2003
DOI: 10.1209/epl/i2003-00185-0
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Chaos and open orbits in hole-antidot arrays with non-isotropic Fermi surface

Abstract: Periodic antidot arrays imposed upon two-dimensional hole systems (2DHSs) display a striking dependence of the positive low-field magnetoresistance on the in-plane crystallographic orientation of the superlattice. An enhanced positive magnetoresistance can be ascribed to the 2DHSs non-circular Fermi surface which stabilizes chaotic trajectories for specific crystallographic directions. The effect provides a first example of the role of non-spherical Fermi surfaces on the classical chaotic dynamics of charge ca… Show more

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Cited by 8 publications
(9 citation statements)
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“…7 It has been shown to lead to multiband transport, 4,6 to modified Landau level degeneracies, [4][5][6] and to additional harmonics in the cyclotron resonance modes. 7 In general, Fermi surface anisotropy is also expected to have effects on the mesoscopic transport properties, 8,9 such as anisotropic electron conduction. This effect has recently been evidenced in ballistic transport experiments in BLG and attributed to TW.…”
Section: Main Textmentioning
confidence: 99%
“…7 It has been shown to lead to multiband transport, 4,6 to modified Landau level degeneracies, [4][5][6] and to additional harmonics in the cyclotron resonance modes. 7 In general, Fermi surface anisotropy is also expected to have effects on the mesoscopic transport properties, 8,9 such as anisotropic electron conduction. This effect has recently been evidenced in ballistic transport experiments in BLG and attributed to TW.…”
Section: Main Textmentioning
confidence: 99%
“…That the cyclotron orbit from one antidot to the other affects magnetoresistance properties suggests that the antidot lattice could be used to detect anisotropy of the Fermi surface [11]. To illustrate the basic idea, here we consider the simplest cases in panels (i)-(iii) of Fig.…”
Section: (B)mentioning
confidence: 99%
“…Therefore, detection of an anisotropic cyclotron orbit is direct proof of an anisotropic Fermi surface. Such proof could be acquired in a ballistic transport experiment using an antidot lattice [41][42], which, as shown schematically in Fig. 1(c), is a regular array of nano-holes [42][43][44][46][47][48][49][50][51].…”
Section: Introductionmentioning
confidence: 97%
“…1(c), is a regular array of nano-holes [42][43][44][46][47][48][49][50][51]. If the mean free path of the conductor is sufficiently long, the magnetoresistance shows peaks (commensurability peaks) arising from matching of the cyclotron diameter with the distance between antidots [42][43][44][46][47][48][49][50] (cases 1-3 in Fig. 1(c)).…”
Section: Introductionmentioning
confidence: 99%