2011
DOI: 10.1140/epjb/e2010-10737-0
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Distribution of persistent currents in a multi-arm mesoscopic ring

Abstract: We propose an idea to investigate persistent current in individual arms of a multi-arm mesoscopic ring. Following a brief description of persistent current in a traditional Aharonov-Bohm (AB) ring, we examine the behavior of persistent currents in separate arms of a three-arm mesoscopic ring. Our analysis may be helpful in studying magnetic response of any complicated quantum network.

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Cited by 11 publications
(8 citation statements)
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“…Persistent current being one such exotic quantum mechanical phenomenon observed in normal metal mesoscopic rings and nanotubes pierced by Aharonov-Bohm (AB) flux φ. Prior to its experimental evidence, the possibility of a non-decaying current in normal metal rings was first predicted by Büttiker, Imry and Landauer 3 in a pioneering work, and, in the sub-sequent years theoretical attempts were made [4][5][6][7][8][9][10][11][12][13][14][15][16][17] to understand the actual mechanism behind it. The experimental realization of this phenomenon of non-decaying current in metallic rings/cylinders has been established quite in late.…”
Section: Introductionmentioning
confidence: 99%
“…Persistent current being one such exotic quantum mechanical phenomenon observed in normal metal mesoscopic rings and nanotubes pierced by Aharonov-Bohm (AB) flux φ. Prior to its experimental evidence, the possibility of a non-decaying current in normal metal rings was first predicted by Büttiker, Imry and Landauer 3 in a pioneering work, and, in the sub-sequent years theoretical attempts were made [4][5][6][7][8][9][10][11][12][13][14][15][16][17] to understand the actual mechanism behind it. The experimental realization of this phenomenon of non-decaying current in metallic rings/cylinders has been established quite in late.…”
Section: Introductionmentioning
confidence: 99%
“…We note that a related multiring or multiarm setup has recently been studied within the non-interacting tight-binding formalism. 45 We take the hopping amplitude between the sites within the ring and within the lead as a constant, t 0 = −t, and measure all energies in the units of t. For the ring part of the system, we consider rings with the next-nearest neighbour coupling (2NN) that is given by the hopping amplitude t ′ .…”
Section: Model and Methodsmentioning
confidence: 99%
“…Through a Fourier transformation and the implementation of the fluctuation‐dissipation theorem, we can write the total current as I=dωfωjp()ω+jJ()ωwith jpfalse(ωfalse) being the current density for the persistent current contribution given by [ 60 ] jpω=eπk2sin2πNnormalΦ+kImfalse⟨ck;ckfalse⟩ωrwhich is completely equivalent to expression (13). Hence, jJfalse(ωfalse) is the Josephson density current, given by truerightj()ω=left4ehkIm[λeikjImfalse⟨a;ckfalse⟩ωr+λ+eikjImfalse⟨a;ckfalse⟩ωrleft+λImfalse⟨f;ckfalse⟩ωr+λ+Imfalse⟨f;ck…”
Section: Persistent and DC Josephson Currentsmentioning
confidence: 99%