Chapter/Index: Introduction | A | B | C | D | E | F | G | H | I | J | K | L | M | N | O | P | Q | R | S | T | U | V | W | X | Y | Z | Appendix
| The modern electron microscopes (EMs) are highly versatile and normally controlled by computer functions on the illumination conditions, the detection configurations (diffraction and image), and many other tunable parameters such as accelerating voltage, beam current, beam tilt, defocus, spherical aberration constant, specimen position, orientation, pixel size of the camera, etc. Functions of some parts in SEM shown in Figure 4231:
Figure 4231. Example of computer-controlled EMs: SEM system. Moreover, electrons emitted from the gun do not always pass precisely through the center of the lens system. To correct this, the gun-alignment coil is adjusted using a dedicated control system. In modern electron microscopes (EMs), computer control facilitates easy switching between various operation modes—such as SEM, STEM, bright-field and dark-field TEM, nanobeam electron diffraction (NBED), and CBED—once the lens settings have been preset. High-voltage TEMs often have columns exceeding 3 meters in height, making it challenging to access the aperture drives and specimen airlock during operation. Fortunately, modern microscopes are equipped with computer or remote control devices, eliminating the need for a ladder. For TEM, it is advisable to relocate all computers with fans out of the room, as the fans can generate and circulate heat, potentially affecting the microscopy environment.
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