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This topic has been discussed in Refs [15, 35], finding only a slow N 1 / 3 growth of the errors due to spontaneous emission.
Similar model has been discussed in Refs. [51, 52], which mainly focus on thermoelectric and electronic transport rather than the band structure and disorder effect studied in this work.
The general effect of incomplete probe synthesis on the hybridization of microarrays has been discussed in refs. [49] and [13].
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The formation mechanism of the rodlike shaped apertures has been discussed in Ref. [22] in detail.
SEM and TEM micrographs of these materials have been discussed in Ref. [14] and are not shown here.
An analytical method based on Truncated Region Eigenfunction Expansion (TREE) has been discussed in Ref. [27], which shows a good accuracy with experimental test data.
It has been discussed in Ref. [38] for a broader class of spin models that alternating behavior is characteristic for systems with open boundary conditions, though typically with a much smaller amplitude than in the case of the Majumdar-Ghosh chain.
A similar effect has already been discussed in Ref. [ 10], where the spectroelectrochemical response of fullerene films in the neutral and reduced form was influenced by solubility in organic solvents.
34 The effects of spin rotation interactions on the spectra of the confined H2 in the solid state have been discussed in ref. 35 where it is shown that the spin rotation interaction would affect only the spectra in levels with E symmetry, resulting in lineshapes with a characteristic concavity at the centre of the spectra.
Further details on the bundles behavior in these two limit cases were discussed in Refs. [19] and [20].
Simple results in this case are discussed in Ref. [39].
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