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Pion Physics at Finite Volume

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At low energy the infinite volume Compton scattering amplitude ... Talk by A. Alexandru, C. Aubin, B. Tiburzi, S. Moerschbacher. A lot of systematic errors ... – PowerPoint PPT presentation

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Title: Pion Physics at Finite Volume


1
Pion Physics at Finite Volume
  • Jie Hu, Fu-Jiun Jiang, Brian Tiburzi
  • Duke University
  • Lattice 2008, William Mary, VA
  • July 16, 2008

2
QCD
Lattice QCD
Systematic Errors Quenching Large
pion mass Volume effects
Chiral Perturbation Theory
3
Compton Scattering Electromagnetic
Polarizabilities
  • At low energy the infinite volume Compton
    scattering amplitude for a real photon to scatter
    off a pion can be parametrized as

4
Predictions from ChiPT
  • One loop result
  • Two loop result

B. R. Holstein, Comments Nucl. Part. Phys. 19,
239 (1990)
Gasser, Ivanov and Sainio, Nulc. Phys. B745, 84
(2006)
?
Experimental
J.Ahrens et al. Eur. Phys. J. A23 (2005)
Dispersion relation calculation
L.V. Filkov and V. L. Kashevarov, Phys. Rev. C
73, 035210 (2006)
5
Can This be Calculated on Lattice?
Lattice four point function? Not now.
Background field method measure energy shift in
classical background electromagnetic fields.
Talk by A. Alexandru, C. Aubin, B. Tiburzi, S.
Moerschbacher A lot of systematic errors
Quenching Large pion mass Volume
effects ...
F.X. Lee, L. M. Zhou, W. Wilcox, and J.
Christensen, Phys. Rev. D 73, 034503 (2006)
6
Chiral Lagrangian
J. F. Domoghue, E. Golowich, and B.R. Holstein
7
Finite Volume ChPT
  • We choose time direction to be continuous and
    finite spatial volume with periodic boundary
    condition.
  • The momentum modes are .
  • Power counting
  • Same Chiral lagrangian and same diagrams with
  • Observable X at finite volume

8
Pion Current Renormalizations at Finite Volume
(?0)
J. H., F.-J. Jiang and B. C. Tiburzi, Phys. Lett.
B653, 350 (2007)
At infinite volume
At finite volume
9
Ward-Takahashi Identity at Finite Volume
J. H., F.-J. Jiang and B. C. Tiburzi, Phys. Lett.
B653, 350 (2007)
Ward-Takahashi identity is valid at finite
volume.
Ward identity is not achieved at finite volume
since pion momentum is not differentiable at
finite volume.
10
Charged Pion Current at Finite Volume
J. H., F.-J. Jiang and B. C. Tiburzi, Phys. Lett.
B653, 350 (2007)
11
Compton Scattering at Zero Photon Energy
At infinite volume T(?0) 0 for p0
At finite volume ?T(L)
12
Ward-Takahashi Identity at Finite Volume
J. H., F.-J. Jiang and B. C. Tiburzi, Phys. Lett.
B653, 350 (2007)
Ward-Takahashi identity is valid at finite
volume.
Ward identity is not achieved at finite volume
since pion momentum is not differentiable at
finite volume.
13
Neutral Pion Compton Scattering at Zero Photon
Energy at Finite Volume
J. H., F.-J. Jiang and B. C. Tiburzi, Phys. Lett.
B653, 350 (2007)
14
Effective Lagrangian at Finite Volume
J. H., F.-J. Jiang and B. C. Tiburzi, Phys. Lett.
B653, 350 (2007)
  • Under gauge symmetry, write down the general
    form of the ultra low energy effective theory for
    a simple f field coupled to zero frequency
    photons.
  • The new couplings are determined from finite
    volume calculations and are exponentially small
    in asymptotically large volume.

15
Compton Scattering at Finite Volume
  • The amplitude for a real photon to scatter off
    a pion in infinite volume

The amplitude for a real photon to scatter off
a pion in finite volume? Volume corrections to
pion polarizabilities?
16
Volume Corrections to Pion Polarizabilities?
  • All terms are form factors in . Because of
    momentum quantization , these form
    factors cannot be expanded in for the
    smallest modes.
  • Thus we cannot use the finite volume Compton
    tensor to deduce finite volume corrections to
    polarizabilities.

17
Summary
  • Recent discrepancies between ChPT measurements
    of pion polarizabilities motivate lattice
    calculations.
  • Use ChPT to get finite volume effects.
  • Demonstrate that the conserved current are
    additively renormalized at finite volume.
  • Ward-Takahashi identity is valid for all volume.
  • Single particle effective theory is derived.
  • Finite volume corrections to the Compton
    scattering tensor of pions are determined.
  • Finite volume effects to polarizabilities are not
    achieved.

18
Thank You.
19
Compton Tensor at Low Energy
  • Typical diagrams to one-loop order

20
The Most Recent Experimental Measurements
  • MAMI at Mainz results
  • More new results?
  • COMPASS at CERN increased statistics for
  • Jefferson lab has plans to measure pion
    polarizabilities

J.Ahrens et al. Eur. Phys. J. A23 (2005)
21
Other Experimental Data for Pion Polarizabilities
J.Ahrens et al. Eur. Phys. J. A23 (2005)
22
Pion Polarizabilities to One-loop
For both neutral and charged pions
B. R. Holstein, Comments Nucl. Part. Phys. 19,
221 (1990)
23
Volume Corrections to Pion Polarizabilities?
  • All terms are form factors in . Because of
    momentum quantization, these form factors cannot
    be expanded in for the smallest modes.
  • Thus we cannot use the finite volume Compton
    tensor to deduce finite volume corrections to
    polarizabilities.

24
Finite Volume Corrections to Neutral Pion Compton
Amplitude
25
Finite Volume Corrections to Charged Pion Compton
Amplitude
26
Gasser, Ivanov and Sainio, Nulc. Phys. B745, 84
(2006)
27
Finite Volume ChPT
  • Cubic box of with periodic boundary
    condition.

Matching terms
28
PQChPT Lagrangian
29
Gauge Invariance on a Torus
30
Effective Lagrangian at Finite Volume
31
Finite corrections to pion polarizabilities?
  • Matching terms

32
Polarizabilities
  • Atomic polarizabilities are well described
    theoretically
  • Pion polarizabilities involve non-perturbative
    effects
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