A Systematic Lagrangian Formulation for Quantum and Classical Gravity at High Energies

TL;DR

This paper develops a systematic Lagrangian framework for quantum and classical gravity at high energies, enabling precise calculations of scattering amplitudes and revealing connections to Regge trajectories and BFKL equations.

Contribution

It introduces a novel Lagrangian approach that incorporates rapidity renormalization group techniques and factorization, advancing the understanding of quantum gravity in the super-Planckian regime.

Findings

Derived a resummation method for logarithmic corrections in high-energy gravity.

Connected the graviton Regge trajectory with the leading operator running.

Established the gravitational BFKL equation and its relation to QCD kernels.

Abstract

We derive a systematic Lagrangian approach for quantum gravity in the super-Planckian limit where $s\gg M_{pl}^2\gg t$. The action can be used to calculate to arbitrary accuracy in the quantum and classical expansion parameters $\alpha_Q= \frac{t}{M_{pl}^2}$ and $\alpha_C= \frac{st}{M_{pl}^4}$, respectively, for the scattering of massless particles. The perturbative series contains powers of $\log(s/t)$ which can be resummed using a rapidity renormalization group equation (RRGE) that follows from a factorization theorem which allows us to write the amplitude as a convolution of a soft and collinear jet functions. We prove that the soft function is composed of an infinite tower of operators which do not mix under rapidity renormalization. The running of the leading order (in $G$) operator leads to the graviton Regge trajectory while the next to leading operator running corresponds to the gravitational BFKL equation. For the former, we find agreement with one of the two results previously presented in the literature, while for the ladder our result agrees (up to regulator dependent pieces) with those of Lipatov. We find that the convolutive piece of the gravitational BFKL kernel is the square of that of QCD. The power counting simplifies considerably in the classical limit where we can use our formalism to extract logs at any order in the PM expansion. The leading log at any order in the PM expansion can be calculated without going beyond one loop. The log at $(2N+1)$ order in the Post-Minkowskian expansion follows from calculating the one loop anomalous dimension for the $N+1$th order piece of the soft function and perturbatively solving the RRGE $N-1$ times. The factorization theorem implies that the classical logs which arise alternate between being real and imaginary in nature as $N$ increases.