Abstract

We present a detailed theoretical analysis of very rare, exclusive hadronic decays of the electroweak gauge bosons V=W, Z from first principles of QCD. Our main focus is on the radiative decays V->M+gamma, in which M is a pseudoscalar or vector meson. At leading order in an expansion in powers of Lambda_{QCD}/m_V the decay amplitudes can be factorized into convolutions of calculable hard-scattering coefficients with the leading-twist light-cone distribution amplitude of the meson M. Power corrections to the decay rates arise first at order (Lambda_{QCD}/m_V)^2. They can be estimated in terms of higher-twist distribution amplitudes and are predicted to be tiny. We include one-loop O(alpha_s) radiative corrections to the hard-scattering coefficients and perform the resummation of large logarithms [alpha_s log(m_V^2/mu_0^2)]^n (with mu_0=1 GeV a typical hadronic scale) to all orders in perturbation theory. Evolution effects have an important impact both numerically and conceptually, since they reduce the sensitivity to poorly determined hadronic parameters. We present detailed numerical predictions and error estimates, which can serve as benchmarks for future precision measurements. We also present an exploratory study of the weak radiative decays Z->M+W. Some of the decay modes studied here have branching ratios large enough to be accessible in the high-luminosity run of the LHC. Many of them can be measured with high accuracy at a future lepton collider. This will provide stringent tests of the QCD factorization formalism and enable novel searches for new physics.

Highlights

  • Be derived, in which all non-perturbative physics associated with the initial-state nucleon can be described in te√rms of parton distribution functions (PDFs), up to power corrections suppressed by ΛQCD/ s

  • We present a comprehensive analysis of a large class of radiative decays of W and Z bosons using the QCD factorization approach, including for the first time a consistent treatment of O(αs) corrections and performing the resummation of large logarithms of order αs ln(m2Z /μ20) n, with μ0 ≈ 1 GeV, to all orders in perturbation theory

  • The basis of our study is a factorization theorem derived in soft-collinear effective theory, which expresses the decay amplitudes as convolutions of calculable hard-scattering kernels with light-cone distribution amplitudes (LCDAs), in a systematic expansion in powers of (ΛQCD/mZ,W )2 and2

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Summary

Theoretical framework

Our main focus in this work is on the rare, exclusive radiative decays Z → M γ and W → M γ, where M denotes a pseudoscalar or vector meson. We assign momentum k to the final-state meson and q to the photon. The decay plane is spanned by the vectors k and q. We only consider cases where the mass of the final-state meson satisfies mM ≪ mZ. Up to corrections suppressed as (mM /mZ ), this mass can be set to zero. In this limit, we have kμ = Enμ and qμ = Enμ, where E = mZ /2 is the energy of the final-state particles in the Z-boson rest frame, and n and nare two light-like vectors satisfying n · n = 2

Derivation of the factorization formula
Systematics of the Gegenbauer expansion
Radiative corrections and RG evolution
Flavor wave functions of neutral mesons
Radiative decays of electroweak gauge bosons
Radiative hadronic decays of Z bosons
Radiative hadronic decays of W bosons
Absence of enhanced contributions from the axial anomaly
Phenomenological results
Experimental considerations
Summary and conclusions
A Light-cone projectors for vector mesons
B Determinations of meson decay constants
C Gegenbauer expansion of the convolution integrals
Findings
D Connection with the approach by Manohar
Full Text
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