Nonperturbative Collins-Soper Kernel from Chiral Quarks with Physical Masses
arXiv:2403.00664 · doi:10.1016/j.physletb.2024.138617
Abstract
We present a lattice QCD calculation of the rapidity anomalous dimension of quark transverse-momentum-dependent distributions, i.e., the Collins-Soper (CS) kernel, up to transverse separations of about 1 fm. This unitary lattice calculation is conducted, for the first time, employing the chiral-symmetry-preserving domain wall fermion discretization and physical values of light and strange quark masses. The CS kernel is extracted from the ratios of pion quasi-transverse-momentum-dependent wave functions (quasi-TMDWFs) at next-to-leading logarithmic perturbative accuracy. Also for the first time, we utilize the recently proposed Coulomb-gauge-fixed quasi-TMDWF correlator without a Wilson line. We observe significantly slower signal decay with increasing quark separations compared to the established gauge-invariant method with a staple-shaped Wilson line. This enables us to determine the CS kernel at large nonperturbative transverse separations and find its near-linear dependence on the latter. Our result is consistent with the recent lattice calculation using gauge-invariant quasi-TMDWFs, and agrees with various recent phenomenological parametrizations of experimental data.
7 pages, 4 figures; published version
References in corpus (7)
- On the Renormalizability of Quasi Parton Distribution Functions
- Soft-/rapidity- anomalous dimensions correspondence
- Understanding the large-distance behavior of transverse-momentum-dependent parton densities and the Collins-Soper evolution kernel
- Soft Factor Subtraction and Transverse Momentum Dependent Parton Distributions on Lattice
- Non-perturbative QCD effects in spectra of Drell-Yan and -boson production
- One-loop renormalization of staple-shaped operators in continuum and lattice regularizations
- Single Transverse-Spin Asymmetry and Sivers Function in Large Momentum Effective Theory