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Orbitals, Is and

However, there exist cases where it is advantageous to be able to use a larger set of active orbitals. The dimension of the CAS wave function can then become prohibitively large, and it may be of interest to look for other means of restricting the expansion length. This can be done in many ways, and results in a number of different types of MCSCF expansions. Assume that the number of inactive orbitals is and the number of active orbitals t, the number of active electrons being Na. We can then formally write the corresponding CAS wave function as ... [Pg.234]

These numbers explain the shape of the periodic table. Each element has one more electron (and one more proton and perhaps more neutrons) than the one before. At first the lowest energy shell (n = 1) is filled. There is only one orbital, Is, and we can put one or two electrons in it. There are therefore two elements in this block, H and He. Next we must move to the second shell ( = 2), filling 2s first so we start the top of groups 1 and 2 with Li and Be. These occupy the top of the red stack marked s block because all the elements in this block have one or two electrons in their outermost s orbital and no electrons in the outermost p orbital. Then we can start on the 2p orbitals. There are three of these so we can put in six electrons and get six elements B, C, N, O, F, and Ne. They occupy the top row of the black p block. Most of the elements we need in this book are in those blocks. Some, Na, K, and Mg for example, are in the s block and others, Si, P, and S for example, are in the second row of the p block. [Pg.89]

This has a structure in which the two borons each form two boron-hydrogen single bonds and are linked by two hydrogen bridges. The bridging hydrogens have only one valence electron and one valence orbital, Is, and yet they are bonded to two borons. How ... [Pg.72]

Beryllium has two filled orbitals (Is- and the 2s-orbital) but this is not the end of the 2 period since there are three 2p-orbitals to be filled before the period is ended. The filling of electrons in the three 2p-orbitals is to be started ... [Pg.31]

Fluorescence overcomes other processes the better, the smaller the excitation energy is in comparison to the energy of bonding, the more delocalised the JT-orbital is, and if n —> jt transitions are at shorter wavelength than JT —> JT transitions. [Pg.275]

How are the many-electron states obtained from the orbitals If we have two orbitals. Is and 2s, we may create Slater determinants with different spin functions ... [Pg.65]

If we instead use the orbitals Is and 2p, there are more Slater determinants. Every orbital has either a or p spin function. The orbital 2p may have different quantum niunbers m. Altogether there are 12 different functions ... [Pg.65]

The orbitals Is and Isg are not orthogonal to each other at finite R (otherwise the overlap integral S R) would always be zero). State whether or not the following pairs of orbitals are orthogonal and whether or not your answer depends on R ... [Pg.255]

An s orbital is spherically symmetrical and can contain a maximum of two electrons with opposed spins. A p orbital has a solid figure-of-eight shape there are three equivalent p orbitals for each principal quantum number they correspond to the three axes of rectangular coordinates. [Pg.152]

For a free electron gas, it is possible to evaluate the Flartree-Fock exchange energy directly [3, 16]. The Slater detemiinant is constructed using ftee electron orbitals. Each orbital is labelled by a k and a spin index. The Coulomb... [Pg.94]

There are complicating issues in defmmg pseudopotentials, e.g. the pseudopotential in equation Al.3.78 is state dependent, orbitally dependent and the energy and spatial separations between valence and core electrons are sometimes not transparent. These are not insunnoimtable issues. The state dependence is usually weak and can be ignored. The orbital dependence requires different potentials for different angular momentum components. This can be incorporated via non-local operators. The distinction between valence and core states can be addressed by incorporating the core level in question as part of the valence shell. For... [Pg.112]

For both types of orbitals, the coordinates r, 0 and cji refer to the position of the electron relative to a set of axes attached to the centre on which the basis orbital is located. Although STOs have the proper cusp behaviour near the nuclei, they are used primarily for atomic- and linear-molecule calculations because the multi-centre integrals which arise in polyatomic-molecule calculations caimot efficiently be perfonned when STOs are employed. In contrast, such integrals can routinely be done when GTOs are used. This fiindamental advantage of GTOs has led to the dominance of these fimetions in molecular quantum chemistry. [Pg.2170]

A minimal basis in which the number of STO or GOTO orbitals is equal to the number of core and valence AOs in tlie atom. [Pg.2171]

The electronic energy W in the Bom-Oppenlieimer approxunation can be written as W= fV(q, p), where q is the vector of nuclear coordinates and the vector p contains the parameters of the electronic wavefimction. The latter are usually orbital coefficients, configuration amplitudes and occasionally nonlinear basis fiinction parameters, e.g., atomic orbital positions and exponents. The electronic coordinates have been integrated out and do not appear in W. Optimizing the electronic parameters leaves a function depending on the nuclear coordinates only, E = (q). We will assume that both W q, p) and (q) and their first derivatives are continuous fimctions of the variables q- and py... [Pg.2332]

H at m energy of 1.2 eV in the center-of-mass frame. By using an atomic orbital basis and a representation of the electronic state of the system in terms of a Thouless determinant and the protons as classical particles, the leading term of the electronic state of the reactants is... [Pg.231]

Hiickel-type systems (such as Hilcfcel pericyclic reactions and suprafacial sigmatropic shifts) obey the same rules as for sigma electron. The rationale for this observation is clear If the overlap between adjacent p-electron orbitals is positive along the reaction coordinate, only the peraiutational mechanism can... [Pg.346]


See other pages where Orbitals, Is and is mentioned: [Pg.262]    [Pg.389]    [Pg.110]    [Pg.345]    [Pg.110]    [Pg.37]    [Pg.12]    [Pg.745]    [Pg.188]    [Pg.637]    [Pg.269]    [Pg.523]    [Pg.31]    [Pg.262]    [Pg.389]    [Pg.110]    [Pg.345]    [Pg.110]    [Pg.37]    [Pg.12]    [Pg.745]    [Pg.188]    [Pg.637]    [Pg.269]    [Pg.523]    [Pg.31]    [Pg.158]    [Pg.27]    [Pg.30]    [Pg.37]    [Pg.434]    [Pg.1135]    [Pg.1143]    [Pg.2171]    [Pg.2174]    [Pg.2341]    [Pg.3057]    [Pg.3062]    [Pg.143]    [Pg.300]    [Pg.342]    [Pg.389]    [Pg.389]    [Pg.484]   
See also in sourсe #XX -- [ Pg.2 , Pg.4 ]




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Is orbital

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