0000000001309325

AUTHOR

Dipankar Das

showing 8 related works from this author

S3 symmetry and the quark mixing matrix

2016

We impose an $S_3$ symmetry on the quark fields under which two of three quarks transform like a doublet and the remaining one as singlet, and use a scalar sector with the same structure of $SU(2)$ doublets. After gauge symmetry breaking, a $\mathbb{Z}_2$ subgroup of the $S_3$ remains unbroken. We show that this unbroken subgroup can explain the approximate block structure of the CKM matrix. By allowing soft breaking of the $S_3$ symmetry in the scalar sector, we show that one can generate the small elements, of quadratic or higher order in the Wolfenstein parametrization of the CKM matrix. We also predict the existence of exotic new scalars, with unconventional decay properties, which can …

QuarkPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixSpontaneous symmetry breakingScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciences01 natural scienceslcsh:QC1-999High Energy Physics - PhenomenologyExplicit symmetry breakingHigh Energy Physics - Phenomenology (hep-ph)Quadratic equation0103 physical sciencesHigh Energy Physics::ExperimentSinglet state010306 general physicslcsh:PhysicsGauge symmetryPhysics Letters B
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Updated scalar sector constraints in the Higgs triplet model

2016

We show that in the Higgs triplet model, after the Higgs discovery, the mixing angle in the CP-even sector can be strongly constrained from unitarity. We also discuss how large quantum effects in $h\to\gamma\gamma$ may arise in a SM-like scenario and a certain part of the parameter space can be ruled out from the diphoton signal strength. Using $T$-parameter and diphoton signal strength measurements, we update the bounds on the nonstandard scalar masses.

PhysicsParticle physicsUnitarity010308 nuclear & particles physicsScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Signal strength0103 physical sciencesHiggs boson010306 general physicsMixing (physics)
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A model of neutrino mass and dark matter with large neutrinoless double beta decay

2017

We propose a model where neutrino masses are generated at three loop order but neutrinoless double beta decay occurs at one loop. Thus we can have large neutrinoless double beta decay observable in the future experiments even when the neutrino masses are very small. The model receives strong constraints from the neutrino data and lepton flavor violating decays, which substantially reduces the number of free parameters. Our model also opens up the possibility of having several new scalars below the TeV regime, which can be explored at the collider experiments. Additionally, our model also has an unbroken $Z_2$ symmetry which allows us to identify a viable Dark Matter candidate.

Nuclear and High Energy PhysicsParticle physicsHiggs PhysicsDark matterFOS: Physical sciences01 natural scienceslaw.inventionHigh Energy Physics - Phenomenology (hep-ph)lawDouble beta decay0103 physical sciencesNeutrino Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity010306 general physicsColliderPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísicaObservableSymmetry (physics)High Energy Physics - PhenomenologyBeyond Standard Modellcsh:QC770-798High Energy Physics::ExperimentNeutrinoLeptonFree parameterJournal of High Energy Physics
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Effective theories of flavor and the nonuniversal MSSM

2016

Flavor symmetries \`{a} la Froggatt-Nielsen~(FN) provide a compelling way to explain the hierarchies of fermionic masses and mixing angles in the Yukawa sector. In Supersymmetric~(SUSY) extensions of the Standard Model where the mediation of SUSY breaking occurs at scales larger than the breaking of flavor, this symmetry must be respected not only by the Yukawas of the superpotential, but by the soft-breaking masses and trilinear terms as well. In this work we show that contrary to naive expectations, even starting with completely flavor blind soft-breaking in the full theory at high scales, the low-energy sfermion mass matrices and trilinear terms of the effective theory, obtained upon int…

PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologySuperpotentialYukawa potentialFOS: Physical sciencesSupersymmetry01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Sfermion0103 physical sciencesEffective field theoryHigh Energy Physics::Experiment010306 general physicsPhenomenology (particle physics)Minimal Supersymmetric Standard ModelPhysical Review D
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Synthesis and Structure of Trimethylplatinum(IV) Iodide Complex of 4'-(4-Methoxyphenyl)-2,2':6',2''-terpyridine Ligand and its Halogen Bonding Proper…

2020

Inorganic Chemistrychemistry.chemical_classificationNMR spectra databasechemistry.chemical_compoundHalogen bondchemistryChemical bondLigandIodideX-ray crystallographyPolymer chemistryMoleculeTerpyridineZeitschrift für anorganische und allgemeine Chemie
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Can measurements of 2HDM parameters provide hints for high scale supersymmetry?

2018

Two-Higgs-doublet models (2HDMs) are minimal extensions of the Standard Model (SM) that may still be discovered at the LHC. The quartic couplings of their potentials can be determined from the measurement of the masses and branching ratios of their extended scalar sectors. We show that the evolution of these couplings through renormalization group equations can determine whether the observed 2HDM is a low energy manifestation of a more fundamental theory, as for instance, supersymmetry, which fixes the quartic couplings in terms of the gauge couplings. At leading order, the minimal supersymmetric extension of the SM (MSSM) dictates all the quartic couplings, which can be translated into a p…

PhysicsLarge Hadron ColliderSupersymmetry breaking scale010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetryRenormalization group01 natural sciencesPartícules (Física nuclear)Theoretical physicsHigh Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)Quartic function0103 physical sciencesCamps Teoria quàntica de010306 general physicsMinimal Supersymmetric Standard Model
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CCDC 1947525: Experimental Crystal Structure Determination

2020

Related Article: Dipankar Das, Sourav Sutradhar, Kari Rissanen, Biswa Nath Ghosh|2020|Z.Anorg.Allg.Chem.|646|301|doi:10.1002/zaac.201900201

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parametershemikis(iodo-(4'-(4-methoxyphenyl)-22':6'2''-terpyridine)-trimethyl-platinum) hemikis(chloro-iodo-(4'-(4-methoxyphenyl)-22':6'2''-terpyridine)-dimethyl-platinum) 1245-tetrafluoro-36-diiodobenzeneExperimental 3D Coordinates
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CCDC 1947524: Experimental Crystal Structure Determination

2020

Related Article: Dipankar Das, Sourav Sutradhar, Kari Rissanen, Biswa Nath Ghosh|2020|Z.Anorg.Allg.Chem.|646|301|doi:10.1002/zaac.201900201

Space GroupCrystallographyCrystal SystemCrystal StructureCell Parametersiodo-(4'-(4-methoxyphenyl)-22':6'2''-terpyridine)-trimethyl-platinumExperimental 3D Coordinates
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