Figure 1: A high-resolution cross-sectional
TEM image showing overgrowth of a 2212 superconductor film on
a SrTiO3 substrate (001) surface. The view is
along the (100) axis of the SrTiO3 substrate.
Registry between planes in the substrate and overlayer is
nearly perfect, resulting in a coherent interface. The BiO
planes are continuous throughout the image, even directly
above rough areas on the SrTiO3 surface.
Figure 2: A high-resolution cross-sectional
TEM image of a 2201/2212 superlattice. The view is along the
(001) axis of the SrTiO3 substrate. The
alternation of the 15.4 Å period of 2212 and the 12.3
Å period of 2201 is readily identifiable. Also shown
are image simulations of 2212 and 2201 which were calculated
using the known lattice constants of the materials.
Parameters for the simulations are focus = -450, thickness =
200Å.
Figure 3: Hypothetical crystal structure of
the Bi-2278. The c-axis lattice constant is 71.2 Å, so
the thickness of a single layer should be 35.6 Å. The
in-plane lattice constants are assumed to be the same as in
2212. The view is along the (001) axis. Shown for comparison
is the well-known crystal structure of the 2212 phase.
Figure 4: High-resolution cross-sectional
image of a 2278 barrier layer sandwiched between two thick
films of 2212. The view is along the (001) axis of the
SrTiO3 substrate.
Figure 5: High-resolution cross-sectional
image of a twinned section of a 2212 film. The layers on the
right-hand side of the image have the b-axis normal to the
plane of the figure and show incommensurate modulation.
Layers on the left-hand side have the a-axis normal to the
plane of the figure.
Figure 6: Stacking defects in a 2212 film
grown on SrTiO3 substrate. View is along the (001)
axis of the SrTiO3 substrate. The antiphase
boundary is indicated by a black arrow.
Figure 7: Low-resolution micrograph of a
BiSrCaCuO film with three barriers each consisting of a
single molecular layer of 2278, separated by thicker layers
of 2212. This image demonstrates the long lateral coherence
length which is typically observed in BiSrCaCuO-based
heterostructures grown by ALL-MBE.