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Year of publication
Document Type
- Preprint (820) (remove)
Language
- English (820) (remove)
Has Fulltext
- yes (820) (remove)
Is part of the Bibliography
- no (820)
Keywords
- quark-gluon plasma (3)
- RHIC (2)
- heavy-ion collisions (2)
- natural scenes (2)
- neuronal populations (2)
- primary visual cortex (2)
- stimulus encoding (2)
- visual attention (2)
- Amblyopia (1)
- Antiteilchen (1)
Institute
- Frankfurt Institute for Advanced Studies (FIAS) (820) (remove)
Winckelmann, Luke Andreas ; Bass, Steffen A. ; Bleicher, Marcus ; Brandstetter, Mathias ; Dumitru, Adrian Bogdan ; Ernst, Christoph ; Gerland, Lars ; Konopka, Jens ; Soff, Sven ; Spieles, Christian ; Weber, Henning ; Hartnack, Christoph ; Aichelin, Jörg ; Amelin, Nikolai ; Stöcker, Horst ; Greiner, Walter
The behavior of hadronic matter at high baryon densities is studied within Ultrarelativistic Quantum Molecular Dynamics (URQMD). Baryonic stopping is observed for Au+Au collisions from SIS up to SPS energies. The excitation function of flow shows strong sensitivities to the underlying equation of state (EOS), allowing for systematic studies of the EOS. Effects of a density dependent pole of the rho-meson propagator on dilepton spectra are studied for different systems and centralities at CERN energies.
We introduce a smooth mapping of some discrete space-time symmetries into quasi-continuous ones. Such transformations are related with q-deformations of the dilations of the Euclidean space and with the non-commutative space. We work out two examples of Hamiltonian invariance under such symmetries. The Schrodinger equation for a free particle is investigated in such a non-commutative plane and a connection with anyonic statistics is found. PACS: 03.65.Fd, 11.30.Er
Zschiesche, Detlef ; Bass, Steffen A. ; Bleicher, Marcus ; Brachmann, Jörg ; Gerland, Lars ; Paech, Kerstin ; Scherer, Stefan ; Soff, Sven ; Spieles, Christian ; Weber, Henning ; Stöcker, Horst ; Greiner, Walter
Compelling evidence for the creation of a new form of matter has been claimed to be found in Pb+Pb collisions at SPS. We discuss the uniqueness of often proposed experimental signatures for quark matter formation in relativistic heavy ion collisions. It is demonstrated that so far none of the proposed signals like J/psi meson production/suppression, strangeness enhancement, dileptons, and directed flow unambigiously show that a phase of deconfined matter has been formed in SPS Pb+Pb collisions. We emphasize the need for systematic future measurements to search for simultaneous irregularities in the excitation functions of several observables in order to come close to pinning the properties of hot, dense QCD matter from data.
The wave function of a spheroidal harmonic oscillator without spin-orbit interaction is expressed in terms of associated Laguerre and Hermite polynomials. The pairing gap and Fermi energy are found by solving the BCS system of two equations. Analytical relationships for the matrix elements of inertia are obtained function of the main quantum numbers and potential derivative. They may be used to test complex computer codes one should develop in a realistic approach of the fission dynamics. The results given for the 240 Pu nucleus are compared with a hydrodynamical model. The importance of taking into account the correction term due to the variation of the occupation number is stressed.
Complex fission phenomena
(2004)
Complex fission phenomena are studied in a unified way. Very general reflection asymmetrical equilibrium (saddle point) nuclear shapes are obtained by solving an integro-differential equation without being necessary to specify a certain parametrization. The mass asymmetry in binary cold fission of Th and U isotopes is explained as the result of adding a phenomenological shell correction to the liquid drop model deformation energy. Applications to binary, ternary, and quaternary fission are outlined.
Mishra, Amruta ; Bratkovskaya, Elena L. ; Schaffner-Bielich, Jürgen ; Schramm, Stefan ; Stöcker, Horst
Abstract: The medium modification of kaon and antikaon masses, compatible with low energy KN scattering data, are studied in a chiral SU(3) model. The mutual interactions with baryons in hot hadronic matter and the e ects from the baryonic Dirac sea on the K( ¯K ) masses are examined. The in-medium masses from the chiral SU(3) e ective model are compared to those from chiral perturbation theory. Furthermore, the influence of these in-medium e ects on kaon rapidity distributions and transverse energy spectra as well as the K, ¯K flow pattern in heavy-ion collision experiments at 1.5 to 2 A·GeV are investigated within the HSD transport approach. Detailed predictions on the transverse momentum and rapidity dependence of directed flow v1 and the elliptic flow v2 are provided for Ni+Ni at 1.93 A·GeV within the various models, that can be used to determine the in-medium K± properties from the experimental side in the near future.
Antibaryons bound in nuclei
(2004)
We study the possibility of producing a new kind of nuclear systems which in addition to ordinary nucleons contain a few antibaryons (B = p, , etc.). The properties of such systems are described within the relativistic mean field model by employing G parity transformed interactions for antibaryons. Calculations are first done for infinite systems and then for finite nuclei from 4He to 208Pb. It is demonstrated that the presence of a real antibaryon leads to a strong rearrangement of a target nucleus resulting in a significant increase of its binding energy and local compression. Noticeable e ects remain even after the antibaryon coupling constants are reduced by factor 3 4 compared to G parity motivated values. We have performed detailed calculations of the antibaryon annihilation rates in the nuclear environment by applying a kinetic approach. It is shown that due to significant reduction of the reaction Q values, the in medium annihilation rates should be strongly suppressed leading to relatively long lived antibaryon nucleus systems. Multi nucleon annihilation channels are analyzed too. We have also estimated formation probabilities of bound B + A systems in pA reactions and have found that their observation will be feasible at the future GSI antiproton facility. Several observable signatures are proposed. The possibility of producing multi quark antiquark clusters is discussed. PACS numbers: 25.43.+t, 21.10.-k, 21.30.Fe, 21.80.+a
To be published in J. Phys. G - Proceedings of SQM 2004 : We review the results from the various hydrodynamical and transport models on the collective flow observables from AGS to RHIC energies. A critical discussion of the present status of the CERN experiments on hadron collective flow is given. We emphasize the importance of the flow excitation function from 1 to 50 A.GeV: here the hydrodynamic model has predicted the collapse of the v2-flow ~ 10 A.GeV; at 40 A.GeV it has been recently observed by the NA49 collaboration. Since hadronic rescattering models predict much larger flow than observed at this energy we interpret this observation as evidence for a first order phase transition at high baryon density r b. Moreover, the connection of the elliptic flow v2 to jet suppression is examined. It is proven experimentally that the collective flow is not faked by minijet fragmentation. Additionally, detailed transport studies show that the away-side jet suppression can only partially (< 50%) be due to hadronic rescattering. Furthermore, the change in sign of v1, v2 closer to beam rapidity is related to the occurence of a high density first order phase transition in the RHIC data at 62.5, 130 and 200 A.GeV.
We investigate the effects of strong color fields and of the associated enhanced intrinsic transverse momenta on the phi-meson production in ultrarelativistic heavy ion collisions at RHIC. The observed consequences include a change of the spectral slopes, varying particle ratios, and also modified mean transverse momenta. In particular, the composition of the production processes of phi-mesons, that is, direct production vs. coalescence-like production, depends strongly on the strength of the color fields and intrinsic transverse momenta and thus represents a sensitive probe for their measurement.
A critical discussion of the present status of the CERN experiments on charm dynamics and hadron collective flow is given. We emphasize the importance of the flow excitation function from 1 to 50 A·GeV: here the hydrodynamic model has predicted the collapse of the v1-flow and of the v2-flow at 10 A·GeV; at 40 A·GeV it has been recently observed by the NA49 collaboration. Since hadronic rescattering models predict much larger flow than observed at this energy we interpret this observation as potential evidence for a first order phase transition at high baryon density B. A detailed discussion of the collective flow as a barometer for the equation of state (EoS) of hot dense matter at RHIC follows. Here, hadronic rescattering models can explain < 30% of the observed elliptic flow, v2, for pT > 2 GeV/c. This is interpreted as evidence for the production of superdense matter at RHIC with initial pressure far above hadronic pressure, p > 1 GeV/fm3. We suggest that the fluctuations in the flow, v1 and v2, should be measured in future since ideal hydrodynamics predicts that they are larger than 50 % due to initial state fluctuations. Furthermore, the QGP coe cient of viscosity may be determined experimentally from the fluctuations observed. The connection of v2 to jet suppression is examined. It is proven experimentally that the collective flow is not faked by minijet fragmentation. Additionally, detailed transport studies show that the awayside jet suppression can only partially (< 50%) be due to hadronic rescattering. We, finally, propose upgrades and second generation experiments at RHIC which inspect the first order phase transition in the fragmentation region, i.e. at µB 400 MeV (y 4 5), where the collapse of the proton flow should be seen in analogy to the 40 A·GeV data. The study of Jet-Wake-riding potentials and Bow shocks caused by jets in the QGP formed at RHIC can give further information on the equation of state (EoS) and transport coe cients of the Quark Gluon Plasma (QGP).
String theory suggests modifications of our spacetime such as extra dimensions and the existence of a mininal length scale. In models with addidional dimensions, the Planck scale can be lowered to values accessible by future colliders. Effective theories which extend beyond the standart-model by including extra dimensions and a minimal length allow computation of observables and can be used to make testable predictions. Expected effects that arise within these models are the production of gravitons and black holes. Furthermore, the Planck-length is a lower bound to the possible resolution of spacetime which might be reached soon.
Greiner, Carsten ; Koch-Steinheimer, Peter ; Liu, Fu-Ming ; Šovkovyj, Ihor Andrijovyč ; Stöcker, Horst
A scenario of heavy resonances, called massive Hagedorn states, is proposed which exhibits a fast (t H 1 fm/c) chemical equilibration of (strange) baryons and anti-baryons at the QCD critical temperature Tc. For relativistic heavy ion collisions this scenario predicts that hadronization is followed by a brief expansion phase during which the equilibration rate is higher than the expansion rate, so that baryons and antibaryons reach chemical equilibrium before chemical freeze-out occurs. PACS-Nr.: 12.38.Mh
We study the phase diagram of a generalized chiral SU(3)-flavor model in mean-field approxi- mation. In particular, the influence of the baryon resonances, and their couplings to the scalar and vector fields, on the characteristics of the chiral phase transition as a function of temperature and baryon-chemical potential is investigated. Present and future finite-density lattice calculations might constrain the couplings of the fields to the baryons. The results are compared to recent lattice QCD calculations and it is shown that it is non-trivial to obtain, simultaneously, stable cold nuclear matter.
Bratkovskaya, Elena L. ; Bleicher, Marcus ; Dumitru, Adrian Bogdan ; Paech, Kerstin ; Reiter, Manuel ; Soff, Sven ; Stöcker, Horst ; Weber, Henning ; Leeuwen, Marco van ; Cassing, Wolfgang
We investigate hadron production and transverse hadron spectra in nucleus-nucleus collisions from 2 A·GeV to 21.3 A·TeV within two independent transport approaches (UrQMD and HSD) based on quark, diquark, string and hadronic degrees of freedom. The enhancement of pion production in central Au+Au (Pb+Pb) collisions relative to scaled pp collisions (the ’kink’) is described well by both approaches without involving a phase transition. However, the maximum in the K+ p+ ratio at 20 to 30 A·GeV (the ’horn’) is missed by ~ 40%. Also, at energies above ~5 A·GeV, the measured K± mT-spectra have a larger inverse slope than expected from the models. Thus the pressure generated by hadronic interactions in the transport models at high energies is too low. This finding suggests that the additional pressure - as expected from lattice QCD at finite quark chemical potential and temperature - might be generated by strong interactions in the early pre-hadronic/partonic phase of central heavy-ion collisions. Finally, we discuss the emergence of density perturbations in a first-order phase transition and why they might affect relative hadron multiplicities, collective flow, and hadron mean-free paths at decoupling. A minimum in the collective flow v2 excitation function was discovered experimentally at 40 A·GeV - such a behavior has been predicted long ago as signature for a first order phase transition.
We discuss modifications of the gyromagnetic moment of electrons and muons due to a minimal length scale combined with a modified fundamental scaleMf . First-order deviations from the theoretical standard model value for g-2 due to these String Theory-motivated e ects are derived. Constraints for the new fundamental scale Mf are given.
Potential energy surfaces are calculated by using the most advanced asymmetric two-center shell model allowing to obtain shell and pairing corrections which are added to the Yukawa-plus-exponential model deformation energy. Shell effects are of crucial importance for experimental observation of spontaneous disintegration by heavy ion emission. Results for 222Ra, 232U, 236Pu and 242Cm illustrate the main ideas and show for the first time for a cluster emitter a potential barrier obtained by using the macroscopic-microscopic method.
The D-meson spectral density at finite temperature is obtained within a self-consistent coupled-channel approach. For the bare meson-baryon interaction, a separable potential is taken, whose parameters are fixed by the position and width of the Lambda_c (2593) resonance. The quasiparticle peak stays close to the free D-meson mass, indicating a small change in the effective mass for finite density and temperature. However, the considerable width of the spectral density implies physics beyond the quasiparticle approach. Our results indicate that the medium modifications for the D-mesons in nucleus-nucleus collisions at FAIR (GSI) will be dominantly on the width and not, as previously expected, on the mass.
Wei, F.X. ; Mao, Guangjun ; Ko, Che Ming ; Kisslinger, Leonard S. ; Stöcker, Horst ; Greiner, Walter
We study the effects of isovector-scalar meson delta on the equation of state (EOS) of neutron star matter in strong magnetic fields. The EOS of neutron-star matter and nucleon effective masses are calculated in the framework of Lagrangian field theory, which is solved within the mean-field approximation. From the numerical results one can find that the delta-field leads to a remarkable splitting of proton and neutron effective masses. The strength of delta-field decreases with the increasing of the magnetic field and is little at ultrastrong field. The proton effective mass is highly influenced by magnetic fields, while the effect of magnetic fields on the neutron effective mass is negligible. The EOS turns out to be stiffer at B < 10^15G but becomes softer at stronger magnetic field after including the delta-field. The AMM terms can affect the system merely at ultrastrong magnetic field(B > 10^19G). In the range of 10^15 G - 10^18 G the properties of neutron-star matter are found to be similar with those without magnetic fields.
We study Mach shocks generated by fast partonic jets propagating through a deconfined strongly-interacting matter. Our main goal is to take into account different types of collective motion during the formation and evolution of this matter. We predict a significant deformation of Mach shocks in central Au+Au collisions at RHIC and LHC energies as compared to the case of jet propagation in a static medium. The observed broadening of the near-side two-particle correlations in pseudorapidity space is explained by the Bjorken-like longitudinal expansion. Three-particle correlation measurements are proposed for a more detailed study of the Mach shock waves.
Nuclear collisions at intermediate, relativistic, and ultra-relativistic energies offer unique opportunities to study in detail manifold fragmentation and clustering phenomena in dense nuclear matter. At intermediate energies, the well known processes of nuclear multifragmentation -- the disintegration of bulk nuclear matter in clusters of a wide range of sizes and masses -- allow the study of the critical point of the equation of state of nuclear matter. At very high energies, ultra-relativistic heavy-ion collisions offer a glimpse at the substructure of hadronic matter by crossing the phase boundary to the quark-gluon plasma. The hadronization of the quark-gluon plasma created in the fireball of a ultra-relativistic heavy-ion collision can be considered, again, as a clustering process. We will present two models which allow the simulation of nuclear multifragmentation and the hadronization via the formation of clusters in an interacting gas of quarks, and will discuss the importance of clustering to our understanding of hadronization in ultra-relativistic heavy-ion collisions.
The recently proposed baryon-strangeness correlation (C_BS) is studied with a string-hadronic transport model (UrQMD) for various energies from E_lab=4 AGeV to \sqrt s=200 AGeV. It is shown that rescattering among secondaries can not mimic the predicted correlation pattern expected for a Quark-Gluon-Plasma. However, we find a strong increase of the C_BS correlation function with decreasing collision energy both for pp and Au+Au/Pb+Pb reactions. For Au+Au reactions at the top RHIC energy (\sqrt s=200 AGeV), the C_BS correlation is constant for all centralities and compatible with the pp result. With increasing width of the rapidity window, C_BS follows roughly the shape of the baryon rapidity distribution. We suggest to study the energy and centrality dependence of C_BS which allow to gain information on the onset of the deconfinement transition in temperature and volume.
The cumulant method is applied to study elliptic flow (v_2) in Au+Au collisions at sqrt s=200 AGeV, with the UrQMD model. In this approach, the true event plane is known and both the non-flow effects and event-by-event spatial (epsilon) and v_2 fluctuations exist. Qualitatively, the hierarchy of v_2 's from two, four and six-particle cumulants is consistent with the STAR data, however, the magnitude of v_2 in the UrQMD model is only 60% of the data. We find that the four and six-particle cumulants are good measures of the real elliptic flow over a wide range of centralities except for the most central and very peripheral events. There the cumulant method is affected by the v_2 fluctuations. In mid-central collisions, the four and six-particle cumulants are shown to give a good estimation of the true differential v_2, especially at large transverse momentum, where the two-particle cumulant method is heavily affected by the non-flow effects.
Phase diagram of strongly interacting matter is discussed within the exactly solvable statistical model of the quark-gluon bags. The model predicts two phases of matter: the hadron gas at a low temperature T and baryonic chemical potential muB, and the quark-gluon gas at a high T and/or muB. The nature of the phase transition depends on a form of the bag mass-volume spectrum (its pre-exponential factor), which is expected to change with the muB/T ratio. It is therefore likely that the line of the 1st} order transition at a high muB/T ratio is followed by the line of the 2nd order phase transition at an intermediate muB/T, and then by the lines of "higher order transitions" at a low muB/T.
Konchakovski, Volodymyr P. ; Haussler, Stéphane ; Gorenstein, Mark I. ; Bratkovskaya, Elena L. ; Bleicher, Marcus ; Stöcker, Horst
Event-by-event multiplicity fluctuations in nucleus-nucleus collisions are studied within the HSD and UrQMD transport models. The scaled variances of negative, positive, and all charged hadrons in Pb+Pb at 158 AGeV are analyzed in comparison to the data from the NA49 Collaboration. We find a dominant role of the fluctuations in the nucleon participant number for the final hadron multiplicity fluctuations. This fact can be used to check di erent scenarios of nucleus-nucleus collisions by measuring the final multiplicity fluctuations as a function of collision centrality. The analysis reveals surprising e ects in the recent NA49 data which indicate a rather strong mixing of the projectile and target hadron production sources even in peripheral collisions. PACS numbers: 25.75.-q,25.75.Gz,24.60.-k
Probing the density dependence of the symmetry potential in intermediate energy heavy ion collisions
(2005)
Based on the ultrarelativistic quantum molecular dynamics (UrQMD) model, the effects of the density-dependent symmetry potential for baryons and of the Coulomb potential for produced mesons are investigated for neutron-rich heavy ion collisions at intermediate energies. The calculated results of the Delta-/Delta++ and pi -/pi + production ratios show a clear beam-energy dependence on the density-dependent symmetry potential, which is stronger for the pi -/pi + ratio close to the pion production threshold. The Coulomb potential of the mesons changes the transverse momentum distribution of the pi -/pi + ratio significantly, though it alters only slightly the pi- and pi+ total yields. The pi- yields, especially at midrapidity or at low transverse momenta and the p-/pi+ ratios at low transverse momenta, are shown to be sensitive probes of the density-dependent symmetry potential in dense nuclear matter. The effect of the density-dependent symmetry potential on the production of both, K0 and K+ mesons, is also investigated.
The influence of the isospin-independent, isospin- and momentum-dependent equation of state (EoS), as well as the Coulomb interaction on the pion production in intermediate energy heavy ion collisions (HICs) is studied for both isospin-symmetric and neutron-rich systems. The Coulomb interaction plays an important role in the reaction dynamics, and strongly influences the rapidity and transverse momentum distributions of charged pions. It even leads to the pi- pi+ ratio deviating slightly from unity for isospin-symmetric systems. The Coulomb interaction between mesons and baryons is also crucial for reproducing the proper pion flow since it changes the behavior of the directed and the elliptic flow components of pions visibly. The EoS can be better investigated in neutron-rich system if multiple probes are measured simultaneously. For example, the rapidity and the transverse momentum distributions of the charged pions, the pi- pi+ ratio, the various pion flow components, as well as the difference of pi+-pi- flows. A new sensitive observable is proposed to probe the symmetry potential energy at high densities, namely the transverse momentum distribution of the elliptic flow difference [Delta v_2^pi+ - pi-(p_t rm c.m.].
We investigate the sensitivity of several observables to the density dependence of the symmetry potential within the microscopic transport model UrQMD (ultrarelativistic quantum molecular dynamics model). The same systems are used to probe the symmetry potential at both low and high densities. The influence of the symmetry potentials on the yields of pi-, pi+, the pi-/pi+ ratio, the n/p ratio of free nucleons and the t/3He ratio are studied for neutron-rich heavy ion collisions (208Pb+208Pb, 132Sn+124Sn, 96Zr+96Zr) at E_b=0.4A GeV. We find that these multiple probes provides comprehensive information on the density dependence of the symmetry potential.
The study of hidden charm production is an important part of the heavy ion program. The standard approach to this problem [1] assumes that c¯c bound states are created only at the initial stage of the reaction and then partially destroyed at later stages due to interactions with the medium [2, 3, 4].
Charmonium production and suppression in heavy-ion collisions at relativistic energies is investigated within di erent models, i.e. the comover absorption model, the threshold suppression model, the statistical coalescence model and the HSD transport approach. In HSD the charmonium dissociation cross sections with mesons are described by a simple phase-space parametrization including an e ective coupling strength |Mi|2 for the charmonium states i =Xc,J/psi, psi'. This allows to include the backward channels for charmonium reproduction by DD channels which are missed in the comover absorption and threshold suppression model employing detailed balance without introducing any new parameters. It is found that all approaches yield a reasonable description of J/psi suppression in S+U and Pb+Pb collisions at SPS energies. However, they di er significantly in the psi'/J/psi ratio versus centrality at SPS and especially at RHIC energies. These pronounced differences can be exploited in future measurements at RHIC to distinguish the hadronic rescattering scenarios from quark coalescence close to the QGP phase boundary.
Results from various theoretical approaches and ideas presented at this exciting meeting (summary talk at the 5th International Conference on Physics and Astrophysics of Quark Gluon Plasma (ICPAQGP - 2005)) are reviewed. I also point towards future directions, in particular hydrodynamic behaviour induced by jets traveling through the quark-gluon plasma, which might be worth looking at in more detail.
Dumitru, Adrian Bogdan ; Katscher, Ulrich ; Maruhn, Joachim ; Stöcker, Horst ; Greiner, Walter ; Rischke, Dirk-Hermann
We calculate thermal photon and neutral pion spectra in ultrarelativistic heavy-ion collisions in the framework of three-fluid hydrodynamics. Both spectra are quite sensitive to the equation of state used. In particular, within our model, recent data for S + Au at 200 AGeV can only be understood if a scenario with a phase transition (possibly to a quark-gluon plasma) is assumed. Results for Au+Au at 11 AGeV and Pb + Pb at 160 AGeV are also presented.
We obtain the D-meson spectral density at finite temperature for the conditions of density and temperature expected at FAIR. We perform a self-consistent coupled-channel calculation taking, as a bare interaction, a separable potential model. The Lambda_c (2593) resonance is generated dynamically. We observe that the D-meson spectral density develops a sizeable width while the quasiparticle peak stays close to the free position. The consequences for the D-meson production at FAIR are discussed.
Event-by-event fluctuations of the net baryon number and electric charge in nucleus-nucleus collisions are studied in Pb+Pb at SPS energies within the HSD transport model. We reveal an important role of the fluctuations in the number of target nucleon participants. They strongly influence all measured fluctuations even in the samples of events with rather rigid centrality trigger. This fact can be used to check different scenarios of nucleus-nucleus collisions by measuring the multiplicity fluctuations as a function of collision centrality in fixed kinematical regions of the projectile and target hemispheres. The HSD results for the event-by-event fluctuations of electric charge in central Pb+Pb collisions at 20, 30, 40, 80 and 158 A GeV are in a good agreement with the NA49 experimental data and considerably larger than expected in a quark-gluon plasma. This demonstrate that the distortions of the initial fluctuations by the hadronization phase and, in particular, by the final resonance decays dominate the observable fluctuations.
We develop a 1+1 dimensional hydrodynamical model for central heavy-ion collisions at ultrarelativistic energies. Deviations from Bjorken's scaling are taken into account by implementing finite-size profiles for the initial energy density. The calculated rapidity distributions of pions, kaons and antiprotons in central Au+Au collisions at the c.m. energy 200 AGeV are compared with experimental data of the BRAHMS Collaboration. The sensitivity of the results to the choice of the equation of state, the parameters of initial state and the freeze-out conditions is investigated. The best fit of experimental data is obtained for a soft equation of state and Gaussian-like initial profiles of the energy density.
The concept of Large Extra Dimensions (LED) provides a way of solving the Hierarchy Problem which concerns the weakness of gravity compared with the strong and electro-weak forces. A consequence of LED is that miniature Black Holes (mini-BHs) may be produced at the Large Hadron Collider in p+p collisions. The present work uses the CHARYBDIS mini-BH generator code to simulate the hadronic signal which might be expected in a mid-rapidity particle tracking detector from the decay of these exotic objects if indeed they are produced. An estimate is also given for Pb+Pb collisions.
The experimental signatures of TeV-mass black hole (BH) formation in heavy ion collisions at the LHC is examined. We find that the black hole production results in a complete disappearance of all very high p_T (> 500 GeV) back-to-back correlated di-jets of total mass M > M_f ~ 1 TeV. We show that the subsequent Hawking-decay produces multiple hard mono-jets and discuss their detection. We study the possibility of cold black hole remnant (BHR) formation of mass ~ M_f and the experimental distinguishability of scenarios with BHRs and those with complete black hole decay. Due to the rather moderate luminosity in the first year of LHC running the least chance for the observation of BHs or BHRs at this early stage will be by ionizing tracks in the ALICE TPC. Finally we point out that stable BHRs would be interesting candidates for energy production by conversion of mass to Hawking radiation.
Schweda, Kai ; Zhu, Xianglei ; Bleicher, Marcus ; Huang, Shengli ; Stöcker, Horst ; Xu, Nu ; Zhuang, Pengfei
We propose to measure azimuthal correlations of heavy-flavor hadrons to address the status of thermalization at the partonic stage of light quarks and gluons in high-energy nuclear collisions. In particular, we show that hadronic interactions at the late stage cannot significantly disturb the initial back-to-back azimuthal correlations of DDbar pairs. Thus, a decrease or the complete absence of these initial correlations does indicate frequent interactions of heavy-flavor quarks and also light partons in the partonic stage, which are essential for the early thermalization of light partons.
Betz, Barbara ; Bleicher, Marcus ; Harbach, Ulrich ; Humanic, Thomas J. ; Koch, Benjamin ; Stöcker, Horst
We examine experimental signatures of TeV-mass black hole formation in heavy ion collisions at the LHC. We find that the black hole production results in a complete disappearance of all very high p_T (> 500 GeV) back-to-back correlated di-jets of total mass M > M_f ~ 1 TeV. We show that the subsequent Hawking-decay produces multiple hard mono-jets and discuss their detection. We study the possibility of cold black hole remnant (BHR) formation of mass ~ M_f and the experimental distinguishability of scenarios with BHRs and those with complete black hole decay. Finally we point out that a Heckler-Kapusta-Hawking plasma may form from the emitted mono-jets. In this context we present new simulation data of Mach shocks and of the evolution of initial conditions until the freeze-out.
The production of Large Extra Dimension (LXD) Black Holes (BHs), with a new, fundamental mass scale of M_f = 1 TeV, has been predicted to occur at the Large Hadron Collider, LHC, with the formidable rate of 10^8 per year in p-p collisions at full energy, 14 TeV, and at full luminosity. We show that such LXD-BH formation will be experimentally observable at the LHC by the complete disappearance of all very high p_t (> 500 GeV) back-to-back correlated Di-Jets of total mass M > M_f = 1 TeV. We suggest to complement this clear cut-off signal at M > 2*500 GeV in the di-jet-correlation function by detecting the subsequent, Hawking-decay products of the LXD-BHs, namely either multiple high energy (> 100 GeV) SM Mono-Jets (i.e. away-side jet missing), sprayed off the evaporating BHs isentropically into all directions or the thermalization of the multiple overlapping Hawking-radiation in a eckler-Kapusta-Plasma. Microcanonical quantum statistical calculations of the Hawking evaporation process for these LXD-BHs show that cold black hole remnants (BHRs) of Mass sim M_f remain leftover as the ashes of these spectacular Di-Jet-suppressed events. Strong Di-Jet suppression is also expected with Heavy Ion beams at the LHC, due to Quark-Gluon-Plasma induced jet attenuation at medium to low jet energies, p_t < 200 GeV. The (Mono-)Jets in these events can be used to trigger for Tsunami-emission of secondary compressed QCD-matter at well defined Mach-angles, both at the trigger side and at the awayside (missing) jet. The Machshock-angles allow for a direct measurement of both the equation of state EoS and the speed of sound c_s via supersonic bang in the "big bang" matter. We discuss the importance of the underlying strong collective flow - the gluon storm - of the QCD- matter for the formation and evolution of these Machshock cones. We predict a significant deformation of Mach shocks from the gluon storm in central Au+Au collisions at RHIC and LHC energies, as compared to the case of weakly coupled jets propagating through a static medium. A possible complete stopping of pt > 50 GeV jets at the LHC in 2-3 fm yields nonlinear high density Mach shocks in he quark gluon plasma, which can be studied in the complex emission and disintegration pattern of the possibly supercooled matter. We report on first full 3-dimensional fluid dynamical studies of the strong effects of a first order phase transition on the evolution and the Tsunami-like Mach shock emission of the QCD matter.
We have calculated the D-meson spectral density at finite temperature within a self-consistent coupled-channel approach that generates dynamically the Lambda_c (2593) resonance. We find a small mass shift for the D-meson in this hot and dense medium while the spectral density develops a sizeable width. The reduced attraction felt by the D-meson in hot and dense matter together with the large width observed have important consequences for the D-meson production in the future CBM experiment at FAIR.
The rapidity dependence of the single- and double- neutron to proton ratios of nucleon emission from isospin-asymmetric but mass-symmetric reactions Zr+Ru and Ru+Zr at energy range 100 ~ 800 A MeV and impact parameter range 0 ~ 8 fm is investigated. The reaction system with isospin-asymmetry and mass-symmetry has the advantage of simultaneously showing up the dependence on the symmetry energy and the degree of the isospin equilibrium. We find that the beam energy- and the impact parameter dependence of the slope parameter of the double neutron to proton ratio (F_D) as function of rapidity are quite sensitive to the density dependence of symmetry energy, especially at energies E_b ~ 400 A MeV and reduced impact parameters around 0.5. Here the symmetry energy effect on the F_D is enhanced, as compared to the single neutron to proton ratio. The degree of the equilibrium with respect to isospin (isospin mixing) in terms of the F_D is addressed and its dependence on the symmetry energy is also discussed.
Zhu, Xianglei ; Bleicher, Marcus ; Huang, Shengli ; Schweda, Kai ; Stöcker, Horst ; Wöhri, Hermine K. ; Xu, Nu ; Zhuang, Pengfei
We propose to measure correlations of heavy-flavor hadrons to address the status of thermalization at the partonic stage of light quarks and gluons in high-energy nuclear collisions, shown on the example of azimuthal correlations of D-Dbar pairs. We show that hadronic interactions at the late stage can not disturb these correlations significantly. Thus, a decrease or the complete absence of these initial correlations indicates frequent interactions of heavy-flavor quarks in the partonic stage. Therefore, early thermalization of light quarks is likely to be reached. PACS numbers: 25.75.-q
Elliptic flow analysis at RHIC with the Lee-Yang Zeroes method in a relativistic transport approach
(2006)
The Lee-Yang zeroes method is applied to study elliptic flow (v_2) in Au+Au collisions at sqrt s =200 A GeV, with the UrQMD model. In this transport approach, the true event plane is known and both the nonflow effects and event-by-event v_2 fluctuations exist. Although the low resolutions prohibit the application of the method for most central and peripheral collisions, the integral and differential elliptic flow from the Lee-Yang zeroes method agrees with the exact v_2 values very well for semi-central collisions.
Several observables of unbound nucleons which are to some extent sensitive to the medium modifications of nucleon-nucleon elastic cross sections in neutron-rich intermediate energy heavy ion collisions are investigated. The splitting effect of neutron and proton effective masses on cross sections is discussed. It is found that the transverse flow as a function of rapidity, the Q_zz as a function of momentum, and the ratio of halfwidths of the transverse to that of longitudinal rapidity distribution R_t/l are very sensitive to the medium modifications of the cross sections. The transverse momentum distribution of correlation functions of two-nucleons does not yield information on the in-medium cross section.
The pion source as seen through HBT correlations at RHIC energies is investigated within the UrQMD approach. We find that the calculated transverse momentum, centrality, and system size dependence of the Pratt-HBT radii R_L and R_S are reasonably well in line with experimental data. The predicted R_O values in central heavy ion collisions are larger as compared to experimental data. The corresponding quantity sqrt R_O^2-R_S^2 of the pion emission source is somewhat larger than experimental estimates.
Lu, Yang ; Bleicher, Marcus ; Liu, Fuming ; Liu, Zuhua ; Sorensen, Paul ; Stöcker, Horst ; Xu, Nu ; Zhu, Xianglei
The transverse momentum dependence of the anisotropic flow v_2 for pi, K, nucleon, Lambda, Xi and Omega is studied for Au+Au collisions at sqrt s_NN = 200 GeV within two independent string-hadron transport approaches (RQMD and UrQMD). Although both models reach only 60% of the absolute magnitude of the measured v_2, they both predict the particle type dependence of v_2, as observed by the RHIC experiments: v_2 exhibits a hadron-mass hierarchy (HMH) in the low p_T region and a number-of-constituent-quark (NCQ) dependence in the intermediate p_T region. The failure of the hadronic models to reproduce the absolute magnitude of the observed v_2 indicates that transport calculations of heavy ion collisions at RHIC must incorporate interactions among quarks and gluons in the early, hot and dense phase. The presence of an NCQ scaling in the string-hadron model results suggests that the particle-type dependencies observed in heavy-ion collisions at intermediate p_T are related to the hadronic cross sections in vacuum rather than to the hadronization process itself, as suggested by quark recombination models.
Abelev, Betty ; Adam, Jaroslav ; Adamová, Dagmar ; Aggarwal, Madan Mohan ; Aglieri Rinella, Gianluca ; Agnello, Michelangelo ; Agostinelli, Andrea ; Agrawal, Neelima ; Ahammed, Zubayer ; Ahmad, Nazeer ; Ahmed, Ijaz ; Ahn, Sang Un ; Ahn, Sul-Ah ; Aimo, Ilaria ; Aiola, Salvatore ; Ajaz, Muhammad ; Akindinov, Alexander ; Alam, Sk Noor ; Aleksandrov, Dmitry ; Alessandro, Bruno ; Alexandre, Didier ; Alici, Andrea ; Alkin, Anton ; Alme, Johan ; Alt, Torsten ; Altinpinar, Sedat ; Altsybeev, Igor ; Prado, Caio Alves Garcia ; Andrei, Cristian ; Andronic, Anton ; Anguelov, Venelin ; Anielski, Jonas ; Antičić, Tome ; Antinori, Federico ; Antonioli, Pietro ; Aphecetche, Laurent Bernard ; Appelshäuser, Harald ; Arcelli, Silvia ; Armesto Perez, Nestor ; Arnaldi, Roberta ; Aronsson, Tomas ; Arsene, Ionut Cristian ; Arslandok, Mesut ; Augustinus, Andre ; Averbeck, Ralf Peter ; Awes, Terry ; Azmi, Mohd Danish ; Bach, Matthias ; Badalà, Angela ; Baek, Yong Wook ; Bagnasco, Stefano ; Bailhache, Raphaëlle ; Bala, Renu ; Baldisseri, Alberto ; Baltasar Dos Santos Pedrosa, Fernando ; Baral, Rama Chandra ; Barbera, Roberto ; Barile, Francesco ; Barnaföldi, Gergely Gábor ; Barnby, Lee Stuart ; Ramillien Barret, Valerie ; Bartke, Jerzy ; Basile, Maurizio ; Bastid, Nicole ; Basu, Sumit ; Bathen, Bastian ; Batigne, Guillaume ; Batista Camejo, Arianna ; Batyunya, Boris ; Bätzing, Paul Christoph ; Baumann, Christoph Heinrich ; Bearden, Ian Gardner ; Beck, Hans ; Bedda, Cristina ; Behera, Nirbhay Kumar ; Belikov, Iouri ; Bellini, Francesca ; Bellwied, Rene ; Belmont Moreno, Ernesto ; Belmont Iii, Ronald John ; Belyaev, Vladimir ; Bencédi, Gyula ; Beolè, Stefania ; Berceanu, Ionela ; Bercuci, Alexandru ; Berdnikov, Yaroslav ; Berényi, Dániel ; Berger, Martin Emanuel ; Bertens, Redmer Alexander ; Berzano, Dario ; Betev, Latchezar ; Bhasin, Anju ; Bhat, Inayat Rasool ; Bhati, Ashok Kumar ; Bhattacharjee, Buddhadeb ; Bhom, Jihyun ; Bianchi, Livio ; Bianchi, Nicola ; Bianchin, Chiara ; Bielčík, Jaroslav ; Bielčíková, Jana ; Bilandzic, Ante ; Bjelogrlic, Sandro ; Blanco, Fernando ; Blau, Dmitry S. ; Blume, Christoph ; Bock, Friederike ; Bogdanov, Alexey A. ; Bøggild, Hans ; Bogolyubskiy, Mikhail ; Boehmer, Felix Valentin ; Boldizsar, Laszlo ; Bombara, Marek ; Book, Julian ; Borel, Herve ; Borissov, Alexander ; Borri, Marcello ; Bossú, Francesco ; Botje, Michiel ; Botta, Elena ; Boettger, Stefan ; Braun-Munzinger, Peter ; Bregant, Marco ; Breitner, Timo ; Broker, Theo Alexander ; Browning, Tyler Allen ; Broz, Michal ; Bruna, Elena ; Bruno, Giuseppe Eugenio ; Budnikov, Dmitry ; Büsching, Henner ; Bufalino, Stefania ; Bunčić, Predrag ; Busch, Oliver ; Buthelezi, Edith Zinhle ; Caffarri, Davide ; Cai, Xu ; Caines, Helen Louise ; Calero Diaz, Liliet ; Caliva, Alberto ; Calvo Villar, Ernesto ; Camerini, Paolo ; Carena, Francesco ; Carena, Wisla ; Castillo Castellanos, Javier Ernesto ; Castro, Andrew John ; Casula, Ester Anna Rita ; Catanescu, Vasile Ioan ; Cavicchioli, Costanza ; Ceballos Sanchez, Cesar ; Čepila, Jan ; Cerello, Piergiorgio ; Chang, Beomsu ; Chapeland, Sylvain ; Charvet, Jean-Luc Fernand ; Chattopadhyay, Subhasis ; Chattopadhyay, Sukalyan ; Chelnokov, Volodymyr ; Cherney, Michael Gerard ; Cheshkov, Cvetan Valeriev ; Cheynis, Brigitte ; Chibante Barroso, Vasco Miguel ; Chinellato, David Dobrigkeit ; Chochula, Peter ; Chojnacki, Marek ; Choudhury, Subikash ; Christakoglou, Panagiotis ; Christensen, Christian Holm ; Christiansen, Peter L. ; Chujo, Tatsuya ; Chung, Suh-Urk ; Cicalò, Corrado ; Cifarelli, Luisa ; Cindolo, Federico ; Cleymans, Jean Willy Andre ; Colamaria, Fabio Filippo ; Colella, Domenico ; Collu, Alberto ; Colocci, Manuel ; Conesa Balbastre, Gustavo ; Conesa Del Valle, Zaida ; Connors, Megan Elizabeth ; Contreras Nuno, Jesus Guillermo ; Cormier, Thomas Michael ; Corrales Morales, Yasser ; Cortese, Pietro ; Cortes Maldonado, Ismael ; Cosentino, Mauro Rogerio ; Costa, Filippo ; Crochet, Philippe ; Cruz Albino, Rigoberto ; Cuautle Flores, Eleazar ; Cunqueiro Mendez, Leticia ; 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Esposito, Marco ; Estienne, Magali Danielle ; Esumi, ShinIchi ; Evans, David ; Evdokimov, Sergey ; Fabris, Daniela ; Faivre, Julien ; Falchieri, Davide ; Fantoni, Alessandra ; Fasel, Markus ; Fehlker, Dominik ; Feldkamp, Linus ; Felea, Daniel ; Feliciello, Alessandro ; Feofilov, Grigory ; Ferencei, Jozef ; Fernández Téllez, Arturo ; Gonzalez Ferreiro, Elena ; Ferretti, Alessandro ; Festanti, Andrea ; Figiel, Jan ; Figueredo, Marcel Araujo Silva ; Filchagin, Sergey ; Finogeev, Dmitry ; Fionda, Fiorella Maria Celeste ; Fiore, Enrichetta Maria ; Floratos, Emmanouil ; Floris, Michele ; Foertsch, Siegfried Valentin ; Foka, Panagiota ; Fokin, Sergey ; Fragiacomo, Enrico ; Francescon, Andrea ; Frankenfeld, Ulrich ; Fuchs, Ulrich ; Furget, Christophe ; Furs, Artur ; Fusco Girard, Mario ; Gaardhoeje, Jens Joergen ; Gagliardi, Martino ; Gago Medina, Alberto Martín ; Gallio, Mauro ; Gangadharan, Dhevan Raja ; Ganoti, Paraskevi ; Gao, Chaosong ; Garabatos Cuadrado, Jose ; Garcia-Solis, Edmundo Javier ; 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Meddi, Franco ; Menchaca-Rocha, Arturo Alejandro ; Meninno, Elisa ; Mercado Pérez, Jorge ; Meres, Michal ; Miake, Yasuo ; Mikhaylov, Konstantin ; Milano, Leonardo ; Milošević, Jovan ; Mischke, André ; Mishra, Aditya Nath ; Miśkowiec, Dariusz Czesław ; Mitra, Jubin ; Mitu, Ciprian Mihai ; Mlynarz, Jocelyn ; Mohammadi, Naghmeh ; Mohanty, Bedangadas ; Molnar, Levente ; Montaño Zetina, Luis Manuel ; Montes Prado, Esther ; Morando, Maurizio ; Godoy, Denise Aparecida Moreira de ; Moretto, Sandra ; Morreale, Astrid ; Morsch, Andreas ; Muccifora, Valeria ; Mudnic, Eugen ; Muhlheim, Daniel ; Muhuri, Sanjib ; Mukherjee, Maitreyee ; Muller, Hans ; Gameiro Munhoz, Marcelo ; Murray, Sean ; Musa, Luciano ; Musinsky, Jan ; Nandi, Basanta Kumar ; Nania, Rosario ; Nappi, Eugenio ; Nattrass, Christine ; Nayak, Kishora ; Nayak, Tapan Kumar ; Nazarenko, Sergey ; Nedosekin, Alexander ; Nicassio, Maria ; Niculescu, Mihai ; Niedziela, Jeremi ; Nielsen, Borge Svane ; Nikolaev, Sergey ; Nikulin, Sergey ; Nikulin, Vladimir ; 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Vrlakova, Janka ; Vulpescu, Bogdan ; Vyushin, Alexey ; Wagner, Boris ; Wagner, Jan ; Wagner, Vladimir ; Wang, Mengliang ; Wang, Yifei ; Watanabe, Daisuke ; Weber, Michael ; Weber, Steffen Georg ; Wessels, Johannes P. ; Westerhoff, Uwe ; Wiechula, Jens ; Wikne, Jon ; Wilde, Martin ; Wilk, Grzegorz Andrzej ; Wilkinson, Jeremy John ; Williams, M. Crispin S. ; Windelband, Bernd ; Winn, Michael ; Yaldo, Chris G ; Yamaguchi, Yorito ; Yang, Hongyan ; Yang, Ping ; Yang, Shiming ; Yano, Satoshi ; Yasnopolskiy, Stanislav ; Yi, Jungyu ; Yin, Zhongbao ; Yoo, In-Kwon ; Yushmanov, Igor ; Zaborowska, Anna ; Zaccolo, Valentina ; Zaman, Ali ; Zampolli, Chiara ; Zaporozhets, Sergey ; Zarochentsev, Andrey ; Závada, Petr ; Zavyalov, Nikolay ; Zbroszczyk, Hanna Paulina ; Zgura, Sorin Ion ; Zhalov, Mikhail ; Zhang, Haitao ; Zhang, Xiaoming ; Zhang, Yonghong ; Zhao, Chengxin ; Zhigareva, Natalia ; Zhou, Daicui ; Zhou, Fengchu ; Zhou, You ; Zhou, Zhuo ; Zhu, Hongsheng ; Zhu, Jianhui ; Zhu, Xiangrong ; Zichichi, Antonino ; Zimmermann, Alice ; Zimmermann, Markus ; Zinovjev, Gennady M. ; Zoccarato, Yannick Denis ; Zyzak, Maksym
The differential charged jet cross sections, jet fragmentation distributions, and jet shapes are measured in minimum bias proton-proton collisions at centre-of-mass energy s√=7 TeV using the ALICE detector at the LHC. Jets are reconstructed from charged particle momenta in the mid-rapidity region using the sequential recombination kT and anti-kT as well as the SISCone jet finding algorithms with several resolution parameters in the range R=0.2 to 0.6. Differential jet production cross sections measured with the three jet finders are in agreement in the transverse momentum (pT) interval 20<pjet,chT<100 GeV/c. They are also consistent with prior measurements carried out at the LHC by the ATLAS collaboration. The jet charged particle multiplicity rises monotonically with increasing jet pT, in qualitative agreement with prior observations at lower energies. The transverse profiles of leading jets are investigated using radial momentum density distributions as well as distributions of the average radius containing 80% (⟨R80⟩) of the reconstructed jet pT. The fragmentation of leading jets with R=0.4 using scaled pT spectra of the jet constituents is studied. The measurements are compared to model calculations from event generators (PYTHIA, PHOJET, HERWIG). The measured radial density distributions and ⟨R80⟩ distributions are well described by the PYTHIA model (tune Perugia-2011). The fragmentation distributions are better described by HERWIG.
Abelev, Betty ; Adam, Jaroslav ; Adamová, Dagmar ; Aggarwal, Madan Mohan ; Aglieri Rinella, Gianluca ; Agnello, Michelangelo ; Agostinelli, Andrea ; Agrawal, Neelima ; Ahammed, Zubayer ; Ahmad, Nazeer ; Ahmed, Ijaz ; Ahn, Sang Un ; Ahn, Sul-Ah ; Aimo, Ilaria ; Aiola, Salvatore ; Ajaz, Muhammad ; Akindinov, Alexander ; Alam, Sk Noor ; Aleksandrov, Dmitry ; Alessandro, Bruno ; Alexandre, Didier ; Alici, Andrea ; Alkin, Anton ; Alme, Johan ; Alt, Torsten ; Altinpinar, Sedat ; Altsybeev, Igor ; Prado, Caio Alves Garcia ; Andrei, Cristian ; Andronic, Anton ; Anguelov, Venelin ; Anielski, Jonas ; Antičić, Tome ; Antinori, Federico ; Antonioli, Pietro ; Aphecetche, Laurent Bernard ; Appelshäuser, Harald ; Arcelli, Silvia ; Armesto Perez, Nestor ; Arnaldi, Roberta ; Aronsson, Tomas ; Arsene, Ionut Cristian ; Arslandok, Mesut ; Augustinus, Andre ; Averbeck, Ralf Peter ; Awes, Terry ; Azmi, Mohd Danish ; Bach, Matthias ; Badalà, Angela ; Baek, Yong Wook ; Bagnasco, Stefano ; Bailhache, Raphaëlle ; Bala, Renu ; Baldisseri, Alberto ; Baltasar Dos Santos Pedrosa, Fernando ; Baral, Rama Chandra ; Barbera, Roberto ; Barile, Francesco ; Barnaföldi, Gergely Gábor ; Barnby, Lee Stuart ; Ramillien Barret, Valerie ; Bartke, Jerzy ; Basile, Maurizio ; Bastid, Nicole ; Basu, Sumit ; Bathen, Bastian ; Batigne, Guillaume ; Batista Camejo, Arianna ; Batyunya, Boris ; Bätzing, Paul Christoph ; Baumann, Christoph Heinrich ; Bearden, Ian Gardner ; Beck, Hans ; Bedda, Cristina ; Behera, Nirbhay Kumar ; Belikov, Iouri ; Bellini, Francesca ; Bellwied, Rene ; Belmont Moreno, Ernesto ; Belmont Iii, Ronald John ; Belyaev, Vladimir ; Bencédi, Gyula ; Beolè, Stefania ; Berceanu, Ionela ; Bercuci, Alexandru ; Berdnikov, Yaroslav ; Berényi, Dániel ; Berger, Martin Emanuel ; Bertens, Redmer Alexander ; Berzano, Dario ; Betev, Latchezar ; Bhasin, Anju ; Bhat, Inayat Rasool ; Bhati, Ashok Kumar ; Bhattacharjee, Buddhadeb ; Bhom, Jihyun ; Bianchi, Livio ; Bianchi, Nicola ; Bianchin, Chiara ; Bielčík, Jaroslav ; Bielčíková, Jana ; Bilandzic, Ante ; Bjelogrlic, Sandro ; Blanco, Fernando ; Blau, Dmitry S. ; Blume, Christoph ; Bock, Friederike ; Bogdanov, Alexey A. ; Bøggild, Hans ; Bogolyubskiy, Mikhail ; Boehmer, Felix Valentin ; Boldizsar, Laszlo ; Bombara, Marek ; Book, Julian ; Borel, Herve ; Borissov, Alexander ; Bossú, Francesco ; Botje, Michiel ; Botta, Elena ; Boettger, Stefan ; Braun-Munzinger, Peter ; Bregant, Marco ; Breitner, Timo ; Broker, Theo Alexander ; Browning, Tyler Allen ; Broz, Michal ; Bruna, Elena ; Bruno, Giuseppe Eugenio ; Budnikov, Dmitry ; Büsching, Henner ; Bufalino, Stefania ; Bunčić, Predrag ; Busch, Oliver ; Buthelezi, Edith Zinhle ; Caffarri, Davide ; Cai, Xu ; Caines, Helen Louise ; Calero Diaz, Liliet ; Caliva, Alberto ; Calvo Villar, Ernesto ; Camerini, Paolo ; Carena, Francesco ; Carena, Wisla ; Castillo Castellanos, Javier Ernesto ; Casula, Ester Anna Rita ; Catanescu, Vasile Ioan ; Cavicchioli, Costanza ; Ceballos Sanchez, Cesar ; Čepila, Jan ; Cerello, Piergiorgio ; Chang, Beomsu ; Chapeland, Sylvain ; Charvet, Jean-Luc Fernand ; Chattopadhyay, Subhasis ; Chattopadhyay, Sukalyan ; Chelnokov, Volodymyr ; Cherney, Michael Gerard ; Cheshkov, Cvetan Valeriev ; Cheynis, Brigitte ; Chibante Barroso, Vasco Miguel ; Chinellato, David Dobrigkeit ; Chochula, Peter ; Chojnacki, Marek ; Choudhury, Subikash ; Christakoglou, Panagiotis ; Christensen, Christian Holm ; Christiansen, Peter L. ; Chujo, Tatsuya ; Chung, Suh-Urk ; Cicalò, Corrado ; Cifarelli, Luisa ; Cindolo, Federico ; Cleymans, Jean Willy Andre ; Colamaria, Fabio Filippo ; Colella, Domenico ; Collu, Alberto ; Colocci, Manuel ; Conesa Balbastre, Gustavo ; Conesa Del Valle, Zaida ; Connors, Megan Elizabeth ; Contreras Nuno, Jesus Guillermo ; Cormier, Thomas Michael ; Corrales Morales, Yasser ; Cortese, Pietro ; Cortes Maldonado, Ismael ; Cosentino, Mauro Rogerio ; Costa, Filippo ; Crochet, Philippe ; Cruz Albino, Rigoberto ; Cuautle Flores, Eleazar ; Cunqueiro Mendez, Leticia ; Dainese, Andrea ; Dang, Ruina ; Danu, Andrea ; Das, Debasish ; Das, Indranil ; Das, Kushal ; Das, Supriya ; Dash, Ajay Kumar ; Dash, Sadhana ; De, Sudipan ; Delagrange, Hugues ; Deloff, Andrzej ; Denes, Ervin Sandor ; D’Erasmo, Ginevra ; De Caro, Annalisa ; De Cataldo, Giacinto ; Cuveland, Jan de ; De Falco, Alessandro ; De Gruttola, Daniele ; De Marco, Nora ; De Pasquale, Salvatore ; De Rooij, Raoul Stefan ; Diaz Corchero, Miguel Angel ; Dietel, Thomas ; Dillenseger, Pascal ; Divià, Roberto ; Di Bari, Domenico ; Di Liberto, Sergio ; Di Mauro, Antonio ; Di Nezza, Pasquale ; Djuvsland, Øystein ; Dobrin, Alexandru Florin ; Dobrowolski, Tadeusz Antoni ; Domenicis Gimenez, Diogenes ; Donigus, Benjamin ; Dordic, Olja ; Dorheim, Sverre ; Dubey, Anand Kumar ; Dubla, Andrea ; Ducroux, Laurent ; Dupieux, Pascal ; Dutt Mazumder, Abhee Kanti ; Hilden, Timo Eero ; Ehlers Iii, Raymond James ; Elia, Domenico ; Engel, Heiko ; Erazmus, Barbara Ewa ; Erdal, Hege Austrheim ; Eschweiler, Dominic ; Espagnon, Bruno ; Esposito, Marco ; Estienne, Magali Danielle ; Esumi, ShinIchi ; Evans, David ; Evdokimov, Sergey ; Fabris, Daniela ; Faivre, Julien ; Falchieri, Davide ; Fantoni, Alessandra ; Fasel, Markus ; Fehlker, Dominik ; Feldkamp, Linus ; Felea, Daniel ; Feliciello, Alessandro ; Feofilov, Grigory ; Ferencei, Jozef ; Fernández Téllez, Arturo ; Gonzalez Ferreiro, Elena ; Ferretti, Alessandro ; Festanti, Andrea ; Figiel, Jan ; Figueredo, Marcel Araujo Silva ; Filchagin, Sergey ; Finogeev, Dmitry ; Fionda, Fiorella Maria Celeste ; Fiore, Enrichetta Maria ; Floratos, Emmanouil ; Floris, Michele ; Foertsch, Siegfried Valentin ; Foka, Panagiota ; Fokin, Sergey ; Fragiacomo, Enrico ; Francescon, Andrea ; Frankenfeld, Ulrich ; Fuchs, Ulrich ; Furget, Christophe ; Fusco Girard, Mario ; Gaardhoeje, Jens Joergen ; Gagliardi, Martino ; Gago Medina, Alberto Martín ; Gallio, Mauro ; Gangadharan, Dhevan Raja ; Ganoti, Paraskevi ; Gao, Chaosong ; Garabatos Cuadrado, Jose ; Garcia-Solis, Edmundo Javier ; Gargiulo, Corrado ; Garishvili, Irakli ; Gerhard, Jochen ; Germain, Marie ; Gheata, Andrei George ; Gheata, Mihaela ; Ghidini, Bruno ; Ghosh, Premomoy ; Ghosh, Sanjay Kumar ; Gianotti, Paola ; Giubellino, Paolo ; Gładysz-Dziaduś, Ewa ; Glässel, Peter ; Gómez Ramírez, Andrés ; González Zamora, Pedro ; Gorbunov, Sergey ; Görlich, Lidia Maria ; Gotovac, Sven ; Graczykowski, Łukasz Kamil ; Grelli, Alessandro ; Grigoras, Alina Gabriela ; Grigoraș, Costin ; Grigoryev, Vladislav ; Grigoryan, Ara ; Grigoryan, Smbat ; Grynyov, Borys ; Grion, Nevio ; Große-Oetringhaus, Jan Fiete ; Grossiord, Jean-Yves ; Grosso, Raffaele ; Guber, Fedor ; Guernane, Rachid ; Guerzoni, Barbara ; Guilbaud, Maxime Rene Joseph ; Gulbrandsen, Kristjan Herlache ; Gulkanyan, Hrant ; Gumbo, Mervyn ; Gunji, Taku ; Gupta, Anik ; Gupta, Ramni ; Khan, Kamal ; Haake, Rüdiger ; Haaland, Øystein Senneset ; Hadjidakis, Cynthia Marie ; Haiduc, Maria ; Hamagaki, Hideki ; Hamar, Gergö ; Hanratty, Luke David ; Hansen, Alexander ; Harris, John William ; Hartmann, Helvi ; Harton, Austin Vincent ; Hatzifotiadou, Despina ; Hayashi, Shinichi ; Heckel, Stefan Thomas ; Heide, Markus ; Helstrup, Håvard ; Herghelegiu, Andrei Ionut ; Herrera Corral, Gerardo Antonio ; Hess, Benjamin Andreas ; Hetland, Kristin Fanebust ; Hippolyte, Boris ; Hladkỳ, Jan ; Hristov, Peter ; Huang, Meidana ; Humanic, Thomas J. ; Hussain, Nur ; Hutter, Dirk ; Hwang, Dae Sung ; Ilkaev, Radiy ; Ilkiv, Iryna ; Inaba, Motoi ; Innocenti, Gian Michele ; Ionita, Costin ; Ippolitov, Mikhail ; Irfan, Muhammad ; Ivanov, Marian ; Ivanov, Vladimir ; Jacholkowski, Adam Wlodzimierz ; Jacobs, Peter Martin ; Jahnke, Cristiane ; Jang, Haeng Jin ; Janik, Malgorzata Anna ; Pahula Hewage, Sandun ; Jena, Chitrasen ; Jena, Satyajit ; Jiménez Bustamante, Raúl Tonatiuh ; Jones, Peter Graham ; Jung, Hyungtaik ; Jusko, Anton ; Kadyshevskiy, Vladimir ; Kalcher, Sebastian ; Kalinak, Peter ; Kalweit, Alexander Philipp ; Kamin, Jason Adrian ; Kang, Ju Hwan ; Kaplin, Vladimir ; Kar, Somnath ; Karasu Uysal, Ayben ; Karavichev, Oleg V. ; Karavicheva, Tatiana L. ; Karpechev, Evgeny ; Kebschull, Udo ; Keidel, Ralf ; Keijdener, Darius Laurens D. ; Khan, Mohammed Mohisin ; Khan, Palash ; Khan, Shuaib Ahmad ; Khanzadeev, Alexei ; Kharlov, Yury ; Kileng, Bjarte ; Kim, Beomkyu ; Kim, Do Won ; Kim, Dong Jo ; Kim, Jinsook ; Kim, Mimae ; Kim, Minwoo ; Kim, Se Yong ; Kim, Taesoo ; Kirsch, Stefan ; Kisel, Ivan ; Kiselev, Sergej N. ; Kisiel, Adam Ryszard ; Kiss, Gabor ; Klay, Jennifer Lynn ; Klein, Jochen ; Klein-Bösing, Christian ; Kluge, Alexander ; Knichel, Michael Linus ; Knospe, Anders Garritt ; Kobdaj, Chinorat ; Varga-Kofarago, Monika ; Köhler, Markus Konrad ; Kollegger, Thorsten ; Kolozhvari, Anatoly ; Kondratev, Valerii ; Kondratyeva, Natalia ; Konevskikh, Artem ; Kovalenko, Vladimir ; Kowalski, Marek ; Kox, Serge ; Koyithatta Meethaleveedu, Greeshma ; Kral, Jiří ; Králik, Ivan ; Kravčáková, Adela ; Křelina, Michal ; Kretz, Matthias ; Krivda, Marian ; Krizek, Filip ; Kryshen, Evgeny ; Krzewicki, Mikolaj ; Kucera, Vit ; Kucheryaev, Yury ; Kugathasan, Thanushan ; Kuhn, Christian Claude ; Kuijer, Paulus Gerardus ; Kulakov, Igor ; Kumar, Jitendra ; Kurashvili, Podist ; Kurepin, Alexander ; Kurepin, Alexey B. ; Kuryakin, Alexey ; Kushpil, Svetlana ; Kweon, Min Jung ; Kwon, Youngil ; Ladron de Guevara, Pedro ; Lagana Fernandes, Caio ; Lakomov, Igor ; Langoy, Rune ; Lara Martinez, Camilo Ernesto ; Lardeux, Antoine Xavier ; Lattuca, Alessandra ; La Pointe, Sarah Louise ; La Rocca, Paola ; Lea, Ramona ; Leardini, Lucia ; Lee, Graham Richard ; Legrand, Iosif ; Lehnert, Joerg Walter ; Lemmon, Roy Crawford ; Lenti, Vito ; Leogrande, Emilia ; Leoncino, Marco ; Leon Monzon, Ildefonso ; Lévai, Peter ; Li, Shuang ; Lien, Jørgen André ; Lietava, Roman ; Lindal, Svein ; Lindenstruth, Volker ; Lippmann, Christian ; Lisa, Michael A. ; Ljunggren, Hans Martin ; Lodato, Davide Francesco ; Lønne, Per-Ivar ; Loggins, Vera Renee ; Loginov, Vitaly ; Lohner, Daniel ; Loizides, Constantinos ; Lopez, Xavier Bernard ; López Torres, Ernesto ; Lu, Xianguo ; Lüttig, Philipp ; Lunardon, Marcello ; Luparello, Grazia ; Ma, Rongrong ; Maevskaya, Alla ; Mager, Magnus ; Mahapatra, Durga Prasad ; Mahmood, Sohail Musa ; Maire, Antonin ; Majka, Richard Daniel ; Malaev, Mikhail ; Maldonado Cervantes, Ivonne Alicia ; Malinina, Liudmila ; Mal’Kevich, Dmitry ; Malzacher, Peter ; Mamonov, Alexander ; Manceau, Loic Henri Antoine ; Manko, Vladislav ; Manso, Franck ; Manzari, Vito ; Marchisone, Massimiliano ; Mareš, Jiří ; Margagliotti, Giacomo Vito ; Margotti, Anselmo ; Marin, Ana Maria ; Markert, Christina ; Marquard, Marco ; Martashvili, Irakli ; Martin, Nicole Alice ; Martinengo, Paolo ; Martínez Hernández, Mario Iván ; García Martínez, Ginés ; Martin Blanco, Javier ; Martynov, Yevgen ; Mas, Alexis Jean-Michel ; Masciocchi, Silvia ; Masera, Massimo ; Masoni, Alberto ; Massacrier, Laure Marie ; Mastroserio, Annalisa ; Matyja, Adam Tomasz ; Mayer, Christoph ; Mazer, Joel Anthony ; Mazzoni, Alessandra Maria ; Meddi, Franco ; Menchaca-Rocha, Arturo Alejandro ; Mercado Pérez, Jorge ; Meres, Michal ; Miake, Yasuo ; Mikhaylov, Konstantin ; Milano, Leonardo ; Milošević, Jovan ; Mischke, André ; Mishra, Aditya Nath ; Miśkowiec, Dariusz Czesław ; Mitra, Jubin ; Mitu, Ciprian Mihai ; Mlynarz, Jocelyn ; Mohammadi, Naghmeh ; Mohanty, Bedangadas ; Molnar, Levente ; Montaño Zetina, Luis Manuel ; Montes Prado, Esther ; Morando, Maurizio ; Godoy, Denise Aparecida Moreira de ; Moretto, Sandra ; Morreale, Astrid ; Morsch, Andreas ; Muccifora, Valeria ; Mudnic, Eugen ; Muhlheim, Daniel ; Muhuri, Sanjib ; Mukherjee, Maitreyee ; Muller, Hans ; Gameiro Munhoz, Marcelo ; Murray, Sean ; Musa, Luciano ; Musinsky, Jan ; Nandi, Basanta Kumar ; Nania, Rosario ; Nappi, Eugenio ; Nattrass, Christine ; Nayak, Kishora ; Nayak, Tapan Kumar ; Nazarenko, Sergey ; Nedosekin, Alexander ; Nicassio, Maria ; Niculescu, Mihai ; Nielsen, Borge Svane ; Nikolaev, Sergey ; Nikulin, Sergey ; Nikulin, Vladimir ; Nilsen, Bjorn Steven ; Noferini, Francesco ; Nomokonov, Petr V. ; Nooren, Gerardus ; Norman, Jaime ; Nyanin, Alexander ; Nystrand, Joakim Ingemar ; Oeschler, Helmut ; Oh, Saehanseul ; Oh, Sun Kun ; Okatan, Ali ; Oláh, László ; Oleniacz, Janusz ; Silva, Antonio Carlos Oliveira da ; Onderwaater, Jacobus ; Oppedisano, Chiara ; Ortiz Velasquez, Antonio ; Oskarsson, Anders Nils Erik ; Otwinowski, Jacek Tomasz ; Oyama, Ken ; Özdemir, Mahmut ; Sahoo, Pragati ; Pachmayer, Yvonne C. ; Pachr, Milos ; Pagano, Paola ; Paic, Guy ; Painke, Florian ; Pajares Vales, Carlos ; Pal, Susanta Kumar ; Palmeri, Armando ; Pant, Divyash ; Papikyan, Vardanush ; Pappalardo, Giuseppe Salvatore ; Pareek, Pooja ; Park, WooJin ; Parmar, Sonia ; Passfeld, Annika ; Patalakha, Dmitry ; Paticchio, Vincenzo ; Paul, Biswarup ; Pawlak, Tomasz Jan ; Peitzmann, Thomas ; Pereira da Costa, Hugo Denis Antonio ; Pereira De Oliveira Filho, Elienos ; Peresunko, Dmitry Yurevich ; Pérez Lara, Carlos Eugenio ; Pesci, Alessandro ; Peskov, Vladimir ; Pestov, Yury N. ; Petráček, Vojtech ; Petran, Michal ; Petris, Mariana ; Petrovici, Mihai A. ; Petta, Catia ; Piano, Stefano ; Pikna, Miroslav ; Pillot, Philippe ; Pinazza, Ombretta ; Pinsky, Lawrence ; Piyarathna, Danthasinghe ; Płoskoń, Mateusz ; Planinic, Mirko ; Pluta, Jan Marian ; Pochybova, Sona ; Podesta Lerma, Pedro Luis Manuel ; Poghosyan, Martin G. ; Pohjoisaho, Esko Heikki Oskari ; Polishchuk, Boris ; Poljak, Nikola ; Pop, Amalia ; Porteboeuf, Sarah Julie ; Porter, R. Jefferson ; Potukuchi, Baba ; Prasad, Sidharth Kumar ; Preghenella, Roberto ; Prino, Francesco ; Pruneau, Claude A. ; Pshenichnov, Igor A. ; Puddu, Giovanna ; Pujahari, Prabhat Ranjan ; Punin, Valery ; Putschke, Jörn H. ; Qvigstad, Henrik ; Rachevski, Alexandre ; Raha, Sibaji ; Rak, Jan ; Rakotozafindrabe, Andry Malala ; Ramello, Luciano ; Raniwala, Rashmi ; Raniwala, Sudhir ; Räsänen, Sami Sakari ; Rascanu, Bogdan Theodor ; Rathee, Deepika ; Rauf, Aamer Wali ; Razazi, Vahedeh ; Read, Kenneth Francis ; Real, Jean-Sébastien ; Redlich, Krzysztof ; Reed, Rosi Jan ; Rehman, Attiq ur ; Reichelt, Patrick ; Reicher, Martijn ; Reidt, Felix ; Renfordt, Rainer Arno Ernst ; Reolon, Anna Rita ; Reshetin, Andrey ; Rettig, Felix Vincenz ; Revol, Jean-Pierre ; Reygers, Klaus ; Riabov, Viktor ; Ricci, Renato Angelo ; Richert, Tuva Ora Herenui ; Richter, Matthias Rudolph ; Riedler, Petra ; Riegler, Werner ; Riggi, Francesco ; Rivetti, Angelo ; Rocco, Elena ; Rodrı́guez Cahuantzi, Mario ; Rodriguez Manso, Alis ; Røed, Ketil ; Rogochaya, Elena ; Sharma, Rohni ; Rohr, David ; Röhrich, Dieter ; Romita, Rosa ; Ronchetti, Federico ; Ronflette, Lucile ; Rosnet, Philippe ; Rossi, Andrea ; Roukoutakis, Filimon ; Roy, Ankhi ; Roy, Christelle Sophie ; Roy, Pradip Kumar ; Rubio Montero, Antonio Juan ; Rui, Rinaldo ; Russo, Riccardo ; Ryabinkin, Evgeny ; Ryabov, Yury ; Rybicki, Andrzej ; Sadovskiy, Sergey ; Šafařík, Karel ; SahlmÜller, Baldo ; Sahoo, Raghunath ; Sahu, Pradip Kumar ; Saini, Jogender ; Sakai, Shingo ; Salgado Lopez, Carlos Alberto ; Salzwedel, Jai ; Sambyal, Sanjeev Singh ; Samsonov, Vladimir ; Sanchez Castro, Xitzel ; Sanchez Rodriguez, Fernando Javier ; Šándor, Ladislav ; Sandoval, Andres ; Sano, Masato ; Santagati, Gianluca ; Sarkar, Debojit ; Scapparone, Eugenio ; Scarlassara, Fernando ; Scharenberg, Rolf Paul ; Schiaua, Claudiu Cornel ; Schicker, Rainer ; Schmidt, Christian Joachim ; Schmidt, Hans Rudolf ; Schuchmann, Simone ; Schukraft, Jürgen ; Schulc, Martin ; Schuster, Tim ; Schutz, Yves Roland ; Schwarz, Kilian Eberhard ; Schweda, Kai Oliver ; Scioli, Gilda ; Scomparin, Enrico ; Scott, Rebecca Michelle ; Segato, Gianfranco ; Seger, Janet Elizabeth ; Sekiguchi, Yuko ; Selyuzhenkov, Ilya ; Seo, Jeewon ; Serradilla Rodriguez, Eulogio ; Sevcenco, Adrian ; Shabetai, Alexandre ; Shabratova, Galina ; Shahoyan, Ruben ; Shangaraev, Artem ; Sharma, Natasha ; Sharma, Satish ; Shigaki, Kenta ; Shtejer Diaz, Katherin ; Sibiryak, Yury ; Siddhanta, Sabyasachi ; Siemiarczuk, Teodor ; Silvermyr, David Olle Rickard ; Silvestre, Catherine Micaela ; Simatovic, Goran ; Singaraju, Rama Narayana ; Singh, Ranbir ; Singha, Subhash ; Singhal, Vikas ; Sinha, Bikash ; Sarkar - Sinha, Tinku ; Sitar, Branislav ; Sitta, Mario ; Skaali, Toralf Bernhard ; Skjerdal, Kyrre ; Slupecki, Maciej ; Smirnov, Nikolai ; Snellings, Raimond ; Soegaard, Carsten ; Soltz, Ron ; Song, Jihye ; Song, Myunggeun ; Soramel, Francesca ; Sorensen, Soren Pontoppidan ; Spacek, Michal ; Spiriti, Eleuterio ; Sputowska, Iwona Anna ; Spyropoulou-Stassinaki, Martha ; Srivastava, Brijesh Kumar ; Stachel, Johanna ; Stan, Ionel ; Stefanek, Grzegorz ; Steinpreis, Matthew Donald ; Stenlund, Evert Anders ; Steyn, Gideon Francois ; Stiller, Johannes Hendrik ; Stocco, Diego ; Stolpovskiy, Mikhail ; Strmen, Peter ; Suaide, Alexandre Alarcon do Passo ; Sugitate, Toru ; Suire, Christophe Pierre ; Suleymanov, Mais Kazim Oglu ; Sultanov, Rishat ; Šumbera, Michal ; Šuša, Tatjana ; Symons, Timothy ; Szabo, Alexander ; Toledo, Alejandro Szanto de ; Szarka, Imrich ; Szczepankiewicz, Adam ; Szymanski, Maciej Pawel ; Takahashi, Jun ; Tangaro, Marco-Antonio ; Tapia Takaki, Jesus Daniel ; Tarantola Peloni, Attilio ; Tarazona Martinez, Alfonso ; Tarzila, Madalina-Gabriela ; Tauro, Arturo ; Tejeda Muñoz, Guillermo ; Telesca, Adriana ; Terrevoli, Cristina ; Thäder, Jochen ; Thomas, Deepa ; Tieulent, Raphael Noel ; Timmins, Anthony Robert ; Toia, Alberica ; Trubnikov, Victor ; Trzaska, Wladyslaw Henryk ; Tsuji, Tomoya ; Tumkin, Alexandr ; Turrisi, Rosario ; Tveter, Trine Spedstad ; Ullaland, Kjetil ; Uras, Antonio ; Usai, Gianluca ; Vajzer, Michal ; Vala, Martin ; Valencia Palomo, Lizardo ; Vallero, Sara ; Vyvre, Pierre vande ; Maarel, Jasper van der ; Hoorne, Jacobus Willem van ; Leeuwen, Marco van ; Vargas Treviño, Maria Aurora Diozcora ; Vargyas, Márton ; Varma, Raghava ; Vasileiou, Maria ; Vasiliev, Andrey ; Vechernin, Vladimir ; Veldhoen, Misha ; Velure, Arild ; Venaruzzo, Massimo ; Vercellin, Ermanno ; Vergara Limon, Sergio ; Vernet, Renaud ; Verweij, Marta ; Vicković, Linda ; Viesti, Giuseppe ; Viinikainen, Jussi Samuli ; Vilakazi, Zabulon ; Villalobos Baillie, Orlando ; Vinogradov, Alexander ; Vinogradov, Leonid ; Vinogradov, Yury I. ; Virgili, Tiziano ; Viyogi, Yogendra P. ; Vodopyanov, Alexander ; Volkl, Martin Andreas ; Voloshin, Kirill ; Voloshin, Sergei ; Volpe, Giacomo ; Haller, Barthélémy von ; Vorobyev, Ivan ; Vranić, Danilo ; Vrlakova, Janka ; Vulpescu, Bogdan ; Vyushin, Alexey ; Wagner, Boris ; Wagner, Jan ; Wagner, Vladimir ; Wang, Mengliang ; Wang, Yifei ; Watanabe, Daisuke ; Weber, Michael ; Wessels, Johannes P. ; Westerhoff, Uwe ; Wiechula, Jens ; Wikne, Jon ; Wilde, Martin ; Wilk, Grzegorz Andrzej ; Wilkinson, Jeremy John ; Williams, M. Crispin S. ; Windelband, Bernd Stefan ; Winn, Michael ; Yaldo, Chris G ; Yamaguchi, Yorito ; Yang, Hongyan ; Yang, Ping ; Yang, Shiming ; Yano, Satoshi ; Yasnopolskiy, Stanislav ; Yi, Jungyu ; Yin, Zhongbao ; Yoo, In-Kwon ; Yushmanov, Igor ; Zaccolo, Valentina ; Zach, Cenek ; Zaman, Ali ; Zampolli, Chiara ; Zaporozhets, Sergey ; Zarochentsev, Andrey ; Závada, Petr ; Zavyalov, Nikolay ; Zbroszczyk, Hanna Paulina ; Zgura, Sorin Ion ; Zhalov, Mikhail ; Zhang, Haitao ; Zhang, Xiaoming ; Zhang, Yonghong ; Zhao, Chengxin ; Zhigareva, Natalia ; Zhou, Daicui ; Zhou, Fengchu ; Zhou, You ; Zhou, Zhuo ; Zhu, Hongsheng ; Zhu, Jianhui ; Zhu, Xiangrong ; Zichichi, Antonino ; Zimmermann, Alice ; Zimmermann, Markus ; Zinovjev, Gennady M. ; Zoccarato, Yannick Denis ; Zyzak, Maksym
The ALICE collaboration at the LHC reports measurement of the inclusive production cross section of electrons from semi-leptonic decays of beauty hadrons with rapidity |y|<0.8 and transverse momentum 1<pT<10 GeV/c, in pp collisions at s√= 2.76 TeV. Electrons not originating from semi-electronic decay of beauty hadrons are suppressed using the impact parameter of the corresponding tracks. The production cross section of beauty decay electrons is compared to the result obtained with an alternative method which uses the distribution of the azimuthal angle between heavy-flavour decay electrons and charged hadrons. Perturbative QCD calculations agree with the measured cross section within the experimental and theoretical uncertainties. The integrated visible cross section, σb→e=3.47±0.40(stat)+1.12−1.33(sys)±0.07(norm)μb, was extrapolated to full phase space using Fixed Order plus Next-to-Leading Log (FONLL) predictions to obtain the total bb¯ production cross section, σbb¯=130±15.1(stat)+42.1−49.8(sys)+3.4−3.1(extr)±2.5(norm)±4.4(BR)μb.