Universal behaviors of magnon-mediated spin transport in disordered nonmagnetic metal-ferromagnetic insulator heterostructures
Gaoyang Li1, Fuming Xu1, Jian Wang1,2()
1. College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, China 2. Department of Physics, The University of Hong Kong, Pokfulam Road, Hong Kong, China
We numerically investigate magnon-mediated spin transport through nonmagnetic metal/ferromagnetic insulator (NM/FI) heterostructures in the presence of Anderson disorder, and discover universal behaviors of the spin conductance in both one-dimensional (1D) and 2D systems. In the localized regime, the variance of logarithmic spin conductance σ2(lnGT) shows a universal linear scaling with its average ⟨lnGT⟩, independent of Fermi energy, temperature, and system size in both 1D and 2D cases. In 2D, the competition between disorder-enhanced density of states at the NM/FI interface and disorder-suppressed spin transport leads to a non-monotonic dependence of average spin conductance on the disorder strength. As a result, in the metallic regime, average spin conductance is enhanced by disorder, and a new linear scaling between spin conductance fluctuation rms(GT) and average spin conductance GT is revealed which is universal at large system width. These universal scaling behaviors suggest that spin transport mediated by magnon in disordered 2D NM/FI systems belongs to a new universality class, different from that of charge conductance in 2D normal metal systems.
P. Umbach C., Washburn S., B. Laibowitz R., A. Webb R.. Magnetoresistance of small, quasi-one-dimensional, normal-metal rings and lines. Phys. Rev. B, 1984, 30(7): 4048 https://doi.org/10.1103/PhysRevB.30.4048
L. Altshuler B.. Fluctuations in the extrinsic conductivity of disordered conductors. JETP Lett., 1985, 41: 648
4
A. Lee P., D. Stone A., Fukuyama H.. Universal conductance fluctuations in metals: Effects of finite temperature, interactions, and magnetic field. Phys. Rev. B, 1987, 35(3): 1039 https://doi.org/10.1103/PhysRevB.35.1039
5
Qiao Z., Xing Y., Wang J.. Universal conductance fluctuation of mesoscopic systems in the metal-insulator crossover regime. Phys. Rev. B, 2010, 81(8): 085114 https://doi.org/10.1103/PhysRevB.81.085114
6
Zhang L., Zhuang J., Xing Y., Li J., Wang J., Guo H.. Universal transport properties of three-dimensional topological insulator nanowires. Phys. Rev. B, 2014, 89(24): 245107 https://doi.org/10.1103/PhysRevB.89.245107
Abrahams E., W. Anderson P., C. Licciardello D., V. Ramakrishnan T.. Scaling theory of localization: Absence of quantum diffusion in two dimensions. Phys. Rev. Lett., 1979, 42(10): 673 https://doi.org/10.1103/PhysRevLett.42.673
14
W. Anderson P., J. Thouless D., Abrahams E., S. Fisher D.. New method for a scaling theory of localization. Phys. Rev. B, 1980, 22(8): 3519 https://doi.org/10.1103/PhysRevB.22.3519
15
A. Müller C.Delande D., Disorder and interference: Localization phenomena, arXiv: 1005.0915 (2010)
16
Shapiro B., in: Percolation Structures and Processes, edited by G. Deutscher, R. Zallen, and J. Adler, Ann. Isr. Phys. Soc. 5, 367 (1983)
17
Shapiro B.. Scaling properties of probability distributions in disordered systems. Philos. Mag. B, 1987, 56: 1031
18
MacKinnon A., Kramer B.. One-parameter scaling of localization length and conductance in disordered systems. Phys. Rev. Lett., 1981, 47(21): 1546 https://doi.org/10.1103/PhysRevLett.47.1546
19
MacKinnon A., Kramer B.. The scaling theory of electrons in disordered solids: Additional numerical results. Z. Phys. B, 1983, 53(1): 1 https://doi.org/10.1007/BF01578242
20
Prior J., M. Somoza A., Ortuno M.. Conductance fluctuations and single-parameter scaling in two-dimensional disordered systems. Phys. Rev. B, 2005, 72(2): 024206 https://doi.org/10.1103/PhysRevB.72.024206
21
La Magna A., Deretzis I., Forte G., Pucci R.. Violation of the single-parameter scaling hypothesis in disordered graphene nanoribbons. Phys. Rev. B, 2008, 78(15): 153405 https://doi.org/10.1103/PhysRevB.78.153405
22
La Magna A., Deretzis I., Forte G., Pucci R.. Conductance distribution in doped and defected graphene nanoribbons. Phys. Rev. B, 2009, 80(19): 195413 https://doi.org/10.1103/PhysRevB.80.195413
23
N. Dorokhov O.. Transmission coefficient and the localization length of an electron in N bond disorder chains. JETP Lett., 1982, 36: 318
Plerou V., Q. Wang Z.. Conductances, conductance fluctuations, and level statistics on the surface of multilayer quantum Hall states. Phys. Rev. B, 1998, 58(4): 1967 https://doi.org/10.1103/PhysRevB.58.1967
26
A. Muttalib K., Wolfle P.. “One-sided” log-normal distribution of conductances for a disordered quantum wire. Phys. Rev. Lett., 1999, 83(15): 3013 https://doi.org/10.1103/PhysRevLett.83.3013
I. Deych L., A. Lisyansky A., L. Altshuler B.. Single parameter scaling in one-dimensional localization revisited. Phys. Rev. Lett., 2000, 84(12): 2678 https://doi.org/10.1103/PhysRevLett.84.2678
29
García-Martín A., J. Saenz J.. Universal conductance distributions in the crossover between diffusive and localization regimes. Phys. Rev. Lett., 2001, 87(11): 116603 https://doi.org/10.1103/PhysRevLett.87.116603
30
Schreiber M., Ottomeier M.. Localization of electronic states in 2D disordered systems. J. Phys.: Condens. Matter, 1992, 4(8): 1959 https://doi.org/10.1088/0953-8984/4/8/011
31
M. Somoza A., Ortuno M., Prior J.. Universal distribution functions in two-dimensional localized systems. Phys. Rev. Lett., 2007, 99(11): 116602 https://doi.org/10.1103/PhysRevLett.99.116602
32
M. Somoza A., Prior J., Ortuno M., V. Lerner I.. Crossover from diffusive to strongly localized regime in two-dimensional systems. Phys. Rev. B, 2009, 80(21): 212201 https://doi.org/10.1103/PhysRevB.80.212201
33
W. Kantelhardt J., Bunde A.. Sublocalization, superlocalization, and violation of standard single-parameter scaling in the Anderson model. Phys. Rev. B, 2002, 66(3): 035118 https://doi.org/10.1103/PhysRevB.66.035118
34
L. A. Queiroz S.. Failure of single-parameter scaling of wave functions in Anderson localization. Phys. Rev. B, 2002, 66(19): 195113 https://doi.org/10.1103/PhysRevB.66.195113
35
In Ref. [20], lnR is used instead of lnG. Note the resistence R is the inverse of conductance G, then we have ⟨ln G ⟩ = −⟨ln R⟩ thus the same result is obtained
Tserkovnyak Y., Brataas A., E. W. Bauer G.. Spin pumping and magnetization dynamics in metallic multilayers. Phys. Rev. B, 2002, 66(22): 224403 https://doi.org/10.1103/PhysRevB.66.224403
38
Tserkovnyak Y., Brataas A., E. W. Bauer G., I. Halperin B.. Nonlocal magnetization dynamics in ferromagnetic heterostructures. Rev. Mod. Phys., 2005, 77(4): 1375 https://doi.org/10.1103/RevModPhys.77.1375
39
Azevedo A., H. V. Leão L., L. Rodriguez-Suarez R., B. Oliveira A., M. Rezende S.. dc effect in ferromagnetic resonance: Evidence of the spin-pumping effect?. J. Appl. Phys., 2005, 97: 10C715 https://doi.org/10.1063/1.1855251
40
Saitoh E., Ueda M., Miyajima H., Tatara G.. Conversion of spin current into charge current at room temperature: Inverse spin-Hall effect. Appl. Phys. Lett., 2006, 88(18): 182509 https://doi.org/10.1063/1.2199473
41
Uchida K., Takahashi S., Harii K., Ieda J., Koshibae W., Ando K., Maekawa S., Saitoh E.. Observation of the spin Seebeck effect. Nature, 2008, 455(7214): 778 https://doi.org/10.1038/nature07321
42
Uchida K., Xiao J., Adachi H., Ohe J., Takahashi S., Ieda J., Ota T., Kajiwara Y., Umezawa H., Kawai H., E. W. Bauer G., Maekawa S., Saitoh E.. Spin Seebeck insulator. Nat. Mater., 2010, 9(11): 894 https://doi.org/10.1038/nmat2856
M. Tang G., B. Chen X., Ren J., Wang J.. Rectifying full-counting statistics in a spin Seebeck engine. Phys. Rev. B, 2018, 97(8): 081407 https://doi.org/10.1103/PhysRevB.97.081407
46
Wu H., Huang L., Fang C., S. Yang B., H. Wan C., Q. Yu G., F. Feng J., X. Wei H., F. Han X.. Magnon valve effect between two magnetic insulators. Phys. Rev. Lett., 2018, 120(9): 097205 https://doi.org/10.1103/PhysRevLett.120.097205
F. Jakobsen M., Qaiumzadeh A., Brataas A.. Scattering theory of transport through disordered magnets. Phys. Rev. B, 2019, 100(13): 134431 https://doi.org/10.1103/PhysRevB.100.134431
49
Yang L., Gu Y., Chen L., Zhou K., Fu Q., Wang W., Li L., Yan C., Li H., Liang L., Li Z., Pu Y., Du Y., Liu R.. Absence of spin transport in amorphous YIG evidenced by nonlocal spin transport experiments. Phys. Rev. B, 2021, 104(14): 144415 https://doi.org/10.1103/PhysRevB.104.144415
50
Li G., Jin H., Wei Y., Wang J.. Giant effective electron−magnon coupling in a nonmagnetic metal–ferromagnetic insulator heterostructure. Phys. Rev. B, 2022, 106(20): 205303 https://doi.org/10.1103/PhysRevB.106.205303
51
S. Wang J., K. Agarwalla B., Li H., Thingna J.. Nonequilibrium Green’s function method for quantum thermal transport. Front. Phys., 2014, 9(6): 673 https://doi.org/10.1007/s11467-013-0340-x
52
Zhang C., Xu F., Wang J.. Full counting statistics of phonon transport in disordered systems. Front. Phys., 2021, 16(3): 33502 https://doi.org/10.1007/s11467-020-1027-8
53
Z. Yu Z.H. Xiong G.F. Zhang L., A brief review of thermal transport in mesoscopic systems from nonequilibrium Green’s function approach, Front. Phys. 16(4), 43201 (2021)
54
S. Wang J., Peng J., Q. Zhang Z., M. Zhang Y., Zhu T.. Transport in electron–photon systems. Front. Phys., 2023, 18(4): 43602 https://doi.org/10.1007/s11467-023-1260-z
55
Holstein T., Primakoff H.. Field dependence of the intrinsic domain magnetization of a ferromagnet. Phys. Rev., 1940, 58(12): 1098 https://doi.org/10.1103/PhysRev.58.1098
56
S. Zheng J., Bender S., Armaitis J., E. Troncoso R., A. Duine R.. Green’s function formalism for spin transport in metal−insulator−metal heterostructures. Phys. Rev. B, 2017, 96(17): 174422 https://doi.org/10.1103/PhysRevB.96.174422
57
Ren J.. Predicted rectification and negative differential spin Seebeck effect at magnetic interfaces. Phys. Rev. B, 2013, 88(22): 220406 https://doi.org/10.1103/PhysRevB.88.220406
Datta S., Electronic Transport in Mesoscopic Systems, Cambridge University Press, New York, 1995, Chapter 3
60
I. Melnikov V., Fluctuations in the resistivity of a finite disordered system, Fiz. Tverd. Tela (Leningrad) 23, 782 (1981) [Sov. Phys. Solid State 23, 444 (1981)]
Ren W., Wang J., S. Ma Z.. Conductance fluctuations and higher order moments of a disordered carbon nanotube. Phys. Rev. B, 2005, 72(19): 195407 https://doi.org/10.1103/PhysRevB.72.195407
64
When calculating spin conductance for one specific disorder sample, one has to perform a double integration [see Eq. (13)]. In the calculation, we have chosen grid points 100 × 100 which amounts to an increase of computational cost by the factor of 10000 comparing with the charge conductance calculation in normal metal systems
65
The Fermi energies used in scaling analysis (Fig.5 and Fig.6) are near the center of the first subband. This is the region where SPS works in normal metal system [20]. Although the ranges of Fermi energies and temperatures are not very wide, the spin conductance in Fig.5(a) varies large enough in magnitude to support our scaling analysis.
66
Mohanty P., A. Webb R.. Anomalous conductance distribution in quasi-one-dimensional gold wires: Possible violation of the one-parameter scaling hypothesis. Phys. Rev. Lett., 2002, 88: 146601 https://doi.org/10.1103/PhysRevLett.88.146601
67
M. Somoza A., Prior J., Ortuño M.. Conductance fluctuations in the localized regime: Numerical study in disordered noninteracting systems. Phys. Rev. B, 2006, 73: 184201 https://doi.org/10.1103/PhysRevB.73.184201