2013
DOI: 10.1155/2013/517858
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Semiclassical Strings in (2+1)-Dimensional Backgrounds

Abstract: This study analyzes the geometrical relationship between a classical string and its semi-classical quantum model. From an arbitrary (2 + 1)−dimensional geometry, a specific ansatz for a classical string is used to generate a semi-classical quantum model. In this framework, examples of quantum oscillations and quantum free particles are presented that uniquely determine a classical string and the spacetime geometry where its motion takes place.

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Cited by 2 publications
(7 citation statements)
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“…Quantum fluctuation depends on the function g, which determines the geometry of the space and the momentum operatorΠ. Some possibilities for g have already been discussed in the context of moving strings [3], and we bring them to the context of the static string in the next section.…”
Section: The Semi-classical Descriptionmentioning
confidence: 97%
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“…Quantum fluctuation depends on the function g, which determines the geometry of the space and the momentum operatorΠ. Some possibilities for g have already been discussed in the context of moving strings [3], and we bring them to the context of the static string in the next section.…”
Section: The Semi-classical Descriptionmentioning
confidence: 97%
“…where E = √ λṫ andṫ = κ have been used as the classical energy of the string andṫ 2 = g 2 y ′ 2 has been used from (3). Thus, the quantum solutions are free particles whose squared energy is given by the difference between the squared classical energy E 2 and the squared quantum…”
Section: The Semi-classical Descriptionmentioning
confidence: 99%
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“…When the parameter is set to zero, the deformed sphere becomes the usual five dimensional sphere and consequently the Lunin-Maldacena space recovers AdS 5 × S 5 in this limit. Some other axisymmetric space-times have been used in semi-classical string theory [2,3].…”
Section: Introductionmentioning
confidence: 99%