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SRC Users' Meeting - Synchrotron Radiation Center - University of ...

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1<br />

1<br />

0.8<br />

0.8<br />

0.6<br />

0.6<br />

0.4<br />

0.4<br />

0.2<br />

0.2<br />

Ky<br />

0<br />

Ky<br />

0<br />

-0.2<br />

-0.2<br />

-0.4<br />

-0.4<br />

-0.6<br />

-0.6<br />

-0.8<br />

-0.8<br />

-1<br />

-1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1<br />

Kx<br />

-1<br />

-1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1<br />

Kx<br />

Figure 3a: Calculated Fermi Surface<br />

change with doping (band filling) <strong>of</strong> nonstrained<br />

LSCO, assuming an unchanged<br />

band shape, ie. identical to that <strong>of</strong> Fig 2<br />

left. From the outside to the inside,<br />

doping values are x = 0.05, 0.10, 0.15,<br />

0.22, and 0.30. Note that these simulated<br />

Fermi Surfaces are in excellent<br />

agreement with the experimentally<br />

measured ones by Ino et al. [Ino]<br />

Figure 3b: Calculated Fermi Surface<br />

change (band filling) <strong>of</strong> in-plane<br />

compressed LSCO films assuming an<br />

unchanged band shape, ie. identical to<br />

that <strong>of</strong> Fig 2 right. From the outside to<br />

the inside, doping values are x = 0.05,<br />

0.08, 0.15, 0.2, 0.3.<br />

References<br />

[Loquet]: J.P. Locquet et al., Nature 394, 453 (1998)<br />

[Ino]: A. Ino et al., PRB 65, 945041 (2002)<br />

[Abrecht]: M. Abrecht et al., PRL 91 570021 (2003); reference is attached.

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