Marco Campetella
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Marco Campetella has a total of 85 co-authors. Here are the top co-authors by number of shared publications:
- Lorenzo Gontrani
Department of Chemical Science and Technologies, University of Rome Tor Vergata, Via Della Ricerca Scientifica 1, 00133 Rome, Italy
23 shared publications - Ruggero Caminiti
Dipartimento di Chimica, Università di Roma “La Sapienza”, Piazzale Aldo Moro 5, 00185 Roma, Italy
7 shared publications - Ilaria Ciofini
Institute of Chemistry for Life and Health Sciences (iCLeHS UMR 8060), ChimieParisTech ‐PSL CNRS PSL University Paris France
6 shared publications - Enrico Bodo
Department of Chemistry, Sapienza University of Rome, P. le Aldo Moro 5, 00185 Rome, Italy
5 shared publications - Juan Sanz García
MSME, Université Gustave Eiffel, CNRS, 5 Boulevard Descartes, 77454 Marne-la-Vallée, France
5 shared publications - Alessandro Mariani
Department of Chemistry, Materials and Chemical Engineering “G. Natta” Politecnico di Milano Milano Italy
4 shared publications
Latest Publications
- 18 July 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (2) , 024304
Electron-phonon driven charge density wave in CuTe
The compound CuTe (vulcanite) undergoes a quasi-one-dimensional charge density wave (CDW) at K with a periodicity. The mechanism at its origin is debated. Several theoretical works claimed that semilocal functionals are unable to describe its occurrence and ascribed its formation only to strong electron-electron interaction. Moreover, the possible role of quantum anharmonicity has not been addressed. Here, by performing quantum-anharmonic calculations, we show that semilocal functionals correctly describe the occurrence of a CDW in CuTe if ultradense electron-momentum grids allowing for small electronic temperatures are used. The distortion is driven by the perfect nesting among one-dimensional Fermi surface sheets extending in the direction. Quantum anharmonic effects are important and tend to suppress both the distortion and . The quantum anharmonic structural minimization of the CDW phase in the generalized gradient approximation leads, however, to distorted Te-Te bond lengths in the low temperature phase that are of the experimental ones at K. This suggests that, even if the electron-electron interaction is not crucial for the mechanism of CDW formation, it is relevant to accurately describe the structural data for the low- phase. We assess the effect of electron-electron interaction on the CDW by using the approximation with parameters calculated from first principles. We find that electron-electron interaction enhances the Te-Te distortion, , and the total energy gain by the distortion.- 18 July 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (2) , 024304
Electron-phonon driven charge density wave in CuTe
The compound CuTe (vulcanite) undergoes a quasi-one-dimensional charge density wave (CDW) at K with a periodicity. The mechanism at its origin is debated. Several theoretical works claimed that semilocal functionals are unable to describe its occurrence and ascribed its formation only to strong electron-electron interaction. Moreover, the possible role of quantum anharmonicity has not been addressed. Here, by performing quantum-anharmonic calculations, we show that semilocal functionals correctly describe the occurrence of a CDW in CuTe if ultradense electron-momentum grids allowing for small electronic temperatures are used. The distortion is driven by the perfect nesting among one-dimensional Fermi surface sheets extending in the direction. Quantum anharmonic effects are important and tend to suppress both the distortion and . The quantum anharmonic structural minimization of the CDW phase in the generalized gradient approximation leads, however, to distorted Te-Te bond lengths in the low temperature phase that are of the experimental ones at K. This suggests that, even if the electron-electron interaction is not crucial for the mechanism of CDW formation, it is relevant to accurately describe the structural data for the low- phase. We assess the effect of electron-electron interaction on the CDW by using the approximation with parameters calculated from first principles. We find that electron-electron interaction enhances the Te-Te distortion, , and the total energy gain by the distortion.- Open Access
Electron-phonon driven charge density wave in CuTe
The compound CuTe (vulcanite) undergoes a quasi one dimensional charge density wave (CDW) at $T< T_{\mathrm{CDW}}=335$ K with a $5\times1\times2$ periodicity. The mechanism at its origin is debated. Several theoretical works claimed that semilocal functionals are unable to describe its occurrence and ascribed its formation only to strong electron-electron interaction. Moreover, the possible role of quantum anharmonicity has not been addressed. Here, by performing quantum anharmonic calculations, we show that semilocal functionals correctly describe the occurrence of a CDW in CuTe if ultradense electron momentum grids allowing for small electronic temperatures are used. The distortion is driven by the perfect nesting among 1D Fermi surface sheets extending in the $k_y$ direction. Quantum anharmonic effects are important and tend to suppress both the distortion and $T_{\mathrm{CDW}}$. The quantum anharmonic structural minimization of the CDW phase in the generalized gradient approximation leads, however, to distorted Te-Te bond lengths in the low temperature phase that are $21\%$ of the experimental ones at $T=20$ K. This suggests that, even if the electron-electron interaction is not crucial for the mechanism of CDW formation, it is relevant to accurately describe the structural data for the low-T phase. We assess the effect of correlation on the CDW by using the DFT+U+V approximation with parameters calculated from first principles. We find that correlation enhances the Te-Te distortion, T$_{CDW}$ and the total energy gain by the distortion.Open AccessElectron-phonon driven charge density wave in CuTe
The compound CuTe (vulcanite) undergoes a quasi one dimensional charge density wave (CDW) at $T< T_{\mathrm{CDW}}=335$ K with a $5\times1\times2$ periodicity. The mechanism at its origin is debated. Several theoretical works claimed that semilocal functionals are unable to describe its occurrence and ascribed its formation only to strong electron-electron interaction. Moreover, the possible role of quantum anharmonicity has not been addressed. Here, by performing quantum anharmonic calculations, we show that semilocal functionals correctly describe the occurrence of a CDW in CuTe if ultradense electron momentum grids allowing for small electronic temperatures are used. The distortion is driven by the perfect nesting among 1D Fermi surface sheets extending in the $k_y$ direction. Quantum anharmonic effects are important and tend to suppress both the distortion and $T_{\mathrm{CDW}}$. The quantum anharmonic structural minimization of the CDW phase in the generalized gradient approximation leads, however, to distorted Te-Te bond lengths in the low temperature phase that are $21\%$ of the experimental ones at $T=20$ K. This suggests that, even if the electron-electron interaction is not crucial for the mechanism of CDW formation, it is relevant to accurately describe the structural data for the low-T phase. We assess the effect of correlation on the CDW by using the DFT+U+V approximation with parameters calculated from first principles. We find that correlation enhances the Te-Te distortion, T$_{CDW}$ and the total energy gain by the distortion. - Open Access
- 9 December 2022
- Published by Royal Society of Chemistry (RSC) in Physical Chemistry Chemical Physics
- Vol. 25 (3) , 2523-2536
Solvent effects on catechol's binding affinity: investigating the role of the intra-molecular hydrogen bond through a multi-level computational approach
A multi-level computational approach is employed to investigate catechol's conformational dynamics in different solvents, unraveling the interplay between the intramolecular hydrogen bond and the interactions with the surrounding molecules.
- 9 December 2022
- Published by Royal Society of Chemistry (RSC) in Physical Chemistry Chemical Physics
- Vol. 25 (3) , 2523-2536
Open AccessSolvent effects on catechol's binding affinity: investigating the role of the intra-molecular hydrogen bond through a multi-level computational approach
A multi-level computational approach is employed to investigate catechol's conformational dynamics in different solvents, unraveling the interplay between the intramolecular hydrogen bond and the interactions with the surrounding molecules.
- 23 November 2021
- Published by American Physical Society (APS) in Physical Review B
- Vol. 104 (17) , 174111
Polar magnetic metallic state in few-layerRecently, few-layer suspended stoichiometric flakes were synthesized and found to display large tetragonality and giant dipole moments per unit surface. Little is known, however, about the ground state properties of this compound in the two-dimensional (2D) limit. By performing first-principles electronic structure calculations, we determine the ground state structural, magnetic, and electronic properties of suspended stoichiometric flakes with number of layers () ranging from 1 to 4. We show that, even if the orthorhombic flakes with G-type antiferromagnetic order are the most stable ones for , the metastable cubic multilayers have physical properties in excellent agreement with experimental data, including enhanced tetragonality and large dipole moments per unit surface in the 2D limit. In these cubic multilayers, the broken inversion symmetry, determined by the different top and bottom terminations, results in a strong Fe offset along the direction coexisting with metallicity. Our work shows that the cubic phase, nonmagnetic and stable only above in bulk and in thin films, is a “polar” magnetic metal and a type I “multiferroic” in the 2D limit at room temperature.- 23 November 2021
- Published by American Physical Society (APS) in Physical Review B
- Vol. 104 (17) , 174111
Polar magnetic metallic state in few-layerRecently, few-layer suspended stoichiometric flakes were synthesized and found to display large tetragonality and giant dipole moments per unit surface. Little is known, however, about the ground state properties of this compound in the two-dimensional (2D) limit. By performing first-principles electronic structure calculations, we determine the ground state structural, magnetic, and electronic properties of suspended stoichiometric flakes with number of layers () ranging from 1 to 4. We show that, even if the orthorhombic flakes with G-type antiferromagnetic order are the most stable ones for , the metastable cubic multilayers have physical properties in excellent agreement with experimental data, including enhanced tetragonality and large dipole moments per unit surface in the 2D limit. In these cubic multilayers, the broken inversion symmetry, determined by the different top and bottom terminations, results in a strong Fe offset along the direction coexisting with metallicity. Our work shows that the cubic phase, nonmagnetic and stable only above in bulk and in thin films, is a “polar” magnetic metal and a type I “multiferroic” in the 2D limit at room temperature.- 25 May 2021
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 154 (20) , 204102
Chasing unphysical TD-DFT excited states in transition metal complexes with a simple diagnostic tool
Transition Metal Complexes (TMCs) are known for the rich variety of their excited states showing different nature and degrees of locality. Describing the energies of these excited states with the same degree of accuracy is still problematic when using time-dependent density functional theory in conjunction with the most current density functional approximations. In particular, the presence of unphysically low lying excited states possessing a relevant Charge Transfer (CT) character may significantly affect the spectra computed at such a level of theory and, more relevantly, the interpretation of their photophysical behavior. In this work, we propose an improved version of the MAC index, recently proposed by the authors and collaborators, as a simple and computationally inexpensive diagnostic tool that can be used for the detection and correction of the unphysically predicted low lying excited states. The analysis, performed on five prototype TMCs, shows that spurious and ghost states can appear in a wide spectral range and that it is difficult to detect them only on the basis of their CT extent. Indeed, both delocalization of the excited state and CT extent are criteria that must be combined, as in the MAC index, to detect unphysical states.
- 25 May 2021
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 154 (20) , 204102
Chasing unphysical TD-DFT excited states in transition metal complexes with a simple diagnostic tool
Transition Metal Complexes (TMCs) are known for the rich variety of their excited states showing different nature and degrees of locality. Describing the energies of these excited states with the same degree of accuracy is still problematic when using time-dependent density functional theory in conjunction with the most current density functional approximations. In particular, the presence of unphysically low lying excited states possessing a relevant Charge Transfer (CT) character may significantly affect the spectra computed at such a level of theory and, more relevantly, the interpretation of their photophysical behavior. In this work, we propose an improved version of the MAC index, recently proposed by the authors and collaborators, as a simple and computationally inexpensive diagnostic tool that can be used for the detection and correction of the unphysically predicted low lying excited states. The analysis, performed on five prototype TMCs, shows that spurious and ghost states can appear in a wide spectral range and that it is difficult to detect them only on the basis of their CT extent. Indeed, both delocalization of the excited state and CT extent are criteria that must be combined, as in the MAC index, to detect unphysical states.
- Open Access
- 1 February 2021
- Published by Elsevier in Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy
- Vol. 247, 119061
New insights into chloromethyl-oxirane and chloromethyl-thiirane in liquid and solid phase from low-temperature infrared spectroscopy and ab initio modeling
- 1 February 2021
- Published by Elsevier in Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy
- Vol. 247, 119061
Open AccessNew insights into chloromethyl-oxirane and chloromethyl-thiirane in liquid and solid phase from low-temperature infrared spectroscopy and ab initio modeling
- Open Access
- 25 September 2020
- Published by Ant Publishing in Clinical surgery research communications
- Vol. 4 (3) , 17-18
Double J stent migration in the contralateral ureter during robotassisted pyeloplasty: an unique complication
The placement of double-J (DJ) stent in the urinary tract is a part of urologic practice for many indications. However, this may cause many complications ranging from stent-related irritative lower urinary tract symptoms (LUTS) to advanced renal failure. Although complications such as encrustations, proximal, and distal migrations within the pelvicaliceal system (PCS) are reported frequently in the literature, stent displacement into the contralateral ureter is rare and not previously described at our knowledge. Keywords: Double J stent dislocation; robotic pyeloplasty; hydronephrosis
- 25 September 2020
- Published by Ant Publishing in Clinical surgery research communications
- Vol. 4 (3) , 17-18
Open AccessDouble J stent migration in the contralateral ureter during robotassisted pyeloplasty: an unique complication
The placement of double-J (DJ) stent in the urinary tract is a part of urologic practice for many indications. However, this may cause many complications ranging from stent-related irritative lower urinary tract symptoms (LUTS) to advanced renal failure. Although complications such as encrustations, proximal, and distal migrations within the pelvicaliceal system (PCS) are reported frequently in the literature, stent displacement into the contralateral ureter is rare and not previously described at our knowledge. Keywords: Double J stent dislocation; robotic pyeloplasty; hydronephrosis
- Open Access
- 24 July 2020
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 153 (4) , 044106
Automated parameterization of quantum-mechanically derived force-fields including explicit sigma holes: A pathway to energetic and structural features of halogen bonds in gas and condensed phase
In classical molecular dynamics, general purpose atomistic force-fields (FFs) often deliver inaccurate results when dealing with halogen bonds (XBs), notwithstanding their crucial role in many fields of science, ranging from material design to drug development. Given the large dimensions of the systems of interest, it would be therefore desirable to increase the FF accuracy maintaining the simplicity of the standard Lennard-Jones (LJ) plus point charge description to avoid an excessive computational cost. A simple yet effective strategy consists in introducing a number of virtual sites able to mimic the so-called “explicit σ-hole.” In this work, we present an automated FF parameterization strategy based on a global optimization of both LJ and charge parameters with respect to accurate quantum mechanical data, purposely computed for the system under investigation. As a test case, we report on two homologue series, characterized either by weak or strong XBs, namely, the di-halogenated methanes and the mono-, di-, and tri-substituted acetonitriles, taking into consideration Cl, Br, and I substituents. The resulting quantum mechanically derived FFs are validated for each compound in the gas and in the condensed phase by comparing them to general purpose and specific FFs without virtual sites and to highly accurate reference quantum mechanical data. The results strongly support the adoption of the specific FFs with virtual sites, which overcome the other investigated models in representing both gas phase energetics and the structural patterns of the liquid phase structure related to the presence of XBs.
- 24 July 2020
- Published by AIP Publishing in The Journal of Chemical Physics
- Vol. 153 (4) , 044106
Open AccessAutomated parameterization of quantum-mechanically derived force-fields including explicit sigma holes: A pathway to energetic and structural features of halogen bonds in gas and condensed phase
In classical molecular dynamics, general purpose atomistic force-fields (FFs) often deliver inaccurate results when dealing with halogen bonds (XBs), notwithstanding their crucial role in many fields of science, ranging from material design to drug development. Given the large dimensions of the systems of interest, it would be therefore desirable to increase the FF accuracy maintaining the simplicity of the standard Lennard-Jones (LJ) plus point charge description to avoid an excessive computational cost. A simple yet effective strategy consists in introducing a number of virtual sites able to mimic the so-called “explicit σ-hole.” In this work, we present an automated FF parameterization strategy based on a global optimization of both LJ and charge parameters with respect to accurate quantum mechanical data, purposely computed for the system under investigation. As a test case, we report on two homologue series, characterized either by weak or strong XBs, namely, the di-halogenated methanes and the mono-, di-, and tri-substituted acetonitriles, taking into consideration Cl, Br, and I substituents. The resulting quantum mechanically derived FFs are validated for each compound in the gas and in the condensed phase by comparing them to general purpose and specific FFs without virtual sites and to highly accurate reference quantum mechanical data. The results strongly support the adoption of the specific FFs with virtual sites, which overcome the other investigated models in representing both gas phase energetics and the structural patterns of the liquid phase structure related to the presence of XBs.
- 31 January 2020
- Published by Wiley in Journal of Computational Chemistry
- Vol. 41 (12) , 1156-1164
Following the evolution of excited states along photochemical reaction pathways
Analyzing the behavior of potential energy surfaces (PESs) of diabatic excited states (ESs) becomes of crucial importance for a complete understanding of complex photochemical reactions. Since the definition of a compact representation for the transition density matrix, the use of the natural transition orbitals (NTOs) has become a routine practice in time‐dependent density functional theory calculations. Their popularity has remarkably grown due to its simple orbital description of electronic excitations. Indeed, very recently, we have presented a new formalism used for the optimization of ESs by tracking the state of interest computing the NTO's overlap between consecutive steps of the procedure. In this new contribution, we generalize the use of this NTO's overlap‐based state‐tracking formalism for the analysis of all the desired diabatic states along any chemical reaction pathway. Determining the PES of the different diabatic states has been automatized by developing an extension of our recently presented algorithm, the so‐called SDNTO: “Steepest Descent minimization using NTOs.” This automatized overlap‐based procedure allows an agile and convenient analysis of the evolution of the ESs avoiding the intrinsic ambiguity of visualizing orbitals or comparing physical observables. The analysis of two photochemical reactions of the same nature with different PES landscapes perfectly illustrates the utility of this new tool.
- 31 January 2020
- Published by Wiley in Journal of Computational Chemistry
- Vol. 41 (12) , 1156-1164
Following the evolution of excited states along photochemical reaction pathways
Analyzing the behavior of potential energy surfaces (PESs) of diabatic excited states (ESs) becomes of crucial importance for a complete understanding of complex photochemical reactions. Since the definition of a compact representation for the transition density matrix, the use of the natural transition orbitals (NTOs) has become a routine practice in time‐dependent density functional theory calculations. Their popularity has remarkably grown due to its simple orbital description of electronic excitations. Indeed, very recently, we have presented a new formalism used for the optimization of ESs by tracking the state of interest computing the NTO's overlap between consecutive steps of the procedure. In this new contribution, we generalize the use of this NTO's overlap‐based state‐tracking formalism for the analysis of all the desired diabatic states along any chemical reaction pathway. Determining the PES of the different diabatic states has been automatized by developing an extension of our recently presented algorithm, the so‐called SDNTO: “Steepest Descent minimization using NTOs.” This automatized overlap‐based procedure allows an agile and convenient analysis of the evolution of the ESs avoiding the intrinsic ambiguity of visualizing orbitals or comparing physical observables. The analysis of two photochemical reactions of the same nature with different PES landscapes perfectly illustrates the utility of this new tool.