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Microscope field ion

The field ion microscope (FIM) has been used to monitor surface self-diflfiision in real time. In the FIM, a sharp, crystalline tip is placed in a large electric field in a chamber filled with Fie gas [14]. At the tip. Fie ions are fonned, and then accelerated away from the tip. The angular distribution of the Fie ions provides a picture of the atoms at the tip with atomic resolution. In these images, it has been possible to monitor the diflfiision of a single adatom on a surface in real time [15]. The limitations of FIM, however, include its applicability only to metals, and the fact that the surfaces are limited to those that exist on a sharp tip, i.e. difhision along a large... [Pg.292]

The atom probe field-ion microscope (APFIM) and its subsequent developments, the position-sensitive atom probe (POSAP) and the pulsed laser atom probe (PLAP), have the ultimate sensitivity in compositional analysis (i.e. single atoms). FIM is purely an imaging technique in which the specimen in the form of a needle with a very fine point (radius 10-100 nm) is at low temperature (liquid nitrogen or helium) and surrounded by a noble gas (He, Ne, or Ar) at 10 -10 Pa. A fluorescent screen or a... [Pg.179]

In addition to the wet and optical spectrometric methods, which are often used to analyse elements present in very small proportions, there are also other techniques which can only be mentioned here. One is the method of mass spectrometry, in which the proportions of separate isotopes can be measured this can be linked to an instrument called a field-ion microscope, in which as we have seen individual atoms can be observed on a very sharp hemispherical needle tip through the mechanical action of a very intense electric field. Atoms which have been ionised and detached can then be analysed for isotopic mass. This has become a powerful device for both curiosity-driven and applied research. [Pg.234]

The atom probe (AP) consists of a modified field ion microscope (FIM), and we will first review the basic phenomena involved in the operation of the FIM. [Pg.3]

Diffuse reflectance infrared Fourier transform spectroscopy deuterium triglycine sulphate energy compensated atom probe energy dispersive analysis energy-loss near edge structure electron probe X-ray microanalysis elastic recoil detection analysis (see also FreS) electron spectroscopy for chemical analysis extended energy-loss fine structure field emission gun focused ion beam field ion microscope... [Pg.226]

The opening chapter, however, gives an account of the ultimate technique in local analysis, namely that of the atom probe field ion microscope. Here no probe is employed as in the above list, but individual atoms of the specimen are removed and identified by mass spectroscopy. [Pg.229]

Field emission microscopy was the first technique capable of imaging surfaces at resolution close to atomic dimensions. The pioneer in this area was E.W. Muller, who published the field emission microscope in 1936 and later the field ion microscope in 1951 [23]. Both techniques are limited to sharp tips of high melting metals (tungsten, rhenium, rhodium, iridium, and platinum), but have been extremely useful in exploring and understanding the properties of metal surfaces. We mention the structure of clean metal surfaces, defects, order/disorder phenomena,... [Pg.191]

Evidently, Eq. (39) cannot be valid whenever the tip does not possess an exact hemispherical symmetry for instance, whenever traces of crystallographic planes are visible in the field-ion microscope, the value of the radius of curvature becomes nearer to infinity than to the r of Fig. 5. It is interesting to note also that the theory admits no direct effect of the electrostatic field on the value of ys. In liquids, the effect of E on y gave rise to a whole branch of science usually known as electro-capillarity. An attempt to inaugurate an electrocapillarity of solids is mentioned in Section III.9. [Pg.28]

A particular complex problem has been the modelling of Si/W(l 10) Amar et have included pairwise interactions up to the sixth nearest neighbor shell, as estimated experimentally from field-ion microscopic studies The predicted phase diagram (Fig. 30) exhibits (5 x 1), (6 x 1) and p(2 x 1) commensurate phases, as well as a broad regime of an incommensurate phase. In contrast to the ANNNI model the present model does seem to have a finite-temperature Lifshitz point, where the incommensurate, commensurate... [Pg.139]

Fig. 1.32. Schematics of a field-ion microscope (FIM). The sample, a tip of radius 100 A is at a high positive voltage relative to a fluorescent screen, placed in a chamber filled with a few millitorrs of He. The He ions generated at the tip surface projects an atomic image of the tip. (Reproduced from Tsong, 1990, with permission.)... Fig. 1.32. Schematics of a field-ion microscope (FIM). The sample, a tip of radius 100 A is at a high positive voltage relative to a fluorescent screen, placed in a chamber filled with a few millitorrs of He. The He ions generated at the tip surface projects an atomic image of the tip. (Reproduced from Tsong, 1990, with permission.)...
Tsong, T, T. (1979). Quantitative atom-probe and field ion microscope studies at atomic resolution. Direct Imaging of Atoms in Crystals and Molecules Nobel Symposium 47, The Royal Swedish Academy of Sciences, 7-15. [Pg.402]

Basic principle of the atom-probe field ion microscope... [Pg.7]


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Atom-probe field ion microscope

Basic design of the field ion microscope

Resolution of the field ion microscope

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