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Volumn 58, Issue 6, 1998, Pages 4779-4783

Fermi accelerator in atom optics

Author keywords

[No Author keywords available]

Indexed keywords

AMPLITUDE MODULATION; CHAOS THEORY; DIFFERENTIAL EQUATIONS; ELECTROMAGNETIC WAVE REFLECTION; ELECTRON TRANSITIONS; GRAVITATIONAL EFFECTS; GROUND STATE; LASERS; LYAPUNOV METHODS; PARTICLE ACCELERATORS; PLASMA OSCILLATIONS; SPONTANEOUS EMISSION;

EID: 0032382059     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.58.4779     Document Type: Article
Times cited : (81)

References (36)
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    • PHRVAO
    • E. Fermi, Phys. Rev. 75, 1169 (1949).PHRVAO
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  • 10
    • 4243100403 scopus 로고    scopus 로고
    • For a review of the field of atom optics see the special issues: Appl. Phys. B: Photophys. Laser Chem. 54, 319 (1992), edited by J. Mlynek, V. Balykin, and P. Meystre
    • For a review of the field of atom optics see the special issues: Appl. Phys. B: Photophys. Laser Chem. 54, 319 (1992), edited by J. Mlynek, V. Balykin, and P. Meystre;
  • 11
    • 0343694197 scopus 로고
    • J. Phys. II 4, 1877 (1994), edited by P. Pillet;
    • (1994) J. Phys. II , vol.4 , pp. 1877
  • 12
    • 0007760999 scopus 로고    scopus 로고
    • Quantum Semiclassic. Opt. 8, 495 (1996), edited by E. Arimondo and H.-A. Bachor.
    • (1996) Quantum Semiclassic. Opt. , vol.8 , pp. 495
  • 14
    • 0002636980 scopus 로고
    • PLRAAN
    • The field of atom optics as a testing ground for quantum chaos started with the theoretical proposal of R. Graham, M. Schlautmann, and P. Zoller, Phys. Rev. A 45, R19 (1992), followed by the experiment of PLRAAN
    • (1992) Phys. Rev. A , vol.45 , pp. R19
    • Graham, R.1    Schlautmann, M.2    Zoller, P.3
  • 17
    • 0000505664 scopus 로고    scopus 로고
    • PLRAAN
    • For the microwave-driven hydrogen atom, the continuum plays an important role. See, for example, F. Benvenuto, G. Casati, and D. L. Shepelyansky, Phys. Rev. A 55, 1732 (1997); PLRAAN
    • (1997) Phys. Rev. A , vol.55 , pp. 1732
    • Benvenuto, F.1    Casati, G.2    Shepelyansky, D.L.3
  • 21
    • 4243839784 scopus 로고    scopus 로고
    • PRLTAO
    • Another example is the ion in a Paul trap interacting with a standing light field. The ion is driven either by the explicit time dependence of the trap or of the standing wave. See, for example, M. El Ghafar, P. Törmä, V. Savichev, E. Mayr, A. Zeiler, and W. P. Schleich, Phys. Rev. Lett. 78, 4181 (1997); PRLTAO
    • (1997) Phys. Rev. Lett. , vol.78 , pp. 4181
    • El Ghafar, M.1    Törmä, P.2    Savichev, V.3    Mayr, E.4    Zeiler, A.5    Schleich, W.P.6
  • 26
    • 85037213148 scopus 로고    scopus 로고
    • We indicate the physical variables with tildes, and we will drop all the tildes later when we introduce the dimensionless variables
    • We indicate the physical variables with tildes, and we will drop all the tildes later when we introduce the dimensionless variables.
  • 28
    • 85037214834 scopus 로고    scopus 로고
    • This value of (Formula presented) is also consistent with the commutation rela-tion (Formula presented) for the dimensionless canonical variables z and p
    • This value of (Formula presented) is also consistent with the commutation rela-tion (Formula presented) for the dimensionless canonical variables z and p.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.