synthetic differential geometry
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from point-set topology to differentiable manifolds
geometry of physics: coordinate systems, smooth spaces, manifolds, smooth homotopy types, supergeometry
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(shape modality $\dashv$ flat modality $\dashv$ sharp modality)
$(ʃ \dashv \flat \dashv \sharp )$
dR-shape modality$\dashv$ dR-flat modality
$ʃ_{dR} \dashv \flat_{dR}$
(reduction modality $\dashv$ infinitesimal shape modality $\dashv$ infinitesimal flat modality)
$(\Re \dashv \Im \dashv \&)$
fermionic modality$\dashv$ bosonic modality $\dashv$ rheonomy modality
$(\rightrightarrows \dashv \rightsquigarrow \dashv Rh)$
Models
Models for Smooth Infinitesimal Analysis
smooth algebra ($C^\infty$-ring)
differential equations, variational calculus
Euler-Lagrange equation, de Donder-Weyl formalism?,
Chern-Weil theory, ∞-Chern-Weil theory
Cartan geometry (super, higher)
Ricci flow is the gradient flow of the action functional of dilaton gravity: the Einstein-Hilbert action coupled to a dilaton field.
Equivalently it is the renormalization group flow of the bosonic string sigma-model for background fields containing gravity and dilaton (reviewed e.g. in Woolgra 07, Carfora 10, see also the introduction of Tseytlin 06).
In (Perelman 02) Ricci flow for dilaton gravity in 3d was shown to enjoy sufficient monotonicity properties such as to complete Richard Hamilton‘s proof of the Poincaré conjecture. Hamilton’s strategy was to equip a compact simply connected 3d manifold with a Riemannian metric, argue that its Ricci flow will, after many “pinchings” (points where the metric degenerates) produce a collection of 3-spheres and conclude that therefor the original manifold must have been a 3-sphere, too. The technical problem is to control the number of pinchings, which may occur rapidly. Adding also the dilaton field turns out not to change the qualitative nature of the flow but make it “monotone enough” to control the pinching.
In Rubinstein-Sinclair a typical such Ricci flow with pinchings is visualized as follows:
A quick survey is in the slides
and a detailed survey is in
Visualization is in
The monotonicity of the Ricci flow for the string sigma-model in dilaton gravity background was established in
This was a key step in his completion of Hamilton’s program for how to prove the Poincare conjecture.
The identification of Ricci flow with the renormalization group flow of the bosonic string sigma-model is reviewed for instance in
Kasper Olsen, From Polyakov to Perelman
E. Woolgar, Some Applications of Ricci Flow in Physics, Can.J.Phys.86:645,2008 (arXiv:0708.2144)
Mauro Carfora, Renormalization Group and the Ricci flow (arXiv:1001.3595)
and discussed in more detail for instance in
T Oliynyk, V Suneeta, E Woolgar, Irreversibility of World-sheet Renormalization Group Flow, Phys.Lett. B610 (2005) 115-121 (arXiv:hep-th/0410001)
T Oliynyk, V Suneeta, E Woolgar, A Gradient Flow for Worldsheet Nonlinear Sigma Models, Nucl.Phys. B739 (2006) 441-458 (arXiv:hep-th/0510239)
Arkady Tseytlin, On sigma model RG flow, “central charge” action and Perelman’s entropy, Phys.Rev.D75:064024,2007 (arXiv:hep-th/0612296)
See also at string theory – References – Fields medal work related to string theory.
See also
Alexander Frenkel, Petr Horava, Stephen Randall, Topological Quantum Gravity of the Ricci Flow (arXiv:2010.15369)
Alexander Frenkel, Petr Horava, Stephen Randall, Perelman’s Ricci Flow in Topological Quantum Gravity (arXiv:2011.11914)
Last revised on November 25, 2020 at 09:07:16. See the history of this page for a list of all contributions to it.