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Dive into the research topics where E. D. Freeland is active.

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Featured researches published by E. D. Freeland.


Physical Review Letters | 2005

Charmed-meson decay constants in three-flavor lattice QCD

C. Aubin; C. Bernard; Carleton DeTar; M. Di Pierro; E. D. Freeland; Steven Gottlieb; U. M. Heller; James Edward Hetrick; A. X. El-Khadra; Andreas S. Kronfeld; L. Levkova; Paul B. Mackenzie; D. Menscher; F. Maresca; M. Nobes; M. Okamoto; Dru B. Renner; James N. Simone; R. L. Sugar; D. Toussaint; Howard D. Trottier

We present the first lattice QCD calculation with realistic sea quark content of the D+-meson decay constant f(D+). We use the MILC Collaborations publicly available ensembles of lattice gauge fields, which have a quark sea with two flavors (up and down) much lighter than a third (strange). We obtain f(D+)=201+/-3+/-17 MeV, where the errors are statistical and a combination of systematic errors. We also obtain f(Ds)=249+/-3+/-16 MeV for the Ds meson.


Physical Review D | 2009

B̄→D*ℓν̄ form factor at zero recoil from three-flavor lattice QCD: A model independent determination of |Vcb|

C. Bernard; Carleton DeTar; M. Di Pierro; A. X. El-Khadra; R. T. Evans; E. D. Freeland; E. Gamiz; Steven Gottlieb; U. M. Heller; James Edward Hetrick; Andreas S. Kronfeld; J. Laiho; L. Levkova; Paul B. Mackenzie; M. Okamoto; James N. Simone; R. L. Sugar; D. Toussaint; R. S. Van De Water

We present the first lattice QCD calculation of the form factor for B → D*lv with three flavors of sea quarks. We use an improved staggered action for the light valence and sea quarks (the MILC configurations), and the Fermilab action for the heavy quarks. The form factor is computed at zero recoil using a new double ratio method that yields the form factor more directly than the previous Fermilab method. Other improvements over the previous calculation include the use of much lighter light-quark masses, and the use of lattice (staggered) chiral perturbation theory in order to control the light-quark discretization errors and chiral extrapolation. We obtain for the form factor, F B→D * (1) = 0.921(13)(20), where the first error is statistical and the second is the sum of all systematic errors in quadrature. Applying a 0.7% electromagnetic correction and taking the latest PDG average for F B→D * (1)|V cb | leads to |V rb | = (38.7 ± 0.9 exp ± 1.0 theo ) X 10 -3 .


Physical Review Letters | 2012

Refining New-Physics Searches inB→Dτνwith Lattice QCD

Jon A. Bailey; A. Bazavov; C. Bernard; C. M. Bouchard; Carleton E. DeTar; Daping Du; A.X. El-Khadra; J. Foley; E. D. Freeland; E. Gamiz; Steven Gottlieb; Urs M. Heller; Jongjeong Kim; A. S. Kronfeld; J. Laiho; L. Levkova; P.B. Mackenzie; Y. Meurice; E. T. Neil; M.B. Oktay; Si-Wei Qiu; J.N. Simone; R. Sugar; D. Toussaint; R. S. Van De Water; Ran Zhou

The semileptonic decay channel B→Dτν is sensitive to the presence of a scalar current, such as that mediated by a charged-Higgs boson. Recently, the BABAR experiment reported the first observation of the exclusive semileptonic decay B→Dτ(-)ν, finding an approximately 2σ disagreement with the standard-model prediction for the ratio R(D)=BR(B→Dτν)/BR(B→Dℓν), where ℓ = e,μ. We compute this ratio of branching fractions using hadronic form factors computed in unquenched lattice QCD and obtain R(D)=0.316(12)(7), where the errors are statistical and total systematic, respectively. This result is the first standard-model calculation of R(D) from ab initio full QCD. Its error is smaller than that of previous estimates, primarily due to the reduced uncertainty in the scalar form factor f(0)(q(2)). Our determination of R(D) is approximately 1σ higher than previous estimates and, thus, reduces the tension with experiment. We also compute R(D) in models with electrically charged scalar exchange, such as the type-II two-Higgs-doublet model. Once again, our result is consistent with, but approximately 1σ higher than, previous estimates for phenomenologically relevant values of the scalar coupling in the type-II model. As a by-product of our calculation, we also present the standard-model prediction for the longitudinal-polarization ratio P(L)(D)=0.325(4)(3).


Physical Review D | 2014

Update of

Jon A. Bailey; R. S. Van De Water; A. S. Kronfeld; P.B. Mackenzie; J.N. Simone; Si-Wei Qiu; E. T. Neil; J. Laiho; D. Toussaint; L. Levkova; Daping Du; A.X. El-Khadra; E. D. Freeland; A. Bazavov; Urs M. Heller; Steven Gottlieb; Ran Zhou; C. Bernard; Carleton DeTar; J. Foley; R. Sugar; E. Gamiz; C. M. Bouchard

We compute the zero-recoil form factor for the semileptonic decay


arXiv: High Energy Physics - Lattice | 2015

|V_{cb}|

S. Basak; A. Bazavov; C. Bernard; Carleton DeTar; E. D. Freeland; J. Foley; Steven Gottlieb; U. M. Heller; J. Komijani; J. Laiho; L. Levkova; James C. Osborn; R. L. Sugar; A. Torok; D. Toussaint; R. S. Van De Water; Ran Zhou

\bar{B}^0\to D^{*+}\ell^-\bar{\nu}


arXiv: High Energy Physics - Lattice | 2005

from the

Andreas S. Kronfeld; Ian F. Allison; Christopher Alan Aubin; C. Bernard; C. T. H. Davies; Carleton E. DeTar; M. Di Pierro; E. D. Freeland; Steven Gottlieb; Alan Gray; E. Gregor; J.E. Hetrick; A. X. El-Khadra; L. Levkova; P.B. Mackenzie; F. Maresca; D. Menscher; M. Nobes; M. Okamoto; M.B. Oktay; U Glasgow; U Columbia; U Utah; U DePaul; U Indiana; U Arizona; New York Aps; Stockton U. Pacific; Urbana Illinois U.; Santa Barbara Uc

(and modes related by isospin and charge conjugation) using lattice QCD with three flavors of sea quarks. We use an improved staggered action for the light valence and sea quarks (the MILC \asqtad\ configurations), and the Fermilab action for the heavy quarks. Our calculations incorporate higher statistics, finer lattice spacings, and lighter quark masses than our 2008 work. As a byproduct of tuning the new data set, we obtain the


arXiv: High Energy Physics - Lattice | 2015

\bar{B}\to D^*\ell\bar{\nu}

C. M. Bouchard; E. D. Freeland; C. Bernard; Chia Cheng Chang; A. X. El-Khadra; M. Elvira Gámiz; A. S. Kronfeld; J. Laiho; Ruth S. Van de Water

D_s


Physical Review D | 2014

form factor at zero recoil with three-flavor lattice QCD

Jon A. Bailey; A. Bazavov; C. Bernard; C. M. Bouchard; Carleton E. DeTar; Daping Du; A.X. El-Khadra; J. Foley; E. D. Freeland; E. Gamiz; Steven Gottlieb; Urs M. Heller; A. S. Kronfeld; J. Laiho; L. Levkova; P.B. Mackenzie; E. T. Neil; Si-Wei Qiu; J.N. Simone; R. Sugar; D. Toussaint; R. S. Van De Water; Ran Zhou

and


Proceedings of The XXVIII International Symposium on Lattice Field Theory — PoS(Lattice 2010) | 2011

Finite-volume effects and the electromagnetic contributions to kaon and pion masses

E. D. Freeland; C. Bernard

B_s


International Journal of Modern Physics A | 2006

Predictions from Lattice QCD

Andreas S. Kronfeld; Ian F. Allison; C. Aubin; C. Bernard; C. T. H. Davies; Carleton DeTar; M. Di Pierro; E. D. Freeland; Steven Gottlieb; Alan Gray; Eric Brittain Gregory; U. M. Heller; James Edward Hetrick; A. X. El-Khadra; L. Levkova; Paul B. Mackenzie; F. Maresca; D. Menscher; M. Nobes; M. Okamoto; M.B. Oktay; J. Osborn; Dru B. Renner; James N. Simone; R. L. Sugar; D. Toussaint; Howard D. Trottier

hyperfine splittings with few-MeV accuracy. For the zero-recoil form factor, we obtain

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C. Bernard

Washington University in St. Louis

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Urs M. Heller

Florida State University

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Carleton E. DeTar

Washington University in St. Louis

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