Hirota dynamics of quantum integrability
... • No single analyticity friendly gauge for T’s of right, left and upper bands. We parameterize T’s of 3 bands in different, analyticity friendly gauges, also respecting their reality and certain symmetries. • Quantum analogue of classical ...
... • No single analyticity friendly gauge for T’s of right, left and upper bands. We parameterize T’s of 3 bands in different, analyticity friendly gauges, also respecting their reality and certain symmetries. • Quantum analogue of classical ...
NP-complete Problems and Physical Reality
... My immediate reaction was that the paper was a parody. However, a visit to Bringsjord’s home page2 suggested that it was not. Impelled, perhaps, by the same sort of curiosity that causes people to watch reality TV shows, I checked the discussion of this paper on the comp.theory newsgroup to see if ...
... My immediate reaction was that the paper was a parody. However, a visit to Bringsjord’s home page2 suggested that it was not. Impelled, perhaps, by the same sort of curiosity that causes people to watch reality TV shows, I checked the discussion of this paper on the comp.theory newsgroup to see if ...
Quantum numbers for relative ground states of antiferromagnetic
... numbers N of spin sites and spin quantum numbers s where the interaction is given by antiferromagnetic nearest neighbor exchange7–12 . One quantity of interest is the shift quantum number k = 0, . . . N − 1 associated with the cyclic shift symmetry of the rings. The corresponing crystal momentum is ...
... numbers N of spin sites and spin quantum numbers s where the interaction is given by antiferromagnetic nearest neighbor exchange7–12 . One quantity of interest is the shift quantum number k = 0, . . . N − 1 associated with the cyclic shift symmetry of the rings. The corresponing crystal momentum is ...
Operator Imprecision and Scaling of Shor’s Algorithm
... performance of the algorithm in such a way that the polynomial complexity of the algorithm no longer describes the scaling behavior of the algorithm’s execution time. It is possible to show that, in the presence of operator precision errors, Shor’s algorithm is no more efficient than classical algo ...
... performance of the algorithm in such a way that the polynomial complexity of the algorithm no longer describes the scaling behavior of the algorithm’s execution time. It is possible to show that, in the presence of operator precision errors, Shor’s algorithm is no more efficient than classical algo ...
Quantum Theory of Particles and Fields
... 【5】 Y.L.Ma and Y.L.Wu, “Anomaly and anomaly-free treatment of QFTs based on symmetry-preserving loop regularization” Int. J. Mod. Phys. A 21, 6383 (2006) [arXiv:hepph/0509083]. 【6】Y.L.Ma and Y.L.Wu, “On the radiatively induced Lorentz and CPT violating ChernSimons term” Phys. Lett. B 647, 427 (2007) ...
... 【5】 Y.L.Ma and Y.L.Wu, “Anomaly and anomaly-free treatment of QFTs based on symmetry-preserving loop regularization” Int. J. Mod. Phys. A 21, 6383 (2006) [arXiv:hepph/0509083]. 【6】Y.L.Ma and Y.L.Wu, “On the radiatively induced Lorentz and CPT violating ChernSimons term” Phys. Lett. B 647, 427 (2007) ...
Heralded atomic-ensemble quantum memory for photon polarization states
... The heralded storage occurs rarely ( p ∼ 10−6 per incident photon in our non-optimized set-up), but when it does, the incident photon is stored and can later be recreated with good efficiency (ε ∼ 50%) and sub-Poissonian statistics (g2 ≈ 0.24), while its polarization state is restored with very high ...
... The heralded storage occurs rarely ( p ∼ 10−6 per incident photon in our non-optimized set-up), but when it does, the incident photon is stored and can later be recreated with good efficiency (ε ∼ 50%) and sub-Poissonian statistics (g2 ≈ 0.24), while its polarization state is restored with very high ...
5 Discrete Symmetries
... exists an ambiguity in defining the phases of transformed states. Take for example a state of electric charge |qi also assumed to have good parity, P |qi = η |qi . If now the parity operator is redefined as P 0 ≡ P exp(iαQ), where α is some real constant and Q the charge operator, then the parity of ...
... exists an ambiguity in defining the phases of transformed states. Take for example a state of electric charge |qi also assumed to have good parity, P |qi = η |qi . If now the parity operator is redefined as P 0 ≡ P exp(iαQ), where α is some real constant and Q the charge operator, then the parity of ...
Earth-Moon Lagrangian points as a testbed for general relativity and
... to establish the most accurate classical counterpart of the putative quantum framework that we have set up. By taking seriously into account the important role played by the Einstein theory within this scheme, in the last part of this paper we describe a new quantum corrected regime where the underl ...
... to establish the most accurate classical counterpart of the putative quantum framework that we have set up. By taking seriously into account the important role played by the Einstein theory within this scheme, in the last part of this paper we describe a new quantum corrected regime where the underl ...