A method is proposed to measure the photon polarisation parameter $$\lambda _{\gamma }$$ in $${{b}} \!\rightarrow {s} {\gamma } $$ transitions using an amplitude analysis of $$B\!\rightarrow K\pi \pi {\gamma } $$ decays. Simplified models of the $${K} {\pi } {\pi } $$ system are used to simulate $${{{B} ^+}} \!\rightarrow {{K} ^+} {{\pi } ^-} {{\pi } ^+} {\gamma } $$ and $${{B} ^0} \!\rightarrow {{K} ^+} {{\pi } ^-} {{\pi } ^0} {\gamma } $$ decays, validate the amplitude analysis method, and demonstrate the feasibility of a measurement of the $$\lambda _{\gamma }$$ parameter irrespective of the model parameters. Similar sensitivities to $$\lambda _{\gamma }$$ are obtained with both the charged and neutral hadronic systems. In the absence of any background and distortion due to experimental effects, the statistical uncertainty expected from an analysis of $${{{B} ^+}} \!\rightarrow {{K} ^+} {{\pi } ^-} {{\pi } ^+} {\gamma } $$ decays in an LHCb data set corresponding to an integrated luminosity of 9 $$\,\hbox {fb}^{-1}$$ is estimated to be 0.009. A similar measurement using $${{B} ^0} \!\rightarrow {{K} ^+} {{\pi } ^-} {{\pi } ^0} {\gamma } $$ decays in a Belle II data sample corresponding to an integrated luminosity of 5 $$\hbox {\,ab}^{-1}$$ would lead to a statistical uncertainty of 0.018.
{ "_oai": { "updated": "2019-08-27T03:43:49Z", "id": "oai:repo.scoap3.org:48763", "sets": [ "EPJC" ] }, "authors": [ { "affiliations": [ { "country": "Switzerland", "value": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), Lausanne, Switzerland", "organization": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL)" } ], "surname": "Bell\u00e9e", "email": "violaine.bellee@epfl.ch", "full_name": "Bell\u00e9e, V.", "given_names": "V." }, { "affiliations": [ { "country": "Switzerland", "value": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), Lausanne, Switzerland", "organization": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL)" } ], "surname": "Pais", "email": "preema.pais@epfl.ch", "full_name": "Pais, P.", "given_names": "P." }, { "affiliations": [ { "country": "Switzerland", "value": "Physik-Institut, Universit\u00e4t Z\u00fcrich, Z\u00fcrich, Switzerland", "organization": "Universit\u00e4t Z\u00fcrich" } ], "surname": "Puig Navarro", "email": "albert.puig@cern.ch", "full_name": "Puig Navarro, A.", "given_names": "A." }, { "affiliations": [ { "country": "Switzerland", "value": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), Lausanne, Switzerland", "organization": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL)" } ], "surname": "Blanc", "email": "fred.blanc@epfl.ch", "full_name": "Blanc, F.", "given_names": "F." }, { "affiliations": [ { "country": "Switzerland", "value": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), Lausanne, Switzerland", "organization": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL)" } ], "surname": "Schneider", "email": "olivier.schneider@epfl.ch", "full_name": "Schneider, O.", "given_names": "O." }, { "affiliations": [ { "country": "France", "value": "LAL, Univ. Paris-Sud, CNRS/IN2P3, Universit\u00e9 Paris-Saclay, Orsay, France", "organization": "Universit\u00e9 Paris-Saclay" } ], "surname": "Trabelsi", "email": "trabelsi@lal.in2p3.fr", "full_name": "Trabelsi, K.", "given_names": "K." }, { "affiliations": [ { "country": "Switzerland", "value": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL), Lausanne, Switzerland", "organization": "Institute of Physics, \u00c9cole Polytechnique F\u00e9d\u00e9rale de Lausanne (EPFL)" } ], "surname": "Veneziano", "email": "giovanni.veneziano@alumni.epfl.ch", "full_name": "Veneziano, G.", "given_names": "G." } ], "titles": [ { "source": "Springer", "title": "Using an amplitude analysis to measure the photon polarisation in $$B \\rightarrow K\\pi \\pi \\gamma $$ <math><mrow><mi>B</mi><mo>\u2192</mo><mi>K</mi><mi>\u03c0</mi><mi>\u03c0</mi><mi>\u03b3</mi></mrow></math> decays" } ], "dois": [ { "value": "10.1140/epjc/s10052-019-7127-3" } ], "publication_info": [ { "page_end": "15", "journal_title": "European Physical Journal C", "material": "article", "journal_volume": "79", "artid": "s10052-019-7127-3", "year": 2019, "page_start": "1", "journal_issue": "7" } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "acquisition_source": { "date": "2019-08-27T05:34:07.585234", "source": "Springer", "method": "Springer", "submission_number": "f317b6b0c87a11e9be7702163e01809a" }, "page_nr": [ 15 ], "license": [ { "url": "https://creativecommons.org/licenses//by/4.0", "license": "CC-BY-4.0" } ], "copyright": [ { "holder": "The Author(s)", "year": "2019" } ], "control_number": "48763", "record_creation_date": "2019-07-25T17:30:27.760867", "_files": [ { "checksum": "md5:5401637bfd7614a75cb469adc888e728", "filetype": "xml", "bucket": "c3bdbcc1-f6f1-416e-915f-7ac6eb854119", "version_id": "f0131536-5af8-40e2-8194-bd48ac643f62", "key": "10.1140/epjc/s10052-019-7127-3.xml", "size": 26982 }, { "checksum": "md5:22cb423b4df6b6720b4d7468549ac04c", "filetype": "pdf/a", "bucket": "c3bdbcc1-f6f1-416e-915f-7ac6eb854119", "version_id": "e282e58a-3344-4e74-850f-46000c993438", "key": "10.1140/epjc/s10052-019-7127-3_a.pdf", "size": 996053 } ], "collections": [ { "primary": "European Physical Journal C" } ], "abstracts": [ { "source": "Springer", "value": "A method is proposed to measure the photon polarisation parameter $$\\lambda _{\\gamma }$$ <math><msub><mi>\u03bb</mi><mi>\u03b3</mi></msub></math> in $${{b}} \\!\\rightarrow {s} {\\gamma } $$ <math><mrow><mi>b</mi><mspace width=\"-0.166667em\"></mspace><mo>\u2192</mo><mi>s</mi><mi>\u03b3</mi></mrow></math> transitions using an amplitude analysis of $$B\\!\\rightarrow K\\pi \\pi {\\gamma } $$ <math><mrow><mi>B</mi><mspace width=\"-0.166667em\"></mspace><mo>\u2192</mo><mi>K</mi><mi>\u03c0</mi><mi>\u03c0</mi><mi>\u03b3</mi></mrow></math> decays. Simplified models of the $${K} {\\pi } {\\pi } $$ <math><mrow><mi>K</mi><mi>\u03c0</mi><mi>\u03c0</mi></mrow></math> system are used to simulate $${{{B} ^+}} \\!\\rightarrow {{K} ^+} {{\\pi } ^-} {{\\pi } ^+} {\\gamma } $$ <math><mrow><msup><mrow><mi>B</mi></mrow><mo>+</mo></msup><mspace width=\"-0.166667em\"></mspace><mo>\u2192</mo><msup><mrow><mi>K</mi></mrow><mo>+</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mo>-</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mo>+</mo></msup><mi>\u03b3</mi></mrow></math> and $${{B} ^0} \\!\\rightarrow {{K} ^+} {{\\pi } ^-} {{\\pi } ^0} {\\gamma } $$ <math><mrow><msup><mrow><mi>B</mi></mrow><mn>0</mn></msup><mspace width=\"-0.166667em\"></mspace><mo>\u2192</mo><msup><mrow><mi>K</mi></mrow><mo>+</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mo>-</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mn>0</mn></msup><mi>\u03b3</mi></mrow></math> decays, validate the amplitude analysis method, and demonstrate the feasibility of a measurement of the $$\\lambda _{\\gamma }$$ <math><msub><mi>\u03bb</mi><mi>\u03b3</mi></msub></math> parameter irrespective of the model parameters. Similar sensitivities to $$\\lambda _{\\gamma }$$ <math><msub><mi>\u03bb</mi><mi>\u03b3</mi></msub></math> are obtained with both the charged and neutral hadronic systems. In the absence of any background and distortion due to experimental effects, the statistical uncertainty expected from an analysis of $${{{B} ^+}} \\!\\rightarrow {{K} ^+} {{\\pi } ^-} {{\\pi } ^+} {\\gamma } $$ <math><mrow><msup><mrow><mi>B</mi></mrow><mo>+</mo></msup><mspace width=\"-0.166667em\"></mspace><mo>\u2192</mo><msup><mrow><mi>K</mi></mrow><mo>+</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mo>-</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mo>+</mo></msup><mi>\u03b3</mi></mrow></math> decays in an LHCb data set corresponding to an integrated luminosity of 9 $$\\,\\hbox {fb}^{-1}$$ <math><mrow><mspace width=\"0.166667em\"></mspace><msup><mtext>fb</mtext><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> is estimated to be 0.009. A similar measurement using $${{B} ^0} \\!\\rightarrow {{K} ^+} {{\\pi } ^-} {{\\pi } ^0} {\\gamma } $$ <math><mrow><msup><mrow><mi>B</mi></mrow><mn>0</mn></msup><mspace width=\"-0.166667em\"></mspace><mo>\u2192</mo><msup><mrow><mi>K</mi></mrow><mo>+</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mo>-</mo></msup><msup><mrow><mi>\u03c0</mi></mrow><mn>0</mn></msup><mi>\u03b3</mi></mrow></math> decays in a Belle II data sample corresponding to an integrated luminosity of 5 $$\\hbox {\\,ab}^{-1}$$ <math><mrow><mspace width=\"0.166667em\"></mspace><msup><mtext>ab</mtext><mrow><mo>-</mo><mn>1</mn></mrow></msup></mrow></math> would lead to a statistical uncertainty of 0.018." } ], "imprints": [ { "date": "2019-08-26", "publisher": "Springer" } ] }