Experimental nonlocal and surreal Bohmian trajectories
... in classical mechanics. In orthodox quantum mechanics, however, a particle does not follow a trajectory, because it does not have a simultaneous position and momentum. Nonetheless, it is possible to reinterpret the quantum formalism as describing particles following definite trajectories, each with ...
... in classical mechanics. In orthodox quantum mechanics, however, a particle does not follow a trajectory, because it does not have a simultaneous position and momentum. Nonetheless, it is possible to reinterpret the quantum formalism as describing particles following definite trajectories, each with ...
Shock waves, rarefaction waves and non
... is that the steady state is formed by propagating wavefronts emanating from the contact region. For small temperature differences these wavefronts are ordinary sound waves, but for large temperature differences their dynamics is non-linear. The properties of the NESS are constrained by the equation ...
... is that the steady state is formed by propagating wavefronts emanating from the contact region. For small temperature differences these wavefronts are ordinary sound waves, but for large temperature differences their dynamics is non-linear. The properties of the NESS are constrained by the equation ...
Dynamic model of elementary particles and the nature of mass and
... m0 is significantly less than the associated one ma , then the mass of the particle will be defined only by its associated mass ma and it is the field mass in the central exchange. Obviously, the rest mass of the particle m0 is the associated one with respect to the deeper level of the field of matt ...
... m0 is significantly less than the associated one ma , then the mass of the particle will be defined only by its associated mass ma and it is the field mass in the central exchange. Obviously, the rest mass of the particle m0 is the associated one with respect to the deeper level of the field of matt ...
Imaging electrostatically confined Dirac fermions in graphene
... Our observations can be explained by considering the behaviour of massless Dirac fermions in response to a circular electrostatic potential. Due to Klein tunnelling, a graphene p–n junction perfectly transmits quasiparticles at normal incidence to the boundary, but reflects them at larger angles of ...
... Our observations can be explained by considering the behaviour of massless Dirac fermions in response to a circular electrostatic potential. Due to Klein tunnelling, a graphene p–n junction perfectly transmits quasiparticles at normal incidence to the boundary, but reflects them at larger angles of ...
ON THE EQUATIONAL THEORY OF PROJECTION LATTICES OF
... Lemma 2.2. An ortholattice identity t = 0 with m occurences of variables holds in a given atomic MOL L if any only if it holds in all sections [0, u] of L with dim u ≤ m. Proof. As usual, we write x for sequences (x1 , . . . , xn ) with n varying according to the context. We show by induction on com ...
... Lemma 2.2. An ortholattice identity t = 0 with m occurences of variables holds in a given atomic MOL L if any only if it holds in all sections [0, u] of L with dim u ≤ m. Proof. As usual, we write x for sequences (x1 , . . . , xn ) with n varying according to the context. We show by induction on com ...
The Light of Existence
... That it is because it is has never been a very satisfactory answer in science. In quantum realism, the speed of light is the network refresh rate, which is finite because every processor runs at a finite rate, e.g. a 5GHz computer runs at 5,000,000,000 cycles per second. If light goes from one node ...
... That it is because it is has never been a very satisfactory answer in science. In quantum realism, the speed of light is the network refresh rate, which is finite because every processor runs at a finite rate, e.g. a 5GHz computer runs at 5,000,000,000 cycles per second. If light goes from one node ...
Few-Particle Effects in Semiconductor Quantum Dots: Spectrum Calculations on
... symmetry in semiconductor quantum dots using configuration interaction calculation. Moreover, to compare with the experimental data, we studied the effects of hidden symmetry. The 2D single-band model and the 3D single-band model were used to generate the single-particle states. How the spectra affe ...
... symmetry in semiconductor quantum dots using configuration interaction calculation. Moreover, to compare with the experimental data, we studied the effects of hidden symmetry. The 2D single-band model and the 3D single-band model were used to generate the single-particle states. How the spectra affe ...
Universal quantum simulation with prethreshold superconducting qubits: Single-excitation subspace method
... Current quantum computing architectures lack the size and fidelity required for universal fault-tolerant operation, limiting the practical implementation of key quantum algorithms to all but the smallest problem sizes. In this work we propose an alternative method for general-purpose quantum computa ...
... Current quantum computing architectures lack the size and fidelity required for universal fault-tolerant operation, limiting the practical implementation of key quantum algorithms to all but the smallest problem sizes. In this work we propose an alternative method for general-purpose quantum computa ...
Lecture 1 Review of hydrogen atom Heavy proton (put at the origin
... Elementary particles carry intrinsic angular momentum S in addition to L. Spin of elementary particles has nothing to do with rotation, does not depend on coordinates and , and is purely a quantum mechanical phenomena. ...
... Elementary particles carry intrinsic angular momentum S in addition to L. Spin of elementary particles has nothing to do with rotation, does not depend on coordinates and , and is purely a quantum mechanical phenomena. ...
Full text in PDF form
... So the chain above must be symmetrized by accompaniment of the arrow on the left ,so in an ordinary situation we have a chain: (Early Universe, origin singularity, QMFL, density pro-matrix) → (Large-scale limit, QM, density matrix)→ (Black Hole, singularity, QMFL, density pro-matrix), So it’s more c ...
... So the chain above must be symmetrized by accompaniment of the arrow on the left ,so in an ordinary situation we have a chain: (Early Universe, origin singularity, QMFL, density pro-matrix) → (Large-scale limit, QM, density matrix)→ (Black Hole, singularity, QMFL, density pro-matrix), So it’s more c ...
Functional RG for few
... → action evolves with regulator scale k becomes full effective action as k → 0 Legendre-transformed action Γ (generator for 1PI diagrams) evolves according to “one-loop” RG equation ...
... → action evolves with regulator scale k becomes full effective action as k → 0 Legendre-transformed action Γ (generator for 1PI diagrams) evolves according to “one-loop” RG equation ...
Quantum Teleportation
... each letter has been shifted up by 13 places, with letters above the thirteenth in the alphabet rotated to the beginning. Or they can be very complex, such as a very very long string of binary digits. Here is an example of using binary numbers to encrypt and decrypt a message, in this case the lette ...
... each letter has been shifted up by 13 places, with letters above the thirteenth in the alphabet rotated to the beginning. Or they can be very complex, such as a very very long string of binary digits. Here is an example of using binary numbers to encrypt and decrypt a message, in this case the lette ...
Multimode quantum memory based on atomic frequency combs
... tial mode defined by the direction of propagation of the input field兲, ␦ j the detuning of the atom with respect to the laser frequency, and the amplitudes c j depend on the frequency and on the spatial position of the particular atom j. The collective state can be understood as a coherent excitatio ...
... tial mode defined by the direction of propagation of the input field兲, ␦ j the detuning of the atom with respect to the laser frequency, and the amplitudes c j depend on the frequency and on the spatial position of the particular atom j. The collective state can be understood as a coherent excitatio ...
Building and bounding quantum Bernoulli factories
... the output type of the factory. For instance, the “quantum Bernoulli factory” of DJR becomes a “quantum coin factory” in our terminology since it uses quoins to make coins. We will use the term “Bernoulli factory” to refer generally to algorithms that use a black-box input hiding a probability distr ...
... the output type of the factory. For instance, the “quantum Bernoulli factory” of DJR becomes a “quantum coin factory” in our terminology since it uses quoins to make coins. We will use the term “Bernoulli factory” to refer generally to algorithms that use a black-box input hiding a probability distr ...
A categorification of a quantum Frobenius map
... simplified relation-checking criterion of Brundan [Bru16] for Khovanov-Lauda-Rouquier’s 2-KacMoody categorification theorem. In the course of the proof, we also obtain a reduction result (Theorem 4.12) which shows that D(U̇ ) can be generated by 1-morphisms of the form E 1n , E (p) 1n , F 1n , F (p) ...
... simplified relation-checking criterion of Brundan [Bru16] for Khovanov-Lauda-Rouquier’s 2-KacMoody categorification theorem. In the course of the proof, we also obtain a reduction result (Theorem 4.12) which shows that D(U̇ ) can be generated by 1-morphisms of the form E 1n , E (p) 1n , F 1n , F (p) ...
Lecture 7
... More specific: Is it possible by using only black box techniques? And not the precise problem structure E.g. SAT Problem: given a CNF formula on n variables, is there a satisfying assignment? Trivial approach: Try all 2n assignments of the variables Can a quantum computer do this efficiently? ...
... More specific: Is it possible by using only black box techniques? And not the precise problem structure E.g. SAT Problem: given a CNF formula on n variables, is there a satisfying assignment? Trivial approach: Try all 2n assignments of the variables Can a quantum computer do this efficiently? ...