CVC test in e + e − →KK cross section and data on τ − →K − K 0 ν τ decay
Dispersive analysis for pion-kaon scattering€¦ · K B 0 s + K J= Crossed channel ˇˇ!KK :...
Transcript of Dispersive analysis for pion-kaon scattering€¦ · K B 0 s + K J= Crossed channel ˇˇ!KK :...
Dispersive analysis for pion-kaon scattering
J. Ruiz de Elvira
Institute for Theoretical Physics, University of Bern
TRR110 workshop: amplitudes for three-body final states, Garching, July 12th, 2018
Motivation: Why πK scattering?
Low energies: test chiral dynamics in the strange-quark sector
B Scattering lengths lowest energy observables
→ Spontaneous and explicit chiral symmetry breaking
Higher energies: resonances, hadron spectrum
→ κ(800) non-ordinary meson, PDG “needs confirmation”
Input for Heavy-meson decays: CP-violation and New Physics searches
D+
π+
π+
K−
B0s
π+
K−
J/Ψ
Crossed channel ππ → K K : first inelastic contribution to ππ scattering
→ Γ(f0(500)→ K K ) nature of the σ meson
→ Nucleon form factors, g − 2 . . .
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 2
Pion-kaon interaction
Simplest scattering process involving strangeness
Two independent amplitudes Is = 1/2, 3/2 or I± = +,−
T 1/2 = T + + 2T−, T 3/2 = T + − T−
Leading-order O(p2) = O(m2i ) predictions for πK
a− =mπmK
8π(mπ + mK )f 2π
+O(m4i ) a+ = O(m4
i )
Next-to-leading order: low-energy constants L1−8 [Bernard, Kaiser, Meißner 91]
B Loop contribution suppressed at threshold
a−LECs =2mK m3
π
π(mπ + mK )f 4π
L5 +O(m6i ) [Weinberg 1966]
a+LECs =
2m2K m2
π
π(mπ + mK )f 4π
(4(L1 + L2 − L4) + 2L3 − L5 + 2(2L6 + 2L8)) +O(m6i )
Next-to-next to leading order: C1−32, 10 for a− and 23 for a+
[Bijnens,Dhonte,Talavera 2004], [Bijnens, Ecker 2014]
KK
π π
KK
π π
1/f 2π
(a)
KK
π π
Li
(b)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 3
Pion-kaon interaction
Simplest scattering process involving strangeness
Two independent amplitudes Is = 1/2, 3/2 or I± = +,−
T 1/2 = T + + 2T−, T 3/2 = T + − T−
Leading-order O(p2) = O(m2i ) predictions for πK
a− =mπmK
8π(mπ + mK )f 2π
+O(m4i ) a+ = O(m4
i )
Next-to-leading order: low-energy constants L1−8 [Bernard, Kaiser, Meißner 91]
B Loop contribution suppressed at threshold
a−LECs =2mK m3
π
π(mπ + mK )f 4π
L5 +O(m6i ) [Weinberg 1966]
a+LECs =
2m2K m2
π
π(mπ + mK )f 4π
(4(L1 + L2 − L4) + 2L3 − L5 + 2(2L6 + 2L8)) +O(m6i )
Next-to-next to leading order: C1−32, 10 for a− and 23 for a+
[Bijnens,Dhonte,Talavera 2004], [Bijnens, Ecker 2014]
KK
π π
KK
π π
1/f 2π
(a)
KK
π π
Li
(b)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 3
Pion-kaon interaction
Simplest scattering process involving strangeness
Two independent amplitudes Is = 1/2, 3/2 or I± = +,−
T 1/2 = T + + 2T−, T 3/2 = T + − T−
Leading-order O(p2) = O(m2i ) predictions for πK
a− =mπmK
8π(mπ + mK )f 2π
+O(m4i ) a+ = O(m4
i )
Next-to-leading order: low-energy constants L1−8 [Bernard, Kaiser, Meißner 91]
B Loop contribution suppressed at threshold
a−LECs =2mK m3
π
π(mπ + mK )f 4π
L5 +O(m6i ) [Weinberg 1966]
a+LECs =
2m2K m2
π
π(mπ + mK )f 4π
(4(L1 + L2 − L4) + 2L3 − L5 + 2(2L6 + 2L8)) +O(m6i )
Next-to-next to leading order: C1−32, 10 for a− and 23 for a+
[Bijnens,Dhonte,Talavera 2004], [Bijnens, Ecker 2014]
KK
π π
KK
π π
1/f 2π
(a)
KK
π π
Li
(b)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 3
Pion-kaon interaction
Simplest scattering process involving strangeness
Two independent amplitudes Is = 1/2, 3/2 or I± = +,−
T 1/2 = T + + 2T−, T 3/2 = T + − T−
Leading-order O(p2) = O(m2i ) predictions for πK
a− =mπmK
8π(mπ + mK )f 2π
+O(m4i ) a+ = O(m4
i )
Next-to-leading order: low-energy constants L1−8 [Bernard, Kaiser, Meißner 91]
B Loop contribution suppressed at threshold
a−LECs =2mK m3
π
π(mπ + mK )f 4π
L5 +O(m6i ) [Weinberg 1966]
a+LECs =
2m2K m2
π
π(mπ + mK )f 4π
(4(L1 + L2 − L4) + 2L3 − L5 + 2(2L6 + 2L8)) +O(m6i )
Next-to-next to leading order: C1−32, 10 for a− and 23 for a+
[Bijnens,Dhonte,Talavera 2004], [Bijnens, Ecker 2014]
KK
π π
KK
π π
1/f 2π
(a)
KK
π π
Li
(b)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 3
Pion-kaon interaction
Simplest scattering process involving strangeness
Two independent amplitudes Is = 1/2, 3/2 or I± = +,−
T 1/2 = T + + 2T−, T 3/2 = T + − T−
Leading-order O(p2) = O(m2i ) predictions for πK
a− =mπmK
8π(mπ + mK )f 2π
+O(m4i ) a+ = O(m4
i )
Next-to-leading order: low-energy constants L1−8 [Bernard, Kaiser, Meißner 91]
B Loop contribution suppressed at threshold
a−LECs =2mK m3
π
π(mπ + mK )f 4π
L5 +O(m6i ) [Weinberg 1966]
a+LECs =
2m2K m2
π
π(mπ + mK )f 4π
(4(L1 + L2 − L4) + 2L3 − L5 + 2(2L6 + 2L8)) +O(m6i )
Next-to-next to leading order: C1−32, 10 for a− and 23 for a+
[Bijnens,Dhonte,Talavera 2004], [Bijnens, Ecker 2014]
KK
π π
KK
π π
1/f 2π
(a)
KK
π π
Li
(b)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 3
Pion-kaon interaction
Simplest scattering process involving strangeness
Two independent amplitudes Is = 1/2, 3/2 or I± = +,−
T 1/2 = T + + 2T−, T 3/2 = T + − T−
Leading-order O(p2) = O(m2i ) predictions for πK
a− =mπmK
8π(mπ + mK )f 2π
+O(m4i ) a+ = O(m4
i )
Next-to-leading order: low-energy constants L1−8 [Bernard, Kaiser, Meißner 91]
B Loop contribution suppressed at threshold
a−LECs =2mK m3
π
π(mπ + mK )f 4π
L5 +O(m6i ) [Weinberg 1966]
a+LECs =
2m2K m2
π
π(mπ + mK )f 4π
(4(L1 + L2 − L4) + 2L3 − L5 + 2(2L6 + 2L8)) +O(m6i )
Next-to-next to leading order: C1−32, 10 for a− and 23 for a+
[Bijnens,Dhonte,Talavera 2004], [Bijnens, Ecker 2014]
KK
π π
KK
π π
1/f 2π
(a)
KK
π π
Li
(b)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 3
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 4
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 4
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 4
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 4
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 4
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 4
Current status
Experimental values: DIRAC collaboration
B lifetime of πK atoms at CERN⇒ isovector scattering length
Γ1S ∝∣∣∣T(π+K−→π0K 0)
∣∣∣2 ∝ |a−|2[Deser, Goldberger, Baumann, Thirring 1954]
B Current result:
a− = (−0.072+0.031−0.020)m−1
π
[DIRAC 2017]
→ huge uncertainties
B Room for improvement: near future increase statistics by 10
3s 3p 3d
2s 2p
1s
Γ1s
ǫ1s
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 5
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 6
πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 6
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Lattice analysis: unquenched results only
B Constraint from semileptonic Kl3 decays [Flynn, Nieves 2007]
a1/2 = 0.179(17)(14)m−1π
B NPLQCD: dynamical Nf = 2 + 1 calculation, mπ = 290− 600 MeV [NPLQCD 2006]
a1/2 = (0.173+0.003−0.016)m−1
π , a3/2 = (−0.057+0.003−0.006)m−1
π
B Z. Fu: dynamical Nf = 2 + 1 fermions, mπ = 330− 466 MeV [Fu 2012]
a1/2 = 0.182(4)m−1π , a3/2 = −0.051(2)m−1
π
B PACs: dynamical Nf = 2 + 1 fermions, mπ = 170− 710 MeV [PACs-Cs 2014]
a1/2 = 0.142(14)(27)m−1π , a3/2 = −0.047(2)(2)m−1
π
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 7
Current status
Dispersive determination: Roy-Steiner equations analysis
B Most precise results up to date
a1/2 = 0.224(22)m−1π , a3/2 = −0.045(8)m−1
π
[Büttiker, Descontes-Genon, Moussallam 2003]
→ More than 3.5σ from O(p4) ChPT results
This talk: where does this discrepancy come from?
→ Overview of Roy-Steiner equation for πK scattering
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 8
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 8
Current status
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14Buettiker et al. 04
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 8
Current status
Dispersive determination: Roy-Steiner equations analysis
B Most precise results up to date
a1/2 = 0.224(22)m−1π , a3/2 = −0.045(8)m−1
π
[Büttiker, Descontes-Genon, Moussallam 2003]
→ More than 3.5σ from O(p4) ChPT results
This talk: where does this discrepancy come from?
→ Overview of Roy-Steiner equation for πK scattering
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 8
Current status
Dispersive determination: Roy-Steiner equations analysis
B Most precise results up to date
a1/2 = 0.224(22)m−1π , a3/2 = −0.045(8)m−1
π
[Büttiker, Descontes-Genon, Moussallam 2003]
→ More than 3.5σ from O(p4) ChPT results
This talk: where does this discrepancy come from?
→ Overview of Roy-Steiner equation for πK scattering
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 8
Current status
Dispersive determination: Roy-Steiner equations analysis
B Most precise results up to date
a1/2 = 0.224(22)m−1π , a3/2 = −0.045(8)m−1
π
[Büttiker, Descontes-Genon, Moussallam 2003]
→ More than 3.5σ from O(p4) ChPT results
This talk: where does this discrepancy come from?
→ Overview of Roy-Steiner equation for πK scattering
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 8
Why Roy-Steiner equations?
Roy(-Steiner) eqs. = Partial-Wave (Hyberbolic) Dispersion Relationscoupled by unitarity and crossing symmetry
Respect all symmetries: analyticity, unitarity, crossing
Model independent⇒ the actual parametrization of the data is irrelevant once it is used inthe integral.
Framework allows for systematic improvements (subtractions, higher partial waves, ...)
PW(H)DRs help to study processes with high precision:
ππ-scattering: [Ananthanarayan et al. (2001), García-Martín et al. (2011)]
πK -scattering: [Büttiker et al. (2004)]
γγ → ππ scattering: [Hoferichter et al. (2011)]
πN scattering: [Hoferichter et al. (2015)]
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 9
Roy equations for ππ scattering
ππ → ππ⇒ fully crossing symmetric in Mandelstam variables s, t , and u = 4Mπ − s − t
Start from twice-subtracted fixed-t DRs
T I(s, t) = c(t) +1π
∞∫4m2π
ds′
s′2
[s2
(s′ − s)−
u2
(s′ − u)
]ImT I(s′, t)
Subtraction functions c(t) are determined via crossing symmetry
→ functions of the I=0,2 scattering lengths: a00 and a2
0
PW-projection and expansion yields the Roy-equations [Roy (1971)]
t IJ (s) = ST I
J (s) +∞∑
J′=0
(2J′ + 1)∑
I′=0,1,2
∞∫4m2π
ds′K II′JJ′ (s′, s) Im t I′
J′ (s′)
K II′JJ′ (s′, s) ≡ kernels⇒ analytically known
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 10
Solving Roy-equations: flow information
Roy-equations rigorously valid for a finite energy range
⇒ introduce a matching point sm
only partial waves with J ≤ Jmax are solved
Assume isospin limit
InputHigh-energy region: Imt I
J (s) for s ≥ sm and for all J
Higher partial waves: Imt IJ (s) for J > Jmax and for all s
Inelasticities η(s)
OutputSelf-consistent solution for δIJ (s) for J ≤ Jmax and sth ≤ s ≤ sm
Subtraction constants
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 11
Roy-equations: existence and uniqueness
Solution characterized by subtraction constants and high-energy input (a, A)
Existence and uniqueness depends on δi dynamically at sm
m =∑
i
mi , mi =
⌊
2δi (sm)π
⌋if δi (sm) > 0,
−1 if δi (sm) < 0,
bxc ⇒ largest integer ≤ x .[Gasser, Wanders 1999, Wanders 2000]
m = 0, a unique solution exists for any (a, A)
m > 0, m-parameter family of solutions for any (a, A)
m < 0, only for a specific choice of the input constrained by |m| conditions
Physical solution characterized by smooth matching
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 12
Roy-equations: ππ results
Solution for the ππ S0-wave
400 600 800 1000 1200 1400
s1/2
(MeV)
0
50
100
150
200
250
300
CFDOld K decay data
Na48/2K->2 π decay
Kaminski et al.Grayer et al. Sol.B
Grayer et al. Sol. C
Grayer et al. Sol. D
Hyams et al. 73
δ0
(0)
1000 1100 1200 1300 1400
s1/2
(MeV)
0
0.5
1
η0
0(s)
Cohen et al.Etkin et al.Wetzel et al.Hyams et al. 75
Kaminski et al.Hyams et al. 73
Protopopescu et al.
CFD .
ππ KK
ππ ππ
Garcia-Martin, Kaminski, Pelaez, JRE (2011)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 13
Roy–Steiner equations for πK : differences to ππ Roy equations
Key differences compared to ππ Roy equations
Crossing: coupling between πK → πK (s-channel) and ππ → K K (t -channel)
⇒ need a different kind of dispersion relations [Hite, Steiner 1973, Büttiker et al. 2004]
Unitarity in t-channel, e.g. single-channel approximation
Imf J±(t) = σπt f J
±(t)t lJ (t)∗ tIJ f I
J
⇒Watson’s theorem: phase of f J±(t) equals δIJ [Watson 1954]
B solution in terms of Omnès function [Muskhelishvili 1953, Omnès 1958]
→ ππ scattering δIJ need as input
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 14
Roy–Steiner equations for πK : flow of information
Limited range of validity: hyperbolic dispersion relations
√s ≤√
sm = 0.985 GeV t ≤ tm = 2 GeV2
Input/Constraints
S- and P-waves above matching points > sm (t > tm)
Inelasticities
Higher waves (D-, F-, · · · )ππ phase shifts below the K Kthreshold
Output
S- and P-wave phase-shifts at lowenergies s < sm (t < tm)
Subtraction constants
Subthreshold parameters: c+00, c+
01, c−00
→ πK scattering lengths
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 15
Solving Roy-Steiner equations for πK : t-channel
General solution in terms of Omnes function [Muskhelishvili 1953, Omnes 1958]
Ω(t) = exp
(tπ
tm∫tπ
δ(t′)dt′
t′(t′−t)
), with Ω(t ∼ tm) ∼ |t ′ − tm|
δ(tm)π
δIJ (tm) > π⇒ one free parameter αIJ
gIJ (t) = ∆IJ (t) +tnΩIJ (t)
tm−t
(αIJ + t
π
tm∫tπ
dt′
t′ n+1∆IJ (t′)sin δIJ (t′)
t′−ttm−t|Ω(t′)| + t
π
∞∫tm
dt′
t′ n+1Im gIJ (t′)
t′−ttm−t|Ω(t′)|
)∆IJ (t) ≡ subtraction constants, s-channel pw, J>1 t-channel pw
gIJ (tm) is continuous but gIJ ′(tm) has a cusp (divergent)
→ αIJ analytically determined from a non-cusp condition
Ω(t ′)−1 obeys a dispersion relation⇒ Ω−1IJ (t) = Pn(t)− 1
π
tm∫tπ
dt′
t′ nsin δIJ (t′)
|ΩIJ (t′)|(t′−t)
→ ∆IJ (t)|ST polynomial in t ⇒ gIJ (tm)|ST can be computed analytically
→ ∆IJ (t)|s−channel expanded as polynomial using splines
Exact solution of the MO problem while solving the s-channel RS equations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 16
Solving Roy-Steiner equations for πK : t-channel
General solution in terms of Omnes function [Muskhelishvili 1953, Omnes 1958]
Ω(t) = exp
(tπ
tm∫tπ
δ(t′)dt′
t′(t′−t)
), with Ω(t ∼ tm) ∼ |t ′ − tm|
δ(tm)π
δIJ (tm) > π⇒ one free parameter αIJ
gIJ (t) = ∆IJ (t) +tnΩIJ (t)
tm−t
(αIJ + t
π
tm∫tπ
dt′
t′ n+1∆IJ (t′)sin δIJ (t′)
t′−ttm−t|Ω(t′)| + t
π
∞∫tm
dt′
t′ n+1Im gIJ (t′)
t′−ttm−t|Ω(t′)|
)∆IJ (t) ≡ subtraction constants, s-channel pw, J>1 t-channel pw
gIJ (tm) is continuous but gIJ ′(tm) has a cusp (divergent)
→ αIJ analytically determined from a non-cusp condition
Ω(t ′)−1 obeys a dispersion relation⇒ Ω−1IJ (t) = Pn(t)− 1
π
tm∫tπ
dt′
t′ nsin δIJ (t′)
|ΩIJ (t′)|(t′−t)
→ ∆IJ (t)|ST polynomial in t ⇒ gIJ (tm)|ST can be computed analytically
→ ∆IJ (t)|s−channel expanded as polynomial using splines
Exact solution of the MO problem while solving the s-channel RS equations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 16
Solving Roy-Steiner equations for πK : t-channel
General solution in terms of Omnes function [Muskhelishvili 1953, Omnes 1958]
Ω(t) = exp
(tπ
tm∫tπ
δ(t′)dt′
t′(t′−t)
), with Ω(t ∼ tm) ∼ |t ′ − tm|
δ(tm)π
δIJ (tm) > π⇒ one free parameter αIJ
gIJ (t) = ∆IJ (t) +tnΩIJ (t)
tm−t
(αIJ + t
π
tm∫tπ
dt′
t′ n+1∆IJ (t′)sin δIJ (t′)
t′−ttm−t|Ω(t′)| + t
π
∞∫tm
dt′
t′ n+1Im gIJ (t′)
t′−ttm−t|Ω(t′)|
)∆IJ (t) ≡ subtraction constants, s-channel pw, J>1 t-channel pw
gIJ (tm) is continuous but gIJ ′(tm) has a cusp (divergent)
→ αIJ analytically determined from a non-cusp condition
Ω(t ′)−1 obeys a dispersion relation⇒ Ω−1IJ (t) = Pn(t)− 1
π
tm∫tπ
dt′
t′ nsin δIJ (t′)
|ΩIJ (t′)|(t′−t)
→ ∆IJ (t)|ST polynomial in t ⇒ gIJ (tm)|ST can be computed analytically
→ ∆IJ (t)|s−channel expanded as polynomial using splines
Exact solution of the MO problem while solving the s-channel RS equations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 16
Solving Roy-Steiner equations for πK : t-channel
General solution in terms of Omnes function [Muskhelishvili 1953, Omnes 1958]
Ω(t) = exp
(tπ
tm∫tπ
δ(t′)dt′
t′(t′−t)
), with Ω(t ∼ tm) ∼ |t ′ − tm|
δ(tm)π
δIJ (tm) > π⇒ one free parameter αIJ
gIJ (t) = ∆IJ (t) +tnΩIJ (t)
tm−t
(αIJ + t
π
tm∫tπ
dt′
t′ n+1∆IJ (t′)sin δIJ (t′)
t′−ttm−t|Ω(t′)| + t
π
∞∫tm
dt′
t′ n+1Im gIJ (t′)
t′−ttm−t|Ω(t′)|
)∆IJ (t) ≡ subtraction constants, s-channel pw, J>1 t-channel pw
gIJ (tm) is continuous but gIJ ′(tm) has a cusp (divergent)
→ αIJ analytically determined from a non-cusp condition
Ω(t ′)−1 obeys a dispersion relation⇒ Ω−1IJ (t) = Pn(t)− 1
π
tm∫tπ
dt′
t′ nsin δIJ (t′)
|ΩIJ (t′)|(t′−t)
→ ∆IJ (t)|ST polynomial in t ⇒ gIJ (tm)|ST can be computed analytically
→ ∆IJ (t)|s−channel expanded as polynomial using splines
Exact solution of the MO problem while solving the s-channel RS equations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 16
Solving Roy-Steiner equations for πK : t-channel
General solution in terms of Omnes function [Muskhelishvili 1953, Omnes 1958]
Ω(t) = exp
(tπ
tm∫tπ
δ(t′)dt′
t′(t′−t)
), with Ω(t ∼ tm) ∼ |t ′ − tm|
δ(tm)π
δIJ (tm) > π⇒ one free parameter αIJ
gIJ (t) = ∆IJ (t) +tnΩIJ (t)
tm−t
(αIJ + t
π
tm∫tπ
dt′
t′ n+1∆IJ (t′)sin δIJ (t′)
t′−ttm−t|Ω(t′)| + t
π
∞∫tm
dt′
t′ n+1Im gIJ (t′)
t′−ttm−t|Ω(t′)|
)∆IJ (t) ≡ subtraction constants, s-channel pw, J>1 t-channel pw
gIJ (tm) is continuous but gIJ ′(tm) has a cusp (divergent)
→ αIJ analytically determined from a non-cusp condition
Ω(t ′)−1 obeys a dispersion relation⇒ Ω−1IJ (t) = Pn(t)− 1
π
tm∫tπ
dt′
t′ nsin δIJ (t′)
|ΩIJ (t′)|(t′−t)
→ ∆IJ (t)|ST polynomial in t ⇒ gIJ (tm)|ST can be computed analytically
→ ∆IJ (t)|s−channel expanded as polynomial using splines
Exact solution of the MO problem while solving the s-channel RS equations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 16
Solving Roy-Steiner equations for πK : t-channel
General solution in terms of Omnes function [Muskhelishvili 1953, Omnes 1958]
Ω(t) = exp
(tπ
tm∫tπ
δ(t′)dt′
t′(t′−t)
), with Ω(t ∼ tm) ∼ |t ′ − tm|
δ(tm)π
δIJ (tm) > π⇒ one free parameter αIJ
gIJ (t) = ∆IJ (t) +tnΩIJ (t)
tm−t
(αIJ + t
π
tm∫tπ
dt′
t′ n+1∆IJ (t′)sin δIJ (t′)
t′−ttm−t|Ω(t′)| + t
π
∞∫tm
dt′
t′ n+1Im gIJ (t′)
t′−ttm−t|Ω(t′)|
)∆IJ (t) ≡ subtraction constants, s-channel pw, J>1 t-channel pw
gIJ (tm) is continuous but gIJ ′(tm) has a cusp (divergent)
→ αIJ analytically determined from a non-cusp condition
Ω(t ′)−1 obeys a dispersion relation⇒ Ω−1IJ (t) = Pn(t)− 1
π
tm∫tπ
dt′
t′ nsin δIJ (t′)
|ΩIJ (t′)|(t′−t)
→ ∆IJ (t)|ST polynomial in t ⇒ gIJ (tm)|ST can be computed analytically
→ ∆IJ (t)|s−channel expanded as polynomial using splines
Exact solution of the MO problem while solving the s-channel RS equations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 16
Solving s-channel: strategy
Parameterize S and P waves up to s < sm
B Imposing a continuous and differentiable matching point
Introduce as many subtractions as necessary to match d.o.f [Gasser, Wanders 1999]
B m = 0, three non-cusp conditions: S1/2, S3/2 and P1/2
→ three free parameters: c+00, c+
01, c−00
Minimize difference between LHS and the RHS on a grid of points Wj
χ2phys =
∑l,Is
N∑j=1
(Re f Is
l±(Wj )− F [cIsnm, f
Isl±](Wj )
)2
Re f Isl±(Wj )2
B F [cIsnm, f
Isl±](Wj ) ≡ right hand side of RS-equations
Parametrization and subthreshold parameters are the fitting parameters
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 17
Roy-Steiner solution: preliminary results
0.5 0.6 0.7 0.8 0.9s GeV2
−0.4−0.20.00.20.40.60.81.0 f
1/20
flfr
0.5 0.6 0.7 0.8 0.9s GeV2
−1.0
−0.5
0.0
0.5
1.0 f1/21
0.5 0.6 0.7 0.8 0.9s GeV2
−0.5−0.4−0.3−0.2−0.10.00.1 f
3/20
0.5 0.6 0.7 0.8 0.9s GeV2
−0.10−0.08−0.06−0.04−0.020.000.02 f
3/21
f tot
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 18
Preliminary results: s-channel phase shifts
0.65 0.70 0.75 0.80 0.85 0.90 0.95√s GeV2
0
10
20
30
40
50
60
70
80 δ1/20 (s)
LRSLACLASS
0.65 0.70 0.75 0.80 0.85 0.90 0.95√s GeV2
0
50
100
150
200 δ1/21 (s)
LRSLACLASS
0.65 0.70 0.75 0.80 0.85 0.90 0.95√s GeV2
−35
−30
−25
−20
−15
−10
−5
0 δ3/20 (s)
LRSLAC
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 19
Preliminary results: t-channel solution
0.0 0.5 1.0 1.5 2.0t GeV2
0.0
0.5
1.0
1.5
2.0
2.5
3.0
| g0 0( t
) |
LongacreCohen
0.0 0.5 1.0 1.5 2.0t GeV2
0
1
2
3
4
5
6
7
| g1 1( t
) |
Cohen
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 20
Preliminary results: kappa pole
600 650 700 750 800 850 900 950M (MeV)
-400
-350
-300
-250
-200
-150
-100 −
Γ/2
(M
eV)
Breit-Wigner-like parameterizations
Zhou et al.PelaezBugg
Bonvicini et al.Descotes-Genon et al.Padé result, Pelaez, Rodas, JREPelaez and RodasColangelo, Maurizio, JRE (preliminary)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 21
πK Scattering length puzzle: BDM solution
Fixed-t dispersion relation
B cI(t) extracted from a hyperbolic dispersion relation at threshold
s · u = m2K −m2
π
Twice/once subtracted version for I = +,−
c+(t) = 8π(mπ + mK )a+ + b+t
c−(t) = 8π(mπ+mK )mπmK
a−pπ(t)qK (t)
b+ extracted from a sum rule involving a−
a+ and a− extracted from RS self-consistent solution
χ2phys =
∑l,Is
N∑j=1
(Re f Is
l (sj )− F [f Isl ](sj )
)2
Re f Isl (sj )2
B F [f Isl ](sj ) ≡ right hand side of RS-equations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 22
Roy-Steiner solution for πK
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
0.6
0.8
0.4 0.5 0.6 0.7 0.8 0.9 1
Re fIs
l(s)
s (GeV2)
f01/2
f11/2
f03/2
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 23
Dispersive determination of πK scattering lengths
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14Buettiker et al. 04
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 24
Stability of the solution
How stable is the solution?
→ ππ scattering case⇒ universal band in the a00, a2
0 plane [Ananthanarayan et al. (2001)]
0.15 0.2 0.25 0.3
a0
0
−0.06
−0.05
−0.04
−0.03
−0.02
a02
S0
S1
S2
S3
B similar for πN scattering [Hoferichter et al. (2015)]
→ look for πK RS solutions in a grid
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 25
Universal band on the scattering length plane
0.16 0.18 0.20 0.22 0.24 0.26 0.28
- 0.08
- 0.07
- 0.06
- 0.05
- 0.04
- 0.03
a01/ 2 M π
a03/2M
π
0
20
40
60
80
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 26
Subthreshold parameter plane
0.5 1.0 1.5 2.0 2.5 3.0
8.0
8.2
8.4
8.6
8.8
9.0
9.2
9.4
C +00
C-00
0
5
10
15
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 27
πK scattering lengths: preliminary results
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14Buettiker et al. 04
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 28
πK scattering lengths: preliminary results
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14Buettiker et al. 04Universal Band
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 28
Looking for a unique solution
Unique solution: as many subtractions as necessary to match d.o.f [Gasser, Wanders 1999]
→ two non-cusp conditions⇒ two free scattering lengths [Büttiker, Descontes-Genon, Moussallam 2003]
Are the two scattering lengths independent?
8π(mπ + mK )a−SR
mπmK=
1π
∫ ∞sth
ds′
λ(s′)Im F−(s′, t ′) +
1π
∫ ∞tπ
dt ′
t ′Im
G1(t ′, s′)8pπ(t ′)pK (t ′)
Ks Kt Ds Dt As At Total
a−i,SR (mπ102) 0.86 6.10 0.60 0.13 0.00 0.37 8.05a− (mπ102) – – – – – – 8.96
→ once a+ is fixed, a− is obtained from a convergent sum rule
New approach: HDR subtracted at subthreshold
B three non-cusp conditions⇒ three subthreshold parameters constrained by SR
χ2tot = χ2
phys +
(c−00 − c−00,SR
)2
∆c−002
+
(c10
+ − c+10,SR
)2
∆c+10
2
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 29
Unique solution for πK scattering
- 2 - 1 0 1 2
7.0
7.5
8.0
8.5
C +00
C-00
5
10
15
20
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 30
πK scattering without χ2c−00
- 2 - 1 0 1
7.0
7.5
8.0
8.5
9.0
C +00
C-00
0
10
20
30
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 31
πK scattering lengths: preliminary results
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14Buettiker et al. 04Universal Band
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 32
πK scattering lengths: preliminary results
0.14 0.16 0.18 0.20 0.22 0.24 0.26 0.28 0.30a
120Mπ
−0.080
−0.075
−0.070
−0.065
−0.060
−0.055
−0.050
−0.045
−0.040
a3 2 0Mπ
CA
FLAG 16BE14 p4 14BE14 p6 Ci =0
BE14 p6RχPT p6Dirac 17Flynn et al. 07NPLQCD 06Fu 12PACS 14Buettiker et al. 04Universal Band
HDR
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 32
Thank you
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 33
Spare slides
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 34
πK subthreshold parameter plane
−3 −2 −1 0 1 2 3C +00
7.0
7.5
8.0
8.5
9.0
9.5
10.0C
− 00
C-RdE-M
FLAG
Bijnens 13
GL∗
Ci=0
BE14
BE14
FIT 10
Lang
B-M-DG
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 35
Dispersion relations in a nutshell
Effective field theories⇒ systematically improvable but
B number of LECs increase rapidly
B convergence problems: low-lying resonances, strong rescattering effects
Dispersion relations: analyticity, crossing, unitarity
B analitycity constrains the energy depedence of scattering amplitude
B crossing symmetry connects different physical regions
B unitarity constrains imaginary part
Roy(-Steiner) eqs. =Partial-Wave (Hyberbolic) Dispersion Relationscoupled by unitarity and crossing symmetry
→ model independent aproach
→ analytic continuation for the complex plane⇒ resonances, unphysical regions
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 36
From Cauchy’s theorem to dispersion relations
Cauchy’s Theorem
f (s) =1
2πi
∫∂Ω
ds′f (s′)s′ − s
→ analyticity
Subtractions
f (s) = f (0) +sπ
∫cuts
ds′Im f (s′)s′(s′ − s)
Imaginary part from Cutkosky rules→ forward direction: optical theorem
Unitarity for partial waves
Im f (s) = σ(s)|f (s)|2, f (s) =η(s)e2iδIJ (s) − 1
2iσ(s), σ(s) =
√1−
4m2π
s
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 37
From Cauchy’s theorem to dispersion relations
Cauchy’s Theorem
f (s) =1
2πi
∫∂Ω
ds′f (s′)s′ − s
→ analyticity
Subtractions
f (s) = f (0) +sπ
∫cuts
ds′Im f (s′)s′(s′ − s)
Imaginary part from Cutkosky rules→ forward direction: optical theorem
Unitarity for partial waves
Im f (s) = σ(s)|f (s)|2, f (s) =η(s)e2iδIJ (s) − 1
2iσ(s), σ(s) =
√1−
4m2π
s
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 37
From Cauchy’s theorem to dispersion relations
Dispersion relation
f (s) =1π
∫cuts
ds′Im f (s′)s′ − s
→ analyticity
Subtractions
f (s) = f (0) +sπ
∫cuts
ds′Im f (s′)s′(s′ − s)
Imaginary part from Cutkosky rules→ forward direction: optical theorem
Unitarity for partial waves
Im f (s) = σ(s)|f (s)|2, f (s) =η(s)e2iδIJ (s) − 1
2iσ(s), σ(s) =
√1−
4m2π
s
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 37
From Cauchy’s theorem to dispersion relations
Dispersion relation
f (s) =1π
∫cuts
ds′Im f (s′)s′ − s
→ analyticity
Subtractions
f (s) = f (0) +sπ
∫cuts
ds′Im f (s′)s′(s′ − s)
Imaginary part from Cutkosky rules→ forward direction: optical theorem
Unitarity for partial waves
Im f (s) = σ(s)|f (s)|2, f (s) =η(s)e2iδIJ (s) − 1
2iσ(s), σ(s) =
√1−
4m2π
s
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 37
From Cauchy’s theorem to dispersion relations
Dispersion relation
f (s) =1π
∫cuts
ds′Im f (s′)s′ − s
→ analyticity
Subtractions
f (s) = f (0) +sπ
∫cuts
ds′Im f (s′)s′(s′ − s)
Imaginary part from Cutkosky rules→ forward direction: optical theorem
Unitarity for partial waves
Im f (s) = σ(s)|f (s)|2, f (s) =η(s)e2iδIJ (s) − 1
2iσ(s), σ(s) =
√1−
4m2π
s
t(s) t(s)
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 37
Roy equations: range of convergence
Convergence for T I(s, t) guaranteed for t < 4m2
Where does the partial wave expansion converge?
Assumption: Mandelstam analyticity [Mandelstam (1958,1959)]
T (s, t) =1π2
∫∫ds′dt ′
ρst (s′, t ′)(s′ − s)(t ′ − t)
+ (t ↔ u) + (s ↔ u)
→ integration on the support of the double spectral densities ρ
Boundaries of ρ
(I) (II)
Lehmann ellipses
→ largest ellipses, which do not enter any ρ
-40 -20 0 20 40
-40
-20
0
20
40
s [M2π ]
u[M
2 π]
ρtuρsu
ρst
[Lehmann (1958)]
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 38
Outline
Why is pion-kaon scattering important?
B Relevance of pion-kaon scattering lengths
Chiral perturbation in SU(3)
B Convergence of the chiral series
Dispersive techniques in meson-meson scattering
B Roy-Steiner equation for pion-kaon scattering
On a dispersive determination of πK scatteringin collaboration with Gilberto Colangelo and Stefano Maurizio
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 39
Roy equations and resonance pole parameters
tIJ (s) known in the Lehmann ellipsis
Resonances
→ poles on unphysical Riemann sheets
SII(s − iε, t) = SI(s + iε, t)
→ t IIIJ (s) = tIJ (s) · (1 + 2i Σ(s)tIJ (s))−1
Elastic scattering: II RS is known exactly
Coupled channels
tIJ (s) =
t(11)IJ (s) t(12)
IJ (s)
t(12)IJ (s) t(22)
IJ (s)
Σ(s) =
(σ1(s) 0
0 σ2(s)
)
→ III and IV RS require crossed channels
t IVIJ (s) = t(11)
IJ (s)−2iσ2(s)t(12)
IJ (s)2
1 + 2iσ2(s)t(22)IJ (s)
0 20 40 60
Res
-40
-20
0
20
40
Ims
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 40
Dip vs no-dip solutions
The dip vs no-dip⇒ long-standing controversy [Pennington, Bugg, Zou, Achasov] · · ·
→ no clear preference for any of the two scenarios in previous works
Is it possible to satisfy Roy Equations with a non-dip scenario?
1000 1100 1200 1300 1400
s1/2(MeV)
0
0.25
0.5
0.75
1
η00(s)
Cohen et al.Etkin et al.Wetzel et al.ndUFDCFD 2010ndCFD enlarged errors
→ the non-dip scenario is rejected by DR
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 41
f0(500) pole 2010
400 500 600 700 800 900 1000 1100 1200
Re sσ1/2
(MeV)
-500
-400
-300
-200
-100
0
Im s
σ1/2 (
MeV
)
PDT estimate (2006)PDT citations (2006)Dobado, Pelaez 1996Colangelo, Gasser, Leutwyler 2001Pelaez 2004Caprini, Colangelo, Leutwyler 2006Garcia-Martin, Pelaez, Yndurain 2007Zhou 2004CFD + disersive relations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 42
f0(500) pole 2012
400 500 600 700 800 900 1000 1100 1200
Re sσ1/2
(MeV)
-500
-400
-300
-200
-100
0
Im s
σ1/2 (
MeV
)
PDT estimate (2012)PDT citations (2006)Dobado, Pelaez 1996Colangelo, Gasser, Leutwyler 2001Pelaez 2004Caprini, Colangelo, Leutwyler 2006Garcia-Martin, Pelaez, Yndurain 2007Zhou 2004CFD + disersive relations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 43
f0(980) pole 2010
960 980 1000 1020 1040 1060 1080 1100
Re sσ1/2
(MeV)
-100
-50
0
Ims σ1/
2 (M
eV)
PGD citations (2006)PGD estimate (2006)Caprini et alCFD + dispersion relations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 44
f0(980) pole 2012
960 980 1000 1020 1040 1060 1080 1100
Re sσ1/2
(MeV)
-100
-50
0
Ims σ1/
2 (M
eV)
PGD citations (2006)PGD estimate (2012)Caprini et alCFD + dispersion relations
J. Ruiz de Elvira (ITP) Pion-kaon scattering TRR110 workshop 45