Patent US5319494A successfully refreshed from Google Patents.
← Back to Patent Explorer
US5319494A Expired / Lapsed US ⏱️ 0.0 years remaining

Light waveguide type polarized light beam splitter

Assignee: Pioneer Corp
•
Filing: 1992-10-28
•
Granted: 1994-06-07
•
Expires: 2012-10-28
📄 Original PDF 🌐 Google Patents 🔄 Sync Now

Abstract

Abstract A polarized beam splitter is provided for transmitting a beam of linearly polarized light vibrating in a predetermined plane. A titanium diffused layer is developed on the lithium niobate substrate and then, a portion of the same is treated by proton exchange thus forming a proton exchanged region. The boundary surface between the titanium diffused and proton exchanged regions is used as a polarizing plane allowing an incoming polarized light vibrating in the predetermined plane to pass through and a polarized light vibrating at a right angle to the plane to reflect.

Inventors

  • 👤 Satoshi Miyaguchi
  • 👤 Atoshi Onoe

Bibliographic Details

Application Number —
Jurisdiction US
Data Source google_patents
Last Synchronized 2026-11-08 15:56
CPC Classifications
G; G02; G02B; G02B27/00; G02B27/10; G02B27/14; G02B27/142; G02B27/28; G02B27/283

Claims Analysis

Total Claims: 4
Claim 1
Independent Claim 241 words
A light waveguide type polarized light beam splitter comprising: a first region; a second region; and a boundary surface formed between said first region and said second region; wherein: said first region is a titanium diffused layer developed through diffusion of titanium into a lithium niobate substrate; said second region is a portion of the titanium diffused layer treated by a proton exchange process; said first region and said second region have differing refractive indices; said beam splitter is configured to pass an incident linearly polarized light beam, oscillating in a predetermined plane, propagating in a predetermined direction and entering the beam splitter via said second region, through said boundary surface, and is configured to reflect a return light beam, oscillating in a shifted plane of polarization, propagating in a return direction and entering the beam splitter via said first region, at said boundary surface; said boundary surface is inclined by an angle of θ 1 with respect to the direction of propagation of the linearly polarized light, and is inclined by an angle of θ 2 with respect to the direction of propagation of the return light beam; and the angle θ 2 is determined to satisfy the condition of °<θ.sub. ≦ cos.sup.-1 (n.sub.oP /n.sub.oT) wherein n oT represents a refractive index of the titanium diffused layer against ordinary rays, and n oP represents a refractive index of said second region treated by the proton exchange process against ordinary rays.
Claim 2
Dependent Claim 241 words
A light waveguide type polarized light beam splitter comprising: a first region; a second region; and a boundary surface formed between said first region and said second region; wherein: said first region is a titanium diffused layer developed through diffusion of titanium into a lithium niobate substrate; said second region is a portion of the titanium diffused layer treated by a proton exchange process; said first region and said second region have differing refractive indices; said beam splitter is configured to pass an incident linearly polarized light beam, oscillating in a predetermined plane, propagating in a predetermined direction and entering the beam splitter via said second region, through said boundary surface, and is configured to reflect a return light beam, oscillating in a shifted plane of polarization, propagating in a return direction and entering the beam splitter via said first region, at said boundary surface; said boundary surface is inclined by an angle of θ 1 with respect to the direction of propagation of the linearly polarized light, and is inclined by an angle of θ 2 with respect to the direction of propagation of the return light beam; and the angle θ 2 is determined to satisfy the condition of °<θ.sub. ≦ cos.sup.-1 (n.sub.oP /n.sub.oT) wherein n oT represents a refractive index of the titanium diffused layer against ordinary rays, and n oP represents a refractive index of said second region treated by the proton exchange process against ordinary rays.
Claim 3
Dependent Claim 229 words
A light waveguide type polarized light beam splitter comprising: a first region; a second region; and a boundary surface formed between said first region and said second region; wherein: said first region is a titanium diffused layer developed through diffusion of titanium into a lithium niobate substrate; said second region is a portion of the titanium diffused layer treated by a proton exchange process; said first region and said second region have differing refractive indices; said beam splitter is configured to pass an incident linearly polarized light beam, oscillating in a predetermined plane, propagating in a predetermined direction and entering the beam splitter via said second region, through said boundary surface, and is configured to reflect a return light beam, oscillating in a shifted plane of polarization, propagating in a return direction and entering the beam splitter via said first region, at said boundary surface; said boundary surface is inclined by an angle of θ 1 with respect to the direction of propagation of the linearly polarized light, and is inclined by an angle of θ 2 with respect to the direction of propagation of the return light beam, and a λ/4 plate and a reflection plane positioned outside the beam splitter are provided for shifting the plane of polarization and altering the direction of propagation of the passed linearly polarized light beam, for producing the return light beam.
Claim 4
Dependent Claim 229 words
A light waveguide type polarized light beam splitter comprising: a first region; a second region; and a boundary surface formed between said first region and said second region; wherein: said first region is a titanium diffused layer developed through diffusion of titanium into a lithium niobate substrate; said second region is a portion of the titanium diffused layer treated by a proton exchange process; said first region and said second region have differing refractive indices; said beam splitter is configured to pass an incident linearly polarized light beam, oscillating in a predetermined plane, propagating in a predetermined direction and entering the beam splitter via said second region, through said boundary surface, and is configured to reflect a return light beam, oscillating in a shifted plane of polarization, propagating in a return direction and entering the beam splitter via said first region, at said boundary surface; said boundary surface is inclined by an angle of θ 1 with respect to the direction of propagation of the linearly polarized light, and is inclined by an angle of θ 2 with respect to the direction of propagation of the return light beam, and a λ/4 plate and a reflection plane positioned outside the beam splitter are provided for shifting the plane of polarization and altering the direction of propagation of the passed linearly polarized light beam, for producing the return light beam.

References Cited (Backward Citations)

US3401590A Cited
US3563633A Cited
JPS53111743A Cited
JPS57167006A Cited
US4778234A Cited
US4691984A Cited
US4725774A Cited
US4991937A Cited
US5029988A Cited
US5070488A Cited
US5078482A Cited

USPTO Annuity & Maintenance Windows

Annuity Stage Window Opens Payment Deadline Surcharge Period Until Estimated Fee Status
3.5 Years (Year 4) 1997-06-06 1997-12-06 1998-06-07 $2000.00 Window Closed / Lapsed
7.5 Years (Year 8) 2001-06-06 2001-12-06 2002-06-07 $3760.00 Window Closed / Lapsed
11.5 Years (Year 12) 2005-06-06 2005-12-06 2006-06-07 $7700.00 Window Closed / Lapsed

Assigned Categories & Tags

No categories assigned to this patent yet.

Assign Category Tag