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University of Central Florida

2010

Faculty Bibliography 2010s

Physics

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Poly(3-Hexylthiophene) Crystalline Nanoribbon Network For Organic Field Effect Transistors (Vol 96, 243304, 2010), M. Arif, Jianhua Liu, Lei Zhai, Saiful I. Khondaker Jan 2010

Poly(3-Hexylthiophene) Crystalline Nanoribbon Network For Organic Field Effect Transistors (Vol 96, 243304, 2010), M. Arif, Jianhua Liu, Lei Zhai, Saiful I. Khondaker

Faculty Bibliography 2010s

No abstract provided.


Epitaxial Growth Of A Silicene Sheet, Boubekeur Lalmi, Hamid Oughaddou, Hanna Enriquez, Abdelkader Kara, Sébastien Vizzini, Bénidicte Ealet, Bernard Aufray Jan 2010

Epitaxial Growth Of A Silicene Sheet, Boubekeur Lalmi, Hamid Oughaddou, Hanna Enriquez, Abdelkader Kara, Sébastien Vizzini, Bénidicte Ealet, Bernard Aufray

Faculty Bibliography 2010s

Using atomic resolved scanning tunneling microscopy, we present here the experimental evidence of a silicene sheet (graphenelike structure) epitaxially grown on a close-packed silver surface [Ag(111)]. This has been achieved via direct condensation of a silicon atomic flux onto the single-crystal substrate in ultrahigh vacuum conditions. A highly ordered silicon structure, arranged within a honeycomb lattice, is synthesized and present two silicon sublattices occupying positions at different heights (0.02 nm) indicating possible sp(2)-sp(3) hybridizations.


Dynamics Of Entanglement Between A Quantum Dot Spin Qubit And A Photon Qubit Inside A Semiconductor High-Q Nanocavity, Hubert Pascal Seigneur, Gabriel Gonzalez, Michael Niklaus Leuenberger, Winston Vaughan Schoenfeld Jan 2010

Dynamics Of Entanglement Between A Quantum Dot Spin Qubit And A Photon Qubit Inside A Semiconductor High-Q Nanocavity, Hubert Pascal Seigneur, Gabriel Gonzalez, Michael Niklaus Leuenberger, Winston Vaughan Schoenfeld

Faculty Bibliography 2010s

We investigate in this paper the dynamics of entanglement between a QD spin qubit and a single photon qubit inside a quantum network node, as well as its robustness against various decoherence processes. First, the entanglement dynamics is considered without decoherence. In the small detuning regime (Delta = 78 mu eV), there are three different conditions for maximum entanglement, which occur after 71, 93, and 116 picoseconds of interaction time. In the large detuning regime (Delta = 1.5 meV), there is only one peak for maximum entanglement occurring at 625 picoseconds. Second, the entanglement dynamics is considered with decoherence by …