1990
DOI: 10.1016/0550-3213(90)90248-c
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Stringy cosmic strings and noncompact Calabi-Yau manifolds

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Cited by 456 publications
(920 citation statements)
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“…(The explicit factors of (z−z (n) i∞ ) −1/12 cancel out the zeroes of the Dedekind eta function at these points). These solutions were first constructed in [24] as "stringy cosmic strings," before the invention of D-branes, and they were later interpreted as D7-brane solutions by [25]. A recent analysis is given in [26], whose notation we follow.…”
Section: Review Of 1/2-bps Seven-brane Solutionsmentioning
confidence: 99%
“…(The explicit factors of (z−z (n) i∞ ) −1/12 cancel out the zeroes of the Dedekind eta function at these points). These solutions were first constructed in [24] as "stringy cosmic strings," before the invention of D-branes, and they were later interpreted as D7-brane solutions by [25]. A recent analysis is given in [26], whose notation we follow.…”
Section: Review Of 1/2-bps Seven-brane Solutionsmentioning
confidence: 99%
“…Then, the warp factor becomes one, h = 1, and we recover the D7 brane solution in the so-called weak-coupling approximation. Here the complete D7 brane dilaton profile [104] (shown as a dashed curve in fig. 13a) is approximated by the logarithmic profile (4.5) (solid curve in fig.…”
Section: The D3/d7 Supergravity Solutionmentioning
confidence: 99%
“…One can show that membranes constructed in this manner have representatives which are holomorphic two-cycles in T , albeit with respect to a different complex structure than the usual one compatible with the elliptic fibration. The class of such membranes lies in the relative homology H 2 (T /F, Z) and will be denoted by v. If T = K3, then [25] the self-intersection number of any class v containing a holomorphic two-cycle is given by…”
Section: Kodaira Type Imentioning
confidence: 99%