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(a) Surface after heating (b) SEM view of zone III380 k jpeg |
Fig. 1: (a) Growth on the heated surface. (Binocular microscope image.) The heating has resulted in segregation in four zones. I: Drops of solidified boron. II: h-BN platelets. III (75 microns large ring): Thin BN nanotubes have grown self-assembled in ropes forming a crown perpendicular to the surface. The most developed part of the crown (up image) is close to a large boron drop in the hole (arrow). IV: The surface is covered by BN nano-polyhedrons. Diameter of the hole:0.55 mm. (b) SEM view of the crown-like material (corresponds to Fig. 1a, ring III, up image). Tangled BN ropes, as long as 40 microns, are mixed with BN nano-polyhedrons powders. Scale bar 10 microns. |
TEM imaging of BN tubes. |
Fig. 2: (a) Curl of a rope. A section of a rope, which is perpendicular to the electron beam, appears contrasted. It contains ~ 10 tubes. During the imaging, the rope is slightly vibrating due to the charging effect under the electron beam. Scale bar 10 nm. (b) Section image of a three-layer tube showing a circular section. Scale bar 2 nm. (c) Two-layer tube. Scale bar 2 nm. |
EELS Spectra |
Fig. 3: On a BN rope (beam focused to the diameter of the rope ~ 40 nm), the inelastic electron energy loss is very similar to that of (stoichiometric) h-BN. For a large (50 nm) BN nano-polyhedrons containing a boron nano-crystal (20 nm probe), the N/B ration is non-stoichiometric. Spectra have been background corrected, vertically expended to an equal N-K loss and vertically shifted of an arbitrary offset. |
BN onion of crystalline B core |
Fig. 4: TEM imaging of a BN nano-polyhedron containing a boron nano-crystal (direction 0001, hexagonal indexing). New layers of BN seem to be emerging from the boron lattice (arrow) in a recombination process. Scale bar 10 nm. |
To contact me: thomaslaudeABC@uminokai.net (Remove ABC, it is against spam.)
The material present here is copyrighted. Key-words: nanotechnology, science, nanotubes.
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