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SCET Insights Into Heavy-to-Light Form Factors
Matthias Neubert - Cornell December 13, 2003 Vxb Workshop - SLAC
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Some Open Issues Field-theoretic understanding of the “soft overlap” contribution Systematic separation of short- and long-distance contributions Sudakov suppression of the soft contribution? pQCD vs. QCD factorization
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Soft Overlap Have used SCET to define the soft overlap term: [Lange, Neubert: hep-ph/ ] Combination of soft, collinear and messenger contributions
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More Artistic View Messenger exchange: soft collinear messenger sector
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Sudakov Resummation Can use SCET to systematically resum all short-distance Sudakov logarithms: for physical values of the B-meson mass, there is no sizable Sudakov suppression E-dependence of the low-energy matrix element remains, which can only be controlled using a truly non-perturbative approach (lattice?) 0.5 0.75 αs(μ) = 1
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Importance of Non-Valence Fock States ?
SCET shows that 3-particle Fock states (in both B and π) contribute at the same order in Λ/mb as the leading Fock states Not suppressed by any small parameter A puzzle (to us) is why their effect appears to be tiny (<3%) in the light-cone sum rule approach
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Toy Model Regularize endpoint singularities using cut-offs adjusted such that the leading Fock states reproduce LCSR (crude):
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Result Find potentially large effects, which tend to reduce the values of the form factors Effects tend to be larger for B V form factors Is this effect real? Could it indicate a problem with light-cone sum rules (continuum model)?
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Summary Physics of heavy-to-light form factors is subtle:
Transformation of soft collinear partons Subleading quantities in SCET power counting (vanish at leading order) This physics is not captured in quark models (ISGW, BSW, …) based on wave-function overlap integrals
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