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<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi mathvariant="normal">SU</mml:mi><mml:mrow><mml:msub><mml:mrow><mml:mn/><mml:mo>(</mml:mo><mml:mn>3</mml:mn><mml:mo>)</mml:mo><mml:mn/></mml:mrow><mml:mrow><mml:mi>E</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>-invariant form factor for pseudoscalar mesons

Arno Böhm,M. Igarashi,J. Werle-1977-05-01-Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields
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TL;DRAbstract

The use of a form factor which is invariant with respect to the spectrum-generating SU(3) leads to a definition for the strangeness-changing suppression factor for ${K}_{{l}_{3}}$ decay which is numerically equal to the strangeness-changing suppression factor for ${K}_{{l}_{2}}$ decay and close to $\frac{{m}_{\ensuremath{\pi}}}{{m}_{K}}$. It also predicts the electromagnetic radius of the pseudoscalar mesons in terms of ${\ensuremath{\lambda}}_{+}$.

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The use of a form factor which is invariant with respect to the spectrum-generating SU(3) leads to a definition for the strangeness-changing suppression factor for ${K}_{{l}_{3}}$ decay which is numerically equal to the strangeness-changing suppression factor for ${K}_{{l}_{2}}$ decay and close to $\frac{{m}_{\ensuremath{\pi}}}{{m}_{K}}$. It also predicts the electromagnetic radius of the pseudoscalar mesons in terms of ${\ensuremath{\lambda}}_{+}$.

Keywords

StrangenessPhysicsLambdaParticle physicsHadronCrystallographyQuantum mechanicsChemistry

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