Abstract

We report on the development of a high-resolution and highly efficient beamline for soft X-ray resonant inelastic X-ray scattering (RIXS) located at the Taiwan Photon Source. This beamline adopts an optical design that uses an active grating monochromator (AGM) and an active grating spectrometer (AGS) to implement the energy compensation principle of grating dispersion. Active gratings are utilized to diminish defocus, coma and higher-order aberrations, as well as to decrease the slope errors caused by thermal deformation and optical polishing. The AGS is mounted on a rotatable granite platform to enable momentum-resolved RIXS measurements with scattering angles over a wide range. Several high-precision instruments developed in-house for this beamline are described briefly. The best energy resolution obtained from this AGM-AGS beamline was 12.4 meV at 530 eV, achieving a resolving power of 4.2× 104, while the bandwidth of the incident soft X-rays was kept at 0.5 eV. To demonstrate the scientific impact of high-resolution RIXS, we present an example of momentum-resolved RIXS measurements on a high-temperature superconducting cuprate, i.e. La2-xSrxCuO4. The measurements reveal the A1g buckling phonons in superconducting cuprates, opening a new opportunity to investigate the coupling between these phonons and charge-density waves.

Highlights

  • The energy dispersion of low-energy elementary excitations in momentum space reflects the fundamental physical properties of materials

  • Resonant inelastic X-ray scattering (RIXS) is a powerful technique to probe these excitations with momentum resolution, and provides direct information about the dynamics arising from fluctuations of spin, charge and orbital degrees of freedom (Kotani & Shin, 2001; Ament et al, 2011a)

  • We report on the development of the soft X-ray active grating monochromator (AGM)–active grating spectrometer (AGS) RIXS beamline located at Taiwan Photon Source (TPS) port 41A

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Summary

Introduction

The energy dispersion of low-energy elementary excitations in momentum space reflects the fundamental physical properties of materials. If the energy of the incident photons is tuned to an absorption resonance in which a core-level electron is excited to an unoccupied state, the subsequent X-ray emission spectrum depends strongly on the incident photon energy; this process is called resonant IXS, i.e. RIXS (Kotani & Shin, 2001; Ament et al, 2011a).

Photon source
Focusing optics and slits
Singh et al Soft X-ray AGM–AGS RIXS beamline 979
AGM–AGS scheme
Active gratings
Optical tables and AGS rotation platform
Sample manipulation
Soft X-ray 2D detector
Instrumentation control and user interface
Beam size
Adjustment of the grating surface profile
Resolution optimization
Photon flux on the sample
Phonon excitations of superconducting cuprates
Summary and future plan

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