Braid Topologies for Quantum Computation
... found which approximate any even number, 2m, of windings of the static quasiparticles. Figure 3(b) shows a twoqubit braid in which the pattern from Fig. 3(a) is used to weave the control pair through the target qubit. If the control qubit is in the state |0L i this weave does nothing, but if it is i ...
... found which approximate any even number, 2m, of windings of the static quasiparticles. Figure 3(b) shows a twoqubit braid in which the pattern from Fig. 3(a) is used to weave the control pair through the target qubit. If the control qubit is in the state |0L i this weave does nothing, but if it is i ...
functions and (so-called px- and py-orbitals) are linear combinations
... quantum mechanics. As a result, the “real” and “imaginary” terms of the Ψ function are regarded in QM erroneously as qualitatively similar. Accordingly, the complicated orbitals built on the basis of mixture of the “real” and “imaginary” components (i.e., mathematical mixture of physically immiscibl ...
... quantum mechanics. As a result, the “real” and “imaginary” terms of the Ψ function are regarded in QM erroneously as qualitatively similar. Accordingly, the complicated orbitals built on the basis of mixture of the “real” and “imaginary” components (i.e., mathematical mixture of physically immiscibl ...
Experimental one-way quantum computing
... Standard quantum computation is based on sequences of unitary quantum logic gates that process qubits. The one-way quantum computer proposed by Raussendorf and Briegel is entirely different. It has changed our understanding of the requirements for quantum computation and more generally how we think ...
... Standard quantum computation is based on sequences of unitary quantum logic gates that process qubits. The one-way quantum computer proposed by Raussendorf and Briegel is entirely different. It has changed our understanding of the requirements for quantum computation and more generally how we think ...
Newton`s cradle analogue with Bose
... The system and its dynamics are introduced in Section 2; in Section 3 we consider two antithetical cases: the simplest uniform lattice, with an unluckily poor dynamics, and the perfectly transmitting lattice, with individually constructed couplings. Note that in both these cases the net number-of-at ...
... The system and its dynamics are introduced in Section 2; in Section 3 we consider two antithetical cases: the simplest uniform lattice, with an unluckily poor dynamics, and the perfectly transmitting lattice, with individually constructed couplings. Note that in both these cases the net number-of-at ...
referring
... quantum mechanics courses, in contrast, for example, to Einstein’s approach in the teaching of relativity. Indeed Heisenberg’s paper is widely regarded as being difficult to understand and of mainly historical interest today. For example, Weinberg7 has written that ‘‘If the reader is mystified at wh ...
... quantum mechanics courses, in contrast, for example, to Einstein’s approach in the teaching of relativity. Indeed Heisenberg’s paper is widely regarded as being difficult to understand and of mainly historical interest today. For example, Weinberg7 has written that ‘‘If the reader is mystified at wh ...
Randomness in (Quantum) Information Processing
... The second approach tries to fix problems where no solution exists even for high-quality weak random sources. The central idea is to design efficient procedures to post-process the output of weak sources to obtain (almost) unbiased uncorrelated bits, usually at the cost that such a post-processing, ...
... The second approach tries to fix problems where no solution exists even for high-quality weak random sources. The central idea is to design efficient procedures to post-process the output of weak sources to obtain (almost) unbiased uncorrelated bits, usually at the cost that such a post-processing, ...
(Total Four Semesters, 100 marks in each Paper followed by
... Curvilinear Coordinates and various operators in circular, cylindrical and spherical coordinate systems, classification of Tensors, Rank of a Tensor, covariant and contra-variant tensors, symmetric and anti-symmetric Tensors, Kronecker delta symbol. Contraction of Tensor, metric Tensor and Tensor de ...
... Curvilinear Coordinates and various operators in circular, cylindrical and spherical coordinate systems, classification of Tensors, Rank of a Tensor, covariant and contra-variant tensors, symmetric and anti-symmetric Tensors, Kronecker delta symbol. Contraction of Tensor, metric Tensor and Tensor de ...
Kondo Effect in Quantum Dots
... Figure 8: Conductance versus temperature (Data taken from: Sara M. Cronenwett, T. Oosterkamp, L.Kouwenhoven: ”A Tunable Kondo effect in Quantum Dots”, Science vol 281, 540 (1998)) ...
... Figure 8: Conductance versus temperature (Data taken from: Sara M. Cronenwett, T. Oosterkamp, L.Kouwenhoven: ”A Tunable Kondo effect in Quantum Dots”, Science vol 281, 540 (1998)) ...
Dynamical quantum-electrodynamics embedding: Combining time
... nanostructure systems,24–28 revealing the importance of quantum effect at sub-nanometer contacting regime. However, due to numerical constraints, only nanostructures involving hundreds of atoms have been computationally studied, sizes beyond ∼2 nm are not accessible by fully quantum methods. To brid ...
... nanostructure systems,24–28 revealing the importance of quantum effect at sub-nanometer contacting regime. However, due to numerical constraints, only nanostructures involving hundreds of atoms have been computationally studied, sizes beyond ∼2 nm are not accessible by fully quantum methods. To brid ...
Momentum Maps, Dual Pairs and Reduction in
... If J is a momentum map for a weakly hamiltonian action ψ, then J([v, w]) and {J(v), J(w)} are both hamiltonians corresponding to the vector field [v, w]M . Thus, since we are assuming M connected, we have c(v, w) = J([v, w]) − {J(v), J(w)} ∈ R. Note that c defines a skew-symmetric bilinear form on g ...
... If J is a momentum map for a weakly hamiltonian action ψ, then J([v, w]) and {J(v), J(w)} are both hamiltonians corresponding to the vector field [v, w]M . Thus, since we are assuming M connected, we have c(v, w) = J([v, w]) − {J(v), J(w)} ∈ R. Note that c defines a skew-symmetric bilinear form on g ...