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Where a zeta function and multiple zeta function may be assigned to a suitable variety, so a motivic multiple zeta function is attached to the corresponding motive, like a motivic L-function is.
Where zeta functions appear in physics as expressions for vacuum amplitudes, so multiple zeta functions appear in expressions for more general scattering amplitudes. The intricate combinatorics of these becomes often more tractable when re-expressing them as motivic multiple zeta values (e.g. Schlotterer-Stieberger 12).
Francis Brown, On the decomposition of motivic multiple zeta values (arXiv:1102.1310v2)
A. B. Goncharov, Galois symmetries of fundamental groupoids and noncommutative geometry (arXiv:math/0208144)
Of the superstring:
O. Schlotterer, Stephan Stieberger, Motivic Multiple Zeta Values and Superstring Amplitudes (arXiv:1205.1516)
Stephan StiebergerMotivic superstring amplitudes, 2013 (pdf)
In N=4 D=4 super Yang-Mills theory:
See also at motives in physics.
Last revised on March 2, 2015 at 14:21:23. See the history of this page for a list of all contributions to it.