Overlay error measurement apparatus and method
A technology of overlay error and measuring device, which is applied in the field of equipment in the field of integrated circuit manufacturing, can solve the problems of small depth of focus, measurement wavelength cannot use wide band, and difficulty in focal plane control, so as to achieve limited measurement accuracy and rich effective measurement signals , to obtain short-term effects
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Embodiment 1
[0057] Please refer to figure 1 , figure 1 It is a schematic structural diagram of an overlay error measuring device according to Embodiment 1 of the present invention. The overlay error measurement device includes: a light source system; specifically, the light source system includes a light source 41 and a light source shaping system 43, and the light source is a broadband light source, for example, a white light source, or composed of several discrete spectral lines A composite light source, such as obtained by mixing several lasers with different wavelengths. The measurement light generated by the light source 41 is preferably a two-dimensional surface beam, that is, the cross-section 42 is a rectangle (not shown), and of course it can also be any other two-dimensional shape.
[0058] After passing through the light source shaping system 43 , the measuring light forms a one-dimensional line beam 44 from a surface beam. Please refer to figure 2 , which is a schematic...
Embodiment 2
[0062] Please refer to Figure 5 , which is a schematic structural diagram of the overlay error measuring device in Embodiment 2 of the present invention. For simplicity, in this embodiment, unless otherwise specified, the same components as in Embodiment 1 are given the same reference numerals, and their descriptions are omitted.
[0063] like Figure 5 As shown, the overlay error measurement device of this embodiment further includes a polarizer 416 and an analyzer 417 . The polarizer 416 is located between the light source system and the beam splitter 45 , so that the linear measurement beam 44 generates polarized light of TE mode or polarized light of TM mode after passing through the polarizer 416 . The analyzer 417 is added between the spectroscope 45 and the detector 411 in the measurement light path, so that the diffraction spectrum measurement signal 413 recorded can be the change of the TE mode reflectivity with the incident angle and wavelength, or can be the TM mo...
Embodiment 3
[0066] Please refer to Image 6 , which is a structural schematic diagram of the overlay error measuring device in Embodiment 3 of the present invention. For the sake of simplicity, in this embodiment, unless otherwise specified, the same components as in Embodiment 2 use the same symbols, and their descriptions are omitted.
[0067] The spatial frequency of each order of the diffracted light is sinθ=m×λ / p, where θ is the diffraction angle, m is the diffraction order, λ is the wavelength, and p is the period of the overlay mark. Since the measurement uses broadband light, within the same diffraction order, the diffracted light of each wavelength is spatially separated. In the present invention, the overlay error is determined by measuring the asymmetry of the diffracted light intensity at the same wavelength and the same incident angle. Therefore, it is necessary to accurately determine the position of the diffracted light of the same wavelength on the detector 411 . like ...
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