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Transmission probability

The classical expression for the transmission probability associated with figure A3.11.1(a) or figure A3.11.1 (b) is straightforward, namely... [Pg.958]

Fig. 10. Molecular-transmission probability (a) for circular cylinder (b) having two restricted ends where the soHd line represents fraction transmitted without wall encounter and the dashed line, prediction of this fraction by the formula vs L,/R. (R/Rq) 1, oo 2, 3 3, 2 4, 1.5 5, 1.0. (0) Argon,... Fig. 10. Molecular-transmission probability (a) for circular cylinder (b) having two restricted ends where the soHd line represents fraction transmitted without wall encounter and the dashed line, prediction of this fraction by the formula vs L,/R. (R/Rq) 1, oo 2, 3 3, 2 4, 1.5 5, 1.0. (0) Argon,...
A and A = 0.1 eV. The adiabatic ground potential energy surface is shown in Fig. 11. The present results (solid line) are in good agreement with the quantum mechanical ones (solid circles). The minimum energy crossing point (MECP) is conventionally used as the transition state and the transition probability is represented by the value at this point. This is called the MECP approximation and does not work well, as seen in Fig. 10. This means that the coordinate dependence of the nonadiabatic transmission probability on the seam surface is important and should be taken into account as is done explicitly in Eq. (18). [Pg.114]

Zhu and Nakamura proved that the intriguing phenomenon of complete reflection occurs in the ID NT type potential curve crossing [1, 14]. At certain discrete energies higher than the bottom of the upper adiabatic potential, the particle cannot transmit through the potential from right to left or vice versa. The overall transmission probability P (see Fig. 45) is given by... [Pg.177]

Figure 62. Hydrogen transmission probability as a function of total energy (eV) for the center approach. Taken from Ref [47]. Figure 62. Hydrogen transmission probability as a function of total energy (eV) for the center approach. Taken from Ref [47].
The overall transmission probability from the left to the right or the vice versa is given by... [Pg.203]

In this energy region, physically meaningful quantities are the overall transmission and reflection probabilities. The transmission probability is given by... [Pg.205]

Landauer proposed in 1957 the first mesoscopic theoretical approach to charge transport [176]. Transport is treated as a scattering problem, ignoring initially all inelastic interactions. Phase coherence is assumed to be preserved within the entire conductor. Transport properties, such as the electrical conductance, are intimately related to the transmission probability for an electron to cross the system. Landauer considered the current as a consequence of the injection of electrons at one end of a sample, and the probability of the electrons reaching the other end. The total conductance is determined by the sum of all current-carrying eigenmodes and their transmission probability, which leads to the Landauer formula of a ID system ... [Pg.133]

Fig. 6.2 (a) Bell (parabolic) and Eckart barriers, both widely used in approximate TST calculations of quantum mechanical tunneling, (b) Transmission probability (Bell tunneling) as a function of energy for two values of the reduced barrier width, a... [Pg.191]

The tunnelling correction P is the transmission probability through the potential barrier averaged over all possible crossing points and potential energies . An asymmetrical banier of the Eckart type l is assumed in the present model. [Pg.87]

The approximate calculation of transmission probabilities Vacuum, 28,1978, No. 3, Seite 151... [Pg.188]

In contrast to the discussion above with amorphous barriers, it is possible to use first-principles electron-structure calculations to describe TMR with crystalline tunnel barriers. In the Julliere model the TMR is dependent only on the polarization of the electrodes, and not on the properties of the barrier. In contrast, theoretical work by Butler and coworkers showed that the transmission probability for the tunneling electrons depends on the symmetry of the barrier, which has a dramatic influence on the calculated TMR values [20]. In the case of Fe(100)/Mg0(100)/Fe (100) the majority of electrons in the Fe are spin-up. They are derived from a band of delta-symmetry. In 2004 these theoretical predictions were experimentally confirmed by Parkin et al. and Yusha et al. [21, 22]. Remarkably, by 2005 TMR read heads were introduced into commercial hard disk drives. [Pg.280]

For z > zo, the distorted wavefunction has the same exponential dependence on z as the free wavefunction. Thus, d f dz gains the same factor. The tip wavefunction x gains a similar factor. Therefore, the transmission probability becomes... [Pg.71]

The expressions presented above are restricted since we used the parabolic barrier transmission probabilities. Extension of the theory to temperatures below the crossover temperature may be foimd in Ref 136. More sophisticated quantum rate theories will be discussed in Section V. [Pg.22]

In order to obtain estimates of quantum transport at the molecular scale [105], electronic structure calculations must be plugged into a formalism which would eventually lead to observables such as the linear conductance (equilibrium transport) or the current-voltage characteristics (nonequilibrium transport). The directly measurable transport quantities in mesoscopic (and a fortiori molecular) systems, such as the linear conductance, are characterized by a predominance of quantum effects—e.g., phase coherence and confinement in the measured sample. This was first realized by Landauer [81] for a so-called two-terminal configuration, where the sample is sandwiched between two metalhc electrodes energetically biased to have a measurable current. Landauer s great intuition was to relate the conductance to an elastic scattering problem and thus to quantum transmission probabilities. [Pg.206]

Fig. 20 Schematic representation of a two-terminal device. The scattering region (enclosed in the dashed-line frame) with transmission probability T(E) is connected to semi-infinite left (L) and right (R) leads which end in electronic reservoirs (not shown) at chemical potentials Eu and r, kept fixed at the same value p for linear transport. By applying a small potential difference electronic transport will occur. The scattering region or molecule may include in general parts of the leads (shaded areas) (adapted from [105] with permission Copyright 2002 by Springer)... Fig. 20 Schematic representation of a two-terminal device. The scattering region (enclosed in the dashed-line frame) with transmission probability T(E) is connected to semi-infinite left (L) and right (R) leads which end in electronic reservoirs (not shown) at chemical potentials Eu and r, kept fixed at the same value p for linear transport. By applying a small potential difference electronic transport will occur. The scattering region or molecule may include in general parts of the leads (shaded areas) (adapted from [105] with permission Copyright 2002 by Springer)...
As a first test [22] of the semiclassical approach described above we have computed the transmission probability through the lie kart potential barrier,... [Pg.865]


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