English
Related papers

Related papers: The DIRAC experiment at CERN

200 papers

SHIP is a new general purpose fixed target facility, proposed at the CERN SPS accelerator. In five years, $2\times 10^{20}$ protons of 400 GeV/c momentum will be dumped on a Molybdenum target. A detector downstream of the target will allow…

Instrumentation and Detectors · Physics 2019-08-13 Annarita Buonaura

Dirac coupled channel calculations are performed phenomenologically for the high-lying excited states that belong to the 2$^+$ gamma vibrational band at the 800-MeV polarized proton inelastic scatterings from the s-d shell nuclei, $^{24}$Mg…

Nuclear Theory · Physics 2017-04-26 Sugie Shim

DIRAC is a freely distributed general-purpose program system for 1-, 2- and 4-component relativistic molecular calculations at the level of Hartree--Fock, Kohn--Sham (including range-separated theory), multiconfigurational…

At photonic Dirac points, electromagnetic waves are governed by the same equations as two-component massless relativistic fermions. However, photonic Dirac points are known to occur in pairs in "photonic graphene" and other similar photonic…

Aims: We measure transition probabilities for Cr II transitions from the z ^4H_J, z ^2D_J, y ^4F_J, and y ^4G_J levels in the energy range 63000 to 68000 cm^{-1}. Methods: Radiative lifetimes were measured using time-resolved laser-induced…

Solar and Stellar Astrophysics · Physics 2015-05-14 J. Gurell , H. Nilsson , L. Engstrom , H. Lundberg , R. Blackwell-Whitehead , K. E. Nielsen , S. Mannervik

COMPASS is a multi-purpose fixed-target experiment at CERN's M2 beam line aimed at studying the structure and spectrum of hadrons. It has collected the so far world's largest data set on diffractive production of the $K^-\pi^-\pi^+$ final…

High Energy Physics - Experiment · Physics 2023-01-03 S. Wallner

The muLan experiment at the Paul Scherrer Institute will measure the lifetime of the positive muon with a precision of 1 ppm, giving a value for the Fermi coupling constant G_F at the level of 0.5 ppm. Meanwhile, by measuring the observed…

Nuclear Experiment · Physics 2020-05-20 F. E. Gray

This report presents a project of an experiment for precision studies of the elastic electron proton scattering in the low momentum transfer region. The project is based on an innovative experimental method which allows for detection of…

Nuclear Experiment · Physics 2019-10-23 A. Vorobyev

The COMPASS experiment makes use of the CERN SPS high-intensitymuon and hadron beams for the investigation of the nucleon spin structure and the spectroscopy of hadrons. One or more outgoing particles are detected in coincidence with the…

High Energy Physics - Experiment · Physics 2008-11-26 COMPASS Collaboration , P. Abbon

The DIRC is a new type of Cherenkov imaging device that will be used for the first time in the BABAR detector at the asymmetric B-factory, PEP-II. It is based on total internal reflection and uses long, rectangular bars made from synthetic…

High Energy Physics - Experiment · Physics 2015-06-25 DIRC Collaboration

AMBER (NA66) is a fixed-target facility at the M2 beam line of CERN SPS, which performs worldwide unique research on the internal structure and the excitation spectrum of hadrons. The approved first phase of the experiment focuses on three…

High Energy Physics - Experiment · Physics 2026-01-13 Bernhard Ketzer , Michela Chiosso

The neutron lifetime is one of the basic parameters in the weak interaction, and is used for predicting the light element abundance in the early universe. Our group developed a new setup to measure the lifetime with the goal precision of…

Interaction cross sections and charged pion spectra in p+C interactions at 31 GeV/c were measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS. These data are required to improve predictions of the neutrino flux for the…

High Energy Physics - Experiment · Physics 2015-03-18 N. Abgrall , A. Aduszkiewicz , B. Andrieu , T. Anticic , N. Antoniou , J. Argyriades , A. G. Asryan , B. Baatar , A. Blondel , J. Blumer , M. Bogusz , L. Boldizsar , A. Bravar , W. Brooks , J. Brzychczyk , A. Bubak , S. A. Bunyatov , O. Busygina , T. Cetner , K. -U. Choi , P. Christakoglou , P. Chung , T. Czopowicz , N. Davis , F. Diakonos , S. Di Luise , W. Dominik , J. Dumarchez , R. Engel , A. Ereditato , L. S. Esposito , G. A. Feofilov , Z. Fodor , A. Ferrero , A. Fulop , X. Garrido , M. Gazdzicki , M. Golubeva , K. Grebieszkow , A. Grzeszczuk , F. Guber , H. Hakobyan , T. Hasegawa , S. Igolkin , A. S. Ivanov , Y. Ivanov , A. Ivashkin , K. Kadija , A. Kapoyannis , N. Katrynska , D. Kielczewska , D. Kikola , J. -H. Kim , M. Kirejczyk , J. Kisiel , T. Kobayashi , O. Kochebina , V. I. Kolesnikov , D. Kolev , V. P. Kondratiev , A. Korzenev , S. Kowalski , S. Kuleshov , A. Kurepin , R. Lacey , J. Lagoda , A. Laszlo , V. V. Lyubushkin , M. Mackowiak , Z. Majka , A. I. Malakhov , A. Marchionni , A. Marcinek , I. Maris , V. Marin , T. Matulewicz , V. Matveev , G. L. Melkumov , A. Meregaglia , M. Messina , St. Mrowczynski , S. Murphy , T. Nakadaira , P. A. Naumenko , K. Nishikawa , T. Palczewski , G. Palla , A. D. Panagiotou , W. Peryt , O. Petukhov , R. Planeta , J. Pluta , B. A. Popov , M. Posiadala , S. Pulawski , W. Rauch , M. Ravonel , R. Renfordt , A. Robert , D. Rohrich , E. Rondio , B. Rossi , M. Roth , A. Rubbia , M. Rybczynski , A. Sadovsky , K. Sakashita , T. Sekiguchi , P. Seyboth , M. Shibata , A. N. Sissakian , E. Skrzypczak , M. Slodkowski , A. S. Sorin , P. Staszel , G. Stefanek , J. Stepaniak , C. Strabel , H. Strobele , T. Susa , P. Szaflik , M. Szuba , M. Tada , A. Taranenko , R. Tsenov , R. Ulrich , M. Unger , M. Vassiliou , V. V. Vechernin , G. Vesztergombi , A. Wilczek , Z. Wlodarczyk , A. Wojtaszek , J. -G. Yi , I. -K. Yoo , W. Zipper

At Central Michigan University we are developing a high-precision Penning trap mass spectrometer (CHIP-TRAP)that will focus on measurements with long-lived radioactive isotopes. CHIP-TRAP will consist of a pair of hyperbolic…

The DIRC is a Cherenkov imaging detector based on total internal reflection for the BaBar detector at PEP-II. The principles of the DIRC ring imaging Cherenkov technique are explained and its choice for the BaBar detector particle…

High Energy Physics - Experiment · Physics 2009-10-30 J. Schwiening

We suggest to measure Pomeron phase and discover odderon via the measurement of charge asymmetry of pions in the diffractive processes $ep\to e\pi^+\pi^- p$, $eA\to e\pi^+\pi^- A$ and in the processes $AA\to AA\pi^+\pi^-$ with two rapidity…

High Energy Physics - Phenomenology · Physics 2007-05-23 I. F. Ginzburg , I. P. Ivanov

The COMPASS experiment at CERN's SPS investigates the structure and excitations of strongly interacting systems. Using reactions of 190 GeV/c pions with protons and nuclear targets, mediated by the strong and electromagnetic interaction, an…

High Energy Physics - Experiment · Physics 2019-08-13 Bernhard Ketzer

We propose an experiment for an accurate measurement of the proton radius. A key feature of our proposal is an iron-free magnetic spectrometer. Projected systematics uncertainties will allow a 1% level accuracy for the $r_p$ value.

Nuclear Experiment · Physics 2015-10-06 B. Wojtsekhowski

The PHENIX experiment, has recently acquired $\sim$ 1 billion minimum bias Au+Au events at $\sqrt s = 200$GeV during the year-2004 run. This high statistics data set, coupled with a state-of-the-art analysis technique, allows for the…

Nuclear Experiment · Physics 2009-11-11 P. Chung

A timely and long-term programme of kaon decay measurements at a new level of precision is presented, leveraging the capabilities of the CERN Super Proton Synchrotron (SPS). The proposed programme is firmly anchored on the experience built…

High Energy Physics - Experiment · Physics 2022-12-01 E. Cortina Gil , J. Jerhot , N. Lurkin , T. Numao , B. Velghe , V. W. S. Wong , D. Bryman , L. Bician , Z. Hives , T. Husek , K. Kampf , M. Koval , A. T. Akmete , R. Aliberti , V. Büscher , L. Di Lella , N. Doble , L. Peruzzo , M. Schott , H. Wahl , R. Wanke , B. Döbrich , L. Montalto , D. Rinaldi , F. Dettori , A. Cardini , A. Lai , L. Bomben , S. Carsi , M. Prest , A. Selmi , G. Lezzani , P. Monti-Guarnieri , L. Perna , P. Dalpiaz , V. Guidi , A. Mazzolari , I. Neri , F. Petrucci , M. Soldani , L. Bandiera , A. Cotta Ramusino , A. Gianoli , M. Romagnoni , A. Sytov , M. Lenti , I. Panichi , G. Ruggiero , A. Bizzeti , F. Bucci , A. Antonelli , E. Di Meco , G. Lanfranchi , S. Martellotti , M. Martini , M. Moulson , D. Paesani , I. Sarra , T. Spadaro , G. Tinti , E. Vallazza , F. Ambrosino , R. Giordano , P. Massarotti , M. Napolitano , G. Saracino , C. Di Donato , G. D'Ambrosio , M. D'Errico , M. Mirra , S. Neshatpour , R. Fiorenza , I. Rosa , D. De Salvador , F. Sgarbossa , G. Anzivino , S. Germani , R. Volpe , P. Cenci , S. Cutini , V. Duk , P. Lubrano , M. Pepe , M. Piccini , F. Costantini , S. Donati , M. Giorgi , S. Giudici , G. Lamanna , E. Pedreschi , J. Pinzino , M. Sozzi , R. Fantechi , V. Giusti , F. Spinella , I. Mannelli , M. Raggi , A. Biagioni , P. Cretaro , O. Frezza , F. Lo Cicero , A. Lonardo , M. Turisini , P. Vicini , R. Ammendola , V. Bonaiuto , A. Fucci , A. Salamon , F. Sargeni , R. Arcidiacono , B. Bloch-Devaux , E. Menichetti , E. Migliore , C. Biino , F. Marchetto , D. Baigarashev , Y. Kambar , D. Kereibay , Y. Mukhamejanov , S. Sakhiyev , A. Briano Olvera , J. Engelfried , N. Estrada-Tristan , R. Piandani , M. A. Reyes Santos , K. A. Rodriguez Rivera , P. C. Boboc , A. M. Bragadireanu , S. A. Ghinescu , O. E. Hutanu , T. Blazek , V. Cerny , A. Kleimenova , Z. Kucerova , D. Martinez Santos , C. Prouve , M. Boretto , F. Brizioli , A. Ceccucci , M. Corvino , H. Danielsson , F. Duval , E. Gamberini , R. Guida , E. B. Holzer , B. Jenninger , G. Lehmann Miotto , P. Lichard , K. Massri , E. Minucci , M. Perrin-Terrin , V. Ryjov , J. Swallow , M. Van Dijk , M. Zamkovsky , R. Marchevski , A. Gerbershagen , J. R. Fry , F. Gonnella , E. Goudzovski , J. Henshaw , C. Kenworthy , C. Lazzeroni , C. Parkinson , A. Romano , J. Sanders , A. Shaikhiev , A. Tomczak , H. Heath , D. Britton , A. Norton , D. Protopopescu , J. B. Dainton , R. W. L. Jones , A. De Santo , F. Salvatore , P. Cooper , D. Coward , P. Rubin
‹ Prev 1 8 9 10 Next ›