{ "id": "1501.02506", "version": "v1", "published": "2015-01-11T22:57:52.000Z", "updated": "2015-01-11T22:57:52.000Z", "title": "Special-case closed form of the Baker-Campbell-Hausdorff formula", "authors": [ "Alexander Van-Brunt", "Matt Visser" ], "comment": "5 pages", "categories": [ "math-ph", "math.MP", "quant-ph" ], "abstract": "The Baker-Campbell-Hausdorff formula is a general result for the quantity $Z(X,Y)=\\ln( e^X e^Y )$, where $X$ and $Y$ are not necessarily commuting. For completely general commutation relations between $X$ and $Y$, (the free Lie algebra), the general result is somewhat unwieldy. However in specific physics applications the commutator $[X,Y]$, while non-zero, might often be relatively simple, which sometimes leads to explicit closed form results. We consider the special case $[X,Y] = u X + vY + cI$, and show that in this case the general result reduces to \\[ Z(X,Y)=\\ln( e^X e^Y ) = X+Y+ f(u,v) \\; [X,Y]. \\] Furthermore we explicitly evaluate the symmetric function $f(u,v)=f(v,u)$, demonstrating that \\[ f(u,v) = {(u-v)e^{u+v}-(ue^u-ve^v)\\over u v (e^u - e^v)}, \\] and relate this to previously known results. For instance this result includes, but is considerably more general than, results obtained from either the Heisenberg commutator $[P,Q]=-i\\hbar I$ or the creation-destruction commutator $[a,a^\\dagger]=I$.", "revisions": [ { "version": "v1", "updated": "2015-01-11T22:57:52.000Z" } ], "analyses": { "keywords": [ "special-case closed form", "baker-campbell-hausdorff formula", "general result reduces", "explicit closed form results", "general commutation relations" ], "publication": { "doi": "10.1088/1751-8113/48/22/225207", "journal": "Journal of Physics A Mathematical General", "year": 2015, "month": "Jun", "volume": 48, "number": 22, "pages": 225207 }, "note": { "typesetting": "TeX", "pages": 5, "language": "en", "license": "arXiv", "status": "editable", "inspire": 1340118, "adsabs": "2015JPhA...48v5207V" } } }