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The Fubini-Furlan-Rossetti sum rule. LET.

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Presentation on theme: "The Fubini-Furlan-Rossetti sum rule. LET."— Presentation transcript:

1 The Fubini-Furlan-Rossetti sum rule

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8 LET

9 Pion Photoproduction    (k) i 4 Lorentz invariant functions of = (s-u)/4M N and t  + N !  + N Lorentz invariance, and P, C and T symmetries:

10 PCAC hypothesis current algebra Pion Low Energy Theorems soft pion limit LET for pion photoproduction Born with pseudovector coupling the contribution from is zero

11 Dispersion Relations at fixed t LET soft pion limit ( = 0, t =0 )

12 POLE BORN-PV obtained from tree-level Feynman diagrams:

13 FFR Sum Rule Fubini, Furlan, Rossetti, Nuovo Cimento 43 (1966) 161 Dispersion Relation with Im A 1 from MAID2003 HBChPT Corrections from physical pion mass as function of at fixed FFR discrepancy Heavy Baryon Chiral Perturbation Theory

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16 pion threshold soft pion point physical region of pion photoproduction

17 extrapolation to the unphysical region

18 FFR Discrepancy  from HBChPT (heavy baryon chiral perturbation theory ) Dispersion integral at fixed t=t thr with Im A 1 from MAID03

19 EXP t =0) (t=t thr ) MAID03 ( t =0) (t=t thr ) HBChPT MAID03 Proton 1.793 1.792 1.662.29/2.33/2.37 2.24 Neutron 1.913 1.986 1.822.52/2.56/2.79 2.44 HBChPT: Bernard, Kaiser, Meissner, Z. Phys. C70 (1996) Bernard, Kaiser, Meissner, Phys. Lett. B378 (1996) Bernard, Kaiser, Meissner, Eur. Phys. J. A11 (2001) S wave at O (p 4 ) P waves at O(p 3 ) S and P waves at O (p 4 ) FFR +  ( thr, t thr ) FFR ( = 0,t=0 )  p, -n-n  (0, t thr )

20 neutron proton FFR discrepancy  from MAID03 Pasquini, Drechsel, Tiator, Eur. Phys. J A23 (2005) t = t thr

21 Integrands from MAID03 third resonance region D 13 (1520)  1232)  loops t = t thr  S +  S   S +  S =   V +  V =   V +  V = 

22 PROTON Bernard, et al., PLB378 (1996) HBChPT at O(p 3 ) Bernard, et al., ZPC70 (1996) HBChPT at O(p 3 ) DR-MAID Bernard, et al. EPJ A11 (2001) HBChPT at O(p 4 ) Mainz experiment, Schmidt, et al., PRL 87 (2001) t = t thr

23 NEUTRON Bernard, et al., ZPC70 (1996) HBChPT at O(p 3 ) DR-MAID Bernard, et al. EPJ A11 (2001) HBChPT at O(p 4 ) Bernard, et al., PLB378 (1996) HBChPT at O(p 3 ) t = t thr

24 Summary  FFR sum rule: relation between the anomalous magnetic moment and single pion-photoproduction on the nucleon in the soft pion limit (m  2 =0, =t=0)  Predictions at =, t=0 : extrapolation of MAID amplitudes in the unphysical region give very good results  p = 1.792 (exp: 1.793)  n = - 1.986 (exp: -1.913)  Corrections to the sum rule from the physical pion mass:  (, t thr ) good agreement between MAID and HBChPT in the threshold region ( = thr ) problems at low  thr because of the non-relativistic approximation of HBChPT


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