Superconducting Circuits and Quantum Computation—T. P. Orlando
... Chapter 20. Superconducting Circuits and Quantum Computation Figure 1a shows a SEM image of the persistent current qubit (inner loop) and the measuring dc SQUID (outer) loop. A schematic of the qubit and the measuring circuit is shown in Figure 1b, where the Josephson junctions are denoted by x's. ...
... Chapter 20. Superconducting Circuits and Quantum Computation Figure 1a shows a SEM image of the persistent current qubit (inner loop) and the measuring dc SQUID (outer) loop. A schematic of the qubit and the measuring circuit is shown in Figure 1b, where the Josephson junctions are denoted by x's. ...
Introduction - Princeton University Press
... In most of the existent literature on noninteracting topological insulators, it is implicitly assumed that nontrivial topology implies the presence of gapless edge states in the energy spectrum of a system with boundaries. However, it is well known from the literature on topological phases that such ...
... In most of the existent literature on noninteracting topological insulators, it is implicitly assumed that nontrivial topology implies the presence of gapless edge states in the energy spectrum of a system with boundaries. However, it is well known from the literature on topological phases that such ...
Two-resonator circuit quantum electrodynamics: Dissipative theory
... the qubit-resonator detuning and can have a positive or negative sign. The second one has a definite sign and stems from the fact that qubit and resonators are not pointlike objects but extended circuits. Provided that the qubit always is in a suitable energy eigenstate, the switch is turned off whe ...
... the qubit-resonator detuning and can have a positive or negative sign. The second one has a definite sign and stems from the fact that qubit and resonators are not pointlike objects but extended circuits. Provided that the qubit always is in a suitable energy eigenstate, the switch is turned off whe ...
Nanomechanical shuttle transfer of electrons
... transport properties can be described by a Master equation. We will refer to this situation as classical shuttling of particles. In the case of coherent tunnelling, the electrons should be treated as wave packets while keeping track of the properties of their wave functions. In this situation we wil ...
... transport properties can be described by a Master equation. We will refer to this situation as classical shuttling of particles. In the case of coherent tunnelling, the electrons should be treated as wave packets while keeping track of the properties of their wave functions. In this situation we wil ...
Precisely Timing Dissipative Quantum Information
... how to perform D1WQC by using the timer and initialization gadgets. Before we start, let us emphasize that one does not need to have any coherent unitary control over the quantum system but instead merely makes use of dissipative dynamics exhibiting quantum and classical features. Still, it is the v ...
... how to perform D1WQC by using the timer and initialization gadgets. Before we start, let us emphasize that one does not need to have any coherent unitary control over the quantum system but instead merely makes use of dissipative dynamics exhibiting quantum and classical features. Still, it is the v ...
Topics in Applied Physics Volume 115
... combined with the rich and fertile physics of low-dimensional semiconducting structures and with the possibility to change, for example, carrier density, electric fields or coupling to other quantum systems in a controlled way, an extremely exciting and interesting research field is opened. Most comme ...
... combined with the rich and fertile physics of low-dimensional semiconducting structures and with the possibility to change, for example, carrier density, electric fields or coupling to other quantum systems in a controlled way, an extremely exciting and interesting research field is opened. Most comme ...
Chapter 6 Quantum Computation
... or NO. It is believed (though not proved) that NP 6= co−NP . (For example, we can show that a graph has a Hamiltonian path by exhibiting an example, but we don’t know how to show that it has no Hamiltonian path that way!) Assuming that NP 6= co−NP , there is a theorem that says that no co-NP problem ...
... or NO. It is believed (though not proved) that NP 6= co−NP . (For example, we can show that a graph has a Hamiltonian path by exhibiting an example, but we don’t know how to show that it has no Hamiltonian path that way!) Assuming that NP 6= co−NP , there is a theorem that says that no co-NP problem ...
Mechanical Systems - Rose
... showed phases like those of the moon, indicating that it must orbit the sun rather than the Earth. I’ll only mention a few of his ideas which strongly influenced dynamics. By 1604 he had determined the correct relationship for falling bodies (d ∝ t2) and had stated that bodies of different weights s ...
... showed phases like those of the moon, indicating that it must orbit the sun rather than the Earth. I’ll only mention a few of his ideas which strongly influenced dynamics. By 1604 he had determined the correct relationship for falling bodies (d ∝ t2) and had stated that bodies of different weights s ...
drastically
... The Mollow Absorption Spectrum of a Neutral QD . . . . . . . . . . 37 Band Structure and Energy Level Diagram of The Trion State . . . . 44 Trion Mollow Absorption Spectrum . . . . . . . . . . . . . . . . . . . 46 Signatures of Heavy-light Hole Mixing . . . . . . . . . . . . . . . . . 54 Signature o ...
... The Mollow Absorption Spectrum of a Neutral QD . . . . . . . . . . 37 Band Structure and Energy Level Diagram of The Trion State . . . . 44 Trion Mollow Absorption Spectrum . . . . . . . . . . . . . . . . . . . 46 Signatures of Heavy-light Hole Mixing . . . . . . . . . . . . . . . . . 54 Signature o ...
Ferroelectric and antiferroelectric instabilities in BaTiO3/BaO
... rise to a ferroelectric ground state with a spontaneous polarization of 38 µC/cm2 and a relaxed out-of-plane cell parameter of 4.07 Å. The difference of energy between the ferroelectric ground state and the paraelectric reference is ∆E=16 meV which corresponds to the depth of the double well associa ...
... rise to a ferroelectric ground state with a spontaneous polarization of 38 µC/cm2 and a relaxed out-of-plane cell parameter of 4.07 Å. The difference of energy between the ferroelectric ground state and the paraelectric reference is ∆E=16 meV which corresponds to the depth of the double well associa ...
