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A fresh computational approach to atomic structures and. processes relevant for plasma material physics,Simple atomic processes. Quiz Atomic processes in a nutshell,for intermediates in atomic and plasma physics. Quiz Atomic processes in a nutshell,for intermediates in atomic and plasma physics. Indeed these and many similar processes occur in atomic plasma and astro. physics as well as at many places elsewhere, How much help can atomic theory provide Which tools are available. Quiz Atomic processes in a nutshell,for intermediates in atomic and plasma physics.

Demandsfrom,fromexperiment,experiment theory,theory Two. quickexamples,Established,Establishedstructure,structurecodes. codes Strength,Strengthand,andweaknesses,weaknesses. JAC AAfresh,freshapproach,approachtotoatomic,atomiccomputations. computations,Amplitudes,Amplitudes properties,properties processes.

Indeed these and similar,Atomic processes occur in atomic plasma and astro. physics as well as at many,Summary places elsewhere. conclusions,Summary conclusions, How much help can atomic theory provide Which tools are available. Demands for atomic theory, to accurately describe the dynamics of many electron systems. XUV XFEL s,magnetic bottles,Atomic QED techniques,Dirac s equation.

merge beam,experiments,space missions synchrotrons. reaction microscopes,Dirac Fock,Demands for atomic theory. to accurately describe the dynamics of many electron systems. XUV XFEL s,magnetic bottles,Atomic QED techniques,Dirac s equation. merge beam,experiments,space missions synchrotrons. reaction microscopes,Dirac Fock,Demands for atomic theory.

to accurately describe the dynamics of many electron systems. XUV XFEL s,magnetic bottles,Atomic QED techniques,Dirac s equation. merge beam,experiments,space missions,V synchrotrons. reaction microscopes,Dirac Fock,1 Level identification of atoms and ions. Grotrian diagram as a unique finger print,Rubidium I Term diagrams gross fine structure. Allowed transitions and selection rules, 4s2 4p6 5s 5p 4d 6s Useful for one multi electron atoms.

1 Level identification of atoms and ions,unique but often very complex. Rubidium I Iron V,4s2 4p6 5s 5p 4d 6s 3s2 3p6 3d4,1 Level identification of atoms and ions. unique but often very complex,Theoretical,Theoreticalchallenges. challengesfor,heavyelements,strongrelativistic,relativisticand. QEDeffects,oftensystems,systemswith,andf shells,Rubidium I overlapping.

many overlappingand andnearly,nearlydegenerate Iron. degenerateconfigurations,configurations V,largenumber. ofelectrons,identification,4s2 4p6 5s 5p 4d 6s identificationdifficult or. difficult3s,3dfeasible, 2 Ion electron spectra after inner shell excitations. 1s 2p excitation of O recorded at PIPE, O 1s2 2s2 2p5 O 1s 2s2 2p6 2S1 2 O m 1 1s2 2l7 m m e.

merge beam,experiments,Double triple detachments by Auger electron. emission are energetically forbidden,possible only due to shake up. 2s 3s 2p 3p,PIPE Photon Ion spectrometer at PETRA III. S Schippers et al PRA 94 2016 052412, S Schippers and coworkers Gie en Frankfurt Hamburg collaboration 2015. Established tools for atomic structure calculations. including great experience, Clementi Roetti Roothan Hartree Fock wave functions with optimized exponents.

Cowan s HFX support semi empirical adjustment of level structures. transition probabilities cross sections, ATSP Breit Pauli approximation level energies properties. Grasp Ratip Large scale computations of individual energies rates. FAC Modelling and diagnostics of astro plasma processes. Flexible Atomic Code, CI MBPT Combines CI and MBPT methods for bound state properties. Home made Large No of tools for particular purposes. Established tools for atomic structure calculations. including great experience, Clementi Roetti Roothan Hartree Fock wave functions with optimized exponents. Cowan s HFS support semi empirical adjustment of level structures. transition probabilities cross sections,ATSP onnss. Breit Pauli approximation level energies iproperties. a tti o s ic,ppplliicca d pphhyys,o f aap energies.

findividual l a tte,Grasp Ratip Large scale computationsrrof. e o r re e l a rates,Modellingg,diagnostics,A Mastro plasma processes. Flexible Atomic Code itth h a,aan s ffrro omm, CI MBPT attiioonns Combines CI and MBPT methods for bound state properties. Home made Large No of tools for particular purposes. S Fritzsche JESRP 114 116 2001 1155 Comput Phys Commun 183 2012 1525. Many electron,Many electronbasis,basis wave,wavefunction. functionexpansions,expansions,Construction,Constructionand.

andclassification,classificationofofN particle,N particleHilbert. Shellmodel,model Systematically,Systematicallyenlarged. enlargedCSF,Interactions,Interactions,Dirac Coulomb. Dirac CoulombHamiltonian,Hamiltonian,Breitinteractions. interactions QED,Electroncontinuum,continuum scattering.

scatteringphases,Coherencetransfer,transferand,andRydberg. A fresh computational approach to atomic structures and processes relevant for plasma amp material physics A fresh computational approach to atomic structures and processes relevant for plasma amp material physics Simple atomic processes Quiz Atomic processes in a nutshell for intermediates in atomic and plasma physics Quiz Atomic processes in a nutshell for

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