Geodesic
Stationary-phase method for Feynman's continual integral
Teoretičeskaâ i matematičeskaâ fizika, Tome 2 (1970) no. 1, pp. 30-35

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The formula obtained earlier by the author, for the condition that the classical paths of the functional $\smallint Ldt$ are not degenerate, is generalized. 
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     author = {V. P. Maslov},
     title = {Stationary-phase method for {Feynman's} continual integral},
     journal = {Teoreti\v{c}eska\^a i matemati\v{c}eska\^a fizika},
     pages = {30--35},
     publisher = {mathdoc},
     volume = {2},
     number = {1},
     year = {1970},
     language = {ru},
     url = {http://geodesic.mathdoc.fr/item/TMF_1970_2_1_a1/}
}
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V. P. Maslov. Stationary-phase method for Feynman's continual integral. Teoretičeskaâ i matematičeskaâ fizika, Tome 2 (1970) no. 1, pp. 30-35. http://geodesic.mathdoc.fr/item/TMF_1970_2_1_a1/