By Peter W. Hawkes
Advances in Imaging and Electron Physics merges long-running serials--Advances in Electronics and Electron Physics and Advances in Optical and Electron Microscopy. This sequence gains prolonged articles at the physics of electron units (especially semiconductor devices), particle optics at low and high energies, microlithography, picture technological know-how and electronic picture processing, electromagnetic wave propagation, electron microscopy, and the computing equipment utilized in a lot of these domain names. up-to-date with contributions from top foreign students and specialists Discusses sizzling subject components and provides present and destiny study developments offers a useful reference and advisor for physicists, engineers and mathematicians
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Extra resources for Advances in Imaging and Electron Physics
Applied Physics B, 53, 221–225. , & Fischer, J. (1990). Surface-plasmon-enhanced multiphoton photoelectric emission from thin silver films. Optics Letters, 15, 866–868. , & Fischer, J. (1991). Surface-plasmon field-enhanced multiphoton photoelectric emission from metal films. Physical Review B, 43, 8870–8878. , & Farkas, G. (2008). Attosecond electron pulses from interference of above-threshold Varro, de Broglie waves. Laser and Particle Beams, 26, 9–20. ¨ Yakovlev, V. , Udem,, et al. (2003). Phasestabilized 4-fs pulses at the full oscillator repetition rate for a photoemission experiment.
In our case, however, by having taken tunneling emission into account (instead of multiphoton emission) the influence of the CE phase becomes more pronounced. The number of structures observable on the emission maps corresponds to the number of optical cycles in the laser pulse (two in this case). 75π and π/4 serving as a basis for an ideal photoelectron source. Therefore, it is anticipated that the generation of electron beams with the desired spatial, spectral, and temporal features requires femtosecond laser sources with CE phase stabilization.
The higherorder autocorrelation traces revealed in each case that the electron pulse length is roughly n 1/2 times shorter than that of the exciting laser pulse, where n is the order of the photoemission process (n = 2, . . , 4 in these experiments). Therefore, the temporal profile of the electron bunch can be well approximated with Eq. (3). , 2004) where pulses of 27-fs duration were used. For example, the third-order interferometric autocorrelation trace measured with three-photon-induced, SPP-enhanced photoemission in the latter case is depicted in Figure 11.
Advances in Imaging and Electron Physics by Peter W. Hawkes