2007
DOI: 10.1103/physrevb.76.165312
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Pair tunneling and shot noise through a single molecule in a strong electron-phonon coupling regime

Abstract: We investigate the electronic transport through a single molecule in a strong electron-phonon coupling regime. Based on a particle-hole transformation, which is made suitable for a nonequilibrium situation, we treat the pair tunneling and cotunneling on an equal footing. We propose an experimental setup to enhance the visibility of pair tunneling, which has no Franck-Condon suppression. We also discuss the shot noise characteristics.

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Cited by 17 publications
(23 citation statements)
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References 35 publications
(48 reference statements)
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“…For sufficiently strong Holstein coupling, the induced polaronic shift can overcome the Coulomb repulsion, resulting in a bipolaronic attraction between electrons and thus a negative effective charging energy for the QD. This possibility has spurred some theories exploring the manifestation of negative charging energy in transport, which mainly concern the charge Kondo effect [8], pair tunneling [9][10][11], and cotunneling [10]. However, these high-order transport behaviors are fragile, requiring harsh experimental conditions.…”
Section: Introductionmentioning
confidence: 99%
“…For sufficiently strong Holstein coupling, the induced polaronic shift can overcome the Coulomb repulsion, resulting in a bipolaronic attraction between electrons and thus a negative effective charging energy for the QD. This possibility has spurred some theories exploring the manifestation of negative charging energy in transport, which mainly concern the charge Kondo effect [8], pair tunneling [9][10][11], and cotunneling [10]. However, these high-order transport behaviors are fragile, requiring harsh experimental conditions.…”
Section: Introductionmentioning
confidence: 99%
“…This effect is known as the Franck-Condon blockade [12,15,[29][30][31], and arises for the following reason. In a transport situation, the system is voltage-tuned to a point along one of the instability lines, e.g., the 0/2 boundary.…”
Section: Resultsmentioning
confidence: 99%
“…The possibility of vibration-mediated attractive interaction among confined electrons has been discussed, e.g., in the context of amorphous semiconductors [8], vacancies in silicon [9,10], fullerenes [11], and molecular junctions [12][13][14][15]. Figure 1a depicts the simplest model capturing the basic ingredients of the effect: it involves (i) a single vibrational mode (phonon), characterized by a mass m and frequency ω, (ii) a single electronic orbital that can be occupied by one or two electrons, i.e., the occupation number is N ∈ {0, 1, 2}; this orbital is characterized by an on-site energy and a repulsive Coulomb energy U > 0, (iii) the coupling between the phonon and the confined charge, characterized by the force λ encoding the coupling strength, and (iv) a (zero-temperature) electron reservoir, with Fermi energy * Corresponding author: matthias.droth@mail.bme.hu µ = 0, which can supply electrons to the orbital.…”
Section: Introductionmentioning
confidence: 99%
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“…Pair-tunneling.-Single-particle transitions between the reservoir and the wire are excluded for sufficiently low values of temperature and bias Á when U < 0. Two-particle transitions may occur due to higher-order processes in the coupling between the reservoirs and the wire [31,32]: Normal cotunneling results in a weak background conductance for any bias. Pair-tunneling, neglecting the effects of temperature and lifetime broadening, is only allowed for jE 2nþ2 À E 2n j < Á, where E N is the ground state energy of the N-particle state and n is an integer.…”
Section: Fig 2 (Color Onlinementioning
confidence: 99%