Hybrid fiber-rod laser
View Patent ↗Single, or near single transverse mode waveguide definition is produced using a single homogeneous medium to transport both the pump excitation light and generated laser light. By properly configuring the pump deposition and resulting thermal power generation in the waveguide device, a thermal focusing power is established that supports perturbation-stable guided wave propagation of an appropriately configured single or near single transverse mode laser beam and/or laser pulse.
1. An apparatus, comprising;
a core of rod shaped optical material comprising a positive dn/dT, wherein said rod shaped optical material consists essentially of a single homogenous material having no substantial variation in index of refraction; and
a pump excitation source configured for optically pumping via longitudinal excitation said core with pump light, wherein said longitudinal excitation establishes a transverse thermal gradient in said rod according to said positive dn/dT, wherein said transverse thermal gradient produces a distributed thermal lens that supports perturbation stable guided wave propagation of single or near single transverse mode laser light by balancing the diffractive nature of said laser light with the focusing power of said distributed thermal lens as said laser light propagates along its path.
2. The apparatus of claim 1 , further comprising a lower refractive index optical material surrounding said core, wherein said pump excitation source is configured to input light into said lower refractive index optical material to establish said transverse thermal gradient in said rod.
3. The apparatus of claim 2 , further comprising an outer coating surrounding said lower refractive index optical material, wherein said outer coating comprises an index of refraction that is lower than that of said lower refractive index optical material.
4. The apparatus of claim 1 , wherein said rod comprises a laser gain media dopant, wherein said pump excitation source is further configured to generate gain in said core.
5. The apparatus of claim 4 , wherein said dopant is selected from the group consisting of Nd 3+ , Pm 3+ , Sm 3+ , Tb 3+ , Dy 3+ , Ho 3+ , Er 3+ , Tm 3+ , Yb 3+ and Cr 3+ .
6. The apparatus of claim 4 , wherein said dopant is distributed substantially uniformly throughout said transverse thermal gradient.
7. The apparatus of claim 1 , wherein said rod comprises a Raman gain media dopant.
8. The apparatus of claim 1 , wherein said core comprises fused silica.
9. The apparatus of claim 1 , wherein said core comprises a parabolic temperature profile.
10. The apparatus of claim 1 , wherein said transverse thermal gradient comprises a maximum index of refraction increase that will guarantee single mode operation.
11. The apparatus of claim 10 , where a is the radius of said core, wherein said index of refraction increase, Δn, comprises a maximum value according to the following relation,
2π/λ 0 a √{square root over (2 ·n·Δn )}<2.4.
12. The apparatus of claim 1 , wherein the beam waist of said laser light as it propagates is dependent on both the thermal source through the volume of said rod and the material properties of said rod according to the equation
ω
2
=
λ
0
π
2
κ
n
0
ⅆ
n
ⅆ
T
P
Th
′′′
,
where ω is the beam waist of said laser light, κ is the thermal conductivity of the material of said rod material, λ 0 is the vacuum wavelength of the laser light, n 0 is the refractive index of the rod material, dn/dT is the linear change of the refractive index of the rod material with temperature and P Th ′″ is the thermally dissipated power density.
13. A method, comprising;
providing a core of rod shaped optical material comprising a positive dn/dT, wherein said rod shaped optical material consists essentially of a single homogenous material having no substantial variation in index of refraction; and
optically pumping said core with pump light from a pump excitation source, wherein said pump light establishes a transverse thermal gradient in said rod according to said positive dn/dT, wherein said transverse thermal gradient produces a distributed thermal lens that supports perturbation stable guided wave propagation of single or near single transverse mode laser light by balancing the diffractive nature of said laser light with the focusing power of said distributed thermal lens as said laser light propagates along its path.
14. The method of claim 13 , further comprising a lower refractive index optical material surrounding said core, wherein said pump excitation source is configured to input light into said lower refractive index optical material to establish said transverse thermal gradient in said rod.
15. The method of claim 14 , further comprising an outer coating surrounding said lower refractive index optical material, wherein said outer coating comprises an index of refraction that is lower than that of said lower refractive index optical material.
16. The method of claim 13 , wherein said rod comprises a laser gain media dopant, wherein said pump excitation source is further configured to generate gain in said core.
17. The method of claim 16 , wherein said dopant is selected from the group consisting of Nd 3+ , Pm 3+ , Sm 3+ , Tb 3+ , Dy 3+ , Ho 3+ , Er 3+ , Tm 3+ , Yb 3+ and Cr 3+ .
18. The method of claim 16 , wherein said dopant is distributed substantially uniformly throughout said transverse thermal gradient.
19. The method of claim 13 , wherein said rod comprises a Raman gain media dopant.
20. The method of claim 13 , wherein said core comprises fused silica.
21. The method of claim 13 , wherein said core comprises a parabolic temperature profile.
22. The method of claim 13 , wherein said transverse thermal gradient comprises a maximum index of refraction increase that will guarantee single mode operation.
23. The method of claim 22 , where a is the radius of said core, wherein said index of refraction increase, Δn, comprises a maximum value according to the following relation,
2π/λ 0 a √{square root over (2 ·n·Δn )}<2.4.
24. The method of claim 13 , wherein the beam waist of said laser light as it propagates is dependent on both the thermal source through the volume of said rod and the material properties of said rod according to the equation
ω
2
=
λ
0
π
2
κ
n
0
ⅆ
n
ⅆ
T
P
Th
′′′
,
where ω is the beam waist of said laser light, κ is the thermal conductivity of the material of said rod material, λ 0 is the vacuum wavelength of the laser light, n 0 is the refractive index of the rod material, dn/dT is the linear change of the refractive index of the rod material with temperature and P Th ′″ is the thermally dissipated power density.