theorem 106.10 Stationary phase

open in the book · parts/11-qft-standard-model/08-path-integral-quantization.tex:693 · p. 2163

Rests on

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theorem 106.10: Stationary phase106.10equation 106.8: eq:pathint-fresnel106.8proposition 106.11: The semiclassical propagator is the WKB wavefunction106.11proof : ch:08-path-integral-quantization@proof-8proofproposition 106.4: From the kernel to the Schrödinger equation106.4equation 106.3: eq:pathint-hj106.3equation 106.17: eq:pathint-van-vleck106.17proof : ch:08-path-integral-quantization@proof-9proof

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typedirectionnode provenancewhere
depends_on eq:pathint-fresnel declared parts/11-qft-standard-model/08-path-integral-quantization.tex:706
depends_on The semiclassical propagator is the WKB wavefunction declared parts/11-qft-standard-model/08-path-integral-quantization.tex:758
proves ch:08-path-integral-quantization@proof-8 declared parts/11-qft-standard-model/08-path-integral-quantization.tex:709