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This implies that any electron interference effects will be to some degree affected by the presence of such fields.
In this study we examine the distortion effects of external (constant and variable) magnetic fields on electron interference and holography.
We note that the amplitude of Iemission translates to only ~0.08 electrons emitted per optical pulse in average, which suggests that Coulomb repulsion and electron interference effects are negligible during the photoemission process6,7,16.
From the temperature and magnetic field dependence, we infer the oscillations are mesoscopic Coulomb blockade, a type of Coulomb blockade caused by electron interference in an otherwise open system.
The emergence of these fluctuations of conductance at low temperatures confirms the existence of electron interference [17].
The T−1/2 dependence of L ϕ is a typical characteristic of two-dimensional electron interference [18], and it gives evidence of the electrical transport through topological surface states existing in the 10-nm Bi2Te3 ultrathin film.
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Then in such a case, the Coulomb-induced level contributes little to the quantum interference, and a single-electron interference picture remains.
In the AlGaAs/GaAs device, electron wave interference has been detected in all possible four-terminal measurement configuration at a temperature as high as T= 1.5K.
This emerges as the creation of nonbonding edge state localized in the zigzag-shaped edges and electron wave interference in the armchair-shaped ones.
We fabricated zigzag-edged and armchair-edged graphene nanoribbons, and investigated the Raman G-band and STM superlattice which are governed by the electron wave interference at the armchair edges.
The performance of the method is evaluated for the design of an asymmetric Fabry Perot electron-wave interference filter (laser structure) and a dual-band quantum well infrared photodetector (QWIP).
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