activity
20062016
most citedPlasmon modes of graphene nanoribbons with periodic planar arrangements

62 citations · 424 across the 31 of their papers we have counts for

collaborators

33 papers

hep-lat2016★ 1 cited

Importance of closed quark loops for lattice QCD studies of tetraquarks

Joshua Berlin, Abdou Abdel-Rehim, Constantia Alexandrou +5

To investigate the light scalar tetraquark candidate (quantum numbers ), a correlation matrix including a variety of two- and four-quark interpolating operator…

cond-mat.str-el2016★ 41 cited

Plasmon properties and hybridization effects in Silicene

C. Vacacela Gomez, M. Pisarra, M. Gravina +2

The plasmonic character of monolayer silicene is investigated by time-dependent density functional theory in the random phase approximation. The energy-loss function of the system…

cond-mat.str-el2016★ 62 cited

Plasmon modes of graphene nanoribbons with periodic planar arrangements

Cristian Vacacela Gomes, Michele Pisarra, Mario Gravina +2

Among their amazing properties, graphene and related low-dimensional materials show quantized charge-density fluctuations--known as plasmons--when exposed to photons or electrons o…

hep-lat2015

Computation of correlation matrices for tetraquark candidates with and flavor structure

Joshua Berlin, Abdou Abdel-Rehim, Constantia Alexandrou +3

The conjecture that several recently observed mesons have a structure, which is not dominated by an ordinary quark-antiquark pair, but by a four-quark structure, is being actively…

hep-lat2014★ 10 cited

Investigation of the tetraquark candidate : technical aspects and preliminary results

Abdou Abdel-Rehim, Constantia Alexandrou, Joshua Berlin +3

We discuss technical aspects and first results of a lattice QCD study of the state. We employ various interpolating operators of quark-antiquark, mesonic molecule, diqua…

hep-lat2014

Critical behavior and continuum scaling of lattice gauge theories

Oleg Borisenko, Volodymyr Chelnokov, Mario Gravina +1

Three-dimensional lattice gauge theories are studied numerically at finite temperature for = 5, 6, 8, 12, 13, 20 and for =2,4,8. For each model the location of phas…