THE BLACK HOLE INTERPRETATION OF STRING THEORY 1
... other forces such as color and weak charges are not given much attention in this paper . It should be fairly easy to take them into account. ...
... other forces such as color and weak charges are not given much attention in this paper . It should be fairly easy to take them into account. ...
CHAPTER 6: Quantum Mechanics II
... must be single valued. For finite potentials, the wave function and its derivative must be continuous. This is required because the second-order derivative term in the wave equation must be single valued. (There are exceptions to this rule when V is infinite.) In order to normalize the wave function ...
... must be single valued. For finite potentials, the wave function and its derivative must be continuous. This is required because the second-order derivative term in the wave equation must be single valued. (There are exceptions to this rule when V is infinite.) In order to normalize the wave function ...
Pascual Jordan`s resolution of the conundrum of the wave
... require separate mechanisms after all but can be accounted for within a single consistent dynamical framework. The authors presented their unified mechanism in terms of (quantized) waves, but it can also be described in terms of (quantum) particles. Heisenberg (1930) made this quite explicit a few y ...
... require separate mechanisms after all but can be accounted for within a single consistent dynamical framework. The authors presented their unified mechanism in terms of (quantized) waves, but it can also be described in terms of (quantum) particles. Heisenberg (1930) made this quite explicit a few y ...
Lecture 4: Quantum states of light — Fock states • Definition Fock
... Lecture 4: Quantum states of light — Fock states • Definition Fock states, photons • Photon statistics of quantized light prepared in Fock states Fock states, definition: So far, we have concentrated on introducing operators for the vector potential and thus the electric field. We have found that the q ...
... Lecture 4: Quantum states of light — Fock states • Definition Fock states, photons • Photon statistics of quantized light prepared in Fock states Fock states, definition: So far, we have concentrated on introducing operators for the vector potential and thus the electric field. We have found that the q ...
Quantum Computation and Statistical Physics
... measurements is quantum-NP hard Corollary: the planar code state can not be converted to the 2D cluster state by performing one-qubit measurements on a subset of qubits (even with exp. small success probability) ...
... measurements is quantum-NP hard Corollary: the planar code state can not be converted to the 2D cluster state by performing one-qubit measurements on a subset of qubits (even with exp. small success probability) ...
Factorization Method and the Position
... very concept of a PDM system is a fundamental problem which is far from being completely understood. Many contributions have been developed over the last years in different approaches [8–19]. In the quantum mechanical regime, it is well known that an ambiguity in ordering of the mass and the momentum ...
... very concept of a PDM system is a fundamental problem which is far from being completely understood. Many contributions have been developed over the last years in different approaches [8–19]. In the quantum mechanical regime, it is well known that an ambiguity in ordering of the mass and the momentum ...
Lecture 8
... computed f exactly we get a multilinear polynomial of degree 2T that satisfies p(x)=f(x) for all x. If the quantum algorithm has error 1/, then there is a polynomial with p(x)2[0,1/3] for f(x)=0 and p(x)2[2/3,1] for f(x)=1 Now we have to consider the degree of polynomials representing Boolean functi ...
... computed f exactly we get a multilinear polynomial of degree 2T that satisfies p(x)=f(x) for all x. If the quantum algorithm has error 1/, then there is a polynomial with p(x)2[0,1/3] for f(x)=0 and p(x)2[2/3,1] for f(x)=1 Now we have to consider the degree of polynomials representing Boolean functi ...
On Cayley graphs, surface codes, and the limits of homological
... Surface codes also provide the presently only known family of quantum LDPC codes with constant rate and provably growing minimum distance [7], [10]. The minimum distance for these families grows like a logarithm of the blocklength. Published accounts of these families of codes involved sophisticated ...
... Surface codes also provide the presently only known family of quantum LDPC codes with constant rate and provably growing minimum distance [7], [10]. The minimum distance for these families grows like a logarithm of the blocklength. Published accounts of these families of codes involved sophisticated ...
The Structure of Scientific Theory Change
... of theoretical structure, would seem to cast some doubt on the adequacy of that conception. If the use of a theory (in particular to extend the theory to a new domain and, ancillarily, to properly understand the current theory) very often requires that the theory itself be considered to be something ...
... of theoretical structure, would seem to cast some doubt on the adequacy of that conception. If the use of a theory (in particular to extend the theory to a new domain and, ancillarily, to properly understand the current theory) very often requires that the theory itself be considered to be something ...
The Structure Lacuna
... duality was concocted, notwithstanding the wave-mechanical alternative proposed by Schrödinger. As the particle model found its way into textbooks the electronic wave structure was completely forgotten, although the quantum-mechanical model never made any logical sense. In order to rationalize the ...
... duality was concocted, notwithstanding the wave-mechanical alternative proposed by Schrödinger. As the particle model found its way into textbooks the electronic wave structure was completely forgotten, although the quantum-mechanical model never made any logical sense. In order to rationalize the ...
Quantum Computing
... C 2 de nes a measurement whose possible outcomes are the elements of this basis. However, we assume that the output is obtained P by projecting each qubit onto the basis fV0 ; V1 g. When applied to a state s s Vs , this projection produces the string s with probability j s j2 . The quantum measurem ...
... C 2 de nes a measurement whose possible outcomes are the elements of this basis. However, we assume that the output is obtained P by projecting each qubit onto the basis fV0 ; V1 g. When applied to a state s s Vs , this projection produces the string s with probability j s j2 . The quantum measurem ...
Reflection Symmetry and Energy-Level Ordering in Frustrated Spin
... The spin of M can be found by constructing a trial state being a positive superposition of (shifted) Ising basic states and having a definite value of the spin. Then it will overlap with M. The uniqueness of the relative GS then implies that both states have the same spin. As a result, ...
... The spin of M can be found by constructing a trial state being a positive superposition of (shifted) Ising basic states and having a definite value of the spin. Then it will overlap with M. The uniqueness of the relative GS then implies that both states have the same spin. As a result, ...
Wellposedness of a nonlinear, logarithmic Schrödinger equation of
... rise to a modular type nonlinearity κQψ [6, 25], represents a field through which the electrons interact with themselves and can be interpreted as a quantum diffusion term yielding a theory which contains quantum–mechanical confinement ...
... rise to a modular type nonlinearity κQψ [6, 25], represents a field through which the electrons interact with themselves and can be interpreted as a quantum diffusion term yielding a theory which contains quantum–mechanical confinement ...