D spectroscopy 2+1+1 Setup Martin Kalinowski in collaboration - - PowerPoint PPT Presentation

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D spectroscopy 2+1+1 Setup Martin Kalinowski in collaboration - - PowerPoint PPT Presentation

D spectroscopy 2+1+1 Setup Martin Kalinowski in collaboration with Marc Wagner November 26 , 2012 pic/Goethe-Logo lattice D Martin Kalinowski Aims Long term project to compute spectra of mesons with strange and charm quark


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D∗∗ spectroscopy

2+1+1 Setup Martin Kalinowski

in collaboration with Marc Wagner

November 26 , 2012

Martin Kalinowski lattice D∗∗

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Aims

Long term project to compute spectra of mesons with strange and charm quark content using lattice QCD methods. Extrapolation to the physical pion mass and the continuum limit. Here: First steps focussing on tuning valence s and c quark masses and computing low-lying D mesons.

Martin Kalinowski lattice D∗∗

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Wilson twisted mass action

Sl = a4

x

¯ χl(x)

  • D[U] + m0,l + iµlγ5τ 3

χl(x) Sh = a4

x

¯ χh(x)

  • D[U] + m0,h + iµσγ5τ 1 + µδτ 3

χh(x) χl = χu χd

  • ,

χh = χs χc

  • τ 1 =

1 1

  • ,

τ 3 = 1 −1

  • ψphys

h

= e

i 2 ωhγ5τ1χh,

¯ ψphys

h

= e

i 2ωhγ5τ1 ¯

χh.

  • diff. masses

ψphys

l

= e

i 2ωlγ5τ3χl,

¯ ψphys

l

= e

i 2ωlγ5τ3 ¯

χl mass degenerated Tuned to ’maximal’ twist: m0,l = m0,h → mcrit ⇒ ωh = ωl → π

2

⇒ automatic O(a) improvement for physical observables.

Martin Kalinowski lattice D∗∗

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ETMC 2 + 1 + 1 ensembles

Available 2 + 1 + 1 configurations. Mismatch of strange and charm mass. Idea: different valence action for s and c quarks. χc := χc+ χc−

  • ,

DW + mcrit ± iµcγ5

Martin Kalinowski lattice D∗∗

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Switching the basis assuming maximal twist

Mass degenerated doublets ψup ψdn

  • ,

ψs1 ψs2

  • ,

ψc1 ψc2

  • Twisted basis

χup+ χdn−

  • ,

χs+ χs−

  • ,

χc+ χc−

  • ψ = exp(iγ5τ3ω/2)χ,

¯ ψ = ¯ χexp(iγ5τ3ω/2) ¯ ψΓψ = ¯ χ(1 + iγ5τ3)Γ(1 + iγ5τ3)χ ∝ ¯ χΓtwmχ Γphys Γtwm γi γi γiγj γ5γiγj γ5 1 1 γ5 ¯ ψuΓψu Γphys Γtwm γi γ5γi γiγj γiγj γ5 γ5 1 1 ¯ ψuΓψd Example: D - meson ¯ ψupγ5ψc1 → ¯ χupχc+, ¯ ψupγ5ψc2 → ¯ χupγ5χc− Two numbers for every mass.

Martin Kalinowski lattice D∗∗

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Introduction of strange and charm valence quarks

unitary setup valence quark setup

1.8 1.9 2 2.1 2.2 2.3 2.4 2.5 2.6 2.7 2.8 0.22 0.23 0.24 0.25 0.26 0.27 0.28 effective mass [GeV] valence mass charm linear extrapolations from lattice calculations D(exp.) D* (2010) D* 0(2400) D* 1(2420) A1- A1+ T1 T1

Introduction of mass degenerated doublets for charm and strange quarks(Valence sector). χc := χc+ χc−

  • ,

DW + mcrit ± iµcγ5 Calculation at different bare masses and extrapolation to the ’physical’ point (c: mD, s: 2m2

K − m2 PS)

Martin Kalinowski lattice D∗∗

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Example operators

Irrep Continuum JP Operators A1− 0−, 4−, ... ¯ qγ5q ¯ qγ5γiqDi A1+ 0+, 4+, ... ¯ qq ¯ qγiqDi T1− 1−, 3−, ... ¯ qγiq ¯ qqDi ¯ qǫijkγjqDk T1+ 1+, 3+, ... ¯ qγ5γiq ¯ qγ5qDi ¯ qγ5ǫijkγjqDk qDi means a derivative source in direction i. All operators qΓqD stay in the same irrep when Γ is multiplied by γ0.

Martin Kalinowski lattice D∗∗

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Setup

Gauge link configurations with 2 + 1 + 1 dynamical quark flavors (ETMC).

Tuning charm valence quark mass to reproduce physical mD mass. Tuning strange valence quark mass to reproduce physical value of 2m2

K − m2 π mass. Weak dependence on the pion

mass.

Mixed action setup to avoid mixing of strange and charm flavor and repair mismatch in the sea. Gaussian distributed spin diluted timeslice sources with APE smeared gauge links. Parameters of the ensemble: (L/a)3 × (T/a) = 323 × 64, β = 1.9, µ = 0.004, µδ = 0.19, µσ = 0.15, a = 0.0859(5)fm, mπ ≈ 325MeV

Martin Kalinowski lattice D∗∗

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Desults D Ds

1.8 1.9 2 2.1 2.2 2.3 2.4 2.5 2.6 2.7 D D* D* D*

1

mass [GeV]

D mesons

lattice pp lattice PDG

Results for a single ensemble at the pion mass mπ ≈ 325MeV. Rather good agreement with experiment, even without chiral and continuum extrapolation.

1.8 1.9 2 2.1 2.2 2.3 2.4 2.5 2.6 2.7 DS D*

S0

D*

S

D*

S1

mass [GeV]

Ds mesons

lattice pp lattice PDG

Discrepancies for D∗

s0 and

D∗

  • s1. Similar findings in other

lattice studies and phenomenological model calculations.

Martin Kalinowski lattice D∗∗

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quality of the T2(J = 2, 3, 4, ...) channel

0.5 1 1.5 2 2 4 6 8 10 12 ameffective T effective masses T2 am = 1.4141 ± 0.0324 (χ2/dof = 0.23) am = 1.2416 ± 0.0136 (χ2/dof = 0.57)

Thank you for your attention.

Martin Kalinowski lattice D∗∗