382 results on '"Brinet, M."'
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2. Determination of the light, strange and charm quark masses using twisted mass fermions
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Alexandrou, C., Bacchio, S., Bergner, G., Constantinou, M., Di Carlo, M., Dimopoulos, P., Finkenrath, J., Fiorenza, E., Frezzotti, R., Garofalo, M., Hadjiyiannakou, K., Kostrzewa, B., Koutsou, G., Jansen, K., Lubicz, V., Mangin-Brinet, M., Manigrasso, F., Martinelli, G., Pittler, F., Rossi, G. C., Sanfilippo, F., Simula, S., Tarantino, C., Todaro, A., Urbach, C., and Wenger, U.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology - Abstract
We present results for the light, strange and charm quark masses using $N_f=2+1+1$ twisted mass fermion ensembles at three values of the lattice spacing, including two ensembles simulated with the physical value of the pion mass. The analysis is done both in the meson and baryon sectors. The difference in the mean values found in the two sectors is included as part of the systematic error. The presentation is based on the work of Ref. [1], where more details can be found., Comment: Talk presented at the 38th International Symposium on Lattice Field Theory, Lattice 2021, Zoom/Gather@Massachusetts Institute of Technology, 26-30 Jul. 2021; 8 pages, 5 figures
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- 2021
3. Quark masses using twisted mass fermion gauge ensembles
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Alexandrou, C., Bacchio, S., Bergner, G., Constantinou, M., Di Carlo, M., Dimopoulos, P., Finkenrath, J., Fiorenza, E., Frezzotti, R., Garofalo, M., Hadjiyiannakou, K., Kostrzewa, B., Koutsou, G., Jansen, K., Lubicz, V., Mangin-Brinet, M., Manigrasso, F., Martinelli, G., Papadiofantous, E., Pittler, F., Rossi, G. C., Sanfilippo, F., Simula, S., Tarantino, C., Todaro, A., Urbach, C., and Wenger, U.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology - Abstract
We present a calculation of the up, down, strange and charm quark masses performed within the lattice QCD framework. We use the twisted mass fermion action and carry out simulations that include in the sea two light mass-degenerate quarks, as well as the strange and charm quarks. In the analysis we use gauge ensembles simulated at three values of the lattice spacing and with light quarks that correspond to pion masses in the range from 350 MeV to the physical value, while the strange and charm quark masses are tuned approximately to their physical values. We use several quantities to set the scale in order to check for finite lattice spacing effects and in the continuum limit we get compatible results. The quark mass renormalization is carried out non-perturbatively using the RI'-MOM method converted into the $\overline{\rm MS}$ scheme. For the determination of the quark masses we use physical observables from both the meson and the baryon sectors, obtaining $m_{ud} = 3.636(66)(^{+60}_{-57})$~MeV and $m_s = 98.7(2.4)(^{+4.0}_{-3.2})$~MeV in the $\overline{\rm MS}(2\,{\rm GeV})$ scheme and $m_c = 1036(17)(^{+15}_{-8})$~MeV in the $\overline{\rm MS}(3\,{\rm GeV})$ scheme, where the first errors are statistical and the second ones are combinations of systematic errors. For the quark mass ratios we get $m_s / m_{ud} = 27.17(32)(^{+56}_{-38})$ and $m_c / m_s = 11.48(12)(^{+25}_{-19})$., Comment: 37 pages, 23 figures, 24 tables. One reference added
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- 2021
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4. The pion vector form factor from Lattice QCD at the physical point
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Alexandrou, C., Bacchio, S., Dimopoulos, P., Finkenrath, J., Frezzotti, R., Jansen, K., Kostrzewa, B., Mangin-Brinet, M., Sanfilippo, F., Simula, S., Urbach, C., and Wenger, U.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology - Abstract
We present an investigation of the electromagnetic pion form factor, $F_\pi(Q^2)$, at small values of the four-momentum transfer $Q^2$ ($\lesssim 0.25$ GeV$^2$), based on the gauge configurations generated by European Twisted Mass Collaboration with $N_f = 2$ twisted-mass quarks at maximal twist including a clover term. Momentum is injected using non-periodic boundary conditions and the calculations are carried out at a fixed lattice spacing ($a \simeq 0.09$ fm) and with pion masses equal to its physical value, 240 MeV and 340 MeV. Our data are successfully analyzed using Chiral Perturbation Theory at next-to-leading order in the light-quark mass. For each pion mass two different lattice volumes are used to take care of finite size effects. Our final result for the squared charge radius is $\langle r^2 \rangle_\pi = 0.443~(29)$ fm$^2$, where the error includes several sources of systematic errors except the uncertainty related to discretization effects. The corresponding value of the SU(2) chiral low-energy constant $\overline{\ell}_6$ is equal to $\overline{\ell}_6 = 16.2 ~ (1.0)$., Comment: 23 pages, 9 figures, 7 tables
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- 2017
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5. Nucleon scalar and tensor charges using lattice QCD simulations at the physical value of the pion mass
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Alexandrou, C., Constantinou, M., Dimopoulos, P., Frezzotti, R., Hadjiyiannakou, K., Jansen, K., Kallidonis, C., Kostrzewa, B., Koutsou, G., Mangin-Brinet, M., Avilès-Casco, A. Vaquero, and Wenger, U.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology ,Nuclear Experiment ,Nuclear Theory - Abstract
We present results on the light, strange and charm nucleon scalar and tensor charges from lattice QCD, using simulations with $N_f=2$ flavors of twisted mass Clover-improved fermions with a physical value of the pion mass. Both connected and disconnected contributions are included, enabling us to extract the isoscalar, strange and charm charges for the first time directly at the physical point. Furthermore, the renormalization is computed non-perturbatively for both isovector and isoscalar quantities. We investigate excited state effects by analyzing several sink-source time separations and by employing a set of methods to probe ground state dominance. Our final results for the scalar charges are $g_S^u = 5.20(42)(15)(12)$, $g_S^d = 4.27(26)(15)(12)$, $g_S^s=0.33(7)(1)(4)$, $g_S^c=0.062(13)(3)(5)$ and for the tensor charges $g_T^u = 0.782(16)(2)(13)$, $g_T^d = -0.219(10)(2)(13)$, $g_T^s=-0.00319(69)(2)(22)$, $g_T^c=-0.00263(269)(2)(37)$ in the $\overline{\rm MS}$ scheme at 2~GeV. The first error is statistical, the second is the systematic error due to the renormalization and the third the systematic arising from possible contamination due to the excited states., Comment: 20 pages and 13 figures
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- 2017
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6. First Physics Results at the Physical Pion Mass from $N_f = 2$ Wilson Twisted Mass Fermions at Maximal Twist
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ETM Collaboration, Abdel-Rehim, A., Alexandrou, C., Burger, F., Constantinou, M., Dimopoulos, P., Frezzotti, R., Hadjiyiannakou, K., Helmes, C., Jansen, K., Kallidonis, C. Jost. C., Knippschild, B., Kostrzewa, B., Koutsou, G., Liu, L., Mangin-Brinet, M., Ottnad, K., Petschlies, M., Pientka, G., Rossi, G. C., Urbach, C., Wenger, U., and Werner, M.
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High Energy Physics - Lattice - Abstract
We present physics results from simulations of QCD using $N_f = 2$ dynamical Wilson twisted mass fermions at the physical value of the pion mass. These simulations were enabled by the addition of the clover term to the twisted mass quark action. We show evidence that compared to previous simulations without this term, the pion mass splitting due to isospin breaking is almost completely eliminated. Using this new action, we compute the masses and decay constants of pseudoscalar mesons involving the dynamical up and down as well as valence strange and charm quarks at one value of the lattice spacing, $a \approx 0.09$ fm. Further, we determine renormalized quark masses as well as their scale-independent ratios, in excellent agreement with other lattice determinations in the continuum limit. In the baryon sector, we show that the nucleon mass is compatible with its physical value and that the masses of the $\Delta$ baryons do not show any sign of isospin breaking. Finally, we compute the electron, muon and tau lepton anomalous magnetic moments and show the results to be consistent with extrapolations of older ETMC data to the continuum and physical pion mass limits. We mostly find remarkably good agreement with phenomenology, even though we cannot take the continuum and thermodynamic limits., Comment: 45 pages, 15 figures
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- 2015
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7. Nucleon and pion structure with lattice QCD simulations at physical value of the pion mass
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Abdel-Rehim, A., Alexandrou, C., Constantinou, M., Dimopoulos, P., Frezzotti, R., Hadjiyiannakou, K., Jansen, K., Kallidonis, Ch., Kostrzewa, B., Koutsou, G., Mangin-Brinet, M., Oehm, M., Rossi, G. C., Urbach, C., and Wenger, U.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology ,Nuclear Experiment ,Nuclear Theory - Abstract
We present results on the nucleon scalar, axial and tensor charges as well as on the momentum fraction, and the helicity and transversity moments. The pion momentum fraction is also presented. The computation of these key observables is carried out using lattice QCD simulations at a physical value of the pion mass. The evaluation is based on gauge configurations generated with two degenerate sea quarks of twisted mass fermions with a clover term. We investigate excited states contributions with the nucleon quantum numbers by analyzing three sink-source time separations. We find that, for the scalar charge, excited states contribute significantly and to a less degree to the nucleon momentum fraction and helicity moment. Our analysis yields a value for the nucleon axial charge agrees with the experimental value and we predict a value of 1.027(62) in the $\overline{\text{MS}}$ scheme at 2 GeV for the isovector nucleon tensor charge directly at the physical point. The pion momentum fraction is found to be $\langle x\rangle_{u-d}^{\pi^\pm}=0.214(15)(^{+12}_{-9})$ in the $\overline{\rm MS}$ at 2 GeV., Comment: The experimental value of the helicity plotted in Fig.17 is corrected. ETM Collaboration. 25 pages, 19 figures. Version accepted for PRD (volume 92, eid 114513)
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- 2015
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8. The distribution amplitude of the ηc-meson at leading twist from lattice QCD.
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Blossier, B., Mangin-Brinet, M., Morgado Chávez, J. M., and San José, T.
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Distribution amplitudes are functions of non-perturbative matrix elements describing the hadronization of quarks and gluons. Thanks to factorization theorems, they can be used to compute the scattering amplitude of high-energy processes. Recently, new ideas have allowed their computation using lattice QCD, which should provide us with a general, fully relativistic determination. We present the first lattice calculation of the ηc-meson distribution amplitude at leading twist. Starting from the relevant matrix element in discrete Euclidean space on a set of Nf = 2 CLS ensembles, we explain the method to connect to continuum Minkowski spacetime. After addressing several sources of systematic uncertainty, we compare to Dyson-Schwinger and non-relativistic QCD determinations of this quantity. We find significant deviations between the latter and our result even at small Ioffe times. [ABSTRACT FROM AUTHOR]
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- 2024
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9. Progress in Simulations with Twisted Mass Fermions at the Physical Point
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Abdel-Rehim, A., Alexandrou, C., Dimopoulos, P., Frezzotti, R., Jansen, K., Kallidonis, C., Kostrzewa, B., Mangin-Brinet, M., Rossi, G. C., Urbach, C., and Wenger, U.
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High Energy Physics - Lattice - Abstract
In this contribution, results from $N_f=2$ lattice QCD simulations at one lattice spacing using twisted mass fermions with a clover term at the physical pion mass are presented. The mass splitting between charged and neutral pions (including the disconnected contribution) is shown to be around $20(20)~\mathrm{MeV}$. Further, a first measurement using the clover twisted mass action of the average momentum fraction of the pion is given. Finally, an analysis of pseudoscalar meson masses and decay constants is presented involving linear interpolations in strange and charm quark masses. Matching to meson mass ratios allows the calculation of quark mass ratios: $\mu_s/\mu_l=27.63(13)$, $\mu_c/\mu_l=339.6(2.2)$ and $\mu_c/\mu_s=12.29(10)$. From this mass matching the quantities $f_K=153.9(7.5)~\mathrm{MeV}$, $f_D=219(11)~\mathrm{MeV}$, $f_{D_s}=255(12)~\mathrm{MeV}$ and $M_{D_s}=1894(93)~\mathrm{MeV}$ are determined without the application of finite volume or discretization artefact corrections and with errors dominated by a preliminary estimate of the lattice spacing.
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- 2014
10. A novel method for the physical scale setting on the lattice and its application to $N_f$=4 simulations
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Morènas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Lattice - Abstract
This letter reports on a new procedure for the lattice spacing setting that takes advantage of the very precise determination of the strong coupling in Taylor scheme. Although it can be applied for the physical scale setting with the experimental value of $\Lambda_{\overline{\rm MS}}$ as an input, the procedure is particularly appropriate for relative "calibrations". The method is here applied for simulations with four degenerate light quarks in the sea and leads to prove that their physical scale is compatible with the same one for simulations with two light and two heavy flavours., Comment: 5 pages, 2 tables
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- 2013
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11. A first look at maximally twisted mass lattice QCD calculations at the physical point
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Abdel-Rehim, A., Boucaud, Ph., Carrasco, N., Deuzeman, A., Dimopoulos, P., Frezzotti, R., Herdoiza, G., Jansen, K., Kostrzewa, B., Mangin-Brinet, M., Montvay, I., Palao, D., Rossi, G. C., Sanfilippo, F., Scorzato, L., Shindler, A., Urbach, C., and Wenger, U.
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High Energy Physics - Lattice - Abstract
In this contribution, a first look at simulations using maximally twisted mass Wilson fermions at the physical point is presented. A lattice action including clover and twisted mass terms is presented and the Monte Carlo histories of one run with two mass-degenerate flavours at a single lattice spacing are shown. Measurements from the light and heavy-light pseudoscalar sectors are compared to previous $N_f = 2$ results and their phenomenological values. Finally, the strategy for extending simulations to $N_f = 2 + 1 + 1$ is outlined., Comment: presented at the 31st International Symposium on Lattice Field Theory (Lattice 2013), 29 July - 3 August 2013, Mainz, Germany
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- 2013
12. Three-gluon running coupling from lattice QCD at $N_f=2+1+1$: a consistency check of the OPE approach
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Boucaud, Ph., Brinet, M., De Soto, F., Morenas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Phenomenology - Abstract
We present a lattice calculation of the renormalized running coupling constant in symmetric (MOM) and asymmetric ($\widetilde{\rm MOM}$) momentum substraction schemes including $u$, $d$, $s$ and $c$ quarks in the sea. An Operator Product Expansion dominated by the dimension-two $\langle A^2\rangle$ condensate is used to fit the running of the coupling. We argue that the agreement in the predicted $\langle A^2\rangle$ condensate for both schemes is a strong support for the validity of the OPE approach and the effect of this non-gauge invariant condensate over the running of the strong coupling., Comment: Revised version (8 pages, 5 figures)
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- 2013
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13. High statistics determination of the strong coupling constant in Taylor scheme and its OPE Wilson coefficient from lattice QCD with a dynamical charm
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Morenas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Phenomenology ,High Energy Physics - Lattice - Abstract
This paper reports on the determination of $\alpha_S$ from lattice simulations with 2+1+1 twisted-mass dynamical flavours {\it via} the computation of the ghost-gluon coupling renormalized in the MOM Taylor scheme. A high-statistics sample of gauge configurations, used to evaluate the coupling from ghost and gluon propagators, allows for the appropriate update of previous results, now performing an improved analysis of data with reduced statistical errors and the systematical uncertainties under a better control., Comment: 15 pages, 7 figs (final version published in Phys.Rev.D)
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- 2013
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14. Testing the OPE Wilson coefficient for $A^2$ from lattice QCD with a dynamical charm
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Morenas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Phenomenology - Abstract
Gluon and ghost propagators data, obtained in Landau gauge from lattice simulations with two light and two heavy dynamical quark flavours ($N_f$=2+1+1), are described here with a running formula including a four-loop perturbative expression and a nonperturbative OPE correction dominated by the local operator $A^2$. The Wilson coefficients and their variation as a function of the coupling constant are extracted from the numerical data and compared with the theoretical expressions that, after being properly renormalized, are known at ${\cal O}(\alpha^4)$. As also $\Lambda_{\msbar}$ is rather well known for $N_f$=2+1+1, this allows for a precise consistency test of the OPE approach in the joint description of different observables., Comment: 12 pages, 11 figures, 3 tables
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- 2013
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15. Lattice measurement of \alpha_s with a realistic charm quark
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Du, X., Morenas, V., Pene, O., Petrov, K., and Rodriguez-Quintero, J.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology - Abstract
We report on an estimate of \alpha_s, renormalised in the MSbar scheme at the tau and Z^0 mass scales, by means of lattice QCD. Our major improvement compared to previous lattice calculations is that, for the first time, no perturbative treatment at the charm threshold has been required since we have used statistical samples of gluon fields built by incorporating the vacuum polarisation effects of u/d, s and c sea quarks. Extracting \alpha_s in the Taylor scheme from the lattice measurement of the ghost-ghost-gluon vertex, we obtain \alpha_s^{MSbar}(m^2_Z)=0.1200(14) and \alpha_s^{MSbar}(m^2_tau)=0.339(13)., Comment: Proceedings of the "QCD 12" conference in Montpellier
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- 2012
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16. The strong running coupling at $\tau$ and $Z_0$ mass scales from lattice QCD
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Du, X., Morenas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Phenomenology ,High Energy Physics - Lattice - Abstract
This letter reports on the first computation, from data obtained in lattice QCD with $u,d,s$ and $c$ quarks in the sea, of the running strong coupling via the ghost-gluon coupling renormalized in the MOM Taylor scheme. We provide with estimates of $\ams(m_\tau^2)$ and $\ams(m_Z^2)$ in very good agreement with experimental results. Including a dynamical c quark makes safer the needed running of $\ams$., Comment: 5 pages, 4 figures, 1 table (references updated)
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- 2012
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17. Nucleon form factors and moments of parton distributions in twisted mass lattice QCD
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Alexandrou, C., Brinet, M., Carbonell, J., Constantinou, M., Guichon, P., Harraud, P. A., Jansen, K., Kallidonis, C., Korzec, T., and Papinutto, M.
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High Energy Physics - Lattice - Abstract
We present results on the electroweak form factors and on the lower moments of parton distributions of the nucleon, within lattice QCD using two dynamical flavors of degenerate twisted mass fermions. Results are obtained on lattices with three different values of the lattice spacings, namely a=0.089 fm, a=0.070 fm and a=0.056 fm, allowing the investigation of cut-off effects. The volume dependence is examined by comparing results on two lattices of spatial length L=2.1 fm and L=2.8 fm. The simulations span pion masses in the range of 260-470 MeV. Our results are renormalized non-perturbatively and the values are given in the MS-scheme at a scale mu=2 GeV., Comment: Talk presented in the XXIst International Europhysics Conference on High Energy Physics, 21-27 July 2011, Grenoble, Rhones Alpes France
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- 2011
18. Renormalisation constants of quark bilinears in lattice QCD with four dynamical Wilson quarks
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Blossier, B., Brinet, M., Carrasco, N., Dimopoulos, P., Du, X., Frezzotti, R., Gimenez, V., Herdoiza, G., Jansen, K., Lubicz, V., Palao, D., Pallante, E., Pene, O., Petrov, K., Reker, S., Rossi, G. C., Sanfilippo, F., Scorzato, L., Simula, S., and Urbach, C.
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High Energy Physics - Lattice - Abstract
We present preliminary results of the non-perturbative computation of the RI-MOM renormalisation constants in a mass-independent scheme for the action with Iwasaki glue and four dynamical Wilson quarks employed by ETMC. Our project requires dedicated gauge ensembles with four degenerate sea quark flavours at three lattice spacings and at several values of the standard and twisted quark mass parameters. The RI-MOM renormalisation constants are obtained from appropriate O(a) improved estimators extrapolated to the chiral limit., Comment: 7 pages, 8 figures, Talk presented at the XXIX International Symposium on Lattice Field Theory (Lattice 2011), July 10-16, 2011, Squaw Valley, Lake Tahoe, California, USA
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- 2011
19. RI/MOM renormalization constants (N_f=4) and the strong coupling constant (N_f=2+1+1) from twisted-mass QCD
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Du, X., Gravina, M., Liu, Z., Morenas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Lattice - Abstract
We study RI/MOM renormalization constants of bilinear quark operators for $N_f=4$ and the strong coupling constant for $N_f=2+1+1$ using Wilson twisted-mass fermions. We use the "egalitarian" method to remove H(4) hypercubic artifacts non-perturbatively, which enables us to study physical quantities in a wide range of momenta. We then apply OPE in studying the running behavior of $Z_q$ and $\alpha_s$, from which we are able to extract the Landau gauge dimension-two gluon condensate $
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- 2011
20. Ghost-gluon coupling, power corrections and $\Lambda_{\bar{\rm MS}}$ from lattice QCD with a dynamical charm
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Du, X., Gravina, M., Morenas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Lattice - Abstract
This paper is a first report on the determination of $\Lambda_{\msbar}$ from lattice simulations with 2+1+1 twisted-mass dynamical flavours {\it via} the computation of the ghost-gluon coupling renormalized in the MOM Taylor scheme. We show this approach allows a very good control of the lattice artefacts and confirm the picture from previous works with quenched and ${\rm N}_f$=2 twisted-mass field configurations which prove the necessity to include non-perturbative power corrections in the description of the running. We provide with an estimate of $\Lambda_{\msbar}$ in very good agreement with experimental results. To our knowledge it is the first calculation with a dynamical charm quark which makes the running up to $\alpha_s(M_Z)$ much safer., Comment: 11 pages, 3 figures, 3 tables (new version accepted to be published in Phys. Rev. D)
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- 2011
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21. Design and construction of a Cherenkov imager for charge measurement of nuclear cosmic rays
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Bourrion, O., Bernard, Ch., Bondoux, D., Bouly, J. L., Bouvier, J., Boyer, B., Brinet, M., Buenerd, M., Damieux, G., Derome, L., Eraud, L., Foglio, R., Fombaron, D., Grondin, D., Lee, M. H., Lutz, L., Marton, M., Menchaca-Rocha, A., Pelissier, A., Périé, J. N., Putze, A., Roudier, S., Sallaz-Damaz, Y., Seo, E. S., Scordilis, J. P., and Yoon, Y. S.
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Astrophysics - Instrumentation and Methods for Astrophysics - Abstract
A proximity focusing Cherenkov imager called CHERCAM, has been built for the charge measurement of nuclear cosmic rays with the CREAM instrument. It consists of a silica aerogel radiator plane across from a detector plane equipped with 1,600 1" diameter photomultipliers. The two planes are separated by a ring expansion gap. The Cherenkov light yield is proportional to the charge squared of the incident particle. The expected relative light collection accuracy is in the few percents range. It leads to an expected single element separation over the range of nuclear charge Z of main interest 1 < Z < 26. CHERCAM is designed to fly with the CREAM balloon experiment. The design of the instrument and the implemented technical solutions allowing its safe operation in high altitude conditions (radiations, low pressure, cold) are presented., Comment: 24 pages, 19 figures
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- 2011
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22. Nucleon electromagnetic form factors in twisted mass lattice QCD
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Alexandrou, C., Brinet, M., Carbonell, J., Constantinou, M., Harraud, P. A., Guichon, P., Jansen, K., Korzec, T., and Papinutto, M.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology ,Nuclear Experiment ,Nuclear Theory - Abstract
We present results on the nucleon electromagnetic form factors within lattice QCD using two flavors of degenerate twisted mass fermions. Volume effects are examined using simulations at two volumes of spatial length L=2.1 fm and L=2.8 fm. Cut-off effects are investigated using three different values of the lattice spacings, namely a=0.089 fm, a=0.070 and a=0.056 fm. The nucleon magnetic moment, Dirac and Pauli radii are obtained in the continuum limit and chirally extrapolated to the physical pion mass allowing for a comparison with experiment., Comment: ETM Collaboration, 14 pages, 15 Figures
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- 2011
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23. Vacuum expectation value of A^2 from LQCD
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Pène, O., Blossier, B., Boucaud, Ph., Yaouanc, A. Le, Leroy, J. P., Micheli, J., Brinet, M., Gravina, M., De Soto, F., Liu, Z., Morenas, V., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Lattice - Abstract
We argue from LQCD that there is a non vanishing v.e.v of $A_a^\mu A^a_\mu$ in QCD in the Landau gauge. We use operator product expansion to provide a clear definition of $A_a^\mu A^a_\mu$ and extract a number both in the quenched and unquenched case., Comment: 10 pages, 5 figures, talk at the workshop "The many faces of QCD", November 2-5, 2010, Gent, Belgium
- Published
- 2011
24. A Layer Correlation technique for pion energy calibration at the 2004 ATLAS Combined Beam Test
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Abat, E., Abdallah, J. M., Addy, T. N., Adragna, P., Aharrouche, M., Ahmad, A., Akesson, T. P. A., Aleksa, M., Alexa, C., Anderson, K., Andreazza, A., Anghinolfi, F., Antonaki, A., Arabidze, G., Arik, E., Atkinson, T., Baines, J., Baker, O. K., Banfi, D., Baron, S., Barr, A. J., Beccherle, R., Beck, H. P., Belhorma, B., Bell, P. J., Benchekroun, D., Benjamin, D. P., Benslama, K., Kuutmann, E. Bergeaas, Bernabeu, J., Bertelsen, H., Binet, S., Biscarat, C., Boldea, V., Bondarenko, V. G., Boonekamp, M., Bosman, M., Bourdarios, C., Broklova, Z., Chromek, D. Burckhart, Bychkov, V., Callahan, J., Calvet, D., Canneri, M., Garrido, M. Capeáns, Caprini, M., Sas, L. Cardiel, Carli, T., Carminati, L., Carvalho, J., Cascella, M., Castillo, M. V., Catinaccio, A., Cauz, D., Cavalli, D., Sforza, M. Cavalli, Cavasinni, V., Cetin, S. A., Chen, H., Cherkaoui, R., Chevalier, L., Chevallier, F., Chouridou, S., Ciobotaru, M., Citterio, M., Clark, A., Cleland, B., Cobal, M., Cogneras, E., Muino, P. Conde, Consonni, M., Constantinescu, S., Cornelissen, T., Correard, S., Radu, A. Corso, Costa, G., Costa, M. J., Costanzo, D., Cuneo, S., Cwetanski, P., Da Silva, D., Dam, M., Dameri, M., Danielsson, H. O., Dannheim, D., Darbo, G., Davidek, T., De, K., Defay, P. O., Dekhissi, B., Del Peso, J., Del Prete, T., Delmastro, M., Derue, F., Di Ciaccio, L., Di Girolamo, B., Dita, S., Dittus, F., Djama, F., Djobava, T., Dobos, D., Dobson, M., Dolgoshein, B. A., Dotti, A., Drake, G., Drasal, Z., Dressnandt, N., Driouchi, C., Drohan, J., Ebenstein, W. L., Eerola, P., Efthymiopoulos, I., Egorov, K., Eifert, T. F., Einsweiler, K., Kacimi, M. El, Elsing, M., Emelyanov, D., Escobar, C., Etienvre, A. I., Fabich, A., Facius, K., Fakhr-Edine, A. I., Fanti, M., Farbin, A., Farthouat, P., Fassouliotis, D., Fayard, L., Febbraro, R., Fedin, O. L., Fenyuk, A., Fergusson, D., Ferrari, P., Ferrari, R., Ferreira, B. C., Ferrer, A., Ferrere, D., Filippini, G., Flick, T., Fournier, D., Francavilla, P., Francis, D., Froeschl, R., Froidevaux, D., Fullana, E., Gadomski, S., Gagliardi, G., Gagnon, P., Gallas, M., Gallop, B. J., Gameiro, S., Gan, K. K., Garcia, R., Garcia, C., Gavrilenko, I. L., Gemme, C., Gerlach, P., Ghodbane, N., Giakoumopoulou, V., Giangiobbe, V., Giokaris, N., Glonti, G., Goettfert, T., Golling, T., Gollub, N., Gomes, A., Gomez, M. D., Gonzalez-Sevilla, S., Goodrick, M. J., Gorfine, G., Gorini, B., Goujdami, D., Grahn, K-J., Grenier, P., Grigalashvili, N., Grishkevich, Y., Grosse-Knetter, J., Gruwe, M., Guicheney, C., Gupta, A., Haeberli, C., Haertel, R., Hajduk, Z., Hakobyan, H., Hance, M., Hansen, J. D., Hansen, P. H., Hara, K., Harvey Jr., A., Hawkings, R. J., Heinemann, F. E. W., Correia, A. Henriques, Henss, T., Hervas, L., Higon, E., Hill, J. C., Hoffman, J., Hostachy, J. Y., Hruska, I., Hubaut, F., Huegging, F., Hulsbergen, W., Hurwitz, M., Iconomidou-Fayard, L., Jansen, E., Plante, I. Jen-La, Johansson, P. D. C., Jon-And, K., Joos, M., Jorgensen, S., Joseph, J., Kaczmarska, A., Kado, M., Karyukhin, A., Kataoka, M., Kayumov, F., Kazarov, A., Keener, P. T., Kekelidze, G. D., Kerschen, N., Kersten, S., Khomich, A., Khoriauli, G., Khramov, E., Khristachev, A., Khubua, J., Kittelmann, T. H., Klingenberg, R., Klinkby, E. B., Kodys, P., Koffas, T., Kolos, S., Konovalov, S. P., Konstantinidis, N., Kopikov, S., Korolkov, I., Kostyukhin, V., Kovalenko, S., Kowalski, T. Z., Krüger, K., Kramarenko, V., Kudin, L. G., Kulchitsky, Y., Lacasta, C., Lafaye, R., Laforge, B., Lampl, W., Lanni, F., Laplace, S., Lari, T., Bihan, A-C. Le, Lechowski, M., Ledroit-Guillon, F., Lehmann, G., Leitner, R., Lelas, D., Lester, C. G., Liang, Z., Lichard, P., Liebig, W., Lipniacka, A., Lokajicek, M., Louchard, L., Lourerio, K. F., Lucotte, A., Luehring, F., Lund-Jensen, B., Lundberg, B., Ma, H., Mackeprang, R., Maio, A., Maleev, V. P., Malek, F., Mandelli, L., Maneira, J., Mangin-Brinet, M., Manousakis, A., Mapelli, L., Marques, C., Garcia, S. Marti i, Martin, F., Mathes, M., Mazzanti, M., McFarlane, K. W., McPherson, R., Mchedlidze, G., Mehlhase, S., Meirosu, C., Meng, Z., Meroni, C., Mialkovski, V., Mikulec, B., Milstead, D., Minashvili, I., Mindur, B., Mitsou, V. A., Moed, S., Monnier, E., Moorhead, G., Morettini, P., Morozov, S. V., Mosidze, M., Mouraviev, S. V., Moyse, E. W. J., Munar, A., Myagkov, A., Nadtochi, A. V., Nakamura, K., Nechaeva, P., Negri, A., Nemecek, S., Nessi, M., Nesterov, S. Y., Newcomer, F. M., Nikitine, I., Nikolaev, K., Nikolic-Audit, I., Ogren, H., Oh, S. H., Oleshko, S. B., Olszowska, J., Onofre, A., Aranda, C. Padilla, Paganis, S., Pallin, D., Pantea, D., Paolone, V., Parodi, F., Parsons, J., Parzhitskiy, S., Pasqualucci, E., Passmored, S. M., Pater, J., Patrichev, S., Peez, M., Reale, V. Perez, Perini, L., Peshekhonov, V. D., Petersen, J., Petersen, T. C., Petti, R., Phillips, P. W., Pina, J., Pinto, B., Podlyski, F., Poggioli, L., Poppleton, A., Poveda, J., Pralavorio, P., Pribyl, L., Price, M. J., Prieur, D., Puigdengoles, C., Puzo, P., Røhne, O., Ragusa, F., Rajagopalan, S., Reeves, K., Reisinger, I., Rembser, C., Renstrom, P. A. Bruckman. de., Reznicek, P., Ridel, M., Risso, P., Riu, I., Robinson, D., Roda, C., Roe, S., Rohne, O., Romaniouk, A., Rousseau, D., Rozanov, A., Ruiz, A., Rusakovich, N., Rust, D., Ryabov, Y. F., Ryjov, V., Salto, O., Salvachua, B., Salzburger, A., Sandaker, H., Rios, C. Santamarina, Santi, L., Santoni, C., Saraiva, J. G., Sarri, F., Sauvage, G., Says, L. P., Schaefer, M., Schegelsky, V. A., Schiavi, C., Schieck, J., Schlager, G., Schlereth, J., Schmitt, C., Schultes, J., Schwemling, P., Schwindling, J., Seixas, J. M., Seliverstov, D. M., Serin, L., Sfyrla, A., Shalanda, N., Shaw, C., Shin, T., Shmeleva, A., Silva, J., Simion, S., Simonyan, M., Sloper, J. E., Smirnov, S. Yu., Smirnova, L., Solans, C., Solodkov, A., Solovianov, O., Soloviev, I., Sosnovtsev, V. V., Spanó, F., Speckmayer, P., Stancu, S., Stanek, R., Starchenko, E., Straessner, A., Suchkov, S. I., Suk, M., Szczygiel, R., Tarrade, F., Tartarelli, F., Tas, P., Tayalati, Y., Tegenfeldt, F., Teuscher, R., Thioye, M., Tikhomirov, V. O., Timmermans, C. J. W. P., Tisserant, S., Toczek, B., Tremblet, L., Troncon, C., Tsiareshka, P., Tyndel, M., Unel, M. Karagoez., Unal, G., Unel, G., Usai, G., Van Berg, R., Valero, A., Valkar, S., Valls, J. A., Vandelli, W., Vannucci, F., Vartapetian, A., Vassilakopoulos, V. I., Vasilyeva, L., Vazeille, F., Vernocchi, F., Vetter-Cole, Y., Vichou, I., Vinogradov, V., Virzi, J., Vivarelli, I., Vivie, J. B. de., Volpi, M., Anh, T. Vu, Wang, C., Warren, M., Weber, J., Weber, M., Weidberg, A. R., Weingarten, J., Wells, P. S., Werner, P., Wheeler, S., Wiessmann, M., Wilkens, H., Williams, H. H., Wingerter-Seez, I., Yasu, Y., Zaitsev, A., Zenin, A., Zenis, T., Zenonos, Z., Zhang, H., Zhelezko, A., and Zhou, N.
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Physics - Instrumentation and Detectors ,High Energy Physics - Experiment - Abstract
A new method for calibrating the hadron response of a segmented calorimeter is developed and successfully applied to beam test data. It is based on a principal component analysis of energy deposits in the calorimeter layers, exploiting longitudinal shower development information to improve the measured energy resolution. Corrections for invisible hadronic energy and energy lost in dead material in front of and between the calorimeters of the ATLAS experiment were calculated with simulated Geant4 Monte Carlo events and used to reconstruct the energy of pions impinging on the calorimeters during the 2004 Barrel Combined Beam Test at the CERN H8 area. For pion beams with energies between 20 GeV and 180 GeV, the particle energy is reconstructed within 3% and the energy resolution is improved by between 11% and 25% compared to the resolution at the electromagnetic scale., Comment: 36 pages, 12 figures, accepted by JINST
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- 2010
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25. Axial Nucleon form factors from lattice QCD
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Alexandrou, C., Brinet, M., Carbonell, J., Constantinou, M., Harraud, P. A., Guichon, P., Jansen, K., Korzec, T., and Papinutto, M.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology ,Nuclear Experiment ,Nuclear Theory - Abstract
We present results on the nucleon axial form factors within lattice QCD using two flavors of degenerate twisted mass fermions. Volume effects are examined using simulations at two volumes of spatial length $L=2.1$ fm and $L=2.8$ fm. Cut-off effects are investigated using three different values of the lattice spacings, namely $a=0.089$ fm, $a=0.070$ fm and $a=0.056$ fm. The nucleon axial charge is obtained in the continuum limit and chirally extrapolated to the physical pion mass enabling comparison with experiment., Comment: ETM Collaboration, 14 pages, 12 figures
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- 2010
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26. Renormalisation of quark propagators from twisted-mass lattice QCD at $N_f$=2
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Liu, Z., Morenas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
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High Energy Physics - Phenomenology - Abstract
We present results concerning the non-perturbative evaluation of the renormalisation constant for the quark field, $Z_q$, from lattice simulations with twisted mass quarks and three values of the lattice spacing. We use the RI'-MOM scheme. $Z_q$ has very large lattice spacing artefacts; it is considered here as a test bed to elaborate accurate methods which will be used for other renormalisation constants. We recall and develop the non-perturbative correction methods and propose tools to test the quality of the correction. These tests are also applied to the perturbative correction method. We check that the lattice spacing artefacts scale indeed as $a^2p^2$. We then study the running of $Z_q$ with particular attention to the non-perturbative effects, presumably dominated by the dimension-two gluon condensate $\VEV{A^2}$ in Landau gauge. We show indeed that this effect is present, and not small. We check its scaling in physical units confirming that it is a continuum effect. It gives a $\sim 4%$ contribution at 2 GeV. Different variants are used in order to test the reliability of our result and estimate the systematic uncertainties. Finally combining all our results and using the known Wilson coefficient of $\VEV{A^2}$ we find $g^2(\mu^2) \VEV{A^2}_{\mu^2\; CM} = 2.01(11)(^{+0.61}_{- 0.73}) \;\mathrm {GeV}^2$ at $\mu=10\, \mathrm{GeV}$, in fair agreement within uncertainties with the value indepently extracted from the strong coupling constant., Comment: 38 pages, 8 tables, 8 figures
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- 2010
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27. Nucleon form factors with Nf=2 dynamical twisted mass fermions
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Alexandrou, C., Korzec, T., Koutsou, G., Baron, R., Guichon, P., Brinet, M., Carbonell, J., Harraud, P. -A., and Jansen, K.
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High Energy Physics - Lattice ,High Energy Physics - Phenomenology ,Nuclear Experiment ,Nuclear Theory - Abstract
We present results on the electromagnetic and axial nucleon form factors using two degenerate flavors of twisted mass fermions on lattices of spatial size 2.1 fm and 2.7 fm and a lattice spacing of about 0.09 fm. We consider pion masses in the range of 260-470 MeV. We chirally extrapolate results on the nucleon axial ch arge, the isovector Dirac and Pauli root mean squared radii and magnetic moment to the physical point and co mpare to experiment., Comment: Report no. added; typos corrected. ETM Collaboration, 7 pages, 10 figures, Talk given at the XXVII International Symposium on Lattice Field Theory - LAT2009, July 26-31 2009, Peking University, Beijing, China
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- 2009
28. Partially quenched study of strange baryon with Nf = 2 twisted mass fermions
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Drach, V., Brinet, M., Carbonell, J., Liu, Z., Alexandrou, C., Korzec, T., Koutsou, G., Baron, R., Guichon, P., Pène, O., Pallante, E., Reker, S., Urbach, C., and Jansen, K.
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High Energy Physics - Lattice - Abstract
We present results on the mass of the baryon octet and decuplet using two flavors of light dynamical twisted mass fermions. The strange quark mass is fixed to its physical value from the kaon sector in a partially quenched set up. Calculations are performed for light quark masses corresponding to a pion mass in the range 270-500 MeV and lattice sizes of 2.1 fm and 2.7 fm. We check for cut-off effects and isospin breaking by evaluating the baryon masses at two different lattice spacings. We carry out a chiral extrapolation for the octet baryons and discuss results for the Omega., Comment: 7 pages, 9 figures, Talk presented at The XXVI International Symposium on Lattice Field Theory, LATTICE 2008, July 14 - 19, 2008, Williamsburg, Virginia, USA
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- 2009
29. Electromagnetic form factor via Bethe-Salpeter amplitude in Minkowski space
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Carbonell, J., Karmanov, V. A., and Mangin-Brinet, M.
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High Energy Physics - Phenomenology ,High Energy Physics - Theory ,Nuclear Theory - Abstract
For a relativistic system of two scalar particles, we find the Bethe-Salpeter amplitude in Minkowski space and use it to compute the electromagnetic form factor. The comparison with Euclidean space calculation shows that the Wick rotation in the form factor integral induces errors which increase with the momentum transfer Q^2. At JLab domain (Q^2=10 GeV^2/c^2), they are about 30%. Static approximation results in an additional and more significant error. On the contrary, the form factor calculated in light-front dynamics is almost indistinguishable from the Minkowski space one., Comment: 8 pages, 7 figures, to be published in Eur. Phys. J. A; Reference [15] is added
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- 2008
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30. Alignment of the Pixel and SCT Modules for the 2004 ATLAS Combined Test Beam
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Ahmad, A., Andreazza, A., Atkinson, T., Baines, J., Barr, A. J., Beccherle, R., Bell, P. J., Bernabeu, J., Broklova, Z., de Renstrom, P. A. Bruckman, Cauz, D., Chevalier, L., Chouridou, S., Citterio, M., Clark, A., Cobal, M., Cornelissen, T., Correard, S., Costa, M. J., Costanzo, D., Cuneo, S., Dameri, M., Darbo, G., de Vivie, J. B., Di Girolamo, B., Dobos, D., Drasal, Z., Drohan, J., Einsweiler, K., Elsing, M., Emelyanov, D., Escobar, C., Facius, K., Ferrari, P., Fergusson, D., Ferrere, D., Flick, T., Froidevaux, D., Gagliardi, G., Gallas, M., Gallop, B. J., Gan, K. K., Garcia, C., Gavrilenko, I. L., Gemme, C., Gerlach, P., Golling, T., Gonzalez-Sevilla, S., Goodrick, M. J., Gorfine, G., Goettfert, T., Grosse-Knetter, J., Hansen, P. H., Hara, K., Hartel, R., Harvey, A., Hawkings, R. J., Heinemann, F. E. W., Henns, T., Hill, J. C., Huegging, F., Jansen, E., Joseph, J., Unel, M. Karagoz, Kataoka, M., Kersten, S., Khomich, A., Klingenberg, R., Kodys, P., Koffas, T., Konstantinidis, N., Kostyukhin, V., Lacasta, C., Lari, T., Latorre, S., Lester, C. G., Liebig, W., Lipniacka, A., Lourerio, K. F., Mangin-Brinet, M., Garcia, S. Marti i, Mathes, M., Meroni, C., Mikulec, B., Mindur, B., Moed, S., Moorhead, G., Morettini, P., Moyse, E. W. J., Nakamura, K., Nechaeva, P., Nikolaev, K., Parodi, F., Parzhitski, S., Pater, J., Petti, R., Phillips, P. W., Pinto, B., Poppleton, A., Reeves, K., Reisinger, I., Reznicek, P., Risso, P., Robinson, D., Roe, S., Rozanov, A., Salzburger, A., Sandaker, H., Santi, L., Schiavi, C., Schieck, J., Schultes, J., Sfyrla, A., Shaw, C., Tegenfeldt, F., Timmermans, C. J. W. P., Toczek, B., Troncon, C., Tyndel, M., Vernocchi, F., Virzi, J., Anh, T. Vu, Warren, M., Weber, J., Weber, M., Weidberg, A. R., Weingarten, J., Wells, P. S., and Zhelezko, A.
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Physics - Instrumentation and Detectors ,High Energy Physics - Experiment - Abstract
A small set of final prototypes of the ATLAS Inner Detector silicon tracker (Pixel and SCT) were used to take data during the 2004 Combined Test Beam. Data were collected from runs with beams of different flavour (electrons, pions, muons and photons) with a momentum range of 2 to 180 GeV/c. Four independent methods were used to align the silicon modules. The corrections obtained were validated using the known momenta of the beam particles and were shown to yield consistent results among the different alignment approaches. From the residual distributions, it is concluded that the precision attained in the alignment of the silicon modules is of the order of 5 micrometers in their most precise coordinate., Comment: 22 pages, submitted to JINST, 129 authors
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- 2008
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31. Light baryon masses with dynamical twisted mass fermions
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Alexandrou, C., Baron, R., Blossier, B., Brinet, M., Carbonell, J., Dimopoulos, P., Drach, V., Farchioni, F., Frezzotti, R., Guichon, P., Herdoiza, G., Jansen, K., Korzec, T., Koutsou, G., Liu, Z., Michael, C., Pène, O., Shindler, A., Urbach, C., and Wenger, U.
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High Energy Physics - Lattice - Abstract
We present results on the mass of the nucleon and the Delta using two dynamical degenerate twisted mass quarks and the tree-level Symanzik improved gauge action. The evaluation is performed at four quark masses corresponding to a pion mass in the range of about 300-600 MeV on lattices of 2.1-2.7 fm. We check for cut-off effects by evaluating these baryon masses on lattices of spatial size 2.1 fm at beta=3.9 and beta=4.05 and on a lattice of 2.4 fm at beta=3.8. The values we find are compatible within our statistical errors. Lattice results are extrapolated to the physical limit using continuum chiral perturbation theory. Performing a combined fit to our lattice data at beta=3.9 and beta=4.05 we find a nucleon mass of 964\pm 28 (stat.) \pm 8 (syst.) MeV. The nucleon mass at the physical point provides an independent determination of the lattice spacing. Using heavy baryon chiral perturbation theory at O(p^3) we find a_{\beta=3.9}=0.0890\pm 0.0039(stat.) \pm 0.0014(syst.) fm, and a_{\beta=4.05}= 0.0691\pm 0.0034(stat.) \pm 0.0010(syst.) fm, in good agreement with the values determined from the pion decay constant. Isospin violating lattice artifacts in the Delta-system are found to be compatible with zero for the values of the lattice spacings used in this work. Performing a combined fit to our lattice data at beta=3.9 and beta=4.05 we find for the masses of the Delta^{++,-} and Delta^{+,0} 1316 \pm 60 (stat.) MeV and 1330 \pm 74 (stat.) MeV respectively. We confirm that in the continuum limit they are also degenerate., Comment: 19 pages, 18 figures, Version as accepted in Phys. Rev. D, Discussion on nucleon sigma-term extended, typos corrected
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- 2008
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32. The RICH detector of the AMS-02 experiment: status and physics prospects
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Pereira, Rui, Aguilar-Benitez, M., Arruda, L., Barao, F., Baret, B., Barrau, A., Barreira, G., Belmont, E., Berdugo, J., Borges, J., Buenerd, M., Casadei, D., Casaus, J., Cortina, E., Costado, M., Crespo, D., Delgado, C., Diaz, C., Derome, L., Goncalves, P., Garcia-Lopez, R., de la Guia, C., Herrero, A., Lanciotti, E., Laurenti, G., Malinin, A., Mana, C., Marin, J., Mangin-Brinet, M., Martinez, G., Menchaca-Rocha, A., Palomares, C., Pimenta, M., Putze, A., Sallaz-Damaz, Y., Seo, E. S., Sevilla, I., Torrento, A., Vargas-Trevino, M., and Veziant, O.
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Astrophysics - Abstract
The Alpha Magnetic Spectrometer (AMS), whose final version AMS-02 is to be installed on the International Space Station (ISS) for at least 3 years, is a detector designed to measure charged cosmic ray spectra with energies up to the TeV region and with high energy photon detection capability up to a few hundred GeV. It is equipped with several subsystems, one of which is a proximity focusing RICH detector with a dual radiator (aerogel+NaF) that provides reliable measurements for particle velocity and charge. The assembly and testing of the AMS RICH is currently being finished and the full AMS detector is expected to be ready by the end of 2008. The RICH detector of AMS-02 is presented. Physics prospects are briefly discussed., Comment: 5 pages. Contribution to the 10th ICATPP Conference on Astroparticle, Particle, Space Physics, Detectors and Medical Physics Applications (Como 2007). Presenter: Rui Pereira
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- 2008
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33. Electromagnetic form factor via Minkowski and Euclidean Bethe-Salpeter amplitudes
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Karmanov, V. A., Carbonell, J., and Mangin-Brinet, M.
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High Energy Physics - Phenomenology - Abstract
The electromagnetic form factors calculated through Euclidean Bethe-Salpeter amplitude and through the light-front wave function are compared with the one found using the Bethe-Salpeter amplitude in Minkowski space. The form factor expressed through the Euclidean Bethe-Salpeter amplitude (both within and without static approximation) considerably differs from the Minkowski one, whereas form factor found in the light-front approach is almost indistinguishable from it., Comment: 3 pages, 2 figures. Contribution to the proceedings of the 20th International Conference on Few-Body Problems in Physics (FB20), Pisa, Italy, September 10-14, 2007. To be published in "Few-Body Systems"
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- 2007
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34. The AMS-RICH velocity and charge reconstruction
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Barao, F., Aguilar-Benitez, M., Arruda, L., Baret, B., Barrau, A., Barreira, G., Belmont, E., Berdugo, J., Borges, J., Buenerd, M., Casadei, D., Casaus, J., Cortina, E., Costado, M., Crespo, D., Delgado, C., Diaz, C., Derome, L., Goncalves, P., Garcia-Lopez, R., de la Guia, C., Herrero, A., Lanciotti, E., Laurenti, G., Malinin, A., Mana, C., Marin, J., Mangin-Brinet, M., Martinez, G., Menchaca-Rocha, A., Palomares, C., Pereira, R., Pimenta, M., Putze, A., Sallaz-Damaz, Y., Seo, E. S., Sevilla, I., Torrento, A., Vargas-Trevino, M., and Veziant, O.
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Astrophysics - Abstract
The AMS detector, to be installed on the International Space Station, includes a Ring Imaging Cerenkov detector with two different radiators, silica aerogel (n=1.05) and sodium fluoride (n=1.334). This detector is designed to provide very precise measurements of velocity and electric charge in a wide range of cosmic nuclei energies and atomic numbers. The detector geometry, in particular the presence of a reflector for acceptance purposes, leads to complex Cerenkov patterns detected in a pixelized photomultiplier matrix. The results of different reconstruction methods applied to test beam data as well as to simulated samples are presented. To ensure nominal performances throughout the flight, several detector parameters have to be carefully monitored. The algorithms developed to fulfill these requirements are presented. The velocity and charge measurements provided by the RICH detector endow the AMS spectrometer with precise particle identification capabilities in a wide energy range. The expected performances on light isotope separation are discussed., Comment: Contribution to the ICRC07, Merida, Mexico (2007); Presenter: F. Barao
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- 2007
35. Bethe-Salpeter equation with cross-ladder kernel in Minkowski and Euclidean spaces
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Karmanov, V. A., Carbonell, J., and Mangin-Brinet, M.
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High Energy Physics - Theory ,High Energy Physics - Phenomenology ,Nuclear Theory - Abstract
Some results obtained by a new method for solving the Bethe-Salpeter equation are presented. The method is valid for any kernel given by irreducible Feynman graphs. The Bethe-Salpeter amplitude, both in Minkowski and in Euclidean spaces, and the binding energy for ladder + cross-ladder kernel are found. We calculate also the corresponding electromagnetic form factor., Comment: 4 pages, 3 figures. Contribution to the proceedings of the 18th International IUPAP Conference on Few-Body Problems in Physics (FB18), Santos, Brasil, August 21-26, 2006. To be published in Nucl. Phys. A
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- 2006
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36. The Ring Imaging Cherenkov detector (RICH) of the AMS experiment
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Barao, F., Benitez, M. Aguilar, Alcaraz, J., Arruda, L., Barrau, A., Barreira, G., Belmont, E., Berdugo, J., Brinet, M., Buenerd, M., Casadei, D., Casaus, J., Cortina, E., Delgado, C., Diaz, C., Derome, L., Eraud, L., Garcia-Lopez, R. J., Gallin-Martel, L., Giovacchini, F., Goncalves, P., Lanciotti, E., Laurenti, G., Malinine, A., Mana, C., Marin, J., Martinez, G., Menchaca-Rocha, A., Molla, M., Palomares, C., Panniello, M., Pereira, R., Pimenta, M., Protasov, K., Sanchez, E., Seo, E-S., Sevilla, N., Torrento, A., Vargas-Trevino, M., and Veziant, O.
- Subjects
Astrophysics - Abstract
The Alpha Magnetic Spectrometer (AMS) experiment to be installed on the International Space Station (ISS) will be equipped with a proximity focusing Ring Imaging Cherenkov (RICH) detector for measuring the electric charge and velocity of the charged cosmic particles. A RICH prototype consisting of 96 photomultiplier units, including a piece of the conical reflector, was built and its performance evaluated with ion beam data. Preliminary results of the in-beam tests performed with ion fragments resulting from collisions of a 158 GeV/c/nuc primary beam of Indium ions (CERN SPS) on a Pb target are reported. The collected data included tests to the final front-end electronics and to different aerogel radiators. Cherenkov rings for a large range of charged nuclei and with reflected photons were observed. The data analysis confirms the design goals. Charge separation up to Fe and velocity resolution of the order of 0.1% for singly charged particles are obtained., Comment: 29th International Conference on Cosmic Rays (Pune, India)
- Published
- 2006
37. Two-fermion relativistic bound states in Light-Front Dynamics
- Author
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Mangin-Brinet, M., Carbonell, J., and Karmanov, V. A.
- Subjects
High Energy Physics - Theory ,High Energy Physics - Phenomenology ,Nuclear Theory - Abstract
In the Light-Front Dynamics, the wave function equations and their numerical solutions, for two fermion bound systems, are presented. Analytical expressions for the ladder one-boson exchange interaction kernels corresponding to scalar, pseudoscalar, pseudovector and vector exchanges are given. Different couplings are analyzed separately and each of them is found to exhibit special features. The results are compared with the non relativistic solutions., Comment: 40 pages, to be published in Phys. Rev. C, .tar.gz file
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- 2003
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38. Two-Body Bound States in Light-Front Dynamics
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Carbonell, J., Mangin-Brinet, M., and Karmanov, V. A.
- Subjects
Nuclear Theory - Abstract
We present the main features of the explicitly covariant Light-Front Dynamics formalism and a summary of our recent works on this topic. They concern the bound states of two scalar particles in the Wick-Cutkosky model and of two fermions interacting via the usual OBEP ladder kernels., Comment: Invited contribution to the XIVth International School on Nuclear Physics, Varna, Bulgaria, Sept 25-30. 20 pages, 23 figures
- Published
- 2002
39. Two-fermion bound states in the explicitly covariant Light-Front Dynamics
- Author
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Karmanov, V. A., Carbonell, J., and Mangin-Brinet, M.
- Subjects
Nuclear Theory ,High Energy Physics - Theory - Abstract
We develop a general method to construct two relativistic fermions bound states with a given $J^{\pi}$, in the framework of the explicitly covariant light-front dynamics., Comment: 3 pages, 1 figure, to be published in Nucl. Phys. B (Proc. Suppl.), contribution to the XIth Light-cone Meeting at ECT* in Trento, Sep 3-11, 2001
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- 2001
- Full Text
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40. Stability of two-fermion bound states in the explicitly covariant Light-Front Dynamics
- Author
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Mangin-Brinet, M., Carbonell, J., and Karmanov, V. A.
- Subjects
High Energy Physics - Theory ,Nuclear Theory - Abstract
The covariant light-front equations have been solved exactly for a two fermion system with different boson exchange ladder kernels. We present a method to study the cutoff dependence of these equations and to determine whether they need to be regularized or not. Results are presented for scalar and pseudo-scalar exchange. This latter furthermore exhibits some strange particularities which will be discussed., Comment: 5 pages, 8 figures, to be published in Nucl. Phys. B (Proc. Suppl.), contribution to the XIth Light-cone Meeting at ECT* in Trento, Sep 3-11, 2001
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- 2001
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41. Relativistic bound states in Yukawa model
- Author
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Mangin-Brinet, M., Carbonell, J., and Karmanov, V. A.
- Subjects
High Energy Physics - Theory ,High Energy Physics - Phenomenology ,Nuclear Theory - Abstract
The bound state solutions of two fermions interacting by a scalar exchange are obtained in the framework of the explicitly covariant light-front dynamics. The stability with respect to cutoff of the J$^{\pi}$=$0^+$ and J$^{\pi}$=$1^+$ states is studied. The solutions for J$^{\pi}$=$0^+$ are found to be stable for coupling constants $\alpha={g^2\over4\pi}$ below the critical value $\alpha_c\approx 3.72$ and unstable above it. The asymptotic behavior of the wave functions is found to follow a ${1\over k^{2+\beta}}$ law. The coefficient $\beta$ and the critical coupling constant $\alpha_c$ are calculated from an eigenvalue equation. The binding energies for the J$^{\pi}$=$1^+$ solutions diverge logarithmically with the cutoff for any value of the coupling constant. For a wide range of cutoff, the states with different angular momentum projections are weakly split., Comment: 22 pages, 13 figures, .tar.gz file
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- 2001
- Full Text
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42. Stability of bound states in the light-front Yukawa model
- Author
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Karmanov, V. A., Carbonell, J., and Mangin-Brinet, M.
- Subjects
High Energy Physics - Theory ,High Energy Physics - Phenomenology ,Nuclear Theory - Abstract
We show that in the system of two fermions interacting by scalar exchange, the solutions for J$^{\pi}$=$0^+$ bound states are stable without any cutoff regularization, for values of the coupling constant $\alpha$ below a critical value $\alpha_c$. This latter is calculated from an eigenvalue equation., Comment: 4 pages, 3 figures, .tar.gz file
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- 2001
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43. Selected topics on Low Energy Antiproton Physics
- Author
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Carbonell, J. and Mangin-Brinet, M.
- Subjects
Nuclear Theory - Abstract
Some of the last results on low energy antiproton physics are reviewed. First Faddeev calculations for \={n}d scattering length are presented., Comment: 10 pages, 11 figures Invited talk to the Biennial Conference on Low Energy Antiproton Physics (LEAP 2000), Venice 20-26 August (2000). To appear in Nuclear Physics B
- Published
- 2001
- Full Text
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44. Stability of bound states in the light-front Yukawa model
- Author
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Mangin-Brinet, M., Carbonell, J., and Karmanov, V. A.
- Subjects
High Energy Physics - Theory ,High Energy Physics - Phenomenology ,Nuclear Theory - Abstract
We show that in the system of two fermions interacting by scalar exchange, the solutions for J$^{\pi}$=$0^+$ bound states are stable without any cutoff regularization for coupling constant below some critical value., Comment: 5 pages, 2 figures, submitted to publication
- Published
- 2001
- Full Text
- View/download PDF
45. Weak binding limit and non zero angular momentum states in Light-Front Dynamics
- Author
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Mangin-Brinet, M., Carbonell, J., and Karmanov, V. A.
- Subjects
High Energy Physics - Theory - Abstract
We show some results concerning the weak binding limit for J=0 states -- which turn out to strongly differ from the non relativistic case -- together with the construction of non zero angular momentum states. The calculation of such states in the Light-Front Dynamics (LFD) framework has some peculiarities which are absent in other approaches. They are related to the fact that the rotation generators contain interaction. We present here the construction of non zero angular momentum states in LFD and show how it leads to a restoration of rotational invariance. For this purpose, the use of Light-Front Dynamics in its explicitly covariant formulation is of crucial importance since the dependence of the wave function on the light-front plane is explicitly parametrized., Comment: To appear in Nucl.Phys.B, 6 pages, 3 figures, .tar.gz file
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- 2000
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46. Relativistic wave functions and energies for nonzero angular momentum states in light-front dynamics
- Author
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Karmanov, V. A., Mangin-Brinet, M., and Carbonell, J.
- Subjects
High Energy Physics - Theory - Abstract
Light-front dynamics (LFD) is a powerful approach to the theory of relativistic composite systems (hadrons in the quark models and relativistic nucleons in nuclei). Its explicitly covariant version has been recently applied with success to describe the new CEBAF/TJNAF data on the deuteron electromagnetic form factors. The solutions used in were however not obtained from solving exactly the LFD equations but by means of a perturbative calculation with respect to the non relativistic wave function. Since, a consequent effort has been made to obtain exact solutions of LFD equations. The first results concerning J=0 states in a scalar model have been published in nucl-th/9912050. The construction of $J \ne 0$ states in LFD is complicated by the two following facts. First, the generators of the spatial rotations contain interaction and are thus difficult to handle. Second, one is always forced to work in a truncated Fock space, and consequently, the Poincar\'e group commutation relations between the generators -- ensuring the correct properties of the state vector under rotation -- are in practice destroyed. In the standard approach, with the light-front plane defined as $t+z=0$, this violation of rotational invariance manifests by the fact that the energy depends on the angular momentum projection on $z$-axis. We present here a method to construct $J\ne0$ states in the explicitly covariant formulation of LFD and show how it leads to a restoration of rotational invariance., Comment: To appear in Nucl.Phys.B, 3 pages, 2 figures, .tar.gz file
- Published
- 2000
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47. Exact boundary conditions at finite distance for the time-dependent Schrodinger equation
- Author
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Mangin-Brinet, M., Carbonell, J., and Gignoux, C.
- Subjects
Quantum Physics - Abstract
Exact boundary conditions at finite distance for the solutions of the time-dependent Schrodinger equation are derived. A numerical scheme based on Crank-Nicholson method is proposed to illustrate its applicability in several examples., Comment: Latex.tar.gz file, 20 pages, 9 figures
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- 1998
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48. Lattice measurement of [formula omitted] with a realistic charm quark
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Blossier, B., Boucaud, Ph., Brinet, M., De Soto, F., Du, X., Morénas, V., Pène, O., Petrov, K., and Rodríguez-Quintero, J.
- Published
- 2013
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49. Characterization study of silica aerogel for Cherenkov imaging
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Sallaz-Damaz, Y., Derome, L., Mangin-Brinet, M., Loth, M., Protasov, K., Putze, A., Vargas-Trevino, M., Véziant, O., Buénerd, M., Menchaca-Rocha, A., Belmont, E., Vargas-Magaña, M., Léon-Vargas, H., Ortiz-Velàsquez, A., Malinine, A., Baraõ, F., Pereira, R., Bellunato, T., Matteuzzi, C., and Perego, D.L.
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- 2010
- Full Text
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50. Measurement of the top quark-pair production cross section with ATLAS in pp collisions at $\sqrt{s}=7$ TeV
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Aad, G., Abbott, B., Abdallah, J., Abdelalim, A. A., Abdesselam, A., Abdinov, O., Abi, B., Abolins, M., Abramowicz, H., Abreu, H., Acerbi, E., Acharya, B. S., Ackers, M., Adams, D. L., Addy, T. N., Adelman, J., Aderholz, M., Adomeit, S., Adragna, P., Adye, T., Aefsky, S., Aguilar-Saavedra, J. A., Aharrouche, M., Ahlen, S. P., Ahles, F., Ahmad, A., Ahmed, H., Ahsan, M., Aielli, G., Akdogan, T., Åkesson, T. P. A., Akimoto, G., Akimov, A. V., Alam, M. S., Alam, M. A., Albrand, S., Aleksa, M., Aleksandrov, I. N., Aleppo, M., Alessandria, F., Alexa, C., Alexander, G., Alexandre, G., Alexopoulos, T., Alhroob, M., Aliev, M., Alimonti, G., Alison, J., Aliyev, M., Allport, P. P., Allwood-Spiers, S. E., Almond, J., Aloisio, A., Alon, R., Alonso, A., Alonso, J., Alviggi, M. G., Amako, K., Amaral, P., Amelung, C., Ammosov, V. V., Amorim, A., Amorós, G., Amram, N., Anastopoulos, C., Andeen, T., Anders, C. F., Anderson, K. J., Andreazza, A., Andrei, V., Andrieux, M.-L., Anduaga, X. S., Angerami, A., Anghinolfi, F., Anjos, N., Annovi, A., Antonaki, A., Antonelli, M., Antonelli, S., Antos, J., Antunovic, B., Anulli, F., Aoun, S., Aperio Bella, L., Apolle, R., Arabidze, G., Aracena, I., Arai, Y., Arce, A. T. H., Archambault, J. P., Arfaoui, S., Arguin, J.-F., Arik, E., Arik, M., Armbruster, A. J., Arms, K. E., Armstrong, S. R., Arnaez, O., Arnault, C., Artamonov, A., Artoni, G., Arutinov, D., Asai, S., Asfandiyarov, R., Ask, S., Åsman, B., Asquith, L., Assamagan, K., Astbury, A., Astvatsatourov, A., Atoian, G., Aubert, B., Auerbach, B., Auge, E., Augsten, K., Aurousseau, M., Austin, N., Avramidou, R., Axen, D., Ay, C., Azuelos, G., Azuma, Y., Baak, M. A., Baccaglioni, G., Bacci, C., Bach, A. M., Bachacou, H., Bachas, K., Bachy, G., Backes, M., Badescu, E., Bagnaia, P., Bahinipati, S., Bai, Y., Bailey, D. C., Bain, T., Baines, J. T., Baker, O. K., Baker, S., Baltasar Dos Santos Pedrosa, F., Banas, E., Banerjee, P., Banerjee, Sw., Banfi, D., Bangert, A., Bansal, V., Bansil, H. S., Barak, L., Baranov, S. P., Barashkou, A., Barbaro Galtieri, A., Barber, T., Barberio, E. L., Barberis, D., Barbero, M., Bardin, D. Y., Barillari, T., Barisonzi, M., Barklow, T., Barlow, N., Barnett, B. M., Barnett, R. M., Baroncelli, A., Barr, A. J., Barreiro, F., Barreiro Guimar aes da Costa, J., Barrillon, P., Bartoldus, R., Barton, A. E., Bartsch, D., Bates, R. L., Batkova, L., Batley, J. R., Battaglia, A., Battistin, M., Battistoni, G., Bauer, F., Bawa, H. S., Beare, B., Beau, T., Beauchemin, P. H., Beccherle, R., Bechtle, P., Beck, H. P., Beckingham, M., Becks, K. H., Beddall, A. J., Beddall, A., Bednyakov, V. A., Bee, C., Begel, M., Behar Harpaz, S., Behera, P. K., Beimforde, M., Belanger-Champagne, C., Belhorma, B., Bell, P. J., Bell, W. H., Bella, G., Bellagamba, L., Bellina, F., Bellomo, G., Bellomo, M., Belloni, A., Belotskiy, K., Beltramello, O., Ben Ami, S., Benary, O., Benchekroun, D., Benchouk, C., Bendel, M., Benedict, B. H., Benekos, N., Benhammou, Y., Benjamin, D. P., Benoit, M., Bensinger, J. R., Benslama, K., Bentvelsen, S., Berge, D., Bergeaas Kuutmann, E., Berger, N., Berghaus, F., Berglund, E., Beringer, J., Bernardet, K., Bernat, P., Bernhard, R., Bernius, C., Berry, T., Bertin, A., Bertinelli, F., Bertolucci, F., Besana, M. I., Besson, N., Bethke, S., Bhimji, W., Bianchi, R. M., Bianco, M., Biebel, O., Biesiada, J., Biglietti, M., Bilokon, H., Bindi, M., Bingul, A., Bini, C., Biscarat, C., Bischof, R., Bitenc, U., Black, K. M., Blair, R. E., Blanchard, J.-B., Blanchot, G., Blocker, C., Blocki, J., Blondel, A., Blum, W., Blumenschein, U., Boaretto, C., Bobbink, G. J., Bobrovnikov, V. B., Bocci, A., Bock, R., Boddy, C. R., Boehler, M., Boek, J., Boelaert, N., Böser, S., Bogaerts, J. A., Bogdanchikov, A., Bogouch, A., Bohm, C., Boisvert, V., Bold, T., Boldea, V., Boonekamp, M., Boorman, G., Booth, C. N., Booth, P., Booth, J. R. A., Bordoni, S., Borer, C., Borisov, A., Borissov, G., Borjanovic, I., Borroni, S., Bos, K., Boscherini, D., Bosman, M., Boterenbrood, H., Botterill, D., Bouchami, J., Boudreau, J., Bouhova-Thacker, E. V., Boulahouache, C., Bourdarios, C., Bousson, N., Boveia, A., Boyd, J., Boyko, I. R., Bozhko, N. I., Bozovic-Jelisavcic, I., Braccini, S., Bracinik, J., Braem, A., Brambilla, E., Branchini, P., Brandenburg, G. W., Brandt, A., Brandt, G., Brandt, O., Bratzler, U., Brau, B., Brau, J. E., Braun, H. M., Brelier, B., Bremer, J., Brenner, R., Bressler, S., Breton, D., Brett, N. D., Bright-Thomas, P. G., Britton, D., Brochu, F. M., Brock, I., Brock, R., Brodbeck, T. J., Brodet, E., Broggi, F., Bromberg, C., Brooijmans, G., Brooks, W. K., Brown, G., Brubaker, E., Bruckman de Renstrom, P. A., Bruncko, D., Bruneliere, R., Brunet, S., Bruni, A., Bruni, G., Bruschi, M., Buanes, T., Bucci, F., Buchanan, J., Buchanan, N. J., Buchholz, P., Buckingham, R. M., Buckley, A. G., Buda, S. I., Budagov, I. A., Budick, B., Büscher, V., Bugge, L., Buira-Clark, D., Buis, E. J., Bulekov, O., Bunse, M., Buran, T., Burckhart, H., Burdin, S., Burgess, T., Burke, S., Busato, E., Bussey, P., Buszello, C. P., Butin, F., Butler, B., Butler, J. M., Buttar, C. M., Butterworth, J. M., Buttinger, W., Byatt, T., Cabrera Urbán, S., Caccia, M., Caforio, D., Cakir, O., Calafiura, P., Calderini, G., Calfayan, P., Calkins, R., Caloba, L. P., Caloi, R., Calvet, D., Calvet, S., Camard, A., Camarri, P., Cambiaghi, M., Cameron, D., Cammin, J., Campana, S., Campanelli, M., Canale, V., Canelli, F., Canepa, A., Cantero, J., Capasso, L., Capeans Garrido, M. D. M., Caprini, I., Caprini, M., Caprio, M., Capriotti, D., Capua, M., Caputo, R., Caramarcu, C., Cardarelli, R., Carli, T., Carlino, G., Carminati, L., Caron, B., Caron, S., Carpentieri, C., Carrillo Montoya, G. D., Carron Montero, S., Carter, A. A., Carter, J. R., Carvalho, J., Casadei, D., Casado, M. P., Cascella, M., Caso, C., Castaneda Hernandez, A. M., Castaneda-Miranda, E., Castillo Gimenez, V., Castro, N. F., Cataldi, G., Cataneo, F., Catinaccio, A., Catmore, J. R., Cattai, A., Cattani, G., Caughron, S., Cavallari, A., Cavalleri, P., Cavalli, D., Cavalli-Sforza, M., Cavasinni, V., Cazzato, A., Ceradini, F., Cerna, C., Cerqueira, A. S., Cerri, A., Cerrito, L., Cerutti, F., Cervetto, M., Cetin, S. A., Cevenini, F., Chafaq, A., Chakraborty, D., Chan, K., Chapleau, B., Chapman, J. D., Chapman, J. W., Chareyre, E., Charlton, D. G., Chavda, V., Cheatham, S., Chekanov, S., Chekulaev, S. V., Chelkov, G. A., Chen, H., Chen, L., Chen, S., Chen, T., Chen, X., Cheng, S., Cheplakov, A., Chepurnov, V. F., Cherkaoui El Moursli, R., Chernyatin, V., Cheu, E., Cheung, S. L., Chevalier, L., Chevallier, F., Chiefari, G., Chikovani, L., Childers, J. T., Chilingarov, A., Chiodini, G., Chizhov, M. V., Choudalakis, G., Chouridou, S., Christidi, I. A., Christov, A., Chromek-Burckhart, D., Chu, M. L., Chudoba, J., Ciapetti, G., Ciftci, A. K., Ciftci, R., Cinca, D., Cindro, V., Ciobotaru, M. D., Ciocca, C., Ciocio, A., Cirilli, M., Clark, A., Clark, P. J., Cleland, W., Clemens, J. C., Clement, B., Clement, C., Clifft, R. W., Coadou, Y., Cobal, M., Coccaro, A., Cochran, J., Coe, P., Cogan, J. G., Coggeshall, J., Cogneras, E., Cojocaru, C. D., Colas, J., Colijn, A. P., Collard, C., Collins, N. J., Collins-Tooth, C., Collot, J., Colon, G., Coluccia, R., Comune, G., Conde Mui no, P., Coniavitis, E., Conidi, M. C., Consonni, M., Constantinescu, S., Conta, C., Conventi, F., Cook, J., Cooke, M., Cooper, B. D., Cooper-Sarkar, A. M., Cooper-Smith, N. J., Copic, K., Cornelissen, T., Corradi, M., Correard, S., Corriveau, F., Cortes-Gonzalez, A., Cortiana, G., Costa, G., Costa, M. J., Costanzo, D., Costin, T., Côté, D., Coura Torres, R., Courneyea, L., Cowan, G., Cowden, C., Cox, B. E., Cranmer, K., Cristinziani, M., Crosetti, G., Crupi, R., Crépé-Renaudin, S., Cuenca Almenar, C., Cuhadar Donszelmann, T., Cuneo, S., Curatolo, M., Curtis, C. J., Cwetanski, P., Czirr, H., Czyczula, Z., D’Auria, S., D’Onofrio, M., D’Orazio, A., Da Rocha Gesualdi Mello, A., Da Silva, P. V. M., Da Via, C., Dabrowski, W., Dahlhoff, A., Dai, T., Dallapiccola, C., Dallison, S. J., Dam, M., Dameri, M., Damiani, D. S., Danielsson, H. O., Dankers, R., Dannheim, D., Dao, V., Darbo, G., Darlea, G. L., Daum, C., Dauvergne, J. P., Davey, W., Davidek, T., Davidson, N., Davidson, R., Davies, M., Davison, A. R., Dawe, E., Dawson, I., Dawson, J. W., Daya, R. K., De, K., de Asmundis, R., De Castro, S., De Cecco, S., de Graat, J., De Groot, N., de Jong, P., De La Cruz-Burelo, E., De La Taille, C., De Lotto, B., De Mora, L., De Nooij, L., De Oliveira Branco, M., De Pedis, D., de Saintignon, P., De Salvo, A., De Sanctis, U., De Santo, A., De Vivie De Regie, J. B., Dean, S., Dedes, G., Dedovich, D. V., Degenhardt, J., Dehchar, M., Deile, M., Del Papa, C., Del Peso, J., Del Prete, T., Dell’Acqua, A., Dell’Asta, L., Della Pietra, M., della Volpe, D., Delmastro, M., Delpierre, P., Delruelle, N., Delsart, P. A., Deluca, C., Demers, S., Demichev, M., Demirkoz, B., Deng, J., Denisov, S. P., Dennis, C., Derendarz, D., Derkaoui, J. E., Derue, F., Dervan, P., Desch, K., Devetak, E., Deviveiros, P. O., Dewhurst, A., DeWilde, B., Dhaliwal, S., Dhullipudi, R., Di Ciaccio, A., Di Ciaccio, L., Di Girolamo, A., Di Girolamo, B., Di Luise, S., Di Mattia, A., Di Nardo, R., Di Simone, A., Di Sipio, R., Diaz, M. A., Diaz Gomez, M. M., Diblen, F., Diehl, E. B., Dietl, H., Dietrich, J., Dietzsch, T. A., Diglio, S., Dindar Yagci, K., Dingfelder, J., Dionisi, C., Dita, P., Dita, S., Dittus, F., Djama, F., Djilkibaev, R., Djobava, T., do Vale, M. A. B., Do Valle Wemans, A., Doan, T. K. O., Dobbs, M., Dobinson, R., Dobos, D., Dobson, E., Dobson, M., Dodd, J., Dogan, O. B., Doglioni, C., Doherty, T., Doi, Y., Dolejsi, J., Dolenc, I., Dolezal, Z., Dolgoshein, B. A., Dohmae, T., Donadelli, M., Donega, M., Donini, J., Dopke, J., Doria, A., Dos Anjos, A., Dosil, M., Dotti, A., Dova, M. T., Dowell, J. D., Doxiadis, A. D., Doyle, A. T., Drasal, Z., Drees, J., Dressnandt, N., Drevermann, H., Driouichi, C., Dris, M., Drohan, J. G., Dubbert, J., Dubbs, T., Dube, S., Duchovni, E., Duckeck, G., Dudarev, A., Dudziak, F., Dührssen, M., Duerdoth, I. P., Duflot, L., Dufour, M.-A., Dunford, M., Duran Yildiz, H., Duxfield, R., Dwuznik, M., Dydak, F., Dzahini, D., Düren, M., Ebke, J., Eckert, S., Eckweiler, S., Edmonds, K., Edwards, C. A., Efthymiopoulos, I., Ehrenfeld, W., Ehrich, T., Eifert, T., Eigen, G., Einsweiler, K., Eisenhandler, E., Ekelof, T., El Kacimi, M., Ellert, M., Elles, S., Ellinghaus, F., Ellis, K., Ellis, N., Elmsheuser, J., Elsing, M., Ely, R., Emeliyanov, D., Engelmann, R., Engl, A., Epp, B., Eppig, A., Erdmann, J., Ereditato, A., Eriksson, D., Ernst, J., Ernst, M., Ernwein, J., Errede, D., Errede, S., Ertel, E., Escalier, M., Escobar, C., Espinal Curull, X., Esposito, B., Etienne, F., Etienvre, A. I., Etzion, E., Evangelakou, D., Evans, H., Fabbri, L., Fabre, C., Facius, K., Fakhrutdinov, R. M., Falciano, S., Falou, A. C., Fang, Y., Fanti, M., Farbin, A., Farilla, A., Farley, J., Farooque, T., Farrington, S. M., Farthouat, P., Fasching, D., Fassnacht, P., Fassouliotis, D., Fatholahzadeh, B., Fayard, L., Fazio, S., Febbraro, R., Federic, P., Fedin, O. L., Fedorko, I., Fedorko, W., Fehling-Kaschek, M., Feligioni, L., Fellmann, D., Felzmann, C. U., Feng, C., Feng, E. J., Fenyuk, A. B., Ferencei, J., Ferguson, D., Ferland, J., Fernandes, B., Fernando, W., Ferrag, S., Ferrando, J., Ferrara, V., Ferrari, A., Ferrari, P., Ferrari, R., Ferrer, A., Ferrer, M. L., Ferrere, D., Ferretti, C., Ferretto Parodi, A., Ferro, F., Fiascaris, M., Fiedler, F., Filipčič, A., Filippas, A., Filthaut, F., Fincke-Keeler, M., Fiolhais, M. C. N., Fiorini, L., Firan, A., Fischer, G., Fischer, P., Fisher, M. J., Fisher, S. M., Flammer, J., Flechl, M., Fleck, I., Fleckner, J., Fleischmann, P., Fleischmann, S., Flick, T., Flores Castillo, L. R., Flowerdew, M. J., Föhlisch, F., Fokitis, M., Fonseca Martin, T., Forbush, D. A., Formica, A., Forti, A., Fortin, D., Foster, J. M., Fournier, D., Foussat, A., Fowler, A. J., Fowler, K., Fox, H., Francavilla, P., Franchino, S., Francis, D., Frank, T., Franklin, M., Franz, S., Fraternali, M., Fratina, S., French, S. T., Froeschl, R., Froidevaux, D., Frost, J. 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F., Zemla, A., Zendler, C., Zenin, A. V., Zenin, O., Ženiš, T., Zenonos, Z., Zenz, S., Zerwas, D., Zevi della Porta, G., Zhan, Z., Zhang, D., Zhang, H., Zhang, J., Zhang, X., Zhang, Z., Zhao, L., Zhao, T., Zhao, Z., Zhemchugov, A., Zheng, S., Zhong, J., Zhou, B., Zhou, N., Zhou, Y., Zhu, C. G., Zhu, H., Zhu, Y., Zhuang, X., Zhuravlov, V., Zieminska, D., Zilka, B., Zimmermann, R., Zimmermann, S., Zimmermann, S., Ziolkowski, M., Zitoun, R., Živković, L., Zmouchko, V. V., Zobernig, G., Zoccoli, A., Zolnierowski, Y., Zsenei, A., zur Nedden, M., Zutshi, V., Zwalinski, L., and The ATLAS Collaboration
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