XRay Emission Spectroscopy Photons in and Photons out

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X-Ray Emission Spectroscopy Photons in and Photons out Jan-Erik Rubensson Uppsala University Summer School,

X-Ray Emission Spectroscopy Photons in and Photons out Jan-Erik Rubensson Uppsala University Summer School, Odengården, May 26 - June 2, 2008

Outline • • General Introduction Local Partial Density of States Site Selectivity Typical attenuation

Outline • • General Introduction Local Partial Density of States Site Selectivity Typical attenuation length: 1000Å Instrumentation Soft X-ray spectrometers: Resolution, resolution and the new PGS Synchrotron radiation: Brilliance, brilliance and MAX-IV RIXS; Resonant Inelastic Soft X-ray Scattering Always a one-step process Energy conservation Momentum conservation Symmetry selectivity Dynamics Interference and vibronic coupling Core-hole clock Applications Complex Systems

X-ray emission: Characteristic radiation? H. G. J. Moseley, M. A. Phil. Mag. (1913), p.

X-ray emission: Characteristic radiation? H. G. J. Moseley, M. A. Phil. Mag. (1913), p. 1024

Yes, but also uncharacteristic Valence electronic struture Phys. Rev. 45, 370 (1935)

Yes, but also uncharacteristic Valence electronic struture Phys. Rev. 45, 370 (1935)

Core levels are atomic-like: Local Properties Dipole Selection rules are valid: Symmetry Selectivity Valence

Core levels are atomic-like: Local Properties Dipole Selection rules are valid: Symmetry Selectivity Valence Band Local Si (s+d) Si 2 p Local Cp C 1 s Local Partial Density of States

Very little has been done with synchrotron radiation: Notoriously low count rates Conduction Valence

Very little has been done with synchrotron radiation: Notoriously low count rates Conduction Valence Core Intermediate 0. 1% Final Ground

Rowland spectrometer Source Detector Grating Combining the focussing properties of a sphere with the

Rowland spectrometer Source Detector Grating Combining the focussing properties of a sphere with the dispersive properties of a grating

Still going strong…

Still going strong…

New Concepts for efficiency and resolution PGS: Plane grating spectrometer Two parabolic mirrors and

New Concepts for efficiency and resolution PGS: Plane grating spectrometer Two parabolic mirrors and a plane grating FTS: Fourier Transform Spectrometer Wavefront Beamsplitters and mirrors in grazing incidence

Experiment

Experiment

X-ray scattering; always a one-step process Core Excited Emission: Absorption: Valence Excited Ground State

X-ray scattering; always a one-step process Core Excited Emission: Absorption: Valence Excited Ground State

Linear approximation M. Blume, J. Appl. Phys. 57, 3615 (-85): This equation ’accounts for

Linear approximation M. Blume, J. Appl. Phys. 57, 3615 (-85): This equation ’accounts for most scattering phenomena to the order of . ’

’One can get X-ray emission from everything except hydrogen and helium’ Distinguished Professor Helium

’One can get X-ray emission from everything except hydrogen and helium’ Distinguished Professor Helium Doubly excited states 2 l’n’l’’ Singly excited states 1 snl Ground 1 s 2

Schulz et al. , PRL 1996 2 l’n’l’’ 1 s + e 1 s

Schulz et al. , PRL 1996 2 l’n’l’’ 1 s + e 1 s 2 Autoionizing resonances?

Symmetry resolution in RIXS Strict dipole selection rules: J. Söderström et al. , PRA

Symmetry resolution in RIXS Strict dipole selection rules: J. Söderström et al. , PRA 2008 Influence of s-o coupling and external fields, two-color experiments, PGS measurements…

’A core hole is localized at one atomic site’ Distinguished Professor The oxygen molecule

’A core hole is localized at one atomic site’ Distinguished Professor The oxygen molecule ’ Right? O O Both? Left? O O Strict dipole selection rules apply: Gerade Ungerade Gerade Inversion symmetry is not broken P. Glans, et al. PRL 76, 2488 (-96)

Carbon Dioxide 1. Vibrations break the symmetry O O 2. But not if the

Carbon Dioxide 1. Vibrations break the symmetry O O 2. But not if the energy is detuned Scattering duration time! P. Skytt, et al. , PRL 77, 5035 (-96)

’The core-hole lifetime width will always be limiting the information you can get out

’The core-hole lifetime width will always be limiting the information you can get out of RIXS spectra. ’ Distinguished Professor Energy Conservation 4 d 4 f resonance in La. F 3 Scattering: Gives narrow peaks. intensity indicates that the 4 f electron escapes during the process: Core hole Clock!

’But you can never do band mapping with X-ray emisson because the core hole

’But you can never do band mapping with X-ray emisson because the core hole destroys the translational symmetry. ’ Distinguished Professor Momentum Conservation S. Eisebitt et al. , 1998

Silicon Carbide again J. Lüning et al. , PRB 56 -97

Silicon Carbide again J. Lüning et al. , PRB 56 -97

’This gives me a headache’ Distinguished Professor Site Selectivity in Complex Systems

’This gives me a headache’ Distinguished Professor Site Selectivity in Complex Systems

Looking Through Windows Several 1000 Ångström -gases -liquids -gas/liquid/solid interfaces

Looking Through Windows Several 1000 Ångström -gases -liquids -gas/liquid/solid interfaces

Many applications of liquid studies • Biology, Pharmaceutics, Drug solubility • Electrochemistry, battery technology,

Many applications of liquid studies • Biology, Pharmaceutics, Drug solubility • Electrochemistry, battery technology, corrosion • Environmental Science, etc. . .

Acknowledgements Soft X-ray Group in Uppsala Mjukröntgengruppen http: //usxs. fysik. uu. se/

Acknowledgements Soft X-ray Group in Uppsala Mjukröntgengruppen http: //usxs. fysik. uu. se/