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1.
Phys Rev Lett ; 101(18): 186804, 2008 Oct 31.
Article in English | MEDLINE | ID: mdl-18999849

ABSTRACT

A system consisting of two independently contacted quantum dots with a strong electrostatic interaction shows an interdot Coulomb blockade when the dots are weakly tunnel coupled to their leads. How the blockade can be overcome by correlated tunneling when tunnel coupling to the leads increases is studied experimentally. The experimental results are compared with numerical renormalization group calculations using predefined (measured) parameters. Combining our experimental and theoretical results we identify transport through Kondo correlations due to the electrostatic interaction between the two dots.

2.
Phys Rev Lett ; 86(9): 1837-40, 2001 Feb 26.
Article in English | MEDLINE | ID: mdl-11290261

ABSTRACT

Under an external magnetic field, new branches of spin- and charge-density waves have been studied in a quasi-two-dimensional electron system whose ground state has more than one Landau level occupied by electrons. These collective excitations can be treated as manifestations of the multicomponent nature of the electron system in magnetic field, whereas the occupied Landau levels should be associated with degrees of freedom.

3.
Phys Rev Lett ; 84(25): 5824-7, 2000 Jun 19.
Article in English | MEDLINE | ID: mdl-10991064

ABSTRACT

Zero-bias anomalies in the conductance through quantum dots have recently been identified as Kondo resonances and explained in terms of the Anderson impurity model. The effect requires a degeneracy and it has been proposed that this should occur for odd electron numbers on the dot. In this paper we present data, obtained on a split-gate quantum dot with a small number of electrons, which are in disagreement with this expectation. The mapping of the Anderson model on the quantum dot is discussed in terms of an interacting N electron system demonstrating why this expectation can fail.

4.
Phys Rev Lett ; 77(1): 147-150, 1996 Jul 01.
Article in English | MEDLINE | ID: mdl-10061793
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