Dynamics of Cayley Forms
Autor: | Krasnov, Kirill |
---|---|
Rok vydání: | 2024 |
Předmět: | |
Druh dokumentu: | Working Paper |
Popis: | The most natural first-order PDE's to be imposed on a Cayley 4-form in eight dimensions is the condition that it is closed. As is known, this implies integrability of the Spin(7) structure defined by the Cayley form, as well as Ricci-flatness of the associated metric. We address the question as to what the most natural second-order in derivatives set of conditions is. We start by constructing the most general diffeomorphism invariant second order in derivatives Lagrangian that is quadratic in the perturbations of the Cayley form. We find that there is a one-parameter family of such Lagrangians. We then describe a non-linear completion of the linear story. To this end, we parametrise the intrinsic torsion of a Spin(7) structure by a 3-form, and show that this 3-form is completely determined by the exterior derivative of the Cayley form. We construct an action functional, which depends on the Cayley 4-form and and auxiliary 3-form as independent variables. There is a unique functional whose Euler-Lagrange equation for the auxiliary 3-form states that it is equal to the torsion 3-form. There is, however, a more general one-parameter family of functionals that can be constructed, and we show how the linearisation of these functionals reproduces the linear story. For any member of our family of theories, the Euler-Lagrange equations are written only using the operator of exterior differentiation of forms, and do not require the knowledge of the metric-compatible Levi-Civita connection. Geometrically, there is a preferred member in the family of Lagrangians, and we propose that its Euler-Lagrange equations are the most natural second-order equations to be satisfied by Cayley forms. Our construction also leads to a natural geometric flow in the space of Cayley forms, defined as the gradient flow of our action functional. Comment: 25 pages, no figures |
Databáze: | arXiv |
Externí odkaz: |