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Angular correlation of annihilated radiation

Fig. 6.15. Cylindrically averaged angular correlation of annihilation radiation (ACAR) distributions for positron annihilation in the noble gases, (a) helium, (b) neon, (c) argon, (d) krypton and (e) xenon, from the work of Coleman et al. (1994). Reprinted from Journal of Physics B27, Coleman et al, Angular correlation studies of positron annihilation in the noble gases, 981-991, copyright 1994, with permission from IOP Publishing. Fig. 6.15. Cylindrically averaged angular correlation of annihilation radiation (ACAR) distributions for positron annihilation in the noble gases, (a) helium, (b) neon, (c) argon, (d) krypton and (e) xenon, from the work of Coleman et al. (1994). Reprinted from Journal of Physics B27, Coleman et al, Angular correlation studies of positron annihilation in the noble gases, 981-991, copyright 1994, with permission from IOP Publishing.
A broad overview of traditional methods and recent developments in experimental positron spectroscopy is presented. A discussion of the generation and detection of positrons and their annihilation radiation is followed by a survey of techniques used for positron lifetime measurement, Doppler broadening spectroscopy and angular correlation of annihilation radiation, and the opportunities presented by combining these methods (e.g. in age-momentum correlation) and/or extending their capabilities by the use of monoenergetic positron beams. Novel spectroscopic and microscopic techniques using positron beams are also described. [Pg.37]

Figure 8.12 Cross section in the (kx, ky) plane of the calculated Fermi surface in Y 1 2 3. The experimental results from angle-resolved photoemission (ARPES), de Haas van Alphen measurements (dHvA), and angular correlation of annihilation radiations (ACAR) are indicated. From Pickett etal. [61]. Figure 8.12 Cross section in the (kx, ky) plane of the calculated Fermi surface in Y 1 2 3. The experimental results from angle-resolved photoemission (ARPES), de Haas van Alphen measurements (dHvA), and angular correlation of annihilation radiations (ACAR) are indicated. From Pickett etal. [61].
Additional information on the material under study can be obtained from the measurement of the e+ -e momentum distribution as mirrored in Doppler broadening of annihilation radiation (DEAR) and the angular correlation of annihilation radiation (ACAR). DEAR can be applied to study the chemical surroundings of free-volume holes [Dlubek et al., 2000a Bamford et al., 2006b], while ACAR is able to measure the anisotropy of the hole shape, as observed for highly crystalline fibers, for example [Jean et al., 1996 Bamford et al., 2001b]. [Pg.460]

Positrons can be used as particle probes, suitable to detect low concentrations of defects in materials. Positron physicists generally are in need of intense positron beams for applying positron annihilation techniques such as two dimensional (2D) Angular Correlation of Annihilation Radiation (ACAR) for investigating surfaces and interfaces of materials. The 2D-ACAR technique allows high resolution measurements of the electron momentum distribution for depth, localized defects, thin layer systems, and interfaces. In addition, a submicrometer size positron beam can be created for defect depth profiling on a lateral scale smaller than a micrometer. Vacancy type defects can be mapped in a three dimensional fashion. [Pg.38]

Position sensitive gamma cameras for 2D angular correlation of annihilation radiation measurements. [Pg.39]

Angular Correlation of Annihilation Radiation (ACAR) Method... [Pg.893]


See other pages where Angular correlation of annihilated radiation is mentioned: [Pg.16]    [Pg.16]    [Pg.463]    [Pg.38]    [Pg.56]    [Pg.241]    [Pg.282]    [Pg.316]    [Pg.468]    [Pg.709]    [Pg.298]    [Pg.244]    [Pg.244]    [Pg.1461]    [Pg.1475]    [Pg.1475]    [Pg.457]    [Pg.879]    [Pg.893]    [Pg.188]   


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