Optical low-pass filter and optical apparatus having the same

• US 6,144,493 A
• Filed: 02/20/1997
• Issued: 11/07/2000
• Est. Priority Date: 02/23/1996
• Status: Expired due to Term

• Current Assignee: Canon Kabushiki Kaisha (Canon Inc.)
• Original Assignee: Canon Kabushiki Kaisha (Canon Inc.)
• Inventors: Kobayashi, Shuichi, Wada, Ken, Okuyama, Atsushi
• Primary Examiner(s): SCHUBERG, DARREN E
• Application Number:
  US08/804,155
• Time in Patent Office: 1,356 Days
• Field of Search: 359/558, 359/566, 359/737, 250/201.9, 250/216, 348/335, 348/340
• US Class Current: 359/566
• CPC Class Codes: G02B 26/06 for controlling the phase of light G02B26/08 takes precedence , measuring optical phase difference G01J9/00
• CPC Class Codes: G02B 27/46 Systems using spatial filters

Abstract

An optical low-pass filter comprises a phase advancing area which advances a phase of a wavefront of an incident pencil of rays with respect to a phase of a wavefront of a center of the incident pencil of rays, and a phase retarding area which retards the phase of the wavefront of the incident pencil of rays with respect to the phase of the wavefront of the center of the incident pencil of rays, the phase advancing area and the phase retarding area alternately existing in the optical low-pass filter, and an optical apparatus comprises an image forming optical system, an image pickup element, and such an optical low-pass filter.

Claims

1. An optical low-pass filter comprising:

a phase advancing area which advances a phase of a wavefront of an incident pencil of rays with respect to a phase of a wavefront of a center of the incident pencil of rays; and

a phase retarding area which retards the phase of the wavefront of the incident pencil of rays with respect to the phase of the wavefront of the center of the incident pencil of rays,

said phase advancing area and said phase retarding area being alternately formed in a generally non-linear pattern, and in a rotational direction centered at an origin corresponding to the center of the incident pencil of rays.

2. An optical low-pass filter according to claim 1, wherein said phase advancing area is formed as a shape having a phase advancing action and said phase retarding area is formed as a shape having a phase retarding action.

3. An optical low-pass filter according to claim 1, wherein said phase advancing area is formed of a material having a refractive index having a phase advancing action and said phase retarding area is formed of a material having a refractive index having a phase retarding action.

4. An optical low-pass filter according to claim 1, wherein said phase advancing area and said phase retarding area are continuously formed in a rotational direction.

5. An optical low-pass filter according to claim 1, wherein a shape S(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which p is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">S(ρ

,φ

)=R(ρ

)×

cos(mφ

+δ

),

where R(ρ

) is a radial shape of said optical low-pass filter, m is an integer not less than 2, and δ

is a constant.

6. An optical low-pass filter according to claim 1, wherein a shape S(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, +) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

##EQU19## where Rm(ρ

) is a radial shape of said optical low-pass filter, m is an integer, and Am and δ

m are constants.

7. An optical low-pass filter according to claim 1, wherein a shape S(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">S(ρ

,φ

)=R(ρ

)×

cos{m(φ

+kf(ρ

)+δ

)},

where R(ρ

) is a radial shape of said optical low-pass filter, f(ρ

) is an arbitrary function of ρ

, m is an integer, and k and δ

are constants.

8. An optical low-pass filter according to claim 1, wherein a shape S(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

##EQU20## where Rm(ρ

) is a radial shape of said optical low-pass filter, fm(ρ

) is an arbitrary function of ρ

, m is an integer, and Am and δ

m are constants.

9. An optical low-pass filter according to claim 1, wherein a gradient refractive index N(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">N(ρ

,φ

)=N0+Nr(ρ

)×

cos(mφ

+δ

),

where N0 is a refractive index relative at the origin, Nr(ρ

) is a gradient refractive index relative to the radial direction, m is an integer not less than 2, and δ

is a constant.

10. An optical low-pass filter according to claim 1, wherein a gradient refractive index N(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

##EQU21## where N0 is a refractive index relative at the origin, Nrm(ρ

) is a gradient refractive index relative to the radial direction, m is an integer, and Am and δ

m are constants.

11. An optical low-pass filter according to claim 1, wherein a gradient refractive index N(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">N(ρ

,φ

)=N0+Nr(ρ

)×

cos{m(φ

+kf(ρ

)+δ

)},

where N0 is a refractive index relative at the origin, Nr(ρ

) is a gradient refractive index relative to the radial direction, f(ρ

) is an arbitrary function of ρ

, m is an integer, and k and δ

are constants.

12. An optical low-pass filter according to claim 1, wherein a gradient refractive index N(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

##EQU22## where N0 is a refractive index relative at the origin, Nrm(ρ

) is a gradient refractive index relative to the radial direction, fm(ρ

) is an arbitrary function of ρ

, m is an integer, and Am and δ

m are constants.

13. An optical low-pass filter according to claim 1, wherein a wavefront aberration W(ρ

, φ

) which occurs in a pencil of rays transmitted through said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to a rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">W(ρ

,φ

)=Wr(ρ

)×

Wt(φ

),

provided that the following conditions are satisfied;

space="preserve" listing-type="equation">Wr(0.3)/Wr(0.6)>

0

space="preserve" listing-type="equation">Wr(0.6)/Wr(0.9)>

0

where Wr(ρ

) is a wavefront aberration relative to the radial direction and Wt(φ

) is a wavefront aberration relative to the rotational direction.

14. An optical low-pass filter according to claim 1, wherein a wavefront aberration W(ρ

, φ

) which occurs in a pencil of rays transmitted through said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to a rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">W(ρ

,φ

)=Wr(ρ

)×

Wt(φ

),

and an amount of variation, Wr'"'"'(ρ

), in the wavefront aberration relative to the radial direction is expressed as

space="preserve" listing-type="equation">Wr'"'"'(ρ

)=∂

W(ρ

)/∂

ρ

,

provided that the following conditions are satisfied;

space="preserve" listing-type="equation">Wr'"'"'(0.3)/Wr'"'"'(0.6)>

1,

space="preserve" listing-type="equation">Wr'"'"'(0.6)/Wr'"'"'(0.9)<

1,

where Wr(ρ

) is a wavefront aberration relative to the radial direction and Wt(φ

) is a wavefront aberration relative to the rotational direction.

15. An optical low-pass filter according to claim 1, wherein a shape S(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which p is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to a rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">S(ρ

,100 )=R(ρ

)×

T(φ

),

and an amount of variation in shape, R'"'"'(ρ

), relative to the radial direction is expressed as

space="preserve" listing-type="equation">R'"'"'(ρ

)=∂

R(ρ

)/∂

ρ

,

provided that the following conditions are satisfied;

space="preserve" listing-type="equation">R'"'"'(0.3)/R'"'"'(0.6)>

1,

space="preserve" listing-type="equation">R'"'"'(0.6)/R'"'"'(0.9)<

1,

where R(ρ

) is a shape of said optical low-pass filter relative to the radial direction and T(φ

) is a shape of said optical low-pass filter relative to the rotational direction.

16. An optical low-pass filter according to claim 1, wherein a gradient refractive index N(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to a rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">N(ρ

,φ

)=N0+Nr(ρ

)×

Nt(φ

),

and an amount of variation in refractive index, Nr'"'"'(ρ

), relative to the radial direction is expressed as

space="preserve" listing-type="equation">Nr'"'"'(ρ

)=∂

N(ρ

)/∂

ρ

,

provided that the following conditions are satisfied;

space="preserve" listing-type="equation">Nr'"'"'(0.3)/Nr'"'"'(0.6)>

1,

space="preserve" listing-type="equation">Nr'"'"'(0.6)/Nr'"'"'(0.9)>

1,

where N0 is a refractive index at the origin, Nr(ρ

) is a gradient refractive index relative to the radial direction, and Nt(φ

) is a gradient refractive index relative to the rotational direction.

17. An optical low-pass filter according to claim 1, wherein a wavefront aberration W(ρ

, φ

) which occurs in a pencil of rays transmitted through said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which p is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to a rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">W(ρ

,φ

)=Wr(ρ

)×

Wt(φ

),

and an amount of variation, Wr'"'"'(ρ

), in the wavefront aberration relative to the radial direction is expressed as

space="preserve" listing-type="equation">Wr'"'"'(ρ

)=∂

W(ρ

)/∂

ρ

,

provided that the following conditions are satisfied;

space="preserve" listing-type="equation">Wr(0.25)/Wr(0.75)<

0,

space="preserve" listing-type="equation">Wr'"'"'(0.3)/Wr'"'"'(0.6)<

0,

where Wr(ρ

) is a wavefront aberration relative to the radial direction and Wt(φ

) is a wavefront aberration relative to the rotational direction.

18. An optical low-pass filter according to claim 1, wherein a shape S(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to a rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">S(π

,φ

)=R(ρ

)×

T(+),

and an amount of variation in shape, R'"'"'(ρ

), relative to the radial direction is expressed as

space="preserve" listing-type="equation">R'"'"'(ρ

)=∂

R(ρ

)/∂

ρ

,

provided that the following conditions are satisfied;

space="preserve" listing-type="equation">R(0.25)/R(0.75)<

0,

space="preserve" listing-type="equation">R'"'"'(0.3)/R'"'"'(0.6)<

0,

where R(ρ

) is a shape of said optical low-pass filter relative to the radial direction and T(φ

) is a shape of said optical low-pass filter relative to the rotational direction.

19. An optical low-pass filter according to claim 1, wherein a gradient refractive index N(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to a rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">N(ρ

,φ

)=N0+Nr(ρ

)×

Nt(φ

),

and an amount of variation in refractive index, Nr'"'"'(ρ

), relative to the radial direction is expressed as

space="preserve" listing-type="equation">Nr'"'"'(ρ

)=∂

N(ρ

)/∂

ρ

,

provided that the following conditions are satisfied;

space="preserve" listing-type="equation">Nr(0.25)/Nr(0.75)<

0,

space="preserve" listing-type="equation">Nr'"'"'(0.3)/Nr'"'"'(0.6)<

0,

where N0 is a refractive index at the origin, Nr(ρ

) is a gradient refractive index function relative to the radial direction, and Nt(φ

) is a gradient refractive index function relative to the rotational direction.

20. An optical low-pass filter according to claim 1, wherein said phase advancing area and said phase retarding area exist with a predetermined period in a rotational direction centered at an origin corresponding to the center of the incident pencil of rays, said predetermined period differing from area to area in a radial direction.

21. An optical low-pass filter according to claim 20, wherein a wavefront aberration W(ρ

, φ

) which occurs in a pencil of rays transmitted through said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to the radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

##EQU23## where Wri(ρ

) is a wavefront aberration relative to the radial direction and mi and δ

i are constants.

22. An optical low-pass filter according to claim 21, wherein said optical low-pass filter satisfies the following condition:

space="preserve" listing-type="equation">m1<

m2.

23. An optical low-pass filter according to claim 1, wherein said phase advancing area and said phase retarding area are formed in a step-formed shape.

24. An optical low-pass filter according to claim 23, wherein said phase advancing area and said phase retarding area are alternately formed in the rotational direction centered at an origin corresponding to the center of the incident pencil of rays.

25. An optical low-pass filter according to claim 24, wherein a shape S(ρ

, φ

) of said optical low-pass filter is expressed as follows by a cylindrical coordinate system (ρ

, φ

) whose origin corresponds to the center of the incident pencil of rays and in which ρ

is a coordinate system (0≦

ρ

≦

1) relative to a radial direction of said optical low-pass filter, which coordinate system is standardized on a radius of an effective portion of said optical low-pass filter, and φ

is a coordinate system (0≦

φ

≦

2π

) relative to the rotational direction of said optical low-pass filter;

space="preserve" listing-type="equation">S(ρ

,φ

)=Step(R(ρ

)×

cos(mφ

+δ

)),

where R(ρ

) is a basic shape of said optical low-pass filter relative to the radial direction, δ

is a constant and Step(f) is a function for converting the continuous function f into a predetermined step function.

26. An optical low-pass filter according to claim 1, further comprising a shape which corrects an error occurring during molding.

27. An optical low-pass filter comprising:

an area having an optical path length longer than an optical path length of a center of said optical low-pass filter; and

an area having an optical path length shorter than the optical path length of the center of said optical low-pass filter,

said area having the longer optical path length and said area having the shorter optical path length being alternately formed in a generally non-linear pattern, and in a rotational direction centered at an origin corresponding to the center of the incident pencil of rays.

28. An optical apparatus comprising:

an image forming optical system;

an image pickup element; and

an optical low-pass filter,

said optical low-pass filter alternately including a phase advancing area which advances a phase of a wavefront of an incident pencil of rays with respect to a phase of a wavefront of a center of the incident pencil of rays, and a phase retarding area which retards the phase of the wavefront of the incident pencil of rays with respect to the phase of the wavefront of the center of the incident pencil of rays, said phase advancing area and said phase retarding area being alternately formed in a generally non-linear pattern, and in a rotational direction centered at an origin corresponding to the center of the incident pencil of rays.

29. An optical apparatus according to claim 28, wherein said optical low-pass filter is provided in a vicinity of a stop of said image forming optical system.

30. An optical apparatus according to claim 28, wherein said optical low-pass filter is arranged in such a manner that a direction in which its phase advancing or retarding action is large is inclined in the range of 30°

to 60°

with respect to a direction of array of pixels of said image pickup element.

31. An optical apparatus according to claim 28, wherein said optical low-pass filter is arranged in such a manner that a direction in which its phase advancing or retarding action is large is inclined by approximately 45°

with respect to a direction of array of pixels of said image pickup element.