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A Format for Instantons and Their Characterizations
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hep-th/0507171
A Format for Instantons and Their Characterizations
Gordon Chalmers
e-mail: gordon@
Abstract
A characterization of instanton contributions to gauge field theory is given. The
dynamics of instantons with the gluon field is given in terms of ’classical’ instanton
contributions, i.e. on the same footing as tree amplitudes in field theory. This para-
materization depends on the kinematics of the local instanton operators and their
coupling dependence. A primary advantage of this ’classical’ formulation is that the
weak-strong duality and its relations with the perturbative sector are possibly made
more manifest.
1 Introduction
The classical dynamics of gauge theory has been investigated for many years. Obsta-
cles associated with the computation of these tree amplitudes have been circumvented
for a variety of reasons, including spinor helicity, color ordering, analyticity, KLT re-
lations with gravity, the string-inspired derivation, and the recent twistor formulation
of classical gauge theory. The derivative expansion is useful for finding results in the
quantum regime [1]-[16].
Potential simplifications based on a well-ordered formulation of the instanton
contributions to an n-point scattering amplitude can be useful in finding the total
correction to the quantum amplitudes. These terms to the amplitude take on the
form at n-point,
fm,n = gm,n(g,N)
∏ 1
t
[p],ai,p
i
e
?m 4π
g2
+m θ
2π K(εi, ki) , (1.1)
with ai,p labeling the power of the invariant (both negative and positive). The helicity
content containing the factors εi ·kj and εi ·εj is represented by the function K(εi, kj).
The kinematic invariants t
[p]
i are defined by
t
[p]
i = (ki + ki+1 + . . .+ ki+p?1)
2 , (1.2)
for an ordering of the external legs in the cyclic fashion (1, 2, . . . , n).
The coefficients gm,n enter as a result of the integration of the non-trivial gauge
field configuration a
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