Noncommutative Geometry and String Field Theory

By M. Schnabl. 2014

364 citations recorded by the source corpus.

View Paper: https://www.semanticscholar.org/paper/e51926735a664296324014b4e3a24aa7c88a40d5

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Exact results on the ABJM Fermi gas (2012, background): “For example, the associativity anomaly [32] in cubic string field theory [33] comes from the singularity at the boundary of the moduli space and relates to the translational invariance in string field theory.”
Towards understanding the ultraviolet behavior of quantum loops in infinite-derivative theories of gravity (2014, background): “For instance, we find that K ( ) = −e /M2 for stringy toy model s based onp-adic numbers [13], or random lattices [15, 16], and K ( ) =−( +m2)e /M2 in SFT [11], wherem2(< 0) andM2(> 0) are proportional to the string tension 1.”
Perturbative superstring theory revisited (2012, background): “This entails calculating what one may call the string propagator; in fact, with a standard gauge-fixing, string field theory leads precisely to the propagators that we will calculate (for example, see [22, 42]).”
The Black Hole Information Problem (2016, background): “) The most direct analog for string theory would be string field theory, but in spite of some nice structures such as [2], it does not seem to have answered the question.”
L∞ algebras and field theory (2017, background): “In bosonic open string field theory [1] the interaction of strings is defined by a multiplication rule, a star product of string fields that happens to be associative.”
Stable bounce and inflation in non-local higher derivative cosmology (2012, background): “For more general aspects of string field theory see for instance [33].”