How to test the “quantumness” of a quantum computer? Miroslav Grajcar
... Nevertheless, we believe that this problem can be solved. This will first require developing a better set of theoretical tools. A system of qubits is, after all, a quantum many-body system, which may be amenable to the approaches which worked so well in many applications to condensed matter physics ...
... Nevertheless, we believe that this problem can be solved. This will first require developing a better set of theoretical tools. A system of qubits is, after all, a quantum many-body system, which may be amenable to the approaches which worked so well in many applications to condensed matter physics ...
How to model quantum plasmas Giovanni Manfredi
... we must therefore require that the collision rates of electrons and ions with the neutral molecules be relatively low compared to typical collective phenomena. In the present work, we shall avoid this issue altogether by restricting our analysis to the simpler case of fully ionized gases. When quant ...
... we must therefore require that the collision rates of electrons and ions with the neutral molecules be relatively low compared to typical collective phenomena. In the present work, we shall avoid this issue altogether by restricting our analysis to the simpler case of fully ionized gases. When quant ...
Holographic Quantum Error Correcting Codes - Adrian Franco
... The fact that we are considering orthonormal bases goes a little bit further than just mere computational convenience: in quantum mechanics, states which are proportional to each other are considered to be indistinguishable from a physical point of view. In more precise words, the space of different ...
... The fact that we are considering orthonormal bases goes a little bit further than just mere computational convenience: in quantum mechanics, states which are proportional to each other are considered to be indistinguishable from a physical point of view. In more precise words, the space of different ...
Theory of Chemical Bonds
... the wave function of the atomic orbitals. During the calculation of the eigenvalues of the Schrödinger equation with equ. 4.15, we get integrals which contain the square of the wave function of an atomic orbital (∫ψ1*H ψ1dτ). These integral represent the Coulomb interaction energy between the electr ...
... the wave function of the atomic orbitals. During the calculation of the eigenvalues of the Schrödinger equation with equ. 4.15, we get integrals which contain the square of the wave function of an atomic orbital (∫ψ1*H ψ1dτ). These integral represent the Coulomb interaction energy between the electr ...
Quantum Chaos
... exactly like the classical phase space density. For chaotic systems, the classical phase space distributions develop structures at smaller and smaller scales as time increases ∂3W/∂p3 becomes larger and larger. Even for tiny Planck constant, the corrections will eventually overcome the lowest ...
... exactly like the classical phase space density. For chaotic systems, the classical phase space distributions develop structures at smaller and smaller scales as time increases ∂3W/∂p3 becomes larger and larger. Even for tiny Planck constant, the corrections will eventually overcome the lowest ...
Physics 1001 (Regular) Mechanics Module
... You will firstly investigate the causes of changes in the state of motion — a field of physics called dynamics — in particular to understand the basis and application of Newton’s laws of motion. You will also relate the ideas of Newtonian dynamics to the concepts of work and energy, and the laws of ...
... You will firstly investigate the causes of changes in the state of motion — a field of physics called dynamics — in particular to understand the basis and application of Newton’s laws of motion. You will also relate the ideas of Newtonian dynamics to the concepts of work and energy, and the laws of ...
Quantum-information transport to multiple receivers
... ⍀B j is the TME between B j and 2j − 1, and ci, is the annihilation operator for a qubit with state = 0 , 1 on site i for i = A , 1 , . . . , 2n − 1 , B1 , . . . , Bn. Control of these TMEs is by varying the potential barrier between the sites and the chain. The exact method for this variation is ...
... ⍀B j is the TME between B j and 2j − 1, and ci, is the annihilation operator for a qubit with state = 0 , 1 on site i for i = A , 1 , . . . , 2n − 1 , B1 , . . . , Bn. Control of these TMEs is by varying the potential barrier between the sites and the chain. The exact method for this variation is ...
The strange (hi)story of particles and waves*
... Eugene Wigner spoke of a “Balkanization of physics” – a traditional (Hapsburgian) expression for the deterioration of law and order. ...
... Eugene Wigner spoke of a “Balkanization of physics” – a traditional (Hapsburgian) expression for the deterioration of law and order. ...
