Download Advances in Electronics and Electron Physics, Vol. 70 by Peter W. Hawkes (Ed.) PDF

By Peter W. Hawkes (Ed.)

ISBN-10: 0120146703

ISBN-13: 9780120146703

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Extra resources for Advances in Electronics and Electron Physics, Vol. 70

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Cpo = h/2e is the magnetic flux quantum. For junctions with dimensions equal to or larger than 1, the phasedifference function depends upon the spatial coordinates of the junction since the magnetic self-field of the tunneling current cannot be neglected any more. - R. P. HUEBENER 20 0 L FIG. 10. Density of the maximum Josephson current J ( y ) of a one-dimensional tunnel junction versus the junction coordinate for the case L = 15 1,. L =Junction length; 1, = Josephson penetration depth. First we consider a one-dimensional geometry, where one dimension, say, the width w of the junction (in x-direction), is still much smaller than A,, whereas the length L of the other dimension (in y-direction) is much larger than I , .

34. Peak value of the voltage signal marking the hotspot boundaries versus the frequency v = u)/2nof the beam modulation. Crosses: experimental values. Solid line: theoretical curve obtained from a theoretical analysis. 5 K. , 1974).

Excellent agreement between experiment and theory. If one applies Eq. , 1984). Of course, in any calculation of the beam-induced thermal response of the specimen only the beam power absorbed in the sample plays any role. Therefore, correction factors may have to be applied due to the emission of secondary and backscattered electrons, photons, etc. So far, in our discussion of the thermal sample response to the electron beam irradiation we have concentrated on purely diffusive heat propagation. This mode of energy transfer dominates if local equilibrium is established within the phonon and electron system and also between both systems by means of sufficient scattering.

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