optical fibers and integrated optics

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UEF // University of Eastern Finland Characterization of a ring resonator Advanced Laboratory Practices, 26 th May 2016 Atri Halder Optical fibers and Integrated optics

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Page 1: Optical fibers and Integrated optics

UEF // University of Eastern Finland

Characterization of a ring resonatorAdvanced Laboratory Practices, 26th May 2016

Atri Halder

Optical fibers and Integrated optics

Page 2: Optical fibers and Integrated optics

Resonance

2Guiding in optical fibers / Atri Halder, 26.05.2016

If the frequency of the applied force matches with the natural frequency of any structure, then the amplitude of the field increases after each oscillation. This phenomena is known as resonance.

Y(λ) =

Page 3: Optical fibers and Integrated optics

Resonator

3Guiding in optical fibers / Atri Halder, 26.05.2016

A B

Page 4: Optical fibers and Integrated optics

Ring Resonator

4Guiding in optical fibers / Atri Halder, 26.05.2016

Resonance condition: = N. where, L = 2πR

R is the radius of the ring resonator. is the wavelength of light coupled to the input. is the effective refractive index of the waveguide.

Page 5: Optical fibers and Integrated optics

Full width at half maxima (FWHM)

5Guiding in optical fibers / Atri Halder, 26.05.2016

where is the group index of the medium, r is the self coupling coefficient, a is the resonator round trip loss coefficient and is the resonance wavelength.

FWHM =

Page 6: Optical fibers and Integrated optics

Free Spectral Range (FSR)

6Guiding in optical fibers / Atri Halder, 26.05.2016

FSR =

Page 7: Optical fibers and Integrated optics

Finesse

7Guiding in optical fibers / Atri Halder, 26.05.2016

Finesse =

Page 8: Optical fibers and Integrated optics

Quality Factor (Q-factor)

8Guiding in optical fibers / Atri Halder, 26.05.2016

It represents the number of oscillations required by the confined optical field to get its energy reduced to 1/e of the initial energy.

Q =

Page 9: Optical fibers and Integrated optics

Micro ring resonator

9Guiding in optical fibers / Atri Halder, 26.05.2016

Page 10: Optical fibers and Integrated optics

10

Specification of the ring resonator

Guiding in optical fibers / Atri Halder, 26.05.2016

Page 11: Optical fibers and Integrated optics

Experimental setup

11Guiding in optical fibers / Atri Halder, 26.05.2016

Page 12: Optical fibers and Integrated optics

Result: Reference

12Guiding in optical fibers / Atri Halder, 26.05.2016

Page 13: Optical fibers and Integrated optics

13Guiding in optical fibers / Atri Halder, 26.05.2016

Transmission spectrum of through port for a gap 300 nm.

Page 14: Optical fibers and Integrated optics

Guiding in optical fibers / Atri Halder, 26.05.2016

Enhanced resonance for a gap of 300 nm.

Page 15: Optical fibers and Integrated optics

Guiding in optical fibers / Atri Halder, 26.05.2016

Transmission spectrum of through port for a gap 400 nm.

Page 16: Optical fibers and Integrated optics

Guiding in optical fibers / Atri Halder, 26.05.2016

Enhanced resonance for a gap of 400 nm.

Page 17: Optical fibers and Integrated optics

17Guiding in optical fibers / Atri Halder, 26.05.2016

Transmission spectrum of drop port for a gap 400 nm.

Page 18: Optical fibers and Integrated optics

18Guiding in optical fibers / Atri Halder, 26.05.2016

Transmission spectrum of through and drop port for a gap 400 nm.

Page 19: Optical fibers and Integrated optics

Comparison

19Guiding in optical fibers / Atri Halder, 26.05.2016

Page 20: Optical fibers and Integrated optics

Comparison

20Guiding in optical fibers / Atri Halder, 26.05.2016

Characteristics Gap of 300 nm Gap of 400 nm

FWHM 0.55 nm 0.475 nm

FSR 1.507 nm 1.526 nm

Finesse 2.74 3.21

Q-factor 3005.7 3291.25

Loss 18.40 dB/cm 15.84 dB/cm

Page 21: Optical fibers and Integrated optics

Conclusion

21Guiding in optical fibers / Atri Halder, 26.05.2016

• There was a high loss in between the bus and the ring.• The structure was so small that there was always a problem of coupling.

• As the gap between the bus and the ring was increased, the resonance varied a lot and we can conclude that for a gap of 400 nm the resonance was best.

• The whole experimental work was quite challenging.• Though we got a good result for different parameters of the ring resonator, we failed to generate good data for the drop port. It was due to imperfections of the structure and lot of dust particles on the sample.

Page 22: Optical fibers and Integrated optics

Thank you!

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