Abstract:
A method and tool for conducting NIR overlay metrology is disclosed. Such methods involve generating a filtered illumination beam including NIR radiation and directing that illumination beam onto an overlay target to produce an optical signal that is detected and used to generate overlay metrology measurements. The method is particularly suited to substrate applications having layers of opaque material that are transmissive in the NIR range (e.g., amorphous carbon) and where NTR imaging is used to obtain overlay measurements. A tool implementation includes a means for generating a filtered illumination beam extending into the NIR range and a detector for receiving NIR signal from an NIR illuminated target and a computer for processing the signal data to obtain overlay metrology measurements.
Abstract:
A method of inspecting a phase shift mask is disclosed. The method includes receiving a mask having an alternating phase shift pattern. The method also includes forming the alternating phase shift pattern on a wafer. The method further includes analyzing the alternating phase shift pattern on the wafer to determine the phase difference of the alternating phase shift pattern.
Abstract:
The invention is a method for generating a design rule map having a spatially varying overlay error budget. Additionally, the spatially varying overlay error budget can be employed to determine if wafers are fabricated in compliance with specifications. In one approach a design data file that contains fabrication process information and reticle information is processed using design rules to obtain a design map with a spatially varying overlay error budget that defines a localized tolerance to overlay errors for different spatial locations on the design map. This spatially varying overlay error budget can be used to disposition wafers. For example, overlay information obtained from measured metrology targets on a fabricated wafer are compared with the spatially varying overlay error budget to determine if the wafer overlay satisfies the required specification.
Abstract:
Disclosed is a method of determining an overlay error between two layers of a multiple layer sample. For a plurality of periodic targets that each have a first structure formed from a first layer and a second structure formed from a second layer of the sample, an optical system is employed to thereby measure an optical signal from each of the periodic targets. There are predefined offsets between the first and second structures. An overlay error is determined between the first and second structures by analyzing the measured optical signals from the periodic targets using a scatterometry overlay technique based on the predefined offsets. The optical system comprises any one or more of the following apparatuses: a reflectometric, a ellipsomertic, imaging, interferometric, and/ or scanning angle system.
Abstract:
Disclosed are techniques, apparatus, and targets for determining overlay error between two layers of a sample. A plurality of targets is provided. Each target includes a portion of the first and second structures and each is designed to have an offset between its first and second structure portions. The targets are illuminated with electromagnetic radiation to thereby obtain spectra from each target at a −1st diffraction order and a +1st diffraction order. It is determined whether there are any overlay error between the first structures and the second structures using a scatterometry technique based on the detected spectra by (i) for each target, determining a first differential intensity between the −1st diffraction order and a +1st diffraction order, (ii) for a plurality of pairs of targets each having a first target and a second target, determining a second differential intensity between the first differential intensity of the first target and the first differential intensity of the second target, and (iii) determining any overlay error between the first structures and the second structures using a scatterometry technique based on the second differential intensities determined from each target pair.
Abstract:
Disclosed is a method of determining an overlay error between two layers of a multiple layer sample. For a plurality of periodic targets that each have a first structure formed from a first layer and a second structure formed from a second layer of the sample, an optical system is employed to thereby measure an optical signal from each of the periodic targets. There are predefined offsets between the first and second structures. An overlay error is determined between the first and second structures by analyzing the measured optical signals from the periodic targets using a scatterometry overlay technique based on the predefined offsets. The optical system comprises any one or more of the following apparatuses: a reflectometric, a ellipsomertic, imaging, interferometric, and/ or scanning angle system.
Abstract:
Disclosed are techniques, apparatus, and targets for determining overlay error between two layers of a sample. In one embodiment, a method for determining overlay between a plurality of first structures in a first layer of a sample and a plurality of second structures in a second layer of the sample is disclosed. Targets A, B, C and D that each include a portion of the first and second structures are provided. Target A is designed to have an offset Xa between its first and second structures portions; target B is designed to have an offset Xb between its first and second structures portions; target C is designed to have an offset Xc between its first and second structures portions; and target D is designed to have an offset Xd between its first and second structures portions. Each of the offsets Xa, Xb, Xc and Xd is preferably different from zero; Xa is an opposite sign and differ from Xb; and Xc is an opposite sign and differs from Xd. The targets A, B, C and D are illuminated with electromagnetic radiation to obtain spectra SA, SB, SC, and SD from targets A, B, C, and D, respectively. Any overlay error between the first structures and the second structures is then determined using a linear approximation based on the obtained spectra SA, SB, SC, and SD.