The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
May. 30, 2017

Filed:

May. 19, 2016
Applicant:

Kla-tencor Corporation, Milpitas, CA (US);

Inventors:

Natalia Malkova, Hayward, CA (US);

Leonid Poslavsky, Belmont, CA (US);

Assignee:

KLA-Tencor Corporation, Milpitas, CA (US);

Attorneys:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G01B 11/02 (2006.01); G01B 7/02 (2006.01); G01N 21/21 (2006.01); G01N 21/95 (2006.01); H01L 21/36 (2006.01); H01L 21/66 (2006.01); G01R 31/308 (2006.01); G01N 21/84 (2006.01);
U.S. Cl.
CPC ...
G01R 31/308 (2013.01); G01N 21/211 (2013.01); G01N 21/8422 (2013.01); G01N 21/9501 (2013.01); H01L 22/12 (2013.01); H01L 22/20 (2013.01); G01N 2021/213 (2013.01); G01N 2201/12 (2013.01);
Abstract

Methods and systems for monitoring band structure characteristics and predicting electrical characteristics of a sample early in a semiconductor manufacturing process flow are presented herein. High throughput spectrometers generate spectral response data from semiconductor wafers. In one example, the measured optical dispersion is characterized by a Gaussian oscillator, continuous Cody-Lorentz model. The measurement results are used to monitor band structure characteristics, including band gap and defects such as charge trapping centers, exciton states, and phonon modes in high-K dielectric layers and embedded nanostructures. The Gaussian oscillator, continuous Cody-Lorentz model can be generalized to include any number of defect levels. In addition, the shapes of absorption defect peaks may be represented by Lorentz functions, Gaussian functions, or both. These models quickly and accurately represent experimental results in a physically meaningful manner. The model parameter values can be subsequently used to gain insight and control over a manufacturing process.


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