Svjetlana Fajfer
(University of Ljubljana and J. Stefan Institute)
16/06/2014, 10:00
Valentina Santoro
(INFN Ferrara)
16/06/2014, 12:00
Altug Ozpineci
(METU - Ankara)
16/06/2014, 12:20
Alexis Pompili
(B)
16/06/2014, 12:40
Karl Landsteiner
(Instituto de Fisica Teorica CSIC/UAM)
16/06/2014, 15:00
Marco Bochicchio
(ROMA1)
16/06/2014, 15:30
Mei Huang
(IHEP - CAS)
16/06/2014, 15:50
Eugenio Megias
(Universitat Autonoma de Barcelona)
16/06/2014, 16:20
Floriana Giannuzzi
(BA)
16/06/2014, 17:30
Bora Isildak
(Ozyegin University)
17/06/2014, 09:00
Gennaro Corcella
(LNF)
17/06/2014, 09:30
Manuel Proissl
(Univ. Edinburgh)
17/06/2014, 10:00
Marco Guzzi
(INFN)
17/06/2014, 11:30
Vincent ANDRIEUX
(CEA Saclay)
17/06/2014, 12:20
67.
Rapidity evolution of Wilson lines at the next-to-leading order: Balitsky-JIMWLK equation at NLO
Giovanni Antonio Chirilli
(The Ohio State University)
17/06/2014, 12:40
Spyridon Margetis
(Kent State University)
17/06/2014, 15:00
Enrico Tassi
(Universita della Calabria and INFN Cosenza)
17/06/2014, 15:20
Yoshio Kitadono
(Academia Sinica)
17/06/2014, 15:40
Maria Paola Lombardo
(LNF)
18/06/2014, 09:30
Indranil Das
(Institut de Physique Nucleaire d'Orsay)
18/06/2014, 10:30
Mark Alford
(Washington University in St. Louis)
18/06/2014, 11:40
Marco Ruggieri
(Yukawa Institute for Theoretical Physics, Kyoto University)
18/06/2014, 12:50
Dmitri Melikhov
(Moscow State University)
18/06/2014, 15:00
Yasemin Sarac Oymak
(Atilim University)
18/06/2014, 15:20
Yu-Ming Wang
(TU Munich)
18/06/2014, 15:40
Sevda Esen
(Heidelberg University)
18/06/2014, 16:00
Jan Eeg
(Dep. Phys. Oslo Univ.)
18/06/2014, 16:50
Axel Weber
(Univ. Mihocana - Morelia)
18/06/2014, 17:10
Luigi Delle Rose
(INFN Lecce)
18/06/2014, 17:30
Damir Becirevic
(CNRS and Universite' Paris Sud XI)
19/06/2014, 09:00
Sebastian Uhl
(Technische Universität München)
19/06/2014, 09:50
Juan Jose Sanz-Cillero
(Universidad Autónoma de Madrid)
19/06/2014, 10:20
Olga Shekhovtsova
(IFJ PAN)
19/06/2014, 11:10
Gilberto Colangelo
(Berna University)
19/06/2014, 11:50
Dr
Juan Jose Sanz-Cillero
(Universidad Autónoma de Madrid)
Poster
Based on the mathematically well defined Pade Theory, a theoretically safe new procedure for the extraction of the pole mass and width of a resonance is proposed. In particular, thanks to the Montessus de Ballore theorem we are able to unfold the Second Riemann Sheet of an amplitude to search for the position of the resonant pole in the complex plane (arXiv:1306.6308 [hep-ph]). The method is...
Dr
Hayriye Sundu Pamuk
(Kocaeli University)
Poster
We calculate the shifts in the masses and decay constants of B and D mesons in nuclear medium in the frame work of QCD sum rules. We write the shifts in the masses and decay constants in terms of B-N and D-N scattering lengths and an extra phenomenological parameter entered to calculations. Computing an approciate forward scattering correlation function, we derive the QCD sum rules for the B-N...
Wolfgang LUCHA
(Austrian Academy of Sciences)
Poster
In spite of undeniable similarities of the applied techniques, rather different challenges are encountered when extracting, from QCD sum rules for two-point correlators of appropriate heavy-light interpolating currents, the decay constants of charmed mesons of, on the one hand, pseudoscalar nature and, on the other hand, vector nature. This observation justifies a careful reassessment of the...
Mr
Naser Ahmadiniaz
(Instituto de Física y Matemáticas (IFM) Universidad Michoacana de San Nicolás de Hidalgo (UMSNH) (Un)
Poster
The string-derived Bern-Kosower formalism was originally developed for the computation of on-shell gluon amplitudes. In previous work we have, using worldline methods, shown how to extend and optimize this formalism as a tool for obtaining form-factor decompositions of the off-shell 1PI gluon amplitudes. Following an earlier rederivation of the three-gluon (Ball-Chiu) form factor...
Dr
Eugenio Megias
(Universitat Autonoma de Barcelona)
Poster
QCD at finite temperature has been usually studied within the standard Boltzmann-Gibbs statistics. One of the standard properties of this is that entropy is extensive, which means that for two systems A and B which are independent (in the sense that the probabilities of the states of A+B factorize into those of A and B), the entropy of the joint system S(A+B) is equal to the sum of the...
Pietro Biancofiore
(University of Bari and INFN)
Poster
In the LHC era, the discovery of New Physics signals is the major ambition of the high energy physics community and flavor physics can provide access to new heavy particles (Kaluza—Klein modes, supersymmetric particles …) in complementary way with respect to direct searches. Signals of possible deviations with respect to the Standard Model (SM) have been recently claimed both by BaBar and...
Rafel Escribano
(Universitat Autònoma de Barcelona)
Poster
The η transition form factor is analyzed for the first time in both space-like and time-like regions at low and intermediate energies in a model-independent approach through the use of rational approximants. With the release of the η → e+e−γ data on the very low energy region by the A2 Collaboration we extract the most precise slope and curvature parameters of the form factors as well as their...
Dr
Valeriy Zamiralov
(skobeltsyn institute of nuclear physics of the lomonosov moscow state university)
Poster
Recently we have proposed unitary symmetry relations between the Light-Cone QCD sum rules with meson and photon distribution amplitudes (DA's). But they are not suitable if one deals with the baryon DA's because in this case interpolating currents have different nature: one of them is baryon current while the other one is either a meson or a photon current. As the resulting formules with...
Wolfgang LUCHA
(Austrian Academy of Sciences)
Poster
Observing renewed interest in (semi-) relativistic descriptions of bound states, we would like to make a few comments on the eigenvalue problem posed by the spinless Salpeter equation and, illustrated by the example of the Woods-Saxon potential, recall various elementary tools that practitioners looking for analytic albeit approximate solutions might find useful in their quest.