7 Divergence Properties of Maximal 6 Gravity Loop Amplitudes from 6.1 One-loop four-point example

6.2 Arbitrary numbers of legs at one loop

Surprisingly, the above four-point results can be extended to an arbitrary number of external legs. Using the unitarity methods, the five- and six-point amplitudes with all identical helicity have also been obtained by direct calculation [22Jump To The Next Citation Point In The Article, 23Jump To The Next Citation Point In The Article]. Then by demanding that the amplitudes have the properties described in Section  3.4 for momenta becoming either soft [139Jump To The Next Citation Point In The Article, 10] or collinear [22Jump To The Next Citation Point In The Article], an ansatz for the one-loop maximally helicity-violating amplitudes for an arbitrary number of external legs has also been obtained. These amplitudes were constructed from a set of building blocks called ``half-soft-function'', which have ``half'' of the proper behavior as gravitons become soft. The details of this construction and the explicit forms of the amplitudes may be found in Refs. [22Jump To The Next Citation Point In The Article, 23Jump To The Next Citation Point In The Article].

The all-plus helicity amplitudes turn out to be very closely related to the infinite sequence of one-loop maximally helicity-violating amplitudes in N =8 supergravity. The two sequences are related by a curious ``dimension shifting formula.'' In Ref. [23Jump To The Next Citation Point In The Article], a known dimension shifting formula [18] between identical helicity QCD and N =4 super-Yang-Mills amplitudes was used to obtain the four-, five-, and six-point N =8 amplitudes from the identical helicity gravity amplitudes using the KLT relations in the unitarity cuts. Armed with these explicit results, the soft and collinear properties were then used to obtain an ansatz valid for an arbitrary number of external legs [23Jump To The Next Citation Point In The Article]. This provides a rather non-trivial illustration of how the KLT relations can be used to identify properties of gravity amplitudes using known properties of gauge theory amplitudes.

Interestingly, the all-plus helicity amplitudes are also connected to self-dual gravity [108Jump To The Next Citation Point In The Article, 52Jump To The Next Citation Point In The Article, 109Jump To The Next Citation Point In The Article] and self-dual Yang-Mills [143, 53Jump To The Next Citation Point In The Article, 93, 92, 4Jump To The Next Citation Point In The Article, 30Jump To The Next Citation Point In The Article, 33Jump To The Next Citation Point In The Article], i.e. gravity and gauge theory restricted to self-dual configurations of the respective field strengths, tex2html_wrap_inline2816 and tex2html_wrap_inline2818, with tex2html_wrap_inline2820 . This connection is simple to see at the linearized (free field theory) level since a superposition of plane waves of identical helicity satisfies the self-duality condition. The self-dual currents and amplitudes have been studied at tree and one-loop levels [53, 4, 30, 33Jump To The Next Citation Point In The Article]. In particular, Chalmers and Siegel [33] have presented self-dual actions for gauge theory (and gravity), which reproduce the all-plus helicity scattering amplitudes at both tree and one-loop levels.

The ability to obtain exact expressions for gravity loop amplitudes demonstrates the utility of this approach for investigating quantum properties of gravity theories. The next section describes how this can be used to study high energy divergence properties in quantum gravity.



7 Divergence Properties of Maximal 6 Gravity Loop Amplitudes from 6.1 One-loop four-point example

image Perturbative Quantum Gravity and its Relation to Gauge Theory
Zvi Bern
http://www.livingreviews.org/lrr-2002-5
© Max-Planck-Gesellschaft. ISSN 1433-8351
Problems/Comments to livrev@aei-potsdam.mpg.de