Domain wall QCD with physical quark masses by Blum, T., Boyle, P. A., Christ, N. H., Frison, J., Garron, N., Hudspith, R. J., Izubuchi, T., Janowski, T., Jung, C., Jüttner, A., Kelly, C., Kenway, R. D., Lehner, C., Marinkovic, M., Mawhinney, R. D., McGlynn, G., Murphy, D. J., Ohta, S., Portelli, A., Sachrajda, C. T., Soni, A.

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Direct CP violation and the ΔI = 1/2 rule in K → ππ decay from the standard model by Abbott, R, Blum, T, Boyle, P A, Bruno, M, Christ, N H, Hoying, D, Jung, C, Kelly, C, Lehner, C, Mawhinney, R D, Murphy, D J, Sachrajda, C T, Soni, A, Tomii, M, Wang, T

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Lattice simulations with G -parity boundary conditions by Christ, N. H., Kelly, C., Zhang, D.

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Standard Model Prediction for Direct CP Violation in K→ππ Decay by Bai, Z, Blum, T, Boyle, P A, Christ, N H, Frison, J, Garron, N, Izubuchi, T, Jung, C, Kelly, C, Lehner, C, Mawhinney, R D, Sachrajda, C T, Soni, A, Zhang, D

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K → ππ decay, ε′ and the RBC-UKQCD kaon physics program by Christ, N H

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KL-KS Mass Difference from Lattice QCD by Bai, Z, Christ, N H, Izubuchi, T, Sachrajda, C T, Soni, A, Yu, J

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K L − K S Mass Difference from Lattice QCD by Bai, Z., Christ, N. H., Izubuchi, T., Sachrajda, C. T., Soni, A., Yu, J.

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Neutral-kaon mixing from (2+1)-flavor domain-wall QCD by Antonio, D J, Boyle, P A, Blum, T, Christ, N H, Cohen, S D, Dawson, C, Izubuchi, T, Kenway, R D, Jung, C, Li, S, Lin, M F, Mawhinney, R D, Noaki, J, Ohta, S, Pendleton, B J, Scholz, E E, Soni, A, Tweedie, R J, Yamaguchi, A

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Emerging understanding of the ΔI=1/2 rule from lattice QCD by Boyle, P A, Christ, N H, Garron, N, Goode, E J, Janowski, T, Lehner, C, Liu, Q, Lytle, A T, Sachrajda, C T, Soni, A, Zhang, D

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Lattice determination of I = 0 and 2 π π scattering phase shifts with a physical pion mass by Blum, T., Boyle, P. A., Bruno, M., Christ, N. H., Hoying, D., Kelly, C., Lehner, C., Mawhinney, R. D., Meyer, A. S., Murphy, D. J., Sachrajda, C. T., Soni, A., Wang, T.

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η and η' mesons from lattice QCD by Christ, N H, Dawson, C, Izubuchi, T, Jung, C, Liu, Q, Mawhinney, R D, Sachrajda, C T, Soni, A, Zhou, R

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K→(ππ)(I=2) decay amplitude from lattice QCD by Blum, T, Boyle, P A, Christ, N H, Garron, N, Goode, E, Izubuchi, T, Jung, C, Kelly, C, Lehner, C, Lightman, M, Liu, Q, Lytle, A T, Mawhinney, R D, Sachrajda, C T, Soni, A, Sturm, C

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Overview of the QCDSP and QCDOC computers by Boyle, P A, Chen, D, Christ, N H, Clark, M A

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B -meson decay constants from 2 + 1 -flavor lattice QCD with domain-wall light quarks and relativistic heavy quarks by Christ, N. H., Flynn, J. M., Izubuchi, T., Kawanai, T., Lehner, C., Soni, A., Van de Water, R. S., Witzel, O.

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Effects of finite volume on the KL – KS mass difference by Christ, N.  H., Feng, X., Martinelli, G., Sachrajda, C.  T.

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Lattice simulations with G -parity boundary conditions by Christ, N. H., Kelly, C., Zhang, D.

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Low energy constants of SU ( 2 ) partially quenched chiral perturbation theory from Nf=2+1 domain wall QCD by Boyle, P. A., Christ, N. H., Garron, N., Jung, C., Jüttner, A., Kelly, C., Mawhinney, R. D., McGlynn, G., Murphy, D. J., Ohta, S., Portelli, A., Sachrajda, C. T.

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Prospects for a lattice computation of rare kaon decay amplitudes: K → π ℓ + ℓ − decays by Christ, N. H., Feng, X., Portelli, A., Sachrajda, C. T.

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K → π π Δ I = 3 / 2 decay amplitude in the continuum limit by Blum, T., Boyle, P. A., Christ, N. H., Frison, J., Garron, N., Janowski, T., Jung, C., Kelly, C., Lehner, C., Lytle, A., Mawhinney, R. D., Sachrajda, C. T., Soni, A., Yin, H., Zhang, D.

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Equation of state and QCD transition at finite temperature by Bazavov, A., Bhattacharya, T., Cheng, M., Christ, N. H., DeTar, C., Ejiri, S., Gottlieb, Steven, Gupta, R., Heller, U. M., Huebner, K., Jung, C., Karsch, F., Laermann, E., Levkova, L., Miao, C., Mawhinney, R. D., Petreczky, P., Schmidt, C., Soltz, R. A., Soeldner, W., Sugar, R., Toussaint, D., Vranas, P.

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