Oxford Music Online 2001
DOI: 10.1093/gmo/9781561592630.article.13358
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Hornbostel, Erich M(oritz) von

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“…The expressions (16a) and (16b) correspond to finite and infinite intervals respectively. Note that this requires us to take C 2 = 0 in (15) and limits the acceptable solutions (15) to Bessel functions of order ν = 1/2 (trigonometric). This result also eliminates unbounded wave functions since for large Z, J ν (W (2) Z) ∼ Z −1/2 so our solutions, which are of the form Z ν J ν (••), remain bounded at large Z.…”
Section: Solutionsmentioning
confidence: 99%
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“…The expressions (16a) and (16b) correspond to finite and infinite intervals respectively. Note that this requires us to take C 2 = 0 in (15) and limits the acceptable solutions (15) to Bessel functions of order ν = 1/2 (trigonometric). This result also eliminates unbounded wave functions since for large Z, J ν (W (2) Z) ∼ Z −1/2 so our solutions, which are of the form Z ν J ν (••), remain bounded at large Z.…”
Section: Solutionsmentioning
confidence: 99%
“…Although there are issues with Wheeler-DeWitt theory, it is very often used as an approximation to a theory of quantum gravity, and it is therefore useful to see what predictions it makes in this respect [11][12][13]. Such studies have been performed, for example, in the context of black holes [14][15][16][17], wormholes [18][19][20], and cosmology [21][22][23] (also see references therein). With this in mind we perform the analysis here.…”
Section: Introductionmentioning
confidence: 99%