Magnetic lens and method for focusing charged particle beams
A technology of charged particle beam and magnetic lens, applied in the field of magnetic lens, can solve problems such as impact
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Embodiment 1
[0069] figure 1 A cross-sectional view of a (rotationally symmetric) magnetic lens 10 according to an embodiment of the invention is schematically shown.
[0070] A beam 1 of charged particles (eg electrons) travels along an optical axis 2 . Composite yokes 13 , 16 and electric coils (magnetic field generating means) 12 are provided around the optical axis 2 . The yoke includes a central (axial) bore 11 and includes an outer main part 13 and an inner secondary part 16, the latter (secondary part 16) being mounted as a single insert within the former (main part 13). The secondary portion 16 comprises a waist region 15 (with a reduced outer diameter) which surrounds the hole 11 and acts as a magnetic constriction. In operation (when the coil 12 is energized), the waist region 15 is magnetically saturated, so an axial (focusing) magnetic field is formed in the focusing region 14 . The secondary part 16 (and in particular the waist region 15 ) has high magnetic quality, wherea...
Embodiment 2
[0075] image 3 A lens 10 with an auxiliary electrical coil 18 and a secondary part (insert) 16 for performing high frequency lens modulation is shown schematically.
[0076] The figure shows the secondary part / insert 16 with the waist part 15 . The auxiliary electrical coil 18 is close to (in this case around) the waist portion 15 . During operation of the lens, the auxiliary coil 18 will thus surround the saturated material, and thus the inductance of the coil 18 will be relatively low, allowing the lens power to vary with relatively high frequencies. For axial fields along optical axis 2, shielding due to eddy currents does not occur.
Embodiment 3
[0078] Figure 4 Schematically shown including an alternative secondary part / insert 16 figure 1 details.
[0079]Here, the insert 16 includes a groove 19 which results in the isolation of the peninsula 20 from the rest of the yoke (primary 13, secondary 16). Because such a peninsula is magnetically "free-standing", it shields the axial region from stray magnetic fields. Preferably, the freestanding peninsula-like portion of the insert extends beyond the joint where the insert 16 sits on the rest of the yoke (13, 17), thus avoiding unwanted escape of the magnetic field at said joint.
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