High magnetic-field evolution of the in-plane angular magnetoresistance of electron-doped Sr1-xLaxCuO2 in the normal state
Abstract
We studied the in-plane angular magnetoresistance (AMR), in the normal state, of underdoped superconducting Sr1-xLaxCuO2, which has the simplest crystal structure among cuprates. The measurements of two underdoped thin films with different dopings were performed in intense magnetic field H (up to 22 T). The longitudinal magnetoresistance at temperature T is negative and scales with HIT. For both samples, the AMR is anisotropic and shows an unexpected dependence on H intensity. While at the low magnetic field, one observes essentially twofold AMR oscillations for the more doped sample, fourfold ones start to grow under the high magnetic field, resulting in the coexistence of the two. For the less doped film at the low magnetic field, both twofold and fourfold AMR components exist. With the increase of the magnetic field, the fourfold component survives a pi/4 phase shift, during which its amplitude vanishes, at a magnetic field such as 16 T lt H-c lt 17 T. As a result, at the high m...agnetic field above H-c, the angular dependence of the in-plane magnetoresistance turns out to be the same for both samples. We tentatively ascribe the above features to the presence of antiferromagnetism in the CuO2 planes of underdoped Sr1-xLaxCuO2.
Keywords:
superconductors / electron-doped cuprate / epitaxial thin films / magnetotransport / high magnetic fieldsSource:
Physical Review B, 2021, 103, 1Publisher:
- Amer Physical Soc, College Pk
Funding / projects:
DOI: 10.1103/PhysRevB.103.014520
ISSN: 2469-9950
WoS: 000612136200005
Scopus: 2-s2.0-85100140623
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Institut za multidisciplinarna istraživanjaTY - JOUR AU - Jovanović, Vladimir AU - Raffy, H. AU - Li, Z. Z. AU - Remenyi, G. AU - Monceau, P. PY - 2021 UR - http://rimsi.imsi.bg.ac.rs/handle/123456789/1442 AB - We studied the in-plane angular magnetoresistance (AMR), in the normal state, of underdoped superconducting Sr1-xLaxCuO2, which has the simplest crystal structure among cuprates. The measurements of two underdoped thin films with different dopings were performed in intense magnetic field H (up to 22 T). The longitudinal magnetoresistance at temperature T is negative and scales with HIT. For both samples, the AMR is anisotropic and shows an unexpected dependence on H intensity. While at the low magnetic field, one observes essentially twofold AMR oscillations for the more doped sample, fourfold ones start to grow under the high magnetic field, resulting in the coexistence of the two. For the less doped film at the low magnetic field, both twofold and fourfold AMR components exist. With the increase of the magnetic field, the fourfold component survives a pi/4 phase shift, during which its amplitude vanishes, at a magnetic field such as 16 T lt H-c lt 17 T. As a result, at the high magnetic field above H-c, the angular dependence of the in-plane magnetoresistance turns out to be the same for both samples. We tentatively ascribe the above features to the presence of antiferromagnetism in the CuO2 planes of underdoped Sr1-xLaxCuO2. PB - Amer Physical Soc, College Pk T2 - Physical Review B T1 - High magnetic-field evolution of the in-plane angular magnetoresistance of electron-doped Sr1-xLaxCuO2 in the normal state IS - 1 VL - 103 DO - 10.1103/PhysRevB.103.014520 ER -
@article{ author = "Jovanović, Vladimir and Raffy, H. and Li, Z. Z. and Remenyi, G. and Monceau, P.", year = "2021", abstract = "We studied the in-plane angular magnetoresistance (AMR), in the normal state, of underdoped superconducting Sr1-xLaxCuO2, which has the simplest crystal structure among cuprates. The measurements of two underdoped thin films with different dopings were performed in intense magnetic field H (up to 22 T). The longitudinal magnetoresistance at temperature T is negative and scales with HIT. For both samples, the AMR is anisotropic and shows an unexpected dependence on H intensity. While at the low magnetic field, one observes essentially twofold AMR oscillations for the more doped sample, fourfold ones start to grow under the high magnetic field, resulting in the coexistence of the two. For the less doped film at the low magnetic field, both twofold and fourfold AMR components exist. With the increase of the magnetic field, the fourfold component survives a pi/4 phase shift, during which its amplitude vanishes, at a magnetic field such as 16 T lt H-c lt 17 T. As a result, at the high magnetic field above H-c, the angular dependence of the in-plane magnetoresistance turns out to be the same for both samples. We tentatively ascribe the above features to the presence of antiferromagnetism in the CuO2 planes of underdoped Sr1-xLaxCuO2.", publisher = "Amer Physical Soc, College Pk", journal = "Physical Review B", title = "High magnetic-field evolution of the in-plane angular magnetoresistance of electron-doped Sr1-xLaxCuO2 in the normal state", number = "1", volume = "103", doi = "10.1103/PhysRevB.103.014520" }
Jovanović, V., Raffy, H., Li, Z. Z., Remenyi, G.,& Monceau, P.. (2021). High magnetic-field evolution of the in-plane angular magnetoresistance of electron-doped Sr1-xLaxCuO2 in the normal state. in Physical Review B Amer Physical Soc, College Pk., 103(1). https://doi.org/10.1103/PhysRevB.103.014520
Jovanović V, Raffy H, Li ZZ, Remenyi G, Monceau P. High magnetic-field evolution of the in-plane angular magnetoresistance of electron-doped Sr1-xLaxCuO2 in the normal state. in Physical Review B. 2021;103(1). doi:10.1103/PhysRevB.103.014520 .
Jovanović, Vladimir, Raffy, H., Li, Z. Z., Remenyi, G., Monceau, P., "High magnetic-field evolution of the in-plane angular magnetoresistance of electron-doped Sr1-xLaxCuO2 in the normal state" in Physical Review B, 103, no. 1 (2021), https://doi.org/10.1103/PhysRevB.103.014520 . .