Edge excitations and topological order in a rotating Bose gas
... states with filling fractions = 32 and = 43 of the principal Jain sequence. At even lower angular momentum, we study the edge properties of the state identified1 as the finite-sized Moore-Read 共or Pfaffian兲 state13 共 = 1兲. We observe a number of anomalies that persist up to the largest sizes st ...
... states with filling fractions = 32 and = 43 of the principal Jain sequence. At even lower angular momentum, we study the edge properties of the state identified1 as the finite-sized Moore-Read 共or Pfaffian兲 state13 共 = 1兲. We observe a number of anomalies that persist up to the largest sizes st ...
Direct and Indirect Couplings in Coherent
... The general model considered in this paper is illustrated in Figure 1. This arrangement provides a schematic representation of how a physical system of interest might be influenced by external systems (e.g. uncertainty, disturbances) and noise. The external system Wd is directly coupled to G, while ...
... The general model considered in this paper is illustrated in Figure 1. This arrangement provides a schematic representation of how a physical system of interest might be influenced by external systems (e.g. uncertainty, disturbances) and noise. The external system Wd is directly coupled to G, while ...
A Gentle Introduction to Quantum Computing
... meaning that for the time being we don’t care how they are physically implemented. All we care about the inputs they take and the corresponding outputs. Quantum gates have the property that they have an equivalent number of inputs and outputs. This stems specifically from the fact that quantum mecha ...
... meaning that for the time being we don’t care how they are physically implemented. All we care about the inputs they take and the corresponding outputs. Quantum gates have the property that they have an equivalent number of inputs and outputs. This stems specifically from the fact that quantum mecha ...
Quantum and Semiclassical Theories of Chemical Reaction Rates
... related to the “cellular dynamics” approach of Heller and co-workers” and to some of the IVRs used by Herman et all7 and by Kay.2o The final expression used to generate the results discussed in the the next section is thus ...
... related to the “cellular dynamics” approach of Heller and co-workers” and to some of the IVRs used by Herman et all7 and by Kay.2o The final expression used to generate the results discussed in the the next section is thus ...
PowerPoint file of HBM_Intro _part I
... diversity of the relations that exist between objects that play a role A simple model has a small diversity of its relations. ...
... diversity of the relations that exist between objects that play a role A simple model has a small diversity of its relations. ...
Interaction between quantum dots and superconducting microwave resonators Tobias Frey
... T. Frey, ETH PhD thesis (2013), more details T. Ihn, Oxford University Press (2010) ...
... T. Frey, ETH PhD thesis (2013), more details T. Ihn, Oxford University Press (2010) ...
Powerpoint format
... 1. Pick random x < N. 2. Compute f = gcd(x,N); if f l, return f // f is a factor 3. Find the least r > 0 such that xr 1 (mod N). 4. Compute f1 = gcd(xr/2 – 1,N) ); if f1 l, return f1 // f1 is a factor 5. Compute f2 = gcd(xr/2 + 1,N); if f2 l, return f2 // f2 is a factor 6. Go to 1 and repeat ...
... 1. Pick random x < N. 2. Compute f = gcd(x,N); if f l, return f // f is a factor 3. Find the least r > 0 such that xr 1 (mod N). 4. Compute f1 = gcd(xr/2 – 1,N) ); if f1 l, return f1 // f1 is a factor 5. Compute f2 = gcd(xr/2 + 1,N); if f2 l, return f2 // f2 is a factor 6. Go to 1 and repeat ...
Quantum computation and quantum information
... • With n qubits there are 2n different differential equations that must be solved • The equation above has the formal solution ...
... • With n qubits there are 2n different differential equations that must be solved • The equation above has the formal solution ...
Quantum channels and their capacities: An introduction
... Quantum channel is a linear completely positive trace-preserving map (CPTP) between quantum states. Why is a quantum channel given by a linear CPTP map (i) Linearity: ...
... Quantum channel is a linear completely positive trace-preserving map (CPTP) between quantum states. Why is a quantum channel given by a linear CPTP map (i) Linearity: ...
An Introduction to Elementary Particle Phenomenology
... that, since the matrix γ0 is block-diagonal ± , the parities of the upper and lower components of ψ are opposite. That is, the fermion and antifermion have opposite parities. By convention, the parity of fermions is chosen as positive and antifermions as negative. This particular choice has, of cou ...
... that, since the matrix γ0 is block-diagonal ± , the parities of the upper and lower components of ψ are opposite. That is, the fermion and antifermion have opposite parities. By convention, the parity of fermions is chosen as positive and antifermions as negative. This particular choice has, of cou ...
