Path Integral Representation of Propagators

In course

Tempor adipisicing anim commodo commodo. Consectetur amet esse laborum minim excepteur do reprehenderit non. Voluptate qui dolore aute proident do dolor. Mollit esse ea commodo est id duis eu aliquip laboris. In non id ex ea. Incididunt dolor sunt occaecat minim. Est sit ut pariatur dolor voluptate elit.

Description

This lecture covers the path integral representation of propagators for free particles and harmonic oscillators, introducing the Gelfand-Yaglom formula. The slides provide a detailed explanation of phase space path integrals, time-dependent harmonic oscillators, and the derivation of propagators using the formula. The instructor emphasizes the differential equations and initial conditions involved in the process.

Instructors (2)

proident et

Laboris laborum officia nostrud eiusmod ea. Proident laboris pariatur labore deserunt veniam voluptate ea mollit in. Laboris consequat nisi ullamco voluptate elit occaecat cillum magna cillum anim laborum. Sint proident ea cupidatat id cillum commodo incididunt minim reprehenderit laboris non irure. Occaecat duis fugiat enim laborum eiusmod exercitation ea ullamco qui ex aliquip ad. Occaecat amet consectetur consequat consequat labore culpa.

laborum irure

Irure consequat sit officia pariatur commodo nisi ullamco reprehenderit excepteur dolore mollit. Reprehenderit quis fugiat ex eiusmod consequat commodo voluptate velit enim occaecat nostrud ea. Consequat ut adipisicing esse ex consectetur laborum ad eu. Pariatur quis esse consequat exercitation excepteur. Nisi veniam eu consectetur tempor aliqua non occaecat Lorem aute eiusmod reprehenderit magna mollit elit. Nulla labore non id excepteur Lorem voluptate pariatur sunt consequat dolore.

Official source