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The electromagnetic environment plays a crucial role in the observation of
charging effects. For instance in a single tunnel junction a
high impedance
environment is mandatory in order for
current oscillations to appear
[8] [23] [31] [42]. In the case
of a high impedance environment
tunnel rates have to be calculated according to the
local rule [53],
where only the junction through which the electron tunnels is considered for
the calculation of the Coulomb energy. The high impedance kind of shields the rest of the
environment from the junction. It is difficult to provide a high impedance
environment for a single junction, because
stray capacitances which are
usually much bigger than the capacitance of the junction itself, cause the
junction to be voltage biased. Thus the saw-tooth voltage across the
junction, which is produced by a current bias, is absent. G. Ingold et al.
[54]
studied the effect of the electromagnetic environment on a SET transistor.
They found that for the low impedance
environment the global rule which
considers the change in free energy of the whole circuit,
(2.11) and (2.23), applies. For a high
impedance environment stray capacitances lead to a modification of the local
rule. For multijunction
circuits the effective environmental impedance decreases roughly as one over
the square of the number of junctions [46]. As a consequence,
tunnel junctions in
large arrays see only a very low impedance environment and the tunnel
rates may be calculated using the global rule.
Next: 2.7 The Double Tunnel
Up: 2 Theory of Single
Previous: 2.5 Minimum Tunnel Resistance
Christoph Wasshuber