Three Dimensional Mask Metrology by Off-Axis Electron Holography

2001 ◽  
Vol 7 (S2) ◽  
pp. 574-575
Author(s):  
Bernhard Frost ◽  
David C Joy

Even though all real objects are three dimensional, imaging and metrology performed by using electron-beam tools such as scanning electron microscopes is inherently two dimensional. Any information about the third dimension must therefore be obtained by inference, or by time consuming special methods such as stereo-photogrammetry. If, however, the structures of interest are thin enough to be electron transparent then quantitative three dimensional metrology can be performed directly by using off-axis transmission electron holography. Here we demonstrate the application to a SCALPEL lithography mask which consists of chromium lines on a silicon support film. The off-axis holography was performed in a field emission transmission electron microscope, a Hitachi HF2000 operated at 200keV. The sample is positioned so that half the beam passes through the specimen while the rest travels only through the vacuum. An electrostatic biprism then recombines these two components to form the hologram which is recorded onto a CCD camera.

Author(s):  
T. E. Everhart

Although scanning electron microscopes have been available commercially for a relatively short time, their use is increasing rapidly. Countless persons have marvelled at their great depth of field, which produces an easily interpreted image of a three-dimensional object. Trained electron-microscopists have been impressed by the minimal sample preparation required for scanning microscope observation of inorganic objects, and of some organic objects. Non-specialists find the instrument easy to use, because many of the controls are related to familiar controls on television sets, on cathode-ray oscilloscopes, etc., and because the image on the cathode-ray tube screen is easy to interpret. Now seems the opportune moment to re-emphasize how the scanning electron microscope (SEM) differs fundamentally from the transmission electron (TEM), in order to insure that constraints imposed by the physics of image formation in the TEM will not be taken subconsciously as constraints in the SEM too.


1997 ◽  
Vol 3 (S2) ◽  
pp. 1243-1244 ◽  
Author(s):  
Raynald Gauvin ◽  
Steve Yue

The observation of microstructural features smaller than 300 nm is generally performed using Transmission Electron Microscopy (TEM) because conventional Scanning Electron Microscopes (SEM) do not have the resolution to image such small phases. Since the early 1990’s, a new generation of microscopes is now available on the market. These are the Field Emission Gun Scanning Electron Microscope with a virtual secondary electron detector. The field emission gun gives a higher brightness than those obtained using conventional electron filaments allowing enough electrons to be collected to operate the microscope with incident electron energy, E0, below 5 keV with probe diameter smaller than 5 nm. At 1 keV, the electron range is 60 nm in aluminum and 10 nm in iron (computed using the CASINO program). Since the electron beam diameter is smaller than 5 nm at 1 keV, the resolution of these microscopes becomes closer to that of TEM.


1979 ◽  
Author(s):  
M. Marshall ◽  
J. Staubesand ◽  
H. Hese

The arteries of mini pigs which had been exposed to the local or systemic action of recognised ‘risk factors’ for arterial disease were examined with the light microscope, and the transmission and scanning electron microscopes. Initially the scanning instrument revealed adhesions of platelets in different stages of development, but showed an apparently intact endothelium. With the transmission electron microscope, however, degenerative changes in the endothelium could be observed. Increased blood platelet aggregation was also present. After a few weeks we could see a remarkable focal thickening of the intima, together with deposits on the endothelium of platelets, erythrocytes and fibrin (“mixed microparietal thrombosis”). After 6 months fully developed arteriosclerosis of the abdominal aorta had appeared.


1993 ◽  
Vol 1 (4) ◽  
pp. 6-10
Author(s):  
Stephen E. Rice

Great strides have been made in the last decade in high resolution transmission electron microscopes (TEMs) which can also provide elemental information via energy dispersive X-ray analysis (EDX) or energy loss spectroscopy (EELS), and proponents of various TEM techniques make bold claims. Convergent beam elecjron diffraction and microdifff action shine as techniques for defect structure analysis and means for solving crystal structures. The spectroscopies can now be used to map chemical state information at a level which until recently might be encountered in science fiction. As a pure imaging device, electron holography holds great promise for providing Ehe ultimate (would you believe 0.1Å?) imaging resolution. Although conventional TEMs will never approach this, it appears that we are learning more and more about less and less, until we will soon know everything there is to know about nothing.


2010 ◽  
Vol 644 ◽  
pp. 1-7 ◽  
Author(s):  
Joaquim Portillo ◽  
Edgar F. Rauch ◽  
Stavros Nicolopoulos ◽  
Mauro Gemmi ◽  
Daniel Bultreys

Precession electron diffraction (PED) is a new promising technique for electron diffraction pattern collection under quasi-kinematical conditions (as in X-ray Diffraction), which enables “ab-initio” solving of crystalline structures of nanocrystals. The PED technique may be used in TEM instruments of voltages 100 to 400 kV and is an effective upgrade of the TEM instrument to a true electron diffractometer. The PED technique, when combined with fast electron diffraction acquisition and pattern matching software techniques, may also be used for the high magnification ultra-fast mapping of variable crystal orientations and phases, similarly to what is achieved with the Electron Backscattered Diffraction (EBSD) technique in Scanning Electron Microscopes (SEM) at lower magnifications and longer acquisition times.


Author(s):  
L. C. Sawyer

Recent advances in Analytical Electxon Microscopy (AEM) have changed the methods by which microicopists study polymer and fiber morphology. As polymeric materialis play a major role in our way of living - clothing, shelter, fuel, chemicals - the interest has spread from a small group of theoretical physicists to the larger group of applications scientists. Until forty years ago, optical microscopy (OM) provided the only microicopical means of observing the morphology of materials. Then transmission electron microscopes (TEM) brought a new depth and resolution of fine structures not previously known. The methodology of preparing materials for TEM, ultramicrotomy and replication, are revealing but tedious and replete with artifacts. Bridging the gap between OM and TEM the scanning electron microscopes (SEM), in use over the past fifteen years, have provided easily available and interpretable surface images of fibers, fabrics, membranes, films and composites. Finally, the limited resolution of the SEM has been improved by the use of modern composite instruments known as analytical electron microscopes (AEM).


Author(s):  
J. R. Minter ◽  
K. Schlafer ◽  
G. Sotak ◽  
L. Thom

Since the invention of the microscope, most images were recorded on photographic film. For transmission electron images, Hamilton and Marchant recognized that most photographic films are “nearly perfect detectors, in that they record the input signal without appreciable loss and do not seriously add to the input noise”. Despite film's efficiency as an image recorder, microscopists complained about the long cycle time between image recording and completion of the final print. Quantitative image analysis of images recorded on film is also time-consuming and expensive because microdensitometers capable of producing high quality and high resolution scans of negatives are slow and expensive.Over the past few years several new technologies to record light and electron images have been commercialized. The oldest of these are video-rate cameras and TV-rate cameras built with charge coupled devices (CCDs). These are limited by small image size (512 × 478). Larger format digital cameras built using slow-scan CCD cameras have recently been applied to light and transmission electron microscopy. Digital scan generators and frame buffers have been added to scanning electron microscopes.


Author(s):  
Q. Ru ◽  
J. Endo ◽  
A. Tonomura

Compared with the wavefront-divided electron holography obtained by an electron biprism, the amplitude-divided one proposed by Matteucci et al. has some essential advantages: less necessary coherency, wide interference area and available to most of transmission electron microscopes. In order to confirm and achieve these advantages in practical use, we introduce some improvements in both hologram formation and reconstruction steps. Two electron-optical setups and experimental results are presented for small objects (<1 μm) and much large objects (>1 μm), respectively.The electron-optics for taking the holograms of small objects is illustrated in Figure 1. A single crystal thin film (gold film of 0.2nm lattice spacing is used in our experiment) is placed on the objects (latex particles of 120 nm on a thin carbon film are used here) with a certain gap. In fact, the gap is spontaneously made by the microgrids of the specimen film and the crystal film.


Author(s):  
R.J. Young ◽  
A. Buxbaum ◽  
B. Peterson ◽  
R. Schampers

Abstract Scanning transmission electron microscopy with scanning electron microscopes (SEM-STEM) has become increasing used in both SEM and dual-beam focused ion beam (FIB)-SEM systems. This paper describes modeling undertaken to simulate the contrast seen in such images. Such modeling provides the ability to help understand and optimize imaging conditions and also support improved sample preparation techniques.


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