{ "id": "2211.13284", "version": "v1", "published": "2022-11-23T20:06:47.000Z", "updated": "2022-11-23T20:06:47.000Z", "title": "Fuzzy hyperspheres via confining potentials and energy cutoffs", "authors": [ "Gaetano Fiore" ], "comment": "Latex file, 40 pages, 3 figures", "categories": [ "math-ph", "hep-th", "math.MP" ], "abstract": "We simplify and complete the construction of fully $O(D)$-equivariant fuzzy spheres $S^d_\\Lambda$, for all dimensions $d\\equiv D-1$, initiated in [G. Fiore, F. Pisacane, J. Geom. Phys. 132 (2018), 423-451]. This is based on imposing a suitable energy cutoff on a quantum particle in $\\mathbb{R}^D$ subject to a confining potential well $V(r)$ with a very sharp minimum on the sphere of radius $r=1$; the cutoff and the depth of the well diverge with $\\Lambda\\in\\mathbb{N}$. We show that the irreducible representation ${{\\bf\\pi}}_\\Lambda$ of $O(D\\!+\\!1)$ on the space of harmonic homogeneous polynomials of degree $\\Lambda$ in the Cartesian coordinates of $\\mathbb{R}^{D+1}$ (which we express via trace-free completely symmetric projections) is isomorphic to the Hilbert space $\\mathcal{H}_{\\Lambda}$ of the particle, as a reducible representation of $O(D)\\subset O(D\\!+\\!1)$. Moreover, we show that the algebra of observables is isomorphic to ${{\\bf\\pi}}_\\Lambda\\left(Uso(D\\!+\\!1)\\right)$. As $\\Lambda$ diverges (commutative limit) so does the dimension of $\\mathcal{H}_{\\Lambda}$, and we recover ordinary quantum mechanics on the sphere $S^d$; more formally, we have a fuzzy quantization of a coadjoint orbit of $O(D\\!+\\!1)$ that goes to the classical phase space $T^*S^d$.", "revisions": [ { "version": "v1", "updated": "2022-11-23T20:06:47.000Z" } ], "analyses": { "subjects": [ "81R60", "22C05", "22D10", "22E46", "33C55" ], "keywords": [ "confining potential", "fuzzy hyperspheres", "ordinary quantum mechanics", "equivariant fuzzy spheres", "hilbert space" ], "note": { "typesetting": "LaTeX", "pages": 40, "language": "en", "license": "arXiv", "status": "editable" } } }