- Particle physics theoretical and experimental studies
- Dark Matter and Cosmic Phenomena
- Cosmology and Gravitation Theories
- Computational Physics and Python Applications
- Particle Detector Development and Performance
- Quantum Chromodynamics and Particle Interactions
- Black Holes and Theoretical Physics
- High-Energy Particle Collisions Research
- Distributed and Parallel Computing Systems
- Neutrino Physics Research
- Algorithms and Data Compression
- Astronomy and Astrophysical Research
University of Southampton
2023-2024
Rutherford Appleton Laboratory
2024
Cadi Ayyad University
2024
Nicolaus Copernicus Astronomical Center
2021-2023
Polish Academy of Sciences
2021-2023
Universidad Autónoma de Madrid
2019-2021
Consejo Superior de Investigaciones Científicas
2019-2020
Instituto de Física Teórica
2020
Instituto de Física de Cantabria
2019
Indian Association for the Cultivation of Science
2013-2016
A bstract The recent confirmation by the Fermilab-based Muon g-2 experiment of ( g − 2) μ anomaly has important implications for allowed particle spectra in softly broken supersymmetry (SUSY) models with neutralino dark matter (DM). Generally, DM to be quite light, mass up a few hundred GeV, and bino-dominated if it is provide most Universe. Otherwise, higgsino or wino dominated also but only as strongly subdominant component at percent total density. These general patterns can easily found...
Abstract The electroweak (EW) sector of the Minimal Supersymmetric Standard Model (MSSM), with lightest neutralino as Dark Matter (DM) candidate, can account for a variety experimental data. This includes DM content universe, direct detection limits, EW SUSY searches at LHC and in particular so far persistent $$3-4\,\sigma $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>3</mml:mn> <mml:mo>-</mml:mo> <mml:mn>4</mml:mn> <mml:mspace /> <mml:mi>σ</mml:mi>...
A bstract We suggest an explanation for and explore the consequences of excess around 95 GeV in di-photon di-tau invariant mass distributions recently reported by CMS collaboration at Large Hadron Collider (LHC), together with discrepancy that has long been observed Electron-Positron (LEP) collider $$ b\overline{b} <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>b</mml:mi> <mml:mover> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> mass. Interestingly, most recent findings...
Abstract The recent Fermilab muon $$g-2$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>g</mml:mi> <mml:mo>-</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:math> result and the same for electron due to fine-structure constant measurement through $${}^{133}\textrm{Cs}$$ <mml:msup> <mml:mrow /> <mml:mn>133</mml:mn> </mml:msup> <mml:mtext>Cs</mml:mtext> matter-wave interferometry are probed in relation MSSM with non-holomorphic (NH) trilinear soft SUSY breaking...
Using the chargino-neutralino and slepton search results from LHC in conjunction with WMAP/PLANCK (g − 2) μ data, we constrain several generic pMSSM models decoupled strongly interacting sparticles, heavier Higgs bosons characterized by different hierarchies among EW sparticles. We find that some of them are already under pressure this number increases if bounds direct detection experiments like LUX taken into account, keeping mind associated uncertainties. The XENON1T experiment is likely...
As a sequel to our earlier work on wino-dominated $\tilde \chi_1^{\pm}$ and \chi_2^{0}$ (wino models), we focus the pMSSM models where \chi_{2,3}^{0}$ are either higgsino dominated (higgsino models) or admixtures of significant amount wino components (mixed with without light sleptons. The LHC constraints in trilepton channel significantly weaker even presence sleptons, especially models, compared those mostly studied by collaborations \chi_2^{0}$. modes \chi_{2,3}^{0}\rightarrow...
Abstract The electroweak (EW) sector of the Minimal Supersymmetric Standard Model (MSSM) can account for a variety experimental data. In particular it explain persistent $$3-4\,\sigma $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>3</mml:mn> <mml:mo>-</mml:mo> <mml:mn>4</mml:mn> <mml:mspace /> <mml:mi>σ</mml:mi> </mml:mrow> </mml:math> discrepancy between result anomalous magnetic moment muon, $$(g-2)_\mu <mml:msub> <mml:mo>(</mml:mo> <mml:mi>g</mml:mi>...
Abstract The electroweak (EW) sector of the Minimal Supersymmetric Standard Model (MSSM) can account for a variety experimental data. EW particles with masses few hundred GeV evade LHC searches owing to their small production cross sections. Such light in particular explain reinforced $$4.2\,\sigma $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mn>4.2</mml:mn> <mml:mspace /> <mml:mi>σ</mml:mi> </mml:mrow> </mml:math> discrepancy between result anomalous magnetic...
Abstract Slepton coannihilation is one of the most promising scenarios that can bring predicted Dark Matter (DM) abundance in Minimal Supersymmetric Standard Model (MSSM) into agreement with experimental observation. In this scenario, lightest supersymmetric particle (LSP), usually assumed to be neutralino, $$\tilde{\chi }_{1}^0$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mover> <mml:mi>χ</mml:mi> <mml:mo>~</mml:mo> </mml:mover> <mml:mrow>...
Higgsinos and Wino have strong motivations for being Dark Matter (DM) candidates in supersymmetry, but their annihilation cross sections are quite large. For thermal generation a single component DM setup the higgsinos or wino may masses of around 1 2-3 TeV respectively. such candidates, small amount slepton coannihilation decrease effective section. This, turn reduces lower limit relic density satisfied mass by more than 50%. Almost similar degree reduction same is also seen squark...
Abstract The electroweak (EW) sector of the Minimal Supersymmetric extension Standard Model (MSSM), assuming lightest neutralino as Dark Matter (DM) candidate, can account for a variety experimental results. This includes DM direct detection limits, searches EW superpartners at LHC, and in particular discrepancy between result anomalous magnetic moment muon, $$(g-2)_\mu $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mrow> <mml:mo>(</mml:mo> <mml:mi>g</mml:mi>...
LHC searches for nonstandard scalars in vector boson fusion (VBF) production processes can be particularly efficient probing belonging to triplet or higher multiplet representations of the Standard Model $SU(2{)}_{L}$ gauge group. They especially relevant models where additional do not have any tree level couplings fermions, rendering VBF as their primary mode at LHC. In this work we employ latest data from resonance constrain properties scalars, taking Georgi-Machacek model a prototypical...
The CMS collaboration reported an intriguing \sim 3 sigma (local) excess at 96 GeV in the light Higgs-boson search diphoton decay mode. This mass coincides with a 2 bb final state LEP. We briefly review proposed combined interpretations for two excesses. In more detail we interpretation of this possible signal as lightest Higgs boson Doublet Model additional real singlet (N2HDM). show which channels have best prospects discovery bosons upcoming Run LHC.
A bstract In this paper we explore the possibility of explaining muon g − 2 anomaly in various types supersymmetric extensions Standard Model. particular, investigate and compare phenomenological constraints MSSM with stable neutralino other scenarios where is unstable. For latter case study Gauge Mediated SUSY Breaking (GMSB) scenario very light gravitino UDD -type R-Parity Violating (RPV) scenario. neutralino, parameter region favoured by ( 2) μ strongly constrained relic abundance dark...
We discuss both the minimal supersymmetric Standard Model (MSSM) and next to MSSM scenarios in which lightest Higgs boson with ${m}_{h}=98\text{ }\text{ }\mathrm{GeV}$ is consistent small excess ($\ensuremath{\sim}2.3\ensuremath{\sigma}$) observed at LEP ${e}^{+}{e}^{\ensuremath{-}}\ensuremath{\rightarrow}Zh$, $h\ensuremath{\rightarrow}b\overline{b}$ process heavier of mass close 125 GeV as candidate SM Higgs-like particle LHC. show allowed regions nondecoupling zone parameter space are...
The electroweak (EW) sector of the Minimal Supersymmetric Standard Model (MSSM) can account for a variety experimental data. lighest supersymmetric particle (LSP), which we take as lightest neutralino, $\tilde \chi_1^0$, observed Dark Matter (DM) content universe via coannihilation with next-to-LSP (NLSP), while being in agreement negative results from Direct Detection (DD) experiments. Owing to relatively small production cross-sections comparably light EW MSSM is also unsuccessful searches...
We discuss a $\sim 3\,\sigma$ signal (local) in the light Higgs-boson search diphoton decay mode at 96$ GeV as reported by CMS, together with 2\,\sigma$ excess $b \bar b$ final state LEP same mass range. interpret this possible Higgs boson 2 Doublet Model an additional real singlet (N2HDM). find that lightest of N2HDM can perfectly fit both excesses simultaneously, while second is full agreement measurements 125 GeV, and sector all exclusion bounds from LEP, Tevatron LHC well other...
The stringent constraints from the direct searches for exotic scalars at LHC as well indirect bounds flavor physics measurements have imposed severe restrictions on parameter space of new models featuring extended Higgs sectors. In Type-II 2HDM, this implies a lower bound charged masses $\cal O$(600 GeV). work we analyze phenomenology Z3HDM in alignment limit focusing impact its space. We show that couplings two bosons model feature an additional suppression factor compared to 2HDM. This...
We study two simple and well motivated nonuniversal gaugino mass models, which predict higgsino dark matter. One can account for the observed matter relic density along with Higgs boson of ~ 125 GeV over a large region parameter space each model, corresponding to 1 TeV. In case this covers gluino range 2-3 TeV, parts be probed by 14 TeV LHC experiments. these model predictions in brief detection experiments greater detail.
We revisit the issue of considering stochasticity Grassmannian coordinates in $N=1$ superspace, which was analyzed previously by Kobakhidze et al. In this stochastic supersymmetry (SUSY) framework, soft SUSY breaking terms minimal supersymmetric Standard Model (MSSM) such as bilinear Higgs mixing, trilinear coupling, well gaugino mass parameters are all proportional to a single parameter $\ensuremath{\xi}$, measure arising out stochasticity. While nonvanishing coupling at high scale is...
A bstract As a sequel to our recent paper we examine the phenomenology of full electroweakino sector pMSSM without invoking ad hoc but often employed assumption that heavier ones are decoupled. We showcase importance electroweakinos using several generic models with different hierarchies among slepton and masses. obtain constraints from LHC "Image missing"<!-- image only, no MathML or LaTex --> data which stronger than for decoupled electroweakinos. Using additional observed dark matter...
The recent results reported by the CMS collaboration, indicating "bumps" in $\gamma\gamma$ and $\tau\tau$ channels at $m_\phi\approx 95$ GeV, provide interesting hints for new physics. We find that lightest Higgs state of general 2HDM (2HDM Type-III) can perfectly simultaneously accommodate two excesses alongside with LEP long-standing anomaly observed $b\bar{b}$ channel while meeting all theoretical experimental requirements. Furthermore, study predicts an enhanced production process...
Abstract The quest for supersymmetric (SUSY) particles is among the main search channels currently pursued at LHC. Particularly, electroweak (EW) with masses as low a few hundred GeV are still viable. Recent searches “golden channel”, $$pp \rightarrow \tilde{\chi }_{2}^0 }_{1}^\pm }_{1}^0 Z^{(*)} \, W^{\pm (*)}$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mrow> <mml:mi>p</mml:mi> <mml:mo>→</mml:mo> <mml:msubsup> <mml:mover> <mml:mi>χ</mml:mi> <mml:mo>~</mml:mo>...