2014
DOI: 10.1088/1751-8113/47/35/355402
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Nonlocality in string theory

Abstract: We discuss an aspect of string theory which has been tackled from many different perspectives, but incompletely: the role of nonlocality in the theory and its relation to the geometric shape of the string. In particular, we will describe in quantitative terms how one can zoom out from an extended object such as the string in such a way that, at sufficiently large scales, it appears structureless. Since there are no free parameters in free-string theory, the notion of large scales will be unambiguously determin… Show more

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Cited by 80 publications
(134 citation statements)
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References 26 publications
(71 reference statements)
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“…In general, one of the indicators characterizing quantum geometry, the spectral dimension d S of spacetime, changes with the scale, running from d S 2 (or exactly d S = 2) in the ultraviolet (UV) to the usual, classical value d S ∼ 4 in the infrared (IR). Numerical and analytic examples can be found in causal dynamical triangulations (CDT) [4,5], random combs [6,7] and random multigraphs [8,9] (both sharing some properties with CDT), quantum Einstein gravity (QEG, also called asymptotic safety) [10,11], spin foams [12][13][14][15], Hořava-Lifshitz gravity [16,17], noncommutative geometry at the fundamental [18,19] and effective [20][21][22] levels, field theory on multifractal spacetimes [23][24][25] (in particular, in the realization within multifractional geometry [26][27][28][29][30][31]), and nonlocal super-renormalizable quantum gravity [32][33][34].…”
Section: Introductionmentioning
confidence: 99%
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“…In general, one of the indicators characterizing quantum geometry, the spectral dimension d S of spacetime, changes with the scale, running from d S 2 (or exactly d S = 2) in the ultraviolet (UV) to the usual, classical value d S ∼ 4 in the infrared (IR). Numerical and analytic examples can be found in causal dynamical triangulations (CDT) [4,5], random combs [6,7] and random multigraphs [8,9] (both sharing some properties with CDT), quantum Einstein gravity (QEG, also called asymptotic safety) [10,11], spin foams [12][13][14][15], Hořava-Lifshitz gravity [16,17], noncommutative geometry at the fundamental [18,19] and effective [20][21][22] levels, field theory on multifractal spacetimes [23][24][25] (in particular, in the realization within multifractional geometry [26][27][28][29][30][31]), and nonlocal super-renormalizable quantum gravity [32][33][34].…”
Section: Introductionmentioning
confidence: 99%
“…Due to the young age of the proposal, these tools are largely unexplored and the purpose of this paper is to continue the investigation initiated in Refs. [26][27][28][29], in the meanwhile improving the understanding of dimensional flow as a general phenomenon of quantum geometry.…”
Section: Introductionmentioning
confidence: 99%
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