Sumit Kumar Garg
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Sumit Kumar Garg has a total of 35 co-authors. Here are the top co-authors by number of shared publications:
- Poulose Poulose
St. Joseph’s University
5 shared publications - Arnab Kundu
A CI of Homi Bhabha National Institute
4 shared publications - Chethan Krishnan
Center for High Energy Physics Indian Institute of Science 560012 Bangalore India
4 shared publications - Suman Das
Theory Division Saha Institute of Nuclear Physics A CI of Homi Bhabha National Institute 1/AF 700064 Bidhannagar Kolkata India
4 shared publications - Nilendra G. Deshpande
University of Oregon
3 shared publications B. Ananthanarayan
Indian Inst Sci, Ctr High Energy Phys, Bangalore 560012, Karnataka, India
2 shared publications
Latest Publications
- Open Access
- 8 September 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (5) , 055007
Alternative left-right scenario: Unitarity, vacuum stability, and RG evolution
We study the theoretical constraints on the scalar sector of the alternative left-right model (ALRM), an E 6 -motivated extension of the Standard Model based on the gauge group S U ( 3 ) c ⊗ S U ( 2 ) L ⊗ S U ( 2 ) R ′ ⊗ U ( 1 ) B − L , supplemented by a global U ( 1 ) S symmetry. We derive the complete set of tree-level perturbative unitarity constraints on the model, resulting in 14 independent conditions on the quartic scalar couplings. When combined with the boundedness-from-below conditions and the requirement of positive-definite scalar mass-squared eigenvalues, this yields significantly more stringent restrictions on the parameter space than either set alone. We then perform a one-loop renormalization group analysis, evolving the model parameters up to a high-energy cutoff scale, and requiring that the vacuum stability, the unitarity, and the perturbativity conditions are preserved throughout. The renormalization group evolution is found to restrict the allowed parameter space considerably beyond the tree-level bounds, with the constraints on the quartic couplings becoming more stringent as the cutoff scale is raised. Consequently, the physical scalar masses in the model acquire upper bounds. For the right-hand symmetry breaking scale, v R = 10 TeV and requiring theoretical consistency up to 10 16 GeV , we obtain m H 1 ± ≲ 6.5 TeV , m H 2 ± ≲ 1.5 TeV , and m H 1 0 ≃ m A 1 ≲ 1.5 TeV , with all bounds scaling with v R . These findings offer a predictive and falsifiable framework for searches of the extended Higgs sector of the ALRM at the current and future collider experiments.
- 8 September 2026
- Published by American Physical Society (APS) in Physical Review D
- Vol. 114 (5) , 055007
Open AccessAlternative left-right scenario: Unitarity, vacuum stability, and RG evolution
We study the theoretical constraints on the scalar sector of the alternative left-right model (ALRM), an E 6 -motivated extension of the Standard Model based on the gauge group S U ( 3 ) c ⊗ S U ( 2 ) L ⊗ S U ( 2 ) R ′ ⊗ U ( 1 ) B − L , supplemented by a global U ( 1 ) S symmetry. We derive the complete set of tree-level perturbative unitarity constraints on the model, resulting in 14 independent conditions on the quartic scalar couplings. When combined with the boundedness-from-below conditions and the requirement of positive-definite scalar mass-squared eigenvalues, this yields significantly more stringent restrictions on the parameter space than either set alone. We then perform a one-loop renormalization group analysis, evolving the model parameters up to a high-energy cutoff scale, and requiring that the vacuum stability, the unitarity, and the perturbativity conditions are preserved throughout. The renormalization group evolution is found to restrict the allowed parameter space considerably beyond the tree-level bounds, with the constraints on the quartic couplings becoming more stringent as the cutoff scale is raised. Consequently, the physical scalar masses in the model acquire upper bounds. For the right-hand symmetry breaking scale, v R = 10 TeV and requiring theoretical consistency up to 10 16 GeV , we obtain m H 1 ± ≲ 6.5 TeV , m H 2 ± ≲ 1.5 TeV , and m H 1 0 ≃ m A 1 ≲ 1.5 TeV , with all bounds scaling with v R . These findings offer a predictive and falsifiable framework for searches of the extended Higgs sector of the ALRM at the current and future collider experiments.
- Open Access
- 2 February 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (2) , 21
Deep learning approaches to top FCNC couplings to photons at the LHC
A bstract: We investigate the sensitivity of the LHC to flavour-changing neutral current interactions involving the top quark and a photon using a model-independent effective field theory framework, focusing on two complementary processes: single top production via qg → tγ and the rare decay t → qγ in top pair events. To enhance signal discrimination, we employ a range of deep learning classifiers, including multi-layer perceptrons, graph attention networks and transformers, and compare them against a traditional cut-based analysis. Our results demonstrate that attention-based architectures, in particular transformer networks, significantly outperform other strategies, yielding up to a factor of five improvement in the expected exclusion limits. In particular, we show that at the high-luminosity LHC, rare top branching ratios can be probed down to values as low as 10 − 6 . Our results thus highlight the significant potential of attention-based architectures for improving the sensitivity to new physics signatures in top quark processes at colliders.
- 2 February 2026
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2026 (2) , 21
Open AccessDeep learning approaches to top FCNC couplings to photons at the LHC
A bstract: We investigate the sensitivity of the LHC to flavour-changing neutral current interactions involving the top quark and a photon using a model-independent effective field theory framework, focusing on two complementary processes: single top production via qg → tγ and the rare decay t → qγ in top pair events. To enhance signal discrimination, we employ a range of deep learning classifiers, including multi-layer perceptrons, graph attention networks and transformers, and compare them against a traditional cut-based analysis. Our results demonstrate that attention-based architectures, in particular transformer networks, significantly outperform other strategies, yielding up to a factor of five improvement in the expected exclusion limits. In particular, we show that at the high-luminosity LHC, rare top branching ratios can be probed down to values as low as 10 − 6 . Our results thus highlight the significant potential of attention-based architectures for improving the sensitivity to new physics signatures in top quark processes at colliders.
- Open Access
- 9 May 2025
- Published by American Physical Society (APS) in Physical Review D
- Vol. 111 (9)
Leptonic probes of alternative left-right symmetric models
We explore constraints on the parameter space of the alternative left-right model originating from the leptonic sector. Our analyses focuses on both lepton-flavor-conserving observables, particularly the anomalous magnetic moment of the muon, and lepton-flavor-violating processes like μ → e γ decay and μ − e conversions in nuclei. While contributions to the anomalous magnetic moment fall below the measured values at 2 σ , current and future experimental sensitivities to flavor-violating branching rations of the Standard Model leptons are expected to impose lower bounds on the mass of the peculiar S U ( 2 ) R gauge boson of the model. This provides complementary constraints relative to existing limits, which are indirect and derived from collider bounds on the mass of the associated neutral gauge boson Z ′ . Published by the American Physical Society 2025
- 9 May 2025
- Published by American Physical Society (APS) in Physical Review D
- Vol. 111 (9)
Open AccessLeptonic probes of alternative left-right symmetric models
We explore constraints on the parameter space of the alternative left-right model originating from the leptonic sector. Our analyses focuses on both lepton-flavor-conserving observables, particularly the anomalous magnetic moment of the muon, and lepton-flavor-violating processes like μ → e γ decay and μ − e conversions in nuclei. While contributions to the anomalous magnetic moment fall below the measured values at 2 σ , current and future experimental sensitivities to flavor-violating branching rations of the Standard Model leptons are expected to impose lower bounds on the mass of the peculiar S U ( 2 ) R gauge boson of the model. This provides complementary constraints relative to existing limits, which are indirect and derived from collider bounds on the mass of the associated neutral gauge boson Z ′ . Published by the American Physical Society 2025
- 1 January 2025
- Published by Springer Nature
- p. 632-635
Exploring the Alternative Left-Right Model with Leptonic Probes
- 1 January 2025
- Published by Springer Nature
- p. 632-635
Exploring the Alternative Left-Right Model with Leptonic Probes
- Open Access
- 27 February 2024
- Published by Elsevier in Physics Letters B
- Vol. 850
Flavour-changing top quark decays in the alternative left-right model
- 27 February 2024
- Published by Elsevier in Physics Letters B
- Vol. 850
Open AccessFlavour-changing top quark decays in the alternative left-right model
- Open Access
What is the Simplest Linear Ramp?
We discuss conditions under which a deterministic sequence of real numbers, interpreted as the set of eigenvalues of a Hamiltonian, can exhibit features usually associated to random matrix spectra. A key diagnostic is the spectral form factor (SFF) -- a linear ramp in the SFF is often viewed as a signature of random matrix behavior. Based on various explicit examples, we observe conditions for linear and power law ramps to arise in deterministic spectra. We note that a very simple spectrum with a linear ramp is $E_n \sim \log n$. Despite the presence of ramps, these sequences do $not$ exhibit conventional level repulsion, demonstrating that the lore about their concurrence needs refinement. However, when a small noise correction is added to the spectrum, they lead to clear level repulsion as well as the (linear) ramp. We note some remarkable features of logarithmic spectra, apart from their linear ramps: they are closely related to normal modes of black hole stretched horizons, and their partition function with argument $s=β+it$ is the Riemann zeta function $ζ(s)$. An immediate consequence is that the spectral form factor is simply $\sim |ζ(it)|^2$. Our observation that log spectra have a linear ramp, is closely related to the Lindelöf hypothesis on the growth of the zeta function. With elementary numerics, we check that the slope of a best fit line through $|ζ(it)|^2$ on a log-log plot is indeed $1$, to the fourth decimal. We also note that truncating the Riemann zeta function sum at a finite integer $N$ causes the would-be-eternal ramp to end on a plateau.Open AccessWhat is the Simplest Linear Ramp?
We discuss conditions under which a deterministic sequence of real numbers, interpreted as the set of eigenvalues of a Hamiltonian, can exhibit features usually associated to random matrix spectra. A key diagnostic is the spectral form factor (SFF) -- a linear ramp in the SFF is often viewed as a signature of random matrix behavior. Based on various explicit examples, we observe conditions for linear and power law ramps to arise in deterministic spectra. We note that a very simple spectrum with a linear ramp is $E_n \sim \log n$. Despite the presence of ramps, these sequences do $not$ exhibit conventional level repulsion, demonstrating that the lore about their concurrence needs refinement. However, when a small noise correction is added to the spectrum, they lead to clear level repulsion as well as the (linear) ramp. We note some remarkable features of logarithmic spectra, apart from their linear ramps: they are closely related to normal modes of black hole stretched horizons, and their partition function with argument $s=β+it$ is the Riemann zeta function $ζ(s)$. An immediate consequence is that the spectral form factor is simply $\sim |ζ(it)|^2$. Our observation that log spectra have a linear ramp, is closely related to the Lindelöf hypothesis on the growth of the zeta function. With elementary numerics, we check that the slope of a best fit line through $|ζ(it)|^2$ on a log-log plot is indeed $1$, to the fourth decimal. We also note that truncating the Riemann zeta function sum at a finite integer $N$ causes the would-be-eternal ramp to end on a plateau. - Top Cited PapersOpen Access
- 26 January 2024
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2024 (1) , 1-15
What is the Simplest Linear Ramp?
We discuss conditions under which a deterministic sequence of real numbers, interpreted as the set of eigenvalues of a Hamiltonian, can exhibit features usually associated to random matrix spectra. A key diagnostic is the spectral form factor (SFF) — a linear ramp in the SFF is often viewed as a signature of random matrix behavior. Based on various explicit examples, we observe conditions for linear and power law ramps to arise in deterministic spectra. We note that a very simple spectrum with a linear ramp is E n ~ log n. Despite the presence of ramps, these sequences do not exhibit conventional level repulsion, demonstrating that the lore about their concurrence needs refinement. However, when a small noise correction is added to the spectrum, they lead to clear level repulsion as well as the (linear) ramp. We note some remarkable features of logarithmic spectra, apart from their linear ramps: they are closely related to normal modes of black hole stretched horizons, and their partition function with argument s = β + it is the Riemann zeta function ζ(s). An immediate consequence is that the spectral form factor is simply −ζ|(it)|2. Our observation that log spectra have a linear ramp, is closely related to the Lindelöf hypothesis on the growth of the zeta function. With elementary numerics, we check that the slope of a best fit line through |ζ(it)|2 on a log-log plot is indeed 1, to the fourth decimal. We also note that truncating the Riemann zeta function sum at a finite integer N causes the would-be-eternal ramp to end on a plateau.
- 26 January 2024
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2024 (1) , 1-15
Top Cited PapersOpen AccessWhat is the Simplest Linear Ramp?
We discuss conditions under which a deterministic sequence of real numbers, interpreted as the set of eigenvalues of a Hamiltonian, can exhibit features usually associated to random matrix spectra. A key diagnostic is the spectral form factor (SFF) — a linear ramp in the SFF is often viewed as a signature of random matrix behavior. Based on various explicit examples, we observe conditions for linear and power law ramps to arise in deterministic spectra. We note that a very simple spectrum with a linear ramp is E n ~ log n. Despite the presence of ramps, these sequences do not exhibit conventional level repulsion, demonstrating that the lore about their concurrence needs refinement. However, when a small noise correction is added to the spectrum, they lead to clear level repulsion as well as the (linear) ramp. We note some remarkable features of logarithmic spectra, apart from their linear ramps: they are closely related to normal modes of black hole stretched horizons, and their partition function with argument s = β + it is the Riemann zeta function ζ(s). An immediate consequence is that the spectral form factor is simply −ζ|(it)|2. Our observation that log spectra have a linear ramp, is closely related to the Lindelöf hypothesis on the growth of the zeta function. With elementary numerics, we check that the slope of a best fit line through |ζ(it)|2 on a log-log plot is indeed 1, to the fourth decimal. We also note that truncating the Riemann zeta function sum at a finite integer N causes the would-be-eternal ramp to end on a plateau.
- Open Access
- 5 October 2023
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2023 (10) , 1-27
Fuzzballs and random matrices
A bstract: Black holes are believed to have the fast scrambling properties of random matrices. If the fuzzball proposal is to be a viable model for quantum black holes, it should reproduce this expectation. This is considered challenging, because it is natural for the modes on a fuzzball microstate to follow Poisson statistics. In a previous paper, we noted a potential loophole here, thanks to the modes depending not just on the n -quantum number, but also on the J -quantum numbers of the compact dimensions. For a free scalar field ϕ , by imposing a Dirichlet boundary condition ϕ = 0 at the stretched horizon, we showed that this J -dependence leads to a linear ramp in the Spectral Form Factor (SFF). Despite this, the status of level repulsion remained mysterious. In this letter, motivated by the profile functions of BPS fuzzballs, we consider a generic profile ϕ = ϕ 0 ( θ ) instead of ϕ = 0 at the stretched horizon. For various notions of genericity (eg. when the Fourier coefficients of ϕ 0 ( θ ) are suitably Gaussian distributed), we find that the J -dependence of the spectrum exhibits striking evidence of level repulsion, along with the linear ramp. We also find that varying the profile leads to natural interpolations between Poisson and Wigner-Dyson(WD)-like spectra. The linear ramp in our previous work can be understood as arising via an extreme version of level repulsion in such a limiting spectrum. We also explain how the stretched horizon/fuzzball is different in these aspects from simply putting a cut-off in flat space or AdS (i.e., without a horizon).
- 5 October 2023
- Published by Springer Nature in Journal of High Energy Physics
- Vol. 2023 (10) , 1-27
Open AccessFuzzballs and random matrices
A bstract: Black holes are believed to have the fast scrambling properties of random matrices. If the fuzzball proposal is to be a viable model for quantum black holes, it should reproduce this expectation. This is considered challenging, because it is natural for the modes on a fuzzball microstate to follow Poisson statistics. In a previous paper, we noted a potential loophole here, thanks to the modes depending not just on the n -quantum number, but also on the J -quantum numbers of the compact dimensions. For a free scalar field ϕ , by imposing a Dirichlet boundary condition ϕ = 0 at the stretched horizon, we showed that this J -dependence leads to a linear ramp in the Spectral Form Factor (SFF). Despite this, the status of level repulsion remained mysterious. In this letter, motivated by the profile functions of BPS fuzzballs, we consider a generic profile ϕ = ϕ 0 ( θ ) instead of ϕ = 0 at the stretched horizon. For various notions of genericity (eg. when the Fourier coefficients of ϕ 0 ( θ ) are suitably Gaussian distributed), we find that the J -dependence of the spectrum exhibits striking evidence of level repulsion, along with the linear ramp. We also find that varying the profile leads to natural interpolations between Poisson and Wigner-Dyson(WD)-like spectra. The linear ramp in our previous work can be understood as arising via an extreme version of level repulsion in such a limiting spectrum. We also explain how the stretched horizon/fuzzball is different in these aspects from simply putting a cut-off in flat space or AdS (i.e., without a horizon).
- Open Access
Fuzzballs and Random Matrices
Black holes are believed to have the fast scrambling properties of random matrices. If the fuzzball proposal is to be a viable model for quantum black holes, it should reproduce this expectation. This is considered challenging, because it is natural for the modes on a fuzzball microstate to follow Poisson statistics. In a previous paper, we noted a potential loophole here, thanks to the modes depending not just on the $n$-quantum number, but also on the $J$-quantum numbers of the compact dimensions. For a free scalar field $φ$, by imposing a Dirichlet boundary condition $φ=0$ at the stretched horizon, we showed that this $J$-dependence leads to a linear ramp in the Spectral Form Factor (SFF). Despite this, the status of level repulsion remained mysterious. In this letter, motivated by the profile functions of BPS fuzzballs, we consider a generic profile $φ= φ_0(θ)$ instead of $φ=0$ at the stretched horizon. For various notions of genericity (eg. when the Fourier coefficients of $φ_0(θ)$ are suitably Gaussian distributed), we find that the $J$-dependence of the spectrum exhibits striking evidence of level repulsion, along with the linear ramp. We also find that varying the profile leads to natural interpolations between Poisson and Wigner-Dyson(WD)-like spectra. The linear ramp in our previous work can be understood as arising via an extreme version of level repulsion in such a limiting spectrum. We also explain how the stretched horizon/fuzzball is different in these aspects from simply putting a cut-off in flat space or AdS (ie., without a horizon).Open AccessFuzzballs and Random Matrices
Black holes are believed to have the fast scrambling properties of random matrices. If the fuzzball proposal is to be a viable model for quantum black holes, it should reproduce this expectation. This is considered challenging, because it is natural for the modes on a fuzzball microstate to follow Poisson statistics. In a previous paper, we noted a potential loophole here, thanks to the modes depending not just on the $n$-quantum number, but also on the $J$-quantum numbers of the compact dimensions. For a free scalar field $φ$, by imposing a Dirichlet boundary condition $φ=0$ at the stretched horizon, we showed that this $J$-dependence leads to a linear ramp in the Spectral Form Factor (SFF). Despite this, the status of level repulsion remained mysterious. In this letter, motivated by the profile functions of BPS fuzzballs, we consider a generic profile $φ= φ_0(θ)$ instead of $φ=0$ at the stretched horizon. For various notions of genericity (eg. when the Fourier coefficients of $φ_0(θ)$ are suitably Gaussian distributed), we find that the $J$-dependence of the spectrum exhibits striking evidence of level repulsion, along with the linear ramp. We also find that varying the profile leads to natural interpolations between Poisson and Wigner-Dyson(WD)-like spectra. The linear ramp in our previous work can be understood as arising via an extreme version of level repulsion in such a limiting spectrum. We also explain how the stretched horizon/fuzzball is different in these aspects from simply putting a cut-off in flat space or AdS (ie., without a horizon). - 10 July 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (1)
Top Yukawa coupling measurement with indefiniteHiggs inWe consider the issue of the top quark Yukawa coupling measurement in a model-independent and general case with the inclusion of $CP$ violation in the coupling. Arguably the best process to study this coupling is the associated production of the Higgs boson along with a $t\overline{t}$ pair in a machine like the International Linear Collider (ILC). While detailed analyses of the sensitivity of the measurement\char22{}assuming a Standard Model (SM)-like coupling is available in the context of the ILC\char22{}conclude that the coupling could be pinned down to about a 10% level with modest luminosity, our investigations show that the scenario could be different in the case of a more general coupling. The modified Lorentz structure resulting in a changed functional dependence of the cross section on the coupling, along with the difference in the cross section itself leads to considerable deviation in the sensitivity. Our studies of the ILC with center-of-mass energies of 500 GeV, 800 GeV, and 1000 GeV show that moderate $CP$ mixing in the Higgs sector could change the sensitivity to about 20%, while it could be worsened to 75% in cases which could accommodate more dramatic changes in the coupling. Detailed considerations of the decay distributions point to a need for a relook at the analysis strategy followed for the case of the SM, such as for a model-independent analysis of the top quark Yukawa coupling measurement. This study strongly suggests that a joint analysis of the $CP$ properties and the Yukawa coupling measurement would be the way forward at the ILC and that caution must be exercised in the measurement of the Yukawa couplings and the conclusions drawn from it.- 10 July 2014
- Published by American Physical Society (APS) in Physical Review D
- Vol. 90 (1)
Top Yukawa coupling measurement with indefiniteHiggs inWe consider the issue of the top quark Yukawa coupling measurement in a model-independent and general case with the inclusion of $CP$ violation in the coupling. Arguably the best process to study this coupling is the associated production of the Higgs boson along with a $t\overline{t}$ pair in a machine like the International Linear Collider (ILC). While detailed analyses of the sensitivity of the measurement\char22{}assuming a Standard Model (SM)-like coupling is available in the context of the ILC\char22{}conclude that the coupling could be pinned down to about a 10% level with modest luminosity, our investigations show that the scenario could be different in the case of a more general coupling. The modified Lorentz structure resulting in a changed functional dependence of the cross section on the coupling, along with the difference in the cross section itself leads to considerable deviation in the sensitivity. Our studies of the ILC with center-of-mass energies of 500 GeV, 800 GeV, and 1000 GeV show that moderate $CP$ mixing in the Higgs sector could change the sensitivity to about 20%, while it could be worsened to 75% in cases which could accommodate more dramatic changes in the coupling. Detailed considerations of the decay distributions point to a need for a relook at the analysis strategy followed for the case of the SM, such as for a model-independent analysis of the top quark Yukawa coupling measurement. This study strongly suggests that a joint analysis of the $CP$ properties and the Yukawa coupling measurement would be the way forward at the ILC and that caution must be exercised in the measurement of the Yukawa couplings and the conclusions drawn from it.