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207 results on '"Danè, E."'

1. Enhancing the light yield of He:CF$_4$ based gaseous detector

Author

Amaro, F. D., Antonietti, R., Baracchini, E., Benussi, L., Bianco, S., Campagnola, R., Capoccia, C., Caponero, M., Cardoso, D. S., de Carvalho, L. G. M., Cavoto, G., Costa, I. Abritta, Croce, A., Dané, E., Dho, G., Di Giambattista, F., Di Marco, E., D'Astolfo, M., D'Imperio, G., Fiorina, D., Iacoangeli, F., Islam, Z., Jùnior, H. P. L., Kemp, E., Maccarrone, G., Mano, R. D. Passos, Gregorio, R. R. M., Marques, D. J. Gaspar, Mazzitelli, G., McLean, A. G., Messina, A., Meloni, P., Monteiro, C. M. Bernardes, Nobrega, R. A., Pains, I. F., Paoletti, E., Passamonti, L., Petrucci, F., Piacentini, S., Piccolo, D., Pierluigi, D., Pinci, D., Prajapati, A., Renga, F., Roque, R. J. da Cruz, Rosatelli, F., Russo, A., Santos, J. M. F. dos, Saviano, G., Silva, P. A. O. C., Spooner, N. J. Curwen, Tesauro, R., Tomassini, S., and Torelli, S.

Subjects
Physics - Instrumentation and Detectors
Abstract

The CYGNO experiment aims to build a large ($\mathcal{O}(10)$ m$^3$) directional detector for rare event searches, such as nuclear recoils (NRs) induced by dark matter (DM), such as weakly interactive massive particles (WIMPs). The detector concept comprises a time projection chamber (TPC), filled with a He:CF$_4$ 60/40 scintillating gas mixture at room temperature and atmospheric pressure, equipped with an amplification stage made of a stack of three gas electron multipliers (GEMs) which are coupled to an optical readout. The latter consists in scientific CMOS (sCMOS) cameras and photomultipliers tubes (PMTs). The maximisation of the light yield of the amplification stage plays a major role in the determination of the energy threshold of the experiment. In this paper, we simulate the effect of the addition of a strong electric field below the last GEM plane on the GEM field structure and we experimentally test it by means of a 10$\times$10 cm$^2$ readout area prototype. The experimental measurements analyse stacks of different GEMs and helium concentrations in the gas mixture combined with this extra electric field, studying their performances in terms of light yield, energy resolution and intrinsic diffusion. It is found that the use of this additional electric field permits large light yield increases without degrading intrinsic characteristics of the amplification stage with respect to the regular use of GEMs., Comment: Correction of typos in Section 2 and 6. Improved quality of plots with some modifications to clarify the content

Published
2024
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2. Charge Amplification in Low Pressure CF4:SF6:He Mixtures with a Multi-Mesh ThGEM for Directional Dark Matter Searches

Author

Amaro, F. D., Baracchini, E., Benussi, L., Bianco, S., Borra, F., Capoccia, C., Caponero, M., Cardoso, D. S., Cavoto, G., Costa, I. A., Crane, T., Dane, E., DAstolfo, M., Dho, G., Di Giambattista, F., DImperio, G., Di Marco, E., Santos, J. M. F. Dos, Ezeribe, A. C., Fiorina, D., Iacoangeli, F., Junior, H. P. Lima, Lopes, G. S. P., Maccarrone, G., Mano, R. D. P., Gregorio, R. R. Marcelo, Marques, D. J. G., Mazzitelli, G., McLean, A. G., Monteiro, C. M. B., Nobrega, R. A., Pains, I. F., Paoletti, E., Passamonti, L., Piacentini, S., Piccolo, D., Pierluigi, D., Pinci, D., Prajapati, A., Renga, F., Roque, R. J. d. C., Rosatelli, F., Russo, A., Saviano, G., Scarff, A., Spooner, N. J. C., Tesauro, R., Tomassini, S., and Torelli, S.

Subjects
Physics - Instrumentation and Detectors
Abstract

The CYGNO collaboration is developing next generation directional Dark Matter (DM) detection experiments, using gaseous Time Projection Chambers (TPCs), as a robust method for identifying Weakly Interacting Massive Particles (WIMPs) below the Neutrino Fog. SF6 is potentially ideal for this since it provides a high fluorine content, enhancing sensitivity to spin-dependent interactions and, as a Negative Ion Drift (NID) gas, reduces charge diffusion leading to improved positional resolution. CF4, although not a NID gas, has also been identified as a favourable gas target as it provides a scintillation signal which can be used for a complimentary light/charge readout approach. These gases can operate at low pressures to elongate Nuclear Recoil (NR) tracks and facilitate directional measurements. In principle, He could be added to low pressure SF6/CF4 without significant detriment to the length of 16S, 12C, and 19F recoils. This would improve the target mass, sensitivity to lower WIMP masses, and offer the possibility of atmospheric operation; potentially reducing the cost of a containment vessel. In this article, we present gas gain and energy resolution measurements, taken with a Multi-Mesh Thick Gaseous Electron Multiplier (MMThGEM), in low pressure SF6 and CF4:SF6 mixtures following the addition of He. We find that the CF4:SF6:He mixtures tested were able to produce gas gains on the order of 10^4 up to a total pressure of 100 Torr. These results demonstrate an order of magnitude improvement in charge amplification in NID gas mixtures with a He component., Comment: Corresponding Author: A.G. McLean

Published
2024

3. The CYGNO experiment, a directional detector for direct Dark Matter searches

Author

Amaro, F. D., Baracchini, E., Benussi, L., Bianco, S., Capoccia, C., Caponero, M., Cardoso, D. S., Cavoto, G., Cortez, A., Costa, I. A., Dané, E., Dho, G., Di Giambattista, F., Di Marco, E., D'Imperio, G., Iacoangeli, F., Jùnior, H. P. L., Lopes, G. S. P., Maccarrone, G., Mano, R. D. P., Gregorio, R. R. M., Marques, D. J. G., Mazzitelli, G., McLean, A. G., Messina, A., Monteiro, C. M. B., Nobrega, R. A., Pains, I. F., Paoletti, E., Passamonti, L., Pelosi, S., Petrucci, F., Piacentini, S., Piccolo, D., Pierluigi, D., Pinci, D., Prajapati, A., Renga, F., Roque, R. J. C., Rosatelli, F., Russo, A., Santos, J. M. F. dos, Saviano, G., Spooner, N. J. C., Tesauro, R., Tomassini, S., and Torelli, S.

Subjects
Physics - Instrumentation and Detectors
Abstract

The CYGNO project aims at the development of a high precision optical readout gaseous Tima Projection Chamber (TPC) for directional dark matter (DM) searches, to be hosted at Laboratori Nazionali del Gran Sasso (LNGS). CYGNO employs a He:CF$_4$ gas mixture at atmospheric pressure with a Gas Electron Multiplier (GEM) based amplification structure coupled to an optical readout comprised of sCMOS cameras and photomultiplier tubes (PMTs). This experimental setup allows to achieve 3D tracking and background rejection down to O(1) keV energy, to boost sensitivity to low WIMP masses. The characteristics of the optical readout approach in terms of the light yield will be illustrated along with the particle identification properties. The project timeline foresees, in the next 2-3 years, the realisation and installation of a 0.4 m$^3$ TPC in the underground laboratories at LNGS to act as a demonstrator. Finally, the studies of the expected DM sensitivities of the CYGNO demonstrator will be presented.

Published
2023
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4. Direct tests of T, CP, CPT symmetries in transitions of neutral K mesons with the KLOE experiment

Author

Babusci, D., Berłowski, M., Bloise, C., Bossi, F., Branchini, P., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., D'Amico, R., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Domenico, A., Diociaiuti, E., Domenici, D., D'Uffizi, A., Fantini, G., Gajos, A., Gamrat, S., Gauzzi, P., Giovannella, S., Graziani, E., Kang, X., Kupść, A., Mandaglio, G., Martini, M., Miscetti, S., Moskal, P., Passeri, A., del Rio, E. Pérez, Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Wiślicki, W., Wolke, M., and Bernabéu, J.

Subjects
High Energy Physics - Experiment
Abstract

Tests of the T, CP and CPT symmetries in the neutral kaon system are performed by the direct comparison of the probabilities of a kaon transition process to its symmetry-conjugate. The exchange of in and out states required for a genuine test involving an anti-unitary transformation implied by time-reversal is implemented exploiting the entanglement of $K^0\bar{K}{}^0$ pairs produced at a $\phi$-factory. A data sample collected by the KLOE experiment at DA$\Phi$NE corresponding to an integrated luminosity of about 1.7 fb$^{-1}$ is analysed to study the $\Delta$t distributions of the $\phi\to K_{S}K_{L}\to \pi^+\pi^- \: \pi^{\pm}e^{\mp}\nu$ and $\phi\to K_{S}K_{L}\to \pi^{\pm}e^{\mp}\nu \: 3\pi^0$ processes, with $\Delta$t the difference of the kaon decay times. A comparison of the measured $\Delta$t distributions in the asymptotic region $\Delta t \gg \tau_{S}$ allows to test for the first time T and CPT symmetries in kaon transitions with a precision of few percent, and to observe CP violation with this novel method., Comment: 26 pages, 10 figures. Minor style corrections applied before journal submission. Sumbmitted to Physics Letters B

Published
2022

5. Measurement of the $K_S \to \pi e \nu$ branching fraction with the KLOE experiment

Author

Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., D'Amico, R., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Diociaiuti, E., Domenici, D., D'Uffizi, A., Fantini, G., Gajos, A., Gamrat, S., Gauzzi, P., Giovannella, S., Graziani, E., Kang, X., Kupsc, A., Mandaglio, G., Martini, M., Miscetti, S., Moskal, P., Passeri, A., del Rio, E. Perez, Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

The branching fraction for the decay $K_S \to \pi e \nu$ has been measured with a sample of 300 million $K_S$ mesons produced in $\phi \to K_L K_S$ decays recorded by the KLOE experiment at the DA$\Phi$NE $e^+e^-$ collider. Signal decays are selected by a boosted decision tree built with kinematic variables and time-of-flight measurements. Data control samples of $K_L \to \pi e \nu$ decays are used to evaluate signal selection efficiencies. A fit to the reconstructed electron mass distribution finds 49647$\pm$316 signal events. Normalising to the $K_S \to \pi^+\pi^-$ decay events the result for the branching fraction is $\mathcal{B}(K_S \to \pi e \nu) = (7.211 \pm 0.046_{\rm stat} \pm 0.052_{\rm syst}) \times10^{-4}$. The combination with our previous measurement gives $\mathcal{B}(K_S \to \pi e \nu) = (7.153 \pm 0.037_{\rm stat} \pm 0.043_{\rm syst}) \times10^{-4}$. From this value we derive $f_+(0)|V_{us}| = 0.2170 \pm 0.009$., Comment: arXiv admin note: substantial text overlap with arXiv:1912.05990

Published
2022

6. Attosecond delays of high harmonic emissions from isotopes of molecular hydrogen measured by Gouy phase XUV interferometer

Author

Mustary, Mumta Hena, Xu, Liang, Wu, Wanyang, Haram, Nida, Laban, Dane E., Xu, Han, He, Feng, Litvinyuk, Igor V., and Sang, R. T.

Subjects
Physics - Atomic Physics, Physics - Chemical Physics, Physics - Optics
Abstract

High harmonic spectroscopy can access structural and dynamical information on molecular systems encoded in amplitude and phase of high harmonic generation (HHG) signals4. However, measurement of the harmonic phase is a daunting task. Here we present a precise measurement of HHG phase difference between two isotopes of molecular hydrogen using the advanced extreme-ultraviolet (XUV) Gouy phase interferometer. The measured phase difference is about 200 mrad, corresponding to 3 attoseconds (1 as = 10^-18 s) time delay which is nearly independent of harmonic order. The measurements agree very well with numerical calculations of a four-dimensional time-dependent Schroedinger equation. Numerical simulations also reveal the effects of molecular orientation and intra-molecular two-centre interference on the measured phase difference. This technique opens a new avenue for measuring the phase of harmonic emission for different atoms and molecules. Together with isomeric or isotopic comparisons it also enables the observation of subtle effects of molecular structures and nuclear motion on electron dynamics in strong laser fields.

Published
2021

7. Precision tests of Quantum Mechanics and CPT symmetry with entangled neutral kaons at KLOE

Author

Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., D'Amico, R., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Diociaiuti, E., Domenici, D., D'Uffizi, A., Fantini, A., Fantini, G., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kang, X., Kisielewska-Kamińska, D., Kozyrev, E. A., Krzemien, W., Kupsc, A., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Moricciani, D., Moskal, P., Passeri, A., Patera, V., del Rio, E. Perez, Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

The quantum interference between the decays of entangled neutral kaons is studied in the process $\phi\rightarrow K_S K_L \rightarrow\pi^+\pi^-\pi^+\pi^-$, which exhibits the characteristic Einstein--Podolsky--Rosen correlations that prevent both kaons to decay into $\pi^+\pi^-$ at the same time. This constitutes a very powerful tool for testing at the utmost precision the quantum coherence of the entangled kaon pair state, and to search for tiny decoherence and CPT violation effects, which may be justified in a quantum gravity framework. The analysed data sample was collected with the KLOE detector at DA$\Phi$NE, the Frascati $\phi$-factory, and corresponds to an integrated luminosity of about 1.7 fb$^{-1}$, i.e. to about $1.7 \times 10^9$ $\phi\rightarrow K_S K_L$ decays produced. From the fit of the observed $\Delta t$ distribution, being $\Delta t$ the difference of the kaon decay times, the decoherence and CPT violation parameters of various phenomenological models are measured with a largely improved accuracy with respect to previous analyses. The results are consistent with no deviation from quantum mechanics and CPT symmetry, while for some parameters the precision reaches the interesting level at which -- in the most optimistic scenarios -- quantum gravity effects might show up. They provide the most stringent limits up to date on the considered models., Comment: 17 pages 6 figures

Published
2021

8. Study of long term stability of a 50 liters TPC, based on TRIPLE-GEM with optical readout, for the CYGNO experiment

Author

Amaro, F.D., Antonietti, R., Baracchini, E., Benussi, L., Bianco, S., Borra, F., Capoccia, C., Caponero, M., Cardoso, D.S., Cavoto, G., Costa, I.A., Dané, E., Dho, G., Di Giambattista, F., Di Marco, E., D’Imperio, G., Iacoangeli, F., Lima, H.P., Júnior, Kemp, E., Lopes, G.S.P., Maccarrone, G., Mano, R.D.P., Marcelo Gregorio, R.R., Marques, D.J.G., Mazzitelli, G., McLean, A.G., Meloni, P., Messina, A., Monteiro, C.M.B., Nobrega, R.A., Pains, I.F., Paoletti, E., Passamonti, L., Petrucci, F., Piacentini, S., Piccolo, D., Pierluigi, D., Pinci, D., Prajapati, A., Renga, F., Roque, R.J.d.C., Rosatelli, F., Russo, A., dos Santos, J.M.F., Saviano, G., Spooner, N.J.C., Tesauro, R., Tomassini, S., and Torelli, S.

Published
2024
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10. Upper limit on the $\eta\to\pi^{+}\pi^{-}$ branching fraction with the KLOE experiment

Author

Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Domenici, D., D'Uffizi, A., Fantini, A., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kang, X., Kisielewska-Kamińska, D., Kozyrev, E. A., Krzemien, W., Kupsc, A., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Moricciani, D., Moskal, P., Parzych, S., Passeri, A., Patera, V., del Rio, E. Perez, Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

Based on an integrated luminosity of 1.61 fb$^{-1}$ $e^+e^-$ collision data collected with the KLOE detector at DA$\Phi$NE, the Frascati $\phi$-factory, a search for the $P$- and $CP$-violating decay $\eta\to\pi^{+}\pi^{-}$ has been performed. Radiative $\phi\to\eta\gamma$ decay is exploited to access the $\eta$ mesons. No signal is observed in the $\pi^{+}\pi^{-}$ invariant mass spectrum, and the upper limit on the branching fraction at 90\% confidence level is determined to be ${\mathcal B}(\eta\to\pi^{+}\pi^{-})<4.9\times10^{-6}$, which is approximately three times smaller than the previous KLOE result. From the combination of these two measurements we get ${\mathcal B}(\eta\to\pi^{+}\pi^{-}) < 4.4\times10^{-6}$ at 90\% confidence level., Comment: 11 pages, 3 figures

Published
2020
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11. Measurement of the branching fraction for the decay $K_S \to \pi \mu \nu$ with the KLOE detector

Author

Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwisnski, E., D'Agostini, G., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Domenici, D., D'Uffizi, A., Fantini, A., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kang, X., Kisielewska-Kamisnska, D., Kozyrev, E. A., Krzemien, W., Kupsc, A., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Moricciani, D., Moskal, P., Parzych, S., Passeri, A., Patera, V., del Rio, E. Perez, Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wislicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract

Based on a sample of 300 million $K_S$ mesons produced in $\phi \to K_L K_S$ decays recorded by the KLOE experiment at the DA$\Phi$NE $e^+e^-$ collider we have measured the branching fraction for the decay $K_S \to \pi \mu \nu$. The $K_S$ mesons are identified by the interaction of $K_L$ mesons in the detector. The $K_S \to \pi \mu \nu$ decays are selected by a boosted decision tree built with kinematic variables and by a time-of-flight measurement. Signal efficiencies are evaluated with data control samples of $K_L \to \pi \mu \nu$ decays. A fit to the reconstructed muon mass distribution finds $7223 \pm 180$ signal events. Normalising to the $K_S \to \pi^+ \pi^-$ decay events the result for the branching fraction is $\mathcal{B}(K_S \to \pi \mu \nu) = (4.56 \pm 0.11_{\rm stat} \pm 0.17_{\rm syst})\times10^{-4}$., Comment: 16 pages, 12 figures, Accepted in PLB

Published
2019
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12. Long-term Operation of the Multi-Wire-Proportional-Chambers of the LHCb Muon System

Author

Albicocco, F. P., Anderlini, L., Anelli, M., Archilli, F., Auriemma, G., Baldini, W., Bencivenni, G., Bondar, N., Bochin, B., Brundu, D., Cadeddu, S., Campana, P., Carboni, G., Cardini, A., Carletti, M., Casu, L., Chubykin, A., Ciambrone, P., Dané, E., De Simone, P., Fontana, M., Fresch, P., Gatta, M., Gavrilov, G., Gets, S., Graziani, G., Kashchuk, A., Korolev, M., Kotriakhova, S., Kuznetsova, E., Lai, A., Levitskaya, O., Maev, O., Maysuzenko, D., Martellotti, G., Nasybulin, S., Neustroev, P., Oldeman, R. G. C., Palutan, M., Passaleva, G., Penso, G., Pinci, D., Santacesaria, R., Santimaria, M., Santovetti, E., Saitta, B., Saputi, A., Sarti, A., Satriano, C., Satta, A., Schmidt, B., Schneider, T., Sciascia, B., Sciubba, A., Vazquez-Gomez, R., Vecchi, S., and Vorobyev, A.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

The muon detector of LHCb, which comprises 1368 multi-wire-proportional-chambers (MWPC) for a total area of 435 m2, is the largest instrument of its kind exposed to such a high-radiation environment. In nine years of operation, from 2010 until 2018, we did not observe appreciable signs of ageing of the detector in terms of reduced performance. However, during such a long period, many chamber gas gaps suffered from HV trips. Most of the trips were due to Malter-like effects, characterised by the appearance of local self-sustained high currents, presumably originating from impurities induced during chamber production. Very effective, though long, recovery procedures were implemented with a HV training of the gaps in situ while taking data. The training allowed most of the affected chambers to be returned to their full functionality and the muon detector efficiency to be kept close to 100%. The possibility of making the recovery faster and even more effective by adding a small percentage of oxygen in the gas mixture has been studied and successfully tested., Comment: 15 pages, 9 figures

Published
2019
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13. 50 litres TPC with sCMOS-based optical readout for the CYGNO project

Author

Mazzitelli, G., Domingues, F. Amaro, Baracchini, E., Benussi, L., Bianco, S., Capoccia, C., Caponero, M., Cardoso, D. Santos, Cavoto, G., Cortez, A., Costa, I. Abritta, Dané, E., Dho, G., Giambattista, F. Di, Marco, E. Di, D’Imperio, G., Iacoangeli, F., Júnior, H. Pessoa Lima, Lopes, G. Sebastiao Pinheiro, Maccarrone, G., Mano, R. Daniel Passos, Gregorio, R. Renz Marcelo, Marques, D. José Gaspar, McLean, A. Gregor, Messina, A., Monteiro, C. Maria Bernardes, Nobrega, R. Antunes, Pains, I. Fonseca, Paoletti, E., Passamonti, L., Pelosi, S., Petrucci, F., Piacentini, S., Piccolo, D., Pierluigi, D., Pinci, D., Prajapati, A., Renga, F., Riggio, C., Rodano, A., da Cruz Roque, R. Joana, Rosatelli, F., Russo, A., Santos, J. Marques Ferreira dos, Saviano, G., Spooner, N. John Curwen, Tesauro, R., Tomassini, S., Torelli, S., and Tozzi, D.

Published
2023
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14. Combined limit on the production of a light gauge boson decaying into $\mu^+\mu^-$ and $\pi^+\pi^-$

Author

Collaboration, KLOE-2, Anastasi, A., Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostinio, G., Dané, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Domenici, D., D'Uffizi, A., Fantini, A., Fantini, G., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kang, X., Kisielewska-Kamińska, D., Kozyrev, E. A., Krzemien, W., Kupsc, A., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Moricciani, D., Moskal, P., Passeri, A., Patera, V., del Rio, E. Perez, Raha, N., Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

We searched for the $\mu^+\mu^-$ decay of a light vector gauge boson, also known as dark photon, in the $e^+ e^- \to \mu^+ \mu^- \gamma_{\rm ISR}$ process by means of the Initial State Radiation (ISR) method. We used 1.93~fb$^{-1}$ of data collected by the KLOE experiment at the DA$\Phi$NE $\phi$-factory. No structures have been observed over the irreducible $\mu^+ \mu^-$ background. A 90\% CL limit on the ratio $\varepsilon^2=\alpha^{\prime}/\alpha$ between the dark coupling constant and the fine structure constant of $ 3\times 10^{-6}-2\times 10^{-7}$ has been set in the dark photon mass region between 519 MeV and 973 MeV. This new limit has been combined with the published result obtained investigating the hypothesis of the dark photon decaying into hadrons in $e^+ e^- \to \pi^+ \pi^- \gamma_{\rm ISR}$ events. The combined 90\% CL limit increases the sensitivity especially in the $\rho-\omega$ interference region and excludes $\varepsilon^2$ greater than $(13-2)\times 10^{-7}$. For dark photon masses greater than 600 MeV the combined limit is lower than 8~$\times\, 10^{-7}$ resulting more stringent than present constraints from other experiments., Comment: 7 pages, 9 figures, 1 table, accepted for publication in Physics Letters B

Published
2018
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15. Measurement of the charge asymmetry for the $K_S \rightarrow \pi e \nu$ decay and test of CPT symmetry with the KLOE detector

Author

Anastasi, A., Babusci, D., Berłowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Cao, B., Capon, G., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Domenici, D., D'Uffizi, A., Fantini, A., Fantini, G., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kang, X., Kisielewska-Kamińska, D., Kozyrev, E. A., Krzemień, W., Kupść, A., Loffredo, S., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Moricciani, D., Moskal, P., Passeri, A., Patera, V., del Rio, E. Perez, Raha, N., Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

Using 1.63 fb$^{-1}$ of integrated luminosity collected by the KLOE experiment about $7\times 10^4$ $K_S \rightarrow \pi^{\pm}e^{\mp}\nu$ decays have been reconstructed. The measured value of the charge asymmetry for this decay is $A_S = (-4.9 \pm 5.7_{stat} \pm 2.6_{syst}) \times 10^{-3}$, which is almost twice more precise than the previous KLOE result. The combination of these two measurements gives $A_S = (-3.8 \pm 5.0_{stat} \pm 2.6_{syst}) \times 10^{-3}$ and, together with the asymmetry of the $K_L$ semileptonic decay, provides significant tests of the CPT symmetry. The obtained results are in agreement with CPT invariance., Comment: submitted to JHEP

Published
2018
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16. The Mu2e Calorimeter Final Technical Design Report

Author

Atanov, N., Baranov, V., Budagov, J., Ceravolo, S., Cervelli, F., Colao, F., Cordelli, M., Corradi, G., Dane, E., Davydov, Y., Di Falco, S., Donati, S., Diociaiuti, E., Donghia, R., Echenard, B., Flood, K., Giovannella, S., Glagolev, V., Grancagnolo, F., Happacher, F., Hitlin, D., Martini, M., Miscetti, S., Miyashita, T., Morescalchi, L., Murat, P., Pasciuto, D., Pezzullo, G., Porter, F., Radicioni, T., Raffaelli, F., Ricci, M., Saputi, A., Sarra, I., Spinella, F., Tagnani, D., Tassielli, G., Tereshchenko, V., Usubov, Z., and Zhu, R. Y.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

Since the first version of the Mu2e TDR released at the beginning of 2015, the Mu2e Calorimeter system has undergone a long list of changes to arrive to its final design. These changes were primarily caused by two reasons: (i) the technology choice between the TDR proposed solution of BaF2 crystals readout with solar blind Avalanche Photodiodes (APDs) and the backup option of CsI crystals readout with Silicon Photomultipliers (SiPM) has been completed and (ii) the channels numbering, the mechanical system and the readout electronics were substantially modified while proceeding with engineering towards the final project. This document updates the description of the calorimeter system adding the most recent engineering drawings and tecnical progresses., Comment: TDR

Published
2018

17. Design, status and perspective of the Mu2e crystal calorimeter

Author

Atanov, N., Baranov, V., Budagov, J., Cervelli, F., Colao, F., Diociaiuti, E., Cordelli, M., Corradi, G., Danè, E., Davydov, Yu., Donati, S., Donghia, R., Di Falco, S., Echenard, B., Morescalchi, L., Giovannella, S., Glagolev, V., Grancagnolo, F., Happacher, F., Hitlin, D., Martini, M., Miscetti, S., Miyashita, T., Murat, P., Pedreschi, E., Pezzullo, G., Porter, F., Raffaelli, F., Ricci, M., Saputi, A., Sarra, I., Spinella, F., Tassielli, G., Tereshchenko, V., and Zhu, R. Y.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

The Mu2e experiment at Fermilab will search for the charged lepton flavor violating process of neutrino-less $\mu \to e$ coherent conversion in the field of an aluminum nucleus. Mu2e will reach a single event sensitivity of about $2.5\cdot 10^{-17}$ that corresponds to four orders of magnitude improvements with respect to the current best limit. The detector system consists of a straw tube tracker and a crystal calorimeter made of undoped CsI coupled with Silicon Photomultipliers. The calorimeter was designed to be operable in a harsh environment where about 10 krad/year will be delivered in the hottest region and work in presence of 1 T magnetic field. The calorimeter role is to perform $\mu$/e separation to suppress cosmic muons mimiking the signal, while providing a high level trigger and a seeding the track search in the tracker. In this paper we present the calorimeter design and the latest R$\&$D results., Comment: 4 pages, conference proceeding for a presentation held at TIPP'2017. To be published on Springer Proceedings in Physics

Published
2018

18. Combination of KLOE $\sigma\big(e^+e^-\rightarrow\pi^+\pi^-\gamma(\gamma)\big)$ measurements and determination of $a_{\mu}^{\pi^+\pi^-}$ in the energy range $0.10 < s < 0.95$ GeV$^2$

Author

Collaboration, The KLOE-2, Anastasi, A., Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkeståhl, L. Caldeira, Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Domenici, D., D'Uffizi, A., Fantini, A., Fantini, G., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kisielewska-Kamińska, D., Kang, X., Kozyrev, E. A., Krzemien, W., Kupsc, A., Loffredo, S., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Passeri, A., Patera, V., del Rio, E. Perez, Raha, N., Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wiślicki, W., Wolke, M., Keshavarzi, A., Müller, S. E., and Teubner, T.

Subjects
High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract

The three precision measurements of the cross section $\sigma\big(e^+e^-\rightarrow\pi^+\pi^-\gamma(\gamma)\big)$ using initial state radiation by the KLOE collaboration provide an important input for the prediction of the hadronic contribution to the anomalous magnetic moment of the muon. These measurements are correlated for both statistical and systematic uncertainties and, therefore, the simultaneous use of these measurements requires covariance matrices that fully describe the correlations. We present the construction of these covariance matrices and use them to determine a combined KLOE measurement for $\sigma\big(e^+e^-\rightarrow\pi^+\pi^-\gamma(\gamma)\big)$. We find, from this combination, a two-pion contribution to the muon magnetic anomaly in the energy range $0.10 < s < 0.95$ GeV$^2$ of $a_{\mu}^{\pi^+\pi^-} = (489.8 \pm 1.7_{\rm stat} \pm 4.8_{\rm sys} ) \times 10^{-10}$., Comment: 20 pages, 8 figures. Version as published in JHEP 1803 (2018) 173

Published
2017

19. Measurement of the KS→ πeν branching fraction with the KLOE experiment

Author

Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D’Agostini, G., D’Amico, R., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Diociaiuti, E., Domenici, D., D’Uffizi, A., Fantini, G., Gajos, A., Gamrat, S., Gauzzi, P., Giovannella, S., Graziani, E., Kang, X., Kupsc, A., Mandaglio, G., Martini, M., Miscetti, S., Moskal, P., Passeri, A., Perez del Rio, E., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Wiślicki, W., and Wolke, M.

Published
2023
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20. The calorimeter of the Mu2e experiment at Fermilab

Author

Atanov, N., Baranov, V., Budagov, J., Cervelli, F., Colao, F., Cordelli, M., Corradi, G., Dané, E., Davydov, Yu. I., Di Falco, S., Diociaiuti, E., Donati, S., Donghia, R., Echenard, B., Flood, K., Giovannella, S., Glagolev, V., Grancagnolo, F., Happacher, F., Hitlin, D. G., Martini, M., Miscetti, S., Miyashita, T., Morescalchi, L., Murat, P., Pezzullo, G., Porter, F., Raffaelli, F., Radicioni, T., Ricci, M., Saputi, A., Sarra, I., Spinella, F., Tassielli, G., Tereshchenko, V., Usubov, Z., and Zhu, R. Y.

Subjects
Physics - Instrumentation and Detectors
Abstract

The Mu2e experiment at Fermilab looks for Charged Lepton Flavor Violation (CLFV) improving by 4 orders of magnitude the current experimental sensitivity for the muon to electron conversion in a muonic atom. A positive signal could not be explained in the framework of the current Standard Model of particle interactions and therefore would be a clear indication of new physics. In 3 years of data taking, Mu2e is expected to observe less than one background event mimicking the electron coming from muon conversion. Achieving such a level of background suppression requires a deep knowledge of the experimental apparatus: a straw tube tracker, measuring the electron momentum and time, a cosmic ray veto system rejecting most of cosmic ray background and a pure CsI crystal calorimeter, that will measure time of flight, energy and impact position of the converted electron. The calorimeter has to operate in a harsh radiation environment, in a 10-4 Torr vacuum and inside a 1 T magnetic field. The results of the first qualification tests of the calorimeter components are reported together with the energy and time performances expected from the simulation and measured in beam tests of a small scale prototype., Comment: 11 pages, 7 figures, proceedings of 14th Topical Seminar on Innovative Particle and Radiation Detectors (IPRD16) 3 - 6 October 2016 Siena, Italy, Journal of Instrumentation, Volume 12, January 2017 http://stacks.iop.org/1748-0221/12/i=01/a=C01061

Published
2017
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21. Measurement of the running of the fine structure constant below 1 GeV with the KLOE Detector

Author

Collaboration, The KLOE-2, Anastasi, A., Babusci, D., Bencivenni, G., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkeståhl, L. Caldeira, Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., Dané, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., D'Uffizi, A., Fantini, A., Felici, G., Fiore, S., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjöld, L., Johansson, T., Kamińska, D., Krzemien, W., Kupsc, A., Loffredo, S., Lukin, P. A., Mandaglio, G., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Papenbrock, M., Passeri, A., Patera, V., del Rio, E. Perez, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Tortora, L., Venanzoni, G., Wiślicki, W., Wolke, M., and Jegerlehner, F.

Subjects
High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract

We have measured the running of the effective QED coupling constant $\alpha(s)$ in the time-like region $0.6<\sqrt s< 0.975$ GeV with the KLOE detector at DA$\Phi$NE using the Initial State Radiation process $e^+e^-\to\mu^+ \mu^-\gamma$. It represents the first measurement of the running of $\alpha(s)$ in this energy region. Our results show a more than 5$\sigma$ significance of the hadronic contribution to the running of $\alpha(s)$, which is the strongest direct evidence both in time- and space-like regions achieved in a single measurement. By using the $e^+e^-\to\pi^+\pi^-$ cross section measured by KLOE, the real and imaginary part of the shift $\Delta\alpha(s)$ has been extracted. By a fit of the real part of $\Delta\alpha(s)$ and assuming the lepton universality the branching ratio $BR(\omega\to\mu^+\mu^-) = (6.6\pm1.4_{stat}\pm1.7_{syst})\cdot 10^{-5} $ has been determined., Comment: 19 pages, 8 figures, version accepted for publication in Phys. Lett. B

Published
2016
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22. Design and status of the Mu2e electromagnetic calorimeter

Author

Atanov, N., Baranov, V., Budagov, J., Carosi, R., Cervelli, F., Colao, F., Cordelli, M., Corradi, G., Dane', E., Davydov, Yu. I., Di Falco, S., Donati, S., Donghia, R., Echenard, B., Flood, K., Giovannella, S., Glagolev, V., Grancagnolo, F., Happacher, F., Hitlin, D. G., Martini, M., Miscetti, S., Miyashita, T., Morescalchi, L., Murat, P., Pasciuto, D., Pezzullo, G., Porter, F., Saputi, A., Sarra, I., Soleti, S. R., Spinella, F., Tassielli, G., Tereshchenko, V., Usubov, Z., and Zhu, R. Y.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

The Mu2e experiment at Fermilab aims at measuring the neutrinoless conversion of a negative muon into an electron and reach a single event sensitivity of 2.5x10^{-17} after three years of data taking. The monoenergetic electron produced in the final state, is detected by a high precision tracker and a crystal calorimeter, all embedded in a large superconducting solenoid (SD) surrounded by a cosmic ray veto system. The calorimeter is complementary to the tracker, allowing an independent trigger and powerful particle identification, while seeding the track reconstruction and contributing to remove background tracks mimicking the signal. In order to match these requirements, the calorimeter should have an energy resolution of O(5)% and a time resolution better than 500 ps at 100 MeV. The baseline solution is a calorimeter composed of two disks of BaF2 crystals read by UV extended, solar blind, Avalanche Photodiode (APDs), which are under development from a JPL, Caltech, RMD consortium. In this paper, the calorimeter design, the R&D studies carried out so far and the status of engineering are described. A backup alternative setup consisting of a pure CsI crystal matrix read by UV extended Hamamatsu MPPC's is also presented., Comment: 5 pages, 6 figures

Published
2016
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23. Design, status and test of the Mu2e crystal calorimeter

Author

Atanov, N., Baranov, V., Budagov, J., Carosi, R., Cervelli, F., Colao, F., Cordelli, M., Corradi, G., Danè, E., Davydov, Y. I., Di Falco, S., Donati, S., Donghia, R., Echenard, B., Flood, K., Giovannella, S., Glagolev, V., Grancagnolo, F., Happacher, F., Hitlin, D. G., Martini, M., Miscetti, S., Miyashita, T., Morescalchi, L., Murat, P., Piacentino, G. M., Pezzullo, G., Porter, F. C., Raffaelli, F., Saputi, A., Sarra, I., Spinella, F., Tassielli, G., Tereshchenko, V., Usubov, Z., and Zhu, R. Y.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

The Mu2e experiment at Fermilab searches for the charged-lepton flavor violating neutrino-less conversion of a negative muon into an electron in the field of a aluminum nucleus. The dynamic of such a process is well modeled by a two-body decay, resulting in a monoenergetic electron with an energy slightly below the muon rest mass (104.967 MeV). The calorimeter of this experiment plays an important role to provide excellent particle identification capabilities and an online trigger filter while aiding the track reconstruction capabilities. The baseline calorimeter configuration consists of two disks each made with about 700 undoped CsI crystals read out by two large area UV-extended Silicon Photomultipliers. These crystals match the requirements for stability of response, high resolution and radiation hardness. In this paper we present the final calorimeter design.

Published
2016
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24. Energy and time resolution for a LYSO matrix prototype of the Mu2e experiment

Author

Atanov, N., Baranov, V., Colao, F., Cordelli, M., Corradi, G., Dane`, E., Davydov, Y. I., Flood, K., Giovannella, S., Glagolev, V., Happacher, F., Hitlin, D. G., Martini, M., Miscetti, S., Miyashita, T., Morescalchi, L., Ott, P., Pezzullo, G., Saputi, A., Sarra, I., Soleti, S. R., Tassielli, G., Tereshchenko, V., and Thomas, A.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

We have measured the performances of a LYSO crystal matrix prototype tested with electron and photon beams in the energy range 60$-$450 MeV. This study has been carried out to determine the achievable energy and time resolutions for the calorimeter of the Mu2e experiment., Comment: 2 pages, 3 figures, 13th Pisa Meeting on Advanced Detectors

Published
2016
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25. Limit on the production of a new vector boson in $\mathrm{e^+ e^-}\rightarrow {\rm U}\gamma$, U$\rightarrow \pi^+\pi^-$ with the KLOE experiment

Author

Collaboration, KLOE-2, Anastasi, A., Babusci, D., Bencivenni, G., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkeståhl, L. Caldeira, Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwinski, E., D'Agostini, G., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., D'Uffizi, A., Fantini, A., Felici, G., Fiore, S., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjöld, L., Andersson, W. Ikegami, Johansson, T., Kamińska, D., Krzemien, W., Kupsc, A., Loffredo, S., Mandaglio, G., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Palladino, A., Papenbrock, M., Passeri, A., Patera, V., del Rio, E. Perez, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Silarski, M., Sirghi, F., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

The recent interest in a light gauge boson in the framework of an extra U(1) symmetry motivates searches in the mass range below 1 GeV. We present a search for such a particle, the dark photon, in ${\rm e^+ e^-}\rightarrow {\rm U}\gamma$, U$\rightarrow \pi^+\pi^-$ based on 28 million $\mathrm{e^+ e^-} \rightarrow \pi^+ \pi^-\gamma$ events collected at DA$\Phi$NE by the KLOE experiment. The $\pi^+ \pi^-$ production by initial-state radiation compensates for a loss of sensitivity of previous KLOE ${\rm U} \rightarrow \mathrm{e^+ e^-}$, $\mu^+\mu^-$ searches due to the small branching ratios in the $\rho-\omega$ resonance region. We found no evidence for a signal and set a limit at 90\% CL on the mixing strength between the photon and the dark photon, $\varepsilon^2$, in the U mass range between $527$ and $987$~MeV. Above 700 MeV this new limit is more stringent than previous ones., Comment: 6 pages, 9 figures, 1 table, submitted to Phys. Lett. B

Published
2016
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27. Measurement of the front-end dead-time of the LHCb muon detector and evaluation of its contribution to the muon detection inefficiency

Author

Anderlini, L., Anelli, M., Archilli, F., Auriemma, G., Baldini, W., Bencivenni, G., Bizzeti, A., Bocci, V., Bondar, N., Bonivento, W., Bochin, B., Bozzi, C., Brundu, D., Cadeddu, S., Campana, P., Carboni, G., Cardini, A., Carletti, M., Casu, L., Chubykin, A., Ciambrone, P., Dané, E., De Simone, P., Falabella, A., Felici, G., Fiore, M., Fontana, M., Fresch, P., Furfaro, E., Graziani, G., Kashchuk, A., Kotriakhova, S., Lai, A., Lanfranchi, G., Loi, A., Maev, O., Manca, G., Martellotti, G., Neustroev, P., Oldeman, R. G. C., Palutan, M., Passaleva, G., Penso, G., Pinci, D., Polycarpo, E., Saitta, B., Santacesaria, R., Santimaria, M., Santovetti, E., Saputi, A., Sarti, A., Satriano, C., Satta, A., Schmidt, B., Schneider, T., Sciascia, B., Sciubba, A., Siddi, B. G., Tellarini, G., Vacca, C., Vazquez-Gomez, R., Vecchi, S., Veltri, M., and Vorobyev, A.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

A method is described which allows to deduce the dead-time of the front-end electronics of the LHCb muon detector from a series of measurements performed at different luminosities at a bunch-crossing rate of 20 MHz. The measured values of the dead-time range from 70 ns to 100 ns. These results allow to estimate the performance of the muon detector at the future bunch-crossing rate of 40 MHz and at higher luminosity.

Published
2016
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28. Precision measurement of the $\eta\to\pi^+\pi^-\pi^0$ Dalitz plot distribution with the KLOE detector

Author

Collaboration, KLOE-2, Anastasi, A., Babusci, D., Bencivenni, G., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkeståhl, L. Caldeira, Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., Dané, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., D'Uffizi, A., Fantini, A., Felici, G., Fiore, S., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjöld, L., Andersson, W. Ikegami, Johansson, T., Kamińska, D., Krzemien, W., Kupsc, A., Loffredo, S., Mandaglio, G., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Papenbrock, M., Passeri, A., Patera, V., del Rio, E. Perez, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Silarski, M., Sirghi, F., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment, Nuclear Experiment
Abstract

Using $1.6$ fb$^{-1}$ of $e^+ e^-\to\phi\to\eta\gamma$ data collected with the KLOE detector at DA$\Phi$NE, the Dalitz plot distribution for the $\eta \to \pi^+ \pi^- \pi^0$ decay is studied with the world's largest sample of $\sim 4.7 \cdot 10^6$ events. The Dalitz plot density is parametrized as a polynomial expansion up to cubic terms in the normalized dimensionless variables $X$ and $Y$. The experiment is sensitive to all charge conjugation conserving terms of the expansion, including a $gX^2Y$ term. The statistical uncertainty of all parameters is improved by a factor two with respect to earlier measurements., Comment: 11 pages, 9 figures, supplement: an ascii table

Published
2016

29. Measurement of the $\phi \to \pi^0 e^+e^-$ transition form factor with the KLOE detector

Author

Collaboration, KLOE-2, Anastasi, A., Babusci, D., Bencivenni, G., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkeståhl, L. Caldeira, Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., D'Uffizi, A., Fantini, A., Felici, G., Fiore, S., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjöld, L., Andersson, W. Ikegami, Johansson, T., Kamińska, D., Krzemien, W., Kupsc, A., Loffredo, S., Mandaglio, G., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Papenbrock, M., Passeri, A., Patera, V., del Rio, E. Perez, Ranieri, A., Santangelo, P. Salabura P., Sarra, I., Schioppa, M., Silarski, M., Sirghi, F., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract

A measurement of the vector to pseudoscalar conversion decay $\phi \to \pi^0 e^+e^-$ with the KLOE experiment is presented. A sample of $\sim 9500$ signal events was selected from a data set of 1.7 fb$^{-1}$ of $e^+e^-$ collisions at $\sqrt{s} \sim m_{\phi}$ collected at the DA$\Phi$NE $e^+e^-$ collider. These events were used to obtain the first measurement of the transition form factor $| F_{\phi \pi^0}(q^2) |$ and a new measurement of the branching ratio of the decay: $\rm{BR}\,(\phi \to \pi^0 e^+e^-) = (\,1.35 \pm 0.05^{\,\,+0.05}_{\,\,-0.10}\,) \times 10 ^{-5}$. The result improves significantly on previous measurements and is in agreement with theoretical predictions., Comment: 13 pages, 4 figures; matches published version

Published
2016
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30. Measurement of time resolution of the Mu2e LYSO calorimeter prototype

Author

Atanov, N., Baranov, V., Colao, F., Cordelli, M., Corradi, G., Dané, E., Davydov, Yu. I., Flood, K., Giovannella, S., Glagolev, V., Happacher, F., Hitlin, D. G., Martini, M., Miscetti, S., Miyashita, T., Morescalchi, L., Pezzullo, G., Saputi, A., Sarra, I., Soleti, S. R., Tassielli, G., and Tereshchenko, V.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

In this paper we present the time resolution measurements of the Lutetium-Yttrium Oxyorthosilicate (LYSO) calorimeter prototype for the Mu2e experiment. The measurements have been performed using the $e^-$ beam of the Beam Test Facility (BTF) in Frascati, Italy in the energy range from 100 to 400 MeV. The calorimeter prototype consisted of twenty five 30x30x130 mm$^3$, LYSO crystals read out by 10x10 mm$^2$ Hamamatsu Avalanche Photodiodes (APDs). The energy dependence of the measured time resolution can be parametrized as $\sigma_{t}(E)=a/\sqrt{E/\mathrm{GeV}} \oplus b$, with the stochastic and constant terms $a=(51\pm1)$ ps and $b=(10\pm4)$ ps, respectively. This corresponds to the time resolution of ($162\pm4$) ps at 100 MeV., Comment: 18 pages, 14 figures, accepted for the journal Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment

Published
2015
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31. Limit on the production of a low-mass vector boson in $\mathrm{e}^{+}\mathrm{e}^{-} \to \mathrm{U}\gamma$, $\mathrm{U} \to \mathrm{e}^{+}\mathrm{e}^{-}$ with the KLOE experiment

Author

Anastasi, A., Babusci, D., Bencivenni, G., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkeståhl, L. Caldeira, Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D'Agostini, G., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., D'Uffizi, A., Fantini, A., Felici, G., Fiore, S., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjöld, L., Andersson, W. Ikegami, Johansson, T., Kamińska, D., Krzemien, W., Kupsc, A., Loffredo, S., Mandaglio, G., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Palladino, A., Papenbrock, M., Passeri, A., Patera, V., del Rio, E. Perez, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Silarski, M., Sirghi, F., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

The existence of a new force beyond the Standard Model is compelling because it could explain several striking astrophysical observations which fail standard interpretations. We searched for the light vector mediator of this dark force, the $\mathrm{U}$ boson, with the KLOE detector at the DA$\Phi$NE $\mathrm{e}^{+}\mathrm{e}^{-}$ collider. Using an integrated luminosity of 1.54 fb$^{-1}$, we studied the process $\mathrm{e}^{+}\mathrm{e}^{-} \to \mathrm{U}\gamma$, with $\mathrm{U} \to \mathrm{e}^{+}\mathrm{e}^{-}$, using radiative-return to search for a resonant peak in the dielectron invariant-mass distribution. We did not find evidence for a signal, and set a 90\%~CL upper limit on the mixing strength between the Standard Model photon and the dark photon, $\varepsilon^2$, at $10^{-6}$--$10^{-4}$ in the 5--520~MeV/c$^2$ mass range.

Published
2015
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32. Search for dark Higgsstrahlung in e+ e- -> mu+ mu- and missing energy events with the KLOE experiment

Author

Collaboration, KLOE-2, Babusci, D., Bencivenni, G., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkestahl, L. Caldeira, Ceradini, F., Ciambrone, P., Curciarello, F., Czerwinski, E., Dane', E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., Fantini, A., Felici, G., Fiore, S., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjold, L., Andersson, W. Ikegami, Johansson, T., Kaminska, D., Krzemien, W., Kupsc, A., Loffredo, S., Mandaglio, G., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Palladino, A., Passeri, A., Patera, V., Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Silarski, M., Tortora, L., Venanzoni, G., Wislicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

We searched for evidence of a Higgsstrahlung process in a secluded sector, leading to a final state with a dark photon U and a dark Higgs boson h', with the KLOE detector at DAFNE. We investigated the case of h' lighter than U, with U decaying into a muon pair and h' producing a missing energy signature. We found no evidence of the process and set upper limits to its parameters in the range 2m_mu

Published
2015
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33. Mu2e Technical Design Report

Author

Bartoszek, L., Barnes, E., Miller, J. P., Mott, J., Palladino, A., Quirk, J., Roberts, B. L., Crnkovic, J., Polychronakos, V., Tishchenko, V., Yamin, P., Cheng, C. -h., Echenard, B., Flood, K., Hitlin, D. G., Kim, J. H., Miyashita, T. S., Porter, F. C., Röhrken, M., Trevor, J., Zhu, R. -Y., Heckmaier, E., Kang, T. I., Lim, G., Molzon, W., You, Z., Artikov, A. M., Budagov, J. A., Davydov, Yu. I., Glagolev, V. V., Simonenko, A. V., Usubov, Z. U., Oh, S. H., Wang, C., Ambrosio, G., Andreev, N., Arnold, D., Ball, M., Bernstein, R. H., Bianchi, A., Biery, K., Bossert, R., Bowden, M., Brandt, J., Brown, G., Brown, H., Buehler, M., Campbell, M., Cheban, S., Chen, M., Coghill, J., Coleman, R., Crowley, C., Deshpande, A., Deuerling, G., Dey, J., Dhanaraj, N., Dinnon, M., Dixon, S., Drendel, B., Eddy, N., Evans, R., Evbota, D., Fagan, J., Feher, S., Fellenz, B., Friedsam, H., Gallo, G., Gaponenko, A., Gardner, M., Gaugel, S., Genser, K., Ginther, G., Glass, H., Glenzinski, D., Hahn, D., Hansen, S., Hartsell, B., Hays, S., Hocker, J. A., Huedem, E., Huffman, D., Ibrahim, A., Johnstone, C., Kashikhin, V., Kashikhin, V. V., Kasper, P., Kiper, T., Knapp, D., Knoepfel, K., Kokoska, L., Kozlovsky, M., Krafczyk, G., Kramp, M., Krave, S., Krempetz, K., Kutschke, R. K., Kwarciany, R., Lackowski, T., Lamm, M. J., Larwill, M., Leavell, F., Leeb, D., Leveling, A., Lincoln, D., Logashenko, V., Lombardo, V., Lopes, M. L., Makulski, A., Martinez, A., McArthur, D., McConologue, F., Michelotti, L., Mokhov, N., Morgan, J., Mukherjee, A., Murat, P., Nagaslaev, V., Neuffer, D. V., Nicol, T., Niehoff, J., Nogiec, J., Olson, M., Orris, D., Ostojic, R., Page, T., Park, C., Peterson, T., Pilipenko, R., Pla-Dalmau, A., Poloubotko, V., Popovic, M., Prebys, E., Prieto, P., Pronskikh, V., Pushka, D., Rabehl, R., Ray, R. E., Rechenmacher, R., Rivera, R., Robotham, W., Rubinov, P., Rusu, V. L., Scarpine, V., Schappert, W., Schoo, D., Stefanik, A., Still, D., Tang, Z., Tanovic, N., Tartaglia, M., Tassotto, G., Tinsley, D., Tschirhart, R. S., Vogel, G., Wagner, R., Wands, R., Wang, M., Werkema, S., White Jr., H. B., Whitmore, J., Wielgos, R., Woods, R., Worel, C., Zifko, R., Ciambrone, P., Colao, F., Cordelli, M., Corradi, G., Dane, E., Giovannella, S., Happacher, F., Luca, A., Miscetti, S., Ponzio, B., Pileggi, G., Saputi, A., Sarra, I., Soleti, R. S., Stomaci, V., Martini, M., Fabbricatore, P., Farinon, S., Musenich, R., Alexander, D., Daniel, A., Empl, A., Hungerford, E. V., Lau, K., Gollin, G. D., Huang, C., Roderick, D., Trundy, B., Brown, D. Na., Ding, D., Kolomensky, Yu. G., Lee, M. J., Cascella, M., Grancagnolo, F., Ignatov, F., Innocente, A., L'Erario, A., Miccoli, A., Maffezzoli, A., Mazzotta, P., Onorato, G., Piacentino, G. M., Rella, S., Rossetti, F., Spedicato, M., Tassielli, G., Taurino, A., Zavarise, G., Hooper, R., Brown, D. No., Djilkibaev, R., Matushko, V., Ankenbrandt, C., Boi, S., Dychkant, A., Hedin, D., Hodge, Z., Khalatian, V., Majewski, R., Martin, L., Okafor, U., Pohlman, N., Riddel, R. S., Shellito, A., de Gouvea, A. L., Cervelli, F., Carosi, R., Di Falco, S., Donati, S., Lomtadze, T., Pezzullo, G., Ristori, L., Spinella, F., Jones, M., Corcoran, M. D., Orduna, J., Rivera, D., Bennett, R., Caretta, O., Davenne, T., Densham, C., Loveridge, P., Odell, J., Bomgardner, R., Dukes, E. C., Ehrlich, R., Frank, M., Goadhouse, S., Group, R., Ho, E., Ma, H., Oksuzian, Y., Purvis, J., Wu, Y., Hertzog, D. W., Kammel, P., Lynch, K. R., and Popp, J. L.

Subjects
Physics - Instrumentation and Detectors, High Energy Physics - Experiment
Abstract

The Mu2e experiment at Fermilab will search for charged lepton flavor violation via the coherent conversion process mu- N --> e- N with a sensitivity approximately four orders of magnitude better than the current world's best limits for this process. The experiment's sensitivity offers discovery potential over a wide array of new physics models and probes mass scales well beyond the reach of the LHC. We describe herein the preliminary design of the proposed Mu2e experiment. This document was created in partial fulfillment of the requirements necessary to obtain DOE CD-2 approval., Comment: compressed file, 888 pages, 621 figures, 126 tables; full resolution available at http://mu2e.fnal.gov; corrected typo in background summary, Table 3.4

Published
2015

34. Study of Dalitz decay phi -> eta e+e- with KLOE detector

Author

Babusci, D., Balwierz-Pytko, I., Bencivenni, G., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkestahl, L. Caldeira, Ceradini, F., Ciambrone, P., Curciarello, F., Czerwinski, E., Dane', E., De Leo, V., De Lucia, E., De Robertis, G., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., Erriquez, O., Fanizzi, G., Fantini, A., Felici, G., Fiore, S., Franzini, P., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjold, L., Hoistad, B., Johansson, T., Kaminska, D., Krzemien, W., Kupsc, A., Lee-Franzini, J., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Palladino, A., Passeri, A., Longhi, V. Patera. Prado, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Silarski, M., Tortora, L., Venanzoni, G., Wislicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

We have studied the vector to pseudoscalar conversion decay phi -> eta e+e-, with eta -> pi0pi0pi0, with the KLOE detector at DAPHNE. The data set of 1.7 fb-1 of e+e- collisions at sqrt(s)~Mphi contains a clear conversion decay signal of ~31,000 events from which we measured a value of BR(phi -> eta e+e-)=(1.075+-0.007+-0.038)x10-4. The same sample is used to determine the transition form factor by a fit to the e+e- invariant mass spectrum, obtaining b(phi eta) =(1.17 +- 0.10 + 0.07) GeV-2, that improves by a factor of five the precision of the previous measurement and is in good agreement with VMD expectations., Comment: 13 pages, 6 figures, submitted to PLB

Published
2014
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35. Search for light vector boson production in $e^+e^- \rightarrow \mu^+ \mu^- \gamma$ interactions with the KLOE experiment

Author

Babusci, D., Balwierz-Pytko, I., Bencivenni, G., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkeståhl, L. Caldeira, Ceradini, F., Ciambrone, P., Curciarello, F., Czerwinski, E., Danè, E., De Leo, V., De Lucia, E., De Robertis, G., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Salvo, R., Domenici, D., Erriquez, O., Fanizzi, G., Fantini, A., Felici, G., Fiore, S., Franzini, P., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjold, L., Hoistad, B., Johansson, T., Kacprzak, K., Kaminska, D., Krzemien, W., Kupsc, A., Lee-Franzini, J., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Palladino, A., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Silarski, M., Tortora, L., Venanzoni, G., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

We have searched for a light vector boson $U$, the possible carrier of a "dark force", with the KLOE detector at the DA$\Phi$NE \epm\ collider, motivated by astrophysical evidence for the presence of dark matter in the universe. Using \epm\ collisions collected with an integrated luminosity of $239.3$~pb$^{-1}$, we look for a dimuon mass peak in the reaction \epm\to$\mu^+ \mu^-$\gam, corresponding to the decay $U\to\mu^+\mu^-$. We find no evidence for a $U$ vector boson signal. We set a 90\% CL upper limit for the mixing parameter squared between the photon and the $U$ boson of 1.6$\times$10$^{-5}$ to 8.6$\times$10$^{-7}$ for the mass region $520

Published
2014
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36. Erratum to: Precision tests of quantum mechanics and CPT symmetry with entangled neutral kaons at KLOE

Author

Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D’Agostini, G., D’Amico, R., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Diociaiuti, E., Domenici, D., D’Uffizi, A., Fantini, A., Fantini, G., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kang, X., Kisielewska-Kamińska, D., Kozyrev, E. A., Krzemien, W., Kupsc, A., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Moricciani, D., Moskal, P., Passeri, A., Patera, V., Perez del Rio, E., Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Published
2022
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37. Precision tests of quantum mechanics and CPT symmetry with entangled neutral kaons at KLOE

Author

Babusci, D., Berlowski, M., Bloise, C., Bossi, F., Branchini, P., Budano, A., Cao, B., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwiński, E., D’Agostini, G., D’Amico, R., Danè, E., De Leo, V., De Lucia, E., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Diociaiuti, E., Domenici, D., D’Uffizi, A., Fantini, A., Fantini, G., Fermani, P., Fiore, S., Gajos, A., Gauzzi, P., Giovannella, S., Graziani, E., Ivanov, V. L., Johansson, T., Kang, X., Kisielewska-Kamińska, D., Kozyrev, E. A., Krzemien, W., Kupsc, A., Lukin, P. A., Mandaglio, G., Martini, M., Messi, R., Miscetti, S., Moricciani, D., Moskal, P., Passeri, A., Patera, V., Perez del Rio, E., Santangelo, P., Schioppa, M., Selce, A., Silarski, M., Sirghi, F., Solodov, E. P., Tortora, L., Venanzoni, G., Wiślicki, W., and Wolke, M.

Published
2022
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38. Test of CPT and Lorentz symmetry in entangled neutral kaons with the KLOE experiment

Author

Collaboration, KLOE-2, Babusci, D., Balwierz-Pytko, I., Bencivenni, G., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkestahl, L. Caldeira, Capon, G., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwinski, E., Danè, E., De Leo, V., De Lucia, E., De Robertis, G., De Santis, A., De Simone, P., Di Cicco, A., Di Domenico, A., Di Donato, C., Di Salvo, R., Domenici, D., Erriquez, O., Fanizzi, G., Fantini, A., Felici, G., Fiore, S., Franzini, P., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjold, L., Hoistad, B., Jacewicz, M., Johansson, T., Kacprzak, K., Kaminska, D., Kupsc, A., Lee-Franzini, J., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Palladino, A., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Silarski, M., Taccini, C., Tortora, L., Venanzoni, G., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

Neutral kaon pairs produced in phi decays in anti-symmetric entangled state can be exploited to search for violation of CPT symmetry and Lorentz invariance. We present an analysis of the CP-violating process phi->K_S K_L->pi+pi-pi+pi- based on 1.7 fb-1 of data collected by the KLOE experiment at the Frascati phi-factory DAFNE. The data are used to perform a measurement of the CPT-violating parameters Delta_amu for neutral kaons in the contest of the Standard Model Extension framework. The parameters measured in the reference frame of the fixed stars are: Delta_ao = (-6.0 +- 7.7_{stat} +- 3.1_{syst}) x 10^{-18} GeV Delta_ax = ( 0.9 +- 1.5_{stat} +- 0.6_{syst}) x 10^{-18} GeV Delta_ay = (-2.0 +- 1.5_{stat} +- 0.5_{syst}) x 10^{-18} GeV Delta_az = ( 3.1 +- 1.7_{stat} +- 0.5_{syst}) x 10^{-18} GeV These are presently the most precise measurements in the quark sector of the Standard Model Extension., Comment: 16 pages, 6 figures, added few typo corrections

Published
2013
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39. Recent results on hadron physics at KLOE

Author

Babusci, D., Badoni, D., Balwierz-Pytko, I., Bencivenni, G., Bini, C., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkest, L. Caldeira, Capon, G., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwinski, E., Dane, E., De Leo, V., De Lucia, E., De Robertis, G., De Santis, A., Di Domenico, A., Di Donato, C., Di Salvo, R., Domenici, D., Erriquez, O., Fanizzi, G., Fantini, A., Felici, G., Fiore, S., Franzini, P., Gajos, A., Gauzzi, P., Giardina, G., Giovannella, S., Graziani, E., Happacher, F., Heijkenskjold, L., Hoistad, B., Iafolla, L., Jacewicz, M., Johansson, T., Kacprzak, K., Kupsc, A., Lee-Franzini, J., Leverington, B., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Palladino, A., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Redmer, C. F., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Silarski, M., Taccini, C., Tortora, L., Venanzoni, G., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

One of the basic motivations of the KLOE and KLOE-2 collaborations is the test of fundamental symmetries and the search for phenomena beyond the Standard Model via the hadronic and leptonic decays of ground-state mesons and via their production in the fusion of virtual gamma quanta exchanged between colliding electrons and positrons. This contribution includes brief description of results of recent analysis of the KLOE data aimed at (i) the search for the dark matter boson, (ii) determination of the hadronic and light-by-light contributions to the g-2 muon anomaly and (iii) tests of QCD anomalies., Comment: 4 pages, Proceedings of the 48th Rencontres de Moriond "QCD and High Energy Interactions", La Thuile, Italy, March 9-16, 2013

Published
2013

40. A new limit on the CP violating decay KS -> 3pi0 with the KLOE experiment

Author

Babusci, D., Badoni, D., Balwierz-Pytko, I., Bencivenni, G., Bini, C., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkestahl, L. Caldeira, Capon, G., Ceradini, F., Ciambrone, P., Curciarello, F., Czerwinski, E., Dane, E., De Leo, V., De Lucia, E., De Robertis, G., De Santis, 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., Jacewicz, M., Johansson, T., Kacprzak, K., Kupsc, A., Lee-Franzini, J., Leverington, B., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Redmer, C. F., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Silarski, M., Taccini, C., Tortora, L., Venanzoni, G., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

We have carried out a new direct search for the CP violating decay KS -> 3pi0 with 1.7 fb^-1 of e+e- collisions collected by the KLOE detector at the phi-factory DAFNE. We have searched for this decay in a sample of about 5.9 x 10^8 KS KL events tagging the KS by means of the KL interaction in the calorimeter and requiring six prompt photons. With respect to our previous search, the analysis has been improved by increasing of a factor four the tagged sample and by a more effective background rejection of fake KS tags and spurious clusters. We find no candidates in data and simulated background samples, while we expect 0.12 standard model events. Normalizing to the number of KS -> 2pi0 events in the same sample, we set the upper limit on BR(KS -> 3pi0 < 2.6 x 10^-8 at 90% C.L., five times lower than the previous limit. We also set the upper limit on the eta_000 parameter, |eta_000 | < 0.0088 at 90% C.L., improving by a factor two the latest direct measurement., Comment: Accepted for publication in Physics Letters B (15 pages, 13 figures)

Published
2013
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41. Precision measurement of $\sigma(e^+e^-\rightarrow\pi^+\pi^-\gamma)/\sigma(e^+e^-\rightarrow \mu^+\mu^-\gamma)$ and determination of the $\pi^+\pi^-$ contribution to the muon anomaly with the KLOE detector

Author

KLOE, Collaborations, KLOE-2, Babusci, D., Badoni, D., Balwierz-Pytko, I., Bencivenni, G., Bini, C., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkestahl, L. Caldeira, 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, P., Di Domenico, A., Di Donato, C., Domenici, D., Erriquez, O., Fanizzi, G., 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., 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., Longhi, I. Prado, 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., and Zdebik, J.

Subjects
High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract

We have measured the ratio $\sigma(e^+e^-\rightarrow\pi^+\pi^-\gamma)/\sigma(e^+e^-\rightarrow \mu^+\mu^-\gamma)$, with the KLOE detector at DA$\Phi$NE for a total integrated luminosity of $\sim$ 240 pb$^{-1}$. From this ratio we obtain the cross section $\sigma(e^+e^-\rightarrow\pi^+\pi^-)$. From the cross section we determine the pion form factor $|F_\pi|^2$ and the two-pion contribution to the muon anomaly $a_\mu$ for $0.592

Published
2012
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42. Measurement of {\eta} meson production in {\gamma}{\gamma} interactions and {\Gamma}({\eta}-->{\gamma}{\gamma}) with the KLOE detector

Author

Collaboration, KLOE-2, Babusci, D., Badoni, D., Balwierz-Pytko, I., Bencivenni, G., Bini, C., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkestaahl, L. Caldeira, Capon, G., Ceradini, F., Ciambrone, P., Czerwinski, E., Dane, E., De Lucia, E., De Robertis, G., De Santis, 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., Heijkenskj, L., Hoistad, B., Iafolla, L., Jacewicz, M., Johansson, T., Kupsc, A., Lee-Franzini, J., Leverington, B., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Redmer, C. F., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Silarski, M., Taccini, C., Tortora, L., Venanzoni, G., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

We present a measurement of {\eta} meson production in photon-photon interactions produced by electron-positron beams colliding with \sqrt{s}=1 GeV. The measurement is done with the KLOE detector at the \phi-factory DA{\Phi}NE with an integrated luminosity of 0.24 fb^{-1}. The e^+e^- --> e^+e^-{\eta} cross section is measured without detecting the outgoing electron and positron, selecting the decays {\eta}-->{\pi}^+{\pi}^-{\pi}^0 and {\eta}-->{\pi}^0{\pi}^0{\pi}^0. The most relevant background is due to e^+e^- --> {\eta}{\gamma} when the monochromatic photon escapes detection. The cross section for this process is measured as {\sigma}(e^+e^- -->{\eta}{\gamma}) = (856 \pm 8_{stat} \pm 16_{syst}) pb. The combined result for the e^+e^- -->e^+e^-{\eta} cross section is {\sigma}(e^+e^- -->e^+e^-{\eta}) = (32.72 \pm 1.27_{stat} \pm 0.70_{syst}) pb. From this we derive the partial width {\Gamma}({\eta}-->{\gamma}{\gamma}) = (520 \pm 20_{stat} \pm 13_{syst}) eV. This is in agreement with the world average and is the most precise measurement to date., Comment: Version accepted by JHEP

Published
2012
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43. Limit on the production of a light vector gauge boson in phi meson decays with the KLOE detector

Author

Collaboration, KLOE-2, Babusci, D., Badoni, D., Balwierz-Pytko, I., Bencivenni, G., Bini, C., Bloise, C., Bossi, F., Branchini, P., Budano, A., Balkestaahl, L. Caldeira, Capon, G., Ceradini, F., Ciambrone, P., Czerwinski, E., Dane, E., De Lucia, E., De Robertis, G., De Santis, 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., Heijkenskj, L., Hoistad, B., Iafolla, L., Jacewicz, M., Johansson, T., Kupsc, A., Lee-Franzini, J., Leverington, B., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Redmer, C. F., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Silarski, M., Taccini, C., Tortora, L., Venanzoni, G., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

We present a new limit on the production of a light dark-force mediator with the KLOE detector at DAPHNE. This boson, called U, has been searched for in the decay phi --> eta U, U --> e+ e-, analyzing the decay eta --> pi0 pi0 pi0 in a data sample of 1.7 fb-1. No structures are observed in the e+e- invariant mass distribution over the background. This search is combined with a previous result obtained from the decay eta --> pi+ pi- pi0, increasing the sensitivity. We set an upper limit at 90% C.L. on the ratio between the U boson coupling constant and the fine structure constant of alpha'/alpha < 1.7x10^-5 for 30

Published
2012
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44. Measurement of \Gamma(\eta -> \pi^+\pi^-\gamma)/\Gamma(\eta -> \pi^+\pi^-\pi^0) with the KLOE Detector

Author

Babusci, D., Badoni, D., Balwierz-Pytko, I., Bencivenni, G., Bini, C., Bloise, C., Bocci, V., Bossi, F., Branchini, P., Budano, A., Balkest, L. Caldeira, Capon, G., Ceradini, F., Ciambrone, P., Czerwinski, E., Dane, E., De Lucia, E., De Robertis, G., De Santis, A., De Simone, P., Di Domenico, A., Di Donato, C., Di Micco, B., 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., Hoistad, B., Iafolla, L., Jacewicz, M., Johansson, T., Kupsc, A., Lee-Franzini, J., Leverington, B., Loddo, F., Loffredo, S., Mandaglio, G., Martemianov, M., Martini, M., Mascolo, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Passeri, A., Patera, V., Longhi, I. Prado, 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., Xu, G., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

The ratio R_{\eta}=\Gamma(\eta -> \pi^+\pi^-\gamma)/\Gamma(\eta -> \pi^+\pi^-\pi^0) has been measured by analyzing 22 million \phi \to \eta \gamma decays collected by the KLOE experiment at DA\PhiNE, corresponding to an integrated luminosity of 558 pb^{-1}. The \eta \to \pi^+\pi^-\gamma proceeds both via the \rho resonant contribution, and possibly a non-resonant direct term, connected to the box anomaly. Our result, R_{\eta}= 0.1856\pm 0.0005_{stat} \pm 0.0028_{syst}, points out a sizable contribution of the direct term to the total width. The di-pion invariant mass for the \eta -> \pi^+\pi^-\gamma decay could be described in a model-independent approach in terms of a single free parameter, \alpha. The determined value of the parameter \alpha is \alpha = (1.32 \pm 0.08_{stat} +0.10/-0.09_{syst}\pm 0.02_{theo}) GeV^{-2}, Comment: Paper in press, accepted by PLB

Published
2012
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45. Measurement of $\Gamma(\eta \to \pi^+\pi^-\gamma)/\Gamma(\eta \to \pi^+\pi^-\pi^0)$ with KLOE experiment

Author

The KLOE Collaboration, Ambrosino, F., Antonelli, A., Antonelli, M., Archilli, F., Balwierz, I., Bencivenni, G., Bini, C., Bloise, C., Bocchetta, S., Bossi, F., Branchini, P., Capon, G., Capussela, T., Ceradini, F., Ciambrone, P., Czerwiski, E., De Lucia, E., De Santis, A., De Simone, P., De Zorzi, G., Denig, A., Di Domenico, A., Di Donato, C., Di Micco, B., Dreucci, M., Felici, G., Fiore, S., Franzini, P., Gatti, C., Gauzzi, P., Giovannella, S., Graziani, E., Jacewicz, M., Lee-Franzini, J., Martemianov, M., Martini, M., Massarotti, P., Meola, S., Miscetti, S., Morello, G., Moulson, M., Muller, S., Napolitano, M., Nguyen, F., Palutan, M., Passeri, A., Patera, V., Longhi, I. Prado, Santangelo, P., Sciascia, B., Silarski, M., Spadaro, T., Taccini, C., Tortora, L., Venanzoni, G., Versaci, R., Xu, G., Zdebik, J., collaboration, as members of the KLOE-2, Babusci, D., Badoni, D., Bocci, V., Budano, A., Bulychjev, S. A., Campana, P., Dané, E., De Robertis, G., Domenici, D., Erriquez, O., Fanizzi, G., Gonnella, F., Happacher, F., Höistad, B., Iarocci, E., Johansson, T., Kulikov, V., Kupsc, A., Loddo, F., Matsyuk, M., Messi, R., Moricciani, D., Moskal, P., Ranieri, A., Sarra, I., Schioppa, M., Sciubba, A., Wiślicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

We report the measurement of the ratio $\Gamma(\eta \to \pi^+\pi^-\gamma)/\Gamma(\eta \to \pi^+\pi^-\pi^0)$ analyzing a large sample of $\phi \to \eta \gamma$ decays recorded with the KLOE experiment at the DA$\Phi$NE $e^+ e^-$ collider, corresponding to an integrated luminosity of 558 pb$^{-1}$. The $\eta \to \pi^+\pi^-\gamma$ process is supposed to proceed both via a resonant contribution, mediated by the $\rho$ meson, and a non resonant direct term, connected to the box anomaly. The presence of the direct term affects the partial width value. Our result $R_{\eta}=\Gamma(\eta \to \pi^+ \pi^- \gamma)/\Gamma(\eta \to \pi^+ \pi^- \pi^0)= 0.1838\pm 0.0005_{stat} \pm 0.0030_{syst}$ is in agreement with a recent CLEO measurement, which differs by more 3 $\sigma$ from the average of previous results.

Published
2011

46. $\gamma\gamma$ physics with the KLOE experiment

Author

Collaboration, The KLOE-2, Archilli, F., Babusci, D., Badoni, D., Balwierz, I., Bencivenni, G., Bini, C., Bloise, C., Bocci, V., Bossi, F., Branchini, P., Budano, A., Bulychjev, S. A., Campana, P., Capon, G., Ceradini, F., Ciambrone, P., Czerwinski, E., Dane, E., De Lucia, E., De Robertis, G., De Santis, A., De Zorzi, G., Di Domenico, A., Di Donato, C., Domenici, D., Erriquez, O., Fanizzi, G., Felici, G., Fiore, S., Franzini, P., Gauzzi, P., Giovannella, S., Gonnella, F., Graziani, E., Happacher, F., Hoistad, B., Iarocci, E., Jacewicz, M., Johansson, T., Kulikov, V., Kupsc, A., Lee-Franzini, J., Loddo, F., Martemianov, M., Martini, M., Matsyuk, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Sciubba, A., Silarski, M., Taccini, C., Tortora, L., Venanzoni, G., Versaci, R., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

The processes $e^+e^-\to e^+e^-X$, with $X$ being either the $\eta$ meson or $\pi^0\pi^0$, are studied at DA$\Phi$NE, with $e^+e^-$ beams colliding at $\sqrt{s}\simeq1$ GeV, below the $\phi$ resonance peak. The data sample is from an integrated luminosity of 240 pb$^{-1}$, collected by the KLOE experiment without tagging of the outgoing $e^+e^-$. Preliminary results are presented on the observation of the $\gamma\gamma\to\eta$ process, with both $\eta\to\pi^+\pi^-\pi^0$ and $\eta\to\pi^0\pi^0\pi^0$ channels, and the evidence for $\gamma\gamma\to\pi^0\pi^0$ production at low $\pi^0\pi^0$ invariant mass., Comment: Contributed paper to the Lepton-Photon 2011 Conference

Published
2011

47. U boson searches at KLOE

Author

Archilli, F., Babusci, D., Badoni, D., Balwierz, I., Bencivenni, G., Bini, C., Bloise, C., Bocci, V., Bossi, F., Branchini, P., Budano, A., Bulychjev, S. A., Campana, P., Capon, G., Ceradini, F., Ciambrone, P., Czerwinski, E., Dane', E., De Lucia, E., De Robertis, G., De Santis, A., De Zorzi, G., Di Domenico, A., Di Donato, C., Domenici, D., Erriquez, O., Fanizzi, G., Felici, G., Fiore, S., Franzini, P., Gauzzi, P., Giovannella, S., Gonnella, F., Graziani, E., Happacher, F., Hoistad, B., Iarocci, E., Jacewicz, M., Johansson, T., Kulikov, V., Kupsc, A., Lee-Franzini, J., Loddo, F., Martemianov, M., Martini, M., Matsyuk, M., Messi, R., Miscetti, S., Morello, G., Moricciani, D., Moskal, P., Nguyen, F., Passeri, A., Patera, V., Longhi, I. Prado, Ranieri, A., Santangelo, P., Sarra, I., Schioppa, M., Sciascia, B., Sciubba, A., Silarski, M., Taccini, C., Tortora, L., Venanzoni, G., Versaci, R., Wislicki, W., Wolke, M., and Zdebik, J.

Subjects
High Energy Physics - Experiment
Abstract

The existence of a secluded gauge sector could explain several puzzling astrophysical observations. This hypothesis can be tested at low energy e+e- colliders such as DAPHNE. Preliminary results obtained with KLOE data and perpectives for the KLOE-2 run, where a larger data sample is expected, are discussed., Comment: 8 pages, 5 figures

Published
2011
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48. Observation of the rare eta->e+e-e+e- decay with the KLOE experiment

Author

The KLOE Collaboration, Ambrosino, F., Antonelli, A., Antonelli, M., Archilli, F., Balwierz, I., Bencivenni, G., Bini, C., Bloise, C., Bocchetta, S., Bossi, F., Branchini, P., Capon, G., Capussela, T., Ceradini, F., Ciambrone, P., Czerwinski, E., DeLucia, E., DeSantis, A., DeSimone, P., DeZorzi, G., Denig, A., DiDomenico, A., DiDonato, C., DiMicco, B., Dreucci, M., Felici, G., Fiore, S., Franzini, P., Gatti, C., Gauzzi, P., Giovannella, S., Graziani, E., Jacewicz, M., Lee-Franzini, J., Martemianov, M., Martini, M., Massarotti, P., Meola, S., Miscetti, S., Morello, G., Moulson, M., Muller, S., Napolitano, M., Nguyen, F., Palutan, M., Passeri, A., Patera, V., PradoLonghi, I., Santangelo, P., Sciascia, B., Silarski, M., Spadaro, T., Taccini, C., Tortora, L., Venanzoni, G., Versaci, R., Xu, G., Zdebik, J., collaboration, as members of the KLOE-2, Babusci, D., Badoni, D., Bocci, V., Budano, A., Bulychjev, S. A., Campana, P., Dane, E., DeRobertis, G., Domenici, D., Erriquez, O., Fanizzi, G., Gonnella, F., Happacher, F., Hoistad, B., Iarocci, E., Johansson, T., Kulikov, V., Kupsc, A., Loddo, F., Matsyuk, M., Messi, R., Moricciani, D., Moskal, P., Ranieri, A., Sarra, I., Schioppa, M., Sciubba, A., Wislicki, W., and Wolke, M.

Subjects
High Energy Physics - Experiment
Abstract

We report the first observation of the rare eta->e+e-e+e- decay based on 1.7 fb^{-1} collected by the KLOE experiment at the DAFNE phi-factory. The selection of the e+e-e+e- final state is fully inclusive of radiation. We have identified 362 +- 29 events resulting in a branching ratio of (2.4 +- 0.2_stat+bckg +- 0.1_syst) x 10^{-5}., Comment: 12 pages, 3 figures, to be published on PLB

Published
2011
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49. First observation of Bs -> D_{s2}^{*+} X mu nu decays

Author

LHCb Collaboration, Aaij, R., Adeva, B., Adinolfi, M., Adrover, C., Affolder, A., Agari, M., Ajaltouni, Z., Albrecht, J., Alessio, F., Alexander, M., Cartelle, P. Alvarez, Alves Jr, A. A., Amato, S., Amhis, Y., Amoraal, J., Anderson, J., Nobrega, R. Antunes, Appleby, R. B., Gutierrez, O. Aquines, Arefyev, A., Arrabito, L., Artuso, M., Aslanides, E., Auriemma, G., Bachmann, S., Bailey, D. S., Balagura, V., Baldini, W., Barlow, R. J., Barschel, C., Barsuk, S., Basiladze, S., Bates, A., Bauer, C., Bauer, Th., Bay, A., Bediaga, I., Belous, K., Belyaev, I., Benayoun, M., Bencivenni, G., Bernet, R., Bettler, M. -O., van Beuzekom, M., Bifani, S., Bizzeti, A., Bjørnstad, P. M., Blake, T., Blanc, F., Blanks, C., Blouw, J., Blusk, S., Bobrov, A., Bocci, V., Bochin, B., Bondar, A., Bondar, N., Bonivento, W., Borghi, S., Borgia, A., Bos, E., Bowcock, T. J. V., Bozzi, C., Brambach, T., Brand, J. van den, Bressieux, J., Brisbane, S., Britsch, M., Britton, T., Brook, N. H., Brown, H., Büchler-Germann, A., Bursche, A., Buytaert, J., Cadeddu, S., Carvajal, J. M. Caicedo, Callot, O., Calvi, M., Gomez, M. Calvo, Camboni, A., Cameron, W., Camilleri, L., Campana, P., Carbone, A., Carboni, G., Cardinale, R., Cardini, A., Carson, L., Akiba, K. Carvalho, Casse, G., Cattaneo, M., Charles, M., Charpentier, Ph., Cheng, J., Chiapolini, N., Chlopik, A., Christiansen, J., Ciambrone, P., Vidal, X. Cid, Clark, P. J., Clarke, P. E. L., Clemencic, M., Cliff, H. V., Closier, J., Coca, C., Coco, V., Cogan, J., Collins, P., Constantin, F., Conti, G., Contu, A., Coombes, M., Corti, G., Cowan, G. A., Currie, R., D'Almagne, B., D'Ambrosio, C., D'Antone, I., Da Silva, W., Dane', E., David, P., De Bonis, I., De Capua, S., De Cian, M., De Lorenzi, F., De Miranda, J. M., De Paula, L., De Simone, P., Decamp, D., Degaudenzi, H., Deissenroth, M., Del Buono, L., Deplano, C., Deschamps, O., Dettori, F., Dickens, J., Dijkstra, H., Dima, M., Donleavy, S., Dornan, P., Dossett, D., Dovbnya, A., Dupertuis, F., Dzhelyadin, R., Eames, C., Easo, S., Egede, U., Egorychev, V., Eidelman, S., van Eijk, D., Eisele, F., Eisenhardt, S., Eklund, L., d'Enterria, D. G., Pereira, D. Esperante, Estève, L., Fanchini, E., Färber, C., Fardell, G., Farinelli, C., Farry, S., Fave, V., Albor, V. Fernandez, Ferro-Luzzi, M., Filippov, S., Fitzpatrick, C., Flegel, W., Fontanelli, F., Forty, R., Frank, M., Frei, C., Frosini, M., Pazos, J. L. Fungueirino, Furcas, S., Torreira, A. Gallas, Galli, D., Gandelman, M., Gandini, P., Gao, Y., Garnier, J-C., Garofoli, J., Garrido, L., Gaspar, C., Gassner, J., Gauvin, N., Gavillet, P., Gersabeck, M., Gershon, T., Ghez, Ph., Gibson, V., Gligorov, V. V., Göbel, C., Golubkov, D., Golutvin, A., Gomes, A., Gong, G., Gong, H., Gordon, H., Gándara, M. Grabalosa, Diaz, R. Graciani, Cardoso, L. A. Granado, Graugés, E., Graziani, G., Grecu, A., Gregson, S., Gui, B., Gushchin, E., Guz, Yu., Guzik, Z., Gys, T., Haefeli, G., Haines, S. C., Hampson, T., Hansmann-Menzemer, S., Harji, R., Harnew, N., Harrison, P. F., He, J., Hennessy, K., Henrard, P., Morata, J. A. Hernando, van Herwijnen, E., Hicheur, A., Hicks, E., Hilke, H. J., Hofmann, W., Holubyev, K., Hopchev, P., Hulsbergen, W., Hunt, P., Huse, T., Huston, R. S., Hutchcroft, D., Iakovenko, V., Escudero, C. Iglesias, Ilgner, C., Ilten, P., Imong, J., Jacobsson, R., Hussein, M. Jahjah, Jans, E., Jansen, F., Jaton, P., Jean-Marie, B., Jing, F., John, M., Johnson, D., Jones, C. R., Jost, B., Kapusta, F., Karbach, T. M., Kashchuk, A., Keaveney, J., Kerzel, U., Ketel, T., Keune, A., Khanji, B., Kim, Y. M., Knecht, M., Koblitz, S., Konoplyannikov, A., Koppenburg, P., Korolev, M., Kozlinskiy, A., Kravchuk, L., Krocker, G., Krokovny, P., Kruse, F., Kruzelecki, K., Kucharczyk, M., Kukulak, S., Kumar, R., Kvaratskheliya, T., La Thi, V. N., Lacarrere, D., Lafferty, G., Lai, A., Lambert, R. W., Lanfranchi, G., Langenbruch, C., Latham, T., Gac, R. Le, van Leerdam, J., Lees, J. -P., Lefèvre, R., Leflat, A., Lefrançois, J., Lehner, F., Leroy, O., Lesiak, T., Li, L., Li, Y. Y., Gioi, L. Li, Libby, J., Lieng, M., Liles, M., Lindner, R., Linn, C., Liu, B., Liu, G., Löchner, S., Lopes, J. H., Asamar, E. Lopez, Lopez-March, N., Luisier, J., M'charek, B., Machefert, F., Machikhiliyan, I. V., Maciuc, F., Maev, O., Magnin, J., Maier, A., Malde, S., Mamunur, R. M. D., Manca, G., Mancinelli, G., Mangiafave, N., Marconi, U., Märki, R., Marks, J., Martellotti, G., Martens, A., Martin, L., Sanchez, A. Martin, Santos, D. Martinez, Massafferri, A., Mathe, Z., Matteuzzi, C., Matveev, M., Matveev, V., Maurice, E., Maynard, B., Mazurov, A., McGregor, G., McNulty, R., Mclean, C., Meissner, M., Merk, M., Merkel, J., Merkin, M., Messi, R., Miglioranzi, S., Milanes, D. A., Minard, M. -N., Monteil, S., Moran, D., Morawski, P., Morris, J. V., Moscicki, J., Mountain, R., Mous, I., Muheim, F., Müller, K., Muresan, R., Murtas, F., Muryn, B., Musy, M., Mylroie-Smith, J., Naik, P., Nakada, T., Nandakumar, R., Nardulli, J., Nawrot, A., Nedos, M., Needham, M., Neufeld, N., Neustroev, P., Nicol, M., Nies, S., Niess, V., Nikitin, N., Oblakowska-Mucha, A., Obraztsov, V., Oggero, S., Okhrimenko, O., Oldeman, R., Orlandea, M., Ostankov, A., Pal, B., Palacios, J., Palutan, M., Panman, J., Papanestis, A., Pappagallo, M., Parkes, C., Parkinson, C. J., Passaleva, G., Patel, G. D., Patel, M., Paterson, S. K., Patrick, G. N., Patrignani, C., Pauna, E., Pauna, C., Pavel, C., Alvarez, A. Pazos, Pellegrino, A., Penso, G., Altarelli, M. Pepe, Perazzini, S., Perego, D. L., Trigo, E. Perez, Yzquierdo, A. Pérez-Calero, Perret, P., Pessina, G., Petrella, A., Petrolini, A., Valls, B. Pie, Pietrzyk, B., Pinci, D., Plackett, R., Playfer, S., Casasus, M. Plo, Polok, G., Poluektov, A., Polycarpo, E., Popov, D., Popovici, B., Potterat, C., Powell, A., Pozzi, S., Pree, T. du, Pugatch, V., Navarro, A. Puig, Qian, W., Rademacker, J. H., Rakotomiaramanana, B., Raniuk, I., Raven, G., Redford, S., Reece, W., Reis, A. C. dos, Ricciardi, S., Rinnert, K., Romero, D. A. Roa, Robbe, P., Rodrigues, E., Rodrigues, F., Cobo, C. Rodriguez, Perez, P. Rodriguez, Rogers, G. J., Romanovsky, V., Rouvinet, J., Ruf, T., Ruiz, H., Rusinov, V., Sabatino, G., Silva, J. J. Saborido, Sagidova, N., Sail, P., Saitta, B., Salzmann, C., Varela, A. Sambade, Sannino, M., Santacesaria, R., Santinelli, R., Santovetti, E., Sapunov, M., Saputi, A., Sarti, A., Satriano, C., Satta, A., Savrie, M., Savrina, D., Schaack, P., Schiller, M., Schleich, S., Schmelling, M., Schmidt, B., Schneider, O., Schneider, T., Schopper, A., Schune, M. -H., Schwemmer, R., Sciubba, A., Seco, M., Semennikov, A., Senderowska, K., Serra, N., Serrano, J., Shao, B., Shapkin, M., Shapoval, I., Shatalov, P., Shcheglov, Y., Shears, T., Shekhtman, L., Shevchenko, O., Shevchenko, V., Shires, A., Simioni, E., Skottowe, H. P., Skwarnicki, T., Smale, N., Smith, A., Smith, A. C., Sobczak, K., Soler, F. J. P., Solomin, A., Somogy, P., Soomro, F., De Paula, B. Souza, Spaan, B., Sparkes, A., Spiridenkov, E., Spradlin, P., Srednicki, A., Stagni, F., Steiner, S., Steinkamp, O., Stenyakin, O., Stoica, S., Stone, S., Storaci, B., Straumann, U., Styles, N., Szczekowski, M., Szczypka, P., Szumlak, T, T'Jampens, S., Talanov, V., Tarkovskiy, E., Teodorescu, E., Terrier, H., Teubert, F., Thomas, C., Thomas, E., van Tilburg, J., Tisserand, V., Tobin, M., Topp-Joergensen, S., Tran, M. T., Traynor, S., Trunk, U., Tsaregorodtsev, A., Tuning, N., Ukleja, A., Urquijo, P., Uwer, U., Vagnoni, V., Valenti, G., Gomez, R. Vazquez, Regueiro, P. Vazquez, Vecchi, S., Velthuis, J. J., Veltri, M., Vervink, K., Viaud, B., Videau, I., Vilasis-Cardona, X., Visniakov, J., Vollhardt, A., Voong, D., Vorobyev, A., Vorobyev, An., Voss, H., Wacker, K., Wandernoth, S., Wang, J., Ward, D. R., Webber, A. D., Websdale, D., Whitehead, M., Wiedner, D., Wiggers, L., Wilkinson, G., Williams, M. P., Williams, M., Wilson, F. F., Wishahi, J., Witek, M., Witzeling, W., Wotton, S. A., Wyllie, K., Xie, Y., Xing, F., Yang, Z., Smit, G. Ybeles, Young, R., Yushchenko, O., Zavertyaev, M., Zeng, M., Zhang, L., Zhang, W. C., Zhang, Y., Zhelezov, A., Zhong, L., and Zverev, E.

Subjects
High Energy Physics - Experiment
Abstract

Using data collected with the LHCb detector in proton-proton collisions at a centre-of-mass energy of 7 TeV, the semileptonic decays Bs -> Ds+ X mu nu and Bs -> D0 K+ X mu nu are detected. Two structures are observed in the D0 K+ mass spectrum at masses consistent with the known D^+_{s1}(2536) and $D^{*+}_{s2}(2573) mesons. The measured branching fractions relative to the total Bs semileptonic rate are B(Bs -> D_{s2}^{*+} X mu nu)/B(Bs -> X mu nu)= (3.3\pm 1.0\pm 0.4)%, and B(Bs -> D_{s1}^+ X munu)/B(Bs -> X mu nu)= (5.4\pm 1.2\pm 0.5)%, where the first uncertainty is statistical and the second is systematic. This is the first observation of the D_{s2}^{*+} state in Bs decays; we also measure its mass and width., Comment: 8 pages 2 figures. Published in Physics Letters B

Published
2011
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50. Measurement of sigma(pp -> b anti-b X) at \sqrt(s)=7 TeV in the forward region

Author

LHCb Collaboration, Aaij, R., Beteta, C. Abellan, Adeva, B., Adinolfi, M., Adrover, C., Affolder, A., Agari, M., Ajaltouni, Z., Albrecht, J., Alessio, F., Alexander, M., Alfonsi, M., Cartelle, P. Alvarez, Alves Jr, A. A., Amato, S., Amhis, Y., Amoraal, J., Anderson, J., Nobrega, R. Antunes, Appleby, R., Gutierrez, O. Aquines, Arefyev, A., Arrabito, L., Artuso, M., Aslanides, E., Auriemma, G., Bachmann, S., Bagaturia, Y., Bailey, D. S., Balagura, V., Baldini, W., Barber, G., Barham, C., Barlow, R. J., Barsuk, S., Basiladze, S., Bates, A., Bauer, C., Bauer, Th., Bay, A., Bediaga, I., Bellunato, T., Belous, K., Belyaev, I., Benayoun, M., Bencivenni, G., Bernet, R., Bernhard, R. P., Bettler, M. -O., van Beuzekom, M., Bibby, J. H., Bifani, S., Bizzeti, A., Bjørnstad, P. M., Blake, T., Blanc, F., Blanks, C., Blouw, J., Blusk, S., Bobrov, A., Bocci, V., Bochin, B., Bonaccorsi, E., Bondar, A., Bondar, N., Bonivento, W., Borghi, S., Borgia, A., Bos, E., Bowcock, T. J. V., Bozzi, C., Brambach, T., Brand, J. van den, Brarda, L., Bressieux, J., Brisbane, S., Britsch, M., Brook, N. H., Brown, H., Brusa, S., Büchler-Germann, A., Bursche, A., Buytaert, J., Cadeddu, S., Carvajal, J. M. Caicedo, Callot, O., Calvi, M., Gomez, M. Calvo, Camboni, A., Cameron, W., Camilleri, L., Campana, P., Carbone, A., Carboni, G., Cardinale, R., Cardini, A., Carroll, J., Carson, L., Akiba, K. Carvalho, Casse, G., Cattaneo, M., Chadaj, B., Charles, M., Charpentier, Ph., Cheng, J., Chiapolini, N., Chlopik, A., Christiansen, J., Ciambrone, P., Vidal, X. Cid, Clark, P. J., Clarke, P. E. L., Clemencic, M., Cliff, H. V., Closier, J., Coca, C., Coco, V., Cogan, J., Collins, P., Comerma-Montells, A., Constantin, F., Conti, G., Contu, A., Cooke, P., Coombes, M., Corajod, B., Corti, G., Cowan, G. A., Currie, R., D'Almagne, B., D'Ambrosio, C., D'Antone, I., Da Silva, W., Dane', E., David, P., De Bonis, I., De Capua, S., De Cian, M., De Lorenzi, F., De Miranda, J. M., De Paula, L., De Simone, P., Decamp, D., Decreuse, G., Degaudenzi, H., Deissenroth, M., Del Buono, L., Densham, C. J., Deplano, C., Deschamps, O., Dettori, F., Dickens, J., Dijkstra, H., Dima, M., Donleavy, S., Dornan, P., Dossett, D., Dovbnya, A., Dumps, R., Dupertuis, F., Dwyer, L., Dzhelyadin, R., Eames, C., Easo, S., Egede, U., Egorychev, V., Eidelman, S., van Eijk, D., Eisele, F., Eisenhardt, S., Eklund, L., d'Enterria, D. G., Pereira, D. Esperante, Estève, L., Fanchini, E., Färber, C., Fardell, G., Farinelli, C., Farry, S., Fave, V., Felici, G., Albor, V. Fernandez, Ferro-Luzzi, M., Filippov, S., Fitzpatrick, C., Flegel, W., Fontanelli, F., Forti, C., Forty, R., Fournier, C., Franek, B., Frank, M., Frei, C., Frosini, M., Pazos, J. L. Fungueirino, Furcas, S., Torreira, A. Gallas, Galli, D., Gandelman, M., Gandini, P., Gao, Y., Garnier, J-C., Garrido, L., Gascon, D., Gaspar, C., Cue, A. Gaspar De Valenzuela, Gassner, J., Gauvin, N., Gavillet, P., Gersabeck, M., Gershon, T., Ghez, Ph., Gibson, V., Gligorov, V. V., Göbel, C., Golubkov, D., Golutvin, A., Gomes, A., Gong, G., Gong, H., Gordon, H., Gándara, M. Grabalosa, Gracco, V., Diaz, R. Graciani, Cardoso, L. A. Granado, Graugés, E., Graziani, G., Grecu, A., Gregson, S., Guerrer, G., Gui, B., Gushchin, E., Guz, Yu., Guzik, Z., Gys, T., Haefeli, G., Haines, S. C., Hampson, T., Hansmann-Menzemer, S., Harji, R., Harnew, N., Harrison, P. F., He, J., Hennessy, K., Henrard, P., Morata, J. A. Hernando, van Herwijnen, E., Hicheur, A., Hicks, E., Hilke, H. J., Hofmann, W., Holubyev, K., Hopchev, P., Hulsbergen, W., Hunt, P., Huse, T., Huston, R. S., Hutchcroft, D., Iacoangeli, F., Iakovenko, V., Escudero, C. Iglesias, Ilgner, C., Ilten, P., Imong, J., Jacobsson, R., Hussein, M. Jahjah, Jamet, O., Jans, E., Jansen, F., Jaton, P., Jean-Marie, B., John, M., Johnson, D., Jones, C. R., Jost, B., Kapusta, F., Karbach, T. M., Kashchuk, A., Katvars, S., Keaveney, J., Kerzel, U., Ketel, T., Keune, A., Khalil, S., Khanji, B., Kim, Y. M., Knecht, M., Koblitz, S., Konoplyannikov, A., Koppenburg, P., Korolev, M., Kozlinskiy, A., Kravchuk, L., Kristic, R., Krocker, G., Krokovny, P., Kruse, F., Kruzelecki, K., Kucharczyk, M., Kudryashov, I., Kukulak, S., Kumar, R., Kvaratskheliya, T., La Thi, V. N., Lacarrere, D., Lafferty, G., Lai, A., Lambert, R. W., Lanfranchi, G., Langenbruch, C., Latham, T., Gac, R. Le, Lees, J. -P., Lefèvre, R., Leflat, A., Lefrançois, J., Lehner, F., Lenzi, M., Leroy, O., Lesiak, T., Li, L., Li, Y. Y., Gioi, L. Li, Libby, J., Lieng, M., Lindner, R., Lindsay, S., Linn, C., Liu, B., Liu, G., Löchner, S., Lopes, J. H., Asamar, E. Lopez, Lopez-March, N., Loveridge, P., Luisier, J., M'charek, B., Machefert, F., Machikhiliyan, I. V., Maciuc, F., Maev, O., Magnin, J., Maier, A., Malde, S., Mamunur, R. M. D., Manca, G., Mancinelli, G., Mangiafave, N., Marconi, U., Märki, R., Marks, J., Martellotti, G., Martens, A., Martin, L., Santos, D. Martinez, Massafferri, A., Mathe, Z., Matteuzzi, C., Matveev, V., Maurice, E., Maynard, B., Mazurov, A., McGregor, G., McNulty, R., Mclean, C., Merk, M., Merkel, J., Merkin, M., Messi, R., Miglioranzi, S., Minard, M. -N., Moine, G., Monteil, S., Moran, D., Morant, J., Morawski, P., Morris, J. V., Moscicki, J., Mountain, R., Mous, I., Muheim, F., Müller, K., Muresan, R., Murtas, F., Muryn, B., Musy, M., Mylroie-Smith, J., Naik, P., Nakada, T., Nandakumar, R., Nardulli, J., Nawrot, A., Nedos, M., Needham, M., Neufeld, N., Neustroev, P., Nicol, M., Nicolas, L., Nies, S., Niess, V., Nikitin, N., Noor, A., Oblakowska-Mucha, A., Obraztsov, V., Oggero, S., Okhrimenko, O., Oldeman, R., Orlandea, M., Ostankov, A., Pal, B., Palacios, J., Palutan, M., Panman, J., Papadelis, A., Papanestis, A., Pappagallo, M., Parkes, C., Parkinson, C. J., Passaleva, G., Patel, G. D., Patel, M., Paterson, S. K., Patrick, G. N., Patrignani, C., Pauna, E., Pauna, C., Pavel, C., Alvarez, A. Pazos, Pellegrino, A., Penso, G., Altarelli, M. Pepe, Perazzini, S., Perego, D. L., Trigo, E. Perez, Yzquierdo, A. Pérez-Calero, Perret, P., Pessina, G., Petrella, A., Petrolini, A., Olloqui, E. Picatoste, Valls, B. Pie, Piedigrossi, D., Pietrzyk, B., Pinci, D., Playfer, S., Casasus, M. Plo, Poli-Lener, M., Polok, G., Poluektov, A., Polycarpo, E., Popov, D., Popovici, B., Poss, S., Potterat, C., Powell, A., Pozzi, S., Pree, T. du, Pugatch, V., Navarro, A. Puig, Qian, W., Rademacker, J. H., Rakotomiaramanana, B., Raniuk, I., Raven, G., Redford, S., Reece, W., Reis, A. C. dos, Ricciardi, S., Riera, J., Rinnert, K., Romero, D. A. Roa, Robbe, P., Rodrigues, E., Rodrigues, F., Cobo, C. Rodriguez, Perez, P. Rodriguez, Rogers, G. J., Romanovsky, V., Sanabria, E. Rondan, Rosello, M., Rouvinet, J., Roy, L., Ruf, T., Ruiz, H., Rummel, C., Rusinov, V., Sabatino, G., Silva, J. J. Saborido, Sagidova, N., Sail, P., Saitta, B., Sakhelashvili, T., Salzmann, C., Varela, A. Sambade, Sannino, M., Santacesaria, R., Santinelli, R., Santovetti, E., Sapunov, M., Sarti, A., Satriano, C., Satta, A., Savidge, T., Savrie, M., Savrina, D., Schaack, P., Schiller, M., Schleich, S., Schmelling, M., Schmidt, B., Schneider, O., Schneider, T., Schopper, A., Schune, M. -H., Schwemmer, R., Sciubba, A., Seco, M., Semennikov, A., Senderowska, K., Serra, N., Serrano, J., Shao, B., Shapkin, M., Shapoval, I., Shatalov, P., Shcheglov, Y., Shears, T., Shekhtman, L., Shevchenko, V., Shires, A., Sigurdsson, S., Simioni, E., Skottowe, H. P., Skwarnicki, T., Smale, N., Smith, A., Smith, A. C., Smith, N. A., Sobczak, K., Soler, F. J. P., Solomin, A., Somogy, P., Soomro, F., De Paula, B. Souza, Spaan, B., Sparkes, A., Spiridenkov, E., Spradlin, P., Srednicki, A., Stagni, F., Stahl, S., Steiner, S., Steinkamp, O., Stenyakin, O., Stoica, S., Stone, S., Storaci, B., Straumann, U., Styles, N., Szczekowski, M., Szczypka, P., Szumlak, T., T'Jampens, S., Tarkovskiy, E., Teodorescu, E., Terrier, H., Teubert, F., Thomas, C., Thomas, E., van Tilburg, J., Tisserand, V., Tobin, M., Topp-Joergensen, S., Tran, M. T., Traynor, S., Trunk, U., Tsaregorodtsev, A., Tuning, N., Ukleja, A., Ullaland, O., Urquijo, P., Uwer, U., Vagnoni, V., Valenti, G., Gomez, R. Vazquez, Regueiro, P. Vazquez, Vecchi, S., Velthuis, J. J., Veltri, M., Vervink, K., Viaud, B., Videau, I., Vilasis-Cardona, X., Visniakov, J., Vollhardt, A., Volyanskyy, D., Voong, D., Vorobyev, A., Vorobyev, An., Voss, H., Wacker, K., Wandernoth, S., Wang, J., Ward, D. R., Webber, A. D., Websdale, D., Whitehead, M., Wiedner, D., Wiggers, L., Wilkinson, G., Williams, M. P., Williams, M., Wilson, F. F., Wishahi, J., Witek, M., Witzeling, W., Woodward, M. L., Wotton, S. A., Wyllie, K., Xie, Y., Xing, F., Yang, Z., Smit, G. Ybeles, Young, R., Yushchenko, O., Zeng, M., Zhang, L., Zhang, Y., Zhelezov, A., and Zverev, E.

Subjects
High Energy Physics - Experiment, High Energy Physics - Phenomenology
Abstract

Decays of b hadrons into final states containing a D0 meson and a muon are used to measure the b anti-b production cross-section in proton-proton collisions at a centre-of-mass energy of 7 TeV at the LHC. In the pseudorapidity interval 2 < eta < 6 and integrated over all transverse momenta we find that the average cross-section to produce b-flavoured or anti-b-flavoured hadrons is (75.3 +/- 5.4 +/- 13.0) microbarns., Comment: 11 pages, 5 figures, to be published in Physics Lett. B; v2 minor changes

Published
2010
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