Kinetically stable glassy phase formation in neodymium nickelate thin films as evidenced by Hall effect and electrical resistivity measurements
Source abstract
Abstract
In this study, we are reporting the time- and temperature-dependence of the electrical resistivity and temperature-dependence of the Hall voltage in neodymium nickelate thin films. The films were deposited on a lanthanum aluminate substrate [LaAlO3(001)] by a pulsed laser deposition technique, with thicknesses ranging from 0.6 to 120 nm. Time-dependent electrical transport measurements indicated the formation of a kinetically stable metallic glassy phase rather than a stable insulating phase on cooling below the transition temperature, TM-I. Comparisons of the low-temperature behavior with that of common insulators further supported this claim. Hall effect measurements on the 1.2-nm sample showed a local maximum in the carrier concentration just below the TM-Ion both the heating and cooling cycles. This again confirmed the proposed low-temperature structure, in that, for the 1.2-nm sample, there was a minimal degree of supercooling before transitioning to a kinetically stable glassy phase.
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Research context
OpenAlex topics: Metallic Glasses and Amorphous Alloys · Phase-change materials and chalcogenides · Theoretical and Computational Physics
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (28)
Show source-provided references
1. 10.1063/1.35811910.1063/1.358119 ↗
2. Theory of semiconductor-to-metal transitions
3. 10.1063/1.346719910.1063/1.3467199 ↗
4. 10.1103/PhysRevB.46.441410.1103/PhysRevB.46.4414 ↗
5. 10.1088/0953-8984/21/18/18540210.1088/0953-8984/21/18/185402 ↗
6. 10.1103/PhysRevB.61.440110.1103/PhysRevB.61.4401 ↗
7. 10.1016/S0921-4526(96)00862-910.1016/S0921-4526(96)00862-9 ↗
8. 10.1088/0953-8984/10/18/00710.1088/0953-8984/10/18/007 ↗
9. 10.1088/0953-8984/21/48/48540210.1088/0953-8984/21/48/485402 ↗
10. 10.1063/1.348139610.1063/1.3481396 ↗
11. 10.1051/rphysap:0198800230403670010.1051/rphysap:01988002304036700 ↗
12. 10.1063/1.37149610.1063/1.371496 ↗
13. 10.1002/adma.20100324110.1002/adma.201003241 ↗
14. 10.1103/PhysRevB.62.789210.1103/PhysRevB.62.7892 ↗
15. 10.1103/PhysRevB.46.1497510.1103/PhysRevB.46.14975 ↗
16. 10.1088/0953-8984/6/30/00910.1088/0953-8984/6/30/009 ↗
17. 10.1063/1.145198410.1063/1.1451984 ↗
18. 10.1103/PhysRevB.68.22040310.1103/PhysRevB.68.220403 ↗
19. 10.1016/0022-4596(89)90008-X10.1016/0022-4596(89)90008-X ↗
20. 10.1103/PhysRevB.45.820910.1103/PhysRevB.45.8209 ↗
21. 10.1103/PhysRevB.68.11340810.1103/PhysRevB.68.113408 ↗
22. 10.1103/PhysRevB.48.1166610.1103/PhysRevB.48.11666 ↗
23. 10.1016/j.ssc.2005.06.01510.1016/j.ssc.2005.06.015 ↗
24. 10.1063/1.345146210.1063/1.3451462 ↗
25. 10.1103/PhysRevB.71.04512810.1103/PhysRevB.71.045128 ↗
26. 10.1016/0022-0248(87)90031-510.1016/0022-0248(87)90031-5 ↗
27. Catalan · 2012 · 44
28. 10.1016/S0025-5408(01)00777-210.1016/S0025-5408(01)00777-2 ↗