IP Library › Granted Patent US 8,724,109
Granted Patent B2
US 8,724,109 · App. 12/865,828 · Granted May 13, 2014

Method and apparatus for angular-resolved spectroscopic lithography characterization

Inventors: Irwan Dani Setija (Utrecht, NL); Maurits Van Der Schaar (Eindhoven, NL)
Assignee: ASML Netherlands B.V.
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Quick Facts
Patent No.
US 8,724,109
App. No.
12/865,828
Granted
May 13, 2014
Kind
B2
Abstract

An apparatus and method to determine overlay of a target on a substrate ( 6 ) by measuring, in the pupil plane ( 40 ) of a high numerical aperture len (L 1 ), an angle-resolved spectrum as a result of radiation being reflected off the substrate. The overlay is determined from the anti-symmetric component of the spectrum, which is formed by subtracting the measured spectrum and a mirror image of the measured spectrum. The measured spectrum may contain only zeroth order reflected radiation from the target.

Claims (34)

1. An inspection apparatus, comprising:

a detector configured to detect an angle-resolved spectrum of radiation reflected from a target formed on a substrate; and

a control system coupled to the detector, the control system being configured to:

compute a mirror image of the angle-resolved spectrum,

generate anti-symmetric components of the angle-resolved spectrum by subtracting the angle-resolved spectrum and the computed mirror image of the angle-resolved spectrum, and

determine an overlay error of the target based on the anti-symmetric components of the angle-resolved spectrum.

2. The inspection apparatus of claim 1 , wherein the control system is configured to determine the overlay error by reference to parts of the anti-symmetric components of the angle-resolved spectrum that are not on an axis of the angle-resolved spectrum.

3. The inspection apparatus of claim 1 , wherein the angle-resolved spectrum of the reflected radiation is one of a transverse magnetic spectrum of the reflected radiation or a transverse electric spectrum of the reflected radiation.

4. The inspection apparatus of claim 1 , wherein the angle-resolved spectrum comprises substantially only a zeroth order of the radiation reflected from the substrate.

5. The inspection apparatus of claim 1 , wherein the target comprises a grating and wherein a pitch of the grating is smaller than a wavelength of the radiation.

6. The inspection apparatus of claim 1 , further comprising:

a high numerical aperture lens configured to collect the reflected radiation;

wherein the detector is configured to measure the angle-resolved spectrum of the reflected radiation in a pupil plane of the high numerical aperture lens.

7. The inspection apparatus of claim 6 , wherein a numerical aperture of the high numerical aperture lens is at least 0.9.

8. The inspection apparatus of claim 1 , wherein the overlay error is related to an extent of a misalignment of two misaligned periodic structures that form the target.

9. An inspection method, comprising:

measuring an angle-resolved spectrum of radiation reflected from a target on a substrate;

computing a mirror image of the angle-resolved spectrum;

subtracting the angle-resolved reflected spectrum and the mirror image of the angle-resolved reflected spectrum to generate anti-symmetric components of the angle-resolved spectrum; and

determining, based on the anti-symmetric components of the angular-resolved reflected spectrum, an overlay error of the target.

10. The method of claim 9 , wherein the determining is performed by reference to parts of the anti-symmetric components of the angle-resolved spectrum that are not on an axis of the angle-resolved spectrum.

11. The method of claim 9 , wherein the measuring comprises measuring one of a transverse magnetic spectrum of the reflected radiation or a transverse electric spectrum of the reflected radiation.

12. The method of claim 9 , wherein the angle-resolved spectrum comprises substantially only a zeroth order of the radiation reflected from the substrate.

13. The method of claim 9 , wherein the target comprises a grating and wherein a pitch of the grating is smaller than a wavelength of the radiation reflected from the substrate.

14. The method of claim 9 , wherein:

the measuring comprises measuring, in a pupil plane of a high numerical aperture lens, the angle-resolved spectrum of the reflected radiation, and

a numerical aperture of the high numerical aperture lens is at least 0.9.

15. The method of claim 9 , wherein the overlay error is related to an extent of a misalignment of two misaligned periodic structures that form the target.

16. A device manufacturing method, comprising:

projecting radiation onto a target portion of a substrate;

measuring an angle-resolved spectrum of the radiation reflected from the target;

computing a mirror image of the angle-resolved spectrum;

subtracting the angle resolved spectrum and the mirror image of the angle-resolved spectrum to generate anti-symmetric components of the angle-resolved spectrum; and

determining, based on the anti-symmetric components of the angle-resolved spectrum, an overlay error of the target.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Oct 20, 2010
From: SETIJA, IRWAN DANI; VAN DER SCHAAR, MAURITS
To: ASML NETHERLANDS B.V.
Reel/Frame 025170/0753 →
Continuity (2)
Provisional Application 61064050 · Feb 13, 2008
Related Publication 20110073775A1 · Mar 31, 2011