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Now showing items 1 - 16 of 53
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The laser control of the muon g-2 experiment at Fermilab
Anastasi, A. Anastasio, A. Avino, S. Basti, A. Bedeschi, F. Boiano, A. Cantatore, G. Cauz, D. Ceravolo, S. Corradi, G. Dabagov, S. Di Meo, P. Driutti, A. Di Sciascio, G. Di Stefano, R. Escalante, O. Ferrari, C. Fienberg, A. T. Fioretti, A. Gabbanini, C. Gagliardi, G. Gioiosa, A. Hampai, D. Hertzog, D. W. Iacovacci, M. Incagli, M. Karuza, M. Kaspar, J. Lusiani, A. Marignetti, F. Mastroianni, S. Moricciani, D. Nath, A. Pauletta, G. Piacentino, G. M. Raha, N. Santi, L. Smith, M. W. Venanzoni, G.
The Muon g - 2 Experiment at Fermilab is expected to start data taking in 2017. It will measure the muon anomalous magnetic moment, a mu =3D (g mu - 2)/2 to an unprecedented precision: the goal is 0.14 parts per million (ppm). The new experiment will require upgrades of detectors, electronics and data acquisition equipment to handle the much higher data volumes and slightly higher instantaneous rates. In particular, it will require a continuous monitoring and state- of- art calibration of the detectors, whose response may vary on both the millisecond and hour long timescale. The calibration system is composed of six laser sources and a light distribution system will provide short light pulses directly into each crystal (54) of the 24 calorimeters which measure energy and arrival time of the decay positrons. A Laser Control board will manage the interface between the experiment and the laser source, allowing the generation of light pulses according to specific needs including detector calibration, study of detector performance in running conditions, evaluation of DAQ performance. Here we present and discuss the main features of the Laser Control board.Download Collect -
Strangeness Photoproduction at the BGO-OD Experiment
Jude, T. C. Alef, S. Bauer, P. Beck, R. Cole, P. Di Salvo, R. Elsner, D. Fantini, A. Freyermuth, O. Ghio, F. Gridnev, A. Hammann, D. Hannappel, J. Kohl, K. Kozlenko, N. Lapik, A. Sandri, P. Levi Lisin, V. Mandaglio, G. Messi, R. Moricciani, D. Nedorezov, V. Novinskiy, D. Pedroni, P. Polonski, A. Reitz, B. Romaniuk, M. Scheluchin, G. Schmieden, H. Sumachev, V. Tarakanov, V. Tillmanns, C.
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CALPRO, an unconventional calorimetry approach
Iacovacci, M. Mastroianni, S. Cimmino, B. Messi, R. Moricciani, D.
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Muon g-2 calibration system data flow
Anastasi, A. Anastasio, A. Avino, S. Bedeschi, F. Boiano, A. Cantatore, G. Cauz, D. Ceravolo, S. Corradi, G. Dabagov, S. Di Falco, S. Di Meo, P. Donati, S. Driutti, A. Di Sciascio, G. Di Stefano, R. Escalante, O. Ferrari, C. Fioretti, A. Gabbanini, C. Gagliardi, G. Gioiosa, A. Hampai, D. Iacovacci, M. Incagli, M. Karuza, M. Lusiani, A. Marignetti, F. Mastroianni, S. Moricciani, D. Nath, A. Pauletta, G. Piacentino, G.M. Raha, N. Santi, L. Smith, M.W. Venanzoni, G.
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Geant4 simulations of the lead fluoride calorimeter
Savchenko, A. A. Tishchenko, A. A. Dabagov, S. B. Anastasi, A. Venanzoni, G. Strikhanov, M. N. Basti, A. Bedeschi, F. Bartolini, M. Cantatore, G. Cauz, D. Corradi, G. Di Sciascio, G. Di Stefano, R. Driutti, A. Escalante, O. Ferrari, C. Fioretti, A. Gabbanini, C. Gioiosa, A. Hampai, D. Iacovacci, M. Karuza, M. Liedl, A. Lusiani, A. Marignetti, F. Mastroianni, S. Moricciani, D. Pauletta, G. Piacentino, G. M. Raha, N. Santi, L.
In this paper we simulate the charged particle interaction with complex structures, including the emission, with help of Geant4. We take into account Cherenkov radiation, transition radiation, bremsstrah-lung, pair production and other accompanying processes. As an application we investigate the full size electromagnetic calorimeter for the muon g-2 experiment at Fermilab. A calorimeter module consists of a Delrin front panel for installation of the laser calibration system, 54 PbF2 Cherenkov crystals wrapped by black Tedlar paper, and silicon photo-multiplier sensors. We report here on results of a simulation of the radiation from positrons striking the calorimeter system. The Cherenkov radiation expansion when a positron moves down through the calorimeter at the arbitrary angle of incidence has been considered. Both spectral and angular distributions of Cherenkov optical photons in different parts of the calorimeter system was evaluated as well as the transition radiation and pre-shower distributions from both the Delrin panel and the Al vacuum chamber of the g-2 storage ring. (C) 2017 Elsevier B.V. All rights reserved.Download Collect -
The calorimeter system of the new muon g-2 experiment at Fermilab
Alonzi, L. P. Anastasi, A. Bjorkquist, R. Cauz, D. Cantatore, G. Dabagov, S. Di Sciascio, G. Di Stefano, R. Fatemi, R. Ferrari, C. Fienberg, A. T. Fioretti, A. Frankenthal, A. Gabbanini, C. Gibbons, L. K. Giovanetti, K. Goadhouse, S. D. Gohn, W. P. Gorringe, T. P. Hampai, D. Hertzog, D. W. Iacovacci, M. Kammel, P. Karuza, M. Kaspar, J. Kiburg, B. Li, L. Marignetti, F. Mastroianni, S. Moricciani, D. Pauletta, G. Peterson, D. A. Pocanic, D. Santi, L. Smith, M. W. Sweigart, D. A. Tishchenko, V. Van Wechelm, T. D. Venanzoni, G. Wall, K. B. Winter, P. Yai, K.
The electromagnetic calorimeter for the new muon (g-2) experiment at Fermilab will consist of arrays of PbF2 Cerenkov crystals read out by large-area silicon photo-multiplier (SiPM) sensors. We report here the requirements for this system, the achieved solution and the results obtained from a test beam using 2.0-4.5 GeV electrons with a 28-element prototype array. (C) 2015 Elsevier B.V. All rights reserved.Download Collect -
A storage ring experiment to detect a proton electric dipole moment
Anastassopoulos, V. Andrianov, S. Baartman, R. Baessler, S. Bai, M. Benante, J. Berz, M. Blaskiewicz, M. Bowcock, T. Brown, K. Casey, B. Conte, M. Crnkovic, J. D. D'Imperio, N. Fanourakis, G. Fedotov, A. Fierlinger, P. Fischer, W. Gaisser, M. O. Giomataris, Y. Grosse-Perdekamp, M. Guidoboni, G. Haciomeroglu, S. Hoffstaetter, G. Huang, H. Incagli, M. Ivanov, A. Kawall, D. Kim, Y. I. King, B. Koop, I. A. Lazarus, D. M. Lebedev, V. Lee, M. J. Lee, S. Lee, Y. H. Lehrach, A. Lenisa, P. Sandri, P. Levi Luccio, A. U. Lyapin, A. MacKay, W. Maier, R. Makino, K. Malitsky, N. Marciano, W. J. Meng, W. Meot, F. Metodiev, E. M. Miceli, L. Moricciani, D. Morse, W. M. Nagaitsev, S. Nayak, S. K. Orlov, Y. F. Ozben, C. S. Park, S. T. Pesce, A. Petrakou, E. Pile, P. Podobedov, B. Polychronakos, V. Pretz, J. Ptitsyn, V. Ramberg, E. Raparia, D. Rathmann, F. Rescia, S. Roser, T. Sayed, H. Kamal Semertzidis, Y. K. Senichev, Y. Sidorin, A. Silenko, A. Simos, N. Stahl, A. Stephenson, E. J. Stroeher, H. Syphers, M. J. Talman, J. Talman, R. M. Tishchenko, V. Touramanis, C. Tsoupas, N. Venanzoni, G. Vetter, K. Vlassis, S. Won, E. Zavattini, G. Zelenski, A. Zioutas, K.
A new experiment is described to detect a permanent electric dipole moment of the proton with a sensitivity of 10(-29) e . cm by using polarized "magic" momentum 0.7 GeV/c protons in an all-electric storage ring. Systematic errors relevant to the experiment are discussed and techniques to address them are presented. The measurement is sensitive to new physics beyond the standard model at the scale of 3000 TeV. (C) 2016 Author(s).Download Collect -
The BGO Calorimeter of BGO-OD Experiment
Bantes, B. Bayadilov, D. Beck, R. Becker, M. Bella, A. Bielefeldt, P. Bieling, J. Bleckwenn, M. Boese, S. Braghieri, A. Brinkmann, K. -Th. Burdeynyi, D. Curciarello, F. De Leo, V. Di Salvo, R. Dutz, H. Elsner, D. Fantini, A. Freyermuth, S. Friedrich, S. Frommberger, F. Ganenko, V. Geffers, D. Gervino, G. Ghio, F. Giardina, G. Girolami, B. Glazier, D. Goertz, S. Gridnev, A. Gutz, E. Hammann, D. Hannappel, J. Hartmann, P. -F. Hillert, W. Ignatov, A. Jahn, R. Joosten, R. Jude, T. C. Klein, F. Koop, K. Krusche, B. Lapik, A. Sandri, P. Levi Lopatin, I. Mandaglio, G. Mei, P. Messil, F. Messi, R. Metag, V. Moricciani, D. Nanova, M. Nedorezov, V. Novinskiy, D. Pedroni, P. Romaniuk, M. Rostomyan, T. Rudnev, N. Schaerf, C. Scheluchin, G. Schmieden, H. Sumachev, V. Tarakanov, V. Vegna, V. Walther, D. Watts, D. Zaunick, H. -G. Zimmermann, T.
The BGO Rugby Ball is a large solid angle electromagnetic calorimeter now installed in the ELSA Facility in Bonn. The BGO is operating in the BGO-OD experiment aiming to study meson photoproduction off proton and neutron induced by a Bremsstrahlung polarized gamma beam of energies from 0.2 to 3.2 GeV and an intensity of 5 x 10(7) photons per second. The scintillating material characteristics and the photomultiplier read-out make this detector particularly suited for the detection of medium energy photons and electrons with very good energy resolution. The detector has been equipped with a new electronics read-out system, consisting of 30 sampling ADC Wie-Ne-R modules which perform the off-line reconstruction of the signal start-time allowing for a good timing resolution. Performances in linearity, resolution and time response have been carefully tested at the Beam Test Facility of the INFN National Laboratories in Frascati by using a matrix of 7 BGO crystals coupled to photomultipliers and equipped with the Wie-Ne-R sampling ADCs.Download Collect -
The Measurement of the Anomalous Magnetic Moment of the Muon at Fermilab
Logashenko, I. Grange, J. Winter, P. Carey, R. M. Hazen, E. Kinnaird, N. Miller, J. P. Mott, J. Roberts, B. L. Crnkovic, J. Morse, W. M. Sayed, H. Kamal Tishchenko, V. Druzhinin, V. P. Shatunov, Y. M. Bjorkquist, R. Chapelain, A. Eggert, N. Frankenthal, A. Gibbons, L. Kim, S. Mikhailichenko, A. Orlov, Y. Rider, N. Rubin, D. Sweigart, D. Allspach, D. Barzi, E. Casey, B. Convery, M. E. Drendel, B. Freidsam, H. Johnstone, C. Johnstone, J. Kiburg, B. Kourbanis, I. Lyon, A. L. Merritt, K. W. Morgan, J. P. Nguyen, H. Ostiguy, J. -F. Para, A. Polly, C. C. Popovic, M. Ramberg, E. Rominsky, M. Soha, A. K. Still, D. Walton, T. Yoshikawa, C. Jungmann, K. Onderwater, C. J. G. Debevec, P. Leo, S. Pitts, K. Schlesier, C. Anastasi, A. Babusci, D. Corradi, G. Hampai, D. Palladino, A. Venanzoni, G. Dabagov, S. Ferrari, C. Fioretti, A. Gabbanini, C. Di Stefano, R. Marignetti, S. Iacovacci, M. Mastroianni, S. Di Sciascio, G. Moricciani, D. Cantatore, G. Karuza, M. Giovanetti, K. Baranov, V. Duginov, V. Khomutov, N. Krylov, V. Kuchinskiy, N. Volnykh, V. Gaisser, M. Haciomeroglu, S. Kim, Y. Lee, S. Lee, M. Semertzidis, Y. K. Won, E. Fatemi, R. Gohn, W. Gorringe, T. Bowcock, T. Carroll, J. King, B. Maxfield, S. Smith, A. Teubner, T. Whitley, M. Wormald, M. Wolski, A. Al-Kilani, S. Chislett, R. Lancaster, M. Motuk, E. Stuttard, T. Warren, M. Flay, D. Kawall, D. Meadows, Z. Syphers, M. Tarazona, D. Chupp, T. Tewlsey-Booth, A. Quinn, B. Eads, M. Epps, A. Luo, G. McEvoy, M. Pohlman, N. Shenk, M. de Gouvea, A. Welty-Rieger, L. Schellman, H. Abi, B. Azfar, F. Henry, S. Gray, F. Fu, C. Ji, X. Li, L. Yang, H. Stockinger, D. Cauz, D. Pauletta, G. Santi, L. Baessler, S. Frlez, E. Pocanic, D. Alonzi, L. P. Fertl, M. Fienberg, A. Froemming, N. Garcia, A. Hertzog, D. W. Kammel, P. Kaspar, J. Osofsky, R. Smith, M. Swanson, E. Lynch, K.
The anomalous magnetic moment of the muon is one of the most precisely measured quantities in experimental particle physics. Its latest measurement at Brookhaven National Laboratory deviates from the Standard Model expectation by approximately 3.5 standard deviations. The goal of the new experiment, E989, now under construction at Fermilab, is a fourfold improvement in precision. Here, we discuss the details of the future measurement and its current status. (C) 2015 AIP Publishing LLC.Download Collect -
U Boson Search in the E ++e -rarrmu +mu -gamma process
Curciarello, F. Babusci, D. Badoni, D. Balwierz-Pytko, I. Bencivenni, G. Bini, C. Bloise, C. Bossi, F. Branchini, P. Budano, A. Caldeira Balkesahl, L. Capon, G. Ceradini, F. Ciambrone, P. Curciarello, F. Czerwinski, E. Dane, E. De Leo, V. De Lucia, E. De Robertis, G. De Santis, A. De Simone, A. Di Domenico, A. Di Donato, C. Di Salvo, R. Domenici, D. Erriquez, O. Fanizzi, G. Fantini, A. Felici, G. Fiore, S. Franzini, P. Gauzzi, P. Giardina, G. Giovannella, S. Gonnella, F. Graziani, E. Happacher, F. Heijkenskjold, L. Hoistad, B. Iafolla, L. Iarocci, E. Jacewicz, M. Johansson, T. Kacprzak, K. Kluge, W. Kupsc, A. Lee-Franzini, J. Loddo, F. Lukin, P. Mandaglio, G. Martemianov, M. Martini, M. Mascolo, M. Messi, R. Miscetti, S. Morello, G. Moricciani, D. Moskal, P. Muller, S. Nguyen, F. Passeri, A. Patera, V. Prado Longhi, I. Ranieri, A. Redmer, C.F. Santangelo, P. Sarra, I. Schioppa, M. Sciascia, B. Silarski, M. Taccini, C. Tortora, L. Venanzoni, G. Versaci, R. Wislicki, W. Wolke, M. Zdebik, J.
Following recent puzzling astrophysical results and recent theoretical studies, a search for a relatively low mass (1 GeV ) new vector gauge boson (called the U boson) was performed by means of the KLOE detector. Investigations were carried out using the Initial State Radiation and searching for the signal from the U boson in the e ++e -rarrmu +mu -gamma process. The KLOE experiment, at the phi-factory DAPhiNE (INFN-LNF), is the first to have exploited ISR to precisely determine cross sections of e ++e -rarrpi +pi - gamma(gamma) and e ++e -rarrmu +mu -gamma(gamma) processes below 1 GeV . Investigations were based on the data sample collected in 2002, which corresponds to integrated luminosity of 239.29 pb -1 . No evidence was found and a preliminary upper limit in the mass range between 600 and 1000 MeV was extracted.Download Collect -
Test of candidate light distributors for the muon (g-2) laser calibration system
Anastasi, A. Babusci, D. Baffigi, F. Cantatore, G. Cauz, D. Corradi, G. Dabagov, S. Di Sciascio, G. Di Stefano, R. Ferrari, C. Fienberg, A. T. Fioretti, A. Fulgentini, L. Gabbanini, C. Gizzi, L. A. Hampai, D. Hertzog, D. W. Iacovacci, M. Karuza, M. Kaspar, J. Koester, P. Labate, L. Mastroianni, S. Moricciani, D. Pauletta, G. Santi, L. Venanzoni, G.
The new muon (g-2) experiment E989 at Fermilab will be equipped with a laser calibration system for all the 1296 channels of the calorimeters. An integrating sphere and an alternative system based on an engineered diffuser have been considered as possible light distributors for the experiment. We present here a detailed comparison of the two based on temporal response, spatial uniformity, transmittance and time stability. (C) 2015 Elsevier B.V. All rights reserved.Download Collect -
–2 experiment
Driutti, A. Basti, A. Bedeschi, F. Cantatore, G. Cauz, D. Corradi, G. Dabagov, S. Di Falco, S. Di Sciascio, G. Di Stefano, R. Donati, S. Escalante, O. Ferrari, C. Fioretti, A. Gabbanini, C. Gioiosa, A. Hampai, D. Iacovacci, M. Incagli, M. Karuza, M. Lusiani, A. Marignetti, F. Mastroianni, S. Moricciani, D. Nath, A. Pauletta, G. Piacentino, G.M. Raha, N. Santi, L. Smith, M. Sorbara, M. Venanzoni, G.
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Results from polarized experiments at LEGS and GRAAL
D'Angelo, A. Ardashev, K. Bade, C. Bartalini, O. Bellini, V. Blecher, M. Bocquet, J. -P. Capogni, M. Caracappa, A. Casano, L. E. Castoldi, M. Di Salvo, R. Fantini, A. Franco, D. Gervino, G. Ghio, F. Giardina, G. Gibson, C. Girolami, B. Giusa, A. Gluekler, H. Hicks, K. Hoblit, S. Honig, A. Kageya, T. Khandaker, M. Kistner, O. C. Kizilgul, S. Kucuker, S. Lapik, A. Lehmann, A. Sandri, P. Levi Lieres, A. Lowry, M. Lucas, M. Mahon, J. Mammoliti, F. Mandaglio, G. Manganaro, M. Miceli, L. Moricciani, D. Mushkarenkov, A. Nedorezov, V. Norum, B. Pap, M. Preedom, B. Seyfarth, H. Randieri, C. Rebreyend, D. Rudnev, N. Russo, G. Sandorfi, A. Schaerf, C. Sperduto, M. -L. Stroher, H. Sutera, M. -C. Thorn, C. E. Turinge, A. Vegna, V. Whisnant, C. S. Wang, K. Wei, X.
Compton backscattering gamma ray beams are characterized by a high degree of linear and circular polarization with low unpolarized backgrounds and have proven to provide very precise measurements of polarization observables. Latest results from LEGS and GRAAL experiments on proton and deuteron targets are presented. The Sigma beam asymmetry for omega photoproduction has been measured by the GRAAL collaboration for both the omega -> pi(0)gamma and the omega -> pi(+)pi(+)pi(0) decay channels on the proton target; single and double polarization asymmetries have been provided also for the K photoproduction channel. E and G double polarization asymmetries for single pion photoproduction on the proton and deuteron have been measured at LEGS using a frozen spin HD target.Download Collect -
Complete Photo-production Experiments
D'Angelo, A. Ardashev, K. Bade, C. Bartalini, O. Bellini, V. Blecher, M. Bocquet, J. -P. Capogni, M. Caracappa, A. Casano, L. E. Castoldi, M. Di Salvo, R. Fantini, A. Franco, D. Gervino, G. Ghio, F. Giardina, G. Gibson, C. Girolami, B. Giusa, A. Gluekler, H. Hicks, K. Hoblit, S. Honig, A. Kageya, T. Khandaker, M. Kistner, O. C. Kizilgul, S. Kucuker, S. Lapik, A. Lehmann, A. Sandri, P. Levi Lleres, A. Lowry, M. Lucas, M. Mahon, J. Mammoliti, F. Mandaglio, G. Manganaro, M. Miceli, L. Moricciani, D. Mushkarenkov, A. Nedorezov, V. Norum, B. Pap, M. Preedom, B. Seyfarth, H. Randieri, C. Rebreyend, D. Rudnev, N. Russo, G. Sandorfi, A. Schaerf, C. Sperduto, M. -L. Stroeher, H. Sutera, M. -C. Thorn, C. E. Turinge, A. Vegna, V. Whisnant, C. S. Wang, K. Wei, X.
The extraction of resonance parameters from meson photo-reaction data is a challenging effort, that would greatly benefit from the availability of several polarization observables, measured for each reaction channel on both proton and neutron targets. In the aim of obtaining such complete experiments, polarized photon beams and targets have been developed at facilities, worldwide. We report on the latest results from the LEGS and GRAAL collaborations, providing single and double polarization measurements on pseudo-scalar meson photo-production from the nucleon.Download Collect -
The monitoring electronics of the laser calibration system in the Muon g-2 experiment
Anastasi, A. Anastasio, A. Avino, S. Bedeschi, F. Boiano, A. Cantatore, G. Cauz, D. Ceravolo, S. Corradi, G. Dabagov, S. Di Falco, S. Di Meo, S. Donati, S. Driutti, A. Di Sciascio, G. Di Stefano, R. Escalante, O. Ferrari, C. Fioretti, A. Gabbanini, C. Gagliardi, G. Gioiosa, A. Hampai, D. Iacovacci, M. Incagli, M. Karuza, M. Lusiani, A. Marignetti, F. Mastroianni, S. Moricciani, D. Nath, A. Pauletta, G. Piacentino, G.M. Raha, N. Santi, L. Smith, M.W. Venanzoni, G.
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omega PHOTOPRODUCTION AT GRAAL RID B-1239-2012 RID A-2439-2012 RID B-7657-2011
Vegna, V. Bellini, V. Bocquet, J. P. Casano, L. D'Angelo, A. Di Salvo, R. Fantini, A. Franco, D. Gervino, G. Ghio, F. Giardina, G. Girolami, B. Giusa, A. Ignatov, A. S. Lapik, A. Lleres, A. Sandri, P. Levi Mammoliti, F. Mandaglio, G. Manganaro, M. Moricciani, D. Mushkarenkov, A. N. Nedorezov, V. G. Randieri, C. Rebreyend, D. Rudnev, N. V. Russo, G. Schaerf, C. Sperduto, M. L. Sutera, M. C. Turinge, A.
The study of meson photoproduction on the nucleon is a very important tool to complete the puzzle of baryon excited states. GRAAL aim is the measurement of cross sections and of beam asymmetries for all the photonuclear reactions accessible in the energy range from 600 MeV up to 1.5 GeV. In the following preliminary results of the Sigma beam asymmetry for omega photoproduction on the free proton in Hydrogen and on the quasi-free nucleon in Deuterium are shown. GRAAL is the first experiment in which both the charged and the radiative decay of omega meson are studied. Since the beam asymmetry is independent of the decay mode, the comparison of the results from the two channel allows an important check on data consistency. Results on the free proton are in good agreement with theoretical prediction from Zhao model and confirm the presence of P(13)(1720) state. The analysis performed for the radiative decay is applied to the process of. photoproduction on the quasi free nucleon in Deuterium.Download Collect