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Oxide Heterostructure

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Presentation on theme: "Oxide Heterostructure"— Presentation transcript:

1 Oxide Heterostructure
Shuhua Liang UTK Physics Dept.

2 Perovskite Stucture ABO3

3 LCMO (magnetic material) La0.67Ca0.33MnO3

4 High Tc Superconductor Lattice
LSCO (High Tc Sc) (La1-xSrxCuO3 )

5 YBCO High Tc Sc YBa2Cu3O7-x CuO2 Plane More layers Higher Tc Distance
Carriers in CuO2 Plane

6 Metallic Interfaces between Insulators
LaTiO3 layers (bright) of varying thickness spaced by 5 layers of SrTiO3

7 LaTiO3 La 3+ one more e Ti 3+ Mott insulator A=0.397nm SrTiO3 Sr 2+ Ti 4+ Band insulator A=0.391nm

8 Charge leakage the Ti3+ signal is considerably wider than that of the La “Ti3+”~extra electron The ‘tail’ of Ti3+ have a decay length of 1nm as an order of screening length!

9 Metallic Structure Fraction of Ti3+ is a function of the number of LaTiO3 unit cells. Conductivity is a function of the thickness of LaTi3 and SrTi3

10 CMR Colossal magnetoresistance

11 LaMnO3

12 Double-exchange mechanism
Ca 2+ cause electron free to move.

13 Oxide heterostructure interface

14 Ferromagnetic/Sc oxide interface
Sc: YBa2Cu3O7-x FM: La0.67Ca0.33MnO3

15 interface

16 Electrons transfer

17 Thank you!


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