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Localization and interaction effects in strongly underdoped La2-xSrxCuO4
Marta Z Cieplak1, A Malinowski, S Guha
1Institute of Physics, Polish Academy of Sciences, 02 668 Warsaw, Poland.
Physical Review Letters
|June 1, 2004
Summary
Magnetoresistance in lanthanum strontium copper oxide films reveals interaction effects at high temperatures and spin scattering at low temperatures. Superconducting fluctuations appear near the antiferromagnetic phase boundary.
Area of Science:
- Condensed Matter Physics
- Materials Science
- Superconductivity
Background:
- Investigating the electronic properties of La(2-x)Sr(x)CuO4 (LSCO) films is crucial for understanding high-temperature superconductivity.
- The interplay between magnetic ordering and electronic transport in LSCO remains a key area of research.
Purpose of the Study:
- To study the in-plane magnetoresistance (MR) of LSCO films with specific doping levels (0.03 < x < 0.05).
- To elucidate the temperature-dependent evolution of electronic transport mechanisms in LSCO.
- To explore the relationship between magnetic phases and superconducting fluctuations.
Main Methods:
- Measurements of in-plane magnetoresistance (MR) were performed on La(2-x)Sr(x)CuO4 films.
- Experiments were conducted over a temperature range of 1.6 K to 100 K.
- Magnetic fields up to 14 T were applied parallel and perpendicular to the CuO2 planes.
Main Results:
- Magnetoresistance behavior indicates a transition from interaction-dominated effects at high temperatures to spin scattering-dominated effects at low temperatures.
- Weak localization effects were found to be absent in the studied samples.
- A positive orbital magnetoresistance was observed near the antiferromagnetic and spin-glass phase boundary.
Conclusions:
- The findings suggest a gradual shift in dominant scattering mechanisms with decreasing temperature.
- The emergence of orbital MR near magnetic phase boundaries points to complex electronic behavior.
- Evidence for Maki-Thompson superconducting fluctuations was found deep within the insulating phase of LSCO.