29th International Symposium on Lattice Field Theory (Lattice 2011)
Lattice 2011 was held July 10–16, 2011, at The Village at Squaw Valley in Lake Tahoe, California, USA.
Conference proceedings are available on Proceedings of Science.
- Event Information
- Program Overview
- Plenary Program
- Parallel Sessions
- Poster Session
- Committees and Contacts
- Links
Event Information
Dates: July 10–16, 2011
Location: The Village at Squaw Valley, California, USA
Topics
The program included plenary talks, parallel talks, and a poster session on the following topics:
- Algorithms and machines
- Applications beyond QCD
- Chiral symmetry
- Hadron spectroscopy and interactions
- Hadron structure
- Nonzero temperature and density
- Standard model parameters and renormalization
- Theoretical developments
- Vacuum structure and confinement
- Weak decays and matrix elements
Organizing Institutions
- Lawrence Livermore National Laboratory (LLNL)
- Lawrence Berkeley National Laboratory
- San Francisco State University
- University of California (UC) Los Angeles
- UC Santa Barbara
- UC Davis
- UC San Diego
- University of the Pacific
Sponsors
- US Department of Energy, Office of Science
- Lawrence Berkeley National Laboratory
- LLNL
- Jefferson Lab
- NVIDIA
- Globus
- UC Davis Division of Mathematical and Physical Sciences
- UC Davis Department of Physics
- Brookhaven National Laboratory
Program Overview
| Time | Sunday July 10 |
Monday July 11 |
Tuesday July 12 |
Wednesday July 13 |
Thursday July 14 |
Friday July 15 |
Saturday July 16 |
|---|---|---|---|---|---|---|---|
| 8:30 | Welcome | Parallel Session 8:30–10:10 | Plenary Session 08:45–10:00 | ||||
| 9:00 | Plenary Session 08:45–10:30 | Plenary Session 09:00–10:30 | Plenary Session 09:00–10:30 | Plenary Session 09:00–10:35 | |||
| 9:30 | |||||||
| 10:00 | Break | Break | |||||
| 10:30 | Break | Break | Parallel Session 10:40–12:20 | Break | Break | Plenary Session 10:30–12:15 | |
| 11:00 | Plenary Session 11:00–12:45 | Plenary Session 11:00–12:15 | Plenary Session 11:00–12:30 | Plenary Session 11:00–12:45 | |||
| 11:30 | |||||||
| 12:00 | Ken Wilson Lattice Award | Closing | |||||
| 12:30 | Lunch Break 12:45–15:00 | Lunch Break 12:30–15:00 | Lunch Break 12:20–14:00 | Lunch Break 12:30–15:00 | Lunch Break 12:45–15:00 | ||
| 13:00 | |||||||
| 13:30 | |||||||
| 14:00 | Excursions 14:00–19:00 | ||||||
| 14:30 | |||||||
| 15:00 | Parallel Session 15:00–16:40 | Parallel Session 15:00–16:40 | Parallel Session 15:00–16:40 | Parallel Session 15:00–16:40 | |||
| 15:30 | |||||||
| 16:00 | Registration & Reception 16:00–20:00 |
||||||
| 16:30 | Break | Break | Break | Break | |||
| 17:00 | Parallel Session 17:10–18:50 | Parallel Session 17:10–18:30 | Parallel Session 17:10–18:30 | Parallel Session 17:10–18:50 | |||
| 17:30 | |||||||
| 18:00 | |||||||
| 18:30 | Poster Session 18:30–20:30 | Gondola to Banquet Cash Bar (every 15 min., 90 ppl. per trip) | |||||
| 19:00 | |||||||
| 19:30 | |||||||
| 20:00 | Banquet 20:00–22:00 | ||||||
| 20:30 |
Plenary Program
| Session | Time | Title | Speaker |
|---|---|---|---|
| Monday | 8:30–8:45 | Welcome | |
| 8:45–9:15 | Determination of alpha_s from lattice QCD | Eigo Shintani | |
| 9:15–10:00 | Topological insulators, superconductors and their connections to lattice gauge theory | Shoucheng Zhang | |
| 10:00–10:30 | Large-N volume independence, conformality and confinement | Mithat Unsal | |
| 10:30–11:00 | Break | ||
| 11:00–11:45 | Holography and colliding gravitational shock waves | Larry Yaffe | |
| 11:45–12:15 | Asymptotic Safety and Lattice Quantum Gravity | Jack Laiho | |
| 12:15–12:45 | Flavor blindness and patterns of flavor sym. breaking in 3-flavor sims |
Paul Rakow | |
| Tuesday | 9:00–9:30 | Large extra dimensions and lattices | Aleksi Kurkela |
| 9:30–10:30 | Signals in the TeV era and the Lattice | Adam Martin | |
| 10:30–11:00 | Break | ||
| 11:00–11:45 | Exploring Models for New Physics on the Lattice | Ethan Neil | |
| 11:45–12:15 | SU(3) gauge theory with sextet fermions | Daniel Nogradi | |
| 12:15–12:30 | Ken Wilson Lattice Award | ||
| Thursday | 9:00–9:45 | Connecting the Lattice Points: What Lattice QCD Calculations can tell us about the Quark Gluon Plasma | Barbara Jacak |
| 9:45–10:30 | QCD at Finite Temperature and Density | Ludmila Levkova | |
| 10:30–11:00 | Break | ||
| 11:00–11:30 | Fluctuations, correlations: from lattice QCD to heavy ion collisions | Swagato Mukherjee | |
| 11:30–12:00 | Looking for U(1)_A in Hot QCD Matter with Domain-Wall Fermions | Prasad Hegde | |
| 12:00–12:30 | GPUs for the Lattice | Balint Joo | |
| Friday | 9:00–9:35 | Listening to Noise | David Kaplan |
| 9:35–10:20 | Hadron interactions | Kostas Orginos | |
| 10:20–10:35 | Report from Japan after the earthquake | Shoji Hashimoto | |
| 10:35–11:00 | Break | ||
| 11:00–11:45 | Flavor Physics in the LHC era: the role of the lattice | Enrico Lunghi | |
| 11:45–12:30 | Standard Model Flavor physics on the Lattice | Christine Davies | |
| 12:30–12:45 | Thanks to conference secretariats and Lattice 2012 announcement | ||
| Saturday | 8:30–9:00 | Lattice QCD with Classical and Quantum Electrodynamics | Brian Tiburzi |
| 9:00–9:30 | Progress on Excited Hadrons in Lattice QCD | John Bulava | |
| 9:30–10:00 | Nonperturbative QCD corrections to electroweak observables | Dru Renner | |
| 10:00–10:30 | Break | ||
| 10:30–11:00 | Low energy Particle Physics and Chiral Extrapolations | Hartmut Wittig | |
| 11:00–11:45 | Direct and Indirect Kaon Physics Directly Below KT-22: A Lattice 2011 Review | Bob Mawhinney | |
| 11:45–12:15 | Reweighting in the quark mass | Ana Hasenfratz | |
| 12:15–12:30 | Closing | ||
Plenary Session Chairs
| Session | Chair | Subject |
|---|---|---|
| Monday (8:30–10:30) | Herbert Neuberger | Theory |
| Monday (11:00–12:45) | Norboru Kawamoto | Theory |
| Tuesday (9:00–10:30) | Tom DeGrand | BSM |
| Tuesday (11:00–12:30) | Luigi Del Debbio | BSM |
| Thursday (9:00–10:30) | Zoltan Fodor | Thermo |
| Thursday (11:00–12:30) | Shinji Ejiri | Thermo |
| Friday (9:00–10:20) | Yoshinobu Kuramashi | Nuclear |
| Friday (11:00–12:30) | Laurent Lellouch | HEP |
| Saturday (8:30–10:00) | Derek Leinweber | Nuclear |
| Saturday (10:30–12:15) | Steve Sharpe | Chiral/Weak |
Parallel Sessions
Monday 1
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Chiral Symmetry | Hadron Spectroscopy | Hadron Structure | Weak Decays and Matrix Elements |
| 3:00 | T Ishikawa Chiral Magnetic Effect on the domain-wall fermion |
J Kuti Twelve flavors with three colors and two flavors with six colors below the conformal window |
M Schroeck Effects of the low lying Dirac modes on the spectrum of ground state mesons |
G Engel Excited meson spectroscopy with two chirally improved quarks |
R Schiel An Update on Distribution Amplitudes of the Nucleon and its Parity Partner |
R Gupta Probing TeV scale physics via ultra cold neutron decays and calculating non-standard baryon matrix elements |
| 3:20 | G Endrodi The finite temperature QCD transition in external magnetic fields |
G Fleming Infrared conformality and lattice simulations |
E G Ramos Topological susceptibility and chiral condensate with Nf=2+1+1 dynamical flavors of maximally twisted mass fermions. |
N Mathur Meson spectra and decay constants from overlap fermion on domain wall gauge configurations |
A Sternbeck First moments of the nucleon generalized parton distributions from lattice QCD |
T Bhattacharya Theoretical Bounds on New Four-Fermion Interactions and TeV Scale Physics |
| 3:40 | A Yamamoto TALK MOVED TO THU 5:50 Alpenglow |
X-Y Jin Lattice QCD with 12 Degenerate Quark Flavors |
T-W Chiu Chiral Properties of the Pseudoscalar Meson in Two Flavors QCD |
C Thomas Excited light isoscalar mesons from lattice QCD |
W Detmold Medium effects in parton distributions |
H-W Lin Probing TeV Physics through Lattice Neutron-Decay Matrix Elements |
| 4:00 | F James Complex Langevin dynamics: criteria for correctness |
K Ogawa The Infrared behavior of SU(3) Nf=12 gauge theory -about the existence of conformal fixed point- |
T-H Hsieh Topological fluctuations in Two flavors Lattice QCD |
D Richards Energy-dependent I=2 Pi-Pi Scattering Phase Shift in Lattice QCD |
A Ramos Octet baryon sigma terms |
F Sanfilippo Lattice QCD calculation of isospin breaking effects due to the up-down mass difference |
| 4:20 | T Sano Complex Langevin simulation applied to chiral random matrix model at finite density |
E Itou The Infrared behavior of SU(3) Nf=12 gauge theory -measurement of the anomalous dimension- |
A De Topological susceptibility with Wilson fermions |
D Lenkner Isoscalar and Multi- Hadron States via the Stochastic LapH Algorithm |
R Horsley Nucleon sigma terms for 2+1 quark flavours |
N Carrasco-Vela Kaon oscillations in the Standard Model and Beyond using Nf=2+1+1 dynamical sea quarks |
Monday 2
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Hadron Structure | Weak Decays and Matrix Elements | Algorithms and Machines | Hadron Spectroscopy |
| 5:10 | L Cosmai Phase diagram of QCD with two degenerate staggered quarks |
E Pallante On the spectrum of many-flavor QCD |
M Gong Strange and charm quark contents of nucleon from chiral fermions |
E Gamiz Extraction of |V_{us}| from the calculation of K- >pi l nu form factors with Nf=2+1 flavors of staggered quarks |
J Simone Data analysis using the Gnu R system for statistical computation |
J Foley Group-theoretical construction of finite-momentum and multiparticle operators for lattice hadron spectroscopy |
| 5:30 | M Wagner Towards finite density QCD with Taylor expansions |
Y Aoki KMI project on many flavor QCD with N_f=12 and 16 |
C Liu Radiative transitions in charmonium from Nf=2 twisted mass lattice QCD |
T Kaneko Kaon semileptonic form factors in QCD with exact chiral symmetry |
F Di Renzo Status of the AuroraScience Project |
C Pelissier Rho Resonance on the Lattice |
| 5:50 | D Smith Universal critical behavior in three flavor QCD |
K-I Nagai KMI (Nagoya) project; Many flavor QCD as exploration of the walking behavior with approximate IR fixed point |
X Feng Two-photon decays of neutral pion from 2+1 flavor lattice QCD |
J Yu Long distance contribution to K_{L} K_ {S} mass difference |
C Pinke LatticeQCD using OpenCL |
S Prelovsek Decay of the rho and a1 mesons on the lattice using distillation |
| 6:10 | H Saito Finite density QCD phase transition in the heavy quark mass region |
M Lin Lattice simulations of SU(3) gauge theory with ten flavors of Dirac fermions |
M Giordano Rising total cross sections and soft high-energy scattering on the lattice |
N Christ Computing the longdistance contribution to the kaon mixing parameter epsilon_K |
D Rossetti APEnet+ project status |
N Ishizuka Rho meson decay width from 2+1 flavor lattice QCD |
| 6:30 | GLOBUS ONLINE (SPONSOR) Reliable Data Movement via SaaS (Raj Kettimuthu) |
C Schroeder The Running Coupling and Finite Temperature for Twelve Flavors and Three Colors |
N Ishii Time-dependent effective Schroedinger equation for lattice nuclear potentials |
Q Liu Practical methods for a direct calculation of \Delta I=1/2 K to \pi\pi Decay |
H Kawai (CANCELLED) Multicanonical HMC simulation of the SU(3) lattice gauge theory |
B Menadue The 1405 MeV Lambda Resonance in Full-QCD |
Tuesday 1
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Chiral Symmetry | Hadron Spectroscopy | SM Parameters and Renormalization | Weak Decays and Matrix Elements |
| 3:00 | B Klein Scaling behavior in two-flavor QCD, finite quark masses and finite volume effects |
D Schaich S parameter and parity doubling below the conformal window |
P Buividovich A method for resummation of perturbative xpansion based on the stochastic solution of Schwinger- Dyson equations |
D Leinweber (for M. Mahbub) Nucleon Mass Spectrum in Full QCD |
S Sharpe Non-perturbative renormalization for general improved staggered bilinears |
E Freeland Standard Model matrix elements for Bbbar Mixing from 2+1 flavor lattice QCD |
| 3:20 | A Mishra (CANCELLED) Meta-stable States in Quark-Gluon Plasma |
H Ohki Study of the infrared behavior in SU(2) gauge theory with eight flavors |
A Hietanen Interface tension of 3d 4- states Potts model using the Wang-Landau algorithm |
S Wallace Excited state baryon spectroscopy from lattice QCD |
X Du RI-MOM scheme renormalization constants (Nf=4) and the running coupling constant (Nf=2+1+1) using twisted-Wilson quarks |
C Bouchard The hadronic contribution to beyond the Standard Model B-mixing |
| 3:40 | S Lottini Strong coupling effective theory with heavy fermions |
T Karavirta Exploring the conformal window: SU (2) gauge theory on the lattice |
Y Meurice QCD calculations with optical lattices? |
T Yamazaki Bound state of twonucleon systems in quenched lattice QCD |
D Palao Renormalization constants of quark bilinears in lattice QCD with four dynamical Wilson quarks |
J Shigemitsu Studies of B and B_s Meson Leptonic Decays with NRQCD Bottom and HISQ Light/Strange Quarks |
| 4:00 | N Yamamoto Universality of phase diagrams in QCD and QCD-like theories |
G Voronov Lattice Study of the Extent of the Conformal Window in Two-Color Yang-Mills Theory |
B Leder Fermions as global correction in lattice QCD |
T Inoue Bound H-dibaryon from Full QCD Simulation on the Lattice |
M Hasegawa Renormalization constants for Iwasaki action |
R Zhou Form factors for B to Kll semileptonic decay from three-flavor lattice QCD |
| 4:20 | J Langelage Towards a nonperturbative measurement of the heavy quark momentum diffusion coefficient |
M Buchoff Pion scattering in QCD-like theories below conformality |
M Striebel Symmetric Partitioned Runge-Kutta Methods for Differential Equations on Lie-Groups |
C Morningstar Excited-state hadron masses using the stochastic LapH method |
C Lehner RI/SMOM schemes for Delta S=1 and Delta S=2 operators |
D Du Semileptonic form-factor ratio f_0(B\to D)/f_0(B_s\to D_s) and its application to BR(B_s\to\mu^+\mu^-) |
Tuesday 2
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Theoretical Developments | Hadron Structure | SM Parameters and Renormalization | Hadron Spectroscopy |
| 5:10 | K Anagnostopoulos Towards an Effective Importance Sampling in Monte Carlo Simulations of a System with a Complex Action |
T DeGrand Gauge theories with fermions in the twoindex symmetric representation |
M Golterman Flavor symmetry breaking in mixed-action QCD |
S Syritsyn Quark contribution to nucleon momentum and spin from calculations with Domain Wall fermions |
C Bauer The static quark self-energy at large orders from NSPT |
D Bolton Charm meson spectroscopy and decay constants |
| 5:30 | J Bloch Evading the sign problem in random matrix simulations |
Y Shamir Renormalized coupling from gluon exchange in the Schrodinger functional |
Y Liu Volume Effects in Discrete Beta Functions |
J Green Excited state contamination in nucleon structure calculations |
D Hesse Automated lattice perturbation theory applied to HQET |
R Briceno Charm baryon spectroscopy |
| 5:50 | W Unger Continuous Time Monte Carlo for QCD in the Strong Coupling Limit |
D Sinclair The chiral phase transition for QCD with sextet quarks |
H Zou Comparison of improved perturbative methods |
S Ohta Nucleon structure from 2+1f dynamical DWF lattice QCD at nearly physical pion mass |
A Lytle Non-perturbative renormalization of kaon fourquark operators on coarse domain wall ensembles |
Y Chen Lattice study on glueballs in J/psi radiative decays |
| 6:10 | Y Delgado Worm Algorithms for the QCD Phase Diagram with Effective Theories |
S Sint Perturbative lattice artefacts in the SF coupling for technicolor-inspired models |
M Hanada Recent progress of lattice and non-lattice super Yang-Mills |
K Liu Quark and glue momenta and angular momentum in the nucleon |
N Garron NPR of K\to\pi\pi operators with a step scaling matrix |
A Athenodorou Cutoff effects of heavy quark vacuum polarization at one-loop order |
Wednesday 1
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Theoretical Developments | Chiral Symmetry | Hadron Spectroscopy | Weak Decays and Matrix Elements |
| 8:30 | S Katz Correlations and fluctuations at finite temperature |
L Keegan Systematic Errors of the MCRG Method |
N Kawamoto A new lattice SUSY formulation for D=N=2 Wess-Zumino model with species doublers as supermultiplet |
G Colangelo Hard pion chiral perturbation theory |
L Liu Charmonium Spectrum from Anisotropic Lattices |
I Kanamori Disconnected contributions to Dmeson semi-leptonic decay form factors |
| 8:50 | F Burger Thermodynamics from Twisted Mass Lattice QCD |
T Tomboulis Fermion RG blocking transformations and conformal windows |
M Honda Testing the AdS/CFT correspondence by Monte Carlo calculation of BPS and non-BPS Wilson loops in N=4 super-Yang-Mills theory |
M Lightman Staggered chiral perturbation theory fits to light pseudoscalar masses and decay constants from HISQ ensembles |
S Ryan Disconnected diagrams in charmonium physics |
G Donald Axial vector form factors in Ds to phi semileptonic decays from lattice QCD |
| 9:10 | S Krieg The QCD equation of state and the effects of the charm |
A Hasenfratz MCRG study of 12 fundamental flavors with mixed fundamental-adjoint gauge action |
K Usui Reflection Positivity of N=1 Wess-Zumino model on the lattice with exact U(1) _R symmetry |
H-J Kim Non-Goldstone pion masses with NLO in Staggered Chiral Perturbation Theory |
D Mohler Charmed meson spectroscopy on the lattice |
J Koponen The D to K and D to pi semileptonic decay form factors from Lattice QCD |
| 9:30 | H-T Ding Exploring the QCD phase diagram at \mu=0 with HISQ fermions |
L Del Debbio RG flows in 3D scalar field theory |
D Baumgartner Supersymmetry on the lattice: Exact results for supersymmetric quantum mechanics |
F Bernardoni Determination of the Wilson ChPT low energy constant c2 |
Y Namekawa Charm quark system on the physical point in 2+1 flavor lattice QCD |
H Na Heavy-light meson semileptonic decays and precision tests of the Standard Model |
| 9:50 | H Ohno Eigenvalue distribution of the Dirac operator at finite temperature with (2+1)- flavor dynamical quarks using the HISQ action |
U Wenger Supersymmetry on the lattice: the N=1 Wess- Zumino model |
A Walker Loud Evidence for chiral logarithms in the baryon spectrum |
P Rubio Spectra of heavy-light and heavy-heavy mesons containing charm quarks, including higher spin states for Nf=2+1 QCDSF configurations |
J Bailey Semileptonic form factors and |V_cs(d) | from 2+1 flavor lattice QCD |
Wednesday 2
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Vacuum Structure and Confinement | Hadron Spectroscopy | Chiral Symmetry | Algorithms and Machines |
| 10:40 | A Bazavov Determination of the transition temperature T_c in 2+1 flavor QCD: combined result with the p4, asqtad and HISQ/tree actions |
A Patella Finite volume effects in SU(2) with two adjoint fermions |
F Gruber Topology of dynamical lattice configurations including results from overlap fermions |
N Ukita 1+1+1 flavor QCD+QED simulation at the physical point |
U Heller Low-lying Dirac operator eigenvalues, lattice effects and random matrix theory |
S Cohen Multigrid Algorithms for Domain-Wall Fermions |
| 11:00 | D Nogradi QCD thermodynamics with Wilson fermions |
M Koren Large-N reduction in QCD with two adjoint Dirac fermions |
H Thacker Chiral Quark Dynamics and the Ramond-Ramond U(1) Gauge Field |
K Ottnad Masses of eta, eta' Mesons from 2+1+1 Twisted Mass Lattice QCD |
J Osborn Chiral random matrix theory for staggered fermions |
K Kahl Adaptive Algebraic Multigrid in QCD computations |
| 11:20 | M Cheng The finite temperature QCD phase transition from domain wall fermions |
P Korcyl Preliminary study of two-dimensional SU(N) Yang-Mills theory with adjoint matter with Hybrid Monte Carlo approach |
F Negro Chiral Properties of Strong Interactions in a Magnetic Background |
E Gregory The eta' meson with staggered fermions |
E Follana Spectral Flow and Index Theorem for Staggered Fermions |
Y Nakamura Modified block BiCGSTAB for lattice QCD |
| 11:40 | Z Lin Dirac Eigenvalue Spectrum at Finite Temperature Using Domain Wall Fermions |
K Miura Thermodynamic Study for Conformal Phase in Large Nf Gauge Theory |
S Edwards Fractional electric charge and quark confinement |
D Adams (CANCELLED) Pseudoscalar mesons in lattice QCD with staggered Wilson fermions |
J Verbaarschot Progress on the Microscopic Spectrum of the Dirac Operator for QCD with Wilson Fermions |
S Birk dsBlockCG: CG for multiple right hand sides and multiple shifts |
| 12:00 | E Goode Delta I = 3/2 K to pi pi decay amplitudes with nearly physical kinematics |
A Alexandru Absolute X-distribution and self-duality |
E Scholz SU(2) low-energy constants from staggered 2+1 flavor simulations |
T Kimura Index Theorem and Overlap Formalism with Naive and Minimally Doubled Fermions |
M Rottmann Aggregation-based Multilevel Methods for Lattice QCD |
Thursday 1
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Theoretical Developments | Algorithms and Machines | Chiral Symmetry | Hadron Structure |
| 3:00 | M Ogilvie (CANCELED) Phases of SU(N) Gauge Theories on R^ (4-p) x T^p |
C Rebbi Hybrid Monte Carlo simulation of graphene |
F Bruckmann Dressed Wilson loops as dual condensates in response to magnetic and electric fields |
S Gottlieb Progress on the QUDA code suite |
S Necco Light quark correlators in a mixed action setup |
J Wasem First Calculation of Nuclear Parity Violation from Lattice QCD |
| 3:20 | B Berg SU(3) Deconfining phase transition with lower boundary temperatures in the scaling region |
R Brower The time continuum limit for the Graphene Tight Binding Model |
A Shindler On the spectral density of the Wilson operator |
M Clark Using domain decomposition algorithms to strong scale past 100 GPUs |
H Fukaya Chiral interpolation in a finite volume |
H Nemura Baryon-Baryon Interaction of Strangeness S=-1 Sector |
| 3:40 | M Panero Renormalization of Polyakov loops in different representations and the large-N limit |
Y Araki Chiral symmetry restoration in monolayer graphene induced by Kekule distortion |
A Deuzeman Topology and chiral perturbation theory from the Wilson Dirac spectrum |
F Winter Accelerating QDP++ using GPUs |
A Vaquero Symmetries and vacuum structure inside the Aoki phase |
T Doi Three-Nucleon Forces explored by Lattice QCD Simulations |
| 4:00 | L Giusti Thermal momentum distribution from shifted boundary conditions |
J Drut The unitary Fermi gas at finite temperature: momentum distribution and contact. |
J Giedt Backwards Running From Creutz Ratios |
K Petrov Automated LQCD code generation for future architectures |
T Misumi Aoki Phases in the Lattice Gross-Neveu Model with Flavored Mass terms |
K Sasaki Strangeness S=-2 baryon-baryon interactions from lattice QCD |
| 4:20 | T Lahde Strongly coupled Graphene on the Lattice |
V Maillart Loop formulation of O(N) Gross-Neveu models: Results for the Thirring model |
A Frommer Accurate error bounds and estimates for the sign function |
N Cundy Gell Mann Oakes Renner relation for multiple chiral symmetries |
Y Ikeda S-wave meson-baryon potentials with strangeness from Lattice QCD |
Thursday 2
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Vacuum Structure and Confinement | SM Parameters and Renormalization | Theoretical Developments | Hadron Structure |
| 5:10 | F Pittler Poisson statistics in the high temperature QCD Dirac spectrum |
D Mehta Sign problem for supersymmetric Yang- Mills theories on the lattice |
A Bakry Gluonic profile of the static baryon at finite temperature |
C Sachrajda Determination of Light Quark Masses |
H Vairinhos Phase transitions in centerstabilized lattice gauge theories |
V Drach Nucleon scalar matrix elements with N_f=2+1+1 twisted mass fermions |
| 5:30 | T Kovacs Quark localization by Polyakov loops in high temperature QCD |
R Galvez Numerical results regarding the sign problem in 2 dimensional Supersymmetric Yang- Mills theories with 4 and 16 supercharges |
J Greensite k-string tensions and the 1/N expansion |
Z Fodor Lattice QCD at the physical point |
H Neuberger Continuous smearing of Wilson Loops |
C Aubin An improved method for extracting matrix elements from lattice threepoint functions |
| 5:50 | A Yamamoto Lattice QCD simulation at finite chiral chemical potential |
G Bergner Supersymmetric Yang- Mills theory: a first step towards the continuum |
R Millo Vacuum Manifold Projection: a technique for calculating the effective Hamiltonian for low-energy vacuum gauge fields, using Lattice calculations |
C Hoelbling Light quark masses |
R Lohmayer Numerical study of large-N phase transition of smeared Wilson loops in 4D pure YM theory |
S Dinter Excited state Effects in Nucleon Matrix Element Calculations |
| 6:10 | G Cossu Topological susceptibility and axial symmetry at finite temperature |
S-W Kim Lattice study of 4d N=1 super Yang-Mills theory with dynamical overlap gluino |
P Bicudo Colour flux-tubes in static Pentaquark and Tetraquark systems |
S Durr Kaon bag parameter B_K from 2+1 flavor 2- HEX simulations |
J Wosiek Confinement in multiparton sectors of SYM_2 with addjoint fermions |
A Schafer Disconnected Contibutions for nucleon 3-point functions |
Friday 1
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Vacuum Structure and Confinement | Hadron Structure | Algorithms and Machines | Weak Decays and Matrix Elements |
| 3:00 | Y Nakegawa Histogram method in finite density QCD with phase quenched simulations |
S Chandrasekharan The generalized fermion-bag approach |
D Leinweber Impact of center vortex removal on chiral symmetry breaking in SU (3) gauge field theory |
S Sasaki Hyperon vector form factors with 2+1 flavor dynamical domain-wall fermions |
A Abdel- Rehim Application of Quadrature Methods for Re-Weighting in Lattice QCD |
C Kelly Continuum Results for Light Hadronic Quantities using Domain Wall Fermions with the Iwasaki and DSDR Gauge Actions |
| 3:20 | O Philipsen Corrections to the strong coupling limit of staggered QCD |
A Li Quantum Critical Behavior of the Massless Thirring Model |
A Shibata Dual Meissner effect and non-Abelian dual superconductivity in SU(3) Yang-Mills theory |
E Kerrane DWF calculation of the leading order hadronic vacuum polarisation to g- 2 of the muon |
H Yin Improving DWF Simulations: Force Gradient Integrator and the Mobius Accelerated DWF Solver |
B Glaessle EM corrections to pseudoscalar decay constants |
| 3:40 | P de Forcrand Constraints on the two-flavor QCD phase diagram from imaginary chemical potential |
C-J David Lin Study of the Higgs- Yukawa Theory at the Strong-Yukawa Regime |
L von Smekal Lattice Landau Gauges without Frontiers |
J Zanotti Nucleon Form Factors - Closing in on the physical pion |
C Miao Determinant reweighting for O (a) improved Wilson fermions |
Y Yang Radiative decay of \eta_{c2} to \gamma J/\psi |
| 4:00 | P Giudice Quark number susceptibility at finite density and low temperature |
A Maas The Higgs mass, bound states, and gauge invariance |
B Wellegehausen Phase diagram of the G(2) Higgs model |
B Jaeger Lattice Determination of the Anomalous Magnetic Moment of the Muon |
S Schaefer The scaling of the Hybrid Monte Carlo algorithm |
P Fritzsch M_b and f_B from non-perturbatively renormalized HQET with Nf=2 light quarks |
| 4:20 | S Takeda On the phase of quark determinant in lattice QCD with finite chemical potential |
D Mesterhazy Anomalous scaling in the random-forcedriven Burgers equation: A Monte Carlo study |
R Hollwieser Intersections of thick Center Vortices, Dirac Eigenmodes and Fractional Topological Charge in SU(2) Lattice Gauge Theory |
S Meinel Axial couplings of heavy hadrons from domainwall lattice QCD |
C Maynard Tools for the ILDG |
R Sommer On the computation of hadron-tohadron matrix elements |
Friday 2
| Room | Alpenglow | Mountain Stream B | Mountain Stream C | Palisades Hall A | Palisades Hall B | Palisades Hall C |
|---|---|---|---|---|---|---|
| Topic | Nonzero Temp/Density | Applications beyond QCD | Hadron Spectroscopy | Hadron Structure | SM Parameters and Renormalization | Weak Decays and Matrix Elements |
| 5:10 | T Mendes Electric and magnetic screening masses around the deconfinement transition |
F Knechtli Dimensional reduction from five-dimensional gauge theories |
T Hammant Radiative improvement of the lattice NRQCD action using the background field method and application to the hyperfine splitting of quarkonium states |
T Primer Magnetic Properties of the Nucleon |
D Pleiter Quark masses from Nf=2 Clover fermions - an update |
S Qiu Semileptonic B to D decays with 2+1 flavors |
| 5:30 | R Aouane On Gluon and Ghost Propagators in QCD at finite temperature |
K Yoneyama The Lattice Mean-Field Approximation of Gauge-Higgs Unification on the Orbifold |
M Hetzenegger Potentials between pairs of static-light mesons |
G Schierholz Electric Dipole Moment of the Neutron |
M Petschlies Current-Current correlators in Twisted Mass Lattice QCD |
O Witzel B-meson physics with dynamical domain-wall light quarks and nonperturbatively tuned relativisitc bquarks |
| 5:50 | H Iida Inter-quark potentials from NBS amplitudes and their applications |
E Rinaldi Scalar mass corrections from compact extra dimensions on the lattice |
R Dowdall B and bottomonium physics from lattice QCD including c quarks in the sea |
M Lujan Electric polarizability with overlap fermions |
G Koutsou mc/ms with Brillouin improved Wilson fermions |
R Van de Water Pion and kaon decay constants and B_K from mixed-action lattice QCD |
| 6:10 | J-W Lee Extended study for unitary fermions on lattice using cumulant expansion technique |
D Coumbe Exploring the Phase Diagram for Lattice Quantum Gravity |
T Kawanai Interquark potential for the charmonium system with almost physical quark masses |
M Engelhardt Exploration of the electric spin polarizability of the neutron in lattice QCD |
L Lellouch Chiral behavior of Nambu- Goldstone boson masses and decay constants |
B Yoon Covariance fitting of highly correlated B_K data |
| 6:30 | G von Hippel Scale setting via the Omega baryon mass |
A Portelli Electromagnetic corrections to light hadron masses |
M Marinkovic Strange quark mass and Lambda parameter by the ALPHA collaboration |
J Kim Finite volume effects in B_K with improved staggered fermions |
Parallel Session Chairs
| Session | Alpenglow | Mountain Stream B | Mountain Stream C | Pallisades Hall A | Pallisades Hall B | Pallisades Hall C |
|---|---|---|---|---|---|---|
| Monday 1 |
S. Mukherjee (Non-Zero Temp/Density) |
A. Hasenfratz (Applications beyond QCD) |
J. Osborn (Chiral Symmetry) |
C. Morningstar (Hadron Spectroscopy) |
K-F. Liu (Hadron Structure) |
J. Zanotti (Weak Decays & Matrix Elements) |
| Monday 2 |
P. de Forcrand (Non-Zero Temp/Density) |
Y. Shamir (Applications beyond QCD) |
B. Tiburzi (Hadron Structure) |
W. Lee (Weak Decays & Matrix Elements) |
S. Gottlieb (Algorithms & Machines) |
S. Wallace (Hadron Spectroscopy) |
| Tuesday 1 |
F. Karsch (Non-Zero Temp/Density) |
J. Kuti (Applications beyond QCD) |
M. Clark (Algorithms & Machines) |
K. Orginos (Hadron Spectroscopy) |
S. Durr (SM Parameters & Renormalization) |
N. Christ (Weak Decays & Matrix Elements) |
| Tuesday 2 |
J. Verbaarachot (Non-Zero Temp/Density) |
G. Fleming (Applications beyond QCD) |
J. Wosiek (Theoretical Developments) |
Y. Aoki (Hadron Structure) |
A. Kronfeld (SM Parameters & Renormalization) |
S. Ryan (Hadron Spectroscopy) |
| Wednesday 1 |
C. DeTar (Non-Zero Temp/Density) |
S. Takeda (Applications beyond QCD) |
M. Unsal (Theoretical Developments) |
M. Golterman (Chiral Symmetry) |
J. Foley (Hadron Spectroscopy) |
E. Freeland (Weak Decays & Matrix Elements) |
| Wednesday 2 |
R. Gupta (Non-Zero Temp/Density) |
D. Sinclair (Applications beyond QCD) |
M. Hanada (Vacuum Structure & Confinement) |
C. Sachrajda (Hadron Spectroscopy) |
J. Laiho (Chiral Symmetry) |
T. Kennedy (Algorithms & Machines) |
| Thursday 1 |
S. Chandrasekharan (Non-Zero Temp/Density) |
M. Endres (Applications beyond QCD) |
D. Adams (Theoretical Developments) |
B. Joo (Algorithms & Machines) |
G. Colangelo (Chiral Symmetry) |
C. D. Lin (Hadron Structure) |
| Thursday 2 |
A. Bazavov (Non-Zero Temp/Density) |
J. Giedt (Applications beyond QCD) |
H. Thacker (Vacuum Structure & Confinement) |
C. Bernard (SM Parameters & Renormalization) |
S. Sint (Theoretical Developments) |
D. Renner (Hadron Structure) |
| Friday 1 |
S. Krieg (Non-Zero Temp/Density) |
T. Tomboulis (Applications beyond QCD) |
J. Greensite( (Vacuum Structure & Confinement) |
C. Aubin (Hadron Structure) |
R. Brower (Algorithms & Machines) |
B. Mawhinney (Weak Decays & Matrix Elements) |
| Friday 2 |
S. Katz (Non-Zero Temp/Density) |
A. Maas (Applications beyond QCD) |
M. Creutz (Hadron Spectroscopy) |
W. Detmold (Hadron Structure) |
R. Sommer (SM Parameters & Renormalization) |
B. Sugar (Weak Decays & Matrix Elements) |
Poster Session
| Loc | First Name | Last Name | Institution | Title | Abstract | Collaborators |
|---|---|---|---|---|---|---|
| 1 | Andreas | Athenodorou | DESY Zeuthen | Closed 2+1 dimensional SU(N) flux-tubes as bosonic strings | We investigate the spectrum of confining flux-tubes that wind around a spatial torus of variable length l in D=2+1. The energies of the lowest ~30 states are compared to the free string Nambu-Goto model in flat space-time and in addition to recent results on the universal properties of effective string actions. We focus on our calculations in SU(6) at a very small lattice spacing; this is checked to be very close to the large-N continuum limit. Astonishingly, the spectrum of the closed flux-tube can be very well approximated by Nambu-Goto even at short lengths which are comparable to its width and even well below the critical length at which the expansion of the Nambu-Goto energy in powers of 1/l^2 diverges. In contrast to our recent results in D=3+1, we do not find any evidence for the presence of any non-string-like states associated to excitations of massive flux-tube modes. | Andreas Athenodorou, Michael Teper |
| 2 | Pedro | Bicudo | IST, Lisboa | String tension at finite temperature Lattice QCD | The critical curve of string tension as a function of the temperature is computed in SU(3) Lattice QCD. We present the results for the string tension utilizing a pair of Polyakov loop and antiloop, with two different techniques. We compare the colour averaged loop-antiloop which is gauge invariant but is only adequate to study the string tension, and the colour singlet loop-antiloop using the Landau gauge fixing which also enables to compute the coulomb part of the free energy . | Nuno Cardoso, Orlando Oliveira, Pedro Bicudo |
| 3 | Michele | Brambilla | ECT* | Efficiency on multi-core CPUs: the Wilson Dirac operator on Aurora | The Aurora machine is based on Intel Westmere processors, interconnected by a high speed (FPGA-based) torus network. An optimized code has to be tuned to the CPU architecture. A current trend in modern CPUs is the increasing number of cores per socket, with different levels of cache. These can be either shared between cores or reserved to a single one. We present different strategies for the implementation of the Wilson Dirac operator which aim at maximizing the performance on the Aurora architecture. | M. Brambilla, F. Di Renzo and M. Grossi |
| 4 | John | Bulava | DESY Zeuthen | Upper and lower Higgs mass bounds in the presence of a 4th generation | We present ongoing results from a chirally-invariant Higgs-Yukawa model. Specifically, we examine the effect of a potential heavy fourth generation of quarks on the upper and lower Higgs boson mass bounds. | John Bulava, Karl Jansen, Jim Kallarackal, Atilla Nagy |
| 5 | Bipasha | Chakraborty | U of Kentucky | Quark orbital angular momentum from lattice QCD | We calculate the quark orbital angular momentum of the nucleon from the quark energy-momentum tensor form factors on the lattice. The calculation is done on a quenched 16^3 \times 24 lattice at \beta=6.0 and with Wilson fermions at \kappa= 0.154, 0.155, 0.1555. We calculate the disconnected insertion stochastically which employs the Z_2 noise with an unbiased subtraction. This proves to be an efficient method to reduce the error from the noise. | Bipasha Chakraborty, Devdatta Mankame, Mridupawan Deka, Takumi Doi, Terrence Draper, Keh-Fei Liu |
| 6 | Gennaro | Cortese | CSIC U of Zaragoza & U della Calabria | Critical properties of 2D Z(N) vector models for N>4 | We investigate the critical properties of two-dimensional Z(N) vector models for N larger than 4. We locate critical points and determine a few critical indices. We study also the behaviour with N of the helicity modulus. | O. Borisenko, G. Cortese, R. Fiore, M. Gravina, A. Papa |
| 7 | Alan | denBleyker | U of Iowa | Fisher's zeros, complex RG flows and confinement in LGT models. | The zeros of the partition function in the complex beta plane (Fisher's zeros) play an important role in our understanding of phase transitions and RG flows. Recently, it has been argued that they act as gates or separatrices for complex RG flows. Using reweighting and contructions of the density of states, we calculate the Fisher's zeros for pure gauge SU(2) and U(1) on L^4 lattices. For SU(2), these zeros appear to move almost horizontally when the volume increases. They stay away from the real axis which indicates a confining theory at zero temperature. We discuss the effect of an adjoint term on these results. In contrast, using recent multicanonical simulations for the U(1) model for L up to 8 we find that the imaginary part of the zeros scales as L^{-3.07} and pinches the real axis at beta near 1.0113. Preliminary results concerning higher volumes will be presented. We will also discuss recent results for SU (3) with various numbers of flavors. | A. Bazavov, A. Denbleyker, Daping Du, Yuzhi Liu, Y. Meurice, B. Oktay and D. Sinclair |
| 8 | Massimo | DiPierro | DePaul U | A new user interface for the Gauge Connection lattice data archive U | The user interface to the gauge connection is being completely redesigned using web2py and grid tools, giving more functionality for the user. | J. Hetrick, David Skinner, and Shreyas Cholia |
| 9 | Shao-Jing | Dong | U of Kentucky | Flavor-singlet Z_A from Overlap Fermions on 2+1 flavor DWF configurations | The flavor-singlet axial renormalization constant Z_A is calculated via the anomalous Ward identity. Overlap fermion is used as the valence and topological charge operator is defined from the Overlap Dirac operator D^{ov}. The numerical calculation is done with the 2+1 flavor DWF configurations on 24^3 x 64 lattice. | S.J. Dong, A. Li, Ming Gong, K.F.Liu |
| 10 | Eigo | Shintani | RIKEN-BNL | Proton decay matrix elements in 2+1 domain-wall fermion | We present the first result of proton decay matrix elements in 2+1 flavor domain-wall fermion. We show the numerical results of form factor obtained from three-point function (i.e. without reducing the final state pi/K meson) with baryon number asymmetric 6- dimensional operator and twelve independent matrix elements of proton to meson decay in the physical kinematics. We also compare with the results from soft-pion theorem and quenched approximation. | Y. Aoki, T. Izubuchi, E. Shintani, A. Soni (RBC collaboration) |
| 11 | Pietro | Giudice | Swansea U | Lattice Planar QED in external magnetic field | We investigate planar Quantum ElectroDynamics (QED) with two degenerate staggered fermions in an external magnetic field on the lattice. Our preliminary results indicate that in external magnetic fields there is dynamical generation of mass for two-dimensional massless Dirac fermions in the weak coupling region. We comment on possible implications to the quantum Hall effect in graphene. | Paolo Cea, Leonardo Cosmai, Pietro Giudice, Alessandro Papa |
| 12 | Leonardo | Giusti | U of Milano- Bicocca | Glueball masses from ratios of path integrals | By generalizing our previous work on the parity symmetry, the partition function of a Yang--Mills theory is decomposed into a sum of path integrals each giving the contribution from multiplets of states with fixed quantum numbers associated to parity, charge conjugation, translations, rotations and central conjugations Z_N^3. Ratios of path integrals and correlation functions can then be computed with a multi-level Monte Carlo integration scheme whose numerical cost, at a fixed statistical precision and at asymptotically large times, increases power-like with the time extent of the lattice. The strategy is implemented for the SU(3) Yang--Mills theory, and a full-fledged computation of the mass and multiplicity of the lightest glueball with vacuum quantum numbers is carried out at two values of the lattice spacing (0.17 and 0.12 fm). | Michele Della Morte, Leonardo Giusti |
| 13 | Yong-Chull | Jang | Seoul National U | Multi GPU Performance of Conjugate Gradient Solver with Staggered Fermions in Mixed Precision | GPU has a significantly higher performance in single-precision computing than that of double precision. Hence, it is important to take a maximal advantage of the single precision in the CG inverter as suggested by the mixed precision algorithm. We have implemented mixed precision algorithm to our multi GPU conjugate gradient solver. By the single precision calculation, the bandwidth bottleneck is relieved and overall performance is doubled. We use MILC fine lattices (28^3\times 96, 40^3\times 96) to test the performance of nvidia GTX480 GPU. | Yong-Chull Jang, Hyung-Jin Kim, Weonjong Lee |
| 14 | Frithjof | Karsch | Brookhaven National Laboratory | Universal behavior in 3d O(4) models: The scaling function of the free energy and its derivatives | In contrast to the well established scaling function f_G(z) and f_\chi (z), which control the universal behavior of the order parameter and its susceptibility, we calculate the singular part of the free energy of the 3d O(4) spin model in terms of the scaling variable z ~ (T-Tc)/ (Tc H^{1/\beta\delta}). The main motivation for this calculation was to get access to derivatives of the scaling function for the free energy, which play a central role in the discussion of universal properties of moments of baryon number fluctuations in QCD. | Frithjof Karsch and Juergen Engels |
| 15 | Tony | Kennedy | U of Edinburgh | Partial spectrum of large hermitean matrices | We present a new variant of a Krylov space algorithm for finding the eigenpairs of a large hermitean matrix where the eigenvalues lie in a specified low density part of the spectrum. The method uses selective re-orthogonalization and re-starting to find each eigenpair once. We present theoretical bounds on the convergence rate, and show that these work well in practice for the hermitean Wilson Dirac operator. We have implemented the method in Chroma, and we show that it is significantly faster than the Ritz currently available. | A D Kennedy and Chris Johnson |
| 16 | Mario | Kieburg | State U of New York at Stony Brook | Random Matrix Models for Dirac Operators at finite Lattice Spacing | Chiral random matrix theory is a powerful mathematical tool to calculate eigenvalue correlations in the infrared limit of quantum chromodynamics (QCD). Since the 90's it has been successfully applied to the continuum limit of QCD. In this poster we use these methods to study discretization effects for Wilson fermions and staggered fermions. First we discuss a random matrix model for the Wilson-Dirac operator with fermions in the fundamental representation for more than two colors. We have obtained an analytical result for the joint probability density function of this matrix model in terms of a determinantal expression over complex pairs of eigenvalues, and real eigenvalues with positive or negative chirality. The explicit dependence on the lattice spacing can be readily read off from our results which are compared to numerical simulations of the random matrix theory. For the staggered Dirac operator we have studied random matrices modeling the transition to degenerate eigenvalues in the continuum limit. For cases with anti-unitary symmetries the model describes the transition between different antiunitary symmetries in the approach to this limit. | Mario Kieburg, Jacobus Verbaarschot, and Savvas Zafeiropoulos |
| 17 | Andreas | Kronfeld | Fermilab | The 't Hooft vertex for staggered fermions and flavor-singlet mesons | We derive the 't Hooft vertex for staggered fermions and examine its symmetries. We also derive a set of structural properties for the eigenvectors of the staggered Dirac operator, which should emerge in the continuum limit, if staggered fermions yield four species. We show numerically that the needed structure arises. This structure and symmetry of (unrooted) staggered fermions also imply that objections to the rooted determinant based on the ’t Hooft vertex are without foundation. | Gordon Donald, Christine Davies, Eduardo Follana, Andreas Kronfeld |
| 18 | Kim | Kwangwoo | Seoul National U | SU(3) Analysis of B_K with improved staggered quarks | We present a recent progress in data analysis of B_K calculated using improved staggered quarks. The fitting functional form is based on the SU(3) staggered chiral perturbation theory at the next to leading order. The results are compared with those of SU(2) analysis to check the self-consistency. | Kwangwoo Kim, Hyung-jin Kim, Boram Yoon, Jangho Kim, Yongchull Jang, Sunghee Kim, Weonjong Lee, Chulwoo Jung, Steve Sharpe |
| 19 | Bjorn | Leder | Wuppertal U | The static potential with dynamical fermions from Wilson loops | We present the analysis of the static potential extracted from Wilson loops measured on CLS ensembles generated with Wilson gauge action and Nf=2 flavors of O(a) improved Wilson quarks at three different lattice spacings and a range of quark masses. The shape of the static potential at distances well below the string breaking region is studied in terms of renormalized couplings derived from the static force and its derivative. We comment on the (im)possibility of extracting the Lambda parameter at our smallest lattice spacing a=0. 05 fm. Finally we give an update on the scale determination through r0. | Francesco Knechtli, Bjorn Leder |
| 20 | Frank | Lee | George Washington U | Spin Polarizabilties on the Lattice | Spin polarizabilities provide information on the internal struture of hadrons in the presence of weak electromagnetic fields, and are actively studied by Compton scattering experiments. They provide finer detail than the regular polarizabilties since they are induced by space and time-varying fields. We present a feasibility study of extracting spin polarizabilities using the background field method and lattice techniques. | Frank X. Lee, Andrei Alexdandru |
| 21 | Weonjong | Lee | Seoul National U | Discritization error and fitting in B_K | We have accumulated 9 times more statistics on the MILC fine ensembles to calculate B_K. As a result the data point is shifted by about one sigma. However, it is enough to spoil the linear fitting in a^2. Hence, we need a new fitting functional form and fitting strategy. We discuss about this inconvenient truth. | Weonjong Lee, SWME Collaboration |
| 22 | Kohtaroh | Miura | LNF-INFN | QCD Phase Diagram in Strong Coupling Lattice QCD with Polyakov Loops | In FAIR experiments and beam energy scan program at RHIC, it is the goal to search for the position of the critical point and first-order phase boundary in the QCD phase diagram. Strong Coupling Lattice QCD has been applied to investigate the QCD phase diagram at finite temperature (T) and chemical potential. We take account of both the chiral and Z3-deconfinement dynamics in the strong coupling lattice QCD. We report following results: 1. The critical temperature at zero chemical potential is consistent with those of Monte Carlo simulations in the strong coupling region. 2. In the finite chemical potential region, the critical point temperature reduces and the first order chiral phase transition line shrinks due to the Polyakov loop effects. 3. The Polyakov loop increasing rate (dl/dT) as well as the Polyakov loop susceptibility show double-peak structure as a function of T, a chiral-induced and Z_3-induced peaks in the widerange of beta=2Nc/g^2. These results would give a useful milestone to Monomer-Dimer-Polymer simulations. | Kohtaroh Miura, Akira Ohnishi, Takashi Z. Nakano, and Noboru Kawamoto |
| 23 | Keiko | Murano | RIKEN, Nishina Center | Nuclear forces in the odd parity sector and the LS forces | It was recently pointed out that baryon-baryon potentials can be constructed in lattice QCD from Nambu-Bethe-Salpeter (NBS) wave functions through Schrodinger's equation. In this method cental and tensor potentials appear at the leading order of the derivative expansion, while the LS potential is at next to leading order. Whereas these three potentials play important roles in nuclear physics, only the central and tensor potentials in the even parity sector have been calculated so far. Remaining terms such as the central and tensor potentials in the odd parity sector as well as the LS potential must be determined, in order to employ these potentils in nuclear physics. As a first step toward this direction, we calculate NBS wave functions in the odd parity sector including ones with higher partial waves in Lattice QCD. | K. Murano for HAL QCD Collaboration |
| 24 | Ethan | Neil | Fermilab | B and D meson decay constants from 2+1 flavor improved staggered simulations | We give a preliminary report on new results for the decay constants f_B, f_Bs, f_D, and f_Ds, based on extended runs with higher statistics. These quantities are important tests of the standard model, in particular entering as inputs to the CKM unitarity triangle. This study makes use of MILC (2+1)-flavor asqtad ensembles, with heavy quarks incorporated using the clover action with the Fermilab method. Ensembles used vary in lattice spacing from a = 0.06 to 0.15 fm, with light sea quark masses down to 1/20 of the strange quark mass. Partially quenched, staggered chiral perturbation theory is used to extract the decay constants at the physical point. Final results from an older version of the calculation are also presented. | Ethan T. Neil, Jon A. Bailey, A. Bazavov, C. Bernard, C. 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, and R.S. Van de Water |
| 25 | James | Osborne | San Francisco State U | On the Extraction of the Strong Coupling Constant from Hadronic Tau Decay | The extraction of the strong coupling constant from hadronic tau decay provides its most precise experimental determination, resulting in uncertainties competitive with determinations on the lattice. We examine the effect of duality violations in the analysis of this data, and propose a more comprehensive method of analysis which accounts for such systematic uncertainties. We conclude that the presence of duality violations contributes a non-negligible systematic uncertainty to the analysis of tau decay data. Our analysis provides a new estimate of the uncertainties, replacing previous incomplete estimates. | D. Boito, O. Cata, M. Golterman, M. Jamin, K. Maltman, J. Osborne, S. Peris |
| 26 | Alessandro | Papa | Universita` della Calabria and INFN-Cosenza | Flux tubes in the SU(3) vacuum | We analyze the distribution of the chromoelectric field generated by a static quark-antiquark pair in the SU(3) vacuum. We find that the transverse profile of the flux tube resembles the dual version of the Abrikosov vortex field distribution and give an estimate of the London penetration length in the confined vacuum. | M.S. Cardaci, P. Cea, L. Cosmai, R. Falcone, A. Papa |
| 27 | Gregory | Petropoulos | U of Colorado | MCRG study of the SU(2) pure gauge model with mixed fundamental-adjoint action | We investigate the bare step scaling function of the pure gauge SU (2) model with mixed fundamental-adjoint plaquette action, using MCRG techniques. The goal of this study is to reveal how MCRG behaves near the first order phase transition line and along its extension toward the fundamental axis and negative adjoint couplings. Our results indicate that the renormalization group flow is not governed any longer by the perturbative fixed point at couplings near or beyond the first order line or its immediate extension. RG matching is no longer feasible in this region. | Anna Hasenfratz, Gregory Petropoulos, Oscar Henriksson |
| 28 | Andrew | Pochinsky | MIT | Lattice QCD with Qlua | We present a Qlua programming language for Lattice QCD. Qlua interfaces the data parallel paradigm with the Lua programming language. It provides a natural framework for integrating highly optimized routines with USQCD libraries into an application. Resulting Qlua scripts are fully portable across architectures. The system has been ported to most of available LQCD platforms. Qlua is available under an open source license. | Andrew V. Pochinsky, Sergey N. Syrithsyn |
| 29 | Takuya | Saito | Kochi U | The center magnetic vortex and its influence on physical quantities in the gluon plasma | We show the evidence that magnetic degrees of freedom are so singular even in the deconfinement phase via a numerical lattice simulation of center magnetic vortex.The magnetic vortices in thermal medium affect gluon propagators, transport coefficients and equation of state of plasma. | T. Saito, Y. Nakagawa and A. Nakamura |
| 30 | Dmitry | Shcherbakov | U Wuppertal | Geometric Numerical Integration Structure-Preserving Algorithms for QCD Simulations | It is well known that molecular dynamics integrators, which can be applied for QCD simulations, often suffer from instabilities. Besides, such issues can arise already in rather simple model systems. Hence, it is a crucial task to avoid these instabilities and we propose to consider state-of-the-art geometric integrators to resolve this problem. Hereby, our goal is to construct a multistep method which preserves both symplectic and symmetry properties of the numerical solution for QCD equations without any losses in accuracy or additional computational efforts. In order to get a first illustrative insight, we apply the integration schemes to the model system of the simple harmonic oscillator and demonstrate the conservation of the geometric properties for the solution of this system. Based on this preliminary investigations, we will decide upon our next steps towards a proper application of these newly obtained methods for more complicated systems, like lattice QCD simulations. References: 1. E. Hairer, C. Lubich, G. Wanner ‚"Geometric Numerical Integration Structure-Preserving Algorithms for Ordinary Differential Equations", Springer Series in Computational Mathematics Vol. 31, 2nd Edition, Springer Heidelberg, 2006. 2. B. Joo ‚"Reversibility and Instabilities in Hybrid Monte Carlo Simulations", in: "QCD and Numerical Analysis", Springer Heidelberg, 2005, pp. 91-99. | Dmitry Shcherbakov |
| 31 | Zhifeng | Shi | The College of William and Mary | Investigations of QCD at nonzero isospin density | We investigate QCD at large isospin density induced by explicit construction of many pion systems via multi-source recursion relations. At large isospin density, corresponding to an isospin chemical potential \mu_I \sim m_{\rho}, we find indications of a phase transition to a conjectured \rho-condensed phase. Further investigations are performed by directly studying rho meson propagation in a pionic medium. | Zhifeng Shi, William Detmold |
| 32 | Tiago | Nunes da Silva | U of Groningen | The strong coupling bulk transition of twelve flavors | We give an update on the status of our study of the phase diagram of SU(3) Yang-Mills theory with twelve flavors of staggered fermions in the fundamental representation. More specifically, we explore the nature of the bulk (zero temperature) transition at strong coupling. The latter has been found in Deuzeman, Lombardo, Pallante "Evidence for a Conformal Phase in SU(3) gauge theories", PRD 82 (2010) 074503, to separate a weak coupling chirally symmetric phase from a strongly coupled chirally broken phase, in accordance with the Appelquist-Miransky-Yamawaki scenario for a conformal window. | Albert Deuzeman, Elisabetta Pallante, Maria Paola Lombardo and Tiago Nunes da Silva |
| 33 | Amarjit | Soni | BNL | Challenges of hadronic weak decays of B-mesons on the lattice | Lattice computation for hadronic weak decays is very challenging. Here we revisit the B -> D P (where P is a pion or kaon) amplitudes. In this we have a situation where there is potentially interesting and important phenomenology and no mixing of lower dimensional operators and consequently also no eye contractions. Furthermore, of most interest for applications to extract the unitarity angle gamma is the ratio: (B->D^0P)/(B-> \bar D^0 P) wherein many systematics will cancel. Taking cue from previous work with kaonic processes such as K to 2pi and as well as semileptonic B and K decays where the final mesons may have a large momentum, we investigate the possible use of such \Hard Pion Heavy-Light ChPT\" to B -> D P. Also direct lattice simulations may have a possible role to the extent that the presence of nearby resonances may be identifiable by studying the time dependence of the relevant correlators" | Christopher Aubin, C.- J. David Lin and Amarjit Soni |
| 34 | Yusuke | Taniguchi | U of Tsukuba | Renormalization factor of four fermi operators with clover fermion and Iwasaki gauge action | We shall present renormalization factors of the four fermi operators at one loop level for the clover fermion and Iwasaki gauge action. We consider the (Delta S)=1 operators and shall simplify the mixing structure by adopting the parity odd part. We shall present both contributions from the penguin diagram and the ordinary four fermi diagram. | N. Ishizuka, Y. Taniguchi, A. Ukawa and T. Yoshie for PACS-CS Collaboration |
| 35 | Chik Him | Wong | Carnegie Mellon U | Excited states and Multi-Hadron Scattering using the stochastic LapH method | The stochastic LapH method is used to study multi-hadron scattering, in particular the two-pion I=0,1,2 scattering and rho meson decay. Quantities of interest such as scattering lengths and phase shifts are extracted from correlator matrices which include disconnected and box diagram contributions. Extraction of excitedstate masses is also presented. | Colin Morningstar, John Bulava, Justin Foley, You-Cyuan Jhang, Keisuke Juge, David Lenkner, Chik Him Wong |
| 36 | Norikazu | Yamada | KEK | Exploring infrared fixed point in SU(N) gauge theories | This talk consists two parts. One is an update of the running coupling constant and the preliminary result of mass anomalous dimension in ten-flavor QCD theory. The other is spectroscopy in many-flavor twocolor QCD, focusing on the phase structure of the Wilson fermion. Both studies are devoted to exploration of infrared fixed point and hence to the construction of realistic technicolor models. | N. Yamada, M. Hayakawa, K.-I. Ishikawa, Y. Osaki, S. Takeda, S. Uno |
| 37 | Raj | Kettimuthu | GLOBUS Online (SPONSOR) | Accelerating Data Movement to Support Lattice QCD Computations |
Committees and Contacts
Local Organizing Committee
Chair: Pavlos Vranas, Lawrence Livermore National Laboratory, vranas2 [at] llnl.gov (vranas2[at]llnl[dot]gov)
Co-Chair: Jim Hetrick, University of the Pacific, jhetrick [at] pacific.edu (jhetrick[at]pacific[dot]edu)
Committee Members:
- Mike Buchoff (Lawrence Livermore National Laboratory)
- Michael Cheng (Lawrence Livermore National Laboratory)
- Maarten Golterman (San Francisco State University)
- Jeff Greensite (San Francisco State University)
- Kieran Holland (University of the Pacific)
- Keisuke Juge (University of the Pacific)
- Joe Kiskis (University of California, Davis)
- Julius Kuti (University of California, San Diego)
- Tom Luu (Lawrence Livermore National Laboratory)
- Ron Soltz (Lawrence Livermore National Laboratory)
- Bob Sugar (University of California, Santa Barbara)
- Sergey Syritsyn (Lawrence Berkeley National Laboratory)
- Terry Tomboulis (University of California, Los Angeles)
- Andre Walker-Loud (Lawrence Berkeley National Laboratory)
- Joe Wasem (Lawrence Livermore National Laboratory)
Conference Secretariat: Catie Dibble, Lawrence Livermore National Laboratory, dibble8 [at] llnl.gov (dibble8[at]llnl[dot]gov)
Artistic Design: Brett DeBoer, University of the Pacific, Chair, Dept. of Visual Arts
Webmaster: Jim McInnis, Lawrence Livermore National Laboratory
International Advisory Committee
- Konstantinos Anagnostopoulos (National Technical University of Athens, Greece)
- Tom Appelquist (Yale University, USA)
- Norman Christ (Columbia University, USA)
- Philippe de Forcrand (ETHZ, Switzerland)
- Luigi Del Debbio (University of Edinburgh, UK)
- George Fleming (Yale University, USA)
- Margarita Garcìa Pérez IFT UAM-CSIC, Spain
- Rajiv Gavai (Tata Institute of Fundamental Research, India)
- Anna Hasenfratz (University of Colorado, Boulder, USA)
- Shoji Hashimoto (KEK, Japan)
- Wick Haxton (University of California, Berkeley and LBNL, USA)
- Karl Jansen (DESY, Germany)
- David Kaplan (University of Washington, USA)
- Frithjof Karsch (Brookhaven National Laboratory, USA)
- Tony Kennedy (University of Edinburgh, UK)
- Derek Leinweber (University of Adelaide, Australia)
- Paul Mackenzie (Fermilab, USA)
- John Negele (Massachusetts Institute of Technology, USA)
- Kostas Orginos (College of William and Mary, USA)
- Giancarlo Rossi (University and INFN of Rome Tor Vergata, Italy)
- Junko Shigemitsu (Ohio State University, USA)
- Frank Wilczek (Massachusetts Institute of Technology, USA)




