RE.PUBLIC@POLIMI pubblicazioni di ricerca del Politecnico di Milano

An end-station for resonant inelastic X-ray scattering and (resonant) X-ray emission spectroscopy at beamline ID20 of ESRF - The European Synchrotron is presented. The spectrometer hosts five crystal analysers in Rowland geometry for large solid angle collection and is mounted on a rotatable arm for scattering in both the horizontal and vertical planes. The spectrometer is optimized for high-energy-resolution applications, including partial fluorescence yield or high-energy-resolution fluorescence detected X-ray absorption spectroscopy and the study of elementary electronic excitations in solids. In addition, it can be used for non-resonant inelastic X-ray scattering measurements of valence electron excitations.An end-station for resonant inelastic X-ray scattering at beamline ID20 of ESRF - The European Synchrotron is described. The spectrometer is optimized for high-energy-resolution applications, including partial fluorescence yield or high-energy-resolution fluorescence detected X-ray absorption spectroscopy and the study of elementary electronic excitations in solids.

A high-energy-resolution resonant inelastic X-ray scattering spectrometer at ID20 of the European Synchrotron Radiation Facility

Sala, M. Moretti;
2018-01-01

Abstract

An end-station for resonant inelastic X-ray scattering and (resonant) X-ray emission spectroscopy at beamline ID20 of ESRF - The European Synchrotron is presented. The spectrometer hosts five crystal analysers in Rowland geometry for large solid angle collection and is mounted on a rotatable arm for scattering in both the horizontal and vertical planes. The spectrometer is optimized for high-energy-resolution applications, including partial fluorescence yield or high-energy-resolution fluorescence detected X-ray absorption spectroscopy and the study of elementary electronic excitations in solids. In addition, it can be used for non-resonant inelastic X-ray scattering measurements of valence electron excitations.An end-station for resonant inelastic X-ray scattering at beamline ID20 of ESRF - The European Synchrotron is described. The spectrometer is optimized for high-energy-resolution applications, including partial fluorescence yield or high-energy-resolution fluorescence detected X-ray absorption spectroscopy and the study of elementary electronic excitations in solids.
2018
JOURNAL OF SYNCHROTRON RADIATION
ESRF; ID20 beamline; resonant inelastic X-ray scattering; RIXS spectrometer; X-ray emission; Radiation; Nuclear and High Energy Physics; Instrumentation
01.1 Articolo in Rivista
{% } %}
{%# o.licenseName %}
File in questo prodotto:
File Dimensione Formato  
sendreprint.pdf

accesso aperto

: Publisher’s version
Dimensione 1.21 MB
Formato Adobe PDF
Visualizza/Apri
1.21 MB Adobe PDF Visualizza/Apri

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11311/1049071
Citazioni
  • ???jsp.display-item.citation.pmc??? 16
'); $.ajax({ url: '/itemExternalCitation/pmc/get.json', dataType: 'json', data: { discriminator: 'pmc', itemId: 'e0c31c21-83f9-4599-e053-1705fe0aef77', forceUpdate: forceUpdate } }).done(function(adata) { $('#pmcCitedResultTotal').tooltip('dispose'); $('#pmcCitedResultTotal').prop("onclick", null).off("click"); if (adata.total==null){ $('#pmcCitedResultTotal').html('16'); } else { $('#pmcCitedResultTotal').html(adata.total); } var year=new Date().getFullYear(); pmcChartData[0] = (adata.yearTotalMap[''+(year-5)]!=null ? adata.yearTotalMap[''+(year-5)] : 0); pmcChartData[1] = (adata.yearTotalMap[''+(year-4)]!=null ? adata.yearTotalMap[''+(year-4)] : 0); pmcChartData[2] = (adata.yearTotalMap[''+(year-3)]!=null ? adata.yearTotalMap[''+(year-3)] : 0); pmcChartData[3] = (adata.yearTotalMap[''+(year-2)]!=null ? adata.yearTotalMap[''+(year-2)] : 0); pmcChartData[4] = (adata.yearTotalMap[''+(year-1)]!=null ? adata.yearTotalMap[''+(year-1)] : 0); pmcChartData[5] = (adata.yearTotalMap[''+year]!=null ? adata.yearTotalMap[''+year] : 0); drawChart(); }).always(function(adata){ //console.log('end pmcUpdateCitation'); runningExternal=false; }); }
  • Scopus 76
    • '); $.ajax({ url: '/itemExternalCitation/scopus/get.json', dataType: 'json', data: { discriminator: 'scopus', itemId: 'e0c31c21-83f9-4599-e053-1705fe0aef77', forceUpdate: forceUpdate } }).done(function(adata) { $('#scopusCitedResultTotal').tooltip('dispose'); $('#scopusCitedResultTotal').prop("onclick", null).off("click"); if (adata.total==null){ $('#scopusCitedResultTotal').html('76'); } else { $('#scopusCitedResultTotal').html(adata.total); } var year=new Date().getFullYear(); scopusChartData[0] = (adata.yearTotalMap[''+(year-5)]!=null ? adata.yearTotalMap[''+(year-5)] : 0); scopusChartData[1] = (adata.yearTotalMap[''+(year-4)]!=null ? adata.yearTotalMap[''+(year-4)] : 0); scopusChartData[2] = (adata.yearTotalMap[''+(year-3)]!=null ? adata.yearTotalMap[''+(year-3)] : 0); scopusChartData[3] = (adata.yearTotalMap[''+(year-2)]!=null ? adata.yearTotalMap[''+(year-2)] : 0); scopusChartData[4] = (adata.yearTotalMap[''+(year-1)]!=null ? adata.yearTotalMap[''+(year-1)] : 0); scopusChartData[5] = (adata.yearTotalMap[''+year]!=null ? adata.yearTotalMap[''+year] : 0); drawChart(); }).always(function(adata){ //console.log('end scopusUpdateCitation'); runningExternal=false; }); }
  • ???jsp.display-item.citation.isi??? 76
    • '); $.ajax({ url: '/itemExternalCitation/isi/get.json', dataType: 'json', data: { discriminator: 'isi', itemId: 'e0c31c21-83f9-4599-e053-1705fe0aef77', forceUpdate: forceUpdate } }).done(function(adata) { $('#isiCitedResultTotal').tooltip('dispose'); $('#isiCitedResultTotal').prop("onclick", null).off("click"); if (adata.total==null){ $('#isiCitedResultTotal').html('76'); } else { $('#isiCitedResultTotal').html(adata.total); } var year=new Date().getFullYear(); isiChartData[0] = (adata.yearTotalMap[''+(year-5)]!=null ? adata.yearTotalMap[''+(year-5)] : 0); isiChartData[1] = (adata.yearTotalMap[''+(year-4)]!=null ? adata.yearTotalMap[''+(year-4)] : 0); isiChartData[2] = (adata.yearTotalMap[''+(year-3)]!=null ? adata.yearTotalMap[''+(year-3)] : 0); isiChartData[3] = (adata.yearTotalMap[''+(year-2)]!=null ? adata.yearTotalMap[''+(year-2)] : 0); isiChartData[4] = (adata.yearTotalMap[''+(year-1)]!=null ? adata.yearTotalMap[''+(year-1)] : 0); isiChartData[5] = (adata.yearTotalMap[''+year]!=null ? adata.yearTotalMap[''+year] : 0); drawChart(); }).always(function(adata){ //console.log('end isiUpdateCitation'); runningExternal=false; }); }
    social impact