000860801 001__ 860801
000860801 005__ 20240711113845.0
000860801 0247_ $$2doi$$a10.3390/atoms7010030
000860801 0247_ $$2Handle$$a2128/21881
000860801 0247_ $$2WOS$$aWOS:000464282200002
000860801 0247_ $$2altmetric$$aaltmetric:57397491
000860801 037__ $$aFZJ-2019-01462
000860801 082__ $$a530
000860801 1001_ $$0P:(DE-Juel1)167437$$avon Hellermann, Manfred$$b0$$eCorresponding author$$ufzj
000860801 245__ $$aSimulation of Spectra Code (SOS) for ITER Active Beam Spectroscopy
000860801 260__ $$aBasel$$bMDPI$$c2019
000860801 3367_ $$2DRIVER$$aarticle
000860801 3367_ $$2DataCite$$aOutput Types/Journal article
000860801 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1553179996_30752
000860801 3367_ $$2BibTeX$$aARTICLE
000860801 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000860801 3367_ $$00$$2EndNote$$aJournal Article
000860801 520__ $$aThe concept and structure of the Simulation of Spectra (SOS) code is described starting with an introduction to the physics background of the project and the development of a simulation tool enabling the modeling of charge-exchange recombination spectroscopy (CXRS) and associated passive background spectra observed in hot fusion plasmas. The generic structure of the code implies its general applicability to any fusion device, the development is indeed based on over two decades of spectroscopic observations and validation of derived plasma data. Four main types of active spectra are addressed in SOS. The first type represents thermal low-Z impurity ions and the associated spectral background. The second type of spectra represent slowing-down high energy ions created from either thermo-nuclear fusion reactions or ions from injected high energy neutral beams. Two other modules are dedicated to CXRS spectra representing bulk plasma ions (H+, D+, or T+) and beam emission spectroscopy (BES) or Motional Stark Effect (MSE) spectrum appearing in the same spectral range. The main part of the paper describes the physics background for the underlying emission processes: active and passive CXRS emission, continuum radiation, edge line emission, halo and plume effect, or finally the charge exchange (CX) cross-section effects on line shapes. The description is summarized by modeling the fast ions emissions, e.g., either of the α particles of the fusion reaction or of the beam ions itself
000860801 536__ $$0G:(DE-HGF)POF3-174$$a174 - Plasma-Wall-Interaction (POF3-174)$$cPOF3-174$$fPOF III$$x0
000860801 588__ $$aDataset connected to CrossRef
000860801 7001_ $$0P:(DE-HGF)0$$ade Bock, Maarten$$b1
000860801 7001_ $$0P:(DE-Juel1)5739$$aMarchuk, Oleksandr$$b2$$ufzj
000860801 7001_ $$0P:(DE-Juel1)5006$$aReiter, Detlev$$b3$$ufzj
000860801 7001_ $$0P:(DE-HGF)0$$aSerov, Stanislav$$b4
000860801 7001_ $$0P:(DE-HGF)0$$aWalsh, Michael$$b5
000860801 773__ $$0PERI:(DE-600)2704220-0$$a10.3390/atoms7010030$$gVol. 7, no. 1, p. 30 -$$n1$$p30 -$$tAtoms$$v7$$x2218-2004$$y2019
000860801 8564_ $$uhttps://juser.fz-juelich.de/record/860801/files/Invoice_MDPI_atoms-442870_0.00EUR.pdf
000860801 8564_ $$uhttps://juser.fz-juelich.de/record/860801/files/Invoice_MDPI_atoms-442870_0.00EUR.pdf?subformat=pdfa$$xpdfa
000860801 8564_ $$uhttps://juser.fz-juelich.de/record/860801/files/atoms-07-00030.pdf$$yOpenAccess
000860801 8564_ $$uhttps://juser.fz-juelich.de/record/860801/files/atoms-07-00030.pdf?subformat=pdfa$$xpdfa$$yOpenAccess
000860801 8767_ $$8atoms-442870$$92019-02-15$$d2019-02-15$$eAPC$$jZahlung erfolgt$$zWaiver
000860801 909CO $$ooai:juser.fz-juelich.de:860801$$pdnbdelivery$$popenCost$$pVDB$$pdriver$$pOpenAPC$$popen_access$$popenaire
000860801 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)167437$$aForschungszentrum Jülich$$b0$$kFZJ
000860801 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)5739$$aForschungszentrum Jülich$$b2$$kFZJ
000860801 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)5006$$aForschungszentrum Jülich$$b3$$kFZJ
000860801 9131_ $$0G:(DE-HGF)POF3-174$$1G:(DE-HGF)POF3-170$$2G:(DE-HGF)POF3-100$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bEnergie$$lKernfusion$$vPlasma-Wall-Interaction$$x0
000860801 9141_ $$y2019
000860801 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection
000860801 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000860801 915__ $$0StatID:(DE-HGF)0112$$2StatID$$aWoS$$bEmerging Sources Citation Index
000860801 915__ $$0StatID:(DE-HGF)0501$$2StatID$$aDBCoverage$$bDOAJ Seal
000860801 915__ $$0StatID:(DE-HGF)0500$$2StatID$$aDBCoverage$$bDOAJ
000860801 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000860801 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bDOAJ : Blind peer review
000860801 915__ $$0StatID:(DE-HGF)0300$$2StatID$$aDBCoverage$$bMedline
000860801 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List
000860801 920__ $$lyes
000860801 9201_ $$0I:(DE-Juel1)IEK-4-20101013$$kIEK-4$$lPlasmaphysik$$x0
000860801 9801_ $$aAPC
000860801 9801_ $$aFullTexts
000860801 980__ $$ajournal
000860801 980__ $$aVDB
000860801 980__ $$aUNRESTRICTED
000860801 980__ $$aI:(DE-Juel1)IEK-4-20101013
000860801 980__ $$aAPC
000860801 981__ $$aI:(DE-Juel1)IFN-1-20101013