8. 6  Search for Electronic Structures by Means of Weak Emission of Soft X-Rays
- Development of a Highly Efficient Soft X-Ray Spectrometer
 


Fig. 8-12 Schematic for the soft X-ray emission process

Irradiation with synchrotron radiation or with keV-order electrons leads to emission of photoelectrons and soft X-rays. Information about the partial DOS (density of states) in the valence band (VB) region can be obtained by means of soft X-ray emission spectroscopy.


Fig. 8-13 Optical arrangement for soft X-ray spectroscopy

A CCD camera moving on a carriage with a Rowland circle of 1 m radius detects weak soft X-rays.


Fig. 8-14 Si L2,3 emission spectra from a Si single crystal, where the specimen is bombarded with a beam of 5 keV Ar ions

Distinct peak structures A and B observed for the crystalline state are changed into a structureless profile for the amorphous state produced by Ar bombardment.



Since the early 1970's photoemission spectroscopy has been widely used for analyses of electronic structures and, in particular, it has played an important role in research on high Tc superconductors. Recently, a great deal of attention has been paid to soft X-ray emission spectroscopy using high-intensity synchrotron radiation. This kind of spectroscopy can reveal the individual components of atomic orbitals which make up the valence band in solid materials (Fig. 8-12). However, the emissivity is so small that it takes time from ~1 hour to 10 hours to obtain a good spectrum.
A spectrometer which we have developed employs a CCD camera as a detector (Fig. 8-13). The CCD surface consists of a few million pixels (24 micrometer square), each of which works as an independent counter for soft X-rays. To achieve sufficient energy-resolution (E/DeltaE:
500 - 1500) and to cover a wide range of measurable energies (50 - 1500 eV), the soft X-rays are arranged to strike the CCD surface at a low angle (1.5 - 12°). Data obtained for pure silicon suggest that the distribution of atomic orbitals in the crystalline state is quite different from that in the amorphous state (Fig. 8-14).
The present work has brought about a substantial reduction in the measurement time, an extension of the measurable energies, and a reduction of the optical size. The spectrometer will be used for high-speed spectral measurements (i.e., a few seconds) by resonant excitation using synchrotron radiation and for detailed analyses of complicated electronic structures such as strongly-correlated electron systems.



Reference
T. A. Sasaki et al., Performance of Soft X-Ray Emission Spectrometer Employing CCD Detector, Nucl. Instrum. Methods Phys. Res., A, 467-468, 1489 (2001).

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Persistent Quest - Research Activities 2001
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