IP Library › Granted Patent US 9,910,198
Granted Patent B2
US 9,910,198 · App. 14/603,724 · Granted Mar 6, 2018

Optical filter and optical apparatus

Inventor: Kei Ueda (Utsunomiya, JP)
Assignee: CANON KABUSHIKI KAISHA
G02B5/285
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Quick Facts
Patent No.
US 9,910,198
App. No.
14/603,724
Granted
Mar 6, 2018
Kind
B2
Abstract

An optical filter includes a first multi-layer having a width W 1 and including a first optical layer and a second optical layer that are made of materials different from each other and that are alternately laminated, the first optical layer having a refractive index nH and an average layer thickness dH, and the second optical layer having a refractive index nL lower than nH and an average layer thickness dL, a second multi-layer having a width W 2 and including the first and the second optical layers alternately laminated, the first and the second multi-layers are included in each of unit structures arranged being shifted from each other by a shift amount D in a lamination direction of the first and the second optical layers, and predetermined conditions are satisfied.

Claims (41)

1. An optical filter comprising:

a first multi-layer having a width W 1 and including a first optical layer and a second optical layer that are made of materials different from each other and that are alternately laminated, the first optical layer having a refractive index nH and an average layer thickness dH, and the second optical layer having a refractive index nL lower than the refractive index nH and an average layer thickness dL; and

a second multi-layer having a width W 2 and including the first and the second optical layers alternately laminated,

wherein the first and the second multi-layers are included in each of unit structures arranged being shifted from each other by a shift amount D in a lamination direction of the first and the second optical layers, the unit structures being arranged in an array direction orthogonal to the lamination direction, and

expressions below are satisfied:

15°<φ<35°

1.8 <dH/dL< 5.0

( W 1 +W 2)<0.85*λ 0

where an inclination angle φ of each of the unit structures is defined to be tan −1 (|D|/0.5(W 1 +W 2 )) for |D| not greater than 0.5(dL+dH) and tan −1 (((dL+dH)−|D|)/0.5(W 1 +W 2 )) for |D| greater than 0.5(dL+dH), |θ|max and |θ|min respectively represent a maximum value and a minimum value of an absolute value of an incident angle range of a light beam on an incident plane parallel to the lamination direction and the array direction, and λ 0 represents a reflection center wavelength of P polarized light for an incident angle (|θ|max+|θ|min)/2.

2. The optical filter according to claim 1 , wherein expressions below are satisfied:

|Δλplus|<30 nm

cos|θ|min−cos|θ|max>0.365

where λplus represents a wavelength at a reflectance of 50% on a skirt on a long wavelength side of a reflection band of the optical filter, and Δλplus represents a wavelength shift amount when an incident angle of P polarized light is changed from |θ|min to |θ|max.

3. The optical filter according to claim 2 , wherein the average layer thicknesses dH and dL and the refractive indices nH and nL satisfy an expression below:

0.35*λ 0 <( nH*dH+nL*dL )cos φ<0.65*λ 0

where λ 0 represents a reflection center wavelength of P polarized light for an incident angle (|θ|max+|θ|min)/2.

4. The optical filter according to claim 1 , wherein an expression below is satisfied:

0.5(|θ|max+|θ|min)/2<sin −1 ( n eff *sin φ)<1.5(|θ|max+|θ|min)/2

where |θ|max and |θ|min respectively represent a maximum value and a minimum value of an absolute value of an incident angle range of a light beam, and n eff is defined to be {2/(1/nH 2 +1/nL 2 )} 1/2 .

5. The optical filter according to claim 1 , wherein the shift amount D satisfies an expression below:

0.25( dH+dL )≦| D|≦ 0.75( dH+dL ).

6. The optical filter according to claim 1 , wherein an expression below is satisfied:

0.5≦( W 1+ W 2)/ P≦ 1

where P represents a distance between centers of neighboring unit structures among the unit structures.

7. The optical filter according to claim 1 , wherein an untidiness Δz of the shift amount D between neighboring unit structures in the lamination direction satisfies an expression below:

0≦Δ z≦ 2( dH+dL ).

8. The optical filter according to claim 1 , wherein the width W 1 of the first multi-layer and the width W 2 of the second multi-layer satisfy expressions below:

W 1> W 2

W 1/( W 1+ W 2)≦0.8.

9. The optical filter according to claim 1 , wherein the first and the second multi-layers each include a ripple lowering layer.

10. The optical filter according to claim 9 , wherein the ripple lowering layer has a refractive index between the refractive index nH and the refractive index nL.

11. The optical filter according to claim 9 , wherein the ripple lowering layer includes third and fourth optical layers.

12. An optical apparatus comprising an optical filter, wherein the optical filter includes:

a first multi-layer having a width W 1 and including a first optical layer and a second optical layer that are made of materials different from each other and that are alternately laminated, the first optical layer having a refractive index nH and an average layer thickness dH, and the second optical layer having a refractive index nL lower than the refractive index nH and an average layer thickness dL; and

a second multi-layer having a width W 2 and including the first and the second optical layers alternately laminated,

wherein the first and the second multi-layers are included in each of unit structures arranged being shifted from each other by a shift amount D in a lamination direction of the first and the second optical layers, the unit structures being arranged in an array direction orthogonal to the lamination direction, and

expressions below are satisfied:

15°<φ<35°

1.8< dH/dL< 5.0

( W 1+ W 2)<0.85*λ 0

where an inclination angle φ of each of the unit structures is defined to be tan −1 (|D|/0.5 (W 1 +W 2 )) for |D| not greater than 0.5(dL+dH) and tan −1 (((dL+dH)−|D|)/0.5(W 1 +W 2 )) for |D| greater than 0.5(dL+dH), |θ|max and |θ|min respectively represent a maximum value and a minimum value of an absolute value of an incident angle range of a light beam on an incident plane parallel to the lamination direction and the array direction, and λ 0 represents a reflection center wavelength of P polarized light for an incident angle (|θ|max+|θ|min)/2.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 3, 2015
From: UEDA, KEI
To: CANON KABUSHIKI KAISHA
Reel/Frame 035781/0869 →
Priority Claims (1)
JP 2014-013869 · Jan 29, 2014 · national
Continuity (1)
Related Publication 20150212245A1 · Jul 30, 2015