Influence of Small-Angle Diffraction on the Ballistic Conductance Fluctuations in Chaotic Billiards

Journal of the Physical Society of Japan

Volumn 67, Issue 2, 1998, Pages 397-400

  Takane, Yositake ^a   Nakamura, Katsuhiro ^a  

^a Osaka Prefecture University   (Japan)

Author keywords

Ballistic transport; Conductance fluctuation; Quantum chaos; Semiclassical theory

Indexed keywords

EID: 0032395318     PISSN: 00319015     EISSN: None     Source Type: Journal    
DOI: 10.1143/JPSJ.67.397     Document Type: Article

References (14)

1. For a review, see: Chaos and Quantum Transport in Mesoscopic Cosmos, ed. K. Nakamura, Chaos, Solitons & Fractals 8 (1997) No. 7/8.
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4. C. M. Marcus, A. J. Rimberg, R. M. Westervelt, P. F. Hopkins and A. C. Gossard: Phys. Rev. Lett. 69 (1992) 506; M. W. Keller, O. Millo, A. Mittal, D. E. Prober and R. N. Sacks: Surf. Sci. 305 (1994) 501; J. P. Bird, K. Ishibashi, Y. Aoyagi, T. Sugano and Y. Ochiai: Phys. Rev. B 50 (1994) 18678.
5. C. M. Marcus, A. J. Rimberg, R. M. Westervelt, P. F. Hopkins and A. C. Gossard: Phys. Rev. Lett. 69 (1992) 506; M. W. Keller, O. Millo, A. Mittal, D. E. Prober and R. N. Sacks: Surf. Sci. 305 (1994) 501; J. P. Bird, K. Ishibashi, Y. Aoyagi, T. Sugano and Y. Ochiai: Phys. Rev. B 50 (1994) 18678.
6. We use the terminology accepted in quantum transport theories in the diffusive regime. The diffuson (cooperon) is the pair propagator representing the interference in the particle-hole (particle-particle) channel.
7. See, for example, P. A. Lee, A. D. Stone and H. Fukuyama: Phys. Rev. B 35 (1987) 1039.
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9. H. U. Baranger and P. A. Mello: Phys. Rev. Lett. 73 (1994) 142; R. A. Jalabert, J.-L. Pichard and C. W. J. Beenakker: Europhys. Lett. 27 (1994) 255.
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12. I. L. Aleiner and A. I. Larkin: Phys. Rev. B 54 (1996) 14423.
13. Details of the calculations will be published elsewhere.
14. N. Argaman: Phys. Rev. B 53 (1996) 7035.