- Open Access
Aspects of propagator sparsening in lattice QCD
Phys. Rev. D 111, 114514 – Published 17 June, 2025
DOI: https://doi.org/10.1103/xfmp-c2d4
Abstract
In lattice field theory, field sparsening aims to replace quantum fields, or objects constructed from them, with approximations that preserve the appropriate symmetries and maintain many aspects of the physics that the fields determine. For example, an effective sparsening of a quark propagator provides an efficient map from a quark propagator on a fine lattice geometry to a quark propagator defined on a coarser geometry in order to reduce storage and computational costs of subsequent calculational stages while maintaining long-distance correlations and corresponding low-energy physical information. Previous studies have focused on decimating lattice sites or randomly sampling lattice sites to reduce the size of the propagator and subsequent costs of Wick contractions. Here, we extend the study of sparsening to incorporate covariant averaging of spatial sites and examine the effects on two-point and three-point correlation functions involving various hadrons. We find that sparsening is most effective in reproducing the unsparsened versions of these correlation functions when weighted covariant-averaging is sequentially applied many times.
Physics Subject Headings (PhySH)
Article Text
Supplemental Material
References (35)
- P. Weisz, Nucl. Phys. B212, 1 (1983).
- P. Weisz and R. Wohlert, Nucl. Phys. B236, 397 (1984); B247, 544(E) (1984).
- K. Symanzik, Nucl. Phys. B226, 187 (1983).
- K. Symanzik, Nucl. Phys. B226, 205 (1983).
- Y. Iwasaki, Nucl. Phys. B258, 141 (1985).
- Y. Iwasaki, arXiv:1111.7054.
- M. Lüscher and P. Weisz, Phys. Lett. 158B, 250 (1985).
- B. Sheikholeslami and R. Wohlert, Nucl. Phys. B259, 572 (1985).
- P. Hasenfratz and F. Niedermayer, Nucl. Phys. B414, 785 (1994).
- W. Bietenholz and U. J. Wiese, Nucl. Phys. B464, 319 (1996).
- T. A. DeGrand, A. Hasenfratz, P. Hasenfratz, and F. Niedermayer, Nucl. Phys. B454, 587 (1995).
- P. Hasenfratz, in Advanced Summer School on Nonperturbative Quantum Field Physics (1998), pp. 137–199, arXiv:hep-lat/9803027.
- M. G. Endres, R. C. Brower, W. Detmold, K. Orginos, and A. V. Pochinsky, Phys. Rev. D 92, 114516 (2015).
- W. Detmold and M. G. Endres, Phys. Rev. D 94, 114502 (2016).
- W. Detmold and M. G. Endres, Phys. Rev. D 97, 074507 (2018).
- P. E. Shanahan, A. Trewartha, and W. Detmold, Phys. Rev. D 97, 094506 (2018).
- R. Abbott, M. S. Albergo, D. Boyda, D. C. Hackett, G. Kanwar, F. Romero-López, P. E. Shanahan, and J. M. Urban, Proc. Sci. LATTICE2023 (2024) 035 [arXiv:2404.10819].
- W. Detmold, D. J. Murphy, A. V. Pochinsky, M. J. Savage, P. E. Shanahan, and M. L. Wagman, Phys. Rev. D 104, 034502 (2021).
- Y. Li, S.-C. Xia, X. Feng, L.-C. Jin, and C. Liu, Phys. Rev. D 103, 014514 (2021).
- S. Amarasinghe, R. Baghdadi, Z. Davoudi, W. Detmold, M. Illa, A. Parreño, A. V. Pochinsky, P. E. Shanahan, and M. L. Wagman, Phys. Rev. D 107, 094508 (2023).
- W. Detmold, M. Illa, W. I. Jay, A. Parreño, R. J. Perry, P. E. Shanahan, and M. L. Wagman, arXiv:2404.12039.
- R. Abbott, W. Detmold, F. Romero-López, Z. Davoudi, M. Illa, A. Parreño, R. J. Perry, P. E. Shanahan, and M. L. Wagman (NPLQCD Collaboration), Phys. Rev. D 108, 114506 (2023).
- R. Abbott, W. Detmold, M. Illa, A. Parreño, R. J. Perry, F. Romero-López, P. E. Shanahan, and M. L. Wagman (NPLQCD Collaboration), Phys. Rev. Lett. 134, 011903 (2025).
- X. Feng, L. Jin, and M. J. Riberdy, Phys. Rev. Lett. 128, 052003 (2022).
- C. Lehner, grid python Toolkit (gpt), https://github.com/lehner/gpt.
- D. Daniel, R. Gupta, G. W. Kilcup, A. Patel, and S. R. Sharpe, Phys. Rev. D 46, 3130 (1992).
- C. Morningstar and M. J. Peardon, Phys. Rev. D 69, 054501 (2004).
- J. M. Zanotti, D. B. Leinweber, A. G. Williams, J. Zhang, W. Melnitchouk, S. Choe et al., Phys. Rev. D 68, 054506 (2003).
- L. Hockley, W. Kamleh, D. Leinweber, and A. Thomas, Few Body Syst. 64, 46 (2023).
- S. R. Beane et al. (NPLQCD, QCDSF Collaborations), Phys. Rev. D 103, 054504 (2021).
- See Supplemental Material at http://link.aps.org/supplemental/10.1103/xfmp-c2d4 for a set of figures similar to Figs. 2 through 9 but for a more comprehensive set of blocking and decimation steps.
- Z. Davoudi, W. Detmold, Z. Fu, A. V. Grebe, W. Jay, D. Murphy, P. Oare, P. E. Shanahan, and M. L. Wagman (NPLQCD Collaboration), Phys. Rev. D 109, 114514 (2024).
- R. G. Edwards and B. Joó (SciDAC, LHPC, UKQCD Collaborations), Nucl. Phys. B, Proc. Suppl. 140, 832 (2005).
- P. A. Boyle, G. Cossu, A. Yamaguchi, and A. Portelli, Proc. Sci. LATTICE2015 (2016) 023.
- A. Reuther, J. Kepner, C. Byun, S. Samsi, W. Arcand, D. Bestor, B. Bergeron, V. Gadepally, M. Houle, M. Hubbell, M. Jones, A. Klein, L. Milechin, J. Mullen, A. Prout, A. Rosa, C. Yee, and P. Michaleas, in Proceedings of the 2018 IEEE High Performance extreme Computing Conference (HPEC) (IEEE, Waltham, MA, 2018), pp. 1–6.