Contrast development in thin cryosections by electron beam exposure at low dose

Contrast development in thin cryosections by electron beam exposure at low dose

426 Abstracts of Tlle Netherlands Society of Electron Microscopy passed through the cabinet and led away into a laboratory fume cupboard. CONTP~.ST...

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426

Abstracts of Tlle Netherlands Society of Electron Microscopy

passed through the cabinet and led away into a laboratory fume cupboard.

CONTP~.ST DEVELOPMENT IN THIN C R Y O S E C T I O N S BY ELECTRON BEAM EXPOSURE AT LOW DOSE P. H. H. Bomans and P. M. F r e d ~ r i k P a t h o l o g y , U n i v e r s i t y o f LY nburg, P. 0. B o x 616, 6200 MC M a a s t r i c h t , The N e t h e r l a n d s

C r y o - e l e c t r o n microscopy of hydrated biological materials requires thin and vitrified specimens. For specimens that cannot be captured in thin films this implies that vitrified samples have to be sectioned on a cryo-ultramicrotome. Vitrification of pancreas samples was accomplished by infiltrating aldehyde-fixed samples in vitrifying concentrations of methanol (80%), propylene glycol (80%) or glycezol (67%). According to the theories of contrast formation there should be an increasing electron o p a c i t y from methanol through glycerol of these aqueous embeddings. In our low-dose pictures of cryo-sections from vitrified pancreas samples no contrast has been observed in the "virgin" exposures; c o n t r a s t developed gradually in consecutive exposures. This was confirmed for the three aqueous embeddings tested. In addition the development of contrast was m o n i t o r e d with a TV cameza with an image intensifier. The video images show an appearance o£ contrast at an electron dose o ~ ca. i000 e/nm 2 . The apparent anomaly in contrast of thin cryo-sections compared to thin vitrified films can only be explained by a larger contribution of m u l t i p l e - s c a t tered electrons to the image of cr,yosections. Our findings d e m o n s t r a t e a contrast-inducing effect of the electron beam, even at low dose conditions, on cryosections from infiltrated and vitrified pancreas samples.

HREM OF S T A C K I N G IRREGULARITIES CHLORITE CRYSTALS

IN

A. J. Bons and D. Schryvers* I n s t i t u u t voor A a r d w e t e n s c h a p p e n , Rijksuniversiteit Utrecht, Budapestlaan 4, U t r e c h t , The N e t h e r l a n d s ; *Rijksuniversitair Centrum Antwerpen, G r o e n e n b o r g e r l a a n 171, A n t w e r p , B e l g i u m

Chl>rite crystals from slate rocks have been studied by high resolution

electron m i c r o s c o p y . Chlorite is one of the most common phyllosilicates in natural rocks. The crystal structure is formed by a l t e r n a t i n g talc-like sheets, (Fe, Mg,AI)3(Si,AI)4OIo(OH) 2, and brucire-like sheets (Fe,Mg,AI) 3(OH) 6. (001)-lattice fringe images of chlorite (d=14~) are characterised by a strong variation in i n t e n s i t y of the individual fringes. D e v i a t i n g fringe s p a c i n g s (7~ and 9~) are also common. The n a t u r e of these irregularities has been i n v e s t i g a ted by HREM p e r f o r m e d on a t o p - e n t r y JEOL 200CX e l e c t r o n microscope at the University of A n t w e r p (RUCA). The v a r i a t i o n in intensity of the lattice fringes can be explained by irregular shifts of the crystal lattice of magnitude b/3 in d i r e c t i o n s parallel to (001). The H R E M images, combined with computer simulations, show that these shifts can take place at two levels in the unit cell: (i) at the centre of the talc sheet and (2) at the b r u c i t e sheet. The 9~ fringes arise from layers w h e r e the brucite sheet is missing. The 7~ fringes are caused by i n t e r c a l a t i o n s w i t h a kaolinite structure.

THE ANALYTICAL $EM AND STEM, AN INDISPENSABLE TOOL IN CERAMICS RESEARCH B. A. Boukamp, A. J. A. Winnubst, K. Keizer, K. J. de Vries and A. J. Burggraaf u n x v e r s i t y o f T w e n t e , P.O. B o x 219, 7500 A E E n s c h e d e , The N e t h e r l a n d s

The analytical scanning and (scanning) transmission e l e c t r o n microscopes are indispensable tools in the research field of advanced ceramics. The EMs are used for c h a r a c t e r i z a t i o n and analysi3 at the various stages in the sample p r e p a r a t i o n procedure and b e y o n d the final stage, in subsequent a n n e a l i n g and aging e x p e r i ments. In this presentation the involvement of EM a n a l y s i s in the ceramic materJals research p r o g r a m of our laboratory is discussed. In the d e v e l o p m e n t of tough ceramics based on tetragonal ZY, the EM is used for monitoring the (precursor) powder particle sizes (about i0 nm), the measurement of grain growth (<0.5 mu) during the sintering process and change in morphology due to aging experiments. (Un)w a n t e d second phase is c h a r a c t e £ i z e d with EDS. Microporous ceramic membranes consisting of one to three layers, with decreasing pore sizes, on top of a porous