By Peter W. Hawkes (Eds.)
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 positive factors prolonged articles at the physics of electron units (especially semiconductor devices), particle optics at low and high energies, microlithography, photo technology and electronic photo processing, electromagnetic wave propagation, electron microscopy, and the computing equipment utilized in a lot of these domains.
* Contributions from prime overseas students and specialists
* Discusses sizzling subject parts and provides present and destiny examine tendencies
* important reference and consultant for physicists, engineers and mathematicians
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Additional resources for Imaging and Electron Physics
CIRCULAR (ANGULAR) CONVOLUTION For two functions f (r) = f (r, θ ) and g (r) = g(r, θ ), the notion of a circular or angular convolution can be defined. This is not the 2D convolution as previously discussed but rather a convolution over the angular variable only, so that it may be defined as 1 f (r) ∗θ g(r) = 2π 2π f (r, θ0 ) g(r, θ − θ0 ) dθ0 . (131) 0 Note the notation ∗θ is used to denote the angular convolution. A Fourier relationship can be defined for this operation of angular convolution: 1 h(r, θ ) = f (r) ∗θ g(r) = 2π 2π fn (r) e n=−∞ ∞ fn (r)gm (r) ejmθ = ∞ jnθ0 0 ∞ ∞ n=−∞ m=−∞ 1 2π gm (r) ejm(θ −θ0 ) dθ0 m=−∞ 2π ejnθ0 e−jmθ0 dθ0 .
47 48 Neil V. Budko of space-time and was used to fix the standard of length definitively (Giacomo, 1984). The realization that nothing can travel faster than light was as profound as the deduction of the impossibility of perpetual motion from the second law of thermodynamics. Often, however, measurements or simulations are reported that seem to demonstrate velocities greater (or smaller) than what is expected from light. It has long been known that the notion of velocity becomes dubious when a wave propagates in a medium with strong anomalous dispersion (see Landau and Lifshitz, 1963).
Green’s Function Coefficients The Green’s function is defined as the solution to the Helmholtz equation for a delta function source at r = r0 for real or complex k: ∇ 2 g r, r0 , ω + k2 g r, r0 , ω = −δ r − r0 , (162) where we use g r, r0 , ω to denote the Green’s function. Taking the 2D Fourier transform of Eq. (162) gives −ρ 2 + k2 G ω, r0 , ω = −e−iω·r0 . (163) For r0 = 0, the definition of G in Eq. (163) is the same as that in Eq. (160). We convert to the polar-coordinate form so that the complex exponential is given by Eq.
Imaging and Electron Physics by Peter W. Hawkes (Eds.)