Effect of a physical phase plate on contrast transfer in an aberration-corrected transmission electron microscope

被引:16
作者
Gamm, B. [1 ]
Schultheiss, K. [1 ]
Gerthsen, D. [1 ]
Schroeder, R. R. [2 ]
机构
[1] Univ Karlsruhe TH, Lab Elekt Mikroskop, D-76128 Karlsruhe, Germany
[2] Max Planck Inst Biophys, D-60438 Frankfurt, Germany
关键词
transmission electron microscopy; phase plate; phase contrast; contrast transfer function; in-focus phase contrast;
D O I
10.1016/j.ultramic.2008.02.009
中图分类号
TH742 [显微镜];
学科分类号
摘要
In this theoretical study we analyze contrast transfer of weak-phase objects in a transmission electron microscope, which is equipped with an aberration corrector (C-s-corrector) in the imaging lens system and a physical phase plate in the back focal plane of the objective lens. For a phase shift of pi/2 between scattered and unscattered electrons induced by a physical phase plate, the sine-type phase contrast transfer function is converted into a cosine-type function. Optimal imaging conditions Could theoretically be achieved if the phase shifts caused by the objective lens defocus and lens aberrations would be equal to zero. In reality this situation is difficult to realize because of residual aberrations and varying, non-zero local defocus values, which in general result from an uneven sample surface topography. We explore the conditions-i.e. range of C-s-values and defocus-for most favourable contrast transfer as a function of the information limit, which is only limited by the effect of partial coherence of the electron wave in C-s-corrected transmission electron microscopes. Under highresolution operation conditions we find that a physical phase plate improves strongly low- and medium-resolution object contrast, while improving tolerance to defocus and C-s-variations, compared to a microscope without a phase plate. (c) 2008 Elsevier B.V. All rights reserved.
引用
收藏
页码:878 / 884
页数:7
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