neeman.pdf
... total-parity and thus fits in the role of a superconnection – a connection-like role for a locally-gauged supergroup. This was the kernel of a mathematical construct devised by D. Quillen [20]. With S. Sternberg [21], we dressed up the 1979 model in Quillen’s formulation, which was mathematically wel ...
... total-parity and thus fits in the role of a superconnection – a connection-like role for a locally-gauged supergroup. This was the kernel of a mathematical construct devised by D. Quillen [20]. With S. Sternberg [21], we dressed up the 1979 model in Quillen’s formulation, which was mathematically wel ...
The basis of discontinuous motion
... other, and then passes through the two slits to arrive at the screen. In this way, when a large number of particles reach the screen, they form the double-slit interference pattern. Now we will demonstrate that this experiment clearly reveals that the motion of particle is discontinuous. If the moti ...
... other, and then passes through the two slits to arrive at the screen. In this way, when a large number of particles reach the screen, they form the double-slit interference pattern. Now we will demonstrate that this experiment clearly reveals that the motion of particle is discontinuous. If the moti ...
Quantum Correlations in Information Theory
... quantum entanglement, i.e. peculiar correlations described by quantum laws which are shared, for example, between the sender and the receiver of a message. However, it has been recently shown that entanglement is not the most general form of quantum correlations. Even unentangled states of compound ...
... quantum entanglement, i.e. peculiar correlations described by quantum laws which are shared, for example, between the sender and the receiver of a message. However, it has been recently shown that entanglement is not the most general form of quantum correlations. Even unentangled states of compound ...
course syllabus
... PEK_W01 identify and describe mathematically the classical concept of mechanical waves and basics of acoustics, including a description of standing waves, the Doppler effect, and interference PEK_W02 explain the basis for human hearing mechanism and the scope audibility PEK_W03 identify and describe ...
... PEK_W01 identify and describe mathematically the classical concept of mechanical waves and basics of acoustics, including a description of standing waves, the Doppler effect, and interference PEK_W02 explain the basis for human hearing mechanism and the scope audibility PEK_W03 identify and describe ...
Non-abelian quantum Hall states and fractional charges in one dimension Emma Wikberg
... mapping the two-dimensional system onto a thin torus, where the problem becomes effectively one-dimensional and hopping is suppressed, meaning that the classical electrostatic interaction dominates. The approach assists with a simplified view of ground states and their degeneracies, as well as of th ...
... mapping the two-dimensional system onto a thin torus, where the problem becomes effectively one-dimensional and hopping is suppressed, meaning that the classical electrostatic interaction dominates. The approach assists with a simplified view of ground states and their degeneracies, as well as of th ...
Non-abelian quantum Hall states and fractional charges in
... mapping the two-dimensional system onto a thin torus, where the problem becomes effectively one-dimensional and hopping is suppressed, meaning that the classical electrostatic interaction dominates. The approach assists with a simplified view of ground states and their degeneracies, as well as of th ...
... mapping the two-dimensional system onto a thin torus, where the problem becomes effectively one-dimensional and hopping is suppressed, meaning that the classical electrostatic interaction dominates. The approach assists with a simplified view of ground states and their degeneracies, as well as of th ...
Information theoretic treatment of tripartite systems and quantum
... In this paper we generalize the notion of a type of quantum information so that it includes not only a projective decomposition of the identity, a set of projectors that sum to the identity, but also a general POVM, a collection of positive operators that sum to the identity. The idea, discussed in ...
... In this paper we generalize the notion of a type of quantum information so that it includes not only a projective decomposition of the identity, a set of projectors that sum to the identity, but also a general POVM, a collection of positive operators that sum to the identity. The idea, discussed in ...
353, 216 (2006) .
... in φ-representation. We then imagine that the overlap of the two states governed by slightly different (perturbed and unperturbed) Hamiltonians may decay fast with time. It means that the dynamical instability regime of the classical system usually corresponds to the low fidelity regime of the quant ...
... in φ-representation. We then imagine that the overlap of the two states governed by slightly different (perturbed and unperturbed) Hamiltonians may decay fast with time. It means that the dynamical instability regime of the classical system usually corresponds to the low fidelity regime of the quant ...
Discrete Symmetries
... • Time reversal symmetry, as you might guess, reverses the time component: T (t, x) = T (−t, x) ...
... • Time reversal symmetry, as you might guess, reverses the time component: T (t, x) = T (−t, x) ...
Coherent manipulations of charge-number states in a Cooper-pair box Y. Nakamura,
... and we obtain a single Bloch band in the phase space (Fig. 1(c)). This means that there is still a single available state within the superconducting gap. On the other hand, if we reduce the size of the junction, the charging energy due to the excess Cooper-pair charge becomes dominant, and the degen ...
... and we obtain a single Bloch band in the phase space (Fig. 1(c)). This means that there is still a single available state within the superconducting gap. On the other hand, if we reduce the size of the junction, the charging energy due to the excess Cooper-pair charge becomes dominant, and the degen ...
Quantization of bi-Hamiltonian systems J.
... From the viewpoint of quantum mechanics, the existence of more than one Hamiltonian structure for a given classical mechanical system raises the possibility of there existing more than one quantized version of this system, even at the level of quantization considered in Ref. 1. The resulting ambigui ...
... From the viewpoint of quantum mechanics, the existence of more than one Hamiltonian structure for a given classical mechanical system raises the possibility of there existing more than one quantized version of this system, even at the level of quantization considered in Ref. 1. The resulting ambigui ...
achieving 128-bit security against quantum attacks in openvpn
... (which is always possible because NAND is functionally complete), and then converting this circuit to a quantum circuit built from Toffoli gates, as described in [11]. For example, f can be implemented as a function that returns 0 if and only if the input is an AES-key for a certain plaintextciphert ...
... (which is always possible because NAND is functionally complete), and then converting this circuit to a quantum circuit built from Toffoli gates, as described in [11]. For example, f can be implemented as a function that returns 0 if and only if the input is an AES-key for a certain plaintextciphert ...
Quantum groups and integrable lattice models UMN Math Physics Seminar
... Consider an (N + 1)-fold tensor product V0 ⊗ V1 ⊗ · · · ⊗ VN (Vi = V ) and let Rij be the operator acting on the Vi ⊗ Vj component of this product as R and as identity on any other Vl . R0N . . . R02 R01 : V0 ⊗ (V1 ⊗ · · · ⊗ VN ) → V0 ⊗ (V1 ⊗ · · · ⊗ VN ) ...
... Consider an (N + 1)-fold tensor product V0 ⊗ V1 ⊗ · · · ⊗ VN (Vi = V ) and let Rij be the operator acting on the Vi ⊗ Vj component of this product as R and as identity on any other Vl . R0N . . . R02 R01 : V0 ⊗ (V1 ⊗ · · · ⊗ VN ) → V0 ⊗ (V1 ⊗ · · · ⊗ VN ) ...