Kurt Symanzik—a stable fixed point beyond triviality
... Nobel Prize in Physics honouring the contribution of Gross, Politzer and Wilczek (obviously performed under the strong influence of, e.g., Coleman, and in the presence of complementary or foregoing related research work by scientists like, e.g., ’t Hooft and Symanzik) ‘. . . for the discovery of asy ...
... Nobel Prize in Physics honouring the contribution of Gross, Politzer and Wilczek (obviously performed under the strong influence of, e.g., Coleman, and in the presence of complementary or foregoing related research work by scientists like, e.g., ’t Hooft and Symanzik) ‘. . . for the discovery of asy ...
The Threshold for Fault-Tolerant Quantum Computation
... Gottesman, Preskill, quant-ph/0504218; also Reichardt, quant-ph/0509203), assuming all desiderata. Best methods trade extra ancilla qubits for error rate: Ancilla factories create complex ancilla states to substitute for most gates on the data. Errors on ancillas are less serious, since bad ancillas ...
... Gottesman, Preskill, quant-ph/0504218; also Reichardt, quant-ph/0509203), assuming all desiderata. Best methods trade extra ancilla qubits for error rate: Ancilla factories create complex ancilla states to substitute for most gates on the data. Errors on ancillas are less serious, since bad ancillas ...
Demonstration of a Stable Atom-Photon Entanglement Source for
... netic sublevels and efficiency of frequency mixing limits the further application. Another kind of atom-photon entanglement is realized using the orbital angular momentum (OAM) states [19], which could also extend to highdimensional entanglement. However, the divergence property of different OAM mod ...
... netic sublevels and efficiency of frequency mixing limits the further application. Another kind of atom-photon entanglement is realized using the orbital angular momentum (OAM) states [19], which could also extend to highdimensional entanglement. However, the divergence property of different OAM mod ...
Edge-mode superconductivity in a two
... paths enclose half the junction area. Alternatively, one could consider interference around the full junction area by particles of charge e instead of Cooper pairs with charge 2e. The occurrence of e-interference is rare because supercurrent probes the coherence between superconductors by exchange o ...
... paths enclose half the junction area. Alternatively, one could consider interference around the full junction area by particles of charge e instead of Cooper pairs with charge 2e. The occurrence of e-interference is rare because supercurrent probes the coherence between superconductors by exchange o ...
11 Selection Postulates and Probability Rules in the Problem of
... some single pure state from a complete set of orthogonal states of the measured system - it is selection part of the projection postulate. Second, it predicts the probabilities to find these outcomes - this is probabilistic part of the projection postulate (Born's rule for probabilities). We will se ...
... some single pure state from a complete set of orthogonal states of the measured system - it is selection part of the projection postulate. Second, it predicts the probabilities to find these outcomes - this is probabilistic part of the projection postulate (Born's rule for probabilities). We will se ...
Phys. Chem. Chem. Phys. 14, 9411-20
... known, to date, it is still a technical challenge to generate and manipulate many qubits in any quantum structure. So far, the two experimental realizations of static molecular modeling have been performed via an improved version of the PEA.22,29 Essentially, by iterating the PEA process and modifyi ...
... known, to date, it is still a technical challenge to generate and manipulate many qubits in any quantum structure. So far, the two experimental realizations of static molecular modeling have been performed via an improved version of the PEA.22,29 Essentially, by iterating the PEA process and modifyi ...
Fidelity as a figure of merit in quantum error correction
... When more than e errors occur for a coded qubit, the ensuing state either fall into a space orthogonal to the code space, or overlap it. If such an erroneous state belongs to the orthogonal space, it can be identified but not corrected. There are then two conceivable strategies: One is to apply some ...
... When more than e errors occur for a coded qubit, the ensuing state either fall into a space orthogonal to the code space, or overlap it. If such an erroneous state belongs to the orthogonal space, it can be identified but not corrected. There are then two conceivable strategies: One is to apply some ...