The Classical Theory of Fields (Book): Difference between revisions

The Classical Theory of Fields (Book) (edit)

Revision as of 00:29, 3 February 2024

33 bytes added , 3 February

m

no edit summary

Anisomorphism

Bureaucrats, Interface administrators, Suppressors, Administrators, Widget editors

447

edits

@@ Line 24: / Line 24: @@
 Finally, Yang-Mills by Atiyah. These lecture notes introduce some of the early results of the theory like the construction of instanton solutions and the conversion of these equations to Penrose's complex-geometry Twistor setting in a notation familiar to physicists, in coordinates, matrices, quaternions. As you will see in studying the mathematical aspects of Yang-Mills theory (YM) on 4-dimensional space-time, this dimension is particularly interesting. Penrose's book on Spinors and Space-Time shows this uniqueness in another way, converting the tensor calculus of GR into spinor calculus, another equally geometric formulation but specific to this dimension. He shows that the equations of both EM and GR can be put in this setting, and in his second volume expands on this to his Twistor-space formulation of particle physics. Milnor's Characteristic Classes and Atiyah's K-theory books pick up where Bott & Tu left off and characterize the algebra of vector bundles in two different ways. Characteristic classes are the language by which curvature and an invariant polynomial on a Lie group are associated to an underlying class of a vector bundle, which is the hinted combination of curvature and differential forms from earlier. This is used to count a deformation-invariant type of gauge theoretic state, and is known as a topological quantum number in quantum field theory and condensed matter physics. K-theory as another fundamental invariant looks at vector bundles with a fixed type of geometric structure but over all dimensions, meaning e.g. it describes properties of the rotation or unitary groups that are 'stable' in all dimensions. It has a subtle meaning, but is connected to spinors and Clifford algebras via Bott periodicity.
-Kobayashi & Nomizu's book series is like a sequel to Sternberg's lectures in that its focus is on the definitions of geometric structures rather than algebraic invariants, and begins on connection theory where Sternberg's book ends. It also describes characteristic classes in an alternate way, via the Chern-Weil homomorphism with its starting point being curvature and connections rather than abstract algebraic invariants (since Milnor only references the curvature story in his appendix). Here, we can also get an impression of how gauge theory began in mathematics independently of its current incarnation in particle physics. Lie groups are the simplest curved spaces without the unnecessary restriction to two dimensions (there are no nonabelian 2-dimensional Lie groups), and their quotients offer alternative definitions of important topological spaces such as spheres, Grassmannians, Euclidean and Hyperbolic spaces. Continuing with Sternberg's explanation of the structure of Euclidean spaces, all of these 'symmetric spaces' and homogeneous spaces come with some naturally-equipped structures such as invariant 1-forms or metrics which are generalized to other compact Lie groups and used to give the most concrete constructions of curvature or other functions available in differential geometry. These spaces then became the starting point for more general bundle theory, as they are also equipped with natural bundles. Unlike these spaces, curvature in GR is not generally uniform and dynamically varies with the matter content of space-time. As such, Gauge theory is also equipped with the language to describe more general curvatures on manifolds.
+Kobayashi & Nomizu's book series is like a sequel to Sternberg's lectures in that its focus is on the definitions of geometric structures rather than algebraic invariants, and begins on connection theory where Sternberg's book ends. It also describes characteristic classes in an alternate way, via the Chern-Weil homomorphism with its starting point being curvature and connections rather than abstract algebraic invariants (since Milnor only references the curvature story in his appendix). Here, we can also get an impression of how gauge theory began in mathematics independently of its current incarnation in particle physics with Ehresmann, Weyl, and Cartan. Lie groups are the simplest curved spaces without the unnecessary restriction to two dimensions (there are no nonabelian 2-dimensional Lie groups), and their quotients offer alternative definitions of important topological spaces such as spheres, Grassmannians, Euclidean and Hyperbolic spaces. Continuing with Sternberg's explanation of the structure of Euclidean spaces, all of these 'symmetric spaces' and homogeneous spaces come with some naturally-equipped structures such as invariant 1-forms or metrics which are generalized to other compact Lie groups and used to give the most concrete constructions of curvature or other functions available in differential geometry. These spaces then became the starting point for more general bundle theory, as they are also equipped with natural bundles. Unlike these spaces, curvature in GR is not generally uniform and dynamically varies with the matter content of space-time. As such, Gauge theory is also equipped with the language to describe more general curvatures on manifolds.
 Spin geometry specializes back to Riemannian geometry.