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Nonlocal transport mediated by spin supercurrents
Phys. Rev. B 90, 220401(R) – Published 1 December, 2014
DOI: https://doi.org/10.1103/PhysRevB.90.220401
Abstract
In thin-film ferromagnets with perfect easy-plane anisotropy, the component of total spin perpendicular to the easy plane is a good quantum number and the corresponding spin supercurrent can flow without dissipation. Here we explain how spin supercurrents couple spatially remote spin-mixing vertical transport channels, even when easy-plane anisotropy is imperfect, and discuss the possibility that this effect can be used to fabricate new types of electronic devices.
Article Text
References (20)
- A. Brataas, A. D. Kent, and H. Ohno, Nat. Mater. 11, 372 (2012).
- For a review of theoretical work on this topic, which has a rather long history, see E. B. Sonin, J. Low Temp. Phys. 171, 757 (2013), and references cited therein.
- J. König, M. Chr. Bønsager, and A. H. MacDonald, Phys. Rev. Lett. 87, 187202 (2001).
- F. S. Nogueira and K.-H. Bennemann, Europhys. Lett. 67, 620 (2004).
- S. Takei and Y. Tserkovnyak, Phys. Rev. Lett. 112, 227201 (2014).This paper analyzes a situation similar to the long nanomagnet limit of the present Rapid Communication, but does not recognize the static order dissipationless spin-current regime discussed in this work.
- S. Takei, B. I. Halperin, A. Yacoby, and Y. Tserkovnyak, Phys. Rev. B 90, 094408 (2014).
- The resistance of 1 nm thick permalloy thin films at room temperature is [8] . The resistance area product of the Co/Cu metal stacks is typically near [9]. For a permalloy link of widths of m, and a lateral dimension of the metal stacks of m, the link resistance is substantially larger than the stack resistance . Crosstalk has little influence on device performance unless the stack resistance is comparable to the link resistance.
- A. F. Mayadas, J. F. Janak, and A. Gangulee, J. Appl. Phys. 45, 2780 (1974).
- J. Bass and W. P. Pratt, Jr., J. Magn. Magn. Mater. 200, 274 (1999).
- J. C. Slonczewski, J. Magn. Magn. Mater. 159, L1 (1996); M. Tsoi, A. G. M. Jansen, J. Bass, W.-C. Chiang, M. Seck, V. Tsoi, and P. Wyder, Phys. Rev. Lett. 80, 4281 (1998); E. Myers, D. Ralph, J. Katine, R. Louie, and R. Buhrman, Science 285, 867 (1999); J. Sun, J. Magn. Magn. Mater. 202, 157 (1999).
- D. C. Ralph and M. D. Stiles, J. Magn. Magn. Mater. 320, 1190 (2008).
- Y. Tserkovnyak, A. Brataas, G. E. W. Bauer, and B. I. Halperin, Rev. Mod. Phys. 77, 1375 (2005).
- We have for simplicity assumed that the efficiency factors are identical for spin-transfer torques and spin pumping. This is strictly speaking true only when the source and drain electrodes are fully spin selective.
- S. I. Kiselev, J. C. Sankey, I. N. Krivorotov, N. C. Emley, R. J. Schoelkopf, R. A. Buhrman, and D. C. Ralph, Nature (London) 425, 380 (2003); W. H. Rippard, M. R. Pufall, S. Kaka, S. E. Russek, and T. J. Silva, Phys. Rev. Lett. 92, 027201 (2004).
- A. Garcia-Arribas, E. Fernandez, A. V. Svalov, G. V. Kurlyandskaya, A. Barrainkua, D. Navas, and J. M. Barandiaran, Eur. Phys. J. B 86, 136 (2013); A. Garcia-Arribas, E. Fernandez, I. Orue, and J. M. Barandiaran, Appl. Phys. Lett. 103, 142411 (2013).
- H. Chen, I. Sodemann, and A. H. MacDonald (unpublished).
- J.-J. Su and A. H. MacDonald, Nat. Phys. 4, 799 (2008).
- R. H. Koch, J. A. Katine, and J. Z. Sun, Phys. Rev. Lett. 92, 088302 (2004).
- I. N. Krivorotov, N. C. Emley, A. G. F. Garcia, J. C. Sankey, S. I. Kiselev, D. C. Ralph, and R. A. Buhrman, Phys. Rev. Lett. 93, 166603 (2004).
- V. Ambegaokar and B. I. Halperin, Phys. Rev. Lett. 22, 1364 (1969).