Measurement of the ^{140}Ce(n,γ) Cross Section at n_TOF and Its Astrophysical Implications for the Chemical Evolution of the Universe

^{140}Ce(n,γ) is a key reaction for slow neutron-capture (s-process) nucleosynthesis due to being a bottleneck in the reaction flow. For this reason, it was measured with high accuracy (uncertainty ≈5%) at the n_TOF facility, with an unprecedented combination of a high purity sample and low neutron-sensitivity detectors. The measured Maxwellian averaged cross section is up to 40% higher than previously accepted values. Stellar model calculations indicate a reduction around 20% of the s-process contribution to the Galactic cerium abundance and smaller sizeable differences for most of the heavier elements. No variations are found in the nucleosynthesis from massive stars.

First 80Se(n,γ) cross section measurement with high resolution in the full stellar energy range 1 eV - 100 keV and its astrophysical implications for the s-process

Most elements heavier than iron have been generated in the stellar media by means of neutron capture reactions, approximately half are produced by the slow neutron capture or s-process. Radiative neutron capture cross section measurements are of fundamental importance for the study of this mechanism. In this contribution we present a brief summary on the measurement and results for the 80Se(n,γ) cross-section. The experiment was carried out at CERN n_TOF EAR1 via the time of flight (ToF) technique, using four C6D6 scintillation detectors with very fast response. More than a hundred new resonances have been analyzed for the first time with a high accuracy. The MACS obtained at kT = 8 keV is 36% smaller than the recommended value in KADo-NiS. Some of the astrophysical implications of this result are elucidated in this contribution.

Neutron capture cross section measurements of 241Am at the n_TOF facility

Neutron capture on 241Am plays an important role in the nuclear energy production and also provides valuable information for the improvement of nuclear models and the statistical interpretation of the nuclear properties. A new experiment to measure the 241Am(n, γ) cross section in the thermal region and the first few resonances below 10 eV has been carried out at EAR2 of the n_TOF facility at CERN. Three neutron-insensitive C6D6 detectors have been used to measure the neutron-capture gamma cascade as a function of the neutron time of flight, and then deduce the neutron capture yield. Preliminary results will be presented and compared with previously obtained results at the same facility in EAR1. In EAR1 the gamma-ray background at thermal energies was about 90% of the signal while in EAR2 is up to a 25 factor much more favorable signal to noise ratio. We also extended the low energy limit down to subthermal energies. This measurement will allow a comparison with neutron capture measurements conducted at reactors and using a different experimental technique.

Study of photon strength functions of241Pu and245Cm from neutron capture measurements

We have measured theγ-rays following neutron capture on240Pu and244Cm at the n_TOF facility at CERN with the Total Absorption Calorimeter (TAC) and with C6D6 organic scintillators. The TAC is made of 40 BaF2 crystals operating in coincidence and covering almost the entire solid angle. This allows to obtain information concerning the energy spectra and the multiplicity of the measured captureγ-ray cascades. Additional information is also obtained from the C6D6 detectors. We have analyzed the measured data in order to draw conclusions about the Photon Strength Functions (PSFs) of241Pu and245Cm below their neutron separation energies. The analysis has been performed by fitting the PSFs to the experimental results, using the differential evolution method, in order to find neutron capture cascades capable of reproducing at the same time a great variety of deposited energy spectra.

Measurement of the244Cm capture cross sections at both CERN n_TOF experimental areas

Accurate neutron capture cross section data for minor actinides (MAs) are required to estimate the production and transmutation rates of MAs in light water reactors with a high burnup, critical fast reactors like Gen-IV systems and other innovative reactor systems such as accelerator driven systems (ADS). Capture reactions of244Cm open the path for the formation of heavier Cm isotopes and of heavier elements such as Bk and Cf. In addition,244Cm shares nearly 50% of the total actinide decay heat in irradiated reactor fuels with a high burnup, even after three years of cooling.

Experimental data for this isotope are very scarce due to the difficulties of providing isotopically enriched samples and because the high intrinsic activity of the samples requires the use of neutron facilities with high instantaneous flux. The only two previous experimental data sets for this neutron capture cross section have been obtained in 1969 using a nuclear explosion and, more recently, at J-PARC in 2010. The neutron capture cross sections have been measured at n_TOF with the same samples that the previous experiments in J-PARC. The samples were measured at n_TOF Experimental Area 2 (EAR-2) with three C6D6detectors and also in Experimental Area 1 (EAR-1) with the Total Absorption Calorimeter (TAC). Preliminary results assessing the quality and limitations of these new experimental datasets are presented for the experiments in both areas. Preliminary yields of both measurements will be compared with evaluated libraries for the first time.

Study of the photon strength functions and level density in the gamma decay of the n + 234U reaction

The accurate calculations of neutron-induced reaction cross sections are relevant for many nuclear applications. The photon strength functions and nuclear level densities are essential inputs for such calculations. These quantities for 235U are studied using the measurement of the gamma de-excitation cascades in radiative capture on 234U with the Total Absorption Calorimeter at n_TOF at CERN. This segmented 4π gamma calorimeter is designed to detect gamma rays emitted from the nucleus with high efficiency. This experiment provides information on gamma multiplicity and gamma spectra that can be compared with numerical simulations. The code DICEBOXC is used to simulate the gamma cascades while GEANT4 is used for the simulation of the interaction of these gammas with the TAC materials. Available models and their parameters are being tested using the present data. Some preliminary results of this ongoing study are presented and discussed.

Measurement of the 244Cm and 246Cm neutron-induced capture cross sections at the n_TOF facility

The neutron capture reactions of the 244Cm and 246Cm isotopes open the path for the formation of heavier Cm isotopes and heavier elements such as Bk and Cf in a nuclear reactor. In addition, both isotopes belong to the minor actinides with a large contribution to the decay heat and to the neutron emission in irradiated fuels. There are only two previous 244Cm and 246Cm capture cross section measurements: one in 1969 using a nuclear explosion [1] and the most recent data measured at J-PARC in 2010 [2]. The data for both isotopes are very scarce due to the difficulties in performing the measurements: high intrinsic activity of the samples and limited facilities capable of providing isotopically enriched samples.

We have measured both neutron capture cross sections at the n_TOF Experimental Area 2 (EAR-2) with three C6 D6 detectors and also at Area 1 (EAR-1) with the TAC. Preliminary results assessing the quality and limitations (back-ground subtraction, measurement technique and counting statistics) of this new experimental datasets are presented and discussed.

Measurement of the radiative capture cross section of the s-process branching points 204Tl and 171Tm at the n_TOF facility (CERN)

The neutron capture cross section of some unstable nuclei is especially relevant for s-process nucleosynthesis studies. This magnitude is crucial to determine the local abundance pattern, which can yield valuable information of the s-process stellar environment. In this work we describe the neutron capture (n,γ) measurement on two of these nuclei of interest, 204Tl and 171Tm, from target production to the final measurement, performed successfully at the n_TOF facility at CERN in 2014 and 2015. Preliminary results on the ongoing experimental data analysis will also be shown. These results include the first ever experimental observation of capture resonances for these two nuclei.

Probing the Nodal Structure of Landau Level Wave Functions in Real Space

The inversion layer of p-InSb(110) obtained by Cs adsorption of 1.8% of a monolayer is used to probe the Landau level wave functions within smooth potential valleys by scanning tunneling spectroscopy at 14 T. The nodal structure becomes apparent as a double peak structure of each spin polarized first Landau level, while the zeroth Landau level exhibits a single peak per spin level only. The real space data show single rings of the valley-confined drift states for the zeroth Landau level and double rings for the first Landau level. The result is reproduced by a recursive Green function algorithm using the potential landscape obtained experimentally. We show that the result is generic by comparing the local density of states from the Green function algorithm with results from a well-controlled analytic model based on the guiding center approach.

[Sonographic criteria for diagnosing sentinel node metastases in melanoma patients]

PURPOSE

Ultrasound-guided fine needle aspiration cytology (US-FNAC) prior to surgical excision of a sentinel lymph node (SLN) is a new microinvasive approach for detecting micrometastases in melanoma patients. The aim of the current prospective study was to determine the sensitivity and specificity of the method and to define new diagnostic generally applicable ultrasound criteria.

MATERIALS AND METHODS

In 800 consecutive patients suffering from malignant melanoma of stage I/II, the SNs were examined sonographically after lymphoscintigraphy. US-FNAC was performed in all suspicious lesions in 302 patients. All patients underwent surgical removal of the SLN. The final histopathology and sonographic findings were correlated.

RESULTS

After a follow-up of 37 months and a given median tumor thickness of 1.6 mm in our cohort, 21 % of the patients had a positive SLN in the histologic examination. We calculated a sensitivity and specificity of US-FNAC of 56 % and 99 %, respectively. The positive and negative predictive values were 92 % and 89 %, respectively. The highest positive predictive values were achieved using the ultrasound criterion of peripheral perfusion in power mode. The sensitivity of US-FNAC increased in parallel with an increasing pT stage of the primary tumor and increasing size of the largest diameter of the involved SN nest.

CONCLUSION

Our prospective study shows the impact of ultrasound-guided FNAC in the staging of the SN prior to a planned SLNB. It proved to be an additional, cost-effective diagnostic tool that enhances the discriminatory power for the indication to perform SLNB and spares both the patient and the surgeon a second surgical procedure. Among the tested ultrasound criteria, peripheral perfusion (PP) showed the highest sensitivity for detecting early SN.

Pyrolysis Mass Spectrometry of Protected Phosphotriester Oligodeoxyribonucleotides

Pyrolysis mass spectrometry is shown to be a useful tool in the analysis of the protected intermediate deoxy oligonucleotides synthesized by the phosphotriester approach. Characteristic ions of the protected nucleic acid bases and terminal substituents appear in the mass fragmentation pattern which allows a rapid control of the attachment of the polynucleotide block in the chemical synthesis.

Quantitative analysis of detected sentinel lymph nodes and the incidence of micrometastases using two different methods of surgical melanoma treatment--pilot study

The aim of our study was to compare the number of detected sentinel lymph nodes and the incidence of micrometastases between two groups of patients with cutaneous melanoma.

METHODS

100 patients were divided in to two groups: group V and group D. Group V patients (50) with melanoma underwent a single-stage surgery--radical excision of the tumour with sentinel lymph node biopsy (study group "V"). Group D patients (50) with melanoma underwent two-stage surgery; initially primary diagnostic excision of the tumour (0.5 cm from margins of the lesion) followed by a radical re-excision of the post-operative scar and sentinel lymph node biopsy (study group "D").

RESULTS

Study groups "V" and "D" were tested for homogeneity with regard to age, melanoma thickness, location of melanoma, type of melanoma, and ulceration. The groups were found to be homogenous. The average number of removed sentinel lymph nodes in group "D" was 1.0 more than in group "V" (p < 0.05). The averages were 3.7 and 2.7 respectively with a SD of 1.8. The relationship between the SL node staining and type of surgery was (p < 0.05). 49.6% stained radioactive sentinel lymphnodes at the time of surgery was found in group "V", while 33.9% in group "D".

CONCLUSIONS

Using two different early-stage cutaneous melanoma management techniques significantly more sentinel lymph nodes (p = 0.006) were detected using the two-stage surgery approach. However, there was no significant difference between the two approaches regarding the number of sentinel lymph nodes with micrometastases that were detected and excised.

Energy dependence of the transverse momentum distributions of charged particles in pp collisions measured by ALICE

Differential cross sections of charged particles in inelastic pp collisions as a function of p_T have been measured at [Formula: see text] at the LHC. The p_T spectra are compared to NLO-pQCD calculations. Though the differential cross section for an individual [Formula: see text] cannot be described by NLO-pQCD, the relative increase of cross section with [Formula: see text] is in agreement with NLO-pQCD. Based on these measurements and observations, procedures are discussed to construct pp reference spectra at [Formula: see text] up to p_T=50 GeV/c as required for the calculation of the nuclear modification factor in nucleus-nucleus and proton-nucleus collisions.

Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV

The directed flow of charged particles at midrapidity is measured in Pb-Pb collisions at √(s(NN))=2.76 TeV relative to the collision symmetry plane defined by the spectator nucleons. A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found at the highest RHIC energy is observed. This suggests a smaller longitudinal tilt of the initial system and disfavors the strong fireball rotation predicted for the LHC energies. The rapidity-even directed flow component is measured for the first time with spectators and found to be independent of pseudorapidity with a sign change at transverse momenta p(T) between 1.2 and 1.7  GeV/c. Combined with the observation of a vanishing rapidity-even p(T) shift along the spectator deflection this is strong evidence for dipolelike initial density fluctuations in the overlap zone of the nuclei. Similar trends in the rapidity-even directed flow and the estimate from two-particle correlations at midrapidity, which is larger by about a factor of 40, indicate a weak correlation between fluctuating participant and spectator symmetry planes. These observations open new possibilities for investigation of the initial conditions in heavy-ion collisions with spectator nucleons.

K(S)0 and Λ production in Pb-Pb collisions at √(s(NN))=2.76 TeV

The ALICE measurement of K(S)(0) and Λ production at midrapidity in Pb-Pb collisions at √(s(NN))=2.76 TeV is presented. The transverse momentum (p(T)) spectra are shown for several collision centrality intervals and in the p(T) range from 0.4 GeV/c (0.6 GeV/c for Λ) to 12 GeV/c. The p(T) dependence of the Λ/K(S)(0) ratios exhibits maxima in the vicinity of 3 GeV/c, and the positions of the maxima shift towards higher p(T) with increasing collision centrality. The magnitude of these maxima increases by almost a factor of three between most peripheral and most central Pb-Pb collisions. This baryon excess at intermediate p(T) is not observed in pp interactions at √s=0.9 TeV and at √s=7 TeV. Qualitatively, the baryon enhancement in heavy-ion collisions is expected from radial flow. However, the measured p(T) spectra above 2 GeV/c progressively decouple from hydrodynamical-model calculations. For higher values of p(T), models that incorporate the influence of the medium on the fragmentation and hadronization processes describe qualitatively the p(T) dependence of the Λ/K(S)(0) ratio.

Charmonium and e+e- pair photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at [Formula: see text]

The ALICE Collaboration at the LHC has measured the J/ψ and ψ' photoproduction at mid-rapidity in ultra-peripheral Pb-Pb collisions at [Formula: see text]. The charmonium is identified via its leptonic decay for events where the hadronic activity is required to be minimal. The analysis is based on an event sample corresponding to an integrated luminosity of about 23 μb-1. The cross section for coherent and incoherent J/ψ production in the rapidity interval -0.9 Collapse

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Affiliation(s)

The ALICE Collaboration CERN, 1211 Geneva 23, Switzerland
E. Abbas Academy of Scientific Research and Technology (ASRT), Cairo, Egypt Fachhochschule Köln, Köln, Germany Department of Physics, Gauhati University, Guwahati, India Suranaree University of Technology, Nakhon Ratchasima, Thailand University of Technology and Austrian Academy of Sciences, Vienna, Austria
B. Abelev Lawrence Livermore National Laboratory, Livermore, California United States
J. Adam Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
D. Adamová Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
A. M. Adare Yale University, New Haven, Connecticut United States
M. M. Aggarwal Physics Department, Panjab University, Chandigarh, India
G. Aglieri Rinella European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Agnello Politecnico di Torino, Turin, Italy Sezione INFN, Turin, Italy
A. G. Agocs Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
A. Agostinelli Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
Z. Ahammed Variable Energy Cyclotron Centre, Kolkata, India
N. Ahmad Department of Physics, Aligarh Muslim University, Aligarh, India
A. Ahmad Masoodi Department of Physics, Aligarh Muslim University, Aligarh, India
I. Ahmed COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
S. A. Ahn Korea Institute of Science and Technology Information, Daejeon, South Korea
S. U. Ahn Korea Institute of Science and Technology Information, Daejeon, South Korea
I. Aimo Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Politecnico di Torino, Turin, Italy Sezione INFN, Turin, Italy
M. Ajaz COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
A. Akindinov Institute for Theoretical and Experimental Physics, Moscow, Russia
D. Aleksandrov Russian Research Centre Kurchatov Institute, Moscow, Russia
B. Alessandro Sezione INFN, Turin, Italy
D. Alexandre School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. Alici Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Sezione INFN, Bologna, Italy
A. Alkin Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
E. Almaráz Aviña Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
J. Alme Faculty of Engineering, Bergen University College, Bergen, Norway
T. Alt Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
V. Altini Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
S. Altinpinar Department of Physics and Technology, University of Bergen, Bergen, Norway
I. Altsybeev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
C. Andrei National Institute for Physics and Nuclear Engineering, Bucharest, Romania
A. Andronic Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
V. Anguelov Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
J. Anielski Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
C. Anson Department of Physics, Ohio State University, Columbus, Ohio United States
T. Antičić Rudjer Bošković Institute, Zagreb, Croatia
F. Antinori Sezione INFN, Padova, Italy
P. Antonioli Sezione INFN, Bologna, Italy
L. Aphecetche SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
H. Appelshäuser Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N. Arbor Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
S. Arcelli Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
A. Arend Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N. Armesto Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
R. Arnaldi Sezione INFN, Turin, Italy
T. Aronsson Yale University, New Haven, Connecticut United States
I. C. Arsene Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Arslandok Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Asryan V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
A. Augustinus European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Averbeck Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
T. C. Awes Oak Ridge National Laboratory, Oak Ridge, Tennessee United States
J. Äystö Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
M. D. Azmi Department of Physics, Aligarh Muslim University, Aligarh, India Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
M. Bach Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Badalà Sezione INFN, Catania, Italy
Y. W. Baek Gangneung-Wonju National University, Gangneung, South Korea Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
R. Bailhache Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R. Bala Physics Department, University of Jammu, Jammu, India Sezione INFN, Turin, Italy
A. Baldisseri Commissariat à l’Energie Atomique, IRFU, Saclay, France
F. Baltasar Dos Santos Pedrosa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Bán Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
R. C. Baral Institute of Physics, Bhubaneswar, India
R. Barbera Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
F. Barile Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
G. G. Barnaföldi Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
L. S. Barnby School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
V. Barret Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
J. Bartke The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M. Basile Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
N. Bastid Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
S. Basu Variable Energy Cyclotron Centre, Kolkata, India
B. Bathen Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
G. Batigne SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
B. Batyunya Joint Institute for Nuclear Research (JINR), Dubna, Russia
P. C. Batzing Department of Physics, University of Oslo, Oslo, Norway
C. Baumann Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. G. Bearden Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
H. Beck Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
N. K. Behera Indian Institute of Technology Bombay (IIT), Mumbai, India
I. Belikov Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
F. Bellini Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
R. Bellwied University of Houston, Houston, Texas United States
E. Belmont-Moreno Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
G. Bencedi Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
S. Beole Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
I. Berceanu National Institute for Physics and Nuclear Engineering, Bucharest, Romania
A. Bercuci National Institute for Physics and Nuclear Engineering, Bucharest, Romania
Y. Berdnikov Petersburg Nuclear Physics Institute, Gatchina, Russia
D. Berenyi Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
A. A. E. Bergognon SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
R. A. Bertens Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
D. Berzano Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Sezione INFN, Turin, Italy
L. Betev European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Bhasin Physics Department, University of Jammu, Jammu, India
A. K. Bhati Physics Department, Panjab University, Chandigarh, India
J. Bhom University of Tsukuba, Tsukuba, Japan
L. Bianchi Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
N. Bianchi Laboratori Nazionali di Frascati, INFN, Frascati, Italy
C. Bianchin Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
J. Bielčík Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
J. Bielčíková Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
A. Bilandzic Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
S. Bjelogrlic Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
F. Blanco Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
F. Blanco University of Houston, Houston, Texas United States
D. Blau Russian Research Centre Kurchatov Institute, Moscow, Russia
C. Blume Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Boccioli European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. Böttger Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Bogdanov Moscow Engineering Physics Institute, Moscow, Russia
H. Bøggild Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
M. Bogolyubsky Institute for High Energy Physics, Protvino, Russia
L. Boldizsár Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
M. Bombara Faculty of Science, P.J. Šafárik University, Košice, Slovakia
J. Book Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
H. Borel Commissariat à l’Energie Atomique, IRFU, Saclay, France
A. Borissov Wayne State University, Detroit, Michigan United States
F. Bossú Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
M. Botje Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
E. Botta Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
E. Braidot Lawrence Berkeley National Laboratory, Berkeley, California United States
P. Braun-Munzinger Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Bregant SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
T. Breitner Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T. A. Broker Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
T. A. Browning Purdue University, West Lafayette, Indiana United States
M. Broz Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
R. Brun European Organization for Nuclear Research (CERN), Geneva, Switzerland
E. Bruna Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Sezione INFN, Turin, Italy
G. E. Bruno Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
D. Budnikov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
H. Buesching Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S. Bufalino Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Sezione INFN, Turin, Italy
P. Buncic European Organization for Nuclear Research (CERN), Geneva, Switzerland
O. Busch Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
Z. Buthelezi Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
D. Caffarri Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Sezione INFN, Padova, Italy
X. Cai Central China Normal University, Wuhan, China
H. Caines Yale University, New Haven, Connecticut United States
E. Calvo Villar Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
P. Camerini Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
V. Canoa Roman Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
G. Cara Romeo Sezione INFN, Bologna, Italy
W. Carena European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Carena European Organization for Nuclear Research (CERN), Geneva, Switzerland
N. Carlin Filho Universidade de São Paulo (USP), São Paulo, Brazil
F. Carminati European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Casanova Díaz Laboratori Nazionali di Frascati, INFN, Frascati, Italy
J. Castillo Castellanos Commissariat à l’Energie Atomique, IRFU, Saclay, France
J. F. Castillo Hernandez Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
E. A. R. Casula Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
V. Catanescu National Institute for Physics and Nuclear Engineering, Bucharest, Romania
C. Cavicchioli European Organization for Nuclear Research (CERN), Geneva, Switzerland
C. Ceballos Sanchez Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
J. Cepila Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
P. Cerello Sezione INFN, Turin, Italy
B. Chang Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland Yonsei University, Seoul, South Korea
S. Chapeland European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. L. Charvet Commissariat à l’Energie Atomique, IRFU, Saclay, France
S. Chattopadhyay Variable Energy Cyclotron Centre, Kolkata, India
S. Chattopadhyay Saha Institute of Nuclear Physics, Kolkata, India
M. Cherney Physics Department, Creighton University, Omaha, Nebraska United States
C. Cheshkov European Organization for Nuclear Research (CERN), Geneva, Switzerland Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
B. Cheynis Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
V. Chibante Barroso European Organization for Nuclear Research (CERN), Geneva, Switzerland
D. D. Chinellato University of Houston, Houston, Texas United States
P. Chochula European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Chojnacki Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
S. Choudhury Variable Energy Cyclotron Centre, Kolkata, India
P. Christakoglou Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
C. H. Christensen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
P. Christiansen Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
T. Chujo University of Tsukuba, Tsukuba, Japan
S. U. Chung Pusan National University, Pusan, South Korea
C. Cicalo Sezione INFN, Cagliari, Italy
L. Cifarelli Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
F. Cindolo Sezione INFN, Bologna, Italy
J. Cleymans Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
F. Colamaria Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
D. Colella Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
A. Collu Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
G. Conesa Balbastre Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
Z. Conesa del Valle European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. E. Connors Yale University, New Haven, Connecticut United States
G. Contin Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
J. G. Contreras Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
T. M. Cormier Wayne State University, Detroit, Michigan United States
Y. Corrales Morales Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. Cortese Dipartimento di Scienze e Innovazione Tecnologica dell’Università del Piemonte Orientale and Gruppo Collegato INFN, Alessandria, Italy
I. Cortés Maldonado Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
M. R. Cosentino Lawrence Berkeley National Laboratory, Berkeley, California United States
F. Costa European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. E. Cotallo Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
E. Crescio Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
P. Crochet Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
E. Cruz Alaniz Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
R. Cruz Albino Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
E. Cuautle Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
L. Cunqueiro Laboratori Nazionali di Frascati, INFN, Frascati, Italy
A. Dainese Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Sezione INFN, Padova, Italy
R. Dang Central China Normal University, Wuhan, China
A. Danu Institute of Space Sciences (ISS), Bucharest, Romania
K. Das Saha Institute of Nuclear Physics, Kolkata, India
I. Das Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
S. Das Department of Physics and Centre for Astroparticle Physics and Space Science (CAPSS), Bose Institute, Kolkata, India
D. Das Saha Institute of Nuclear Physics, Kolkata, India
S. Dash Indian Institute of Technology Bombay (IIT), Mumbai, India
A. Dash Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
S. De Variable Energy Cyclotron Centre, Kolkata, India
G. O. V. de Barros Universidade de São Paulo (USP), São Paulo, Brazil
A. De Caro Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
G. de Cataldo Sezione INFN, Bari, Italy
J. de Cuveland Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. De Falco Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
D. De Gruttola Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
H. Delagrange SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
A. Deloff National Centre for Nuclear Studies, Warsaw, Poland
N. De Marco Sezione INFN, Turin, Italy
E. Dénes Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
S. De Pasquale Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
A. Deppman Universidade de São Paulo (USP), São Paulo, Brazil
G. D Erasmo Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
R. de Rooij Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
M. A. Diaz Corchero Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
D. Di Bari Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
T. Dietel Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
C. Di Giglio Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
S. Di Liberto Sezione INFN, Rome, Italy
A. Di Mauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
P. Di Nezza Laboratori Nazionali di Frascati, INFN, Frascati, Italy
R. Divià European Organization for Nuclear Research (CERN), Geneva, Switzerland
Ø. Djuvsland Department of Physics and Technology, University of Bergen, Bergen, Norway
A. Dobrin Division of Experimental High Energy Physics, University of Lund, Lund, Sweden Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands Wayne State University, Detroit, Michigan United States
T. Dobrowolski National Centre for Nuclear Studies, Warsaw, Poland
B. Dönigus Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
O. Dordic Department of Physics, University of Oslo, Oslo, Norway
A. K. Dubey Variable Energy Cyclotron Centre, Kolkata, India
A. Dubla Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
L. Ducroux Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
P. Dupieux Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
A. K. Dutta Majumdar Saha Institute of Nuclear Physics, Kolkata, India
D. Elia Sezione INFN, Bari, Italy
D. Emschermann Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
H. Engel Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
B. Erazmus European Organization for Nuclear Research (CERN), Geneva, Switzerland SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
H. A. Erdal Faculty of Engineering, Bergen University College, Bergen, Norway
D. Eschweiler Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
B. Espagnon Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Estienne SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
S. Esumi University of Tsukuba, Tsukuba, Japan
D. Evans School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
S. Evdokimov Institute for High Energy Physics, Protvino, Russia
G. Eyyubova Department of Physics, University of Oslo, Oslo, Norway
D. Fabris Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Sezione INFN, Padova, Italy
J. Faivre Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
D. Falchieri Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
A. Fantoni Laboratori Nazionali di Frascati, INFN, Frascati, Italy
M. Fasel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
D. Fehlker Department of Physics and Technology, University of Bergen, Bergen, Norway
L. Feldkamp Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
D. Felea Institute of Space Sciences (ISS), Bucharest, Romania
A. Feliciello Sezione INFN, Turin, Italy
B. Fenton-Olsen Lawrence Berkeley National Laboratory, Berkeley, California United States
G. Feofilov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
A. Fernández Téllez Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
A. Ferretti Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
A. Festanti Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
J. Figiel The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M. A. S. Figueredo Universidade de São Paulo (USP), São Paulo, Brazil
S. Filchagin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
D. Finogeev Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
F. M. Fionda Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
E. M. Fiore Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
E. Floratos Physics Department, University of Athens, Athens, Greece
M. Floris European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. Foertsch Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
P. Foka Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
S. Fokin Russian Research Centre Kurchatov Institute, Moscow, Russia
E. Fragiacomo Sezione INFN, Trieste, Italy
A. Francescon Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
U. Frankenfeld Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
U. Fuchs European Organization for Nuclear Research (CERN), Geneva, Switzerland
C. Furget Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
M. Fusco Girard Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
J. J. Gaardhøje Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
M. Gagliardi Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
A. Gago Sección Física, Departamento de Ciencias, Pontificia Universidad Católica del Perú, Lima, Peru
M. Gallio Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
D. R. Gangadharan Department of Physics, Ohio State University, Columbus, Ohio United States
P. Ganoti Oak Ridge National Laboratory, Oak Ridge, Tennessee United States
C. Garabatos Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
E. Garcia-Solis Chicago State University, Chicago, United States
C. Gargiulo European Organization for Nuclear Research (CERN), Geneva, Switzerland
I. Garishvili Lawrence Livermore National Laboratory, Livermore, California United States
J. Gerhard Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Germain SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
C. Geuna Commissariat à l’Energie Atomique, IRFU, Saclay, France
M. Gheata European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Space Sciences (ISS), Bucharest, Romania
A. Gheata European Organization for Nuclear Research (CERN), Geneva, Switzerland
B. Ghidini Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
P. Ghosh Variable Energy Cyclotron Centre, Kolkata, India
P. Gianotti Laboratori Nazionali di Frascati, INFN, Frascati, Italy
P. Giubellino European Organization for Nuclear Research (CERN), Geneva, Switzerland
E. Gladysz-Dziadus The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
P. Glässel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
R. Gomez Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico Universidad Autónoma de Sinaloa, Culiacán, Mexico
E. G. Ferreiro Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
L. H. González-Trueba Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
P. González-Zamora Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
S. Gorbunov Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Goswami Physics Department, University of Rajasthan, Jaipur, India
S. Gotovac Technical University of Split FESB, Split, Croatia
L. K. Graczykowski Warsaw University of Technology, Warsaw, Poland
R. Grajcarek Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A. Grelli Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Grigoras European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Grigoras European Organization for Nuclear Research (CERN), Geneva, Switzerland
V. Grigoriev Moscow Engineering Physics Institute, Moscow, Russia
A. Grigoryan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia
S. Grigoryan Joint Institute for Nuclear Research (JINR), Dubna, Russia
B. Grinyov Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
N. Grion Sezione INFN, Trieste, Italy
P. Gros Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
J. F. Grosse-Oetringhaus European Organization for Nuclear Research (CERN), Geneva, Switzerland
J.-Y. Grossiord Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
R. Grosso European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Guber Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
R. Guernane Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
B. Guerzoni Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
M. Guilbaud Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
K. Gulbrandsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
H. Gulkanyan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia
T. Gunji University of Tokyo, Tokyo, Japan
A. Gupta Physics Department, University of Jammu, Jammu, India
R. Gupta Physics Department, University of Jammu, Jammu, India
R. Haake Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
Ø. Haaland Department of Physics and Technology, University of Bergen, Bergen, Norway
C. Hadjidakis Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Haiduc Institute of Space Sciences (ISS), Bucharest, Romania
H. Hamagaki University of Tokyo, Tokyo, Japan
G. Hamar Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
B. H. Han Department of Physics, Sejong University, Seoul, South Korea
L. D. Hanratty School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. Hansen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
Z. Harmanová-Tóthová Faculty of Science, P.J. Šafárik University, Košice, Slovakia
J. W. Harris Yale University, New Haven, Connecticut United States
M. Hartig Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Harton Chicago State University, Chicago, United States
D. Hatzifotiadou Sezione INFN, Bologna, Italy
S. Hayashi University of Tokyo, Tokyo, Japan
A. Hayrapetyan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. T. Heckel Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Heide Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
H. Helstrup Faculty of Engineering, Bergen University College, Bergen, Norway
A. Herghelegiu National Institute for Physics and Nuclear Engineering, Bucharest, Romania
G. Herrera Corral Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
N. Herrmann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
B. A. Hess Eberhard Karls Universität Tübingen, Tübingen, Germany
K. F. Hetland Faculty of Engineering, Bergen University College, Bergen, Norway
B. Hicks Yale University, New Haven, Connecticut United States
B. Hippolyte Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
Y. Hori University of Tokyo, Tokyo, Japan
P. Hristov European Organization for Nuclear Research (CERN), Geneva, Switzerland
I. Hřivnáčová Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Huang Department of Physics and Technology, University of Bergen, Bergen, Norway
T. J. Humanic Department of Physics, Ohio State University, Columbus, Ohio United States
D. S. Hwang Department of Physics, Sejong University, Seoul, South Korea
R. Ichou Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
R. Ilkaev Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
I. Ilkiv National Centre for Nuclear Studies, Warsaw, Poland
M. Inaba University of Tsukuba, Tsukuba, Japan
E. Incani Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
G. M. Innocenti Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. G. Innocenti European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Ippolitov Russian Research Centre Kurchatov Institute, Moscow, Russia
M. Irfan Department of Physics, Aligarh Muslim University, Aligarh, India
C. Ivan Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Ivanov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. Ivanov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
V. Ivanov Petersburg Nuclear Physics Institute, Gatchina, Russia
O. Ivanytskyi Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
A. Jachołkowski Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
P. M. Jacobs Lawrence Berkeley National Laboratory, Berkeley, California United States
C. Jahnke Universidade de São Paulo (USP), São Paulo, Brazil
H. J. Jang Korea Institute of Science and Technology Information, Daejeon, South Korea
M. A. Janik Warsaw University of Technology, Warsaw, Poland
P. H. S. Y. Jayarathna University of Houston, Houston, Texas United States
S. Jena Indian Institute of Technology Bombay (IIT), Mumbai, India
D. M. Jha Wayne State University, Detroit, Michigan United States
R. T. Jimenez Bustamante Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
P. G. Jones School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
H. Jung Gangneung-Wonju National University, Gangneung, South Korea
A. Jusko School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. B. Kaidalov Institute for Theoretical and Experimental Physics, Moscow, Russia
S. Kalcher Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
P. Kaliňák Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
T. Kalliokoski Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
A. Kalweit European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. H. Kang Yonsei University, Seoul, South Korea
V. Kaplin Moscow Engineering Physics Institute, Moscow, Russia
S. Kar Variable Energy Cyclotron Centre, Kolkata, India
A. Karasu Uysal European Organization for Nuclear Research (CERN), Geneva, Switzerland KTO Karatay University, Konya, Turkey Yildiz Technical University, Istanbul, Turkey
O. Karavichev Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
T. Karavicheva Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
E. Karpechev Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
A. Kazantsev Russian Research Centre Kurchatov Institute, Moscow, Russia
U. Kebschull Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R. Keidel Zentrum für Technologietransfer und Telekommunikation (ZTT), Fachhochschule Worms, Worms, Germany
B. Ketzer Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany Technische Universität München, Munich, Germany
M. M. Khan Department of Physics, Aligarh Muslim University, Aligarh, India
P. Khan Saha Institute of Nuclear Physics, Kolkata, India
S. A. Khan Variable Energy Cyclotron Centre, Kolkata, India
K. H. Khan COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
A. Khanzadeev Petersburg Nuclear Physics Institute, Gatchina, Russia
Y. Kharlov Institute for High Energy Physics, Protvino, Russia
B. Kileng Faculty of Engineering, Bergen University College, Bergen, Norway
M. Kim Yonsei University, Seoul, South Korea
T. Kim Yonsei University, Seoul, South Korea
B. Kim Yonsei University, Seoul, South Korea
S. Kim Department of Physics, Sejong University, Seoul, South Korea
M. Kim Gangneung-Wonju National University, Gangneung, South Korea
D. J. Kim Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
J. S. Kim Gangneung-Wonju National University, Gangneung, South Korea
J. H. Kim Department of Physics, Sejong University, Seoul, South Korea
D. W. Kim Gangneung-Wonju National University, Gangneung, South Korea Korea Institute of Science and Technology Information, Daejeon, South Korea
S. Kirsch Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. Kisel Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
S. Kiselev Institute for Theoretical and Experimental Physics, Moscow, Russia
A. Kisiel Warsaw University of Technology, Warsaw, Poland
J. L. Klay California Polytechnic State University, San Luis Obispo, California United States
J. Klein Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C. Klein-Bösing Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
M. Kliemant Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Kluge European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. L. Knichel Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. G. Knospe Physics Department, The University of Texas at Austin, Austin, TX United States
M. K. Köhler Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
T. Kollegger Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Kolojvari V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
M. Kompaniets V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
V. Kondratiev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
N. Kondratyeva Moscow Engineering Physics Institute, Moscow, Russia
A. Konevskikh Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
V. Kovalenko V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
M. Kowalski The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
S. Kox Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
G. Koyithatta Meethaleveedu Indian Institute of Technology Bombay (IIT), Mumbai, India
J. Kral Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
I. Králik Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
F. Kramer Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Kravčáková Faculty of Science, P.J. Šafárik University, Košice, Slovakia
M. Krelina Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M. Kretz Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Krivda Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
F. Krizek Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
M. Krus Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
E. Kryshen Petersburg Nuclear Physics Institute, Gatchina, Russia
M. Krzewicki Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
V. Kucera Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
Y. Kucheriaev Russian Research Centre Kurchatov Institute, Moscow, Russia
T. Kugathasan European Organization for Nuclear Research (CERN), Geneva, Switzerland
C. Kuhn Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
P. G. Kuijer Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
I. Kulakov Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J. Kumar Indian Institute of Technology Bombay (IIT), Mumbai, India
P. Kurashvili National Centre for Nuclear Studies, Warsaw, Poland
A. Kurepin Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
A. B. Kurepin Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
A. Kuryakin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
V. Kushpil Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
S. Kushpil Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
H. Kvaerno Department of Physics, University of Oslo, Oslo, Norway
M. J. Kweon Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
Y. Kwon Yonsei University, Seoul, South Korea
P. Ladrón de Guevara Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
C. Lagana Fernandes Universidade de São Paulo (USP), São Paulo, Brazil
I. Lakomov Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
R. Langoy Department of Physics and Technology, University of Bergen, Bergen, Norway Vestfold University College, Tonsberg, Norway
S. L. La Pointe Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Lara Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Lardeux SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
P. La Rocca Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
R. Lea Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
M. Lechman European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. C. Lee Gangneung-Wonju National University, Gangneung, South Korea
G. R. Lee School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
I. Legrand European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Lehnert Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
R. C. Lemmon Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
M. Lenhardt Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
V. Lenti Sezione INFN, Bari, Italy
H. León Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
M. Leoncino Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
I. León Monzón Universidad Autónoma de Sinaloa, Culiacán, Mexico
P. Lévai Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
S. Li Central China Normal University, Wuhan, China Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
J. Lien Department of Physics and Technology, University of Bergen, Bergen, Norway Vestfold University College, Tonsberg, Norway
R. Lietava School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
S. Lindal Department of Physics, University of Oslo, Oslo, Norway
V. Lindenstruth Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C. Lippmann European Organization for Nuclear Research (CERN), Geneva, Switzerland Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. A. Lisa Department of Physics, Ohio State University, Columbus, Ohio United States
H. M. Ljunggren Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
D. F. Lodato Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
P. I. Loenne Department of Physics and Technology, University of Bergen, Bergen, Norway
V. R. Loggins Wayne State University, Detroit, Michigan United States
V. Loginov Moscow Engineering Physics Institute, Moscow, Russia
D. Lohner Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C. Loizides Lawrence Berkeley National Laboratory, Berkeley, California United States
K. K. Loo Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
X. Lopez Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
E. López Torres Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
G. Løvhøiden Department of Physics, University of Oslo, Oslo, Norway
X.-G. Lu Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
P. Luettig Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Lunardon Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
J. Luo Central China Normal University, Wuhan, China
G. Luparello Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Luzzi European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Ma Yale University, New Haven, Connecticut United States
K. Ma Central China Normal University, Wuhan, China
D. M. Madagodahettige-Don University of Houston, Houston, Texas United States
A. Maevskaya Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
M. Mager European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, Germany
D. P. Mahapatra Institute of Physics, Bhubaneswar, India
A. Maire Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Malaev Petersburg Nuclear Physics Institute, Gatchina, Russia
I. Maldonado Cervantes Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
L. Malinina Joint Institute for Nuclear Research (JINR), Dubna, Russia
D. Mal’Kevich Institute for Theoretical and Experimental Physics, Moscow, Russia
P. Malzacher Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. Mamonov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
L. Manceau Sezione INFN, Turin, Italy
L. Mangotra Physics Department, University of Jammu, Jammu, India
V. Manko Russian Research Centre Kurchatov Institute, Moscow, Russia
F. Manso Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
V. Manzari Sezione INFN, Bari, Italy
Y. Mao Central China Normal University, Wuhan, China
M. Marchisone Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
J. Mareš Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
G. V. Margagliotti Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy Sezione INFN, Trieste, Italy
A. Margotti Sezione INFN, Bologna, Italy
A. Marín Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
C. Markert Physics Department, The University of Texas at Austin, Austin, TX United States
M. Marquard Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. Martashvili University of Tennessee, Knoxville, Tennessee United States
N. A. Martin Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
P. Martinengo European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. I. Martínez Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
G. Martínez García SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
Y. Martynov Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
A. Mas SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
S. Masciocchi Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Masera Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
A. Masoni Sezione INFN, Cagliari, Italy
L. Massacrier SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
A. Mastroserio Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
A. Matyja The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
C. Mayer The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
J. Mazer University of Tennessee, Knoxville, Tennessee United States
R. Mazumder Indian Institute of Technology Indore (IITI), Indore, India
M. A. Mazzoni Sezione INFN, Rome, Italy
F. Meddi Dipartimento di Fisica dell’Università ‘La Sapienza’ and Sezione INFN, Rome, Italy
A. Menchaca-Rocha Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
J. Mercado Pérez Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Meres Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
Y. Miake University of Tsukuba, Tsukuba, Japan
K. Mikhaylov Institute for Theoretical and Experimental Physics, Moscow, Russia Joint Institute for Nuclear Research (JINR), Dubna, Russia
L. Milano Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Milosevic Department of Physics, University of Oslo, Oslo, Norway
A. Mischke Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
A. N. Mishra Indian Institute of Technology Indore (IITI), Indore, India Physics Department, University of Rajasthan, Jaipur, India
D. Miśkowiec Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
C. Mitu Institute of Space Sciences (ISS), Bucharest, Romania
S. Mizuno University of Tsukuba, Tsukuba, Japan
J. Mlynarz Wayne State University, Detroit, Michigan United States
B. Mohanty National Institute of Science Education and Research, Bhubaneswar, India Variable Energy Cyclotron Centre, Kolkata, India
L. Molnar Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
L. Montaño Zetina Centro de Investigación y de Estudios Avanzados (CINVESTAV), Mexico City and Mérida, Mexico
M. Monteno Sezione INFN, Turin, Italy
E. Montes Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
T. Moon Yonsei University, Seoul, South Korea
M. Morando Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
D. A. Moreira De Godoy Universidade de São Paulo (USP), São Paulo, Brazil
S. Moretto Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
A. Morreale Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
A. Morsch European Organization for Nuclear Research (CERN), Geneva, Switzerland
V. Muccifora Laboratori Nazionali di Frascati, INFN, Frascati, Italy
E. Mudnic Technical University of Split FESB, Split, Croatia
S. Muhuri Variable Energy Cyclotron Centre, Kolkata, India
M. Mukherjee Variable Energy Cyclotron Centre, Kolkata, India
H. Müller European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. G. Munhoz Universidade de São Paulo (USP), São Paulo, Brazil
S. Murray Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
L. Musa European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Musinsky Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
B. K. Nandi Indian Institute of Technology Bombay (IIT), Mumbai, India
R. Nania Sezione INFN, Bologna, Italy
E. Nappi Sezione INFN, Bari, Italy
C. Nattrass University of Tennessee, Knoxville, Tennessee United States
T. K. Nayak Variable Energy Cyclotron Centre, Kolkata, India
S. Nazarenko Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
A. Nedosekin Institute for Theoretical and Experimental Physics, Moscow, Russia
M. Nicassio Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
M. Niculescu European Organization for Nuclear Research (CERN), Geneva, Switzerland Institute of Space Sciences (ISS), Bucharest, Romania
B. S. Nielsen Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
T. Niida University of Tsukuba, Tsukuba, Japan
S. Nikolaev Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Nikolic Rudjer Bošković Institute, Zagreb, Croatia
S. Nikulin Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Nikulin Petersburg Nuclear Physics Institute, Gatchina, Russia
B. S. Nilsen Physics Department, Creighton University, Omaha, Nebraska United States
M. S. Nilsson Department of Physics, University of Oslo, Oslo, Norway
F. Noferini Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Sezione INFN, Bologna, Italy
P. Nomokonov Joint Institute for Nuclear Research (JINR), Dubna, Russia
G. Nooren Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
A. Nyanin Russian Research Centre Kurchatov Institute, Moscow, Russia
A. Nyatha Indian Institute of Technology Bombay (IIT), Mumbai, India
C. Nygaard Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
J. Nystrand Department of Physics and Technology, University of Bergen, Bergen, Norway
A. Ochirov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
H. Oeschler European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut für Kernphysik, Technische Universität Darmstadt, Darmstadt, Germany Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S. Oh Yale University, New Haven, Connecticut United States
S. K. Oh Gangneung-Wonju National University, Gangneung, South Korea
J. Oleniacz Warsaw University of Technology, Warsaw, Poland
A. C. Oliveira Da Silva Universidade de São Paulo (USP), São Paulo, Brazil
J. Onderwaater Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
C. Oppedisano Sezione INFN, Turin, Italy
A. Ortiz Velasquez Division of Experimental High Energy Physics, University of Lund, Lund, Sweden Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
A. Oskarsson Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
P. Ostrowski Warsaw University of Technology, Warsaw, Poland
J. Otwinowski Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
K. Oyama Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
K. Ozawa University of Tokyo, Tokyo, Japan
Y. Pachmayer Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Pachr Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
F. Padilla Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. Pagano Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
G. Paić Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico
F. Painke Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
C. Pajares Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
S. K. Pal Variable Energy Cyclotron Centre, Kolkata, India
A. Palaha School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
A. Palmeri Sezione INFN, Catania, Italy
V. Papikyan A. I. Alikhanyan National Science Laboratory (Yerevan Physics Institute) Foundation, Yerevan, Armenia
G. S. Pappalardo Sezione INFN, Catania, Italy
W. J. Park Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
A. Passfeld Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
D. I. Patalakha Institute for High Energy Physics, Protvino, Russia
V. Paticchio Sezione INFN, Bari, Italy
B. Paul Saha Institute of Nuclear Physics, Kolkata, India
A. Pavlinov Wayne State University, Detroit, Michigan United States
T. Pawlak Warsaw University of Technology, Warsaw, Poland
T. Peitzmann Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
H. Pereira Da Costa Commissariat à l’Energie Atomique, IRFU, Saclay, France
E. Pereira De Oliveira Filho Universidade de São Paulo (USP), São Paulo, Brazil
D. Peresunko Russian Research Centre Kurchatov Institute, Moscow, Russia
C. E. Pérez Lara Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
D. Perrino Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
W. Peryt Warsaw University of Technology, Warsaw, Poland
A. Pesci Sezione INFN, Bologna, Italy
Y. Pestov Budker Institute for Nuclear Physics, Novosibirsk, Russia
V. Petráček Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M. Petran Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
M. Petris National Institute for Physics and Nuclear Engineering, Bucharest, Romania
P. Petrov School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
M. Petrovici National Institute for Physics and Nuclear Engineering, Bucharest, Romania
C. Petta Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
S. Piano Sezione INFN, Trieste, Italy
M. Pikna Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
P. Pillot SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
O. Pinazza European Organization for Nuclear Research (CERN), Geneva, Switzerland
L. Pinsky University of Houston, Houston, Texas United States
N. Pitz Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D. B. Piyarathna University of Houston, Houston, Texas United States
M. Planinic Rudjer Bošković Institute, Zagreb, Croatia
M. Płoskoń Lawrence Berkeley National Laboratory, Berkeley, California United States
J. Pluta Warsaw University of Technology, Warsaw, Poland
T. Pocheptsov Joint Institute for Nuclear Research (JINR), Dubna, Russia
S. Pochybova Wigner Research Centre for Physics, Hungarian Academy of Sciences, Budapest, Hungary
P. L. M. Podesta-Lerma Universidad Autónoma de Sinaloa, Culiacán, Mexico
M. G. Poghosyan European Organization for Nuclear Research (CERN), Geneva, Switzerland
K. Polák Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
B. Polichtchouk Institute for High Energy Physics, Protvino, Russia
N. Poljak Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands Rudjer Bošković Institute, Zagreb, Croatia
A. Pop National Institute for Physics and Nuclear Engineering, Bucharest, Romania
S. Porteboeuf-Houssais Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
V. Pospíšil Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
B. Potukuchi Physics Department, University of Jammu, Jammu, India
S. K. Prasad Wayne State University, Detroit, Michigan United States
R. Preghenella Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Sezione INFN, Bologna, Italy
F. Prino Sezione INFN, Turin, Italy
C. A. Pruneau Wayne State University, Detroit, Michigan United States
I. Pshenichnov Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
G. Puddu Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
V. Punin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
J. Putschke Wayne State University, Detroit, Michigan United States
H. Qvigstad Department of Physics, University of Oslo, Oslo, Norway
A. Rachevski Sezione INFN, Trieste, Italy
A. Rademakers European Organization for Nuclear Research (CERN), Geneva, Switzerland
T. S. Räihä Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
J. Rak Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
A. Rakotozafindrabe Commissariat à l’Energie Atomique, IRFU, Saclay, France
L. Ramello Dipartimento di Scienze e Innovazione Tecnologica dell’Università del Piemonte Orientale and Gruppo Collegato INFN, Alessandria, Italy
S. Raniwala Physics Department, University of Rajasthan, Jaipur, India
R. Raniwala Physics Department, University of Rajasthan, Jaipur, India
S. S. Räsänen Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
B. T. Rascanu Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D. Rathee Physics Department, Panjab University, Chandigarh, India
W. Rauch European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. W. Rauf COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
V. Razazi Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
K. F. Read University of Tennessee, Knoxville, Tennessee United States
J. S. Real Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
K. Redlich National Centre for Nuclear Studies, Warsaw, Poland
R. J. Reed Yale University, New Haven, Connecticut United States
A. Rehman Department of Physics and Technology, University of Bergen, Bergen, Norway
P. Reichelt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
M. Reicher Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
R. Renfordt Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. R. Reolon Laboratori Nazionali di Frascati, INFN, Frascati, Italy
A. Reshetin Institute for Nuclear Research, Academy of Sciences, Moscow, Russia
F. Rettig Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J.-P. Revol European Organization for Nuclear Research (CERN), Geneva, Switzerland
K. Reygers Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
L. Riccati Sezione INFN, Turin, Italy
R. A. Ricci Laboratori Nazionali di Legnaro, INFN, Legnaro, Italy
T. Richert Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
M. Richter Department of Physics, University of Oslo, Oslo, Norway
P. Riedler European Organization for Nuclear Research (CERN), Geneva, Switzerland
W. Riegler European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Riggi Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy Sezione INFN, Catania, Italy
A. Rivetti Sezione INFN, Turin, Italy
M. Rodríguez Cahuantzi Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
A. Rodriguez Manso Nikhef, National Institute for Subatomic Physics, Amsterdam, Netherlands
K. Røed Department of Physics and Technology, University of Bergen, Bergen, Norway Department of Physics, University of Oslo, Oslo, Norway
E. Rogochaya Joint Institute for Nuclear Research (JINR), Dubna, Russia
D. Rohr Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
D. Röhrich Department of Physics and Technology, University of Bergen, Bergen, Norway
R. Romita Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany Nuclear Physics Group, STFC Daresbury Laboratory, Daresbury, United Kingdom
F. Ronchetti Laboratori Nazionali di Frascati, INFN, Frascati, Italy
P. Rosnet Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
S. Rossegger European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Rossi European Organization for Nuclear Research (CERN), Geneva, Switzerland
P. Roy Saha Institute of Nuclear Physics, Kolkata, India
C. Roy Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
A. J. Rubio Montero Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain
R. Rui Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
R. Russo Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
E. Ryabinkin Russian Research Centre Kurchatov Institute, Moscow, Russia
A. Rybicki The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
S. Sadovsky Institute for High Energy Physics, Protvino, Russia
K. Šafařík European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Sahoo Indian Institute of Technology Indore (IITI), Indore, India
P. K. Sahu Institute of Physics, Bhubaneswar, India
J. Saini Variable Energy Cyclotron Centre, Kolkata, India
H. Sakaguchi Hiroshima University, Hiroshima, Japan
S. Sakai Lawrence Berkeley National Laboratory, Berkeley, California United States
D. Sakata University of Tsukuba, Tsukuba, Japan
C. A. Salgado Departamento de Física de Partículas and IGFAE, Universidad de Santiago de Compostela, Santiago de Compostela, Spain
J. Salzwedel Department of Physics, Ohio State University, Columbus, Ohio United States
S. Sambyal Physics Department, University of Jammu, Jammu, India
V. Samsonov Petersburg Nuclear Physics Institute, Gatchina, Russia
X. Sanchez Castro Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
L. Šándor Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia
A. Sandoval Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
M. Sano University of Tsukuba, Tsukuba, Japan
G. Santagati Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Catania, Italy
R. Santoro Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. Sarkamo Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
D. Sarkar Variable Energy Cyclotron Centre, Kolkata, India
E. Scapparone Sezione INFN, Bologna, Italy
F. Scarlassara Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
R. P. Scharenberg Purdue University, West Lafayette, Indiana United States
C. Schiaua National Institute for Physics and Nuclear Engineering, Bucharest, Romania
R. Schicker Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
H. R. Schmidt Eberhard Karls Universität Tübingen, Tübingen, Germany
C. Schmidt Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
S. Schuchmann Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
J. Schukraft European Organization for Nuclear Research (CERN), Geneva, Switzerland
T. Schuster Yale University, New Haven, Connecticut United States
Y. Schutz European Organization for Nuclear Research (CERN), Geneva, Switzerland SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
K. Schwarz Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
K. Schweda Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
G. Scioli Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
E. Scomparin Sezione INFN, Turin, Italy
R. Scott University of Tennessee, Knoxville, Tennessee United States
P. A. Scott School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
G. Segato Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
I. Selyuzhenkov Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
S. Senyukov Institut Pluridisciplinaire Hubert Curien (IPHC), Université de Strasbourg, CNRS-IN2P3, Strasbourg, France
J. Seo Pusan National University, Pusan, South Korea
S. Serci Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
E. Serradilla Centro de Investigaciones Energéticas Medioambientales y Tecnológicas (CIEMAT), Madrid, Spain Instituto de Física, Universidad Nacional Autónoma de México, Mexico City, Mexico
A. Sevcenco Institute of Space Sciences (ISS), Bucharest, Romania
A. Shabetai SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
G. Shabratova Joint Institute for Nuclear Research (JINR), Dubna, Russia
R. Shahoyan European Organization for Nuclear Research (CERN), Geneva, Switzerland
S. Sharma Physics Department, University of Jammu, Jammu, India
N. Sharma University of Tennessee, Knoxville, Tennessee United States
S. Rohni Physics Department, University of Jammu, Jammu, India
K. Shigaki Hiroshima University, Hiroshima, Japan
K. Shtejer Centro de Aplicaciones Tecnológicas y Desarrollo Nuclear (CEADEN), Havana, Cuba
Y. Sibiriak Russian Research Centre Kurchatov Institute, Moscow, Russia
E. Sicking Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
S. Siddhanta Sezione INFN, Cagliari, Italy
T. Siemiarczuk National Centre for Nuclear Studies, Warsaw, Poland
D. Silvermyr Oak Ridge National Laboratory, Oak Ridge, Tennessee United States
C. Silvestre Laboratoire de Physique Subatomique et de Cosmologie (LPSC), Université Joseph Fourier, CNRS-IN2P3, Institut Polytechnique de Grenoble, Grenoble, France
G. Simatovic Instituto de Ciencias Nucleares, Universidad Nacional Autónoma de México, Mexico City, Mexico Rudjer Bošković Institute, Zagreb, Croatia
G. Simonetti European Organization for Nuclear Research (CERN), Geneva, Switzerland
R. Singaraju Variable Energy Cyclotron Centre, Kolkata, India
R. Singh Physics Department, University of Jammu, Jammu, India
S. Singha National Institute of Science Education and Research, Bhubaneswar, India Variable Energy Cyclotron Centre, Kolkata, India
V. Singhal Variable Energy Cyclotron Centre, Kolkata, India
T. Sinha Saha Institute of Nuclear Physics, Kolkata, India
B. C. Sinha Variable Energy Cyclotron Centre, Kolkata, India
B. Sitar Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
M. Sitta Dipartimento di Scienze e Innovazione Tecnologica dell’Università del Piemonte Orientale and Gruppo Collegato INFN, Alessandria, Italy
T. B. Skaali Department of Physics, University of Oslo, Oslo, Norway
K. Skjerdal Department of Physics and Technology, University of Bergen, Bergen, Norway
R. Smakal Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
N. Smirnov Yale University, New Haven, Connecticut United States
R. J. M. Snellings Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
C. Søgaard Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
R. Soltz Lawrence Livermore National Laboratory, Livermore, California United States
M. Song Yonsei University, Seoul, South Korea
J. Song Pusan National University, Pusan, South Korea
C. Soos European Organization for Nuclear Research (CERN), Geneva, Switzerland
F. Soramel Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
I. Sputowska The Henryk Niewodniczanski Institute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
M. Spyropoulou-Stassinaki Physics Department, University of Athens, Athens, Greece
B. K. Srivastava Purdue University, West Lafayette, Indiana United States
J. Stachel Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
I. Stan Institute of Space Sciences (ISS), Bucharest, Romania
G. Stefanek National Centre for Nuclear Studies, Warsaw, Poland
M. Steinpreis Department of Physics, Ohio State University, Columbus, Ohio United States
E. Stenlund Division of Experimental High Energy Physics, University of Lund, Lund, Sweden
G. Steyn Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
J. H. Stiller Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
D. Stocco SUBATECH, Ecole des Mines de Nantes, Université de Nantes, CNRS-IN2P3, Nantes, France
M. Stolpovskiy Institute for High Energy Physics, Protvino, Russia
P. Strmen Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
A. A. P. Suaide Universidade de São Paulo (USP), São Paulo, Brazil
M. A. Subieta Vásquez Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
T. Sugitate Hiroshima University, Hiroshima, Japan
C. Suire Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
M. Suleymanov COMSATS Institute of Information Technology (CIIT), Islamabad, Pakistan
R. Sultanov Institute for Theoretical and Experimental Physics, Moscow, Russia
M. Šumbera Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
T. Susa Rudjer Bošković Institute, Zagreb, Croatia
T. J. M. Symons Lawrence Berkeley National Laboratory, Berkeley, California United States
A. Szanto de Toledo Universidade de São Paulo (USP), São Paulo, Brazil
I. Szarka Faculty of Mathematics, Physics and Informatics, Comenius University, Bratislava, Slovakia
A. Szczepankiewicz European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. Szymański Warsaw University of Technology, Warsaw, Poland
J. Takahashi Universidade Estadual de Campinas (UNICAMP), Campinas, Brazil
M. A. Tangaro Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
J. D. Tapia Takaki Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
A. Tarantola Peloni Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
A. Tarazona Martinez European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Tauro European Organization for Nuclear Research (CERN), Geneva, Switzerland
G. Tejeda Muñoz Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
A. Telesca European Organization for Nuclear Research (CERN), Geneva, Switzerland
A. Ter Minasyan Russian Research Centre Kurchatov Institute, Moscow, Russia
C. Terrevoli Dipartimento Interateneo di Fisica ‘M. Merlin’ and Sezione INFN, Bari, Italy
J. Thäder Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
D. Thomas Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
R. Tieulent Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
A. R. Timmins University of Houston, Houston, Texas United States
D. Tlusty Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
A. Toia Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy Frankfurt Institute for Advanced Studies, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany Sezione INFN, Padova, Italy
H. Torii University of Tokyo, Tokyo, Japan
L. Toscano Sezione INFN, Turin, Italy
V. Trubnikov Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
D. Truesdale Department of Physics, Ohio State University, Columbus, Ohio United States
W. H. Trzaska Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
T. Tsuji University of Tokyo, Tokyo, Japan
A. Tumkin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
R. Turrisi Sezione INFN, Padova, Italy
T. S. Tveter Department of Physics, University of Oslo, Oslo, Norway
J. Ulery Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
K. Ullaland Department of Physics and Technology, University of Bergen, Bergen, Norway
J. Ulrich Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany Kirchhoff-Institut für Physik, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
A. Uras Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
G. M. Urciuoli Sezione INFN, Rome, Italy
G. L. Usai Dipartimento di Fisica dell’Università and Sezione INFN, Cagliari, Italy
M. Vajzer Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic Nuclear Physics Institute, Academy of Sciences of the Czech Republic, Řež u Prahy, Czech Republic
M. Vala Institute of Experimental Physics, Slovak Academy of Sciences, Košice, Slovakia Joint Institute for Nuclear Research (JINR), Dubna, Russia
L. Valencia Palomo Institut de Physique Nucléaire d’Orsay (IPNO), Université Paris-Sud, CNRS-IN2P3, Orsay, France
S. Vallero Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
P. Vande Vyvre European Organization for Nuclear Research (CERN), Geneva, Switzerland
J. W. Van Hoorne European Organization for Nuclear Research (CERN), Geneva, Switzerland
M. van Leeuwen Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
L. Vannucci Laboratori Nazionali di Legnaro, INFN, Legnaro, Italy
A. Vargas Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
R. Varma Indian Institute of Technology Bombay (IIT), Mumbai, India
M. Vasileiou Physics Department, University of Athens, Athens, Greece
A. Vasiliev Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Vechernin V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
M. Veldhoen Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
M. Venaruzzo Dipartimento di Fisica dell’Università and Sezione INFN, Trieste, Italy
E. Vercellin Dipartimento di Fisica dell’Università and Sezione INFN, Turin, Italy
S. Vergara Benemérita Universidad Autónoma de Puebla, Puebla, Mexico
R. Vernet Centre de Calcul de l’IN2P3, Villeurbanne, France
M. Verweij Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
L. Vickovic Technical University of Split FESB, Split, Croatia
G. Viesti Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Padova, Italy
J. Viinikainen Helsinki Institute of Physics (HIP) and University of Jyväskylä, Jyväskylä, Finland
Z. Vilakazi Physics Department, University of Cape Town and iThemba LABS, National Research Foundation, Somerset West, South Africa
O. Villalobos Baillie School of Physics and Astronomy, University of Birmingham, Birmingham, United Kingdom
Y. Vinogradov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
L. Vinogradov V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
A. Vinogradov Russian Research Centre Kurchatov Institute, Moscow, Russia
T. Virgili Dipartimento di Fisica ‘E.R. Caianiello’ dell’Università and Gruppo Collegato INFN, Salerno, Italy
Y. P. Viyogi Variable Energy Cyclotron Centre, Kolkata, India
A. Vodopyanov Joint Institute for Nuclear Research (JINR), Dubna, Russia
M. A. Völkl Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
S. Voloshin Wayne State University, Detroit, Michigan United States
K. Voloshin Institute for Theoretical and Experimental Physics, Moscow, Russia
G. Volpe European Organization for Nuclear Research (CERN), Geneva, Switzerland
B. von Haller European Organization for Nuclear Research (CERN), Geneva, Switzerland
I. Vorobyev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
D. Vranic European Organization for Nuclear Research (CERN), Geneva, Switzerland Research Division and ExtreMe Matter Institute EMMI, GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany
J. Vrláková Faculty of Science, P.J. Šafárik University, Košice, Slovakia
B. Vulpescu Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France
A. Vyushin Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
V. Wagner Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
B. Wagner Department of Physics and Technology, University of Bergen, Bergen, Norway
R. Wan Central China Normal University, Wuhan, China
Y. Wang Central China Normal University, Wuhan, China
Y. Wang Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
M. Wang Central China Normal University, Wuhan, China
K. Watanabe University of Tsukuba, Tsukuba, Japan
M. Weber University of Houston, Houston, Texas United States
J. P. Wessels European Organization for Nuclear Research (CERN), Geneva, Switzerland Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
U. Westerhoff Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
J. Wiechula Eberhard Karls Universität Tübingen, Tübingen, Germany
J. Wikne Department of Physics, University of Oslo, Oslo, Norway
M. Wilde Institut für Kernphysik, Westfälische Wilhelms-Universität Münster, Münster, Germany
G. Wilk National Centre for Nuclear Studies, Warsaw, Poland
M. C. S. Williams Sezione INFN, Bologna, Italy
B. Windelband Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
C. G. Yaldo Wayne State University, Detroit, Michigan United States
Y. Yamaguchi University of Tokyo, Tokyo, Japan
S. Yang Department of Physics and Technology, University of Bergen, Bergen, Norway
P. Yang Central China Normal University, Wuhan, China
H. Yang Commissariat à l’Energie Atomique, IRFU, Saclay, France Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
S. Yasnopolskiy Russian Research Centre Kurchatov Institute, Moscow, Russia
J. Yi Pusan National University, Pusan, South Korea
Z. Yin Central China Normal University, Wuhan, China
I.-K. Yoo Pusan National University, Pusan, South Korea
J. Yoon Yonsei University, Seoul, South Korea
X. Yuan Central China Normal University, Wuhan, China
I. Yushmanov Russian Research Centre Kurchatov Institute, Moscow, Russia
V. Zaccolo Niels Bohr Institute, University of Copenhagen, Copenhagen, Denmark
C. Zach Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, Prague, Czech Republic
C. Zampolli Sezione INFN, Bologna, Italy
S. Zaporozhets Joint Institute for Nuclear Research (JINR), Dubna, Russia
A. Zarochentsev V. Fock Institute for Physics, St. Petersburg State University, St. Petersburg, Russia
P. Závada Institute of Physics, Academy of Sciences of the Czech Republic, Prague, Czech Republic
N. Zaviyalov Russian Federal Nuclear Center (VNIIEF), Sarov, Russia
H. Zbroszczyk Warsaw University of Technology, Warsaw, Poland
P. Zelnicek Institut für Informatik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany
I. S. Zgura Institute of Space Sciences (ISS), Bucharest, Romania
M. Zhalov Petersburg Nuclear Physics Institute, Gatchina, Russia
Y. Zhang Central China Normal University, Wuhan, China
H. Zhang Central China Normal University, Wuhan, China
X. Zhang Central China Normal University, Wuhan, China Laboratoire de Physique Corpusculaire (LPC), Clermont Université, Université Blaise Pascal, CNRS–IN2P3, Clermont-Ferrand, France Lawrence Berkeley National Laboratory, Berkeley, California United States
D. Zhou Central China Normal University, Wuhan, China
Y. Zhou Nikhef, National Institute for Subatomic Physics and Institute for Subatomic Physics of Utrecht University, Utrecht, Netherlands
F. Zhou Central China Normal University, Wuhan, China
H. Zhu Central China Normal University, Wuhan, China
J. Zhu Central China Normal University, Wuhan, China
X. Zhu Central China Normal University, Wuhan, China
J. Zhu Central China Normal University, Wuhan, China
A. Zichichi Centro Fermi - Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Rome, Italy Dipartimento di Fisica e Astronomia dell’Università and Sezione INFN, Bologna, Italy
A. Zimmermann Physikalisches Institut, Ruprecht-Karls-Universität Heidelberg, Heidelberg, Germany
G. Zinovjev Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
Y. Zoccarato Université de Lyon, Université Lyon 1, CNRS/IN2P3, IPN-Lyon, Villeurbanne, France
M. Zynovyev Bogolyubov Institute for Theoretical Physics, Kiev, Ukraine
M. Zyzak Institut für Kernphysik, Johann Wolfgang Goethe-Universität Frankfurt, Frankfurt, Germany

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J/ψ elliptic flow in Pb-Pb collisions at √(s(NN))=2.76 TeV

We report on the first measurement of inclusive J/ψ elliptic flow v2 in heavy-ion collisions at the LHC. The measurement is performed with the ALICE detector in Pb-Pb collisions at √(s(NN))=2.76 TeV in the rapidity range 2.5<y<4.0. The dependence of the J/ψ v2 on the collision centrality and on the J/ψ transverse momentum is studied in the range 0≤p(T)<10 GeV/c. For semicentral Pb-Pb collisions at √(s(NN))=2.76 TeV, an indication of nonzero v2 is observed with a largest measured value of v2=0.116±0.046(stat)±0.029(syst) for J/ψ in the transverse momentum range 2≤p(T)<4 GeV/c. The elliptic flow measurement complements the previously reported ALICE results on the inclusive J/ψ nuclear modification factor and favors the scenario of a significant fraction of J/ψ production from charm quarks in a deconfined partonic phase.

[Phlebology in German departments of dermatology. An analysis on behalf of the German Society of Phlebology]

BACKGROUND

Phlebologic diseases have become extremely common and have major socio-economic impact. However, the percentage of dermatologists working in phlebology appears to be decreasing according to the data of the German Society of Phlebology (DGP).

METHODS

To investigate the reasons for this development, we--on behalf of the DGP--sent a questionnaire to 120 German Departments of Dermatology in autumn 2012.

RESULTS

In 76 returned questionnaires, the number of physicians with additional fellowship training in phlebology averaged 1.5; the average number of those who fulfill the criteria for training fellows in phlebology was 0.9. In 71.1 % of the departments there was a phlebologist. A special phlebologic outpatient clinic existed in 73.7 % of the departments. Sonography with Doppler (89.5 %) and duplex (86.8 %) was used as the most frequent diagnostic tool. For therapy, compression (94.7 %), sclerotherapy (liquid 78.9 %, foam 63.2 %, catheter 18.4 %), endoluminal thermic procedures (radio wave 28.9 %, laser 17.1 %) and surgery (especially crossectomy and stripping 67.1 %, phlebectomy of tributaries 75 %) were used. The average number of treatments was very heterogenous in the different departments.

CONCLUSIONS

Phlebology definitely plays an important role in dermatology. Most departments fulfill the formal criteria for the license to conduct advanced training in phlebology. A wide spectrum of phlebological diagnostic and therapeutic procedures is available.

D meson elliptic flow in noncentral Pb-Pb collisions at sqrt[sNN]=2.76 Tev

Azimuthally anisotropic distributions of D0, D+, and D*+ mesons were studied in the central rapidity region (|y|<0.8) in Pb-Pb collisions at a center-of-mass energy sqrt[sNN]=2.76  TeV per nucleon-nucleon collision, with the ALICE detector at the LHC. The second Fourier coefficient v2 (commonly denoted elliptic flow) was measured in the centrality class 30%-50% as a function of the D meson transverse momentum pT, in the range 2-16  GeV/c. The measured v2 of D mesons is comparable in magnitude to that of light-flavor hadrons. It is positive in the range 2<pT<6  GeV/c with 5.7σ significance, based on the combination of statistical and systematic uncertainties.

Measurement of inelastic, single- and double-diffraction cross sections in proton-proton collisions at the LHC with ALICE

Measurements of cross sections of inelastic and diffractive processes in proton-proton collisions at LHC energies were carried out with the ALICE detector. The fractions of diffractive processes in inelastic collisions were determined from a study of gaps in charged particle pseudorapidity distributions: for single diffraction (diffractive mass MX <200 GeV/c2) [Formula: see text], and [Formula: see text], respectively at centre-of-mass energies [Formula: see text]; for double diffraction (for a pseudorapidity gap Δη>3) σDD/σINEL=0.11±0.03,0.12±0.05, and [Formula: see text], respectively at [Formula: see text]. To measure the inelastic cross section, beam properties were determined with van der Meer scans, and, using a simulation of diffraction adjusted to data, the following values were obtained: [Formula: see text] mb at [Formula: see text] and [Formula: see text] at [Formula: see text]. The single- and double-diffractive cross sections were calculated combining relative rates of diffraction with inelastic cross sections. The results are compared to previous measurements at proton-antiproton and proton-proton colliders at lower energies, to measurements by other experiments at the LHC, and to theoretical models.

Net-charge fluctuations in Pb-Pb collisions at sqrt[sNN]=2.76 TeV

We report the first measurement of the net-charge fluctuations in Pb-Pb collisions at sqrt[sNN]=2.76  TeV, measured with the ALICE detector at the CERN Large Hadron Collider. The dynamical fluctuations per unit entropy are observed to decrease when going from peripheral to central collisions. An additional reduction in the amount of fluctuations is seen in comparison to the results from lower energies. We examine the dependence of fluctuations on the pseudorapidity interval, which may account for the dilution of fluctuations during the evolution of the system. We find that the fluctuations at the LHC are smaller compared to the measurements at the BNL Relativistic Heavy Ion Collider, and as such, closer to what has been theoretically predicted for the formation of a quark-gluon plasma.

Transverse momentum distribution and nuclear modification factor of charged particles in p+Pb collisions at sqrt[s(NN)] = 5.02 TeV

The transverse momentum (p(T)) distribution of primary charged particles is measured in minimum bias (non-single-diffractive) p+Pb collisions at sqrt[s(NN)]=5.02 TeV with the ALICE detector at the LHC. The p(T) spectra measured near central rapidity in the range 0.5<p(T) <20 GeV/c exhibit a weak pseudorapidity dependence. The nuclear modification factor R(pPb) is consistent with unity for p(T) above 2 GeV/c. This measurement indicates that the strong suppression of hadron production at high p(T) observed in Pb+Pb collisions at the LHC is not due to an initial-state effect. The measurement is compared to theoretical calculations.

Pseudorapidity density of charged particles in p+Pb collisions at √(s(NN))=5.02 TeV

The charged-particle pseudorapidity density measured over four units of pseudorapidity in nonsingle-diffractive p+Pb collisions at a center-of-mass energy per nucleon pair √(s(NN))=5.02 TeV is presented. The average value at midrapidity is measured to be 16.81±0.71 (syst), which corresponds to 2.14±0.17 (syst) per participating nucleon, calculated with the Glauber model. This is 16% lower than in nonsingle-diffractive pp collisions interpolated to the same collision energy and 84% higher than in d+Au collisions at s√(s(NN))=0.2 TeV. The measured pseudorapidity density in p+Pb collisions is compared to model predictions and provides new constraints on the description of particle production in high-energy nuclear collisions.

Charge separation relative to the reaction plane in Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV

Measurements of charge-dependent azimuthal correlations with the ALICE detector at the LHC are reported for Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV. Two- and three-particle charge-dependent azimuthal correlations in the pseudorapidity range |η| < 0.8 are presented as a function of the collision centrality, particle separation in pseudorapidity, and transverse momentum. A clear signal compatible with a charge-dependent separation relative to the reaction plane is observed, which shows little or no collision energy dependence when compared to measurements at RHIC energies. This provides a new insight for understanding the nature of the charge-dependent azimuthal correlations observed at RHIC and LHC energies.

Pion, kaon, and proton production in central Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV

In this Letter we report the first results on π(±), K(±), p, and p production at midrapidity (|y|<0.5) in central Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV, measured by the ALICE experiment at the LHC. The p(T) distributions and yields are compared to previous results at sqrt[s(NN)] = 200 GeV and expectations from hydrodynamic and thermal models. The spectral shapes indicate a strong increase of the radial flow velocity with sqrt[s(NN)], which in hydrodynamic models is expected as a consequence of the increasing particle density. While the K/π ratio is in line with predictions from the thermal model, the p/π ratio is found to be lower by a factor of about 1.5. This deviation from thermal model expectations is still to be understood.

Measurement of the cross section for electromagnetic dissociation with neutron emission in Pb-Pb collisions at sqrt[s(NN)] = 2.76 TeV

The first measurement of neutron emission in electromagnetic dissociation of ^{208}Pb nuclei at the LHC is presented. The measurement is performed using the neutron zero degree calorimeters of the ALICE experiment, which detect neutral particles close to beam rapidity. The measured cross sections of single and mutual electromagnetic dissociation of Pb nuclei at sqrt[s(NN)]=2.76 TeV with neutron emission are σ(singleEMD)=187.4 ± 0.2(stat)(-11.2)(+13.2) (syst) b and σ(mutualEMD) = 5.7 ± 0.1(stat) ± 0.4(syst) b, respectively. The experimental results are compared to the predictions from a relativistic electromagnetic dissociation model.

Production of muons from heavy flavor decays at forward rapidity in pp and Pb-Pb collisions at sqrt[s(NN)]=2.76 TeV

The ALICE Collaboration has measured the inclusive production of muons from heavy-flavor decays at forward rapidity, 2.5<y<4, in pp and Pb-Pb collisions at sqrt[s(NN)]=2.76  TeV. The p(t)-differential inclusive cross section of muons from heavy-flavor decays in pp collisions is compared to perturbative QCD calculations. The nuclear modification factor is studied as a function of p(t) and collision centrality. A weak suppression is measured in peripheral collisions. In the most central collisions, a suppression of a factor of about 3-4 is observed in 6<p(t)<10  GeV/c. The suppression shows no significant p(t) dependence.

J/ψ suppression at forward rapidity in Pb-Pb collisions at √s(NN) = 2.76 TeV

The ALICE experiment has measured the inclusive J/ψ production in Pb-Pb collisions at √s(NN) = 2.76 TeV down to zero transverse momentum in the rapidity range 2.5 < y < 4. A suppression of the inclusive J/ψ yield in Pb-Pb is observed with respect to the one measured in pp collisions scaled by the number of binary nucleon-nucleon collisions. The nuclear modification factor, integrated over the 0%-80% most central collisions, is 0.545 ± 0.032(stat) ± 0.083(syst) and does not exhibit a significant dependence on the collision centrality. These features appear significantly different from measurements at lower collision energies. Models including J/ψ production from charm quarks in a deconfined partonic phase can describe our data.