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Related papers: Partially Quenched and Three Flavour ChPT at Two L…

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A brief introduction to the low-energy effective field theory of the standard model, chiral perturbation theory, is presented.

High Energy Physics - Phenomenology · Physics 2007-05-23 Bastian Kubis

We test the positivity property of the chiral perturbation theory (ChPT) pion-pion scattering amplitudes within the Mandelstam triangle. In the one-loop approximation, ${\cal O}(p^4)$, the positivity constrains only the coefficients $b_3$…

High Energy Physics - Phenomenology · Physics 2009-10-31 Petre Diţă

We calculate all neutral vector two-point functions in Chiral Perturbation Theory (ChPT) to two-loop order and use these to estimate the ratio of disconnected to connected contributions as well as contributions involving the strange quark.…

High Energy Physics - Lattice · Physics 2016-12-21 Johan Bijnens , Johan Relefors

Using quenched chiral perturbation theory, we compute the long-distance behaviour of two-point functions of flavour non-singlet axial and vector currents in a finite volume, for small quark masses, and at a fixed gauge-field topology. We…

High Energy Physics - Lattice · Physics 2010-04-05 P. H. Damgaard , P. Hernandez , K. Jansen , M. Laine , L. Lellouch

This talk summarizes recent progress in lattice QCD for dense quark matter. The emphasis is on the insights obtained from analytical results derived within chiral perturbation theory.

High Energy Physics - Lattice · Physics 2009-12-23 M. P. Lombardo , K. Splittorff , J. J. M. Verbaarschot

This talk first discusses some aspects of the chiral expansion with three light flavours related to the (non) applicability of the OZI rule. Next, the extension of ChPT to an effective theory of the full standard model is considered. Some…

High Energy Physics - Phenomenology · Physics 2009-11-11 Bachir Moussallam

Parameters and light fields of the QCD Lagrangian with two heavy flavours, b and c, are related to those in the low-energy effective theory without these flavours, to three-loop accuracy taking into account the exact dependence on m_c/m_b.…

High Energy Physics - Phenomenology · Physics 2012-05-29 Andrey Grozin , Maik Höschele , Jens Hoff , Matthias Steinhauser

The corrections induced by light quark masses to the current algebra result for the $\pi^0$ lifetime are reexamined. We consider NNLO corrections and we compute all the one-loop and the two-loop diagrams which contribute to the decay…

High Energy Physics - Phenomenology · Physics 2010-01-05 Karol Kampf , Bachir Moussallam

Chiral perturbation theory in the two-flavour sector allows one to analyse Green functions in QCD in a limit where the strange quark mass is considered to be large in comparison to the external momenta and to the light quark masses. In this…

High Energy Physics - Phenomenology · Physics 2009-07-28 Juerg Gasser , Christoph Haefeli , Mikhail A. Ivanov , Martin Schmid

I present a quick overview of the current status of Chiral perturbation theory in the meson sector. To illustrate the successes and some problems in the description of the phenomenology, I focus on a few selected examples that are relevant…

High Energy Physics - Phenomenology · Physics 2007-05-23 Gilberto Colangelo

I describe recent progress towards a theory of the NN force which captures the consequences of QCD's chiral symmetry and the pattern of its breaking, and is formulated as an expansion in a ratio of low and high mass scales, M_{lo}/M_{hi}.…

Nuclear Theory · Physics 2013-02-26 Daniel R. Phillips

Recently, we pointed out that chiral transformation properties of penguin operators change in the transition from unquenched to (partially) quenched QCD. As a consequence, new operators appear in (partially) quenched QCD penguins,…

High Energy Physics - Lattice · Physics 2009-11-07 Maarten Golterman , Elisabetta Pallante

We give a brief introduction to chiral perturbation theory in its various settings. We discuss some applications of recent interest including chiral extrapolations for lattice gauge theory.

High Energy Physics - Phenomenology · Physics 2008-11-26 Véronique Bernard , Ulf-G. Meißner

QCD with two flavours of massless colour-sextet quarks is considered as a model for conformal/walking Technicolor. If this theory possess an infrared fixed point, as indicated by 2-loop perturbation theory, it is a conformal(unparticle)…

High Energy Physics - Lattice · Physics 2014-11-20 J. B. Kogut , D. K. Sinclair

In highly improved staggered quark (HISQ) simulations by the HPQCD, MILC, and Fermilab Lattice collaborations, both the light quarks and the charm quark are staggered. We extend chiral perturbation theory for staggered quarks to include…

High Energy Physics - Lattice · Physics 2013-11-27 Claude Bernard , Javad Komijani

We show how quark-disconnected and quark-connected contributions to hadronic n-point functions can be written as independent correlators for which one can derive expressions in partially quenched chiral effective theory. As an example we…

High Energy Physics - Lattice · Physics 2010-12-06 Michele Della Morte , Andreas Juttner

The current state of knowledge of the order parameters of the spontaneously broken chiral symmetry, the quark condensate and the pseudoscalar decay constant in the chiral limit, is briefly reviewed, based on available phenomenological fits…

High Energy Physics - Phenomenology · Physics 2020-12-14 Marián Kolesár , Jiří Novotný

Recent work in low energy pion physics is reviewed. One of the exciting new developments in this field is that simulations of QCD on a lattice now start providing information about the low energy structure of the continuum theory, for…

High Energy Physics - Phenomenology · Physics 2017-08-23 H. Leutwyler

Perturbation theory (PT) might be one of the most powerful and fruitful tools for both physicists and chemists, which evoked an explosion of applications with the blooming of atomic and subatomic physics. Even though PT is well-used today,…

Quantum Physics · Physics 2023-05-16 Junxu Li , Barbara A. Jones , Sabre Kais

Within Chiral Perturbation Theory (CHPT) we compute the form factors A, V and $\gamma = A/V$ in the $\pi \to \nu l \gamma$ decay to $O(p^6)$. A and $\gamma$ obtain corrections of order 25%.

High Energy Physics - Phenomenology · Physics 2016-09-06 J. Bijnens , P. Talavera