journal article·2013-07-14

Kinetically stable glassy phase formation in neodymium nickelate thin films as evidenced by Hall effect and electrical resistivity measurements

Megan Campbell Prestgard, Ashutosh Tiwari

Journal of Materials Research· Volume 28· Issue 13
Publisher page

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.
Source: expertdata · Quality: candidate unverified · Source record ↗

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 ↗