journal article·2020-07-01Open access

Concomitance of superconducting spin–orbit scattering length and normal state spin diffusion length in W on (Bi,Sb)2Te3

Yong-Chang Lau, Ryota Akiyama, Hishiro T Hirose, Ryosuke Nakanishi, Taichi Terashima, Shinya Uji, Shuji Hasegawa, Masamitsu Hayashi

Journal of Physics: Materials· Volume 3· Issue 3

Abstract

Abstract We report the observation of an anomalously large in-plane upper critical field, exceeding at least 2.5 times the Pauli paramagnetic limit, in a thin superconducting W film grown on a topological insulator (Bi,Sb)2Te3. This can be accounted for by setting the spin–orbit scattering length of superconducting W to a value ranging from 1 to 2 nm, which is comparable to the spin diffusion length of normal state W. The coupling between the topological surface states of (Bi,Sb)2Te3 and the wave functions of superconducting W may also contribute to the observed giant critical field. Our results suggest the universality of the spin–orbit scattering formalism for describing the transport involving the diffusive carriers as well as the Cooper pairs in systems with strong spin–orbit coupling.
Source: crossref · Quality: baseline

Research context

OpenAlex topics: Topological Materials and Phenomena · Physics of Superconductivity and Magnetism · Quantum and electron transport phenomena

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (60)

Show source-provided references
1. Superconductivity of tungsten10.1103/PhysRevLett.12.688 ↗
2. Superconductivity of tungsten10.1103/PhysRevLett.16.101 ↗
3. Superconductivity in β tungsten films10.1063/1.1656012 ↗
4. Focused-ion-beam-induced deposition of superconducting nanowires10.1063/1.1842367 ↗
5. Spin transfer torque devices utilizing the giant spin Hall effect of tungsten10.1063/1.4753947 ↗
6. Beta (β) tungsten thin films: structure, electron transport and giant spin Hall effect10.1063/1.4919867 ↗
7. Giant enhancement of the intrinsic spin Hall conductivity in beta-tungsten via substitutional doping10.1103/PhysRevB.96.241105 ↗
8. Correlation between the spin Hall angle and the structural phases of early 5d transition metals10.1063/1.4937452 ↗
9. Interface control of the magnetic chirality in CoFeB/MgO heterostructures with heavy-metal underlayers10.1038/ncomms5655 ↗
10. Spin Hall magnetoresistance induced by a nonequilibrium proximity effect10.1103/PhysRevLett.110.206601 ↗
11. Theory of spin Hall magnetoresistance10.1103/PhysRevB.87.144411 ↗
12. Observation of the spin Nernst effect10.1038/nmat4964 ↗
13. Direct detection of spin Nernst effect in platinum10.1063/1.5021731 ↗
14. Spin Hall magnetoresistance in metallic bilayers10.1103/PhysRevLett.116.097201 ↗
15. Large spin Hall magnetoresistance and its correlation to the spin–orbit torque in W/CoFeB/MgO structures10.1038/srep14668 ↗
16. The spin Nernst effect in tungsten10.1126/sciadv.1701503 ↗
17. Observation of transverse spin Nernst magnetoresistance induced by thermal spin current in ferromagnet/non-magnet bilayers10.1038/s41467-017-01493-5 ↗
18. Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface10.1038/nphys1270 ↗
19. Experimental realization of a three-dimensional topological insulator, Bi2Te310.1126/science.1173034 ↗
20. Observation of time-reversal-protected single-Dirac-cone topological-insulator states in Bi2Te3 and Sb2Te310.1103/PhysRevLett.103.146401 ↗
21. Band structure engineering in (Bi1−xSbx)2Te3 ternary topological insulators10.1038/ncomms1588 ↗
22. Superconducting proximity effect and Majorana fermions at the surface of a topological insulator10.1103/PhysRevLett.100.096407 ↗
23. Generic new platform for topological quantum computation using semiconductor heterostructures10.1103/PhysRevLett.104.040502 ↗
24. Search for Majorana fermions in superconductors10.1146/annurev-conmatphys-030212-184337 ↗
25. Topological superconductors: a review10.1088/1361-6633/aa6ac7 ↗
26. Chiral Majorana fermion modes in a quantum anomalous Hall insulator-superconductor structure10.1126/science.aag2792 ↗
27. Spectroscopic evidence of a topological quantum phase transition in ultrathin Bi2Se3 films10.1103/PhysRevB.81.165432 ↗
28. A method of measuring the resistivity and Hall coefficient on lamellae of arbitrary shape
29. Coll.: saturation of electrical resistivity10.1103/RevModPhys.75.1085 ↗
30. Tuning of tungsten thin film superconducting transition temperature for fabrication of photon number resolving detectors10.1109/TASC.2005.849033 ↗
31. Weak localization in thin films: a time-of-flight experiment with conduction electrons10.1016/0370-1573(84)90103-0 ↗
32. Electrically tunable surface-to-bulk coherent coupling in topological insulator thin films10.1103/PhysRevB.84.233101 ↗
33. Tinkham · 1996
34. Effect of fluxoid quantization on transitions of superconducting films10.1103/PhysRev.129.2413 ↗
35. Anisotropic superconductivity and dimensional crossover in (TMET−STF)2BF410.1103/PhysRevB.64.214517 ↗
36. Critical fields of W/Si multilayers10.1016/0921-4534(94)90722-6 ↗
37. Upper limit for the critical field in hard superconductors10.1103/PhysRevLett.9.266 ↗
38. A note on the maximum critical field of high field superconductors10.1063/1.1777362 ↗
39. Temperature and purity dependence of the superconducting critical field, Hc2. III. electron spin and spin–orbit effects10.1103/PhysRev.147.295 ↗
40. Theory of the upper critical field in layered superconductors10.1103/PhysRevB.12.877 ↗
41. Superconductivity and critical fields in amorphous tungsten/silicon multilayers10.1002/pssa.2211450235 ↗
42. Electrically tunable low-density superconductivity in a monolayer topological insulator10.1126/science.aar4642 ↗
43. Gate-induced superconductivity in a monolayer topological insulator10.1126/science.aar4426 ↗
44. Evidence for two-dimensional ising superconductivity in gated MoS210.1126/science.aab2277 ↗
45. Superconductivity protected by spin-valley locking in ion-gated MoS210.1038/nphys3580 ↗
46. Ising pairing in superconducting NbSe2 atomic layers10.1038/nphys3538 ↗
47. Spintronics: fundamentals and applications10.1103/RevModPhys.76.323 ↗
48. Experimental verification of comparability between spin–orbit and spin-diffusion lengths10.1103/PhysRevLett.110.016805 ↗
49. The electrical conductivity of transition metals10.1098/rspa.1936.0031 ↗
50. Effect of spin–orbit scattering on the upper critical field of high-field superconductors10.1103/PhysRevLett.17.81 ↗
51. Upper critical field limits for bulk type II superconductors10.1063/1.1754905 ↗
52. Upper and lower critical fields of TaS2(pyridine)1/210.1143/JPSJ.46.1112 ↗
53. Superconductivity at 6 K and the violation of Pauli limit in Ta2PdxS510.7566/JPSJ.83.023702 ↗
54. Strong-coupling superconductivity in V3X type of compounds10.1103/PhysRevLett.19.1039 ↗
55. Liu · 2011
56. Spin torque study of the spin Hall conductivity and spin diffusion length in platinum thin films with varying resistivity10.1103/PhysRevLett.116.126601 ↗
57. Spin–orbit torque switching without an external field using interlayer exchange coupling10.1038/nnano.2016.84 ↗
58. Anomalous spin Hall magnetoresistance in Pt/Co bilayers10.1063/1.5021510 ↗
59. Spin pumping and inverse spin Hall effect in platinum: The essential role of spin-memory loss at metallic interfaces10.1103/PhysRevLett.112.106602 ↗
60. All-electric magnetization switching and Dzyaloshinskii-Moriya interaction in WTe2/ferromagnet heterostructures10.1038/s41565-019-0525-8 ↗