IP Library › Granted Patent US 7,468,798
Granted Patent B2
US 7,468,798 · App. 11/627,153 · Granted Dec 23, 2008

System and method for polarization characteristic measurement of optical systems via centroid analysis

Assignee: Canon Kabushiki Kaisha
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Quick Facts
Patent No.
US 7,468,798
App. No.
11/627,153
Granted
Dec 23, 2008
Kind
B2
Abstract

A method for irradiating onto a target optical system plural linearly polarized rays having different polarization directions, and for measuring a polarization characteristic of the target optical system including a birefringence amount R and a fast axis Φ includes the steps of irradiating linearly polarized ray having a polarization direction θ onto the target optical system and obtaining a centroid amount P of the ray that has transmitted through the target optical system, and obtaining the birefringence amount R and the fast axis Φ from P=−R·cos(2θ−Φ) or P=R·cos(2θ−Φ).

Claims (24)

1. A method for irradiating onto a target optical system plural linearly polarized rays having different polarization directions, and for measuring a polarization characteristic of the target optical system including a birefringence amount R and a fast axis Φ, said method comprising the steps of:

irradiating linearly polarized ray having a polarization direction θ onto the target optical system and obtaining a centroid amount P of the ray that has transmitted through the target optical system; and

obtaining the birefringence amount R and the fast axis Φ from P=−R·cos(2θ−Φ) or P=R·cos (2θ−Φ).

2. A method according to claim 1 , wherein the polarization characteristic further includes a Jones matrix M defined in the following equation, and said method further comprising the step of obtaining the Jones matrix M by irradiating two linearly polarized rays having different polarization directions onto the target optical system and measuring transmittances A and A′ of the target optical system for the two linearly polarized rays:

M=[A ·exp( −i·m ), a ·exp( −i·b ); a ·exp( −i·b ), A ′·exp( i·m )]

a= 2 A ″·sin R·Ex·Ey,

A″ =( A+A′ )/2,

b±π/ 2,

m=Arg{A·Ey 2 ·exp( −i·R )+ A′·Ex 2 ·exp( i·R )},

Ex =√{(1+cos Φ)2},

Ex 2 +Ey 2 =1.

3. A method for irradiating onto a target optical system plural linearly polarized rays having different polarization directions, and for measuring a polarization characteristic of the target optical system, said method comprising the steps of:

obtaining a relationship between an actual value of the polarization characteristic of the target optical system and a value of the polarization characteristic obtained under an approximation of an eigenvector of a Jones matrix of the target optical system to a linearly polarized ray;

obtaining a centroid amount determined by light intensities and phases of two rays divided due to birefringence of the target optical system; and

calculating the polarization characteristic based on the relationship and the centroid amount of the rays.

4. A method according to claim 3 , wherein the relationship is a proportion.

5. A method according to claim 3 , wherein the target optical system includes plural lenses, and a distribution range of the birefringence amount falls within 30°.

6. A method according to claim 3 , further comprising the step of changing the polarization direction of the ray.

7. A method according to claim 3 , wherein said centroid obtaining step utilizes a point diffraction interferometry, a lateral shearing interferometry, or Hartmann method.

8. An exposure apparatus comprising a projection optical system for projecting a reticle pattern onto a substrate, the projection optical system being adjusted based on a polarization characteristic measured by a method that irradiates onto the projection optical system plural linearly polarized rays having different polarization directions, the polarization characteristic including a birefringence amount R and a fast axis Φ of the target optical system, the method including the steps of irradiating the linearly polarized ray having a polarization direction θ onto the target optical system and obtaining a centroid amount P of the ray that has transmitted through the target optical system, and obtaining the birefringence amount R and the fast axis Φ from P=−R·cos(2θ−Φ) or P=R·cos(2θ−Φ).

9. A device manufacturing method comprising the steps of:

exposing a substrate using an exposure apparatus; and

developing the substrate exposed,

wherein the exposure apparatus includes a projection optical system for projecting a reticle pattern onto a substrate, the projection optical system being adjusted based on a polarization characteristic measured by a measurement method that irradiates onto the projection optical system plural linearly polarized rays having different polarization directions, the polarization characteristic including a birefringence amount R and a fast axis Φ of the target optical system, the measurement method including the steps of irradiating the linearly polarized ray having a polarization direction θ onto the target optical system and obtaining a centroid amount P of the ray that has transmitted through the target optical system, and obtaining the birefringence amount R and the fast axis Φ from P=−R·cos(2θ−Φ) or P=R·cos(2θ−Φ).

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 22, 2007
From: SHIODE, YOSHIHIRO
To: CANON KABUSHIKI KAISHA
Reel/Frame 018920/0605 →
Priority Claims (1)
JP 2006-017561 · Jan 26, 2006 · national
Continuity (1)
Related Publication 20070171427A1 · Jul 26, 2007