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M. Beneke, G. Buchalla, M. Neubert, and C. T. Sachrajda, QCD factorization for B → K π , π π B\to K\pi,\pi\pi decays: Strong phases and CP violation in the heavy quark limit
1917
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A. Datta, M. Duraisamy, and D. Ghosh, Explaining the B → K ∗ μ + μ − B\to K^{\ast}\mu^{+}\mu^{-} data with scalar interactions
Original
1937
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R. Gauld, F. Goertz, and U. Haisch, On minimal Z ′ Z^{\prime} explanations of the B → K ∗ μ + μ − B\to K^{*}\mu^{+}\mu^{-} anomaly
Original
1959
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W. Buchmuller and D. Wyler, Effective Lagrangian Analysis of New Interactions and Flavor Conservation
1986
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1987
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1990
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F. Pisano and V. Pleitez, An SU(3) x U(1) model for electroweak interactions
1992
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P. H. Frampton, Chiral dilepton model and the flavor question
1992
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G. Buchalla and A. J. Buras, Qcd corrections to rare k k and b b decays for arbitrary top quark mass
1993
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G. Buchalla and A. J. Buras, sin ⁡ 2 β \sin 2\beta from k → π ν ν ¯ k\to\pi\nu\bar{\nu}
1994
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P. Colangelo, F. De Fazio, P. Santorelli, and E. Scrimieri, Rare B → K ( ∗ ) ν ν ¯ B\to K^{(*)}\nu\bar{\nu} decays at B B factories
1997
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Y. Grossman and Y. Nir, K L → π 0 ν ν ¯ K_{L}\to\pi^{0}\nu\bar{\nu} beyond the standard model
1997
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G. Buchalla and A. J. Buras, Two-loop large- m t m_{t} electroweak corrections to k → π ν ν ¯ k\to\pi\nu\bar{\nu} for arbitrary higgs boson mass
1998
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M. Misiak and J. Urban, QCD corrections to FCNC decays mediated by Z penguins and W boxes
1999
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G. Buchalla, G. Hiller, and G. Isidori, Phenomenology of non-standard Z couplings in exclusive semileptonic b → s b\to s transitions
2001
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A. J. Buras and R. Fleischer, Bounds on the unitarity triangle, sin ⁡ 2 β \sin 2\beta and K → π ν ν ¯ K\to\pi\nu\bar{\nu} decays in models with minimal flavor violation
2001
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A. J. Buras and R. Buras, A Lower bound on sin \sin 2 beta from minimal flavor violation
2001
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A. J. Buras, P. Gambino, M. Gorbahn, S. Jager, and L. Silvestrini, Universal unitarity triangle and physics beyond the standard model
2001
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G. D’Ambrosio, G. F. Giudice, G. Isidori, and A. Strumia, Minimal flavour violation: An effective field theory approach
2002
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A. J. Buras, Relations between Δ M s , d \Delta M_{s,d} and B s , d → μ + μ − B_{s,d}\to\mu^{+}\mu^{-} in models with minimal flavour violation
2003
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A. J. Buras, Minimal flavor violation
2003
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M. Pospelov and A. Ritz, Electric dipole moments as probes of new physics
2005
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A. J. Buras, M. Gorbahn, U. Haisch, and U. Nierste, The rare decay K + → π + ν ν ¯ K^{+}\to\pi^{+}\nu\bar{\nu} at the next-to-next-to-leading order in QCD
2005
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M. Gorbahn and U. Haisch, Effective Hamiltonian for non-leptonic | Δ F | = 1 |\Delta F|=1 decays at NNLO in QCD
2005
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A. J. Buras, M. Gorbahn, U. Haisch, and U. Nierste, Charm quark contribution to K + → π + ν ν ¯ K^{+}\to\pi^{+}\nu\bar{\nu} at next-to-next-to-leading order
2006
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M. Blanke, A. J. Buras, B. Duling, A. Poschenrieder, and C. Tarantino, Charged Lepton Flavour Violation and ( g − 2 ) μ (g-2)_{\mu} in the Littlest Higgs Model with T-Parity: a clear Distinction from Supersymmetry
2007
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M. Blanke and A. J. Buras, Lower bounds on Δ M s , d \Delta M_{s,d} from constrained minimal flavour violation
2007
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E. Lunghi and A. Soni, Possible Indications of New Physics in B d B_{d} -mixing and in sin ⁡ ( 2 β ) \sin(2\beta) Determinations
Original
2008
Earlier work this paper cites.
A. J. Buras and D. Guadagnoli, Correlations among new CP violating effects in Δ F = 2 \Delta F=2 observables
Original
2008
Earlier work this paper cites.
U. Nierste, S. Trine, and S. Westhoff, Charged-Higgs effects in a new B → D τ ν B\to D\tau\nu differential decay distribution
Original
2008
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J. F. Kamenik and F. Mescia, B → D τ ν B\to D\tau\nu Branching Ratios: Opportunity for Lattice QCD and Hadron Colliders
Original
2008
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M. Raidal et al., Flavour physics of leptons and dipole moments
Original
2008
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J. Brod and M. Gorbahn, Electroweak Corrections to the Charm Quark Contribution to K + → π + ν ν ¯ K^{+}\to\pi^{+}\nu\bar{\nu}
Original
2008
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T. Hurth, G. Isidori, J. F. Kamenik, and F. Mescia, Constraints on New Physics in MFV models: A Model-independent analysis of Δ F = \Delta F= 1 processes
Original
2009
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G. Isidori, Y. Nir, and G. Perez, Flavor Physics Constraints for Physics Beyond the Standard Model
Original
2010
Earlier work this paper cites.
B. Grzadkowski, M. Iskrzynski, M. Misiak, and J. Rosiek, Dimension-Six Terms in the Standard Model Lagrangian
Original
2010
Earlier work this paper cites.
A. J. Buras, Minimal flavour violation and beyond: Towards a flavour code for short distance dynamics
Original
2010
Earlier work this paper cites.

Similar

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M. Blanke, Insights from the Interplay of K → π ν ν ¯ K\rightarrow\pi\nu\overline{\nu} and ϵ K \epsilon_{K} on the New Physics Flavour Structure
Original
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R. Barlow, The PRISM/PRIME project
2011
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T. Feldmann, Lepton Flavour Violation Theory
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R. Barbieri, P. Campli, G. Isidori, F. Sala, and D. M. Straub, B-decay CP-asymmetries in SUSY with a U ( 2 ) 3 U(2)^{3} flavour symmetry
Original
2011
Cited alongside, same era.

Then

A. J. Buras, F. De Fazio, J. Girrbach, R. Knegjens, and M. Nagai, The Anatomy of Neutral Scalars with FCNCs in the Flavour Precision Era
Original
2013
Later among the works it cites.
A. J. Buras, F. De Fazio, J. Girrbach, and M. V. Carlucci, The Anatomy of Quark Flavour Observables in 331 Models in the Flavour Precision Era
Original
2013
Later among the works it cites.
S. Descotes-Genon, J. Matias, and J. Virto, Understanding the B → K ∗ μ + μ − B\to K^{*}\mu^{+}\mu^{-} Anomaly
Original
2013
Later among the works it cites.
C. Bobeth, G. Hiller, and D. van Dyk, General Analysis of B ¯ → K ¯ ( ∗ ) ℓ + ℓ − \bar{B}\to\bar{K}^{(*)}\ell^{+}\ell^{-} Decays at Low Recoil
Original
2013
Later among the works it cites.
S. Jager and J. M. Camalich, On B → V ℓ ℓ B\to V\ell\ell at small dilepton invariant mass, power corrections, and new physics

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2015

Flavour Expedition to the Zeptouniverse

Buras, Andrzej J.

Understand

After the completion of the Standard Model (SM) through the Higgs discovery particle physicists are waiting for the discovery of new particles either directly with the help of the Large Hadron Collider (LHC) or indirectly through quantum fluctuations causing certain rare processes to occur at different rates than predicted by the SM.

While the later route is very challenging, requiring very precise theory and experiment, it allows a much higher resolution of short distance scales than it is possible with the help of the LHC.
In fact in the coming flavour precision era, in which the accuracy of the measurements of rare processes and of the relevant lattice QCD calculations will be significantly increased, there is a good chance that we may get an insight into the scales as short as 10^{-21} m (Zeptouniverse) corresponding to energy scale of 200 TeV or even shorter distance scales.
We discuss the requirements that have to be met for such a flavour expedition to the Zeptouniverse to be successful.