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.

Highlights

  • The mixing between neutral K, D, B, and Bs mesons and their antiparticles is loop suppressed in the Standard Model and, provides a window into new physics

  • It provides unique information on new-physics contributions to the down-quark sector that is complementary to that provided by kaons and BðsÞ mesons, in which mixing is mediated by up-type quarks

  • Eq (2.22) can be used to test models in which new physics does not change the phase of Γ12.2 A convenient way to do so is illustrated in Fig. 2, which plots jx12jeiφ12 as a complex number

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Summary

INTRODUCTION

The mixing between neutral K, D, B, and Bs mesons and their antiparticles is loop suppressed in the Standard Model and, provides a window into new physics. Still not as precise as experiment, the Standard Model theory for kaon and BðsÞ-meson mixing is under good control, owing to recent lattice-QCD calculations of the relevant hadronic matrix elements for kaons [3,4,5] and for neutral BðsÞ mesons [6]. Final results are provided in double-precision as Supplemental Material [12]

THEORETICAL AND PHENOMENOLOGICAL BACKGROUND
LATTICE SIMULATION
Lattice correlation functions
Statistics and autocorrelations
CORRELATOR ANALYSIS
Correlator fit functions
Method
Prior selection
Fit region
Fit stability
Fit range and number of states
Operator smearing
Error propagation
RENORMALIZATION
CHARM-QUARK MASS CORRECTION
Chiral fit function
Chiral logarithms
Analytic terms in the chiral expansion The analytic terms
Heavy quark discretization effects
Heavy-quark mass adjustment
Renormalization errors
Chiral-continuum fit parameters
Loosely constrained fit parameters
Constrained fit parameters
Fixed inputs
VIII. SYSTEMATIC ERROR ANALYSIS
Base chiral-continuum fit errors
Parametric inputs
Charm-quark mass uncertainty
Renormalization and matching uncertainty
Truncation of the chiral and heavy-meson expansion
Light quark discretization errors
Heavy quark discretization errors
Additional errors
Finite-volume effects
Isospin breaking and electromagnetism
Omission of the charmed sea quark
Other consistency checks and error summary
RESULTS
Matrix elements
Implications for new physics
CNi Pð3 i
SUMMARY AND OUTLOOK
Full Text
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