Frederico Vasconcellos Prudente
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Research Subjects
Frederico Vasconcellos Prudente has a total of 109 co-authors. Here are the top co-authors by number of shared publications:
- Angelo Marconi Maniero
Centro das Ciências Exatas e das Tecnologias Universidade Federal do Oeste da Bahia 47808-021 Barreiras BA Brazil
16 shared publications - Jorge M. Campos Marques
CQC-IMS, Department of Chemistry, University of Coimbra, 3004-535 Coimbra, Portugal
14 shared publications - Carlos Renato De Carvalho
Instituto de Física Universidade Federal do Rio de Janeiro Rio de Janeiro 21941-972 RJ Brazil
10 shared publications - Ricardo R. T. Marinho
Department of Physics, University of Brasília, Brasília, Brazil
10 shared publications - Wallas Santos Nascimento
Instituto de Física Universidade Federal da Bahia 40170-115 Salvador BA Brasil
10 shared publications - Ginette Jalbert
Universidade Federal do Rio de Janeiro
8 shared publications
Latest Publications
- 12 November 2025
- Published by American Physical Society (APS) in Physical Review E
- Vol. 112 (5) , 054120
Entropy production and statistical relaxation of dipolar bosons and fermions in interaction quench dynamics
We study the out-of-equilibrium dynamics of dipolar bosons and fermions after a sudden change in the interaction strength from zero to a finite repulsive value. We simulate the interaction quench on the initial state which is the ground state of harmonic potential with noninteracting bosons and fermions. We solve the time-dependent many-boson Schrödinger equation exactly using numerical methods. To understand the many-body dynamics we analyze several measures of many-body information entropy, monitoring their time evolution and assessing their dependence on interaction strength. We establish that for weak interaction quench the dynamics is statistics independent, both dipolar bosons and fermions do not relax, whereas it is significantly different for dipolar bosons from that of dipolar fermions in the stronger interaction quench. While dipolar bosons exhibit concurrent signature of relaxation in all entropy measures, dipolar fermions fail to relax, exhibiting modulated oscillation in all entropy dynamics. For dipolar bosons and larger interaction quench, the many-body information entropy measures dynamically approach the value predicted for the Gaussian orthogonal ensemble of random matrices, implying statistical relaxation and ergodicity. The entire relaxation process and signature of ergodicity are established by three unique features: dynamical delocalization in Hilbert space, violent orbital fragmentation, and saturation of all entropy measures to the maximum entropy states in the long-time dynamics. It highlights the importance of many-body effects with a possible exploration in quantum simulation with ultracold atoms.
- 12 November 2025
- Published by American Physical Society (APS) in Physical Review E
- Vol. 112 (5) , 054120
Entropy production and statistical relaxation of dipolar bosons and fermions in interaction quench dynamics
We study the out-of-equilibrium dynamics of dipolar bosons and fermions after a sudden change in the interaction strength from zero to a finite repulsive value. We simulate the interaction quench on the initial state which is the ground state of harmonic potential with noninteracting bosons and fermions. We solve the time-dependent many-boson Schrödinger equation exactly using numerical methods. To understand the many-body dynamics we analyze several measures of many-body information entropy, monitoring their time evolution and assessing their dependence on interaction strength. We establish that for weak interaction quench the dynamics is statistics independent, both dipolar bosons and fermions do not relax, whereas it is significantly different for dipolar bosons from that of dipolar fermions in the stronger interaction quench. While dipolar bosons exhibit concurrent signature of relaxation in all entropy measures, dipolar fermions fail to relax, exhibiting modulated oscillation in all entropy dynamics. For dipolar bosons and larger interaction quench, the many-body information entropy measures dynamically approach the value predicted for the Gaussian orthogonal ensemble of random matrices, implying statistical relaxation and ergodicity. The entire relaxation process and signature of ergodicity are established by three unique features: dynamical delocalization in Hilbert space, violent orbital fragmentation, and saturation of all entropy measures to the maximum entropy states in the long-time dynamics. It highlights the importance of many-body effects with a possible exploration in quantum simulation with ultracold atoms.
- Open Access
- 12 November 2025
- Published by American Chemical Society (ACS) in ACS Omega
- Vol. 10 (46) , 56500-56510
Photoabsorption and Photoionization of Acetaldehyde in the 10.8–21.4 eV Range
An experimental and theoretical investigation of acetaldehyde’s photoabsorption and photoionization in the vacuum-ultraviolet energy range is presented. The absorption cross sections and the ionization efficiency were measured using a double-ion-chamber spectrometer in the 10.8–21.4 eV and 13.5–21.4 eV ranges, respectively. No previous reports of these quantities were found in the literature in this energy range. Photoionization and neutral-decay cross sections were derived from these results. Theoretical calculations were performed using the Padé approximant technique and the single-center partial-wave expansion method, which were applied to solve the Lippmann–Schwinger equation to obtain the asymmetry parameters and the photoionization cross sections for the seven outermost valence orbitals. The calculations were performed in the energy range from near-threshold to 35 eV at static-exchange and static-exchange-polarization levels of approximation. Our results are contextualized with recent studies on dissociative photoionization channels and high-resolution photoelectron spectra, enabling correlations with ionic fragmentation pathways. Our experimental and theoretical results were compared between each other and with previous results from the literature, exhibiting good agreement with the available data and providing a comprehensive data set essential for modeling photochemical processes in atmospheric and astrophysical environments.
- 12 November 2025
- Published by American Chemical Society (ACS) in ACS Omega
- Vol. 10 (46) , 56500-56510
Open AccessPhotoabsorption and Photoionization of Acetaldehyde in the 10.8–21.4 eV Range
An experimental and theoretical investigation of acetaldehyde’s photoabsorption and photoionization in the vacuum-ultraviolet energy range is presented. The absorption cross sections and the ionization efficiency were measured using a double-ion-chamber spectrometer in the 10.8–21.4 eV and 13.5–21.4 eV ranges, respectively. No previous reports of these quantities were found in the literature in this energy range. Photoionization and neutral-decay cross sections were derived from these results. Theoretical calculations were performed using the Padé approximant technique and the single-center partial-wave expansion method, which were applied to solve the Lippmann–Schwinger equation to obtain the asymmetry parameters and the photoionization cross sections for the seven outermost valence orbitals. The calculations were performed in the energy range from near-threshold to 35 eV at static-exchange and static-exchange-polarization levels of approximation. Our results are contextualized with recent studies on dissociative photoionization channels and high-resolution photoelectron spectra, enabling correlations with ionic fragmentation pathways. Our experimental and theoretical results were compared between each other and with previous results from the literature, exhibiting good agreement with the available data and providing a comprehensive data set essential for modeling photochemical processes in atmospheric and astrophysical environments.
- Open Access
Entropy production and statistical relaxation of dipolar bosons and fermions in interaction quench dynamics
We study the out-of-equilibrium dynamics of dipolar bosons and fermions after a sudden change in the interaction strength from zero to a finite repulsive value. We simulate the interaction quench on the initial state which is the ground state of harmonic potential with noninteracting bosons and fermions. We solve the time-dependent many-boson Schrödinger equation exactly using numerical methods. To understand the many-body dynamics we analyze several measures of many-body information entropy, monitoring their time evolution and assessing their dependence on interaction strength. We establish that for weak interaction quench the dynamics is statistics independent, both dipolar bosons and fermions do not relax. Whereas it is significantly different for dipolar bosons from that of dipolar fermions in the stronger interaction quench. When dipolar bosons exhibit concurrent signature of relaxation in all entropy measures, dipolar fermions fail to relax. For dipolar bosons and for larger interaction quench, the many-body information entropy measures dynamically approach the value predicted for the Gaussian orthogonal ensemble of random matrices, implying statistical relaxation. The relaxation time is uniquely determined when the orbital fragmentation exhibits a $1/M$ population in each orbital ($M$ is the number of orbitals) and all entropy measures saturate to the maximum entropy values. The relaxation time also becomes independent of the strength of dipolar interaction. Whereas, for the same quench protocol, dipolar fermions exhibit modulated oscillations in all entropy dynamics. Our study is also complemented by the measures of delocalization in Hilbert space, clearly establishing the onset of chaos for strongly interacting dipolar bosons. It highlights the importance of many-body effects with a possible exploration in quantum simulation with ultracold atoms.Open AccessEntropy production and statistical relaxation of dipolar bosons and fermions in interaction quench dynamics
We study the out-of-equilibrium dynamics of dipolar bosons and fermions after a sudden change in the interaction strength from zero to a finite repulsive value. We simulate the interaction quench on the initial state which is the ground state of harmonic potential with noninteracting bosons and fermions. We solve the time-dependent many-boson Schrödinger equation exactly using numerical methods. To understand the many-body dynamics we analyze several measures of many-body information entropy, monitoring their time evolution and assessing their dependence on interaction strength. We establish that for weak interaction quench the dynamics is statistics independent, both dipolar bosons and fermions do not relax. Whereas it is significantly different for dipolar bosons from that of dipolar fermions in the stronger interaction quench. When dipolar bosons exhibit concurrent signature of relaxation in all entropy measures, dipolar fermions fail to relax. For dipolar bosons and for larger interaction quench, the many-body information entropy measures dynamically approach the value predicted for the Gaussian orthogonal ensemble of random matrices, implying statistical relaxation. The relaxation time is uniquely determined when the orbital fragmentation exhibits a $1/M$ population in each orbital ($M$ is the number of orbitals) and all entropy measures saturate to the maximum entropy values. The relaxation time also becomes independent of the strength of dipolar interaction. Whereas, for the same quench protocol, dipolar fermions exhibit modulated oscillations in all entropy dynamics. Our study is also complemented by the measures of delocalization in Hilbert space, clearly establishing the onset of chaos for strongly interacting dipolar bosons. It highlights the importance of many-body effects with a possible exploration in quantum simulation with ultracold atoms. - Open Access
Informational Entropy Analysis of Artificial Helium Atoms
We use the Shannon informational entropies as a tool to study the artificial helium atom, namely, two electrons confined in a quantum dot. We adopt configurations with spherical and cylindrical symmetries for the physical system of interest. Using the informational quantities, we analyze the effects of electronic confinement, we validate the entropic uncertainty relation, we identify that the Coulomb interaction potential between the electrons is no longer important for strong confinements, and we indicate/predict the avoided crossing phenomena. Finally, we carried out a density function analysis. When available, the results are compared with those in the literature.
Open AccessInformational Entropy Analysis of Artificial Helium Atoms
We use the Shannon informational entropies as a tool to study the artificial helium atom, namely, two electrons confined in a quantum dot. We adopt configurations with spherical and cylindrical symmetries for the physical system of interest. Using the informational quantities, we analyze the effects of electronic confinement, we validate the entropic uncertainty relation, we identify that the Coulomb interaction potential between the electrons is no longer important for strong confinements, and we indicate/predict the avoided crossing phenomena. Finally, we carried out a density function analysis. When available, the results are compared with those in the literature.
- Open Access
- 24 February 2025
- Published by American Chemical Society (ACS) in ACS Physical Chemistry Au
- Vol. 5 (3) , 254-265
Photoabsorption and Photoionization Cross-Sections and Asymmetry Parameters of Pyrrole in the Vacuum-Ultraviolet Energy Range
We carried out a joint experimental and theoretical investigation of the interaction of vacuum-ultraviolet radiation with pyrrole molecules in the gas phase. A double-ion chamber spectrometer was used to measure the absolute photoabsorption cross-sections and the photoionization quantum yields from the ionization threshold to 21.5 eV using synchrotron radiation. Moreover, photoionization and neutral-decay cross-sections on an absolute scale were derived directly from the measured data. In addition, theoretical results of the photoionization cross-section (PICS) and asymmetric parameters were obtained from the ionization threshold to 50.0 eV considering all valence orbitals. These calculations were performed using the Padé approximant technique to solve the Lippmann–Schwinger equation at the static-exchange (SE) and static-exchange-polarization (SEP) levels of approximation. Comparisons are also made with the experimental and theoretical data available in the literature. We report, for the first time, experimental ionization efficiency, neutral decay cross-sections, theoretical photoionization cross-sections for each valence orbital, and several asymmetry parameters. In general, the results are consistent and in good agreement with the available data.
- 24 February 2025
- Published by American Chemical Society (ACS) in ACS Physical Chemistry Au
- Vol. 5 (3) , 254-265
Open AccessPhotoabsorption and Photoionization Cross-Sections and Asymmetry Parameters of Pyrrole in the Vacuum-Ultraviolet Energy Range
We carried out a joint experimental and theoretical investigation of the interaction of vacuum-ultraviolet radiation with pyrrole molecules in the gas phase. A double-ion chamber spectrometer was used to measure the absolute photoabsorption cross-sections and the photoionization quantum yields from the ionization threshold to 21.5 eV using synchrotron radiation. Moreover, photoionization and neutral-decay cross-sections on an absolute scale were derived directly from the measured data. In addition, theoretical results of the photoionization cross-section (PICS) and asymmetric parameters were obtained from the ionization threshold to 50.0 eV considering all valence orbitals. These calculations were performed using the Padé approximant technique to solve the Lippmann–Schwinger equation at the static-exchange (SE) and static-exchange-polarization (SEP) levels of approximation. Comparisons are also made with the experimental and theoretical data available in the literature. We report, for the first time, experimental ionization efficiency, neutral decay cross-sections, theoretical photoionization cross-sections for each valence orbital, and several asymmetry parameters. In general, the results are consistent and in good agreement with the available data.
- 30 November 2024
- Published by Elsevier in Physica B: Condensed Matter
- Vol. 699
Informational analysis of the confinement of an electron in an asymmetric double quantum dot
- 30 November 2024
- Published by Elsevier in Physica B: Condensed Matter
- Vol. 699
Informational analysis of the confinement of an electron in an asymmetric double quantum dot
- Open Access
Structure and Thermodynamics of Li+Arn Clusters beyond the Second Solvation Shell
Small Li+Arn clusters are employed in this work as model systems to study microsolvation. Although first and second solvation shells are expected to be the most relevant ones for this type of atomic solvents, it is also interesting to explore larger clusters in order to identify the influence of external atoms on structural and thermodynamic properties. In this work, we perform a global geometry optimization for clusters (with n = 41–100) and parallel tempering Monte Carlo (PTMC) simulations for some selected sizes. The results show that global minimum structures of large clusters always have 6 argon atoms in the first solvation shell while maintaining the number of 14 or 16 argon atoms in the second one. By contrast, third and fourth solvation shells vary significantly the number of argon atoms with the cluster size, and other shells can hardly be assigned due to the reduced influence of on the external argon atoms for large clusters. In turn, PTMC calculations show that the melting of the most external solvation shells of large microsolvation clusters occurs at , which is independent of cluster size. Structural transitions can be observed between quasi-degenerated structures at low temperatures. Moreover, the present results highlight the fluxional character of the external solvation shells of these large clusters, which may be seen as typical “snowball” structures.Open AccessStructure and Thermodynamics of Li+Arn Clusters beyond the Second Solvation Shell
Small Li+Arn clusters are employed in this work as model systems to study microsolvation. Although first and second solvation shells are expected to be the most relevant ones for this type of atomic solvents, it is also interesting to explore larger clusters in order to identify the influence of external atoms on structural and thermodynamic properties. In this work, we perform a global geometry optimization for clusters (with n = 41–100) and parallel tempering Monte Carlo (PTMC) simulations for some selected sizes. The results show that global minimum structures of large clusters always have 6 argon atoms in the first solvation shell while maintaining the number of 14 or 16 argon atoms in the second one. By contrast, third and fourth solvation shells vary significantly the number of argon atoms with the cluster size, and other shells can hardly be assigned due to the reduced influence of on the external argon atoms for large clusters. In turn, PTMC calculations show that the melting of the most external solvation shells of large microsolvation clusters occurs at , which is independent of cluster size. Structural transitions can be observed between quasi-degenerated structures at low temperatures. Moreover, the present results highlight the fluxional character of the external solvation shells of these large clusters, which may be seen as typical “snowball” structures. - Open Access
Electron Confinement study in a double quantum dot by means of Shannon Entropy Information
In this work, we use the Shannon informational entropies to study an electron confined in a double quantum dot; we mean the entropy in the space of positions, $S_r$, in the space of momentum, $S_p$, and the total entropy, $S_t = S_r+S_p$. We obtain $S_r$, $S_p$ and $S_t$ as a function of the parameters $A_2$ and $k$ which rules the height and the width, respectively, of the internal barrier of the confinement potential. We conjecture that the entropy $S_r$ maps the degeneracy of states when we vary $A_2$ and also is an indicator of the level of decoupling/coupling of the double quantum dot. We study the quantities $S_r$ and $S_p$ as measures of delocalization/localization of the probability distribution. Furthermore, we analyze the behaviors of the quantities $S_p$ and $S_t$ as a function of $A_2$ and $k$. Finally, we carried out an energy analysis and, when possible, compared our results with work published in the literature.Open AccessElectron Confinement study in a double quantum dot by means of Shannon Entropy Information
In this work, we use the Shannon informational entropies to study an electron confined in a double quantum dot; we mean the entropy in the space of positions, $S_r$, in the space of momentum, $S_p$, and the total entropy, $S_t = S_r+S_p$. We obtain $S_r$, $S_p$ and $S_t$ as a function of the parameters $A_2$ and $k$ which rules the height and the width, respectively, of the internal barrier of the confinement potential. We conjecture that the entropy $S_r$ maps the degeneracy of states when we vary $A_2$ and also is an indicator of the level of decoupling/coupling of the double quantum dot. We study the quantities $S_r$ and $S_p$ as measures of delocalization/localization of the probability distribution. Furthermore, we analyze the behaviors of the quantities $S_p$ and $S_t$ as a function of $A_2$ and $k$. Finally, we carried out an energy analysis and, when possible, compared our results with work published in the literature. - 21 January 2024
- Published by Elsevier in Physica B: Condensed Matter
- Vol. 677
Electron confinement study in a double quantum dot by means of Shannon entropy information
- 21 January 2024
- Published by Elsevier in Physica B: Condensed Matter
- Vol. 677
Electron confinement study in a double quantum dot by means of Shannon entropy information