PASSIVELY-THERMALLY-STABILIZED PHOTONIC APPARATUS, METHOD, AND APPLICATONS

• US 20110102804A1
• Filed: 11/01/2010
• Published: 05/05/2011
• Est. Priority Date: 11/02/2009
• Status: Active Grant

• Current Assignee: Cornell University
• Original Assignee: Cornell University
• Inventors: Guha, Biswajeet, Lipson, Michal
• Granted Patent: US 8,457,453 B2
• Time in Patent Office: Days
• US Class Current: 356/480
• CPC Class Codes: G02B 6/12007 forming wavelength selective elements, e.g. multiplexer, demultiplexer
• CPC Class Codes: G02B 6/29343 Cascade of loop resonators
• CPC Class Codes: G02B 6/29353 with a wavelength selective element in at least one light guide interferometer arm, e.g. grating, interference filter, resonator

Abstract

Apparatus and methods that compensate for the thermally-induced drift of the resonance frequency of a closed-loop resonator include, in an exemplary embodiment, a waveguide-based Mach-Zehnder interferometer (MZI) and an overcoupled, waveguide-based microring resonator. The temperature-induced red-shifting ring resonance can be balanced by a spectral blueshift with temperature of the MZI. To stabilize the resonance of the ring at a given wavelength, the change in optical path lengths with temperature of the ring and the MZI should be equal and opposite. The interplay of nonlinear change in phase of ring resonator with temperature and linear change in phase of MZI with temperature, along with matching the period of this phase change, gives rise to perfect oscillation in the combined system resonance with temperature.

Claims

1. A photonic apparatus, comprising:

an interferometer having a second arm, wherein the interferometer is characterized by a negative net optical path length change as a function of temperature, δ

L_M/δ

T; and

a waveguide closed loop resonator characterized by a positive optical path length change as a function of temperature, δ

L_R/δ

T, disposed in light-coupling proximity to the second interferometer arm, wherein the absolute value of δ

L_M/δ

T is equal to the absolute value of δ

L_R/δ

T, such that the apparatus is characterized by a resonance having substantially no spectral shift as a function of temperature, wherein the apparatus is an athermal/temperature insensitive, resonant photonic device.

2. The apparatus of claim 1, wherein the interferometer further comprises:

a first waveguide arm having a length L₁ wherein at least a portion of the first waveguide arm, L_1W(1), has a width w₁, and an effective mode index n_eff(1); and

,

wherein the second arm is a waveguide having a length L₂ and a width w₁, wherein at least a portion of the second waveguide arm, L_2W(2), has a maximum width w₂ that is less than w₁ over L_2W(2), and the second waveguide arm is optically coupled to the first waveguide arm,

further wherein the interferometer is characterized by an effective mode index n_eff(2), where |L₂−

L₁|=Δ

L≠

0, L_2W(2)=L_1W(1), w₁−

w₂=Δ

w, and |n_eff(2)−

n_eff(1)|=Δ

n_eff≠

0.

3. The apparatus of claim 1, wherein the interferometer is a waveguide-based Mach-Zehnder interferometer (MZI).

4. The apparatus of claim 1, wherein the closed loop waveguide resonator is a ring resonator having a radius, R.

5. The apparatus of claim 1, wherein the interferometer and the closed loop resonator are integrated on a chip.

6. The apparatus of claim 2, wherein the first and second waveguide arms are each in the form of a coil.

7. The apparatus of claim 1, further characterized by a controllable positive or negative temperature sensitivity.

8. The apparatus of claim 7, characterized by a negative temperature sensitivity having a magnitude equal to or less than −

0.005 nanometers per degree Kelvin (nm/K).

9. The apparatus of claim 7, characterized by a negative temperature sensitivity equal to or less than −

0.5 nm/K.

10. The apparatus of claim 1, wherein the interferometer is further characterized by an interference order, M, where M can be any positive or negative integer or zero at Δ

λ

/Δ

T=0, where Δ

λ

/Δ

T represents the temperature sensitivity of any wavelength value within a given wavelength spectrum.

11. The apparatus of claim 2, wherein the second waveguide arm is tapered over transition regions between L₂ and L_2W(2).

12. The apparatus of claim 1, characterized by an optical resonance that oscillates about a central wavelength with change of temperature.

13. The apparatus of claim 2, characterized by a temperature-dependent transmission function,

ρ

(T)=½

{1+[(t−

α

exp(iβ

L_R(T)))/(1−

α

texp(iβ

L_R(T)))]exp(iβ

L_MZI(T))},

where t is the through-coupling of the ring to the second waveguide arm, (1−

α

) is the round-trip loss in the ring, L_R is the net optical path length of the ring, and L_MZI is the net optical path length of the MZI.

14. The apparatus of claim 3, further comprising only a single MZI and a plurality, n, of waveguide ring resonators serially disposed in light-coupling proximity to the second arm, wherein each ring resonator has a different radius, R_n.

15. The apparatus of claim 14, where each resonator has a resonance such that the resonances are spectrally equidistant and non-overlapping, where λ

_n−

λ

_n-1=(Free spectral range of any resonator)/n.

16. The apparatus of claim 14, wherein the apparatus is a temperature insensitive electro-optic modulator.

17. A method for stabilizing the temperature-induced drift of the optical resonance of a closed loop resonator at a given wavelength, comprising:

providing a closed loop resonator characterized by a phase spectrum in the form of a resonance that non-linearly red-shifts in wavelength with increase in temperature and phase at any given wavelength; and

providing a matching phase spectrum that changes linearly with temperature at the given wavelength,

wherein the matched phase spectrums have a phase change from Φ

₀ to Φ

₀+2π

over the temperature change (Δ

T).

18. The method of claim 17, wherein the closed loop resonator has a positive optical path length change as a function of temperature, δ

L_R/δ

T, and the step of providing a matching phase spectrum further includes coupling light from the closed loop resonator to an arm of an interferometer that is characterized by a negative net optical path length change as a function of temperature, δ

L_M/δ

T, where the absolute value of δ

L_M/δ

T is equal to the absolute value of δ

L_R/δ

T.

19. The method of claim 18, wherein the interferometer is a waveguide-based Mach-Zehnder interferometer (MZI).