High Dynamic Range Pixel Array Detector for Scanning Transmission Electron Microscopy

被引:290
作者
Tate, Mark W. [1 ]
Purohit, Prafull [1 ]
Chamberlain, Darol [2 ]
Nguyen, Kayla X. [3 ]
Hovden, Robert [3 ]
Chang, Celesta S. [4 ]
Deb, Pratiti [4 ]
Turgut, Emrah [3 ]
Heron, John T. [4 ,5 ]
Schlom, Darrell G. [5 ,6 ]
Ralph, Daniel C. [1 ,4 ,6 ]
Fuchs, Gregory D. [3 ,6 ]
Shanks, Katherine S. [1 ]
Philipp, Hugh T. [1 ]
Muller, David A. [3 ,6 ]
Gruner, Sol M. [1 ,2 ,4 ,6 ]
机构
[1] Cornell Univ, Lab Atom & Solid State Phys, Ithaca, NY 14853 USA
[2] Cornell Univ, Cornell High Energy Synchrotron Source CHESS, Ithaca, NY 14853 USA
[3] Cornell Univ, Sch Appl & Engn Phys, Ithaca, NY 14853 USA
[4] Cornell Univ, Dept Phys, Ithaca, NY 14853 USA
[5] Cornell Univ, Dept Mat Sci & Engn, Ithaca, NY 14853 USA
[6] Kavli Inst Cornell Nanoscale Sci, Ithaca, NY 14853 USA
基金
美国国家卫生研究院; 美国国家科学基金会;
关键词
pixel array detector (PAD); STEM; high dynamic range; mixed-mode pixel array detector (MM-PAD); electron microscope pixel array detector (EMPAD); DIFFERENTIAL PHASE-CONTRAST; SENSOR;
D O I
10.1017/S1431927615015664
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We describe a hybrid pixel array detector (electron microscope pixel array detector, or EMPAD) adapted for use in electron microscope applications, especially as a universal detector for scanning transmission electron microscopy. The 128x128 pixel detector consists of a 500 mu m thick silicon diode array bump-bonded pixel-by-pixel to an application-specific integrated circuit. The in-pixel circuitry provides a 1,000,000: 1 dynamic range within a single frame, allowing the direct electron beam to be imaged while still maintaining single electron sensitivity. A 1.1 kHz framing rate enables rapid data collection and minimizes sample drift distortions while scanning. By capturing the entire unsaturated diffraction pattern in scanning mode, one can simultaneously capture bright field, dark field, and phase contrast information, as well as being able to analyze the full scattering distribution, allowing true center of mass imaging. The scattering is recorded on an absolute scale, so that information such as local sample thickness can be directly determined. This paper describes the detector architecture, data acquisition system, and preliminary results from experiments with 80-200 keV electron beams.
引用
收藏
页码:237 / 249
页数:13
相关论文
共 40 条
[1]  
Angello SG, 2004, IEEE NUCL SCI CONF R, P4667
[2]   A rad-hard CMOS active pixel sensor for electron microscopy [J].
Battaglia, Marco ;
Contarato, Devis ;
Denes, Peter ;
Doering, Dionisio ;
Giubilato, Piero ;
Kim, Tae Sung ;
Mattiazzo, Serena ;
Radmilovic, Velimir ;
Zalusky, Sarah .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 2009, 598 (02) :642-649
[3]   CHARGE COUPLED SEMICONDUCTOR DEVICES [J].
BOYLE, WS ;
SMITH, GE .
BELL SYSTEM TECHNICAL JOURNAL, 1970, 49 (04) :587-+
[4]   A high-speed area detector for novel imaging techniques in a scanning transmission electron microscope [J].
Caswell, T. A. ;
Ercius, P. ;
Tate, M. W. ;
Ercan, A. ;
Gruner, S. M. ;
Muller, D. A. .
ULTRAMICROSCOPY, 2009, 109 (04) :304-311
[5]   DIRECT DETERMINATION OF MAGNETIC DOMAIN-WALL PROFILES BY DIFFERENTIAL PHASE-CONTRAST ELECTRON-MICROSCOPY [J].
CHAPMAN, JN ;
BATSON, PE ;
WADDELL, EM ;
FERRIER, RP .
ULTRAMICROSCOPY, 1978, 3 (02) :203-214
[7]   CONFIGURED DETECTORS FOR STEM IMAGING OF THIN SPECIMENS [J].
COWLEY, JM .
ULTRAMICROSCOPY, 1993, 49 (1-4) :4-13
[8]  
DEKKERS NH, 1974, OPTIK, V41, P452
[9]   Digital imaging in transmission electron microscopy [J].
Fan, GY ;
Ellisman, MH .
JOURNAL OF MICROSCOPY, 2000, 200 (01) :1-13
[10]   ASIC-based event-driven 2D digital electron counter for TEM imaging [J].
Fan, GY ;
Datte, P ;
Beuville, E ;
Beche, JF ;
Millaud, J ;
Downing, KH ;
Burkard, FT ;
Ellisman, MH ;
Xuong, NH .
ULTRAMICROSCOPY, 1998, 70 (03) :107-113