1.Interface/Boundary Characterization Using Transmission Electron Microscopy

TEM analysis is an importance technique for determining composition and bonding status at surface/interface/boundary areas. It can deliver an atomic number sensitive Z-contrast image by scanning the electron probe on a single atomic column by a single atomic column. In addition, TEM provides us with the information on chemical species and atom sites inside a nanoscaled structure. By combining them with theoretical modeling and structural simulation, it is possible to exactly know crystallographic, chemical and position information at the nano scale.

  • Conventional Transmission Electron Microscopy (CTEM) for Microstructure, Morphology, Phase Distribution and Defect Analysis.
  • High Resolution Transmission Electron Microscopy (HRTEM), Scanning Transmission Electron Microscopy (STEM) and High Angle Annular Dark Field (HAADF)-STEM
  • Analytical TEM, such as Energy-dispersive X-ray Spectroscopy (EDS), Electron Energy Loss Spectroscopy (EELS), and Energy Filter TEM (EFTEM)

 

 

2.Negative stainning, Cryo-electron Microscopy and 3D-Tomography Techniques

A.Negative stainning


nanotungsten stainnning image of one protein

B.Cryo-electron Microscopy


Cryo image of one virus

C.Electron tomography is a new imaging technology, which employs TEM to collect projections of an object and uses these projections to reconstruct the object.


From W. Baumeister et al. Trend in Cell Biology 9(1999)81

 

3.Protein purification and 3D crystal growth

A.We try to use 4 columns ( two Ni-columns, one Q-coulmn, and one super200 column) to purify one membrance proteins by FPLC.

B.3D crystal


3D crystal image of one membrane protein

 

 

 

 

image gallery

 

1. Epitaxial SrRuO3/Ba0.7Sr0.3TiO3/SrRuO3 thin film capacitors were prepared on SrTiO3 substrates by pulsed laser deposition. The structures of stacked BST films with different thicknesses were investigated by transmission electron microscopy. A distinctive layer of about 3 nm of thickness was identified within BST films thicker than 9 nm at the interface with the SrRuO3 bottom electrode. The distinctive layer is misfit dislocation-free showing pseudoconstant lattice parameters. Misfit dislocations are formed at the interface between the distinctive layer and the BST film bulk layer relaxing the latter as the film thickness increases. The effect of the distinctive layer on the system dielectric response is discussed within the framework of an interfacial dead-layer model.

J.Q.HE et al.

Appl. Phys. Lett. 87 (2005) 062901



2.At the SrRuO3/LaAlO3 interface a type of dissociated superdislocations in connection with Ruddlesen-Popper type planar defects is found. The dissociated superdislocations involving a (001) RP-defect, {111} stacking faults and their accompanied partial dislocations can contribute to the relaxation of misfit stresses.

Vasco et al.

Adv. Mater. 17 (2005), 281



3.The SrTiO3 /Si interface was investigated by transmission electron microscopy for SrTiO3 films grown on s001d Si by molecular-beam epitaxy with different native oxide sSiO2d removal treatments, and Sr/Ti flux ratios. The interface and film microstructure were independent of the process used to remove the native oxide, but the interface reactivity was dependent on the Sr/Ti flux ratio. A low Sr/Ti flux ratio s,0.8d resulted not only in a layer of amorphous material at the film/substrate interface but also in the formation of crystalline C49 TiSi2 precipitates at that interface. These results are consistent with thermodynamic expectations in which it is paramount to maintain separation between TiO2 and the underlying silicon.

J.Q. HE et al.

J. Appl. Phys. 97 (2005), 104921.



4.The microstructure and the interfaces of HfO2 ?lms deposited by metal-organic chemical vapor deposition directly on silicon (0 0 1) substrates were investigated by means of transmission electron microscopy. For two different precursors, Hf(O-i-but)2(mmp)2 and Hf(diethyl-amide)4, electron diffraction analysis showed a gradual transformation from the amorphous phase to the monoclinic phase in the deposition temperature range of 350¨C600C. At an intermediate substrate temperature, 550C, a small amount of tetragonal second phase was additionally observed. For the two types of precursors, the thickness of the interfacial amorphous layer was found to depend on the deposition temperature and showed a major decrease along with the amorphous to crystalline transition of the ?lms. The in?uence of the substrate surface preparation and of post deposition annealing on the thickness of the interfacial layer is also discussed.

J.Q. HE et al.

J. cryst.growth 262 (2004), 295



5.Perovskite La0.7Ca0.3MnO3 (LCMO) thin ?lms were grown epitaxially on SrTiO3 (STO) and NdGaO3 (NGO) substrates by pulsed laser deposition. The microstructure of these ?lms was investigated by means of high-resolution and Bragg-diffraction contrast transmission electron microscopy. Due to the small lattice mismatch in the system of LCMO/NGO, the ?lms showed a higher structural perfection than the ?lms on STO substrates. Mis?t dislocations were not detected over large areas in the LCMO ?lm grown on NGO. In contrast, two types of mis?t dislocations with Burgers vectors a/0 10S and a/110S were frequently observed at the LCMO/STO interface. MnO precipitates were identi?ed in the LCMO ?lms by combining energy-dispersive X-ray spectroscopy with electron diffraction analysis. The MnO precipitates were usually formed in the ?lm away from the film/substrate interface. Their size and density increased with the film thickness.

J.Q. HE et al.

J. cryst.growth 265 (2004), 241



CED-4

J.Q. HE et al.

In Preparation

 

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