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Coupled basis set

The benchmark indicates that the PA of ammonia is very well reproduced employing the 6-311-m-G or the TZVP basis sets coupled with B3LYP, PWP and BP exchange-correlation potentials. For this reason, the PA and GPB of other further compounds reported in Tables 3-5 are calculated at these levels of theory. [Pg.106]

Fig. 1 An example of the time savings achieved when using additive corrections such as those employed in the ccCA methodology. When approximating a large basis set coupled cluster computation on the benzene molecule, a relative savings of almost two orders of magnitude in CPU time is achieved... Fig. 1 An example of the time savings achieved when using additive corrections such as those employed in the ccCA methodology. When approximating a large basis set coupled cluster computation on the benzene molecule, a relative savings of almost two orders of magnitude in CPU time is achieved...
Evaluated with the aug-cc-pVTZ basis set. Coupled-cluster methods estimated via an addition of the difference between MP2 and coupled-cluster correlation energies with the aug-cc-pVDZ basis set to the MP2/aug-cc-pVTZ energies. [Pg.21]

This equation may be solved by the same methods as used with the nonreactive coupled-channel equations (discussed later in section A3.11.4.2). Flowever, because F(p, p) changes rapidly with p, it is desirable to periodically change the expansion basis set ip. To do this we divide the range of p to be integrated into sectors and within each sector choose a (usually the midpoint) to define local eigenfimctions. The coiipled-chaimel equations just given then apply withm each sector, but at sector boundaries we change basis sets. Let y and 2 be the associated with adjacent sectors. Then, at the sector boundary p we require... [Pg.976]

For a coupled spin system, the matrix of the Liouvillian must be calculated in the basis set for the spin system. Usually this is a simple product basis, often called product operators, since the vectors in Liouville space are spm operators. The matrix elements can be calculated in various ways. The Liouvillian is the conmuitator with the Hamiltonian, so matrix elements can be calculated from the commutation rules of spin operators. Alternatively, the angular momentum properties of Liouville space can be used. In either case, the chemical shift temis are easily calculated, but the coupling temis (since they are products of operators) are more complex. In section B2.4.2.7. the Liouville matrix for the single-quantum transitions for an AB spin system is presented. [Pg.2099]

W (Rj.) is an n X n diabatic first-derivative coupling matrix with elements defined using the diabatic electronic basis set as... [Pg.190]

The picture here is of uncoupled Gaussian functions roaming over the PES, driven by classical mechanics. The coefficients then add the quantum mechanics, building up the nuclear wavepacket from the Gaussian basis set. This makes the treatment of non-adiabatic effects simple, as the coefficients are driven by the Hamiltonian matrices, and these elements couple basis functions on different surfaces, allowing hansfer of population between the states. As a variational principle was used to derive these equations, the coefficients describe the time dependence of the wavepacket as accurately as possible using the given... [Pg.295]

Unlike semiempirical methods that are formulated to completely neglect the core electrons, ah initio methods must represent all the electrons in some manner. However, for heavy atoms it is desirable to reduce the amount of computation necessary. This is done by replacing the core electrons and their basis functions in the wave function by a potential term in the Hamiltonian. These are called core potentials, elfective core potentials (ECP), or relativistic effective core potentials (RECP). Core potentials must be used along with a valence basis set that was created to accompany them. As well as reducing the computation time, core potentials can include the effects of the relativistic mass defect and spin coupling terms that are significant near the nuclei of heavy atoms. This is often the method of choice for heavy atoms, Rb and up. [Pg.84]

Cartesian coordinates system for locating points in space based on three coordinates, which are usually given the symbols x, y, z or i, j, k CBS (complete basis set) an ah initio method CC (coupled cluster) a correlated ah initio method CFF (consistent force field) a class of molecular mechanics force fields CFMM (continuous fast multipole method) a method for fast DFT calculations on large molecules... [Pg.361]

The structure of ozone is a well-known pathological case for electronic structure theory. Prior to the QCI and coupled cluster methods, it proved very difficult to model accurately. The following table summarized the results of geometry optimizations of ozone, performed at the MP2, QCISD and QCISD(T) levels using the 6-31G(d) basis set ... [Pg.118]

Compute the isotropic hyperfine coupling constant for each of the atoms in HNCN with the HF, MP2, MP4(SDQ) and QCISD methods, using the D95(d,p) basis set Make sure that the population analysis for each job uses the proper electron density by including the Density=Current keyword in the route section. Also, include the 5D keyword in each job s route sectionfas was done in the original study). [Pg.136]

Barone also introduces two new basis sets, EPR-Il and EPR-llI. These are optimized for the calculation of hyperfine coupling constants by density functional methods. EPR-Il is a double zeta basis set with a single set of polarization functions and an enhanced s part. EPR-III is a triple zeta set including diffuse functions, double d polarization functions and a single set off functions. [Pg.314]

In the following, all isotropic hyperfine coupling constants were calculated using the BLYP functional and the EPR-II basis set. A full geometry optimization was done in all cases. [Pg.314]

Specifically, if T] < 0.02, the CCSD(T) metliod is expected to give results close the full Cl limit for the given basis set. If is larger than 0.02, it indicates that the reference wave function has significant multi-determinant character, and multi-reference coupled cluster should preferentially be employed. Such methods are being developedbut have not yet seen any extensive use. [Pg.140]

The generalization of a Coulson-Fischer type wave function to the molecular case with an arbitrary size basis set is known as Spin Coupled Valence Bond (SCVB) theory. ... [Pg.197]

It should also be noted that the effect of electron correlation at the MP2 level (relative to HF) is largely independent of the basis set, but there is a significant coupling between... [Pg.266]


See other pages where Coupled basis set is mentioned: [Pg.112]    [Pg.70]    [Pg.51]    [Pg.9]    [Pg.2370]    [Pg.112]    [Pg.70]    [Pg.51]    [Pg.9]    [Pg.2370]    [Pg.1031]    [Pg.1502]    [Pg.2050]    [Pg.2212]    [Pg.2225]    [Pg.74]    [Pg.194]    [Pg.260]    [Pg.294]    [Pg.296]    [Pg.296]    [Pg.307]    [Pg.288]    [Pg.112]    [Pg.339]    [Pg.301]    [Pg.313]    [Pg.134]    [Pg.156]    [Pg.162]    [Pg.165]    [Pg.215]    [Pg.288]    [Pg.2]    [Pg.154]    [Pg.69]   
See also in sourсe #XX -- [ Pg.105 , Pg.106 ]




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Basis sets coupled-clusters

Correlation consistent basis sets CCSD (coupled cluster singles

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