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:
Mar. 11, 2008

Filed:

Oct. 27, 2003
Applicants:

Gregg M. Gallatin, Newtown, CT (US);

Emanuel Gofman, Haifa, IL;

Kafai Lai, Poughkeepsie, NY (US);

Mark A. Lavin, Katonah, NY (US);

Maharaj Mukherjee, Wappingers Falls, NY (US);

Dov Ramm, Menashe, IL;

Alan E. Rosenbluth, Yorktown Heights, NY (US);

Shlomo Shlafman, Haifa, IL;

Inventors:

Gregg M. Gallatin, Newtown, CT (US);

Emanuel Gofman, Haifa, IL;

Kafai Lai, Poughkeepsie, NY (US);

Mark A. Lavin, Katonah, NY (US);

Maharaj Mukherjee, Wappingers Falls, NY (US);

Dov Ramm, Menashe, IL;

Alan E. Rosenbluth, Yorktown Heights, NY (US);

Shlomo Shlafman, Haifa, IL;

Attorneys:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
G06F 7/60 (2006.01); G06F 17/50 (2006.01); G06F 19/00 (2006.01); G06K 9/00 (2006.01);
U.S. Cl.
CPC ...
Abstract

A first method to compute a phase map within an optical proximity correction simulation kernel utilizes simulated wavefront information from randomly generated data. A second method uses measured data from optical tools. A phase map is created by analytically embedding a randomly generated two-dimensional array of complex numbers of wavefront information, and performing an inverse Fourier Transform on the resultant array. A filtering function requires the amplitude of each element of the array to be multiplied by a Gaussian function. A power law is then applied to the array. The elements of the array are shuffled, and converted from the phasor form to real/imaginary form. A two-dimensional Fast Fourier Transform is applied. The array is then unshuffled, and converted back to phasor form.


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