Laser composition for preventing photo-induced damage

• US 6,154,598 A
• Filed: 12/22/1997
• Issued: 11/28/2000
• Est. Priority Date: 12/22/1997
• Status: Expired due to Term

• Current Assignee: Hanger Solutions, LLC (IP Investments Group LLC)
• Original Assignee: Polaroid Corporation (PLR IP Holdings LLC)
• Inventors: Goyal, Anish K., Singh, Shobha, Gavrilovic, Pavle, Po, Hong
• Primary Examiner(s): Lee, John D.
• Assistant Examiner(s): NGUYEN, TRAM A
• Application Number:
  US08/995,445
• Time in Patent Office: 1,072 Days
• Field of Search: 385/123, 385/141.2, 372/6.41, 359/341
• US Class Current: 385/141
• CPC Class Codes: H01S 3/06716 Fibre compositions per se C03C13/04or doping with active elements lasing materials in general H01S3/14
• CPC Class Codes: H01S 3/094092 Upconversion pumping
• CPC Class Codes: H01S 3/1603 rare earth
• CPC Class Codes: H01S 3/1698 rare earth

Abstract

An optical waveguide laser, preferably a fiber laser, has unintentionally incorporated impurities disposed in the lasing medium which upconvert a portion of the lasing radiation to radiation of shorter wavelength, thereby introducing defects in the medium which result in increased absorption due to photodarkening. Suitable rare-earth co-dopants are intentionally incorporated during the manufacture of the fiber for effectively shunting the upconversion process. The lifetime of the fiber laser is thereby increased.

Claims

1. An optical medium having propagating therein an intense beam of optical radiation of a first wavelength, the medium containing a plurality of first dopant atoms having a ground state and plurality of excited state levels spaced apart in energy from the ground state such as to be capable of absorbing at least a portion of said optical radiation, said absorbed optical radiation raising a first portion of said first dopant atoms from the ground state to a first excited state and subsequently raising a second portion of said dopant atoms from substantially said first excited state to a second excited state having an energy relative to the ground state of substantially twice the energy of the absorbed optical radiation, the medium further comprising:

a plurality of second dopant atoms, said second dopant atoms having a ground state and at least one excited state spaced apart in energy from the ground state such as to be substantially transparent to said first wavelength, said at least one excited state of the second dopant atoms having an energy level substantially equal to the energy level of at least one of the excited states of the first dopant atoms, wherein said first dopant atoms are de-excited by transferring energy from said at least one excited state of said first dopant atoms to the at least one excited state of the second dopant atoms having an energy state substantially equal to the energy level of said at least one of the excited states of the first dopant atoms, thereby reducing the number of first dopant atoms in the at least one excited state of said first dopant atom.

2. The optical medium of claim 1, wherein said second portion of said first dopant atoms relaxes to an energy level lower in energy than said at least one excited state of the first dopant before being raised by said optical radiation to a second excited state of the first dopant.

3. The optical medium of claim 1 further comprising a plurality of lasing atoms having energy levels capable of generating the intense beam of optical radiation of the first wavelength in response to pump radiation from an external optical pump source.

4. The optical medium of claim 3, wherein said lasing atoms comprises rare earth atoms selected from the group consisting of Nd³⁺ and Yb³⁺.

5. The optical medium of claim 1, wherein said first dopant atom comprise rare earth atoms selected from the group consisting of Tm³⁺, Ho³⁺ and Er³⁺.

6. The optical medium of claim 1, wherein said second dopant atoms comprise rare earth ions selected from the group consisting of Nd³⁺, Tb³⁺ and Eu³⁺.

7. The optical medium of claim 1, wherein said first wavelength is substantially in the range of between 0.9 μ

m and 1.2 μ

m.

8. An optical waveguide comprising:

a core having an index of refraction n1 and comprising a lasing medium, said core disposed in a cladding having an index of refraction n2 which is smaller than the index of refraction n1;

said lasing medium having disposed therein a plurality of lasing dopant atoms for generating lasing radiation having a lasing wavelength characteristic of lasing transitions between electronic states of said lasing atoms, said lasing radiation generated in response to absorption of pump radiation from an external optical pump source;

said lasing medium farther comprising a plurality of first dopant atoms having a ground state and plurality of energy levels spaced apart in energy from the ground state such as to be capable of absorbing at least a portion of said lasing radiation, said absorbed lasing radiation raising a first portion of said first dopant atoms from the ground state to a first energy level of said first dopant atom and subsequently raising a second portion of said dopant atoms from substantially said first energy level to a second energy level of said first dopant atom having an energy relative to the ground state of substantially twice the energy of the absorbed lasing radiation, the lasing medium further comprising;

a plurality of second dopant atoms, said second dopant atoms having a ground state and at least one energy level spaced apart in energy from the ground state such as to be substantially transparent to at least one of the optical radiation at said first wavelength and the pump radiation, said at least one energy level of the second dopant atoms having an energy substantially equal to the first energy level of the first dopant atoms, wherein said first portion of the first dopant atoms in said first energy level of said first dopant atoms is transferred at least partially to the at least one spaced apart energy level of the second dopant atoms having an energy state substantially equal to said energy level of at least one of the excited states of the first dopant atoms and subsequently transitions to the ground state, thereby reducing the number of first dopant atoms in the first energy level of said first dopant atom capable of being raised by said optical radiation to said second energy level of said first dopant atom.

9. The optical waveguide of claim 8, wherein said optical waveguide is an optical fiber.

10. The optical waveguide of claim 8, further comprising a further cladding having an index of refraction n₃ and surrounding said cladding, wherein n₂ >

n₃.

11. The optical waveguide of claim 8, wherein said lasing atoms comprises rare earth atoms selected from the group consisting of Nd³⁺ and yb³⁺.

12. The optical waveguide of claim 11, wherein said lasing atoms have a concentration substantially in the range of 0.5×

10²⁰ atoms/cm³ to 5×

10²⁰ atoms/cm³.

13. The optical waveguide of claim 8, wherein said first dopant atom comprise rare earth atoms selected from the group consisting of Tm³⁺, Ho³⁺ and Er³⁺.

14. The optical waveguide of claim 8, wherein said second dopant atoms comprise rare earth atoms selected from the group consisting of Nd³⁺, Tb³⁺ and Eu³⁺.

15. The optical waveguide of claim 14, wherein said second dopant atoms have a concentration substantially in the range of 1×

10¹⁶ atoms/cm³ to 5×

10²⁰ atoms/cm³.

16. The optical waveguide of claim 8, wherein said lasing radiation has a wavelength substantially in the range of between 0.9 μ

m and 1.2 μ

m.

17. The optical waveguide of claim 8, wherein said pump radiation has a wavelength substantially in the range of 0.8 μ

m to 1.0 μ

m.

18. An optical medium having propagating therein an intense beam of optical radiation of a first wavelength and comprising first dopant atoms having excited energy states, said radiation capable of undergoing upconversion to wavelengths shorter than said first wavelength through excitation of said first dopant atoms to at least one of said excited states by said optical radiation, said medium further comprising second dopant atoms having excited energy states, said second dopant atoms capable of receiving energy at an excited energy level from at least one of excited energy states of said first dopant atoms and capable of de-exciting at least one of said excited energy states of said first dopant atom, thereby effectively shunting the upconversion.

19. Method for preventing upconversion of lasing or pump radiation in optical fiber lasers having a lasing core with an index of refraction n, disposed in a cladding surrounding said core and having an index of refraction n2, wherein n,>

n2, said fiber lasers converting pump radiation into lasing radiation, said upconversion caused by optical transitions to excited states of first dopant atoms present in at least one of said lasing core or cladding, the method comprising doping at least one of the lasing core or cladding with a second dopant atom having excited energy states, said second dopant atoms capable of receiving energy at an excited energy level from at least one of excited energy states of said first dopant atoms and capable of deexciting the excited states of the first dopant atoms such as to effectively shunting said upconversion.

20. The method of claim 19, wherein said first dopant atom comprise rare earth atoms selected from the group consisting of Tm³⁺, Ho³⁺ and Er³⁺.

21. The method of claim 19, wherein said second dopant atoms comprise rare earth atoms selected from the group consisting of Nd³⁺, Tb³⁺ and Eu³⁺.