{ "id": "hep-ph/0108096", "version": "v3", "published": "2001-08-10T13:47:49.000Z", "updated": "2002-03-05T19:52:13.000Z", "title": "Implications of Recent $\\bar{B}^0\\to D^{(*)0}X^0$ Measurements", "authors": [ "Hai-Yang Cheng" ], "comment": "17 pages. The Introduction is substantially revised and the order of the presentation in Sec. 2 is rearranged. To appear in Phys. Rev", "journal": "Phys.Rev. D65 (2002) 094012", "doi": "10.1103/PhysRevD.65.094012", "categories": [ "hep-ph", "hep-ex" ], "abstract": "The recent measurements of the color-suppressed modes $\\bar B^0\\to D^{(*)0}\\pi^0$ imply non-vanishing relative final-state interaction (FSI) phases among various $\\bar B\\to D\\pi$ decay amplitudes. Depending on whether or not FSIs are implemented in the topological quark-diagram amplitudes, two solutions for the parameters $a_1$ and $a_2$ are extracted from data using various form-factor models. It is found that $a_2$ is not universal: $|a_2(D\\pi)|= 0.40-0.55$ and $|a_2(D^*\\pi)|= 0.25-0.35$ with a relative phase of order $(50-55)^\\circ$ between $a_1$ and $a_2$. If FSIs are not included in quark-diagram amplitudes from the outset, $a_2^{eff}/a_1^{eff}$ and $a_2^{eff}$ will become smaller. The large value of $|a_2(D\\pi)|$ compared to $|a_2^{eff}(D\\pi)|$ or naive expectation implies the importance of long-distance FSI contributions to color-suppressed internal $W$-emission via final-state rescatterings of the color-allowed tree amplitude.", "revisions": [ { "version": "v3", "updated": "2002-03-05T19:52:13.000Z" } ], "analyses": { "subjects": [ "13.25.Hw", "13.25.-k" ], "keywords": [ "measurements", "implications", "long-distance fsi contributions", "decay amplitudes", "topological quark-diagram amplitudes" ], "tags": [ "journal article" ], "publication": { "publisher": "APS", "journal": "Phys. Rev. D" }, "note": { "typesetting": "TeX", "pages": 17, "language": "en", "license": "arXiv", "status": "editable", "inspire": 561385 } } }