VAMDC Regional workshop, Belgrade, 14-16 June 2012 S. Sahal-Bréchot Observatoire de Paris, LERMA CNRS UMR 8112, France The STARK-B database for spectral.

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Presentation transcript:

VAMDC Regional workshop, Belgrade, June 2012 S. Sahal-Bréchot Observatoire de Paris, LERMA CNRS UMR 8112, France The STARK-B database for spectral line broadening by collisions with charged particles in the framework of the European project VAMDC (Virtual Atomic and Molecular Data Center) 1

VAMDC Regional workshop, Belgrade, June Calculated widths and shifts: more than 150 pubs ( ) SCP theory updated and operated by M.S. Dimitrijević and S. Sahal-Bréchot and colleagues Technical development: Paris Observatory, LERMA, by N. Moreau, engineer the database has been opened since September 2008: 99% of the existing data are currently implemented It is a part of the atomic and molecular databases of the Paris Observatory Link (and mirror site in progress) to SerVO - Serbian Virtual Observatory It is a part of VAMDC- Virtual Atomic and Molecular Data Centre it follows the standards of VAMDC and Virtual Observatories (Europe: IVOA International Virtual Observatory Alliance) STARK-B Database for "Stark" widths and shifts of isolated spectral lines of atoms and ions, due to collisions with electrons and ions in a plasma b.obspm.fr b.obspm.fr 2

VAMDC Regional workshop, Belgrade, June 2012 STARK-B widths and shifts of isolated spectral lines of atoms and ions, due to collisions with electrons and ions in a plasma Overlapping lines and departures from impact approximation are outside the scope of STARK-B 3 Stark broadening of spectral lines can be applied to many subjects Astrophysics Laboratory plasmas Industrial plasmas Ionization degree ≥ 1% Moderately hot to very hot plasmas ( to ∼ 10 6 K) Moderate electron density (10 13 to cm -3 )

VAMDC Regional workshop, Belgrade, June Diagnostics and Modelling in Astrophysics: Understanding of the evolution of stars Thanks to considerable developments of –Ground based and space-born missions –Increased sensitivity (S/N) and spectral resolution –Powerful computers Interpretation of the faint observed spectrum : faint objects, faint lines (trace elements) Line intensities + line profiles Continuum Spectroscopic diagnostics: -Temperatures -pressure -Abundances -Chemical stratification of the atmosphere Modelling of atmospheres Synthetic spectra: a great number of lines of a same element are required Radiative transfer Stellar interiors studies and Asterosimology opacities: a great number of lines oh higly ionized elements are required Nuclear processes: formation of elements, chemical enrichment

VAMDC Regional workshop, Belgrade, June Diagnostics and Modelling in Astrophysics: Understanding of the evolution of stars Thanks to considerable developments of –Ground based and space-born missions –Increased sensitivity (S/N) and spectral resolution –Powerful computers Interpretation of the faint observed spectrum : faint objects, faint lines (trace elements) Line intensities + line profiles Continuum Spectroscopic diagnostics: -Temperatures -pressure -Abundances -Chemical stratification of the atmosphere Modelling of atmospheres Synthetic spectra: a great number of lines of a same element are required Radiative transfer Stellar interiors studies and Asterosimology opacities: a great number of lines oh higly ionized elements are required Nuclear processes: formation of elements, chemical enrichment

VAMDC Regional workshop, Belgrade, June Diagnostics and Modelling in Astrophysics: Understanding of the evolution of stars Thanks to considerable developments of –Ground based and space-born missions –Increased sensitivity (S/N) and spectral resolution –Powerful computers Interpretation of the faint observed spectrum : faint objects, faint lines (trace elements) Line intensities + line profiles Continuum Spectroscopic diagnostics: -Temperatures -pressure -Abundances -Chemical stratification of the atmosphere Modelling of atmospheres Synthetic spectra: a great number of lines of a same element are required Radiative transfer Stellar interiors studies and Asterosimology opacities: a great number of lines oh higly ionized elements are required Nuclear processes: formation of elements, chemical enrichment Sun abundances

VAMDC Regional workshop, Belgrade, June Diagnostics and Modelling in Laboratory and Industrial plasmas Thanks to developments and needs (devices an research) –Magnetic confinement fusion: moderately dense and hot plasmas (e.g. ITER) –Inertial confinement fusion (laser fusion, ion-beam fusion): dense and very hot plasmas –Low temperatures plasmas –Lighting discharges Analysis and interpretation of the spectrum in fusion devices and Tokamaks Light elements in the divertor and edge plasma regions Importance of Tin, Tungsten, and Aluminium ( Al-pellet Ablation Plasmas in Large Helical Device ) -Temperatures -Pressure Progress in low-energy light sources Discharge lamps and lighting : -optimisation of performances -cold light from hot atoms and molecules.(white light K, discharge up to 45000K),.high electron density (strong and broad emission in the visible spectrum -Fluorescent lamps: improving efficacity (phosphors) Rare earth elements Dy, Ho, Ce: excellent radiation sources HID (High Intensity Discharge): MH (Metal Halide) lamps, e.g. Dy I 3, In I, ZnI3 (LED light-emitting diodes)

VAMDC Regional workshop, Belgrade, June ρ typ /v << ΔT i.e. ρ typ << N -1/3 Impact approximation Collisions between radiators and perturbers act independently and are additive STARK-B data: Basic approximations (theory and calculations) Complete collision approximation  line broadening theory becomes an application of the theory of collisions The atom has no time to emit or absorb a photon during the collision process, the collision is not broken off. Isolated lines Neighbouring levels do not overlap i f i’i’ i’i’ f’f’ f’f’  Lorentz profile; S-matrix, cross-sections LS coupling: fine (hyperfine) structure can be neglected during the collision (S or I : no time to rotate)  The fine structure (hyperfine) components have the same width and the same shift, thet of the multiplet High densities:  Debye screening effect

VAMDC Regional workshop, Belgrade, June STARK-B Methods of calculations of the data 1. The scattering S-matrix SCP: Semi-Classical : atom = quantum description (atomic structure), perturber= particle moving on a classical path + Perturbation theory (2 nd order) – (Sahal-Bréchot, A&A1970 and further papers, 6-8 basic papers) unitarity and symmetrization of the S-matrix, adequate cut-offs hyperbolae for ion-electron and ion-ion (1970), complex atoms (1974), very complex (2008) Feshbach resonances for ion-electron collisions (1977) Updated and operated with MS. Dimitrijević (1984 and after) accuracy: 20%, sometimes better, sometimes worse MSE: Modified Semi-Empirical : atom = simplified quantum description Dimitrijević and colleagues, JQSRT1980 and further A&A papers)

VAMDC Regional workshop, Belgrade, June STARK-B Methods of calculations of the data 2 - The atomic structure –NIST atomic data –VALD (Vienna Atomic Line Database) –Coulomb approximation with quantum defect (Bates & Damgaard 1949) –TOPbase : R-matrix in LS coupling –Cowan code : HFS multi-conf with exchange and relativistic effects (by perturbations) –SUPERSTRUCTURE : scaled Thomas-Fermi-Dirac-Amaldi potential + relativistic effects (Breit-Pauli)

VAMDC Regional workshop, Belgrade, June STARK-B Methods of calculations of the data 3. Calculations leading to a great number of data Atomic structure coupled to the S-matrix calculation: Many widths and shifts for a set of several temperatures and densities in a same run -Ab initio calculations: no external data insertion -SST + SCP: data for 100 lines and more in a same run -Cowan code + SCP : in progress (case of Pb IV, more than 100 lines in a same run) -Coupling to atomic structure databases:  TopBase : data for 150 lines in a same run  VALD: data for more than 1000 lines in a same run (case of CII for white dwarfs)

VAMDC Regional workshop, Belgrade, June 2012 STARK-B: Elements (atoms and ions) currently inserted 12 Ag I, Al I, Al III, Al XI Ar I, Ar II, Ar II, Ar VIII Au I B II, B III Ba I, Ba II Be I, Be II, Be III Br I C II, C III, C IV, C V Ca I, Ca II, Ca V, Ca IX, Ca X Cd I, Cd II Cl I, Cl VII Cr I, Cr II Cu I F I, F II, F III,F IV, F V, F VI, F VII Fe II Ga I Ge I He I Hg II I In II, In III K I, K VIII, K IX Kr I, Kr II, Kr VIII Li I, Li II Mg I, Mg II, Mg XI Mn II N I, N II, N III, N IV, N V Na I, Na X Ne I, Ne II, Ne II, Ne III, Ne IV, Ne V, Ne VIII Ni II O I, O II, O III (in progress), O IV, O V, O VI; O VII P IV, P V Pb IV Pd I Rb I S III, S IV, S V, S VI Sc III, Sc X, Sc XI Se I Si I, Si II, Si IV, Si V, Si VI, Si XI, Si XII, Si XIII Sr I Te I Ti IV, Ti XII, Ti XIII Tl III V V, V XIII Y III Zn I C II in progress (150 lines, 4 temperatures, 3 densities)

VAMDC Regional workshop, Belgrade, June 2012 STARK-Bhttp://stark-b.obspm.frhttp://stark-b.obspm.fr 13

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June STARK-B: Next steps Insertion of MSE data Insertion of little “applets” on line for users: Fitting along temperatures (for astrophysics) extrapolation or interpolation (regularities and systematic trends)  along principal quantum numbers,  charge of the radiating ions (isoelectronic sequences),  homologous ions,  charge of the ion collider Future: SCP code on line: STARK-C project Insertion of quantum data in intermediate coupling : SST + DW especially adapted to highly charged ions and resonance lines (Sahal-Bréchot with Elabidi & Ben Nessib (2004 and after, an also with Dubau and Cornille 2007 and after )

VAMDC Regional workshop, Belgrade, June 2012 VAMDC project Virtual Atomic and Molecular Data Center 29 European project FP7 "Research Infrastructures summer end of 2012 Interoperable e-Infrastructure for exchange of atomic and molecular data 15 administrative partners: 24 teams o from 6 European Union member states, o Serbia, Russian Federation and Venezuela strong coupling o to the users (astrochemistry, atmospheric physics, plasmas) o scientists and engineers from the ICT community (Information and Communication Technologies) used to deal with deploying interoperable e-infrastructure e.g. Europlanet IDISEuroplanet IDIS IVOAIVOA (International Virtual Observatory Alliance) Members: Euro-VO, AstroGrid…Euro-VOAstroGrid

VAMDC Regional workshop, Belgrade, June 2012 VAMDC: portal user 30

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June 2012 Query 32

VAMDC Regional workshop, Belgrade, June 2012 Query by species 33

VAMDC Regional workshop, Belgrade, June 2012 Query by species: atom 34

VAMDC Regional workshop, Belgrade, June 2012 Query by species: atom (following) 35

VAMDC Regional workshop, Belgrade, June 2012 Query by species: atom, processes 36

VAMDC Regional workshop, Belgrade, June 2012 Query by species: atom, processes (following) 37

VAMDC Regional workshop, Belgrade, June 2012 Query : result, click on download 38 Xsams: XML Schema for Atoms, Molecules and Solids XML: Extensible Markup Language Xsams2SME: converts XML document into the CSV- format wanted by Spectroscopy Made Easy (SME)

VAMDC Regional workshop, Belgrade, June 2012 Result of the download: code in XML language for users 39 Xsams XML Schema for Atoms, Molecules and Solids

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June

VAMDC Regional workshop, Belgrade, June 2012 Thank you for your attention 44