USRE49784EActiveUtilityPatentIndex 63
Apparatus of plural charged-particle beams
Est. expiryJan 27, 2036(~9.6 yrs left)· nominal 20-yr term from priority
G01N 2223/6116G01N 2223/418H01J 2237/2817H01J 2237/2448H01J 2237/057G01N 23/2251H01J 37/244H01J 37/1474H01J 37/145H01J 37/06H01J 37/05H01J 37/226H01J 37/28G01N 23/00
63
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Cited by
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References
100
Claims
Abstract
A new multi-beam apparatus with a total FOV variable in size, orientation and incident angle, is proposed. The new apparatus provides more flexibility to speed the sample observation and enable more samples observable. More specifically, as a yield management tool to inspect and/or review defects on wafers/masks in semiconductor manufacturing industry, the new apparatus provide more possibilities to achieve a high throughput and detect more kinds of defects.
Claims
exact text as granted — not AI-modifiedWhat is claimed is:
1. A multi-beam apparatus for observing a surface of a sample, comprising:
an electron source;
a condenser lens below said electron source;
a source-conversion unit below said condenser lens;
an objective lens below said source-conversion unit;
a deflection scanning unit below said source-conversion unit;
a sample stage below said objective lens;
a beam separator below said source-conversion unit;
a secondary projection imaging system; and
an electron detection device with a plurality of detection elements,
wherein said electron source, said condenser lens and said objective lens are aligned with a primary optical axis of said apparatus, and said sample stage sustains said sample so that said surface faces to said objective lens,
wherein said source-conversion unit comprises a beamlet-limit means with a plurality of beam-limit openings, and an image-forming means with a plurality of electron optics elements and movable along said primary optical axis,
wherein said electron source generates a primary-electron beam along said primary optical axis and said condenser lens focuses said primary-electron beam,
wherein a plurality of beamlets of said primary-electron beam pass through said plurality of beam-limit openings respectively, and is deflected by said plurality of electron optics elements towards said primary optical axis to form a plurality of virtual images of said electron source respectively,
wherein said plurality of beamlets is focused by said objective lens onto said surface and therefore forms a plurality of probe spots thereon respectively, and said deflection scanning unit deflects said plurality of beamlets to scan said plurality of probe spots respectively over a plurality of scanned regions within an observed area on said surface,
wherein a plurality of secondary electron beams is generated by said plurality of probe spots respectively from said plurality of scanned regions and directed into said secondary projection imaging system by said beam separator, said secondary projection imaging system focuses and keeps said plurality of secondary electron beams to be detected by said plurality of detection elements respectively, and each detection element therefore provides an image signal of one corresponding scanned region.
2. The apparatus according to claim 1 , wherein deflection angles of said plurality of beamlets due to said plurality of electron optics elements are respectively set to reduce off-axis aberrations of said plurality of probe spots.
3. The apparatus according to claim 2 , wherein pitches of said plurality of probe spots are varied together by moving said image-forming means along said primary optical axis.
4. The apparatus according to claim 2 , wherein said objective lens comprises a magnetic lens and an electrostatic lens.
5. The apparatus according to claim 4 , wherein an orientation of said plurality of probe spots is selectable by varying a ratio of focusing powers of said magnetic lens and said electrostatic lens.
6. The apparatus according to claim 2 , wherein said deflection angles ensure said plurality of beamlets to land on said surface perpendicularly or substantially perpendicularly.
7. The apparatus according to claim 2 , wherein said deflection angles ensure said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
8. The apparatus according to claim 6 , wherein said deflection scanning unit is above a front focal plane of said objective lens.
9. The apparatus according to claim 8 , wherein said deflection scanning unit tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
10. The apparatus according to claim 6 , further comprising a beamlet-tilting deflector between said source-conversion unit and a front focal plane of said objective lens.
11. The apparatus according to claim 10 , wherein said beamlet-tilting deflector tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
12. A multi-beam apparatus for observing a surface of a sample, comprising:
an electron source; a condenser lens below said electron source; a source-conversion unit below said condenser lens; an objective lens below said source-conversion unit; a deflection scanning unit below said source-conversion unit; a sample stage below said objective lens; a beam separator below said source-conversion unit; a secondary projection imaging system; and an electron detection device with a plurality of detection elements,
wherein said electron source, said condenser lens and said objective lens are aligned with a primary optical axis of said apparatus, and said sample stage sustains said sample so that said surface faces to said objective lens,
wherein said source-conversion unit comprises a beamlet-limit means with a plurality of beam-limit openings, a first image-forming means with a plurality of first electron optics elements and a second image-forming means with a plurality of second electron optics elements, said second image-forming means is below said first image-forming means and movable in a radial direction, and one of said first image-forming means and said second image-forming means is used as an active image-forming means,
wherein said electron source generates a primary-electron beam along said primary optical axis and said condenser lens focuses said primary-electron beam,
wherein a plurality of beamlets of said primary-electron beam pass through said plurality of beam-limit openings respectively, and is deflected by said active image-forming means towards said primary optical axis to form a plurality of virtual images of said electron source respectively,
wherein said plurality of beamlets is focused by said objective lens onto said surface and therefore forms a plurality of probe spots thereon respectively, and said deflection scanning unit deflect said plurality of beamlets to scan said plurality of probe spots respectively over a plurality of scanned regions within an observed area on said surface,
wherein a plurality of secondary electron beams is generated by said plurality of probe spots respectively from said plurality of scanned regions and directed into said secondary projection imaging system by said beam separator, said secondary projection imaging system focuses and keeps said plurality of secondary electron beams to be detected by said plurality of detection elements respectively, and each detection element therefore provides an image signal of one corresponding scanned region.
13. The apparatus according to claim 12 , wherein deflection angles of said plurality of beamlets due to said active image-forming means are respectively set to reduce off-axis aberrations of said plurality of probe spots.
14. The apparatus according to claim 13 , wherein pitches of said plurality of probe spots are varied together by changing said active image-forming means between said first image-forming means and said second image-forming means, and when said first image-forming means is selected, said second image-forming means is moved outside so as not to block said plurality of beamlets.
15. The apparatus according to claim 13 , wherein said objective lens comprises a magnetic lens and an electrostatic lens.
16. The apparatus according to claim 15 , wherein an orientation of said plurality of probe spots is selectable by varying a ratio of focusing powers of said magnetic lens and said electrostatic lens.
17. The apparatus according to claim 13 , wherein said deflection angles ensure said plurality of beamlets to land on said surface perpendicularly or substantially perpendicularly.
18. The apparatus according to claim 13 , wherein said deflection angles ensure said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
19. The apparatus according to claim 17 , wherein said deflection scanning unit is above a front focal plane of said objective lens.
20. The apparatus according to claim 19 , wherein said deflection scanning unit tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
21. The apparatus according to claim 17 , further comprising a beamlet-tilting deflector between said source-conversion unit and a front focal plane of said objective lens.
22. The apparatus according to claim 21 , wherein said beamlet-tilting deflector tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
23. An multi-beam apparatus for observing a surface of a sample, comprising:
an electron source; a condenser lens below said electron source; a source-conversion unit below said condenser lens; an objective lens below said source-conversion unit; a deflection scanning unit below said source-conversion unit; a sample stage below said objective lens; a beam separator below said source-conversion unit; a secondary projection imaging system; and an electron detection device with a plurality of detection elements,
wherein said electron source, said condenser lens and said objective lens are aligned with a primary optical axis of said apparatus, a first principal plane of said objective lens is movable along said primary optical axis, and said sample stage sustains said sample so that said surface faces to said objective lens,
wherein said source-conversion unit comprises a beamlet-limit means with a plurality of beam-limit openings, and an image-forming means with a plurality of electron optics elements,
wherein said electron source generates a primary-electron beam along said primary optical axis and said condenser lens focuses said primary-electron beam,
wherein a plurality of beamlets of said primary-electron beam pass through said plurality of beam-limit openings respectively, and is deflected by said plurality of electron optics elements towards said primary optical axis to form a plurality of virtual images of said electron source respectively,
wherein said plurality of beamlets is focused by said objective lens onto said surface and therefore forms a plurality of probe spots thereon respectively, and said deflection scanning unit deflects said plurality of beamlets to scan said plurality of probe spots respectively over a plurality of scanned regions within an observed area on said surface,
wherein a plurality of secondary electron beams is generated by said plurality of probe spots respectively from said plurality of scanned regions and directed into said secondary projection imaging system by said beam separator, said secondary projection imaging system focuses and keeps said plurality of secondary electron beams to be detected by said plurality of detection elements respectively, and each detection element therefore provides an image signal of one corresponding scanned region.
24. The apparatus according to claim 23 , wherein deflection angles of said plurality of beamlets due to said plurality of electron optics elements are respectively set to reduce off-axis aberrations of said plurality of probe spots.
25. The apparatus according to claim 24 , wherein pitches of said plurality of probe spots are varied together by moving said first principal plane along said primary optical axis.
26. The apparatus according to claim 24 , wherein said deflection angles ensure said plurality of beamlets to land on said surface perpendicularly or substantially perpendicularly.
27. The apparatus according to claim 24 , wherein said deflection angles ensure said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
28. The apparatus according to claim 26 , wherein said deflection scanning unit is above a front focal plane of said objective lens.
29. The apparatus according to claim 28 , wherein said deflection scanning unit tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
30. The apparatus according to claim 26 , further comprising a beamlet-tilting deflector between said source-conversion unit and a front focal plane of said objective lens.
31. The apparatus according to claim 30 , wherein said beamlet-tilting deflector tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
32. The apparatus according to claim 24 , wherein said objective lens comprises a lower magnetic lens and an electrostatic lens.
33. The apparatus according to claim 32 , wherein said electrostatic lens comprises a field-control electrode and a field-moving electrode, and generates an electrostatic field.
34. The apparatus according to claim 33 , wherein a potential of said field-control electrode is set to control said electrostatic field on said surface for said sample free of electrical breakdown.
35. The apparatus according to claim 34 , wherein a potential of said field-moving electrode is set to move said electrostatic field for moving said first principal plane.
36. The apparatus according to claim 34 , wherein an orientation of said plurality of probe spots is selectable by varying either or both of potentials of said field-control electrode and said field-moving electrode.
37. The apparatus according to claim 32 , further comprising an upper magnetic lens above said lower magnetic lens.
38. The apparatus according to claim 37 , wherein said first principal plane is moved by varying a ratio of focusing powers of said lower magnetic lens and said upper magnetic lens.
39. The apparatus according to claim 37 , wherein an orientation of said plurality of probe spots is selectable by setting polarities of magnetic fields of said upper and lower magnetic lenses same or opposite.
40. A multi-beam apparatus for observing a surface of a sample, comprising:
an electron source; a condenser lens below said electron source; a source-conversion unit below said condenser lens; a transfer lens below said source-conversion unit; a field lens below said transfer lens; an objective lens below said field lens; a deflection scanning unit below said source-conversion unit; a sample stage below said objective lens; a beam separator below said source-conversion unit; a secondary projection imaging system; and an electron detection device with a plurality of detection elements,
wherein said electron source, said condenser lens, said transfer lens, said field lens and said objective lens are aligned with a primary optical axis of said apparatus, and said sample stage sustains said sample so that said surface faces to said objective lens,
wherein said source-conversion unit comprises a beamlet-limit means with a plurality of beam-limit openings, and an image-forming means with a plurality of electron optics elements,
wherein said electron source generates a primary-electron beam along said primary optical axis and said condenser lens focuses said primary-electron beam,
wherein a plurality of beamlets of said primary-electron beam pass through said plurality of beam-limit openings respectively, and is deflected by said plurality of electron optics elements towards said primary optical axis to form a plurality of first virtual images of said electron source respectively,
wherein said transfer lens images said plurality of first virtual images onto an intermediate image plane and therefore forms a plurality of second real images respectively thereon, said field lens is placed on said intermediate image plane and bends said plurality of beamlets, said objective lens images said plurality of second real images onto said surface and therefore forms a plurality of probe spots thereon respectively, and said deflection scanning unit deflects said plurality of beamlets to scan said plurality of probe spots respectively over a plurality of scanned regions within an observed area on said surface,
wherein a plurality of secondary electron beams is generated by said plurality of probe spots respectively from said plurality of scanned regions and directed into said secondary projection imaging system by said beam separator, said secondary projection imaging system focuses and keeps said plurality of secondary electron beams to be detected by said plurality of detection elements respectively, and each detection element therefore provides an image signal of one corresponding scanned region.
41. The apparatus according to claim 40 , wherein bending angles of said plurality of beamlets due to said field lens are set to reduce off-axis aberrations of said plurality of probe spots.
42. The apparatus according to claim 41 , wherein deflection angles of said plurality of beamlets due to said plurality of electron optics elements are adjusted to change pitches of said plurality of probe spots respectively.
43. The apparatus according to claim 41 , wherein said objective lens comprises a first magnetic lens and a first electrostatic lens.
44. The apparatus according to claim 43 , wherein an orientation of said plurality of probe spots is selectable by varying a ratio of focusing powers of said first magnetic lens and said first electrostatic lens.
45. The apparatus according to claim 41 , wherein said transfer lens comprises a second magnetic lens and a second electrostatic lens.
46. The apparatus according to claim 45 , wherein an orientation of said plurality of probe spots is selectable by varying a ratio of focusing powers of said second magnetic lens and said second electrostatic lens.
47. The apparatus according to claim 41 , wherein said field lens comprises a third magnetic lens and a third electrostatic lens.
48. The apparatus according to claim 47 , wherein an orientation of said plurality of probe spots is selectable by varying a ratio of focusing powers of said third magnetic lens and said third electrostatic lens.
49. The apparatus according to claim 41 , wherein said bending angles and deflection angles of said plurality of beamlets due to said plurality of electron optics elements ensure said plurality of beamlets to land on said surface perpendicularly or substantially perpendicularly.
50. The apparatus according to claim 41 , wherein said bending angles and deflection angles of said plurality of beamlets due to said plurality of electron optics elements ensure said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
51. The apparatus according to claim 49 , wherein said deflection scanning unit is above a front focal plane of said objective lens.
52. The apparatus according to claim 51 , wherein said deflection scanning unit tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
53. The apparatus according to claim 49 , further comprising a beamlet-tilting deflector between said source-conversion unit and a front focal plane of said objective lens.
54. The apparatus according to claim 53 , wherein said beamlet-tilting deflector tilts said plurality of beamlets to obliquely land on said surface with same or substantially same landing angles.
55. A method to configure a multi-beam apparatus for observing a surface of a sample, comprising steps of:
configuring an image-forming means of a source-conversion unit movable along a primary optical axis thereof, the image-forming means having a plurality of electron optics elements;
using said image-forming means to form a plurality of virtual images of an electron source respectively;
using an objective lens to image said plurality of virtual images onto said surface and form a plurality of probe spots thereon; and
moving said image-forming means to vary pitches of said plurality of probe spots.
56. A method to configure a multi-beam apparatus for observing a surface of a sample, comprising steps of:
configuring a source-conversion unit with a first image-forming means and a second image-forming means, wherein said second image-forming means is farther away from an electron source than said first image-forming means and movable in a radial direction of said apparatus; using one of said first image-forming means and said second image-forming means as an active image-forming means, wherein when said first image-forming means is used, said second image-forming means is moved away; using said active image-forming means to form a plurality of virtual images of said electron source respectively; using an objective lens to image said plurality of virtual images onto said surface and form a plurality of probe spots thereon; and changing said active image-forming means between said first image-forming means and said second image-forming means to vary pitches of said plurality of probe spots.
57. A method to configure a multi-beam apparatus for observing a surface of a sample, comprising steps of:
configuring an objective lens with a first principal plane movable along a primary optical axis of said apparatus; using an image-forming means of a source-conversion unit to form a plurality of virtual images of an electron source respectively; using said objective lens to image said plurality of virtual images onto said surface and form a plurality of probe spots thereon; and moving said first principal plane to vary pitches of said plurality of probe spots.
58. A method to configure a multi-beam apparatus for observing a surface of a sample, comprising steps of:
configuring an objective lens with a lower magnetic lens and an electrostatic lens in said apparatus; using an image-forming means of a source-conversion unit to form a plurality of virtual images of an electron source respectively; using said objective lens to image said plurality of virtual images onto said surface and form a plurality of probe spots thereon; and changing a ratio of focusing powers of said magnetic lens and said electrostatic lens to select an orientation of said plurality of probe spots.
59. The method according to claim 58 , further comprising a step of configuring said objective lens with an upper magnetic lens farther away from said surface than said lower magnetic lens.
60. The method according to claim 59 , further comprising a step of changing polarities of magnetic fields of said upper and lower magnetic lenses to select said orientation.
61. A method to configure a multi-beam apparatus for observing a surface of a sample, comprising steps of:
using an image-forming means of a source-conversion unit to deflect a plurality of beamlets from an electron source to form a plurality of first virtual images thereof respectively; using an objective lens to image said plurality of virtual images onto said surface and form a plurality of probe spots thereon; and setting deflection angles of said plurality of beamlets due to said image-forming means so that said plurality of beamlets lands on said surface with same or substantially same landing angles.
62. The method according to claim 61 , further comprising a step of changing said deflection angles to equally vary said landing angles.
63. The method according to claim 61 , further comprising a step of using a deflection scanning unit to tilt said plurality of beamlets so as to equally vary said landing angles.
64. The method according to claim 61 , further comprising a step of using a beamlet-tilting deflector to tilt said plurality of beamlets so as to equally vary said landing angles.
65. A method to configure a multi-beam apparatus for observing a surface of a sample, comprising steps of:
using an image-forming means of a source-conversion unit to deflect a plurality of beamlets from an electron source to form a plurality of first virtual images thereof respectively; using a transfer lens to image said plurality of first virtual images onto an intermediate image plane and forms a plurality of second real images respectively; placing a field lens on said intermediate image plane to bend said plurality of beamlets; and using an objective lens to image said plurality of second real images onto said surface and form a plurality of probe spots thereon.
66. The method according to claim 65 , further comprising a step of changing deflection angles of said plurality of beamlets due to said image-forming means to vary pitches of said plurality of probe spots.
67. The method according to claim 65 , further comprising a step of setting deflection angles of said plurality of beamlets due to said image-forming means and bending angles of said plurality of beamlets due to said field lens so that said plurality of beamlets lands on said surface with same or substantially same landing angles.
68. The method according to claim 67 , further comprising a step of varying said deflection angles to equally change said landing angles.
69. The method according to claim 67 , further comprising a step of using a deflection scanning unit to tilt said plurality of beamlets to equally change said landing angles.
70. The method according to claim 67 , further comprising a step of using a beamlet-tilting deflector to tilt said plurality of beamlets to equally change said landing angles.
71. The method according to claim 65 , further comprising a step of configuring said objective lens with a first magnetic lens and a first electrostatic lens.
72. The method according to claim 71 , further comprising a step of changing a ratio of focusing powers of said first magnetic lens and said first electrostatic lens to select an orientation of said plurality of probe spots.
73. The method according to claim 65 , further comprising a step of configuring said transfer lens with a second magnetic lens and a second electrostatic lens.
74. The method according to claim 73 , further comprising a step of changing a ratio of focusing powers of said second magnetic lens and said second electrostatic lens to select an orientation of said plurality of probe spots.
75. The method according to claim 65 , further comprising a step of configuring said field lens with a third magnetic lens and a third electrostatic lens.
76. The method according to claim 75 , further comprising a step of changing a ratio of focusing powers of said third magnetic lens and said third electrostatic lens to select an orientation of said plurality of probe spots.
77. An apparatus, comprising:
a source for providing a primary charged particle beam;
a source-conversion unit for dividing the primary charged particle beam into a plurality of charged particle beamlets and using which to form a plurality of images of the source respectively, the source-conversion unit comprising a beamlet-limit means with beam-limit openings and an image-forming means with electron optics elements;
an objective lens below said source-conversion unit for projecting the plurality of images onto a sample surface;
wherein pitches of the plurality of charged particle beamlets on the sample surface are adjustable by changing deflection angles of the plurality of charged particle beamlets prior entering a distance from a deflection plane of the source-conversion unit to the objective lens.
78. An apparatus, comprising:
a source for providing a primary charged particle beam;
a beamlet-limit means with beam-limit openings for usingallowing a plurality of beamlets of the primary charged particle beam to pass through, the plurality of beamlets being used to form a plurality of images of the source;
an objective lens for projecting the plurality of images onto a sample surface to form a plurality of probe spots; and
an image-forming means with electron optics elements for adjusting pitches of the plurality of probe spots on the sample surface by moving along a primary optical axis.
79. A method for observing a sample surface, said method comprising steps of:
providing a plurality of charged particle beams with a plurality of crossovers respectively using a source-conversion unit;
projecting the plurality of crossovers onto the sample surface to form a plurality of probe spots thereon using an objective lens;
scanning the plurality of probe spots on the sample surface; and
changing a distance from a deflection angles of the plurality of charged particle beams plane of the source-conversion unit to the objective lens such that pitches of the plurality of probe spots can be adjusted.
80. A source-conversion unit comprising:
a beamlet-limit device with a plurality of beam-limit openings configured to allow a plurality of beamlets to pass through: and an image-forming device movable along a primary optical axis and comprising a plurality of electron optics elements, wherein at least some of the plurality of electron optics are configured to deflect at least some of the plurality of beamlets towards the primary optical axis.
81. The source-conversion unit of claim 80, wherein the deflection of the at least some of the plurality of beamlets towards the primary optical axis form a plurality of virtual images of an electron source.
82. The source-conversion unit of claim 80, wherein the at least some of the plurality of electron optics elements are configured to deflect at least some of the plurality of beamlets at deflection angles to reduce off-axis aberrations of a plurality of probe spots.
83. The source-conversion unit of claim 82, wherein the plurality of probe spots have pitches that are varied together by moving the image-forming device along the primary optical axis.
84. The source-conversion unit of claim 82, wherein the plurality of probe spots have an orientation that is selectable by varying a ratio of focusing powers of a magnetic lens and an electrostatic lens.
85. The source-conversion unit of claim 82, wherein the deflection angles enable the at least some of the plurality of beamlets to land on a surface of a sample perpendicularly or substantially perpendicularly.
86. The source-conversion unit of claim 82, wherein the deflection angles enable the at least some of the plurality of beamlets to obliquely land on a surface of a sample with a same or substantially same landing angles.
87. A multi-beam apparatus comprising:
an electron source configured to generate a charged-particle beam along a primary optical axis: a source-conversion unit comprising: a beamlet-limit device with a plurality of beam-limit openings configured to allow a plurality of beamlets of the charged-particle beam to pass through, and an image-forming device movable along the primary optical axis and comprising a plurality of electron optics elements, wherein at least some of the plurality of electron optics are configured to deflect at least some of the plurality of beamlets towards the primary optical axis: and an objective lens configured to focus the plurality of beamlets on a surface of a sample to form a plurality of probe spots.
88. The multi-beam apparatus of claim 87, wherein the deflection of the at least some of the plurality of beamlets towards the primary optical axis form a plurality of virtual images of the electron source.
89. The multi-beam apparatus of claim 87, wherein the objective lens comprises a magnetic lens and an electrostatic lens.
90. The multi-beam apparatus of claim 89, wherein the magnetic lens and the electrostatic lens are configured to enable a selection of an orientation of the plurality of probe by varying a ratio of focusing powers of the magnetic lens and the electrostatic lens.
91. The multi-beam apparatus of claim 87, wherein the plurality of probe spots have pitches that are varied together by moving the image-forming device along the primary optical axis.
92. The multi-beam apparatus of claim 87, wherein the at least some of the plurality of electron optics elements are configured to deflect at least some of the plurality of beamlets at deflection angles to reduce off-axis aberrations of the plurality of probe spots.
93. The multi-beam apparatus of claim 92, wherein the deflection angles enable the at least some of the plurality of beamlets to land on a surface of a sample perpendicularly or substantially perpendicularly.
94. The multi-beam apparatus of claim 92, wherein the deflection angles enable the at least some of the plurality of beamlets to obliquely land on a surface of a sample with same or substantially same landing angles.
95. The multi-beam apparatus of claim 87, further comprising a deflection scanning unit positioned above a front focal plan of the objective lens.
96. The multi-beam apparatus of claim 95, wherein the deflection scanning unit is configured to tilt the plurality of beamlets to obliquely land on the surface with a same or substantially the same landing angles.
97. The multi-beam apparatus of claim 87, further comprising a beamlet-tilting deflector positioned between the source-conversion unit and a front focal plan of the objective lens.
98. The multi-beam apparatus of claim 97, wherein the beamlet-tilting deflector is configured to tilt the plurality of beamlets to obliquely land on the surface with a same or substantially the same landing angles.
99. A method to configure a multi-beam apparatus for observing a surface of a sample, the method comprising:
forming a plurality of virtual images of an electron source using an image-forming device with electron optics elements, wherein the virtual images are used to form a plurality of probe spots on the surface; and moving the image forming device along a primary axis to vary pitches of the plurality of probe spots.
100. The method of claim 99, further comprising forming the plurality of probe spots on the sample using an objective lens to image the plurality of virtual images on the surface.Cited by (0)
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