Holographic Quantum Error Correcting Codes - Adrian Franco
... is a rank-one projector on the one-dimensional subspace generated by |ψi. Depending on what system we are dealing with, the space of states will have different aspect. For example, if we consider a particle which can move in one dimension, its space of states is spanned by the states {|xi}x∈R , wher ...
... is a rank-one projector on the one-dimensional subspace generated by |ψi. Depending on what system we are dealing with, the space of states will have different aspect. For example, if we consider a particle which can move in one dimension, its space of states is spanned by the states {|xi}x∈R , wher ...
Quantized magnetoresistance in atomic-size
... The entire electrochemical cell was rotated by a step motor in a magnetic field of 1 T produced by an electromagnet. Both the angle and the conductance were synchronically recorded as a function of time. The angular rotation was performed from 0° to 180°, with 0° corresponding to the magnetic field ...
... The entire electrochemical cell was rotated by a step motor in a magnetic field of 1 T produced by an electromagnet. Both the angle and the conductance were synchronically recorded as a function of time. The angular rotation was performed from 0° to 180°, with 0° corresponding to the magnetic field ...
Contextuality, cohomology and paradox
... mechanics, which plays an important rôle in quantum error correction [42] and measurement-based quantum computation [47]. We then show how all such All-vs-Nothing arguments are witnessed by the cohomological obstruction to the extension of local sections to global ones previously studied in [5]. Th ...
... mechanics, which plays an important rôle in quantum error correction [42] and measurement-based quantum computation [47]. We then show how all such All-vs-Nothing arguments are witnessed by the cohomological obstruction to the extension of local sections to global ones previously studied in [5]. Th ...
Spin-1 J1-J2 Heisenberg antiferromagnet on a square lattice: A
... the many-body wave function represented by a TNS should capture the entanglement in the ground state and thus gives a good approximation of the ground state. Contracting over all bond indices gives the wave function coefficient for a given spin state σ1 , . . . ,σN .32–34 In these tensor network-bas ...
... the many-body wave function represented by a TNS should capture the entanglement in the ground state and thus gives a good approximation of the ground state. Contracting over all bond indices gives the wave function coefficient for a given spin state σ1 , . . . ,σN .32–34 In these tensor network-bas ...
1. Homework Set 1
... where W is the solid cylinder defined by the inequalities x2 + y 2 ≤ 4 and −1 ≤ z ≤ 2. Solution. The fact that W is a cylinder should tip you off to use cylindrical coordinates, so let’s do so. Using the simple fact that x2 + y 2 = r2 and the shadow of W in the xy-plane is just a disk of radius 2, w ...
... where W is the solid cylinder defined by the inequalities x2 + y 2 ≤ 4 and −1 ≤ z ≤ 2. Solution. The fact that W is a cylinder should tip you off to use cylindrical coordinates, so let’s do so. Using the simple fact that x2 + y 2 = r2 and the shadow of W in the xy-plane is just a disk of radius 2, w ...
A Glimpse into Symplectic Geometry
... the real and imaginary parts of a complex coordinate zj = xj + iyj , then this quarter turn corresponds to multiplication by i. Below, we call it J0 . Other Examples. Every Kähler manifold (M, J, g) has a symplectic structure ωJ . Recall that a Kähler manifold M is made from pieces of complex Eucl ...
... the real and imaginary parts of a complex coordinate zj = xj + iyj , then this quarter turn corresponds to multiplication by i. Below, we call it J0 . Other Examples. Every Kähler manifold (M, J, g) has a symplectic structure ωJ . Recall that a Kähler manifold M is made from pieces of complex Eucl ...
BettoniPANDASpectroscopy
... based on the non abelian gauge group SU(3). It is part of the Standard Model. ...
... based on the non abelian gauge group SU(3). It is part of the Standard Model. ...
Future of Hadron Physics
... Hadron physics must deploy a diverse array of experimental and theoretical probes and tools in order to define and solve the problems of confinement and its relationship with DCSB These are two of the most important challenges in fundamental Science; and only we are equipped to solve them Craig ...
... Hadron physics must deploy a diverse array of experimental and theoretical probes and tools in order to define and solve the problems of confinement and its relationship with DCSB These are two of the most important challenges in fundamental Science; and only we are equipped to solve them Craig ...