, I-67010 Assergi, Italy d Technische Universit¨ at M¨ unchen, Physik Department, D-85747 Munich, Germany
Abstract. The CRESST experiment seeks hypothetical WIMP particles that could account for the bulk of dark matter in the Universe. The detectors are cryogenic calorimeters in which WIMPs would scatter elastically on nuclei, releasing phonons. The first phase of the experiment has successfully deployed several 262 g sapphire devices in the Gran Sasso underground laboratories. A main source of background has been identified as microscopic mechanical fracturing of the crystals, and has been eliminated, improving the background rate by up to three orders of magnitude at low energies, leaving a rate close to one count per day per kg and per keV above 10 keV recoil energy. This background now appears to be dominated by radioactivity, and future CRESST scintillating calorimeters which simultaneously measure light and phonons will allow rejection of a great part of it.
INTRODUCTION The question of dark matter was first raised by astronomer Fritz Zwicky in a 1933 study of redshifts of galaxies in clusters . In the Coma system, Zwicky found the mean mass density to be at least 400 times greater than the luminous mass density, which led him to postulate the presence of dark matter. Today, the problem remains, at many additional scales in the Universe, and there is a compelling cosmological case for the presence of non-baryonic weakly interacting massive particles (WIMPs) in our galactic halo . WIMPs are all the more appealing that 1)
they arise in supersymmetric theories in the guise of the lightest supersymmetric particle (LSP), which is typically the neutralino. The direct approach to detecting these halo WIMPs is to look for their interactions in a detector, as was first proposed in connection with cryogenic devices [3,4]. The low energies (of the order of keVs) and rates (of the order of counts per day per kg of detector) involved present a major experimental challenge. Historically, the first detectors used were semi-conducting devices, followed by scintillating crystals and more recently, after much development, the cryogenic techniques.
CRESST SAPPHIRE CALORIMETERS In its first phase, the Cryogenic Rare Event Search with Superconducting Thermometers (CRESST) employs calorimeters composed of a 262 g sapphire absorber in which an incident particle creates a nuclear or an electron recoil which in turn produces non-thermal phonons. These phonons make their way to a thin tungsten film deposited on the crystal and maintained in its superconducting transition in the vicinity of 15 mK . The arrival of the phonons heats the film slightly, inducing a relatively large change in its resistance . This change is measured with a SQUID, by passing a constant current through a parallel circuit, one branch of which is the film, and the other a resistor and the inductance coil of the SQUID. Typical tungsten transition curves are not always smooth, therefore reconstructing the energy scale is not necessarily straightforward. CRESST calorimeters are designed to facilitate this task : they have a resistive gold wire bonded to the film, through which it is possible to apply a heat pulse to the thermometer, mimicking the shape of pulses coming from the sapphire absorber. These are employed to inject pulses of known energy into the film, and thereby reconstruct the energy scale and monitor trigger efficiency at low energies. Supplied with constant current, such gold heaters can also serve to stabilize the operating point on the transition curve. Performances of this type of detector include a resolution FWHM of 250 eV at 1.5 keV , which can be improved to 130 eV using active thermal feedback .
RESULTS FROM GRAN SASSO The experimental setup underground is in Hall B of the Gran Sasso National Laboratories in Italy, where the rock shielding, equivalent to 3800 meters of water, reduces the cosmic muon flux to about 1 /m2 /h. The fast neutron flux has been measured as ≈ 10−6 /cm2 /s. The experiment is housed in a 3 storey building, erected around a Faraday cage to shield the apparatus from electromagnetic interferences. Within the cage is a class 100 clean room protecting the cryostat from radioactive dust. The cryostat itself has been designed and constructed to protect the detectors from vibrations as well as from radioactivity and electronic noises. It reaches a base temperature of 6 mK. Though its experimental volume is greater, so far it has housed up to four calorimeters. They are mounted within 10 mm of each
Run 14 vs Run 15
Ch4 Energy (keV)
Run 14, Background
Ch2 Energy (keV)
FIGURE 1. Left, pulses, as seen by both tungsten films on a common crystal, before removal of source of stress on crystal. All pulses are found to be coincident and to be of same energy within the resolution of the detector, and thus originate within the absorber. The agreement between the two channels is also a check of the consistency of the methods used. Right, typical energy spectra before and after modifying crystal mounting.
other and with no interposed material (other than small nibs at the corners of the crystals) so as to make them self-shielding and to allow the study of coincidences between them. More details of this setup are available in Ref. . First results from the detectors were puzzling. The experimental rate was orders of magnitude higher than expected, despite all the pulses having the shape anticipated from calibrations with a 57 Co source. Moreover, the spectrum showed no lines or structures, the time distribution of events did not follow a Poisson distribution, and there were no coincidences between crystals. Several attempts were made to understand this enigma. For instance, the detectors were isolated mechanically with a spring suspension, and the electrical circuits were modified. These changes improved the stability of the setup to external perturbations, but did not affect the overall background significantly. The next step was to install a special calorimeter consisting of a standard 262 g sapphire absorber with two tungsten films on it. All pulses were found to be coincident between these two sensors and of same energy (Fig. 1), demonstrating that the background originated within the sapphire crystal itself rather than in the tungsten films or in the electrical circuitry. The cause was finally traced back to slight fracturing of the sapphire crystal under pressure from the sapphire balls maintaining it in place. Over the course of the run, a network of micro-cracks gradually develops, releasing mechanical energy as it spreads. These micro-cracks have since been observed under microscope. To alleviate this problem, the crystals were next mounted using softer and blunter
Delrin stubs rather than sapphire balls. The improvement in the background is noticeable (Fig. 1), and surpasses three orders of magnitude at low energies. In a run lasting several months, trigger efficiency has been studied by means of the heater pulses, and is found to rise to 100 % by 2 keV. This value is taken as a conservative threshold henceforth. Above it, the time distribution of events is Poissonian. A structure is present in the spectrum at around 8 keV. This could be due to copper and/or nickel X-rays, and is under investigation. Above this contamination, the rate is of the order of 1 count/d/kg/keV. As a whole, the spectrum is an improvement over previous smaller sapphire devices of other groups [10,11]. Limits in terms of WIMPs are in the process of being inferred.
DEVELOPMENT OF SCINTILLATING CALORIMETERS Further progress requires being able to differentiate between the electron recoils caused by the photon and electron background, and the nuclear recoils expected to be induced by the neutron background and the WIMPs. Other groups have achieved this using a simultaneous measure of charge and heat in semiconducting calorimeters [12–14]. The CRESST group is developing an alternative technique, which involves measurement of scintillating light and phonons, using a principal calorimeter made of a scintillating crystal which yields the phonon signal and emits photons read by a very sensitive secondary sapphire calorimeter (scintillation signal). Efficiency is enhanced by placing both calorimeters in a light collector. The proof of principle experiment with a rectangular parallelepiped scintillator  has demonstrated a rejection of electron recoils greater than 99.7 % for a 95 % acceptance of nuclear recoils above 15 keV, and no reduction in performance in the case of surface events. A scaled-up device is in preparation, the challenge being that in the proof of principle experiment, a mere 0.8 % of the energy deposited as electron recoils in the main crystal was converted to scintillation and eventually read in the secondary calorimeter. For a given material and type of recoil, among the factors which may influence this fraction are the shape and size of the scintillator, the efficiency of the light collector, and the size and efficiency of the light detector. A 300 g CaWO4 crystal of the readily available cylindrical geometry is being prepared as the main scintillator. It was initially feared that in such a shape, internal reflections would lead to a reduction of escaping light as the radial position of the interaction increased. This was tested by exposing the bottom of the crystal (itself of 40 mm height and diameter) to a 60 Co source supplying 1.17 and 1.33 MeV photons with interaction lengths in the crystal of between 2.5 and 3 cm. The resulting light spectrum showed that the two peaks were well enough resolved (∆EF W HM /E ≈ 15 %) for one to be able to conclude that the expected bulk effect is in fact not significant. This is interpreted to mean that scattering on impurities in the crystal and non specular refraction out of the crystal at surface irregularities dominate absorption within the crystal. For the tungsten phonon sensor, transition
temperatures of 40 mK have repeatedly been reached on small CaWO4 substrates. The evaporation process is being studied to make the 15 mK transitions obtained in some instances reproducible. The higher transition temperature may already provide a better sensitivity than the glued film used for the demonstration experiment. An alternative solution, proximity effect Ir-Au films , is under investigation. The second thrust of development is the light collector. The present design uses special reflective foil  wrapped into a cylinder concentric to the scintillating crystal, with two diffusive Teflon end-caps, one of which holds the light detector. Using the same light detector as in the demonstration experiment, this has yielded a new ratio of light detected over energy deposited in the scintillator of 0.68 % for electron recoils. Therefore, though the scintillator mass has been increased fiftyfold to 300 g, this setup still gives 85 % of the light of the smaller experiment. The third component being optimized is the light detector, which will be crucial for the threshold of the scaled-up device. Its design presents an apparent dilemma in that sensitivity of the calorimeter requires its size to be small, whereas efficiency of light collection requires its surface to be large. A 40 × 40 × 0.5 mm3 sapphire calorimeter (sixteen times the effective surface area of the demonstration light detector) with a tungsten film has provided encouraging results : resolution FWHM of 150 eV at 6 keV and baseline noise FWHM of 25 eV (in all likelihood dominated by the readout, which is noisier than that at Gran Sasso). Moreover, response to a collimated source shining on three different points of the calorimeter was homogeneous. With a slightly smaller and more sensitive light detector, the scintillator and light collector described above, it is hoped to duplicate the proof of principle rejection factor above phonon energies of 15 keV. Assuming those performances and a background equal to that obtained with the sapphire, and inducing mainly electron recoils, 300 g of CaWO4 exposed for three months would have a sensitivity comparable to the best spin-independent limits , thanks to the background suppression and the large coherent cross section of tungsten.
CONCLUSION AND OUTLOOK The CRESST dark matter experiment has demonstrated the feasibility of running massive cryogenic detectors in stable conditions underground for several months. A main source of background, the micro-cracking of the crystals under stress, has been identified and eliminated. This leaves a background rate which is now competitive with that of other experiments, and is probably dominated by photons or electrons. Scintillating calorimeters being developed by the collaboration will reduce the impact of part of this background. In addition to a two orders of magnitude suppression of the background afforded by the discrimination between electron and nuclear recoils, the spin-independent sensitivity will be much improved through the higher coherent cross section of tungsten. Indeed, assuming a phonon threshold of 15 keV and a background rejection of 99.7 % (both reached on a smaller-scale experiment), and assuming the same exposure time and background as those of the
sapphire devices, a 300 g CaWO4 scintillating calorimeter would have a sensitivity on a par with current best limits . This 300 g device will be a stepping-stone to a 10 kg array of 33 such scintillating calorimeters, for which planning and development are already underway. With adequate neutron shielding, this next major phase of the experiment will cover more of supersymmetric parameter space .
ACKNOWLEDGMENTS This work has been supported by EU-TMR Network for Cryogenic Detectors ERB-FMRX-CT98-0167 and SFB 375-95 f¨ ur Astro-Teilchenphysik der DFG.
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