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Photo-emission

Detector is an internal photo-emission (IPE) device. Detector is a supedattice (SL) device. [Pg.420]

MAGNETIC DICHROISM IN VALENCE BAND X-RAY PHOTO EMISSION SPECTROSCOPY... [Pg.187]

As has been demonstrated by various authors an expression for the photo electron current intensity l E,k,ms uj,q, ) observed in VB-photo emission can be derived by... [Pg.187]

In summary, a fully relativistic theoretical description of photo emission for magnetic solids has been presented that is based on multiple scattering theory. For the VB-XPS case a very simple expression for the photo current intensity is found that can... [Pg.189]

The sensitivity of a photo-emissive cell (phototube) may be considerably increased by means of the so-called photomultiplier tube. The latter consists of an electrode covered with a photo-emissive material and a series of positively charged plates, each charged at a successively higher potential. The plates are covered with a material which emits several (2-5) electrons for each electron collected on its surface. When the electrons hit the first plate, secondary electrons are emitted in greater number than initially struck the plate, with the net result of a large amplification (up to 106) in the current output of the cell. The output of a photomultiplier tube is limited to several milliamperes, and for this reason only low incident radiant energy intensities can be employed. It can measure intensities about 200 times weaker than those measurable with an ordinary photoelectric cell and amplifier. [Pg.659]

Perkins and Andersen, 31 photo emission method (Barker), 41 potentiostatic scrape method, 38 piezo electric method (Gokstein), 42 rapid emergent method (Packham), 38... [Pg.640]

Coherent lattice motions can create periodic modulation of the electronic band structure. Time-resolved photo-emission (TRPE) studies [20-22] demonstrated the capability to detect coherent phonons as an oscillatory shift of... [Pg.52]

Photoemissive tubes are necessary for work in the ultraviolet range and they show greater sensitivity and precision than photoelectric cells. A simple photo-emissive tube consists of two electrodes in a vacuum. A silver cathode coated with an alkali metal is maintained at a potential difference of about 100 V from the anode, which is a plain silver wire and serves to collect the electrons (Figure 2.26(a)). [Pg.68]

The characterization of graphene often involves several techniques in conjunction in order to build up a complete picture of the material. The techniques typically include electron microscopy, Raman spectroscopy, X-ray photo-emission spectroscopy (XPS), Fourier-transform infrared spectroscopy (FTIR) and thermal-gravimetric analysis (TGA). [Pg.33]

In our opinion, the use of and calculations for one-particle Green s functions are uniquely suitable for solid-state systems periodic in any number of dimensions. When faithfully implemented, it satisfies all criteria above. Green s functions offer analytically compact and physically rich tools for representing many properties for extended, periodic systems. They satisfy powerful and elegant relations for quantities such as density of states, lifetimes for excitations, dielectric functions, photo-emission and absorption spectra, total crystal energies, and many more. [Pg.38]

P. Begley, R. Corbin, B.E. Poulger and P.G. Simmonds, Photo-emissive ionization source for ion mobility detectors. Journal of Chromatography 588 (1991) 239-249. [Pg.200]

This chapter is devoted to photoemission spectroscopy and the related inverse photo-emission spectroscopy, which are well developed experimental tools to study occupied and empty electronic levels, respectively. Special emphasis is given to the 5f electrons and their localized or delocalized character. [Pg.199]

Fig. IS. Angle-resolved photo emission from the edge surface of MoS2 single crystal (72), and imaginary sketch of reconstructed (T0I0) and (I0T0) surfaces. Incident angle of He—I was fixed at 30"C. Fig. IS. Angle-resolved photo emission from the edge surface of MoS2 single crystal (72), and imaginary sketch of reconstructed (T0I0) and (I0T0) surfaces. Incident angle of He—I was fixed at 30"C.
The fact that the Sc3N C80 molecule as a whole has only C3 symmetry (or even is reduced to Ci in the solid state [43]) does not give rise to a lifting of the degeneracy of C80 s molecular orbitals visible above the vibronic broadening, which dominates the width of the individual molecular orbitals in valence band photo emission. [Pg.224]

ARPES Angle-Resolved Photo-Emission Spectroscopy A general term for structure sensitive photoemission techniques, including ARPEFS, ARXPS, ARUPS, and ARXPD. [Pg.8]


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Electron photo-emission

Photo emission process

Photo induced electron emission

Photo induced electron emission from metals

X-ray Emission and (Photo)Electron Spectroscopies

X-ray photo emission

X-ray photo-emission spectroscopy

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