2007
DOI: 10.1016/s1049-250x(06)54005-4
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R-Matrix Theory of Atomic, Molecular and Optical Processes

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Cited by 111 publications
(154 citation statements)
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“…The General Relativistic Atomic Structure Package (grasp) (Dyall et al 1989;Grant 2007) formulates and diagonalises a Dirac-Coulomb Hamiltonian (Grant 2007) to produce the relativistic orbitals for input to the Dirac Atomic R-matrix Code (darc) (Chang 1975;Norrington & Grant 1981;Grant 2007;Burke 2011) to obtain the photoionization (PI) cross sections. These darc codes are currently running efficiently on a variety of world-wide parallel High Performance Computer (hpc) architectures (Ballance 2016;McLaughlin et al , 2016McLaughlin et al , 2017.…”
Section: Photoionization Calculationsmentioning
confidence: 99%
“…The General Relativistic Atomic Structure Package (grasp) (Dyall et al 1989;Grant 2007) formulates and diagonalises a Dirac-Coulomb Hamiltonian (Grant 2007) to produce the relativistic orbitals for input to the Dirac Atomic R-matrix Code (darc) (Chang 1975;Norrington & Grant 1981;Grant 2007;Burke 2011) to obtain the photoionization (PI) cross sections. These darc codes are currently running efficiently on a variety of world-wide parallel High Performance Computer (hpc) architectures (Ballance 2016;McLaughlin et al , 2016McLaughlin et al , 2017.…”
Section: Photoionization Calculationsmentioning
confidence: 99%
“…(8), α n 1 l 1 n 2 l 2 ,k , are the normalised 5 eigenvectors obtained when the real symmetric matrix,…”
Section: Hamiltonian Matrix Elements Within a Subregionmentioning
confidence: 99%
“…Notice that, in order to perform the integral over R in equation (1), this wave function must be obtained at different values of R. Several accurate methods have been successfully developed to evaluate ψ 0+ αlαǫα (r, R). Among them, it is worth mentioning (i) the discretized close-coupling (DCC) method [12,[17][18][19] and the convergent close-coupling (CCC) method [20][21][22], in which the electronic wave function is written as a combination of products of target and scattering electronic wave functions with the appropriate boundary conditions, (ii) the exterior complex scaling (ECS) method [23][24][25], in which the electronic coordinates are scaled in the complex plane beyond a certain (usually large) distance r 0 thus ensuring the correct asymptotic behavior for r i < r 0 , and (iii) the Rmatrix method (and its many extensions, see, e.g., [26][27][28] and references therein), in which the problem is first solved within a sphere of finite size and then the asymptotic behavior is switched on later from outside the sphere. In principle, all these methods can be implemented by using different basis sets and/or grid methods.…”
Section: Summary Of Existing Theoriesmentioning
confidence: 99%