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On the unification of Higgs-Nambu Goldstone boson in the formation of near-brane exotic scalar via Scherk-Shwarz breaking in 5-dimensional SU(6) symmetry
Zen F.P.a, Hartanto A.b, Kosasih J.S.a
a Indonesian Center for Theoretical and Mathematical Physics, Theoretical Physics Laboratory, THEPI Research Division, Institut Teknologi Bandung, Bandung, 40132, Indonesia
b Indonesian Center for Theoretical and Mathematical Physics, Indonesia
[vc_row][vc_column][vc_row_inner][vc_column_inner][vc_separator css=”.vc_custom_1624529070653{padding-top: 30px !important;padding-bottom: 30px !important;}”][/vc_column_inner][/vc_row_inner][vc_row_inner layout=”boxed”][vc_column_inner width=”3/4″ css=”.vc_custom_1624695412187{border-right-width: 1px !important;border-right-color: #dddddd !important;border-right-style: solid !important;border-radius: 1px !important;}”][vc_empty_space][megatron_heading title=”Abstract” size=”size-sm” text_align=”text-left”][vc_column_text]© 2014 F.P. Zen, A. Hartanto and J.S. Kosasih.The 5D Scherk-Schwarz breaking with orbifold S1/Z2 in SU(6) symmetry under special condition leads to a dimensional deconstruction without gauge symmetry breaking where SU(6) Little Higgs-like scalars show up either as weakly-coupled or strongly-coupled. The latest, together with the broken fifth component of 5D gauge boson, composes Coleman-Weinberg potential which can be generalized by substituting PNB (Pseudo Nambu-Goldstone boson) Higgs as the broken fifth component, with Nambu-Goldstone boson being the third component of a massive 4D gauge boson in electroweak theory. A doublevacua symmetry emerges, based on Baker-Campbell-Hausdorff approach, with its shift and twist breaking terms which facilitate the unification of Higgs-NGB to become exotic scalars named as Scherk-Schwarz scalars. Under unitary transformation the double-vacua shift symmetry breaks via twistedly-broken manner i.e. the NGB swallowing and digesting mode where the first consists of transferring 2 (two) degrees of freedom from 2 (two) NGBs without additional mass while the second with additional mass to PNB Higgs in the Higgs-NGB unification. The unification results in a free and bonded gauge-like single scalar which becomes the main components of exotic scalars such as 3-scalar Higgs, Higgs-like and gauge-like 3-component scalars. Ranges of masses for the exotic Higgs suit the latest LHC data with excluded zone 145 – 466 GeV while for the exotic 3-component scalars run continuously up to 1.5 TeV.[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Author keywords” size=”size-sm” text_align=”text-left”][vc_column_text][/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Indexed keywords” size=”size-sm” text_align=”text-left”][vc_column_text]Double vacua,Little Higgs,Nambu-Goldstone boson,Orbifold,Scherk-Schwarz breaking,Scherk-Schwarz scalar,Standard Model[/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”Funding details” size=”size-sm” text_align=”text-left”][vc_column_text][/vc_column_text][vc_empty_space][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][vc_empty_space][megatron_heading title=”DOI” size=”size-sm” text_align=”text-left”][vc_column_text]https://doi.org/10.12988/astp.2014.4112[/vc_column_text][/vc_column_inner][vc_column_inner width=”1/4″][vc_column_text]Widget Plumx[/vc_column_text][/vc_column_inner][/vc_row_inner][/vc_column][/vc_row][vc_row][vc_column][vc_separator css=”.vc_custom_1624528584150{padding-top: 25px !important;padding-bottom: 25px !important;}”][/vc_column][/vc_row]