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Dual anode source

Fig. 19. Schematic of dual anode (typically Al and Mg) x-ray source. X-rays produced by electron bombardment of anode face 2 indicated (19). The routine dual-anode x-ray source just described generates nonmonochromatized x-rays in a relatively large spot size (ca 1 cm in diameter). In... Fig. 19. Schematic of dual anode (typically Al and Mg) x-ray source. X-rays produced by electron bombardment of anode face 2 indicated (19). The routine dual-anode x-ray source just described generates nonmonochromatized x-rays in a relatively large spot size (ca 1 cm in diameter). In...
XPS spectra were obtained using a Perkin-Elmer Physical Electronics (PHI) 555 electron spectrometer equipped with a double pass cylindrical mirror analyzer (CMA) and 04-500 dual anode x-ray source. The x-ray source used a combination magnesium-silicon anode, with collimation by a shotgun-type collimator (1.). AES/SAM spectra and photomicrographs were obtained with a Perkin-Elmer PHI 610 Scanning Auger Microprobe, which uses a single pass CMA with coaxial lanthanum hexaboride (LaBe) electron gun. [Pg.38]

The PHI Model 548 ESCA/ AES spectrometer (Physical Electronics Inc., Eden Prairie, MN) previously described (10,13) has been modified by the replacement of the original x-ray source with a PHI Model 1548 dual anode, 300W x-ray source. All binding energies are referenced to the Au 4f peak at 83.8 eV. [Pg.585]

Fig. 19. Schematic of dual anode (typically Al and Mg) x-ray source. X-rays produced by electron bombardment of anode face 2 indicated (19). Fig. 19. Schematic of dual anode (typically Al and Mg) x-ray source. X-rays produced by electron bombardment of anode face 2 indicated (19).
All XPS or ESCA measurements were performed using a Perkin Elmer 5300 ESCA spectrometer equipped with a dual anode (Mg, Al) X-ray source, differentially pumped Ar+ sputter gun, and the variable angle measurement set-up for angle-resolved photoelectron spectroscopic measurements. The data collection and treatment, e.g. smoothing, curve-fitting, intensity measurements, were accomplished by a Perkin Elmer 7500 dedicated computer system using PHI software package. [Pg.447]

XPS was used in Che Li project co characterize Che adsorption of THF on Li surfaces. It was performed in a Perkin-Elmer UHV chamber. The photon source was a Al-Mg dual anode X-Ray gun. The Mg anode was used in this work. The energy of the major Mg x-ray line is 1253.6 eV with a FWHM of 0.65 eV. Mg also has x-ray satellites at energies 8.4, 10.2 17.5, 20 and 48.5 eV higher than the major line. These satellites will cause corresponding satellite peaks of a major XPS peak. The gun was operated at 15-KeV and a power of 400 watts. The incident angle of the photons was typically 55 and the take-off angle of the photoelectrons was 0° with respect to the normal of a sample surface. [Pg.51]

Surface analysis (AES/XPS) Electron spectroscopy for elemental analysis of surfaces, sensitive to as low as two atomic layers. Physical electronics model PHI-570 Auger Electron Spectroscopy/X-ray Photoelectron Spectroscopy System is a double pass cylindrical mirror energy analyzer with dual anode (Mg/Al) X-ray source and has a rapid sample introduction probe. It can detect elements at the first five to ten atomic layers of sample and detect all elements except H and He. [Pg.72]

Radiation Source. The radiation source used in ESCA is a standard X-ray anode tube, as described in Chapter 8. Soft X-rays are used, with A1 and Mg being the most common anodes. Many commercial systems offer a dual anode X-ray tube so that the analyst can switch between excitation wavelengths. It is very important that the X-ray source be monochromatic, with a linewidth extending over as narrow an energy range as possible. A1 and Mg have narrow K emission lines. The Mg K line has an energy of... [Pg.882]

Hawn (1983) has described the performance of a dual-anode X-ray source for XPS using various un-collimated and collimated configurations to make it effective in increasing the signal-to-background ratio and reducing anode cross talk without substantial signal loss. [Pg.222]

X ray photoelectron spectroscopy (XPS) was performed on a Riber MacII XPS instrument (non-monochromated dual anode Al/Mg Ka X ray source, 5 10 ° Torr in analysis chamber, 12 kV / 10 mA power, 50 / 43 ° X-ray incidence / photoelectron take-off angles, 0.9 eV resolution, 0.05 eV / 100 ms steps). C(ls) photoionization peak at 285.0 eV was used for energy calibration. Surface sputtering was achieved with a Riber Cl 50 ion gun (3.0 keV Kr, 4.0 lO " nm.s ). The effects of the thermal treatments were monitored by deriving the ions surface concentrations from the... [Pg.154]

The XPS investigations here described for the various oxide systems have been carried out using a Perkin Elmer O 5600 Multi Technique System located at the Department of Chemistry of the University of Padova (Italy), equipped with a dual Mg - A1 anode as the X-ray source. Magnesium and aluminium are the two materials used universally as anodes in soft X-ray sources (Mg Ka = 1253.6 eV, FWHM = 0.70 eV A1 Ka = 1486.6 eV, FWHM = 0.85 eV). [Pg.135]

Othman, M.H.D. et al., Novel fabrication technique of hollow fibre support for microtubular solid oxide fuel cells. Journal of Power Sources, 2011.196( 11) 5035-5044. Othman, M.H.D. et al., Dual-layer hollow fibres with different anode stmctuies for micro-tubular solid oxide fuel cells. Journal of Power Sources, 2012. 205 272-280. [Pg.346]


See other pages where Dual anode source is mentioned: [Pg.282]    [Pg.11]    [Pg.136]    [Pg.37]    [Pg.42]    [Pg.125]    [Pg.56]    [Pg.293]    [Pg.282]    [Pg.41]    [Pg.199]    [Pg.42]    [Pg.245]    [Pg.282]    [Pg.888]    [Pg.285]    [Pg.1006]    [Pg.1012]    [Pg.18]    [Pg.221]    [Pg.857]    [Pg.63]    [Pg.660]    [Pg.588]    [Pg.168]    [Pg.171]    [Pg.270]    [Pg.540]    [Pg.214]    [Pg.66]    [Pg.5]    [Pg.104]    [Pg.25]    [Pg.76]   
See also in sourсe #XX -- [ Pg.11 ]




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