J.C. Zapata , Yeonkyu Lee , Jeehoon Kim , N. Haberkorn
{"title":"金属帽外延NbN薄膜的涡临界速度","authors":"J.C. Zapata , Yeonkyu Lee , Jeehoon Kim , N. Haberkorn","doi":"10.1016/j.tsf.2025.140710","DOIUrl":null,"url":null,"abstract":"<div><div>We report the impact of proximity effects induced by different capping layers on the vortex dynamics and Larkin-Ovchinnikov instability in epitaxial NbN thin films. Bilayers consisting of 5 nm and 10 nm thick NbN were combined with capping layers of magnetic 5 nm thick Fe<sub>0.2</sub>Ni<sub>0.8</sub> and non-magnetic 5 nm thick Al and 10 nm thick Pt. The critical temperature (<em>T<sub>c</sub></em>), which is approximately 16 K in pure samples, decreases due to the influence of the capping layers. This reduction is more pronounced for Fe<sub>0.2</sub>Ni<sub>0.8</sub>, where <em>T<sub>c</sub></em> is fully suppressed for 5 nm thick NbN and decreases to 10.1 K for 10 nm thick films. Additionally, <em>T<sub>c</sub></em> is restored when an ultrathin AlN insulating layer is introduced, preventing electronic interaction. In contrast, Al and Pt capping layers also reduce <em>T<sub>c</sub></em>, but to a lesser extent compared to magnetic layers. By performing current-voltage curves, we determined the vortex critical velocities as a function of the magnetic field. Initially, the velocities start at approximately 6 km/s at low fields, subsequently decreasing to values between 1.8–2.8 km/s at fields around 1 T While a negligible impact is observed at low fields, the velocities at moderate and high fields tend to increase near <em>T<sub>c</sub></em> for non-magnetic capping layers. These increases (approximately 20 %) may be attributed to changes in the quasiparticle relaxation time, likely due to phonon escape contributions, as well as modifications in the electron diffusion coefficient and heat dissipation to local heating generated by inhomogeneities. Comparatively, the impact of capping layers is significantly smaller than previously reported for NbN and other disordered superconductors, where the initial vortex velocities in pure films were much lower than those observed in the films used in this study.</div></div>","PeriodicalId":23182,"journal":{"name":"Thin Solid Films","volume":"824 ","pages":"Article 140710"},"PeriodicalIF":2.0000,"publicationDate":"2025-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Vortex critical velocities in metallic-capped epitaxial NbN thin films\",\"authors\":\"J.C. Zapata , Yeonkyu Lee , Jeehoon Kim , N. Haberkorn\",\"doi\":\"10.1016/j.tsf.2025.140710\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>We report the impact of proximity effects induced by different capping layers on the vortex dynamics and Larkin-Ovchinnikov instability in epitaxial NbN thin films. Bilayers consisting of 5 nm and 10 nm thick NbN were combined with capping layers of magnetic 5 nm thick Fe<sub>0.2</sub>Ni<sub>0.8</sub> and non-magnetic 5 nm thick Al and 10 nm thick Pt. The critical temperature (<em>T<sub>c</sub></em>), which is approximately 16 K in pure samples, decreases due to the influence of the capping layers. This reduction is more pronounced for Fe<sub>0.2</sub>Ni<sub>0.8</sub>, where <em>T<sub>c</sub></em> is fully suppressed for 5 nm thick NbN and decreases to 10.1 K for 10 nm thick films. Additionally, <em>T<sub>c</sub></em> is restored when an ultrathin AlN insulating layer is introduced, preventing electronic interaction. In contrast, Al and Pt capping layers also reduce <em>T<sub>c</sub></em>, but to a lesser extent compared to magnetic layers. By performing current-voltage curves, we determined the vortex critical velocities as a function of the magnetic field. Initially, the velocities start at approximately 6 km/s at low fields, subsequently decreasing to values between 1.8–2.8 km/s at fields around 1 T While a negligible impact is observed at low fields, the velocities at moderate and high fields tend to increase near <em>T<sub>c</sub></em> for non-magnetic capping layers. These increases (approximately 20 %) may be attributed to changes in the quasiparticle relaxation time, likely due to phonon escape contributions, as well as modifications in the electron diffusion coefficient and heat dissipation to local heating generated by inhomogeneities. Comparatively, the impact of capping layers is significantly smaller than previously reported for NbN and other disordered superconductors, where the initial vortex velocities in pure films were much lower than those observed in the films used in this study.</div></div>\",\"PeriodicalId\":23182,\"journal\":{\"name\":\"Thin Solid Films\",\"volume\":\"824 \",\"pages\":\"Article 140710\"},\"PeriodicalIF\":2.0000,\"publicationDate\":\"2025-06-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Thin Solid Films\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0040609025001105\",\"RegionNum\":4,\"RegionCategory\":\"材料科学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"MATERIALS SCIENCE, COATINGS & FILMS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Thin Solid Films","FirstCategoryId":"88","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0040609025001105","RegionNum":4,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"MATERIALS SCIENCE, COATINGS & FILMS","Score":null,"Total":0}
Vortex critical velocities in metallic-capped epitaxial NbN thin films
We report the impact of proximity effects induced by different capping layers on the vortex dynamics and Larkin-Ovchinnikov instability in epitaxial NbN thin films. Bilayers consisting of 5 nm and 10 nm thick NbN were combined with capping layers of magnetic 5 nm thick Fe0.2Ni0.8 and non-magnetic 5 nm thick Al and 10 nm thick Pt. The critical temperature (Tc), which is approximately 16 K in pure samples, decreases due to the influence of the capping layers. This reduction is more pronounced for Fe0.2Ni0.8, where Tc is fully suppressed for 5 nm thick NbN and decreases to 10.1 K for 10 nm thick films. Additionally, Tc is restored when an ultrathin AlN insulating layer is introduced, preventing electronic interaction. In contrast, Al and Pt capping layers also reduce Tc, but to a lesser extent compared to magnetic layers. By performing current-voltage curves, we determined the vortex critical velocities as a function of the magnetic field. Initially, the velocities start at approximately 6 km/s at low fields, subsequently decreasing to values between 1.8–2.8 km/s at fields around 1 T While a negligible impact is observed at low fields, the velocities at moderate and high fields tend to increase near Tc for non-magnetic capping layers. These increases (approximately 20 %) may be attributed to changes in the quasiparticle relaxation time, likely due to phonon escape contributions, as well as modifications in the electron diffusion coefficient and heat dissipation to local heating generated by inhomogeneities. Comparatively, the impact of capping layers is significantly smaller than previously reported for NbN and other disordered superconductors, where the initial vortex velocities in pure films were much lower than those observed in the films used in this study.
期刊介绍:
Thin Solid Films is an international journal which serves scientists and engineers working in the fields of thin-film synthesis, characterization, and applications. The field of thin films, which can be defined as the confluence of materials science, surface science, and applied physics, has become an identifiable unified discipline of scientific endeavor.