{ "id": "1011.0524", "version": "v1", "published": "2010-11-02T06:53:56.000Z", "updated": "2010-11-02T06:53:56.000Z", "title": "From Quantum Mechanics to Quantum Field Theory: The Hopf route", "authors": [ "Allan I. Solomon", "Gérard Henry Edmond Duchamp", "Pawel Blasiak", "Andrzej Horzela", "Karol A. Penson" ], "journal": "J.Phys.Conf.Ser.284:012055,2011", "doi": "10.1088/1742-6596/284/1/012055", "categories": [ "math-ph", "math.CO", "math.MP" ], "abstract": "We show that the combinatorial numbers known as {\\em Bell numbers} are generic in quantum physics. This is because they arise in the procedure known as {\\em Normal ordering} of bosons, a procedure which is involved in the evaluation of quantum functions such as the canonical partition function of quantum statistical physics, {\\it inter alia}. In fact, we shall show that an evaluation of the non-interacting partition function for a single boson system is identical to integrating the {\\em exponential generating function} of the Bell numbers, which is a device for encapsulating a combinatorial sequence in a single function. We then introduce a remarkable equality, the Dobinski relation, and use it to indicate why renormalisation is necessary in even the simplest of perturbation expansions for a partition function. Finally we introduce a global algebraic description of this simple model, giving a Hopf algebra, which provides a starting point for extensions to more complex physical systems.", "revisions": [ { "version": "v1", "updated": "2010-11-02T06:53:56.000Z" } ], "analyses": { "keywords": [ "quantum field theory", "quantum mechanics", "hopf route", "partition function", "bell numbers" ], "tags": [ "journal article" ], "publication": { "journal": "Journal of Physics Conference Series", "year": 2011, "month": "Mar", "volume": 284, "number": 1, "pages": "012055" }, "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable", "inspire": 875498, "adsabs": "2011JPhCS.284a2055S" } } }