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Dirac integral notation

The notation < i j k 1> introduced above gives the two-electron integrals for the g(r,r ) operator in the so-called Dirac notation, in which the i and k indices label the spin-orbitals that refer to the coordinates r and the j and 1 indices label the spin-orbitals referring to coordinates r. The r and r denote r,0,( ),a and r, 0, ( ), a (with a and a being the a or P spin functions). The fact that r and r are integrated and hence represent dummy variables introduces index permutational symmetry into this list of integrals. For example,... [Pg.280]

Since the Dirac notation suppresses the variables involved in the integration, we re-express the orthogonality relation in integral notation... [Pg.71]

The bracket (bra-c-ket) in

) provides the names for the component vectors. This notation was introduced in Section 3.2 as a shorthand for the scalar product integral. The scalar product of a ket tp) with its corresponding bra (-01 gives a real, positive number and is the analog of multiplying a complex number by its complex conjugate. The scalar product of a bra tpj and the ket Aj>i) is expressed in Dirac notation as (0yjA 0,) or as J A i). These scalar products are also known as the matrix elements of A and are sometimes denoted by Ay. [Pg.81]

Yes, I know. Very confusing. But it s all just notation, and can be understood. In physicist s notation (equivalent to Dirac notation), tpitpjitpk tpi) refers to the two electron integral where and are functions of electron 1, while -j and ipi are functions of electron 2. Chemist s notation (with the square brackets []) places the functions of electron 1 on the left and the functions of... [Pg.9]

Within the old adiabatic approximation, Eq. (39) is the basic starting point. However, from here on, the various approximations diverge. For ease of discussion, we shall first still make the Condon approximation, and then give the further approximations. However, it must be kept in mind that many similar approximations are also made in papers that use a non-Condon approach. The basic premise of the Condon approximation is that the electronic part of the matrix element varies sufficiently slowly with Q so that it can be taken out of the integration over dQ. The matrix element then reduces to products of electronic and vibrational integrals. In Dirac notation... [Pg.42]

In the Dirac notation, quantum mechanical integrals are represented by a shorthand notation using brackets, for instance ... [Pg.123]

Introduction of Dirac notation [66,71] at this point helps us transform the trace of the density operator into an integral over configuration space, which ultimately gives rise to the path-integral representation. We let n> represent a state such that the system is found to have a particular set of quantum numbers n (it is an eigenstate of the measurement of n) similarly, we let x> represent a state in which the system is surely found at a particular position x. According to this picture, the wavefunction n(x) is a projection of the quantum number amplitude upon the position amplitude, specifically, i/rn(x) = and %( ) = partition function becomes... [Pg.128]

Dirac Notation for Integrals Energy Functional to Be Minimized Energy Minimization with Constraints Slater Determinant Subject to a Unitary Transformation The J and K Operators Are Invariant Diagonalization of the Lagrange Multipliers... [Pg.389]

The integrals over the spatial and spin coordinates (0 are the spinorbitals, tp - the orbitals) in the Dirac notation wUl be denoted with angle brackets () h denotes a one-electron operator and r 2 - the distance between electrons 1 and 2), as follows for the one-electron integrals. [Pg.399]

Dirac notation (p. 399) effectiveness of AOs mixing (p. 429) electron affinity (p. 466) electronic configuration (p. 451) electronic pair dimension (p. 475) electronic shells (p. 448) energy functional (p. 400) exchange integral (p. 419) exchange operator (p. 403) excitation energy (p. 458) external localization (p. 469)... [Pg.500]

Here, we have also switched to the bra and ket notation that was introduced by Dirac to deal with wavefunctions in an elegantly compact manner. In Dirac notation, a wavefiinction is denoted by a ket i.e. the Is orbital has been written 1 ) and the corresponding complex conjugate would be shown as (. If a bra and ket appear in the right order to complete a bracket , then integration is implied for example ... [Pg.377]


See other pages where Dirac integral notation is mentioned: [Pg.27]    [Pg.582]    [Pg.147]    [Pg.102]    [Pg.185]    [Pg.207]    [Pg.454]    [Pg.5]    [Pg.35]    [Pg.122]    [Pg.4]    [Pg.86]    [Pg.12]    [Pg.206]    [Pg.168]    [Pg.392]    [Pg.14]    [Pg.399]    [Pg.400]    [Pg.400]    [Pg.1067]    [Pg.334]    [Pg.334]    [Pg.898]    [Pg.399]    [Pg.400]    [Pg.400]    [Pg.1067]    [Pg.280]    [Pg.12]   
See also in sourсe #XX -- [ Pg.185 , Pg.207 ]




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Dirac notation for integrals

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