David Roberts scratch 2021

Here are some thoughts by Urs Schreiber


Let me lay out the picture that I have at the moment, also so that you see where you fit in:


Hypothesis H, full quantum version:

For

  • a GG-orbi ℝ 10,1|32\mathbb{R}^{10,1\vert \mathbf{32}}-fold 𝒳\mathcal{X} (spacetime)

  • with geometric torsion-free Spin(10,1)\mathrm{Spin}(10,1)-structure (i.e. field of super-gravity)

  • further lifted to tangential Sp(2)\mathrm{Sp}(2)-structure τ\tau (anomaly cancellation),

  • consider the cocycle space π G τ(𝒳)\mathbf{\pi}_G^\tau(\mathcal{X}) of τ\tau-twisted equivariant differential 4-Cohomotopy (i.e. the C-field configuration G-space)

  • and then the GG-equivariant EE-cohomology cocycle space of its loop space E G •(Ωπ G τ(𝒳))\mathbf{E}^\bullet_G\big( \Omega \mathbf{\pi}_G^\tau(\mathcal{X}) \big) (quantum states)

  • regarded as a GG-equivariant spectrum (e.g. with E=HℂE = H\mathbb{C} and 𝒳\mathcal{X} a D6⊥D8D6 \perp D8 spacetime as in SS19 this has homotopy groups the weight systems on horizontal chord diagrams)

Unwinding the definitions, this QFT encodes

  • quantum operations between quantum states of C-field configurations

  • associated with HH-fixed loci of the original spacetime orbifold 𝒳\mathcal{X}.

  • But since these loci are conical black brane loci (as in HSS 18) in the spacetime,

  • we see that we have a “classically controlled quantum system” where the classical control parameter says where in a holographic system we are:

    • in the bulk (11-fixed locus)

    • or on a brane (HH-fixed locus)

      • and if so on which of possibly several intersecting ones (choice of subgroup H⊂GH \subset G).

Now take this mathematical picture and compare to the current folklore in string theory. Within the large hand-waving error bars of the latter, this could match well, I think.

Created on May 14, 2021 at 10:04:37. See the history of this page for a list of all contributions to it.