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通过检查倾斜囊泡和自动最可能损失成像来测定冰中的非弹性平均自由程。

Determination of the inelastic mean free path in ice by examination of tilted vesicles and automated most probable loss imaging.

作者信息

Grimm R, Typke D, Bärmann M, Baumeister W

机构信息

Max-Planck-Institut für Biochemie, Martinsried, Germany.

出版信息

Ultramicroscopy. 1996 Jul;63(3-4):169-79. doi: 10.1016/0304-3991(96)00035-6.

Abstract

Using electron microscopy, the thickness of ice-embedded vesicles is estimated examining tilted and untilted views and assuming an ellipsoidal shape of the vesicles that appear to be circular in the untilted view. Another thickness measure is obtained from the ratio of the unfiltered and zero-loss-filtered image intensities of the vesicle. From these two measurements, the mean free path A for inelastic scattering of electrons in ice is calculated as 203 +/- 33 nm for 120 kV acceleration voltage. It is found that vesicles in thin ice films (< or = 1.5 lambda) significantly protrude out of the ice film. Due to surface tension the shape becomes an oblate ellipsoid. In holes covered with a thick ice film (> or = 3 lambda) and strong thickness gradients, vesicles are predominantly found in regions where the ice thickness is appropriate for their size. Also, a way of imaging the most probable loss under low-dose conditions involving thickness measurement is proposed. Even at large ice thicknesses zero-loss filtering always gives better image contrast. Most probable loss imaging can only help where there is no intensity in the zero-loss image, at very large thicknesses (lambda > 8).

摘要

利用电子显微镜,通过检查倾斜和未倾斜视图,并假设在未倾斜视图中呈圆形的囊泡为椭球形,来估计冰包埋囊泡的厚度。另一种厚度测量方法是通过囊泡的未滤波图像强度与零损失滤波图像强度之比获得的。根据这两种测量方法,在120 kV加速电压下,计算出电子在冰中非弹性散射的平均自由程A为203±33 nm。研究发现,薄冰膜(≤1.5λ)中的囊泡明显突出于冰膜之外。由于表面张力,形状变为扁椭球体。在覆盖有厚冰膜(≥3λ)且厚度梯度较大的孔洞中,囊泡主要出现在冰厚度与其大小相适应的区域。此外,还提出了一种在低剂量条件下进行涉及厚度测量的最可能损失成像的方法。即使在冰厚度较大时,零损失滤波始终能提供更好的图像对比度。最可能损失成像仅在零损失图像中没有强度的情况下有帮助,即在非常大的厚度(λ>8)时。

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