2007 APS March Meeting
Volume 52, Number 1
Monday–Friday, March 5–9, 2007;
Denver, Colorado
Session X44: Focus Session: Nanoscale Transport - Molecules III
8:00 AM–11:00 AM,
Friday, March 9, 2007
Colorado Convention Center
Room: 507
Sponsoring
Unit:
DMP
Chair: Mark Hybertsen, Brookhaven National Laboratory
Abstract ID: BAPS.2007.MAR.X44.4
Abstract: X44.00004 : Pair Tunneling through Single Molecules
8:36 AM–9:12 AM
Preview Abstract
Abstract
Author:
Mikhail Raikh
(University of Utah)
Coupling to molecular vibrations induces a polaronic shift, and
can lead to a negative charging energy, U. For negative U, the
occupation of the ground state of the molecule is even. In this
situation, virtual pair transitions between the molecule and the
leads can dominate electron transport. At low temperature, T,
these transitions give rise to the charge-Kondo effect [1]. We
developed the electron transport theory through the negative-U
molecule [2] at relatively high T, when the Kondo correlations
are suppressed. Two physical ingredients distinguish our theory
from the transport through a superconducting grain coupled to
the normal leads [3]: (i) in parallel with sequential
pair-tunneling processes, single-particle cotunneling processes
take place; (ii) the electron pair on the molecule can be created
(or annihilated) by two electrons tunneling in from (or out to)
opposite leads. We found that, even within the rate-equation
description, the behavior of differential conductance through the
negative-U molecule as function of the gate voltage is quite
peculiar: the height of the peak near the degeneracy point is
independent of temperature, while its width is proportional to T.
This is in contrast to the ordinary Coulomb-blockade conductance
peak, whose integral strength is T-independent. At finite
source-drain bias, V$>>$T, the width of the conductance peak is
$\sim$V,
whereas the conventional Coulomb-blockade peak at finite V splits
into two sharp peaks at detunings V/2, and -V/2. Possible
applications to the gate-controlled current rectification and
switching will be discussed.
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[1] A. Taraphder and P. Coleman, Phys. Rev. Lett. 66, 2814 (1991).
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[2] J. Koch, M. E. Raikh, and F. von Oppen,
Phys. Rev. Lett. 96, 056803 (2006).
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[3] F. W. J. Hekking, L. I. Glazman, K. A. Matveev, and R. I.
Shekhter, Phys. Rev. Lett. 70, 4138 (1993).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2007.MAR.X44.4