Noncommutative Geometry, Quantum Fields and Motives |
ما يقوله الناس - كتابة مراجعة
لم نعثر على أي مراجعات في الأماكن المعتادة.
المحتويات
| 1 | |
The Riemann zeta function and noncommutative geometry | 341 |
Quantum statistical mechanics and Galois symmetries | 437 |
Endomotives thermodynamics and the Weil explicit formula | 577 |
Appendix | 733 |
Bibliography | 749 |
Index | 763 |
طبعات أخرى - عرض جميع المقتطفات
عبارات ومصطلحات مألوفة
1-dimensional 2-dimensional Q-lattices abelian adele class space affine group scheme automorphisms bundle C*-algebra Chapter coefficients cohomology commensurability commutative compact condition consider construction corresponding counterterms cyclic cyclic cohomology cyclic modules defined Definition denote dimension Dirac operator dual elements endomorphisms endomotives equation equisingular equivalence explicit fact factor fermions field theory finite following result Fourier transform functor Galois group gauge given gives group scheme groupoid Haar measure Higgs Hilbert space homomorphism Hopf algebra inner fluctuations integral isomorphism L-functions Lagrangian Lemma linear matrix modular module morphism motives multiplication neutrino noncommutative geometry noncommutative space normalization notation obtained pair parameters Proof Proposition quantum statistical mechanical quark quotient relation renormalization representation restriction Riemann satisfies scaling Shimura variety shows spectral action spectral triple Standard Model subalgebra subgroup subspace symmetries Tannakian Tannakian category tensor Theorem trace formula values vector von Neumann algebra zero zeta function
مقاطع مشهورة
الصفحة 198 - The usual notion of dimension of a space is replaced by the dimension spectrum which is a subset of C...
الصفحة 743 - Sauter a pieds joints sur ces calculs; grouper les operations, les classer suivant leurs difficultes et non suivant leurs formes; telle est selon moi, la mission des geometres futurs
الصفحة 308 - Notice that the infrared behavior of these terms approaches the fixed point rj = 0, u> = -0.0228, 9 = 0.327. The coefficient 77 goes to zero in the infrared limit, sufficiently slowly, so that, up to scales of the order of the size of the universe, its inverse remains 0(1). On the other hand...
الصفحة 191 - Under the hypothesis that the dimension spectrum is simple, ie that the spectral functions have at most simple poles, the residue at the pole defines a far reaching extension (cf.
الصفحة 206 - By the principle of gauge invariance, the only quantities which have a chance to be observables in gravity are those which are invariant under the gauge group ie the group of diffeomorphisms of the space-time M . Assuming first that we deal with a classical manifold...
الصفحة 163 - The classification of the leptons and quarks into families according to a mass progression. The first generation consists of the electron and its neutrino and of the up and down quarks. The second generation consists of the muon and its neutrino and of the charm and strange quarks. The third generation consists of the tau and its neutrino and of the bottom and expected top quarks. GeV. (Giga electron volt) A unit of energy equal to one billion (10 V ) electron volts.
الصفحة 308 - On the other hand, 77(4), u(t) and 0(t) have a common singularity at an energy scale of the order of 1023 GeV, which is above the Planck scale. Moreover, within the energy scales that are of interest to our model...
الصفحة 185 - Let us consider the simplest example, where the algebra A = C°°(M, Mn(C)) = C°°(M) ® Mn(C) consists of smooth maps from a manifold M to the algebra Mn(C) of nxn matrices.
الصفحة 190 - This way of defining a geometry by specifying the Dirac operator is meaningful both in mathematical terms (where the Dirac operator specifies the fundamental class in...

