
Toward the Unification of Physics and Number Theory
... “an object that represents itself or something else”. And, finally, we define an object as “anything which can be thought of”. Fundamental particles have distinct geometries and are, in some sense, geometric symbols. For example, at each energy state, an orbiting electron forms a finite set of shape ...
... “an object that represents itself or something else”. And, finally, we define an object as “anything which can be thought of”. Fundamental particles have distinct geometries and are, in some sense, geometric symbols. For example, at each energy state, an orbiting electron forms a finite set of shape ...
ers Mathieu Guay-Paquet and J. Harnad ∗
... in the Cayley graph of Sn generated by transpositions, starting at an element in the conjugacy class with cycle type µ and ending in the class ν, that are weakly monotonically increasing, with λi elements in the successive bands in which the second elements bi remains constant. Remark 2.2. The enume ...
... in the Cayley graph of Sn generated by transpositions, starting at an element in the conjugacy class with cycle type µ and ending in the class ν, that are weakly monotonically increasing, with λi elements in the successive bands in which the second elements bi remains constant. Remark 2.2. The enume ...
Non-classical light and photon statistics
... effect explained with light quanta (Planck, Einstein). • 1920s – wave-particle duality: Quantum mechanics developed (Bohr, Heisenberg, de Broglie…), light and matter have both wave and particle properties. • 1920s-50s – photons: Quantum field theories developed (Dirac, Feynman), electromagnetic fiel ...
... effect explained with light quanta (Planck, Einstein). • 1920s – wave-particle duality: Quantum mechanics developed (Bohr, Heisenberg, de Broglie…), light and matter have both wave and particle properties. • 1920s-50s – photons: Quantum field theories developed (Dirac, Feynman), electromagnetic fiel ...
Bose-glass and Mott-insulator phase in the disordered boson Hubbard model
... 4 we show our results for z51, where one gets a clear intersection point of L r at K c8 50.32560.002. This value is very close to the corresponding value for the pure case K 8c pure50.33360.003 ~Ref. 18! and indicates that the tip of the lobe depends very weakly on the disorder strength or is even i ...
... 4 we show our results for z51, where one gets a clear intersection point of L r at K c8 50.32560.002. This value is very close to the corresponding value for the pure case K 8c pure50.33360.003 ~Ref. 18! and indicates that the tip of the lobe depends very weakly on the disorder strength or is even i ...
the transcendental meditation technique and quantum physics
... mood. Moreover, from the existence of the pure consciousness state, the scientist interested in studying consciousness learns two important facts. First, it becomes evident that conscious awareness does not depend on thought content; it can exist by itself ( 10). Second, it is seen that consciousnes ...
... mood. Moreover, from the existence of the pure consciousness state, the scientist interested in studying consciousness learns two important facts. First, it becomes evident that conscious awareness does not depend on thought content; it can exist by itself ( 10). Second, it is seen that consciousnes ...
Interpreting Quantum Mechanics in Terms of - Philsci
... of observables on a single quantum system without disturbing its state appreciably, and its mechanism is independent of the controversial process of wavefunction collapse and only depends on the linear Schrödinger evolution and the Born rule, which are two established parts of quantum mechanics. As ...
... of observables on a single quantum system without disturbing its state appreciably, and its mechanism is independent of the controversial process of wavefunction collapse and only depends on the linear Schrödinger evolution and the Born rule, which are two established parts of quantum mechanics. As ...
Deterministic secure direct communication using GHZ states and
... from his measurement outcome Φ+ 36 . If Alice and Charlie encode Φ14 , Φ14 , Ψ14 , and Ψ14 as 00, 01, 10, and 11, then they share two classical bits 01. Alice and Charlie sacrifice some randomly selected bits to test the “error rate”. If the error rate is too high, they abort this QKD protocol. Othe ...
... from his measurement outcome Φ+ 36 . If Alice and Charlie encode Φ14 , Φ14 , Ψ14 , and Ψ14 as 00, 01, 10, and 11, then they share two classical bits 01. Alice and Charlie sacrifice some randomly selected bits to test the “error rate”. If the error rate is too high, they abort this QKD protocol. Othe ...
Chapter 10 The Hydrogen Atom The Schrodinger Equation in
... The solutions to equation (10–7) are the spherical harmonic functions, and the l used in the separation constant is, in fact, the same used as the index l in the spherical harmonics Yl,m (θ, φ). In fact, it is the angular momentum quantum number. But where is the index m? How is the magnetic moment ...
... The solutions to equation (10–7) are the spherical harmonic functions, and the l used in the separation constant is, in fact, the same used as the index l in the spherical harmonics Yl,m (θ, φ). In fact, it is the angular momentum quantum number. But where is the index m? How is the magnetic moment ...