# P. Mackenzie - Fermilab

## Contact Details

NameP. Mackenzie |
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AffiliationFermilab |
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CountryUnited States |
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## Pubs By Year |
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## External Links |
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## Pub CategoriesHigh Energy Physics - Lattice (44) High Energy Physics - Phenomenology (33) High Energy Physics - Experiment (12) |

## Publications Authored By P. Mackenzie

**Authors:**J. Komijani, A. Bazavov, C. Bernard, N. Brambilla, N. Brown, C. DeTar, D. Du, A. X. El-Khadra, E. D. Freeland, E. Gámiz, Steven Gottlieb, U. M. Heller, A. S. Kronfeld, J. Laiho, P. B. Mackenzie, C. Monahan, Heechang Na, E. T. Neil, J. N. Simone, R. L. Sugar, D. Toussaint, A. Vairo, R. S. Van de Water

We present a progress report on our calculation of the decay constants $f_B$ and $f_{B_s}$ from lattice-QCD simulations with highly-improved staggered quarks. Simulations are carried out with several heavy valence-quark masses on $(2+1+1)$-flavor ensembles that include charm sea quarks. We include data at six lattice spacings and several light sea-quark masses, including an approximately physical-mass ensemble at all but the smallest lattice spacing, 0. Read More

We discuss the reduction of errors in the calculation of the form factor $f_+^{K \pi}(0)$ with HISQ fermions on the $N_f=2+1+1$ MILC configurations from increased statistics on some key ensembles, new data on ensembles with lattice spacings down to 0.042 fm and the study of finite-volume effects within staggered ChPT. We also study the implications for the unitarity of the CKM matrix in the first row and for current tensions with leptonic determinations of $\vert V_{us}\vert$. Read More

We calculate---for the first time in three-flavor lattice QCD---the hadronic matrix elements of all five local operators that contribute to neutral $B^0$- and $B_s$-meson mixing in and beyond the Standard Model. We present a complete error budget for each matrix element and also provide the full set of correlations among the matrix elements. We also present the corresponding bag parameters and their correlations, as well as specific combinations of the mixing matrix elements that enter the expression for the neutral $B$-meson width difference. Read More

**Authors:**David d'Enterria

^{1}, Peter Z. Skands

^{2}, S. Alekhin, A. Banfi, S. Bethke, J. Blümlein, K. G. Chetyrkin, D. d'Enterria, G. Dissertori, X. Garcia i Tormo, A. H. Hoang, M. Klasen, T. Klijnsma, S. Kluth, J. -L. Kneur, B. A. Kniehl, D. W. Kolodrubetz, J. Kühn, P. Mackenzie, B. Malaescu, V. Mateu, L. Mihaila, S. Moch, K. Mönig, R. Perez-Ramos, A. Pich, J. Pires, K. Rabbertz, G. P. Salam, F. Sannino, J. Soto i Riera, M. Srebre, I. W. Stewart

**Affiliations:**

^{1}eds.,

^{2}eds.

This document provides a writeup of all contributions to the workshop on "High precision measurements of $\alpha_s$: From LHC to FCC-ee" held at CERN, Oct. 12--13, 2015. The workshop explored in depth the latest developments on the determination of the QCD coupling $\alpha_s$ from 15 methods where high precision measurements are (or will be) available. Read More

**Authors:**Fermilab Lattice

^{1}, MILC Collaborations

^{2}, :

^{3}, A. Bazavov

^{4}, C. Bernard

^{5}, C. Bouchard

^{6}, N. Brown

^{7}, C. DeTar

^{8}, D. Du

^{9}, A. X. El-Khadra

^{10}, E. D. Freeland

^{11}, E. Gámiz

^{12}, Steven Gottlieb

^{13}, U. M. Heller

^{14}, J. Komijani

^{15}, A. S. Kronfeld

^{16}, J. Laiho

^{17}, L. Levkova

^{18}, P. B. Mackenzie

^{19}, C. Monahan

^{20}, T. Primer

^{21}, Heechang Na

^{22}, E. T. Neil

^{23}, J. N. Simone

^{24}, R. L. Sugar

^{25}, D. Toussaint

^{26}, R. S. Van de Water

^{27}, R. Zhou

^{28}

**Affiliations:**

^{1}U Iowa,

^{2}U Iowa,

^{3}U Iowa,

^{4}U Iowa,

^{5}Wash U,

^{6}William and Mary U,

^{7}Wash U,

^{8}U Utah,

^{9}Syracuse U,

^{10}U Illinois Urbana,

^{11}School of the Art Institute of Chicago,

^{12}U Granada,

^{13}Indiana U,

^{14}APS,

^{15}Wash U,

^{16}Fermilab,

^{17}Syracuse U,

^{18}U Utah,

^{19}Fermilab,

^{20}U Utah,

^{21}U Arizona,

^{22}U Utah,

^{23}U Colorado,

^{24}Fermilab,

^{25}UC Santa Barbara,

^{26}U Arizona,

^{27}Fermilab,

^{28}Fermilab

**Category:**High Energy Physics - Lattice

We give a progress report on a project aimed at a high-precision calculation of the decay constants $f_B$ and $f_{B_s}$ from simulations with HISQ heavy and light valence and sea quarks. Calculations are carried out with several heavy valence-quark masses on ensembles with 2+1+1 flavors of HISQ sea quarks at five lattice spacings and several light sea-quark mass ratios $m_{ud}/m_s$, including approximately physical sea-quark masses. This range of parameters provides excellent control of the continuum limit and of heavy-quark discretization errors. Read More

**Authors:**Jon A. Bailey, A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, Daping Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gámiz, Steven Gottlieb, U. M. Heller, R. D. Jain, J. Komijani, A. S. Kronfeld, J. Laiho, L. Levkova, Yuzhi Liu, P. B. Mackenzie, Y. Meurice, E. T. Neil, Si-Wei Qiu, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water, Ran Zhou

We compute the form factors for the $B \to Kl^+l^-$ semileptonic decay process in lattice QCD using gauge-field ensembles with 2+1 flavors of sea quark, generated by the MILC Collaboration. The ensembles span lattice spacings from 0.12 to 0. Read More

**Authors:**Jon A. Bailey, A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, Daping Du, A. X. El-Khadra, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, A. S. Kronfeld, J. Laiho, L. Levkova, Yuzhi Liu, E. Lunghi, P. B. Mackenzie, Y. Meurice, E. Neil, Si-Wei Qiu, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water, Ran Zhou

The rare decay $B\to\pi\ell^+\ell^-$ arises from $b\to d$ flavor-changing neutral currents and could be sensitive to physics beyond the Standard Model. Here, we present the first $ab$-$initio$ QCD calculation of the $B\to\pi$ tensor form factor $f_T$. Together with the vector and scalar form factors $f_+$ and $f_0$ from our companion work [J. Read More

**Authors:**Fermilab Lattice

^{1}, MILC Collaborations

^{2}, :

^{3}, Jon A. Bailey

^{4}, A. Bazavov

^{5}, C. Bernard

^{6}, C. M. Bouchard

^{7}, C. DeTar

^{8}, Daping Du

^{9}, A. X. El-Khadra

^{10}, J. Foley

^{11}, E. D. Freeland

^{12}, E. Gámiz

^{13}, Steven Gottlieb

^{14}, U. M. Heller

^{15}, J. Komijani

^{16}, A. S. Kronfeld

^{17}, J. Laiho

^{18}, L. Levkova

^{19}, Yuzhi Liu

^{20}, P. B. Mackenzie

^{21}, Y. Meurice

^{22}, E. T. Neil

^{23}, Si-Wei Qiu

^{24}, J. Simone

^{25}, R. Sugar

^{26}, D. Toussaint

^{27}, R. S. Van de Water

^{28}, Ran Zhou

^{29}

**Affiliations:**

^{1}Seoul Nat. U,

^{2}Seoul Nat. U,

^{3}Seoul Nat. U,

^{4}Seoul Nat. U,

^{5}BNL,

^{6}Washington U,

^{7}College of William and Mary,

^{8}U. Utah,

^{9}U. Illinois,

^{10}U. Illinois,

^{11}U. Utah,

^{12}School of the Art Institute of Chicago,

^{13}U. Granada,

^{14}Indiana U,

^{15}American Physical Society,

^{16}Washington U,

^{17}FNAL,

^{18}Syracuse U,

^{19}U. Utah,

^{20}U. Colorado,

^{21}FNAL,

^{22}U. Iowa,

^{23}U. Colorado,

^{24}U. Utah,

^{25}FNAL,

^{26}U. California Santa Barbara,

^{27}U. Arizona,

^{28}FNAL,

^{29}Indiana U

We present a lattice-QCD calculation of the $B\to\pi\ell\nu$ semileptonic form factors and a new determination of the CKM matrix element $|V_{ub}|$. We use the MILC asqtad 2+1-flavor lattice configurations at four lattice spacings and light-quark masses down to 1/20 of the physical strange-quark mass. We extrapolate the lattice form factors to the continuum using staggered chiral perturbation theory in the hard-pion and SU(2) limits. Read More

**Authors:**Fermilab Lattice

^{1}, MILC Collaborations

^{2}, :

^{3}, Jon A. Bailey

^{4}, A. Bazavov

^{5}, C. Bernard

^{6}, C. M. Bouchard

^{7}, C. DeTar

^{8}, Daping Du

^{9}, A. X. El-Khadra

^{10}, J. Foley

^{11}, E. D. Freeland

^{12}, E. Gámiz

^{13}, Steven Gottlieb

^{14}, U. M. Heller

^{15}, J. Komijani

^{16}, A. S. Kronfeld

^{17}, J. Laiho

^{18}, L. Levkova

^{19}, P. B. Mackenzie

^{20}, E. T. Neil

^{21}, Si-Wei Qiu

^{22}, J. Simone

^{23}, R. Sugar

^{24}, D. Toussaint

^{25}, R. S. Van de Water

^{26}, Ran Zhou

^{27}

**Affiliations:**

^{1}Seoul Nat. U,

^{2}Seoul Nat. U,

^{3}Seoul Nat. U,

^{4}Seoul Nat. U,

^{5}BNL,

^{6}Washington U,

^{7}College of William and Mary,

^{8}U. Utah,

^{9}U. Illinois,

^{10}U. Illinois,

^{11}U. Utah,

^{12}School of the Art Institute of Chicago,

^{13}U. Granada,

^{14}Indiana U,

^{15}American Physical Society,

^{16}Washington U,

^{17}FNAL,

^{18}Syracuse U,

^{19}U. Utah,

^{20}FNAL,

^{21}U. Colorado,

^{22}U. Utah,

^{23}FNAL,

^{24}U. California Santa Barbara,

^{25}U. Arizona,

^{26}FNAL,

^{27}Indiana U

**Category:**High Energy Physics - Lattice

We present the first unquenched lattice-QCD calculation of the hadronic form factors for the exclusive decay $\overline{B} \rightarrow D \ell \overline{\nu}$ at nonzero recoil. We carry out numerical simulations on fourteen ensembles of gauge-field configurations generated with 2+1 flavors of asqtad-improved staggered sea quarks. The ensembles encompass a wide range of lattice spacings (approximately 0. Read More

**Authors:**J. A. Bailey, A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, A. S. Kronfeld, J. Laiho, L. Levkova, Yuzhi Liu, P. B. Mackenzie, Y. Meurice, E. T. Neil, S. Qiu, J. N. Simone, R. L. Sugar, D. Toussaint, R. S. Van de Water, R. Zhou

**Category:**High Energy Physics - Lattice

We compute the $B\to\pi\ell\nu$ semileptonic form factors and update the determination of the CKM matrix element $|V_{ub}|$. We use the MILC asqtad ensembles with $N_f=2+1$ sea quarks at four different lattice spacings in the range $a \approx 0.045$~fm to $0. Read More

**Authors:**A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gámiz, Steven Gottlieb, U. M. Heller, J. Kim, J. Komijani, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, E. T. Neil, J. N. Simone, R. L. Sugar, D. Toussaint, R. S. Van de Water, R. Zhou

**Category:**High Energy Physics - Lattice

We compute the leptonic decay constants $f_{D^+}$, $f_{D_s}$, and $f_{K^+}$, and the quark-mass ratios $m_c/m_s$ and $m_s/m_l$ in unquenched lattice QCD. We use the MILC highly improved staggered quark (HISQ) ensembles with four dynamical quark flavors. Our primary results are $f_{D^+} = 212. Read More

**Authors:**A. Bazavov

^{1}, C. Bernard

^{2}, C. M. Bouchard

^{3}, C. DeTar

^{4}, D. Du

^{5}, A. X. El-Khadra

^{6}, J. Foley

^{7}, E. D. Freeland

^{8}, E. Gámiz

^{9}, Steven Gottlieb

^{10}, U. M. Heller

^{11}, J. Kim

^{12}, J. Komijani

^{13}, A. S. Kronfeld

^{14}, J. Laiho

^{15}, L. Levkova

^{16}, P. B. Mackenzie

^{17}, E. T. Neil

^{18}, J. N. Simone

^{19}, R. Sugar

^{20}, D. Toussaint

^{21}, R. S. Van de Water

^{22}, R. Zhou

^{23}

**Affiliations:**

^{1}Fermilab Lattice and MILC Collaborations,

^{2}Fermilab Lattice and MILC Collaborations,

^{3}Fermilab Lattice and MILC Collaborations,

^{4}Fermilab Lattice and MILC Collaborations,

^{5}Fermilab Lattice and MILC Collaborations,

^{6}Fermilab Lattice and MILC Collaborations,

^{7}Fermilab Lattice and MILC Collaborations,

^{8}Fermilab Lattice and MILC Collaborations,

^{9}Fermilab Lattice and MILC Collaborations,

^{10}Fermilab Lattice and MILC Collaborations,

^{11}Fermilab Lattice and MILC Collaborations,

^{12}Fermilab Lattice and MILC Collaborations,

^{13}Fermilab Lattice and MILC Collaborations,

^{14}Fermilab Lattice and MILC Collaborations,

^{15}Fermilab Lattice and MILC Collaborations,

^{16}Fermilab Lattice and MILC Collaborations,

^{17}Fermilab Lattice and MILC Collaborations,

^{18}Fermilab Lattice and MILC Collaborations,

^{19}Fermilab Lattice and MILC Collaborations,

^{20}Fermilab Lattice and MILC Collaborations,

^{21}Fermilab Lattice and MILC Collaborations,

^{22}Fermilab Lattice and MILC Collaborations,

^{23}Fermilab Lattice and MILC Collaborations

We compute the leptonic decay constants $f_{D^+}$, $f_{D_s}$, and $f_{K^+}$, and the quark-mass ratios $m_c/m_s$ and $m_s/m_l$ in unquenched lattice QCD using the experimentally determined value of $f_{\pi^+}$ for normalization. We use the MILC highly improved staggered quark (HISQ) ensembles with four dynamical quark flavors---up, down, strange, and charm---and with both physical and unphysical values of the light sea-quark masses. The use of physical pions removes the need for a chiral extrapolation, thereby eliminating a significant source of uncertainty in previous calculations. Read More

We discuss the sources of uncertainty in calculations of the partial widths of the Higgs boson within the Standard Model. The uncertainties come from two sources: the truncation of perturbation theory and the uncertainties in input parameters. We review the current status of perturbative calculations and note that these are already reaching the parts-per-mil level of accuracy for the major decay modes. Read More

**Authors:**A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gámiz, Steven Gottlieb, U. M. Heller, J. Kim, J. Komijani, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, D. Mohler, E. T. Neil, M. B. Oktay, S. Qiu, J. N. Simone, R. L. Sugar, D. Toussaint, R. S. Van de Water, R. Zhou

**Category:**High Energy Physics - Lattice

We present a study of the $D$ and $B$ leptonic decay constants on the MILC $N_f=2+1$ asqtad gauge ensembles using asqtad-improved staggered light quarks and clover heavy quarks in the Fermilab interpretation. Our previous analysis \cite{Bazavov:2011aa} computed the decay constants at lattice spacings $a \approx 0.14, 0. Read More

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

We compute the zero-recoil form factor for the semileptonic decay $\bar{B}^0\to D^{*+}\ell^-\bar{\nu}$ (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. Read More

**Authors:**Yuzhi Liu, Ran Zhou, Jon A. Bailey, A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, Daping Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gámiz, Steven Gottlieb, U. M. Heller, R. D. Jain, Jongjeong Kim, A. S. Kronfeld, J. Laiho L. Levkova, P. B. Mackenzie, Y. Meurice, D. Mohler, E. T. Neil, M. B. Oktay, Si-Wei Qiu, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water

We calculate the form factors for the semileptonic decays $B_s\to K\ell\nu$ and $B\to K\ell\ell$ with lattice QCD. We work at several lattice spacings and a range of light quark masses, using the MILC 2+1-flavor asqtad ensembles. We use the Fermilab method for the $b$ quark. Read More

**Authors:**A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gámiz, Steven Gottlieb, U. M. Heller, J. Kim, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, E. T. Neil, M. B. Oktay, Si-Wei Qiu, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water, Ran Zhou

We calculate the kaon semileptonic form factor $f_+(0)$ from lattice QCD, working, for the first time, at the physical light-quark masses. We use gauge configurations generated by the MILC collaboration with $N_f=2+1+1$ flavors of sea quarks, which incorporate the effects of dynamical charm quarks as well as those of up, down, and strange. We employ data at three lattice spacings to extrapolate to the continuum limit. Read More

**Authors:**A. Bazavov

^{1}, C. Bernard

^{2}, C. Bouchard

^{3}, C. DeTar

^{4}, D. Du

^{5}, A. X. El-Khadra

^{6}, J. Foley

^{7}, E. D. Freeland

^{8}, E. Gamiz

^{9}, Steven Gottlieb

^{10}, U. M. Heller

^{11}, J. Kim

^{12}, J. Komijani

^{13}, A. S. Kronfeld

^{14}, J. Laiho

^{15}, L. Levkova

^{16}, P. B. Mackenzie

^{17}, E. T. Neil

^{18}, J. N. Simone

^{19}, R. L. Sugar

^{20}, D. Toussaint

^{21}, R. S. Van de Water

^{22}, R. Zhou

^{23}

**Affiliations:**

^{1}Fermilab Lattice and MILC Collaborations,

^{2}Fermilab Lattice and MILC Collaborations,

^{3}Fermilab Lattice and MILC Collaborations,

^{4}Fermilab Lattice and MILC Collaborations,

^{5}Fermilab Lattice and MILC Collaborations,

^{6}Fermilab Lattice and MILC Collaborations,

^{7}Fermilab Lattice and MILC Collaborations,

^{8}Fermilab Lattice and MILC Collaborations,

^{9}Fermilab Lattice and MILC Collaborations,

^{10}Fermilab Lattice and MILC Collaborations,

^{11}Fermilab Lattice and MILC Collaborations,

^{12}Fermilab Lattice and MILC Collaborations,

^{13}Fermilab Lattice and MILC Collaborations,

^{14}Fermilab Lattice and MILC Collaborations,

^{15}Fermilab Lattice and MILC Collaborations,

^{16}Fermilab Lattice and MILC Collaborations,

^{17}Fermilab Lattice and MILC Collaborations,

^{18}Fermilab Lattice and MILC Collaborations,

^{19}Fermilab Lattice and MILC Collaborations,

^{20}Fermilab Lattice and MILC Collaborations,

^{21}Fermilab Lattice and MILC Collaborations,

^{22}Fermilab Lattice and MILC Collaborations,

^{23}Fermilab Lattice and MILC Collaborations

We update our determinations of $f_{D^+}$, $f_{D_s}$, $f_K$, and quark mass ratios from simulations with four flavors of HISQ dynamical quarks. The availability of ensembles with light quarks near their physical mass means that we can extract physical results with only small corrections for valence- and sea-quark mass mistunings instead of a chiral extrapolation. The adjusted valence-quark masses and lattice spacings may be determined from an ensemble-by-ensemble analysis, and the results for the quark mass ratios then extrapolated to the continuum limit. Read More

**Authors:**E. Gámiz, A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, Steven Gottlieb, U. M. Heller, J. Kim, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, E. T. Neil, M. B. Oktay, Si-Wei Qiu, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water, Ran Zhou

**Category:**High Energy Physics - Lattice

We present results for the form factor $f_+^{K \pi}(0)$, needed to extract the CKM matrix element $|V_{us}|$ from experimental data on semileptonic $K$ decays, on the HISQ $N_f=2+1+1$ MILC configurations. The HISQ action is also used for the valence sector. The data set used for our final result includes three different values of the lattice spacing and data at the physical light quark masses. Read More

We update the lattice calculation of the $B\to\pi$ semileptonic form factors, which have important applications to the CKM matrix element $|V_{ub}|$ and the $B\to\pi\ell^+\ell^-$ rare decay. We use MILC asqtad ensembles with $N_f=2+1$ sea quarks and over a range of lattice spacings $a \approx 0.045$--$0. Read More

**Authors:**J. N. Butler, Z. Ligeti, J. L. Ritchie, V. Cirigliano, S. Kettell, R. Briere, A. A. Petrov, A. Schwartz, T. Skwarnicki, J. Zupan, N. Christ, S. R. Sharpe, R. S. Van de Water, W. Altmannshofer, N. Arkani-Hamed, M. Artuso, D. M. Asner, C. Bernard, A. J. Bevan, M. Blanke, G. Bonvicini, T. E. Browder, D. A. Bryman, P. Campana, R. Cenci, D. Cline, J. Comfort, D. Cronin-Hennessy, A. Datta, S. Dobbs, M. Duraisamy, A. X. El-Khadra, J. E. Fast, R. Forty, K. T. Flood, T. Gershon, Y. Grossman, B. Hamilton, C. T. Hill, R. J. Hill, D. G. Hitlin, D. E. Jaffe, A. Jawahery, C. P. Jessop, A. L. Kagan, D. M. Kaplan, M. Kohl, P. Krizan, A. S. Kronfeld, K. Lee, L. S. Littenberg, D. B. MacFarlane, P. B. Mackenzie, B. T. Meadows, J. Olsen, M. Papucci, Z. Parsa, G. Paz, G. Perez, L. E. Piilonen, K. Pitts, M. V. Purohit, B. Quinn, B. N. Ratcliff, D. A. Roberts, J. L. Rosner, P. Rubin, J. Seeman, K. K. Seth, B. Schmidt, A. Schopper, M. D. Sokoloff, A. Soni, K. Stenson, S. Stone, R. Sundrum, R. Tschirhart, A. Vainshtein, Y. W. Wah, G. Wilkinson, M. B. Wise, E. Worcester, J. Xu, T. Yamanaka

This report represents the response of the Intensity Frontier Quark Flavor Physics Working Group to the Snowmass charge. We summarize the current status of quark flavor physics and identify many exciting future opportunities for studying the properties of strange, charm, and bottom quarks. The ability of these studies to reveal the effects of new physics at high mass scales make them an essential ingredient in a well-balanced experimental particle physics program. Read More

**Authors:**S. Dawson, A. Gritsan, H. Logan, J. Qian, C. Tully, R. Van Kooten, A. Ajaib, A. Anastassov, I. Anderson, D. Asner, O. Bake, V. Barger, T. Barklow, B. Batell, M. Battaglia, S. Berge, A. Blondel, S. Bolognesi, J. Brau, E. Brownson, M. Cahill-Rowley, C. Calancha-Paredes, C. -Y. Chen, W. Chou, R. Clare, D. Cline, N. Craig, K. Cranmer, M. de Gruttola, A. Elagin, R. Essig, L. Everett, E. Feng, K. Fujii, J. Gainer, Y. Gao, I. Gogoladze, S. Gori, R. Goncalo, N. Graf, C. Grojean, S. Guindon, H. Haber, T. Han, G. Hanson, R. Harnik, S. Heinemeyer, U. Heintz, J. Hewett, Y. Ilchenko, A. Ishikawa, A. Ismail, V. Jain, P. Janot, S. Kanemura, S. Kawada, R. Kehoe, M. Klute, A. Kotwal, K. Krueger, G. Kukartsev, K. Kumar, J. Kunkle, M. Kurata, I. Lewis, Y. Li, L. Linssen, E. Lipeles, R. Lipton, T. Liss, J. List, T. Liu, Z. Liu, I. Low, T. Ma, P. Mackenzie, B. Mellado, K. Melnikov, A. Miyamoto, G. Moortgat-Pick, G. Mourou, M. Narain, H. Neal, J. Nielsen, N. Okada, H. Okawa, J. Olsen, H. Ono, P. Onyisi, N. Parashar, M. Peskin, F. Petriello, T. Plehn, C. Pollard, C. Potter, K. Prokofiev, M. Rauch, T. Rizzo, T. Robens, V. Rodriguez, P. Roloff, R. Ruiz, V. Sanz, J. Sayre, Q. Shafi, G. Shaughnessy, M. Sher, F. Simon, N. Solyak, J. Strube, J. Stupak, S. Su, T. Suehara, T. Tanabe, T. Tajima, V. Telnov, J. Tian, S. Thomas, M. Thomson, K. Tsumura, C. Un, M. Velasco, C. Wagner, S. Wang, S. Watanuki, G. Weiglein, A. Whitbeck, K. Yagyu, W. Yao, H. Yokoya, S. Zenz, D. Zerwas, Y. Zhang, Y. Zhou

This report summarizes the work of the Energy Frontier Higgs Boson working group of the 2013 Community Summer Study (Snowmass). We identify the key elements of a precision Higgs physics program and document the physics potential of future experimental facilities as elucidated during the Snowmass study. We study Higgs couplings to gauge boson and fermion pairs, double Higgs production for the Higgs self-coupling, its quantum numbers and $CP$-mixing in Higgs couplings, the Higgs mass and total width, and prospects for direct searches for additional Higgs bosons in extensions of the Standard Model. Read More

This is the report of the Computing Frontier working group on Lattice Field Theory prepared for the proceedings of the 2013 Community Summer Study ("Snowmass"). We present the future computing needs and plans of the U.S. Read More

**Authors:**J. M. Campbell, K. Hatakeyama, J. Huston, F. Petriello, J. Andersen, L. Barze, H. Beauchemin, T. Becher, M. Begel, A. Blondel, G. Bodwin, R. Boughezal, S. Carrazza, M. Chiesa, G. Dissertori, S. Dittmaier, G. Ferrera, S. Forte, N. Glover, T. Hapola, A. Huss, X. Garcia i Tormo, M. Grazzini, S. Hoche, P. Janot, T. Kasprzik, M. Klein, U. Klein, D. Kosower, Y. Li, X. Liu, P. Mackenzie, D. Maitre, E. Meoni, K. Mishra, G. Montagna, M. Moretti, P. Nadolsky, O. Nicrosini, F. Piccinini, L. Reina, V. Radescu, J. Rojo, J. Russ, S. Sapeta, A. Schwartzman, P. Skands, J. Smillie, I. W. Stewart, F. J. Tackmann, F. Tramontano, R. Van de Water, J. R. Walsh, S. Zuberi

**Category:**High Energy Physics - Phenomenology

This is the summary report of the energy frontier QCD working group prepared for Snowmass 2013. We review the status of tools, both theoretical and experimental, for understanding the strong interactions at colliders. We attempt to prioritize important directions that future developments should take. Read More

**Authors:**A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, Daping Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gámiz, Steven Gottlieb, U. M. Heller, Jongjeong Kim, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, E. T. Neil, M. B. Oktay, Si-Wei Qiu, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water, Ran Zhou

Using staggered fermions and twisted boundary conditions, we calculate the K meson semileptonic decay vector form factor at zero momentum transfer. The HISQ formulation is used for the valence quarks, while the sea quarks are simulated with the asqtad action (MILC N_f=2+1 configurations). For the chiral and continuum extrapolation we use two-loop continuum CHPT, supplemented by partially quenched staggered CHPT at one loop. Read More

**Authors:**A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, J. E. Hetrick, J. Kim, A. S. Kronfeld, J. Laiho, L. Levkova, M. Lightman, P. B. Mackenzie, E. T. Neil, M. Oktay, J. N. Simone, R. L. Sugar, D. Toussaint, R. S. Van de Water, R. Zhou, for the Fermilab Lattice Collaboration, for the MILC Collaboration

**Category:**High Energy Physics - Lattice

We present our methods to fit the two point correlators for light, strange, and charmed pseudoscalar meson physics with the highly improved staggered quark (HISQ) action. We make use of the least-squares fit including the full covariance matrix of the correlators and including Gaussian constraints on some parameters. We fit the correlators on a variety of the HISQ ensembles. Read More

**Authors:**E. Gamiz, J. A. Bailey, A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, Steven Gottlieb, U. M. Heller, J. Kim, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, E. T. Neil, M. B. Oktay, Si-Wei Qiu, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water, R. Zhou

**Category:**High Energy Physics - Lattice

We report on the status of our kaon semileptonic form factor calculations using the highly-improved staggered quark (HISQ) formulation to simulate the valence fermions. We present results for the form factor f_+^{K \pi}(0) on the asqtad N_f=2+1 MILC configurations, discuss the chiral-continuum extrapolation, and give a preliminary estimate of the total error. We also present a more preliminary set of results for the same form factor but with the sea quarks also simulated with the HISQ action; these results include data at the physical light quark masses. Read More

**Authors:**A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, D. Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, J. E. Hetrick, J. Kim, A. S. Kronfeld, J. Laiho, L. Levkova, M. Lightman, P. B. Mackenzie, E. T. Neil, M. Oktay, J. N. Simone, R. L. Sugar, D. Toussaint, R. S. Van de Water, R. Zhou, for the Fermilab Lattice Collaboration, for the MILC Collaboration

We present preliminary results for light, strange and charmed pseudoscalar meson physics from simulations using four flavors of dynamical quarks with the highly improved staggered quark (HISQ) action. These simulations include lattice spacings ranging from 0.15 to 0. Read More

**Authors:**Jon A. Bailey, A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, Daping Du, A. X. El-Khadra, J. Foley, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. 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 -> D tau nu 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 -> D tau nu, finding an approximately 2-sigma disagreement with the Standard-Model prediction for the ratio R(D)=BR(B->D tau nu)/BR(B->D l nu), where l=e,mu. We compute this ratio of branching fractions using hadronic form factors computed in unquenched lattice QCD and obtain R(D) = 0. Read More

**Authors:**A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, M. Di Pierro, A. X. El-Khadra, R. T. Evans, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, J. E. Hetrick, R. Jain, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, E. T. Neil, M. B. Oktay, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water

We study SU(3)-breaking effects in the neutral B_d-\bar B_d and B_s-\bar B_s systems with unquenched N_f=2+1 lattice QCD. We calculate the relevant matrix elements on the MILC collaboration's gauge configurations with asqtad-improved staggered sea quarks. For the valence light-quarks (u, d, and s) we use the asqtad action, while for b quarks we use the Fermilab action. Read More

**Authors:**J. L. Hewett, H. Weerts, R. Brock, J. N. Butler, B. C. K. Casey, J. Collar, A. de Gouvea, R. Essig, Y. Grossman, W. Haxton, J. A. Jaros, C. K. Jung, Z. T. Lu, K. Pitts, Z. Ligeti, J. R. Patterson, M. Ramsey-Musolf, J. L. Ritchie, A. Roodman, K. Scholberg, C. E. M. Wagner, G. P. Zeller, S. Aefsky, A. Afanasev, K. Agashe, C. Albright, J. Alonso, C. Ankenbrandt, M. Aoki, C. A. Arguelles, N. Arkani-Hamed, J. R. Armendariz, C. Armendariz-Picon, E. Arrieta Diaz, J. Asaadi, D. M. Asner, K. S. Babu, K. Bailey, O. Baker, B. Balantekin, B. Baller, M. Bass, B. Batell, J. Beacham, J. Behr, N. Berger, M. Bergevin, E. Berman, R. Bernstein, A. J. Bevan, M. Bishai, M. Blanke, S. Blessing, A. Blondel, T. Blum, G. Bock, A. Bodek, G. Bonvicini, F. Bossi, J. Boyce, R. Breedon, M. Breidenbach, S. J. Brice, R. A. Briere, S. Brodsky, C. Bromberg, A. Bross, T. E. Browder, D. A. Bryman, M. Buckley, R. Burnstein, E. Caden, P. Campana, R. Carlini, G. Carosi, C. Castromonte, R. Cenci, I. Chakaberia, M. C. Chen, C. H. Cheng, B. Choudhary, N. H. Christ, E. Christensen, M. E. Christy, T. E. Chupp, E. Church, D. B. Cline, T. E. Coan, P. Coloma, J. Comfort, L. Coney, J. Cooper, R. J. Cooper, R. Cowan, D. F. Cowen, D. Cronin-Hennessy, A. Datta, G. S. Davies, M. Demarteau, D. P. DeMille, A. Denig, R. Dermisek, A. Deshpande, M. S. Dewey, R. Dharmapalan, J. Dhooghe, M. R. Dietrich, M. Diwan, Z. Djurcic, S. Dobbs, M. Duraisamy, B. Dutta, H. Duyang, D. A. Dwyer, M. Eads, B. Echenard, S. R. Elliott, C. Escobar, J. Fajans, S. Farooq, C. Faroughy, J. E. Fast, B. Feinberg, J. Felde, G. Feldman, P. Fierlinger, P. Fileviez Perez, B. Filippone, P. Fisher, B. T. Flemming, K. T. Flood, R. Forty, M. J. Frank, A. Freyberger, A. Friedland, R. Gandhi, K. S. Ganezer, A. Garcia, F. G. Garcia, S. Gardner, L. Garrison, A. Gasparian, S. Geer, V. M. Gehman, T. Gershon, M. Gilchriese, C. Ginsberg, I. Gogoladze, M. Gonderinger, M. Goodman, H. Gould, M. Graham, P. W. Graham, R. Gran, J. Grange, G. Gratta, J. P. Green, H. Greenlee, R. C. Group, E. Guardincerri, V. Gudkov, R. Guenette, A. Haas, A. Hahn, T. Han, T. Handler, J. C. Hardy, R. Harnik, D. A. Harris, F. A. Harris, P. G. Harris, J. Hartnett, B. He, B. R. Heckel, K. M. Heeger, S. Henderson, D. Hertzog, R. Hill, E. A Hinds, D. G. Hitlin, R. J. Holt, N. Holtkamp, G. Horton-Smith, P. Huber, W. Huelsnitz, J. Imber, I. Irastorza, J. Jaeckel, I. Jaegle, C. James, A. Jawahery, D. Jensen, C. P. Jessop, B. Jones, H. Jostlein, T. Junk, A. L. Kagan, M. Kalita, Y. Kamyshkov, D. M. Kaplan, G. Karagiorgi, A. Karle, T. Katori, B. Kayser, R. Kephart, S. Kettell, Y. K. Kim, M. Kirby, K. Kirch, J. Klein, J. Kneller, A. Kobach, M. Kohl, J. Kopp, M. Kordosky, W. Korsch, I. Kourbanis, A. D. Krisch, P. Krizan, A. S. Kronfeld, S. Kulkarni, K. S. Kumar, Y. Kuno, T. Kutter, T. Lachenmaier, M. Lamm, J. Lancaster, M. Lancaster, C. Lane, K. Lang, P. Langacker, S. Lazarevic, T. Le, K. Lee, K. T. Lesko, Y. Li, M. Lindgren, A. Lindner, J. Link, D. Lissauer, L. S. Littenberg, B. Littlejohn, C. Y. Liu, W. Loinaz, W. Lorenzon, W. C. Louis, J. Lozier, L. Ludovici, L. Lueking, C. Lunardini, D. B. MacFarlane, P. A. N. Machado, P. B. Mackenzie, J. Maloney, W. J. Marciano, W. Marsh, M. Marshak, J. W. Martin, C. Mauger, K. S. McFarland, C. McGrew, G. McLaughlin, D. McKeen, R. McKeown, B. T. Meadows, R. Mehdiyev, D. Melconian, H. Merkel, M. Messier, J. P. Miller, G. Mills, U. K. Minamisono, S. R. Mishra, I. Mocioiu, S. Moed Sher, R. N. Mohapatra, B. Monreal, C. D. Moore, J. G. Morfin, J. Mousseau, L. A. Moustakas, G. Mueller, P. Mueller, M. Muether, H. P. Mumm, C. Munger, H. Murayama, P. Nath, O. Naviliat-Cuncin, J. K. Nelson, D. Neuffer, J. S. Nico, A. Norman, D. Nygren, Y. Obayashi, T. P. O'Connor, Y. Okada, J. Olsen, L. Orozco, J. L. Orrell, J. Osta, B. Pahlka, J. Paley, V. Papadimitriou, M. Papucci, S. Parke, R. H. Parker, Z. Parsa, K. Partyka, A. Patch, J. C. Pati, R. B. Patterson, Z. Pavlovic, G. Paz, G. N. Perdue, D. Perevalov, G. Perez, R. Petti, W. Pettus, A. Piepke, M. Pivovaroff, R. Plunkett, C. C. Polly, M. Pospelov, R. Povey, A. Prakesh, M. V. Purohit, S. Raby, J. L. Raaf, R. Rajendran, S. Rajendran, G. Rameika, R. Ramsey, A. Rashed, B. N. Ratcliff, B. Rebel, J. Redondo, P. Reimer, D. Reitzner, F. Ringer, A. Ringwald, S. Riordan, B. L. Roberts, D. A. Roberts, R. Robertson, F. Robicheaux, M. Rominsky, R. Roser, J. L. Rosner, C. Rott, P. Rubin, N. Saito, M. Sanchez, S. Sarkar, H. Schellman, B. Schmidt, M. Schmitt, D. W. Schmitz, J. Schneps, A. Schopper, P. Schuster, A. J. Schwartz, M. Schwarz, J. Seeman, Y. K. Semertzidis, K. K. Seth, Q. Shafi, P. Shanahan, R. Sharma, S. R. Sharpe, M. Shiozawa, V. Shiltsev, K. Sigurdson, P. Sikivie, J. Singh, D. Sivers, T. Skwarnicki, N. Smith, J. Sobczyk, H. Sobel, M. Soderberg, Y. H. Song, A. Soni, P. Souder, A. Sousa, J. Spitz, M. Stancari, G. C. Stavenga, J. H. Steffen, S. Stepanyan, D. Stoeckinger, S. Stone, J. Strait, M. Strassler, I. A. Sulai, R. Sundrum, R. Svoboda, B. Szczerbinska, A. Szelc, T. Takeuchi, P. Tanedo, S. Taneja, J. Tang, D. B. Tanner, R. Tayloe, I. Taylor, J. Thomas, C. Thorn, X. Tian, B. G. Tice, M. Tobar, N. Tolich, N. Toro, I. S. Towner, Y. Tsai, R. Tschirhart, C. D. Tunnell, M. Tzanov, A. Upadhye, J. Urheim, S. Vahsen, A. Vainshtein, E. Valencia, R. G. Van de Water, R. S. Van de Water, M. Velasco, J. Vogel, P. Vogel, W. Vogelsang, Y. W. Wah, D. Walker, N. Weiner, A. Weltman, R. Wendell, W. Wester, M. Wetstein, C. White, L. Whitehead, J. Whitmore, E. Widmann, G. Wiedemann, J. Wilkerson, G. Wilkinson, P. Wilson, R. J. Wilson, W. Winter, M. B. Wise, J. Wodin, S. Wojcicki, B. Wojtsekhowski, T. Wongjirad, E. Worcester, J. Wurtele, T. Xin, J. Xu, T. Yamanaka, Y. Yamazaki, I. Yavin, J. Yeck, M. Yeh, M. Yokoyama, J. Yoo, A. Young, E. Zimmerman, K. Zioutas, M. Zisman, J. Zupan, R. Zwaska

The Proceedings of the 2011 workshop on Fundamental Physics at the Intensity Frontier. Science opportunities at the intensity frontier are identified and described in the areas of heavy quarks, charged leptons, neutrinos, proton decay, new light weakly-coupled particles, and nucleons, nuclei, and atoms. Read More

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

We calculate form-factor ratios between the semileptonic decays \bar{B}->D^+\ell^-\bar{\nu} and \bar{B}_s->D_s^+\ell^-\bar{\nu} with lattice QCD. These ratios are a key theoretical input in a new strategy to determine the fragmentation fractions of the neutral B decays, which are needed for measurements of BR(B^0_s-> \mu^+\mu^-). We use the MILC ensembles of gauge configurations with 2+1 flavors of sea quarks at two lattice spacings of approximately 0. Read More

**Authors:**E. T. Neil, Jon A. Bailey, A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, M. Di Pierro, A. X. El-Khadra, R. T. Evans, E. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, J. E. Hetrick, R. Jain, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, M. B. Oktay, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water, for the Fermilab Lattice Collaboration, for the MILC Collaboration

**Category:**High Energy Physics - Lattice

We give an update on simulation results for the decay constants f_B, f_{B_s}, f_D and f_{D_s}. These decay constants are important for precision tests of the standard model, in particular entering as inputs to the global CKM unitarity triangle fit. The results presented here make use of the MILC (2+1)-flavor asqtad ensembles, with heavy quarks incorporated using the clover action with the Fermilab method. Read More

**Authors:**A. Bazavov, C. Bernard, C. M. Bouchard, C. DeTar, M. Di Pierro, A. X. El-Khadra, R. T. Evans, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, J. E. Hetrick, R. Jain, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, E. T. Neil, M. B. Oktay, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water

We calculate the leptonic decay constants of B_{(s)} and D_{(s)} mesons in lattice QCD using staggered light quarks and Fermilab bottom and charm quarks. We compute the heavy-light meson correlation functions on the MILC asqtad-improved staggered gauge configurations which include the effects of three light dynamical sea quarks. We simulate with several values of the light valence- and sea-quark masses (down to ~m_s/10) and at three lattice spacings (a ~ 0. Read More

We report on the status of the Fermilab-MILC calculation of the form factor f_+^{K pi}(0), needed to extract the CKM matrix element |V_{us}| from experimental data on K semileptonic decays. The HISQ formulation is used in the simulations for the valence quarks, while the sea quarks are simulated with the asqtad action (MILC N_f=2+1 configurations). We discuss the general methodology of the calculation, including the use of twisted boundary conditions to get values of the momentum transfer close to zero and the different techniques applied for the correlators fits. Read More

The experimentally measured rates of the semileptonic decays K -> pi l nu and D -> K(pi) l nu can be combined with lattice calculations of the associated form factors to precisely extract the CKM matrix elements |V_{us}| and |V_{cs(d)}|. We report on the status of form factor calculations with Fermilab charm quarks and staggered light quarks on the 2+1 flavor asqtad staggered MILC ensembles. Analysis of data for the D -> pi l nu form factor provides a nontrivial test of our methods via comparison with CLEO data. Read More

We present an update of our calculation of the form factor for B -> D* l nu at zero recoil, with higher statistics and finer lattices. As before, we use the Fermilab action for b and c quarks, the asqtad staggered action for light valence quarks, and the MILC ensembles for gluons and light quarks (L\"uscher-Weisz married to 2+1 rooted staggered sea quarks). In this update, we have reduced the total uncertainty on F(1) from 2. Read More

We report the non-perturbative tuning of parameters--- kappa_c, kappa_b, and kappa_crit ---that determine the heavy-quark mass in the Fermilab action. This requires the computation of the masses of Ds^(*) and Bs^(*) mesons comprised of a Fermilab heavy quark and a staggered light quark. Additionally, we report the hyperfine splittings for Ds and Bs mesons as a cross-check of our simulation and analysis methods. Read More

**Authors:**A. Bazavov, C. Bernard, C. DeTar, E. D. Freeland, E. Gamiz, Steven Gottlieb, U. M. Heller, J. E. Hetrick, A. X. El-Khadra, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, M. B. Oktay, M. Di Pierro, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water

**Category:**High Energy Physics - Lattice

We present the leptonic decay constants fDs and fD+ computed on the MILC collaboration's 2+1 flavor asqtad gauge ensembles. We use clover heavy quarks with the Fermilab interpretation and improved staggered light quarks. The simultaneous chiral and continuum extrapolation, which determines both decay constants, includes partially-quenched lattice results at lattice spacings a ~ 0:09, 0:12 and 0:15 fm. Read More

We report on calculations of the charmonium and bottomonium spectrum in lattice QCD. We use ensembles of gauge fields with three flavors of sea quarks, simulated with the asqtad improved action for staggered fermions. For the heavy quarks we employ the Fermilab interpretation of the clover action for Wilson fermions. Read More

**Authors:**Jon A. Bailey, A. Bazavov, C. Bernard, C. Bouchard, C. DeTar, A. X. El-Khadra, E. D. Freeland, W. Freeman, E. Gamiz, Steven Gottlieb, U. M. Heller, J. E. Hetrick, A. S. Kronfeld, J. Laiho, L. Levkova, P. B. Mackenzie, M. B. Oktay, M. Di Pierro, J. N. Simone, R. Sugar, D. Toussaint, R. S. Van de Water

**Category:**High Energy Physics - Lattice

Lattice calculations of the form factors for the charm semileptonic decays D to K l nu and D to pi l nu provide inputs to direct determinations of the CKM matrix elements |V(cs)| and |V(cd)| and can be designed to validate calculations of the form factors for the bottom semileptonic decays B to pi l nu and B to K l l-bar. We are using Fermilab charm (bottom) quarks and asqtad staggered light quarks on the 2+1 flavor asqtad MILC ensembles to calculate the charm (bottom) form factors. We outline improvements to the previous calculation of the charm form factors and detail our progress. Read More

**Authors:**T. Burch

^{1}, C. E. DeTar

^{2}, M. Di Pierro

^{3}, A. X. El-Khadra

^{4}, Steven Gottlieb

^{5}, A. S. Kronfeld

^{6}, L. Levkova

^{7}, P. B. Mackenzie

^{8}, J. Simone

^{9}

**Affiliations:**

^{1}U Utah,

^{2}U Utah,

^{3}DePaul U,

^{4}U Ill,

^{5}Indiana U,

^{6}FNAL,

^{7}U Utah,

^{8}FNAL,

^{9}FNAL

**Category:**High Energy Physics - Lattice

We present results from an ongoing lattice study of the lowest lying charmonium and bottomonium level splittings using the Fermilab heavy quark formalism. Our objective is to test the performance of this action on MILC-collaboration ensembles of (2+1) flavors of light improved staggered (asqtad) quarks. Measurements are done on 16 ensembles with degenerate up and down quarks of various masses, thus permitting a chiral extrapolation, and over lattice spacings ranging from 0. Read More

We update results presented at Lattice 2005 on charmonium masses. New ensembles of gauge configurations with 2+1 flavors of improved staggered quarks have been analyzed. Statistics have been increased for other ensembles. Read More

Lattice QCD plays an essential role in testing and determining the parameters of the CKM theory of flavor mixing and CP violation. Very high precisions are required for lattice calculations analysing CKM data; I discuss the prospects for achieving them. Lattice calculations will also play a role in investigating flavor mixing and CP violation beyond the Standard Model. Read More

Comparisons of lattice-QCD calculations of semileptonic form factors with experimental measurements often display two sets of points, one each for lattice QCD and experiment. Here we propose to display the output of a lattice-QCD analysis as a curve and error band. This is justified, because lattice-QCD results rely in part on fitting, both for the chiral extrapolation and to extend lattice-QCD data over the full physically allowed kinematic domain. Read More

We present an update of our calculations of the decay constants of the D, D_s, B, and B_s mesons in unquenched 2+1 flavor QCD. We use the MILC library of improved staggered gauge ensembles at lattice spacings 0.09, 0. Read More

Dramatic progress has been made over the last decade in the numerical study of quantum chromodynamics (QCD) through the use of improved formulations of QCD on the lattice (improved actions), the development of new algorithms and the rapid increase in computing power available to lattice gauge theorists. In this article we describe simulations of full QCD using the improved staggered quark formalism, ``asqtad'' fermions. These simulations were carried out with two degenerate flavors of light quarks (up and down) and with one heavier flavor, the strange quark. Read More

We calculate the form factor f_+(q^2) for B-meson semileptonic decay in unquenched lattice QCD with 2+1 flavors of light sea quarks. We use Asqtad-improved staggered light quarks and a Fermilab bottom quark on gauge configurations generated by the MILC Collaboration. We simulate with several light quark masses and at two lattice spacings, and extrapolate to the physical quark mass and continuum limit using heavy-light meson staggered chiral perturbation theory. Read More

We present the first lattice QCD calculation of the form factor for B-> D* l nu 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. Read More

I discuss the lattice calculations relevant to recent advances in CKM phenomenology, focusing on those relevant to new experimental results reported at this workshop. Read More