Scattering amplitudes describe the probability that particles produce a specific outcome after collision, and are the basis for comparing theoretical predictions with collider experiments. Physicists usually compute amplitudes using perturbation theory, adding quantum corrections level by level, where each level is one "loop." The higher the loop count, the more precise the result, and the computational complexity grows exponentially or even factorially. In actual research, most amplitudes are computed only to two loops, and a few can reach three loops.
Planar N=4 super Yang-Mills theory is a testing ground for amplitude researchers. The theory does not describe the real world, but the delicate balance among particle types greatly simplifies calculations, and researchers use it to hone new methods before extending them to theories closer to reality. The Lance team has advanced loop by loop using the bootstrap method since 2011: first delineating the function space where the answer lies based on physical principles, encoding each candidate function into a sequence using a specific "alphabet," that is, the "symbol" that preserves the main structure of the function, then imposing known constraints one by one to eliminate candidates until only a unique solution remains. The whole process is similar to solving a Sudoku.
By 2019, they had only reached six and seven loops. In 2021, Lance discovered that the amplitude for two gluons colliding to produce four gluons is numerically very similar to the "form factor" for two gluons colliding to produce one gluon and one Higgs boson, the latter being easier to compute. The team then confirmed that reversing the order of each letter sequence in the former's symbol, followed by a variable substitution, yields the latter, a phenomenon named "antipodal duality." In 2022, Lance and collaborators first computed the form factor to eight loops, and in 2023 used antipodal duality to work backward from it to the eight-loop amplitude. Since then, Lance planned to continue completing the ninth loop using this method.