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This simplification does not change the genesis process of the electronic excitations
-
This simplification does not change the genesis process of the electronic excitations.
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29
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4043105401
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Having a finite background charge would lead to the same conclusions we present in this work. It should be noted that small values of the polarization charge have been found in the work reported by, in Ref. 1
-
Having a finite background charge would lead to the same conclusions we present in this work. It should be noted that small values of the polarization charge have been found in the work reported by D. Davidović and M. Tinkham, Phys. Rev. Lett. 83, 1644 (1999) and in Ref. 1.
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The renormalization of the single-electron energy levels combined with the slow relaxation of excited electrons within the nanograin is the source of complexity of the master (Boltzmann) equation. At a given applied bias voltage V, several configurations that belong to different generations carry the current through the nanograin. As the generations form a hierarchy, the rate equations couple different eh-pair subspaces. Furthermore, these couplings would be different depending on the value of V as different single-electron energy levels posses different individual tunneling in and out rates (see Ref. 8 for a model of these quantities)
-
The renormalization of the single-electron energy levels combined with the slow relaxation of excited electrons within the nanograin is the source of complexity of the master (Boltzmann) equation. At a given applied bias voltage V, several configurations that belong to different generations carry the current through the nanograin. As the generations form a hierarchy, the rate equations couple different eh-pair subspaces. Furthermore, these couplings would be different depending on the value of V as different single-electron energy levels posses different individual tunneling in and out rates (see Ref. 8 for a model of these quantities).
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34
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0003462314
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We adopt a Slater-Koster model in which the atomic orbitals on different sites are orthonormal, and consider hopping up to second-nearest neighbors. The Hamiltonian is diagonalized by using a Lanczos algorithm [for an implementation see, Birkhäuser, Boston
-
We adopt a Slater-Koster model in which the atomic orbitals on different sites are orthonormal, and consider hopping up to second-nearest neighbors. The Hamiltonian is diagonalized by using a Lanczos algorithm [for an implementation see J. K. Cullum and R. A. Willoughby, Lanczos Algorithms for Large Symmetric Eigenvalue Computations (Birkhäuser, Boston, 1985)].
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Willoughby, R.A.2
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State-of-the-art molecular dynamics suggest that there is an amorphization on the metal-oxide interface rather than crystalline surface reconstructions—see Ref. 23
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State-of-the-art molecular dynamics suggest that there is an amorphization on the metal-oxide interface rather than crystalline surface reconstructions—see Ref. 23.
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36
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85038974202
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In this model, the geometry can be arbitrary. However, disks and hemispheres are the most widely assumed geometries in the literature. On the other hand, our choice of a fcc lattice host is consistent with the bulk lattices of most of the metals studied experimentally at present
-
In this model, the geometry can be arbitrary. However, disks and hemispheres are the most widely assumed geometries in the literature. On the other hand, our choice of a fcc lattice host is consistent with the bulk lattices of most of the metals studied experimentally at present.
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Sabougni, M.-L.8
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44
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85039007188
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jα) may be implemented the results derived from this simple model should be qualitatively correct
-
jα) may be implemented the results derived from this simple model should be qualitatively correct.
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46
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85039007631
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These numbers correspond to typical parameters for the smallest available nanoparticles (see Refs. 1,2,3,4)
-
These numbers correspond to typical parameters for the smallest available nanoparticles (see Refs. 1,2,3,4).
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-
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47
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85039006936
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F changes a few tens of meV when switching from one disorder realization to another
-
F changes a few tens of meV when switching from one disorder realization to another.
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48
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85039033156
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F
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F.
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49
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85039029385
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F. See Ref. 8 for details
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F. See Ref. 8 for details.
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50
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3543143257
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A. Arbouet, C. Voisin, D. Christofilos, P. Langot, N. Del Fatti, F. Vallée, J. Lermé, G. Celep, E. Cottancin, M. Gaudry, M. Pellarin, M. Broyer, M. Maillard, M.P. Pileni, and M. Treguer, Phys. Rev. Lett. 90, 177401 (2003).
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Celep, G.8
Cottancin, E.9
Gaudry, M.10
Pellarin, M.11
Broyer, M.12
Maillard, M.13
Pileni, M.P.14
Treguer, M.15
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51
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9744236756
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In this paper, the probed grains have typical diameters of about 10 nm which makes it difficult to address the nonequilibrium satellite resonances individually
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M.M. Deshmukh, E. Bonet, A.N. Pasupathy, and D.C. Ralph, Phys. Rev. B 65, 073301 (2002). In this paper, the probed grains have typical diameters of about 10 nm which makes it difficult to address the nonequilibrium satellite resonances individually.
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Deshmukh, M.M.1
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