activity
19972008
most citedNondispersive and dispersive collective electronic modes in carbon nanotubes

7 citations · 17 across the 6 of their papers we have counts for

collaborators

6 papers

cond-mat.mes-hall2008★ 5 cited

Exact-Diagonalization Studies of Inelastic Light Scattering in Self-Assembled Quantum Dots

Alain Delgado, Adriel Dominguez, Ricardo Perez +2

We report exact diagonalization studies of inelastic light scattering in few-electron quantum dots under the strong confinement regime characteristic of self-assembled dots. We app…

cond-mat.other2004★ 7 cited

Nondispersive and dispersive collective electronic modes in carbon nanotubes

Ricardo Perez, William Que

We propose a new theoretical interpretation of the electron energy-loss spectroscopy results of Pichler {\it et al.} on bulk carbon nanotube samples. The experimentally found nondi…

cond-mat.mes-hall2003★ 1 cited

Internal transitions of negatively charged magnetoexcitons in quantum dots

Ricardo Perez, Augusto Gonzalez, Jorge Mahecha

We report calculations of oscillator strengths for the far infrared absorption of light by the excitonic complexes Xn- (the excess charge, n, ranging from one to four) confined in…

cond-mat.mes-hall2001

Internal transitions in the confined biexciton

Ricardo Perez, Augusto Gonzalez

Optical internal transitions relevant to ODR experiments are computed for the biexciton in a quantum dot in the strong confinement regime. Valence sub-band mixing effects are taken…

cond-mat.mes-hall1997★ 3 cited

Few-anyon systems in a parabolic dot

Ricardo Perez, Augusto Gonzalez

The energy levels of two and three anyons in a two-dimensional parabolic quantum dot and a perpendicular magnetic field are computed as power series in 1/|J|, where J is the angula…

cond-mat.mes-hall1997★ 1 cited

Two and three electrons in a quantum dot: 1/|J| - expansion

Augusto Gonzalez, Ricardo Perez, Pavel Fileviez

We consider systems of two and three electrons in a two-dimensional parabolic quantum dot. A magnetic field is applied perpendicularly to the electron plane of motion. We show that…