Excited State Spectroscopy from Lattice QCD

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Presentation transcript:

Excited State Spectroscopy from Lattice QCD Robert Edwards Jefferson Lab CERN 2010 Collaborators: J. Dudek, B. Joo, M. Peardon, D. Richards, C. Thomas, S. Wallace Auspices of the Hadron Spectrum Collaboration TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAAAAA

Spectroscopy Spectroscopy reveals fundamental aspects of hadronic physics Essential degrees of freedom? Gluonic excitations in mesons - exotic states of matter? New spectroscopy programs world-wide E.g., BES III (Beijing), GSI/Panda (Darmstadt) Crucial complement to 12 GeV program at JLab. Excited nucleon spectroscopy (JLab) JLab GlueX: search for gluonic excitations.

Nuclear Physics & Jefferson Lab JLab undergoing a major upgrade Future Hall D Lab doubling beam energy to 12GeV Adding new experimental Hall

Excited states: anisotropy+operators+variational Anisotropic lattices with Nf=2+1 dynamical (clover)fermions Temporal lattice spacing at < as (spatial lattice spacing) High temporal resolution ! Resolve noisy & excited states Major project within USQCD – Hadron Spectrum Collab. Extended operators Sufficient derivatives ! nonzero overlap at origin Variational method: Matrix of correlators ! project onto excited states PRD 78 (2008) & PRD 79 (2009) PRD 72 (2005), PRD 72 (2005), 0907.4516 (PRD), 0909.0200 PRD 76 (2007), PRD 77 (2008), 0909.0200 4

Nf=2+1 Anisotropic Clover Nf = 2 + 1 (u,d + s) Using at m & »=3.5 : as = 0.1227(3)fm, (at)-1 ~ 5.640 GeV 0803.3960 & 0810.3588 5

Spin and Operator Construction Gamma matrices and derivatives in circular basis: Couple to build any J,M via usual CG Only using symmetries of continuum QCD Construct all possible operators up to 3 derivatives (3 units orbital angular momentum) Subduce onto lattice irreps: “remembers” J 0905.2160 (PRD), 0909.0200 (PRL), 1004.4930 (PRD) 6

Distillation 7 Replace smearing with low rank approximation Matrix elements of vk(t) ! propagators, mesons, baryons, etc. Make correlators Gauge covariant, mom. conservation (source & sink) ! reduced “noise” Stochastic variants (lower cost) 0905.2160 (PRD), 1002.0818, Bulava (thesis 2010) 7

Spectrum from variational method Two-point correlator Matrix of correlators Diagonalize: eigenvalues ! spectrum eigenvectors ! wave function overlaps Benefit: orthogonality for near degenerate states 8

Determining spin on a cubic lattice? Spin reducible on lattice T2 E Might be dynamical degeneracies Spin 1, 2, 3, or 4 ? mass T1 T2 E A2

Spin reduction & (re)identification Variational solution: Continuum Lattice Method: Check if converse is true

Spin (re)identification Nf=3 Z values: spin 3 Well identified: suggests small rotational breaking

Isovector Meson Spectrum Nf=3 1004.4930

Isovector Meson Spectrum Nf=3 1G 3S 2D 1F ?? 2P 1D 2S 1P 1S 1004.4930

Isovector Meson Spectrum Nf=2+1, m¼ ~ 520MeV, L~2fm Similar to Nf=3 1004.4930

Exotic matter Exotics: world summary

Exotic matter Current work: (strong) decays Suggests (many) exotics within range of JLab Hall D Previous work: charmonium photo-production rates high Current work: (strong) decays

Vector isoscalars (I=0) light-strange (ls) basis Nf=2+1, m¼ ~ 400MeV, L~2fm I = 0 Must include all disconnected diagrams

Baryon Spectrum “Missing resonance problem” What are collective modes? What is the structure of the states? Major focus of (and motivation for) JLab Hall B Not resolved experimentally @ 6GeV Nucleon spectrum PDG uncertainty on B-W mass

Strange Quark Baryons Strange quark baryon spectrum poorly known Future: Narrow widths: easy(er) to extract (?) ¥ & : unknown spin & parities Widths are small 19

Light quark baryons in SU(6) Conventional non-relativistic construction: 6 quark states in SU(6) Baryons 20

Relativistic operator construction: SU(12) Relativistic construction: 3 Flavors with upper/lower components Times space (derivatives) Dirac Color contraction is Antisymmetric ! Totally antisymmetric operators More operators than SU(6): mixes orbital ang. momentum & Dirac spin 21

Orbital angular momentum via derivatives Couple derivatives onto single-site spinors: Enough D’s – build any J,M Only using symmetries of continuum QCD Use all possible operators up to 2 derivatives (2 units orbital angular momentum) 0905.2160 (PRD), 0909.0200 (PRL), 1004.4930 22

Nucleon & Delta Spectrum

Nucleon & Delta Spectrum Suggests spectrum at least as dense as quark model [20,1+] P-wave [70,2+] D-wave [56,2+] D-wave [56,2+] D-wave [70,1-] P-wave [70,1-] P-wave “Roper”? Change at lighter quark mass? Decays!

Hadronic decays Current spectrum calculations: no evidence of multi-particle levels Plot the non-interacting meson levels as a guide Require multi-particle operators (lattice) helicity construction annihilation diagrams Extract δ(E) at discrete E 25

Phase Shifts: demonstration ¼¼ isospin=2 Extract δ0(E) at discrete E No discernible pion mass dependence

Phase Shifts: demonstration ¼¼ isospin=2 δ2(E)

Hardware: JLab GPU Clusters GPU clusters: ~530 cards Quads 2.4 GHz Nehalem 48 GB memory / node 117 nodes x 4 GPUs -> 468 GPUs Singles 24 GB memory / node 64 nodes x 1 GPU -> 64 GPUs

Inverter Strong Scaling: V=323x256 3 Tflops Local volume on GPU too small (I/O bottleneck)

Prospects Strong effort in excited state spectroscopy New operator & correlator constructions ! high lying states Finite volume extraction of resonance parameters – promising Progress! Still much more to do Initial results for excited state spectrum: Suggests baryon spectrum at least as dense as quark model Suggests multiple exotic mesons within range of Jlab’s Hall D Resonance determination: Start at heavy masses: have some “elastic scattering” Use larger volumes & smaller pion masses (m¼ ~230MeV) Now: multi-particle operators & annihilation diagrams (gpu-s) Need multi-channel finite-volume analysis for (in)elastic scattering Future: Transition FF-s, photo-couplings (0803.3020, 0902.2214)