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Physical Review Letters

Volumn 64, Issue 8, 1990, Pages 938-941

High-resolution incoherent imaging of crystals

(2) Pennycook, S J a Jesson, D E a

a OAK RIDGE NATIONAL LABORATORY (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 11944259078 PISSN: 00319007 EISSN: None Source Type: Journal
DOI: 10.1103/PhysRevLett.64.938 Document Type: Article

Times cited : (543)

References (25)

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10
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- For a review of previous applications, see M. M. J. Treacy and S. B. Rice, J. Microsc. (to be published);

11
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- Pennycock, Berger, and Culbertson, Ref. 7.

12
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- This is an overstringent requirement since the coherent component at high scattering angles also results in similar image characteristics, D. E. Jesson and S. J. Pennycook (to be published).

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18
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- Images are calculated for an objective-lens spherical-aberration coefficient Cs= 1.3 mm with optimum illumination angle, (4 λ / Cs)1/4, and defocus, - ( Csλ )1/2 (λ = 2 π / chi), using 1315 incident orientations. 63 and 91 beams were used at 100- and 300-kV accelerating voltage, respectively.

19
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- At high defocus values the probe shows strong subsidiary maxima which can result in reversed images, although showing much weaker contrast.

20
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21
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- The contrast was difficult to measure due to noise limitations, but appeared weaker than expected. This could be due to a number of effects including the neglect of the high-angle scattering from absorbed electrons, probe instabilities, or probe broadening in an amorphous surface layer.

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- The total coherently scattered intensity in the high-order Laue-zone reflections is less than 1% of the total intensity reaching the annular detector.

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25
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- In principle, this would also allow the possibility of energy-filtered incoherent images.

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.