Theoretical Physics at the End of the Twentieth Century 2002
DOI: 10.1007/978-1-4757-3671-7_2
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Lectures on Branes, Black Holes, and Anti-de Sitter Space

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Cited by 16 publications
(41 citation statements)
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“…There is also a competing physical process that we described in section 3.2 above: the cyclotron resonance. If we keep B/T 2 small (h 1), then we can trust our hydrodynamic approximation of the location of the cyclotron pole at ω c − iγ, given in (30). In figure 2, we plot the dimensionless γ/T against ρ/T 2 σ 0 for an appropriately small B/T 2 = 1.…”
Section: Numerical Results For 1/τ Impmentioning
confidence: 98%
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“…There is also a competing physical process that we described in section 3.2 above: the cyclotron resonance. If we keep B/T 2 small (h 1), then we can trust our hydrodynamic approximation of the location of the cyclotron pole at ω c − iγ, given in (30). In figure 2, we plot the dimensionless γ/T against ρ/T 2 σ 0 for an appropriately small B/T 2 = 1.…”
Section: Numerical Results For 1/τ Impmentioning
confidence: 98%
“…The full action for this abelian truncation can be found for example in ref. [30]. To see which scalar fields remain neutral, it is useful to think of the 35 dimensional representation of SO (8) as the set of symmetric traceless quadratic polynomials in the coordinates on…”
Section: Impurity Relaxation In the Truncated M2 Brane Theorymentioning
confidence: 99%
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“…Rather than presenting the solution and showing that it solves the low energy equations of type II superstring, we will describe some aspects of the art of solution-building. There are many excellent reviews of this area (see, for example, [45,46,47,48,49,50,51,52,53], other general reviews on black holes in string/M theories include [54,55,56]), so we shall be brief. The method of construction of various classical solutions, we will see, will throw light on the microscopic configurations corresponding to these solutions.…”
Section: Construction Of Classical Solutionsmentioning
confidence: 99%