Understanding Quantum Theory
... Argues that probability still makes sense, and that the usual probability rules of quantum theory can be derived from reasonable assumptions. Philip Goyal ...
... Argues that probability still makes sense, and that the usual probability rules of quantum theory can be derived from reasonable assumptions. Philip Goyal ...
Document
... • E.G. MSSM: In general, the MSSM contains many new parameters, including multiple new CP-violating phases, e.g. ...
... • E.G. MSSM: In general, the MSSM contains many new parameters, including multiple new CP-violating phases, e.g. ...
Phys. Rev. Lett. 104, 255303
... Bogoliubov quasiparticles have definite momentum referred to B, they cannot be labeled by ‘, because the condensate configuration breaks the symmetry under translation T y . The constant H 0c in Eq. (5) gives the zero-point correction to h0 which, along with the contribution from thermally excited q ...
... Bogoliubov quasiparticles have definite momentum referred to B, they cannot be labeled by ‘, because the condensate configuration breaks the symmetry under translation T y . The constant H 0c in Eq. (5) gives the zero-point correction to h0 which, along with the contribution from thermally excited q ...
Theoretische und Mathematische Grundlagen der Physik
... part of my talk I will give an overview over the results obtained so far for this manifold with the help of what M. Blau and G. Thompson call “torus gauge fixing”. In the last part of my talk I will sketch what remains to be done in order to complete Steps 1 and 2 for the latter manifold and I will ...
... part of my talk I will give an overview over the results obtained so far for this manifold with the help of what M. Blau and G. Thompson call “torus gauge fixing”. In the last part of my talk I will sketch what remains to be done in order to complete Steps 1 and 2 for the latter manifold and I will ...
1. The Relativistic String
... Although the Lagrangian (1.1) is correct, it’s not fully satisfactory. The reason is that time t and space ~x play very different roles in this Lagrangian. The position ~x is a dynamical degree of freedom. In contrast, time t is merely a parameter providing a label for the position. Yet Lorentz tran ...
... Although the Lagrangian (1.1) is correct, it’s not fully satisfactory. The reason is that time t and space ~x play very different roles in this Lagrangian. The position ~x is a dynamical degree of freedom. In contrast, time t is merely a parameter providing a label for the position. Yet Lorentz tran ...
Lectures on Electric-Magnetic Duality and the Geometric
... The Langlands Program is a far-reaching collection of theorems and conjectures about representations of the absolute Galois group of certain fields. For a recent accessible review see [1]. V. Drinfeld and G. Laumon [2] introduced a geometric analogue which deals with representations of the fundament ...
... The Langlands Program is a far-reaching collection of theorems and conjectures about representations of the absolute Galois group of certain fields. For a recent accessible review see [1]. V. Drinfeld and G. Laumon [2] introduced a geometric analogue which deals with representations of the fundament ...
Acrobat PDF - Electronic Journal of Theoretical Physics
... After introducing an effective field theory for processes with a typical energy less the Planck mass, i.e. with |q 2 | MP2 1038 GeV2 , by Weinberg [27], the effective theory for gravity can been modeled in a manner analogous with that of Chiral Perturbation Theory [28] for QCD. This way to look at ...
... After introducing an effective field theory for processes with a typical energy less the Planck mass, i.e. with |q 2 | MP2 1038 GeV2 , by Weinberg [27], the effective theory for gravity can been modeled in a manner analogous with that of Chiral Perturbation Theory [28] for QCD. This way to look at ...
Quantum Criticality: competing ground states in low
... modified by an overall prefactor if we stretch the length scale (i.e. perform a scale transfor5 ...
... modified by an overall prefactor if we stretch the length scale (i.e. perform a scale transfor5 ...
Computation in a Topological Quantum Field Theory
... The null space of this operator is exactly the stabilizer code space of the toric code. Because the operator is nonnegative, we then see that the stabilizer space of the code is precisely the space of minimal energy for this Hamiltonian. It follows that the excited states, having non-minimal energy, ...
... The null space of this operator is exactly the stabilizer code space of the toric code. Because the operator is nonnegative, we then see that the stabilizer space of the code is precisely the space of minimal energy for this Hamiltonian. It follows that the excited states, having non-minimal energy, ...