theorem 9.72 Connection formulae

open in the book · parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2543 · p. 302

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theorem 9.72: Connection formulae9.72corollary 9.62: The semiclassical wave9.62equation 9.79: eq:slt-wkb-airy-ai9.79equation 9.80: eq:slt-wkb-airy-bi9.80equation 9.76: eq:slt-wkb-airy-equation9.76equation 9.74: eq:slt-wkb-airy-scale9.74postulate A.795: Matching, quotedA.795proposition 23.57: The wave resolution at a turning surface23.57proposition 23.56: The phase jump at a fold23.56proposition 9.74: Connection at a turning point of odd order9.74remark 23.51: Where the expansion breaks, and what is owed23.51theorem 9.78: Semiclassical quantisation of a well9.78theorem 9.76: Semiclassical transmission through a barrier9.76proof : ch:07-odes-sturm-liouville@proof-37proofequation 9.62: eq:slt-wkb-ansatz9.62equation 9.61: eq:slt-wkb-kappa9.61proposition 9.61: Eikonal and transport equations9.61proposition 9.63: The transport equation is flux conservation9.63proof : ch:07-odes-sturm-liouville@proof-32proofproposition 9.69: The integral solves the Airy equation9.69equation 31.32: eq:fluid-ns31.32corollary A.799: The impressed pressure gradientA.799theorem 9.70: Asymptotics of the Airy functions9.70remark 23.58: The caustics that are not turning surfaces23.58remark 23.59: What is observed23.59proof : ch:06-hamilton-jacobi@proof-20proofproposition 23.55: The fold, and the quarter-power law23.55remark 9.79: Where the one half comes from9.79proof : ch:06-hamilton-jacobi@proof-19proofequation 9.83: eq:slt-turning-local9.83proof : ch:07-odes-sturm-liouville@proof-38proofproposition 9.65: Validity criterion9.65equation 9.59: eq:slt-wkb-schrodinger9.59example 9.80: The harmonic oscillator9.80proposition 23.38: Bohr–Sommerfeld and Einstein–Brillouin–Keller quantization23.38proposition 52.24: The p-mode cavity52.24proof : ch:07-odes-sturm-liouville@proof-40proofexperiment : Cockcroft and Walton: lithium split by accelerated protonsexperime…example 9.81: Gamow factor for an alpha particle, in SI9.81phenomenon 117.5: The reaction proceeds far below the Coulomb barrier117.5neighborhood truncated

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typedirectionnode provenancewhere
depends_on The semiclassical wave declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2566
depends_on eq:slt-wkb-airy-ai declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2566
depends_on eq:slt-wkb-airy-bi declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2566
depends_on eq:slt-wkb-airy-equation declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2566
depends_on eq:slt-wkb-airy-scale declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2566
depends_on Matching, quoted declared appendices/A-long-proofs.tex:38939
depends_on The wave resolution at a turning surface declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:1945
depends_on The phase jump at a fold declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:1910
depends_on Connection at a turning point of odd order declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2659
depends_on Where the expansion breaks, and what is owed declared parts/03-classical-mechanics/06-hamilton-jacobi.tex:1762
depends_on Semiclassical quantisation of a well declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2904
depends_on Semiclassical transmission through a barrier declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2783
proves ch:07-odes-sturm-liouville@proof-37 declared parts/02-mathematical-methods/07-odes-sturm-liouville.tex:2569