Multi-particle qubits - Department of Physics — ETH Zurich
... One can divide the non-linear computational mappings into three main categories: Projection on a two-level system (see Section 3.1.1), partial projection (see Section 3.1.2), and no projection at all (see Section 3.1.3). Projection on a two-level system is the most commonly used qubit encoding schem ...
... One can divide the non-linear computational mappings into three main categories: Projection on a two-level system (see Section 3.1.1), partial projection (see Section 3.1.2), and no projection at all (see Section 3.1.3). Projection on a two-level system is the most commonly used qubit encoding schem ...
Quantum Operator Design for Lattice Baryon Spectroscopy
... accurately extracting the lowest seven or eight energy levels in each symmetry channel. A procedure in which the diagonal elements of the correlation matrix of the operators are first evaluated to remove noisy operators, followed by the selection of sixteen operators whose renormalized correlation m ...
... accurately extracting the lowest seven or eight energy levels in each symmetry channel. A procedure in which the diagonal elements of the correlation matrix of the operators are first evaluated to remove noisy operators, followed by the selection of sixteen operators whose renormalized correlation m ...
Coherent manipulation of single quantum systems
... was aided by collaboration with several scientists, most notably Dr. M.V. Gurudev Dutt, who shared equally in design, construction, and execution of the experiments, and Prof. M.D. Lukin, who guided our progress. These results would have been impossible without the generosity of Prof. John Doyle, wh ...
... was aided by collaboration with several scientists, most notably Dr. M.V. Gurudev Dutt, who shared equally in design, construction, and execution of the experiments, and Prof. M.D. Lukin, who guided our progress. These results would have been impossible without the generosity of Prof. John Doyle, wh ...
Breakdown of NRQCD Factorization
... •If the singularity appears in P-wave channel (the 3. line), one should find it in previous studies at one-loop level, because at tree level a gluon can not fragment into P-wave state. • NRQCD is formulated in the rest frame of a heavy quark pair, hence the factorization is made in the rest frame. T ...
... •If the singularity appears in P-wave channel (the 3. line), one should find it in previous studies at one-loop level, because at tree level a gluon can not fragment into P-wave state. • NRQCD is formulated in the rest frame of a heavy quark pair, hence the factorization is made in the rest frame. T ...
Primordial Black Holes - Recent Developments - SLAC
... application of “critical phenomena” to PBH formation. Studies of the collapse of various types of spherically symmetric matter fields have shown that there is always a critical solution which separates those configurations which form a black hole from those which disperse to an asymptotically flat stat ...
... application of “critical phenomena” to PBH formation. Studies of the collapse of various types of spherically symmetric matter fields have shown that there is always a critical solution which separates those configurations which form a black hole from those which disperse to an asymptotically flat stat ...
The crucial role of triplets in photoinduced charge transfer and
... branch of this curve (in the direction of more negative DG) is located in ‘‘ normal region ’’ where |DGi| < lc , where lc is the contact value of electron transfer reorganization energy. The opposite descending branch of the same FEG curve covers the highly exergonic ‘‘ inverted region ’’, where |DG ...
... branch of this curve (in the direction of more negative DG) is located in ‘‘ normal region ’’ where |DGi| < lc , where lc is the contact value of electron transfer reorganization energy. The opposite descending branch of the same FEG curve covers the highly exergonic ‘‘ inverted region ’’, where |DG ...
Patterns of Electro-magnetic Response in Topological Semi
... the “topological” contribution to the electromagnetic response for a TSM with two Dirac points using a fieldtheoretical calculation, and then go on to generalize the picture to a generic number of Dirac points. We also discuss the microscopic origin and subtleties of the response using lattice model ...
... the “topological” contribution to the electromagnetic response for a TSM with two Dirac points using a fieldtheoretical calculation, and then go on to generalize the picture to a generic number of Dirac points. We also discuss the microscopic origin and subtleties of the response using lattice model ...
hydrodynamics of a rotating strongly interacting fermi gas
... Strongly interacting Fermi gases are unique quantum fluids that can be used to model other strongly interacting systems in nature, such as the quark-gluon plasma of the big bang, high temperature superconductors, and nuclear matter. This is made possible through the use of a collisional resonance, p ...
... Strongly interacting Fermi gases are unique quantum fluids that can be used to model other strongly interacting systems in nature, such as the quark-gluon plasma of the big bang, high temperature superconductors, and nuclear matter. This is made possible through the use of a collisional resonance, p ...
For ULSI workshop. OUR SLIDES not ready. In PPT format.
... By iteratively applying the same input test vector (a probabilistic test) we are calculating the probability of getting the observed output. The input vectors are always vectors of pure states. Each successive iteration reduces the probability of obtaining a correct measurement for a faulty circuit. ...
... By iteratively applying the same input test vector (a probabilistic test) we are calculating the probability of getting the observed output. The input vectors are always vectors of pure states. Each successive iteration reduces the probability of obtaining a correct measurement for a faulty circuit. ...
Boundary conditions for integrable quantum systems
... where T ( U ) = T+(U )T-( U ) = LN( U ) . . . L,( U ) and is thus independent of the factorisation of T ( u ) into T+(u) and T-(u). Proof: Using the properties of the permutation operator 9' let us rewrite the definition (21) of F:(u) as ...
... where T ( U ) = T+(U )T-( U ) = LN( U ) . . . L,( U ) and is thus independent of the factorisation of T ( u ) into T+(u) and T-(u). Proof: Using the properties of the permutation operator 9' let us rewrite the definition (21) of F:(u) as ...