Back to Search Start Over

Short-distance matrix elements for $D^0$-meson mixing for $N_f=2+1$ lattice QCD

Authors :
Bazavov, A.
Bernard, C.
Bouchard, C. M.
Chang, C. C.
DeTar, C.
Du, D.
El-Khadra, A. X.
Freeland, E. D.
Gámiz, E.
Gottlieb, Steven
Heller, U. M.
Kronfeld, A. S.
Laiho, J.
Mackenzie, P. B.
Neil, E. T.
Simone, J. N.
Sugar, R.
Toussaint, D.
Van de Water, R. S.
Zhou, R.
Source :
Phys. Rev. D 97, 034513 (2018)
Publication Year :
2017

Abstract

We calculate in three-flavor lattice QCD the short-distance hadronic matrix elements of all five $\Delta C=2$ four-fermion operators that contribute to neutral $D$-meson mixing both in and beyond the Standard Model. We use the MILC Collaboration's $N_f = 2+1$ lattice gauge-field configurations generated with asqtad-improved staggered sea quarks. We also employ the asqtad action for the valence light quarks and use the clover action with the Fermilab interpretation for the charm quark. We analyze a large set of ensembles with pions as light as $M_\pi \approx 180$ MeV and lattice spacings as fine as $a\approx 0.045$ fm, thereby enabling good control over the extrapolation to the physical pion mass and continuum limit. We obtain for the matrix elements in the $\overline{\text{MS}}$-NDR scheme using the choice of evanescent operators proposed by Beneke \emph{et al.}, evaluated at 3 GeV, $\langle D^0|\mathcal{O}_i|\bar{D}^0 \rangle = \{0.0805(55)(16), -0.1561(70)(31), 0.0464(31)(9), 0.2747(129)(55), 0.1035(71)(21)\}~\text{GeV}^4$ ($i=1$--5). The errors shown are from statistics and lattice systematics, and the omission of charmed sea quarks, respectively. To illustrate the utility of our matrix-element results, we place bounds on the scale of CP-violating new physics in $D^0$~mixing, finding lower limits of about 10--50$\times 10^3$ TeV for couplings of $\mathrm{O}(1)$. To enable our results to be employed in more sophisticated or model-specific phenomenological studies, we provide the correlations among our matrix-element results. For convenience, we also present numerical results in the other commonly-used scheme of Buras, Misiak, and Urban.<br />Comment: Published version, 42 pages, 18 figures

Details

Database :
arXiv
Journal :
Phys. Rev. D 97, 034513 (2018)
Publication Type :
Report
Accession number :
edsarx.1706.04622
Document Type :
Working Paper
Full Text :
https://doi.org/10.1103/PhysRevD.97.034513