Musical Modulation by Symmetries
... by Mazzola and Muzzulini an analogy is made to modern physics, where symmetries are used to explain forces of transition. • This modulation model provides direct modulations between all tonalities in C12 in 12 tempered tuning, and the relationships when applied to the diatonic major, harmonic and me ...
... by Mazzola and Muzzulini an analogy is made to modern physics, where symmetries are used to explain forces of transition. • This modulation model provides direct modulations between all tonalities in C12 in 12 tempered tuning, and the relationships when applied to the diatonic major, harmonic and me ...
Polynomial-Time Algorithms for Prime Factorization and Discrete
... of the components, there is a basis state of this vector space that we represent, for example, by |011 · · · 0i, meaning that the first bit is 0, the second bit is 1, and so on. Here, the ket notation |xi means that x is a (pure) quantum state. (Mixed states will not be discussed in this paper, and ...
... of the components, there is a basis state of this vector space that we represent, for example, by |011 · · · 0i, meaning that the first bit is 0, the second bit is 1, and so on. Here, the ket notation |xi means that x is a (pure) quantum state. (Mixed states will not be discussed in this paper, and ...
![arXiv:0905.2946v1 [cond-mat.str-el] 18 May 2009](http://s1.studyres.com/store/data/003310684_1-f6852d9094cc4ebe5853c88b867e67b0-300x300.png)
Critical and oÿ-critical singularities in disordered quantum magnets H. Rieger
... Quantum phase transitions are phase transitions at zero temperature driven by quantum ÿuctuations rather than thermal ÿuctuations. If disorder is involved, as in random magnets, in amorphous bosonic systems or at the Mott-Anderson transition, one encounters new features that are usually absent in pu ...
... Quantum phase transitions are phase transitions at zero temperature driven by quantum ÿuctuations rather than thermal ÿuctuations. If disorder is involved, as in random magnets, in amorphous bosonic systems or at the Mott-Anderson transition, one encounters new features that are usually absent in pu ...
Chapter 9 Angular Momentum Quantum Mechanical Angular
... Notice like the nonsense operators hardness and color, none of the angular momentum component operators commute and none of the eigenvectors correspond. Also comparable, L2 is proportional to the identity operator, except in three dimensions. We can do something similar to the “hardness, color” case ...
... Notice like the nonsense operators hardness and color, none of the angular momentum component operators commute and none of the eigenvectors correspond. Also comparable, L2 is proportional to the identity operator, except in three dimensions. We can do something similar to the “hardness, color” case ...
Multiphoton adiabatic rapid passage: classical transition induced by separatrix crossing
... model and for a full three-dimensional calculation for Li using a model potential that gives the correct quantum defects of the Rydberg states. We are able to confirm that the results of the measurement are due to the microwave transitions described in [3]. We also performed threedimensional quantum ...
... model and for a full three-dimensional calculation for Li using a model potential that gives the correct quantum defects of the Rydberg states. We are able to confirm that the results of the measurement are due to the microwave transitions described in [3]. We also performed threedimensional quantum ...
Topological Orders
... Physicists found that all discovered quantum Hall states have such densities that the filling factors are exactly given by some rational numbers, such as ν = 1, 1/3, 2/3, 2/5, .... quantum Hall states with simple rational filling factors (such as ν = 1, 1/3, 2/3, ...) are more stable and easier to o ...
... Physicists found that all discovered quantum Hall states have such densities that the filling factors are exactly given by some rational numbers, such as ν = 1, 1/3, 2/3, 2/5, .... quantum Hall states with simple rational filling factors (such as ν = 1, 1/3, 2/3, ...) are more stable and easier to o ...
Isotropic restriction in Group Field Theory condensates
... functions. We can define an inner product between any cylindrical functions, which has the essential property to be invariant under SU(2) gauge transformations and 3d diffeomorphisms. HG is the SU(2) gauge-invariant subspace of Hkin . A basis of Hkin is found using the Peter-Weyl decomposition of in ...
... functions. We can define an inner product between any cylindrical functions, which has the essential property to be invariant under SU(2) gauge transformations and 3d diffeomorphisms. HG is the SU(2) gauge-invariant subspace of Hkin . A basis of Hkin is found using the Peter-Weyl decomposition of in ...
Quantum Field Theory Frank Wilczek
... atoms, or molecules. The indistinguishability of particles is so familiar, and so fundamental to all of modern physical science, that we could easily take it for granted. Yet it is by no means obvious. For example, it directly contradicts one of the pillars of Leibniz' metaphysics, his \principle of ...
... atoms, or molecules. The indistinguishability of particles is so familiar, and so fundamental to all of modern physical science, that we could easily take it for granted. Yet it is by no means obvious. For example, it directly contradicts one of the pillars of Leibniz' metaphysics, his \principle of ...
Waveguides, Resonant Cavities, Optical Fibers and
... Electronic transport in conducting solids is generally diffusive. Its flow follows the gradient in the electrochemical potential, constricted by the physical or electrostatic edges of the specimen or device. So, the mean free path of electrons is very short compared to the dimension of the specimen. ...
... Electronic transport in conducting solids is generally diffusive. Its flow follows the gradient in the electrochemical potential, constricted by the physical or electrostatic edges of the specimen or device. So, the mean free path of electrons is very short compared to the dimension of the specimen. ...
Experimental and theoretical challenges for the trapped electron
... different voltage. A trap might be formed above one of the hexagons at U0 = 0 (dark grey in the figure) which is surrounded by six hexagons at U1 = +0.6 V which are again surrounded by 12 hexagons at U2 = −0.5015 V for the compensation of axial anharmonicity. All other electrodes are at U = 0 V. (b) ...
... different voltage. A trap might be formed above one of the hexagons at U0 = 0 (dark grey in the figure) which is surrounded by six hexagons at U1 = +0.6 V which are again surrounded by 12 hexagons at U2 = −0.5015 V for the compensation of axial anharmonicity. All other electrodes are at U = 0 V. (b) ...
Full text in PDF form
... namely the emergence of a gravitational field. All that is encoded in the condensate structure of |OM >. As can be seen from Eqs. (4) and (5) in the Appendix, a constant temperature T = β −1 implies that the M² -frame is static and time-independent. We remark that one of the advantages of the approa ...
... namely the emergence of a gravitational field. All that is encoded in the condensate structure of |OM >. As can be seen from Eqs. (4) and (5) in the Appendix, a constant temperature T = β −1 implies that the M² -frame is static and time-independent. We remark that one of the advantages of the approa ...