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Vatsalya Vaibhav

Publications and source records attributed to Vatsalya Vaibhav.

5 recordsLinked to original sources

Might the radiation era extend back to the Big Bang? On dark matter production and the relic graviton background in quadratic gravity

Naive estimates based on Einstein gravity with Lagrangian $\frac{1}{2}M_{pl}^{2}(R-2Λ)$ suggest that, if the radiation era extended back to the Big Bang (i.e., as far back as the classical spacetime background makes sense), this would result in an over-production of dark matter and a relic cosmic background of thermal gravitons. Here we revisit these conclusions in quadratic gravity, the minimal renormalizable completion of Einstein gravity, whose Lagrangian also includes the terms $\frac{1}{6}f_0^{-2}R^2-\frac{1}{2}f_{2}^{-2}C^{2}$. Assuming the radiation era does extend back to the bang, we find a novel relation between the coefficient $f_{2}$ and the dark matter mass $m_{dm}$, needed to obtain the correct dark matter abundance. This yields a new gravitational production mechanism for dark matter (e.g., stable right-handed neutrinos). Moreover, the presence or absence of the relic graviton background (detectable by forthcoming CMB experiments via its small imprint on $N_{\rm eff}$) will place new constraints on $f_{0}, f_{2}$.

hep-ph↗

A Proposed $E_8 \times E_8$ Kinematic Scaffolding for the Standard Model with Pre-Gravitation

We present a proposed $E_8 \times E_8$ kinematic scaffolding for the standard model with pre-gravitation. The notation $E_8\timesωE_8$ used below records a split-complex exchange grading of two factors; it is not a tensor product of groups. Each factor branches through $SU(3)\times E_6$ and thence through trinification, $E_6 \rightarrow SU(3)^3$. The first factor supplies representation labels associated with the standard-model lineage, and the second supplies a mirror, pre-gravitational lineage. The identification of a single vector-like colour group across the two factors, and the proposed gravitational reading of the right-sector $SU(2)$, remain dynamical hypotheses. Physical chiral fermions are not assigned to the $E_8$ adjoints: they are modelled by minimal ideals of the complex Clifford algebra $Cl_6(\mathbb C)$, while the $496$ adjoint dimensions are used only as a representation-label ledger. The numerical split $208+288$ is therefore a declared roster-matching convention, not an invariant decomposition and not a particle count. Spacetime enters through a selected six-dimensional split-biquaternionic vector space with a separately specified quadratic form of signature $(3,3)$. Its full frame group is $SO(3,3)$; deriving a soldering form and the proposed $BF$/Plebański dynamics remains open. The conventional Clifford--Dirac operator is constructed independently and exactly: $J_2(\mathbb H_s)$ realises the vector space $\mathbb R^{3,3}$ through its determinant, and after choosing $\mathbb H_s\cong M_2(\mathbb R)$ its matrix gradient and adjugate act between real four-dimensional Weyl modules and factorise the wave operator in both orderings. The rank-two algebra supplies the quadratic spacetime layer, whereas $J_3(\mathbb O_{\mathbb C})$ supplies the proposed internal, generation and cubic spectral layer through the magic-star decomposition of $\mathfrak e_8^{\mathbb C}$.

hep-ph↗

Fixed points of classical gravity coupled with a Standard-Model-like theory

Coupling quantum field theory (QFT) \!-\! even free QFT \!-\! to gravity leads to well-known problems. In particular, the stress tensor $T_{μν}$ (gravity's source) and its correlators typically diverge in the UV, creating a conflict between the wildly inhomogeneous spacetime we expect quantum mechanically and the weakly-curved, macroscopic spacetime we observe. Are there QFTs for which these divergences cancel? Here, for simplicity, we consider free quantum fields on a classical curved background. The aforementioned divergences are related to the running of the gravitational couplings. We calculate the corresponding beta functions, identifying a special class of QFTs with UV fixed points at which $\langle T_{μν}\rangle$ and all its correlators $\langle T\ldots T\rangle$ are UV finite. An intriguing example is a theory like the Standard Model (including right-handed neutrinos) with $12$ gauge fields, $3$ generations of $16$ Weyl fermions and $36$ four-derivative (Fradkin-Tseytlin) scalars. In the infrared, this theory has a positive Newton's constant $G$ and an arbitrarily small cosmological constant $Λ$.

hep-th↗

Left-Right symmetric fermions and sterile neutrinos from complex split biquaternions and bioctonions

In this article we investigate the application of complex split biquaternions and bioctonions to the standard model. We show that the Clifford algebras Cl(3) and Cl(7) can be used for making left-right symmetric fermions. Hence we incorporate right-handed neutrinos in the division algebras based approach to the standard model. The right-handed neutrinos, also known as sterile neutrinos, are a potential dark-matter candidate. We discuss the left-right symmetric fermions and their phenomenology using the division algebra approach. We describe the gauge groups associated with the left-right symmetric model and prospects for unification through division algebras. We investigate the possibility of obtaining three generations of fermions and charge/mass ratios through the exceptional Jordan algebra $J_3(O)$ and the exceptional groups $F_4$ and $E_6$.

hep-ph↗

Majorana Neutrinos, Exceptional Jordan Algebra, and Mass Ratios for Charged Fermions

We provide theoretical evidence that the neutrino is a Majorana fermion. This evidence comes from assuming that the standard model and beyond-standard-model physics can be described through division algebras, coupled to a quantum dynamics. We use the division algebras scheme to derive mass ratios for the standard model charged fermions of three generations. The predicted ratios agree well with the observed values if the neutrino is assumed to be Majorana. However, the theoretically calculated ratios completely disagree with known values if the neutrino is taken to be a Dirac particle. Towards the end of the article we discuss prospects for unification of the standard model with gravitation if the assumed symmetry group of the theory is $E_6$, and if it is assumed that space-time is an 8D octonionic space-time, with 4D Minkowski space-time being an emergent approximation. Remarkably, we find evidence that the precursor of classical gravitation, described by the symmetry $SU(3)_{grav} \times SU(2)_R \times U(1)_{grav}$ is the right-handed counterpart of the standard model $SU(3)_{color} \times SU(2)_L \times U(1)_Y$.

hep-ph↗