We investigate several phenomena related to FCNCs in the $$\text {3-3-1-1}$$ model. The sources of FCNCs at the tree-level from both the gauge and Higgs sectors are clarified. Experiments on the oscillation of mesons most stringently constrain the tree-level FCNCs. The lower bound on the new physics scale is imposed more tightly than in the previous, $$\text {M}_{\text {new}}>12 $$ TeV. Under this bound, the tree-level FCNCs make a negligible contribution to the $$\text {Br}(B_s \rightarrow \mu ^+ \mu ^-)$$ , $$\text {Br}(B \rightarrow K^{*} \mu ^+ \mu ^-)$$ and $$\text {Br}(B^{+}\rightarrow K^{+}\mu ^{+}\mu ^{-})$$ . The branching ratio of radiative decay $$b \rightarrow s \gamma $$ is enhanced by the ratio $$\frac{v}{u}$$ via diagrams with the charged Higgs mediation. In contrast, the charged currents of new gauge bosons significantly contribute to the decay process $$\mu \rightarrow e \gamma $$ .
{ "_oai": { "updated": "2021-10-14T00:34:57Z", "id": "oai:repo.scoap3.org:64626", "sets": [ "EPJC" ] }, "authors": [ { "affiliations": [ { "country": "Vietnam", "value": "Institute of Physics, VAST, 10 Dao Tan, Ba Dinh, Hanoi, Vietnam", "organization": "Institute of Physics, VAST" }, { "country": "Vietnam", "value": "Graduate University of Science and Technology, Vietnam Academy of Science and Technology, 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam", "organization": "Vietnam Academy of Science and Technology" } ], "surname": "Nguyen Tuan", "email": "ntdem@iop.vast.ac.vn", "full_name": "Nguyen Tuan, Duy", "given_names": "Duy" }, { "affiliations": [ { "country": "Vietnam", "value": "Institute of Physics, VAST, 10 Dao Tan, Ba Dinh, Hanoi, Vietnam", "organization": "Institute of Physics, VAST" }, { "country": "Japan", "value": "Theoretical Research Division, Nishina Center, RIKEN, Wako, 351-0198, Japan", "organization": "RIKEN" } ], "surname": "Inami", "given_names": "Takeo", "full_name": "Inami, Takeo" }, { "affiliations": [ { "country": "Vietnam", "value": "Institute of Physics, VAST, 10 Dao Tan, Ba Dinh, Hanoi, Vietnam", "organization": "Institute of Physics, VAST" } ], "surname": "Do Thi", "email": "dthuong@iop.vast.ac.vn", "full_name": "Do Thi, Huong", "given_names": "Huong" } ], "titles": [ { "source": "Springer", "title": "Physical constraints derived from FCNC in the 3-3-1-1 model" } ], "dois": [ { "value": "10.1140/epjc/s10052-021-09583-x" } ], "publication_info": [ { "page_end": "16", "journal_title": "European Physical Journal C", "material": "article", "journal_volume": "81", "artid": "s10052-021-09583-x", "year": 2021, "page_start": "1", "journal_issue": "9" } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "acquisition_source": { "date": "2021-10-14T00:31:07.249034", "source": "Springer", "method": "Springer", "submission_number": "ddb2cd522c8511ecbd5e2e123689e85f" }, "page_nr": [ 16 ], "license": [ { "url": "https://creativecommons.org/licenses//by/4.0", "license": "CC-BY-4.0" } ], "copyright": [ { "holder": "The Author(s)", "year": "2021" } ], "control_number": "64626", "record_creation_date": "2021-09-14T15:30:19.897335", "_files": [ { "checksum": "md5:5ddc3c7b13b74fa33723ce3cc5a9a1ef", "filetype": "xml", "bucket": "136cb6eb-2b17-491d-93f4-f38caeff751d", "version_id": "41991429-c312-45aa-b327-af87aadd2488", "key": "10.1140/epjc/s10052-021-09583-x.xml", "size": 19171 }, { "checksum": "md5:fafe258ba8891c979a6d1df08b22b2db", "filetype": "pdf/a", "bucket": "136cb6eb-2b17-491d-93f4-f38caeff751d", "version_id": "a689e693-1c1d-4d35-b0c0-777f5d8fd2f9", "key": "10.1140/epjc/s10052-021-09583-x_a.pdf", "size": 1250288 } ], "collections": [ { "primary": "European Physical Journal C" } ], "abstracts": [ { "source": "Springer", "value": "We investigate several phenomena related to FCNCs in the $$\\text {3-3-1-1}$$ <math> <mtext>3-3-1-1</mtext> </math> model. The sources of FCNCs at the tree-level from both the gauge and Higgs sectors are clarified. Experiments on the oscillation of mesons most stringently constrain the tree-level FCNCs. The lower bound on the new physics scale is imposed more tightly than in the previous, $$\\text {M}_{\\text {new}}>12 $$ <math> <mrow> <msub> <mtext>M</mtext> <mtext>new</mtext> </msub> <mo>></mo> <mn>12</mn> </mrow> </math> TeV. Under this bound, the tree-level FCNCs make a negligible contribution to the $$\\text {Br}(B_s \\rightarrow \\mu ^+ \\mu ^-)$$ <math> <mrow> <mtext>Br</mtext> <mo>(</mo> <msub> <mi>B</mi> <mi>s</mi> </msub> <mo>\u2192</mo> <msup> <mi>\u03bc</mi> <mo>+</mo> </msup> <msup> <mi>\u03bc</mi> <mo>-</mo> </msup> <mo>)</mo> </mrow> </math> , $$\\text {Br}(B \\rightarrow K^{*} \\mu ^+ \\mu ^-)$$ <math> <mrow> <mtext>Br</mtext> <mo>(</mo> <mi>B</mi> <mo>\u2192</mo> <msup> <mi>K</mi> <mrow> <mrow></mrow> <mo>\u2217</mo> </mrow> </msup> <msup> <mi>\u03bc</mi> <mo>+</mo> </msup> <msup> <mi>\u03bc</mi> <mo>-</mo> </msup> <mo>)</mo> </mrow> </math> and $$\\text {Br}(B^{+}\\rightarrow K^{+}\\mu ^{+}\\mu ^{-})$$ <math> <mrow> <mtext>Br</mtext> <mo>(</mo> <msup> <mi>B</mi> <mo>+</mo> </msup> <mo>\u2192</mo> <msup> <mi>K</mi> <mo>+</mo> </msup> <msup> <mi>\u03bc</mi> <mo>+</mo> </msup> <msup> <mi>\u03bc</mi> <mo>-</mo> </msup> <mo>)</mo> </mrow> </math> . The branching ratio of radiative decay $$b \\rightarrow s \\gamma $$ <math> <mrow> <mi>b</mi> <mo>\u2192</mo> <mi>s</mi> <mi>\u03b3</mi> </mrow> </math> is enhanced by the ratio $$\\frac{v}{u}$$ <math> <mfrac> <mi>v</mi> <mi>u</mi> </mfrac> </math> via diagrams with the charged Higgs mediation. In contrast, the charged currents of new gauge bosons significantly contribute to the decay process $$\\mu \\rightarrow e \\gamma $$ <math> <mrow> <mi>\u03bc</mi> <mo>\u2192</mo> <mi>e</mi> <mi>\u03b3</mi> </mrow> </math> ." } ], "imprints": [ { "date": "2021-09-14", "publisher": "Springer" } ] }