Search results for "Derivative"

showing 10 items of 1074 documents

Photochemical intermediates of trans-Rh(CO)L2Cl where L=PMe3, PBu3, and i-Pr2HN and cis-Rh(CO)2(i-Pr2HN)Cl in frozen organic glasses

2002

International audience; The Nujol glass matrix photolyses of Rh(CO)(PMe3)2Cl (1), Rh(CO)(PBu3)2Cl (2), Rh(CO)2(i-Pr2HN)Cl (3), and Rh(CO)(i-Pr2HN)2Cl (4), have been examined. Phototolysis of 1 (λirr>400 nm) and 2 (350<λirr<400 nm) give new species, A, with carbonyl stretching bands slightly below the parent bands. In the case of 1 this species appears to give rise to a second product, C, upon either extended photolysis or annealing. High-energy photolysis of 1, 2, and 4, result in loss of CO and formation of an IR silent species, RhL2Cl. In the case of 1 a new carbonyl species, B, is observed upon high-energy photolysis or annealing of a matrix containing CO and Rh(PMe3)2Cl. B may be conver…

Photolysis010405 organic chemistryChemistryAnnealing (metallurgy)Organic ChemistryPhotodissociationAmine derivatives010402 general chemistryPhotochemistryGlass matrix01 natural sciencesBiochemistry0104 chemical sciencesInorganic ChemistryDFT analysischemistry.chemical_compoundNujolExcited stateMaterials Chemistry[CHIM.COOR]Chemical Sciences/Coordination chemistryPhysical and Theoretical ChemistryPhosphineAmine derivativesJournal of Organometallic Chemistry
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Concentration depending fluorescence of 8-(di-(2-picolyl)) aminoBODIPY in solution

2014

[EN] An 8-dipicolylBODIPY derivative has been prepared and its photophysical properties evaluated under different conditions. Two different structures, hemicyanine and cyanine, are observed (depending on the solvent or the solution concentration). The hemicyanine form is not emissive whereas the cyanine form is fluorescent. This behavior is related with the planarity degree of the BODIPY core. The X-ray structure of the compound is reported and it shows that in solid state the hemicyanine form is present. The hemicyanine form seems to be stabilized by aggregation and is the main compound in concentrated solutions whereas the cyanine form is present in diluted solutions that are photochemica…

Photophysical stabilityOrganic ChemistrySolid-state8-DipicolylBODIPYCyanine formPhotochemistryBiochemistryFluorescencePlanarity testingSolventchemistry.chemical_compoundCocentration influencechemistryDrug DiscoveryBODIPYCyanineDerivative (chemistry)Hemicyanine form
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2-(2-Iodoethyl)isoindole-1,3-dione

2007

The title compound, C10H8INO2, is an N-substituted phthalimide derivative in which the crystallographic inter­molecular contact pattern consists of I⋯I, C—H⋯I, C—H⋯O and aromatic π–π inter­actions.

Phthalimidechemistry.chemical_compoundchemistryGeneral Materials ScienceGeneral ChemistryCondensed Matter PhysicsIsoindoleMedicinal chemistryDerivative (chemistry)Acta Crystallographica Section E Structure Reports Online
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DLPNO-MP2 second derivatives for the computation of polarizabilities and NMR shieldings

2021

We present a derivation and efficient implementation of the formally complete analytic second derivatives for the domain-based local pair natural orbital second order Møller–Plesset perturbation theory (MP2) method, applicable to electric or magnetic field-response properties but not yet to harmonic frequencies. We also discuss the occurrence and avoidance of numerical instability issues related to singular linear equation systems and near linear dependences in the projected atomic orbital domains. A series of benchmark calculations on medium-sized systems is performed to assess the effect of the local approximation on calculated nuclear magnetic resonance shieldings and the static dipole …

Physics010304 chemical physicsGeneral Physics and AstronomyBasis function010402 general chemistry01 natural sciences0104 chemical sciencesComputational physicsDipoleAtomic orbital0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysical and Theoretical ChemistryPerturbation theoryScalingLinear equationNumerical stabilitySecond derivativeThe Journal of Chemical Physics
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Extension of the Launay Quantum Reactive Scattering Code and Direct Computation of Time Delays.

2019

Scattering computations, particularly within the realm of molecular physics, have seen an increase in study since the development of powerful quantum methods. These dynamical processes can be analyzed via (among other quantities) the duration of the collision process and the lifetime of the intermediate complex. We use the Smith matrix Q = -iℏS†dS/dE calculated from the scattering matrix S and its derivative with respect to the total energy. Its real part contains the state-to-state time delays, and its eigenvalues give the lifetimes of the metastable states [ Smith Phys. Rev. 1960 , 118 , 349 - 356 ]. We propose an extension of the Launay HYP3D code [ Launay and Le Dourneuf Chem. Phys. Let…

Physics010304 chemical physicsScattering01 natural sciencesComputer Science ApplicationsEnergy derivativeMatrix (mathematics)Total angular momentum quantum numberQuantum mechanicsMetastability0103 physical sciencesNumerical differentiationPhysical and Theoretical ChemistryQuantumEigenvalues and eigenvectorsJournal of chemical theory and computation
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Benchmark coupled-cluster g-tensor calculations with full inclusion of the two-particle spin-orbit contributions.

2017

We present a parallel implementation to compute electron spin resonance g-tensors at the coupled-cluster singles and doubles (CCSD) level which employs the ACES III domain-specific software tools for scalable parallel programming, i.e., the super instruction architecture language and processor (SIAL and SIP), respectively. A unique feature of the present implementation is the exact (not approximated) inclusion of the five one- and two-particle contributions to the g-tensor [i.e., the mass correction, one- and two-particle paramagnetic spin-orbit, and one- and two-particle diamagnetic spin-orbit terms]. Like in a previous implementation with effective one-electron operators [J. Gauss et al.,…

Physics010304 chemical physicsbusiness.industryGaussGeneral Physics and Astronomy010402 general chemistry01 natural sciences0104 chemical sciencesTheoretical physicsSoftwareCoupled clusterClassical mechanics0103 physical sciencesScalabilityBenchmark (computing)TensorPhysical and Theoretical ChemistryOrbit (control theory)businessSecond derivativeThe Journal of chemical physics
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An exact thermodynamical model of power-law temperature time scaling

2016

In this paper a physical model for the anomalous temperature time evolution (decay) observed in complex thermodynamical system in presence of uniform heat source is provided. Measures involving temperatures T with power-law variation in time as T(t)∝tβ with β∈R shows a different evolution of the temperature time rate T(t) with respect to the temperature time-dependence T(t). Indeed the temperature evolution is a power-law increasing function whereas the temperature time rate is a power-law decreasing function of time. Such a behavior may be captured by a physical model that allows for a fast thermal energy diffusion close to the insulated location but must offer more resistance to the therm…

PhysicsAnomalous conductionDiffusion equationField (physics)business.industryPower-lawTime evolutionTemperature evolutionGeneral Physics and AstronomyAnomalous conduction; Fractional derivative; Fractional Transport; Power-law; Temperature evolution;Function (mathematics)Fractional derivative01 natural sciencesPower law010305 fluids & plasmasFractional Transport010101 applied mathematics0103 physical sciencesStatistical physics0101 mathematicsDiffusion (business)businessSettore ICAR/08 - Scienza Delle CostruzioniScalingThermal energy
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Parallel Calculation of CCSD and CCSD(T) Analytic First and Second Derivatives.

2007

In this paper we present a parallel adaptation of a highly efficient coupled-cluster algorithm for calculating coupled-cluster singles and doubles (CCSD) and coupled-cluster singles and doubles augmented by a perturbative treatment of triple excitations (CCSD(T)) energies, gradients, and, for the first time, analytic second derivatives. A minimal-effort strategy is outlined that leads to an amplitude-replicated, communication-minimized implementation by parallelizing the time-determining steps for CCSD and CCSD(T). The resulting algorithm is aimed at affordable cluster architectures consisting of compute nodes with sufficient memory and local disk space and that are connected by standard co…

PhysicsBasis (linear algebra)Chemical shiftGigabit EthernetBasis functionParallel computingComputer Science ApplicationsComputational physicsPhysics::Atomic and Molecular ClustersCluster (physics)Benchmark (computing)Limit (mathematics)Physics::Chemical PhysicsPhysical and Theoretical ChemistrySecond derivativeJournal of chemical theory and computation
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Frequency-modulated atomic force microscopy operation by imaging at the frequency shift minimum: the dip-df mode.

2014

In frequency modulated non-contact atomic force microscopy, the change of the cantilever frequency (Delta f) is used as the input signal for the topography feedback loop. Around the Delta f(z) minimum, however, stable feedback operation is challenging using a standard proportional-integral-derivative (PID) feedback design due to the change of sign in the slope. When operated under liquid conditions, it is furthermore difficult to address the attractive interaction regime due to its often moderate peakedness. Additionally, the Delta f signal level changes severely with time in this environment due to drift of the cantilever frequency f(0) and, thus, requires constant adjustment. Here, we pre…

PhysicsCantileverbusiness.industrySurface PropertiesPID controllerAbsolute valueDerivativeFeedback loopModels TheoreticalMicroscopy Atomic Force530SignalCalcium CarbonateSetpointOpticsbusinessConstant (mathematics)InstrumentationThe Review of scientific instruments
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Systematic study of octet-baryon electromagnetic form factors in covariant chiral perturbation theory

2017

We perform a complete and systematic calculation of the octet-baryon form factors within the fully covariant approach of SU(3) chiral perturbation theory at O(p^3). We use the extended on-mass shell renormalization scheme, and include explicitly the vector mesons and the spin-3/2 decuplet intermediate states. Comparing these predictions with data including magnetic moments, charges, and magnetic radii, we determine the unknown low-energy constants, and give predictions for yet unmeasured observables, such as the magnetic moment of the Sigma^0, and the charge and magnetic radii of the hyperons.

PhysicsChiral perturbation theoryMeson010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesCharge (physics)01 natural sciencesBaryonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Charge radius0103 physical sciencesCovariant transformationGauge covariant derivative010306 general physicsMathematical physics
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