0000000001251731

AUTHOR

Sam Azadi

showing 4 related works from this author

Quantum Monte Carlo study of high pressure solid molecular hydrogen

2013

We use the diffusion quantum Monte Carlo (DMC) method to calculate the ground state phase diagram of solid molecular hydrogen and examine the stability of the most important insulating phases relative to metallic crystalline molecular hydrogen. We develop a new method to account for finite-size errors by combining the use of twist-averaged boundary conditions with corrections obtained using the Kwee-Zhang-Krakauer (KZK) functional in density functional theory. To study band-gap closure and find the metallization pressure, we perform accurate quasi-particle many-body calculations using the $GW$ method. In the static approximation, our DMC simulations indicate a transition from the insulating…

Condensed Matter - Materials Science540 Chemistry and allied sciencesMaterials scienceCondensed matter physicsBand gapQuantum Monte CarloClose-packing of equal spheresMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesGeneral Physics and Astronomy540 ChemieDensity functional theoryBoundary value problemDiffusion (business)Ground statePhase diagram
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Resonating valence bond quantum Monte Carlo: Application to the ozone molecule

2015

We study the potential energy surface of the ozone molecule by means of Quantum Monte Carlo simulations based on the resonating valence bond concept. The trial wave function consists of an antisymmetrized geminal power arranged in a single-determinant that is multiplied by a Jastrow correlation factor. Whereas the determinantal part incorporates static correlation effects, the augmented real-space correlation factor accounts for the dynamics electron correlation. The accuracy of this approach is demonstrated by computing the potential energy surface for the ozone molecule in three vibrational states: symmetric, asymmetric and scissoring. We find that the employed wave function provides a de…

Chemical Physics (physics.chem-ph)PhysicsQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)Electronic correlationGeminalQuantum Monte CarloFOS: Physical sciencesComputational Physics (physics.comp-ph)Condensed Matter PhysicsBond-dissociation energyMolecular physicsAtomic and Molecular Physics and OpticsCondensed Matter - Strongly Correlated ElectronsPhysics - Chemical PhysicsScissoringPotential energy surfaceValence bond theoryPhysics::Chemical PhysicsPhysical and Theoretical ChemistryQuantum Physics (quant-ph)Wave functionPhysics - Computational PhysicsInternational Journal of Quantum Chemistry
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The fate of the resonating valence bond in graphene

2011

We apply a variational wave function capable of describing qualitatively and quantitatively the so called "resonating valence bond" in realistic materials, by improving standard ab initio calculations by means of quantum Monte Carlo methods. In this framework we clearly identify the Kekul\'e and Dewar contributions to the chemical bond of the benzene molecule, and we establish the corresponding resonating valence bond energy of these well known structures ($\simeq 0.01$eV/atom). We apply this method to unveil the nature of the chemical bond in undoped graphene and show that this picture remains only within a small "resonance length" of few atomic units.

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Quantum Monte CarloCondensed Matter - SuperconductivityQuantum monte carloGeneral Physics and AstronomyFOS: Physical sciencesResonance (chemistry)Atomic unitsMolecular physicsSettore FIS/03 - Fisica della MateriaSuperconductivity (cond-mat.supr-con)Condensed Matter - Strongly Correlated ElectronsChemical bondAb initio quantum chemistry methodsResonance valence bondAtomPhysics::Atomic and Molecular ClustersCondensed Matter::Strongly Correlated ElectronsValence bond theoryGrapheneAtomic physicsGeneralized valence bond
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Anhamonic finite temperature effects on the Raman and Infrared spectra to determine the crystal structure phase III of solid molecular hydrogen

2013

We present theoretical calculations of the Raman and IR spectra, as well as electronic properties at zero and finite temperature to elucidate the crystal structure of phase III of solid molecular hydrogen. We find that anharmonic finite temperature are particularly important and qualitatively influences the main conclusions. While P6$_3$/m is the most likely candidate for phase III at the nuclear ground state, at finite temperature the C2/c structure appears to be more suitable.

Superconductivity (cond-mat.supr-con)Chemical Physics (physics.chem-ph)Condensed Matter - Other Condensed MatterCondensed Matter - Materials ScienceCondensed Matter - SuperconductivityPhysics - Chemical PhysicsMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciencesComputational Physics (physics.comp-ph)Physics - Computational PhysicsOther Condensed Matter (cond-mat.other)
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