1993
DOI: 10.1088/0305-4470/26/9/020
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Remarks on semiclassical quantization rule for broken SUSY

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Cited by 16 publications
(22 citation statements)
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“…In the usual semiclassical stationary phase approximation the action functional S x(t)] is expanded about the classical path x cl (t) as S x(t)] ' S cl (x 00 ; x 0 ; ) + S x(t)] + 2 S x(t)]: (17) The classical action S cl S cl (x 00 ; x 0 ; ) = S x cl (t)] is an action evaluated along the classical path from x 0 to x 00 , determined by S x(t)] = 0. Then the propagator is given by the formula of Van Vleck, Pauli and Morette (VMP) 24], K(x 00 ; x 0 ; ) ' xed X xcl(t) r i 2 h @ 2 S cl @x 0 @x 00 exp i h S cl : (18) If there are classical paths more than one, we have to add up the contributions from all these paths. Thus, the summation in (18) is to cover all the classical paths x cl (t) between x 0 and x 00 with a xed time interval .…”
Section: The Quasi-classical Approachmentioning
confidence: 99%
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“…In the usual semiclassical stationary phase approximation the action functional S x(t)] is expanded about the classical path x cl (t) as S x(t)] ' S cl (x 00 ; x 0 ; ) + S x(t)] + 2 S x(t)]: (17) The classical action S cl S cl (x 00 ; x 0 ; ) = S x cl (t)] is an action evaluated along the classical path from x 0 to x 00 , determined by S x(t)] = 0. Then the propagator is given by the formula of Van Vleck, Pauli and Morette (VMP) 24], K(x 00 ; x 0 ; ) ' xed X xcl(t) r i 2 h @ 2 S cl @x 0 @x 00 exp i h S cl : (18) If there are classical paths more than one, we have to add up the contributions from all these paths. Thus, the summation in (18) is to cover all the classical paths x cl (t) between x 0 and x 00 with a xed time interval .…”
Section: The Quasi-classical Approachmentioning
confidence: 99%
“…Then the propagator is given by the formula of Van Vleck, Pauli and Morette (VMP) 24], K(x 00 ; x 0 ; ) ' xed X xcl(t) r i 2 h @ 2 S cl @x 0 @x 00 exp i h S cl : (18) If there are classical paths more than one, we have to add up the contributions from all these paths. Thus, the summation in (18) is to cover all the classical paths x cl (t) between x 0 and x 00 with a xed time interval . This approximation formula is known to give rise to the exact propagator for the free particle, the harmonic oscillator and more general quadratic systems, but does not directly provide the WKB quantization rule (2).…”
Section: The Quasi-classical Approachmentioning
confidence: 99%
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“…It has recently been shown that for the cases of shape invariant three dimensional oscillator as well as for P oschl-Teller I and II potentials with broken SUSY, this lowest order BSWKB calculation gives the exact spectrum [95,97]. Recently, Dutt et al [96] have also developed a systematic higher order BSWKB expansion and using it have shown that in all the three (shape invariant) cases, the higher order corrections to O( h 6 ) are zero.…”
Section: Introductionmentioning
confidence: 99%
“…It has recently been shown that for the cases of shape invariant three dimensional oscillator as well as for Pöschl-Teller I and II potentials with broken SUSY, this lowest order BSWKB calculation gives the exact spectrum [95,97]. Recently, Dutt et al [96] have also developed a systematic higher order BSWKB expansion and using it have shown that in all the three (shape invariant) cases, the higher order corrections to O(h 6 ) are zero.…”
Section: Introductionmentioning
confidence: 99%