Kuberski, Simon: Standard Model parameters in the heavy quark sector from three-flavor lattice QCD. 2020
Inhalt
- Abstract
- Zusammenfassung
- Contents
- 1 Introduction
- Theory
- 2 QCD on the lattice
- 3 The Schrödinger functional
- 3.1 Continuum formulation
- 3.2 Lattice formulation
- 3.3 Schrödinger functional correlation functions
- 3.3.1 Boundary sources
- 3.3.2 Expectation values
- 3.3.3 Correlation functions
- 3.3.4 Flavor off-diagonal bilinears
- 3.4 Addendum: Open Boundary Conditions
- 4 Operator improvement and renormalization
- 5 Algorithmic techniques
- 5.1 Simulation algorithms
- 5.1.1 Hybrid Monte Carlo
- 5.1.2 Integration schemes
- 5.1.3 HMC with dynamical quarks
- 5.1.4 Rational Hybrid Monte Carlo
- 5.1.5 Reweighting
- 5.2 Frequency splitting
- 5.3 Solver
- 5.3.1 Conjugate Gradient solver
- 5.3.2 Multi-shift Conjugate Gradient solver
- 5.3.3 Even-odd preconditioning
- 5.3.4 Block preconditioning
- 5.3.5 Deflation acceleration
- 5.3.6 Distance preconditioning
- 5.4 Errors in Monte Carlo data
- 6 Extraction of physical observables
- 6.1 Meson masses
- 6.1.1 The spectral decomposition of correlation functions
- 6.1.2 Correlation functions and open boundary conditions
- 6.2 The generalized eigenvalue problem
- 6.3 Fitting
- 6.4 Gradient flow observables
- 6.4.1 The Wilson flow
- 6.4.2 The Zeuthen flow
- 6.4.3 Setting a scale from the flow
- 6.4.4 The gradient flow coupling in the Schrödinger functional
- 6.4.5 The topological charge from the gradient flow
- 6.5 Smearing
- 7 Heavy Quark Effective Theory
- The line of constant physics for a non-perturbative matching of HQET and QCD
- 8 Simulations along a line of constant physics
- 8.1 The line of constant physics: QCD
- 8.1.1 The running of the coupling
- 8.1.2 Interpolation of the coupling at fixed L/a
- 8.1.3 Target precision
- 8.1.4 Tuning towards the critical hopping parameter
- 8.1.5 Step scaling to the matching volume
- 8.1.6 The matching volume
- 8.2 The line of constant physics: HQET
- 8.2.1 Tuning in the matching volume
- 8.2.2 Step scaling towards large volume simulations
- 8.2.3 Contact to the large-volume simulations
- 8.3 The running of the mass
- 8.3.1 The step scaling function of the mass
- 8.3.2 Determination of RGI quark masses
- 8.3.3 Determination of the step scaling function
- 8.4 Conclusions
- 9 Algorithmic experiences
- Renormalization and Improvement from finite-volume simulations
- 10 Strategy
- 10.1 Estimators from time slice averages
- 10.2 Quark mass parametrization
- 10.3 The line of constant physics
- 11 Quark mass improvement in the strongly coupled regime of QCD
- 11.1 Gauge ensembles
- 11.2 Results
- 11.2.1 Mass parametrizations and determination of the estimators
- 11.2.2 Chiral interpolations
- 11.2.3 Interpolation in the coupling
- 11.2.4 Errors and correlations
- 11.3 Ambiguity checks
- 11.4 Estimators from time slice averages
- 11.5 Conclusions
- 12 Quark mass renormalization for the matching of QCD and HQET
- The mass of the charm quark
- 13 CLS ensembles
- 14 Determination of the charm quark mass
- 14.1 Calibration of the measurements
- 14.2 The renormalized charm quark mass from current quark masses
- 15 Lattice computation
- HQET in large volume
- 16 Heavy Quark Effective Theory with open boundary conditions
- 16.1 Setup of the measurements
- 16.2 Optimization of the variational basis
- 16.2.1 Definition of a suitable basis
- 16.2.2 Reduction of the number of smearing procedures
- 16.2.3 Variational basis from smearing method
- 16.3 Boundary effects
- 17 Computation of the B*Bpi coupling
- Conclusions
