Deptuch G, Besson A, Rehak P, Szelezniak M, Wall J, Winter M, Zhu Y
Brookhaven National Laboratory, Upton, NY 11973, USA.
Ultramicroscopy. 2007 Aug;107(8):674-84. doi: 10.1016/j.ultramic.2007.01.003. Epub 2007 Jan 28.
A new imaging device for dynamic electron microscopy is in great demand. The detector should provide the experimenter with images having sufficient spatial resolution at high speed. Immunity to radiation damage, accumulated during exposures, is critical. Photographic film, a traditional medium, is not adequate for studies that require large volumes of data or rapid recording and charge coupled device (CCD) cameras have limited resolution, due to phosphor screen coupling. CCD chips are not suitable for direct recording due to their extreme sensitivity to radiation damage. This paper discusses characterization of monolithic active pixel sensors (MAPS) in a scanning electron microscope (SEM) as well as in a transmission electron microscope (TEM). The tested devices were two versions of the MIMOSA V (MV) chip. This 1M pixel device features pixel size of 17 x 17 microm(2) and was designed in a 0.6 microm CMOS process. The active layer for detection is a thin (less than 20 microm) epitaxial layer, limiting the broadening of the electron beam. The first version of the detector was a standard imager with electronics, passivation and interconnection layers on top of the active region; the second one was bottom-thinned, reaching the epitaxial layer from the bottom. The electron energies used range from a few keV to 30 keV for SEM and from 40 to 400 keV for TEM. Deterioration of the image resolution due to backscattering was quantified for different energies and both detector versions.
对用于动态电子显微镜的新型成像设备有巨大需求。该探测器应能高速为实验人员提供具有足够空间分辨率的图像。在曝光过程中对辐射损伤的耐受性至关重要。传统介质摄影胶片不适用于需要大量数据或快速记录的研究,并且电荷耦合器件(CCD)相机由于磷光屏耦合而分辨率有限。由于CCD芯片对辐射损伤极其敏感,因此不适合直接记录。本文讨论了扫描电子显微镜(SEM)和透射电子显微镜(TEM)中单片有源像素传感器(MAPS)的特性。测试的器件是MIMOSA V(MV)芯片的两个版本。这个拥有100万像素的器件像素尺寸为17×17微米²,采用0.6微米CMOS工艺设计。用于检测的有源层是一个薄(小于20微米)的外延层,限制了电子束的展宽。探测器的第一个版本是一个标准成像器,在有源区域顶部有电子、钝化和互连层;第二个版本是底部减薄的,从底部到达外延层。SEM使用的电子能量范围为几keV到30keV,TEM使用的电子能量范围为40到400keV。针对不同能量和两种探测器版本,对由于背散射导致的图像分辨率恶化进行了量化。