SlideShare a Scribd company logo
1 of 22
UEF // University of Eastern Finland
Characterization of a ring resonator
Advanced Laboratory Practices, 26th May 2016
Atri Halder
Optical fibers and Integrated optics
Resonance
2
Guiding 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) =
1
π
2𝑎
(λ−λ0)2+𝑎2
Resonator
3
Guiding in optical fibers / Atri Halder, 26.05.2016
A B
Ring Resonator
4
Guiding in optical fibers / Atri Halder, 26.05.2016
Resonance condition: L × 𝑛 𝑒𝑓𝑓 = N. λ 𝑑
where, L = 2πR
R is the radius of the ring resonator.
λ 𝑑 is the wavelength of light coupled to the
input.
𝑛 𝑒𝑓𝑓 is the effective refractive index of the
waveguide.
Full width at half maxima (FWHM)
5
Guiding in optical fibers / Atri Halder, 26.05.2016
where 𝑛 𝑔 is the group index of the medium, r is the self coupling
coefficient, a is the resonator round trip loss coefficient and λ 𝑟𝑒𝑠 is the
resonance wavelength.
FWHM =
(1−𝑟𝑎)λ 𝑟𝑒𝑠
2
π𝑛 𝑔 𝐿 𝑟𝑎
Free Spectral Range (FSR)
6
Guiding in optical fibers / Atri Halder, 26.05.2016
FSR =
λ 𝑟𝑒𝑠
2
𝑛 𝑔 𝐿
Finesse
7
Guiding in optical fibers / Atri Halder, 26.05.2016
Finesse =
𝐹𝑆𝑅
𝐹𝑊𝐻𝑀
Quality Factor (Q-factor)
8
Guiding 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 =
λ 𝑟𝑒𝑠
𝐹𝑊𝐻𝑀
Micro ring resonator
9
Guiding in optical fibers / Atri Halder, 26.05.2016
10
Specification of the ring resonator
Guiding in optical fibers / Atri Halder, 26.05.2016
Experimental setup
11
Guiding in optical fibers / Atri Halder, 26.05.2016
Result: Reference
12
Guiding in optical fibers / Atri Halder, 26.05.2016
13
Guiding in optical fibers / Atri Halder, 26.05.2016
Transmission spectrum of through port for a gap 300 nm.
Guiding in optical fibers / Atri Halder, 26.05.2016
Enhanced resonance for a gap of 300 nm.
Guiding in optical fibers / Atri Halder, 26.05.2016
Transmission spectrum of through port for a gap 400 nm.
Guiding in optical fibers / Atri Halder, 26.05.2016
Enhanced resonance for a gap of 400 nm.
17
Guiding in optical fibers / Atri Halder, 26.05.2016
Transmission spectrum of drop port for a gap 400 nm.
18
Guiding in optical fibers / Atri Halder, 26.05.2016
Transmission spectrum of through and drop port for a
gap 400 nm.
Comparison
19
Guiding in optical fibers / Atri Halder, 26.05.2016
Comparison
20
Guiding 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
Conclusion
21
Guiding 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.
Thank you!
uef.fi

More Related Content

What's hot

optical fiber and laser
optical fiber and laseroptical fiber and laser
optical fiber and laser
sweety13696
 
Mode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr Effect
Mode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr EffectMode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr Effect
Mode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr Effect
Kyle McSwain
 
Design edge- and side-coupled microstrip ring resonators
Design edge- and side-coupled microstrip ring resonatorsDesign edge- and side-coupled microstrip ring resonators
Design edge- and side-coupled microstrip ring resonators
Neelam Chopade
 
Frequency wavelength trapping by integrated ring resonators for secured netwo...
Frequency wavelength trapping by integrated ring resonators for secured netwo...Frequency wavelength trapping by integrated ring resonators for secured netwo...
Frequency wavelength trapping by integrated ring resonators for secured netwo...
University of Malaya (UM)
 
Resonator design
Resonator designResonator design
Resonator design
AJEET KUMAR
 
Fabry–pérot interferometer picoseconds dispersive properties
Fabry–pérot interferometer picoseconds dispersive propertiesFabry–pérot interferometer picoseconds dispersive properties
Fabry–pérot interferometer picoseconds dispersive properties
IAEME Publication
 
ConorWilman_Manchester_Investigation of an effective low-cost THz TDS system
ConorWilman_Manchester_Investigation of an effective low-cost THz TDS systemConorWilman_Manchester_Investigation of an effective low-cost THz TDS system
ConorWilman_Manchester_Investigation of an effective low-cost THz TDS system
Conor Wilman
 
Fiber otdr testing
Fiber otdr testingFiber otdr testing
Fiber otdr testing
bsateeshbsnl
 

What's hot (20)

Laser ii 1 ppt
Laser ii 1 pptLaser ii 1 ppt
Laser ii 1 ppt
 
optical fiber and laser
optical fiber and laseroptical fiber and laser
optical fiber and laser
 
The optical time domain reflectometer
The optical time domain reflectometerThe optical time domain reflectometer
The optical time domain reflectometer
 
Optical Time Domain Reflector
Optical Time Domain ReflectorOptical Time Domain Reflector
Optical Time Domain Reflector
 
Laser ii 2 ppt
Laser ii 2 pptLaser ii 2 ppt
Laser ii 2 ppt
 
Mode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr Effect
Mode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr EffectMode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr Effect
Mode-Locked Erbium Doped Pulse Fiber Laser Using the Kerr Effect
 
OPTICAL TIME DOMAIN REFLECTOMETRY-OTDR
OPTICAL TIME DOMAIN REFLECTOMETRY-OTDROPTICAL TIME DOMAIN REFLECTOMETRY-OTDR
OPTICAL TIME DOMAIN REFLECTOMETRY-OTDR
 
OTDR(OPTICAL TIME DOMAIN REFLECTOMETER)
OTDR(OPTICAL TIME DOMAIN REFLECTOMETER)OTDR(OPTICAL TIME DOMAIN REFLECTOMETER)
OTDR(OPTICAL TIME DOMAIN REFLECTOMETER)
 
Design of Rare Earth Ion Doped Polymer Waveguide Lasers
Design of Rare Earth Ion Doped Polymer Waveguide LasersDesign of Rare Earth Ion Doped Polymer Waveguide Lasers
Design of Rare Earth Ion Doped Polymer Waveguide Lasers
 
Design edge- and side-coupled microstrip ring resonators
Design edge- and side-coupled microstrip ring resonatorsDesign edge- and side-coupled microstrip ring resonators
Design edge- and side-coupled microstrip ring resonators
 
Frequency wavelength trapping by integrated ring resonators for secured netwo...
Frequency wavelength trapping by integrated ring resonators for secured netwo...Frequency wavelength trapping by integrated ring resonators for secured netwo...
Frequency wavelength trapping by integrated ring resonators for secured netwo...
 
Laser and optical fiber
Laser and optical fiberLaser and optical fiber
Laser and optical fiber
 
Resonator design
Resonator designResonator design
Resonator design
 
A1070109
A1070109A1070109
A1070109
 
Fabry–pérot interferometer picoseconds dispersive properties
Fabry–pérot interferometer picoseconds dispersive propertiesFabry–pérot interferometer picoseconds dispersive properties
Fabry–pérot interferometer picoseconds dispersive properties
 
radar principles
   radar principles    radar principles
radar principles
 
ConorWilman_Manchester_Investigation of an effective low-cost THz TDS system
ConorWilman_Manchester_Investigation of an effective low-cost THz TDS systemConorWilman_Manchester_Investigation of an effective low-cost THz TDS system
ConorWilman_Manchester_Investigation of an effective low-cost THz TDS system
 
IRJET- Distance Measurement with the Help of Ultrasonic Sensor
IRJET-  	  Distance Measurement with the Help of Ultrasonic SensorIRJET-  	  Distance Measurement with the Help of Ultrasonic Sensor
IRJET- Distance Measurement with the Help of Ultrasonic Sensor
 
Fiber otdr testing
Fiber otdr testingFiber otdr testing
Fiber otdr testing
 
Optical components
Optical componentsOptical components
Optical components
 

Similar to Optical fibers and Integrated optics

Dispersion-Management-of-Optical-Fiber-Presented-by-Titas-Sarker
Dispersion-Management-of-Optical-Fiber-Presented-by-Titas-SarkerDispersion-Management-of-Optical-Fiber-Presented-by-Titas-Sarker
Dispersion-Management-of-Optical-Fiber-Presented-by-Titas-Sarker
Titas Sarker
 
Circuits for Optical Based Line of Sight Voice Communication
Circuits for Optical Based Line of Sight Voice CommunicationCircuits for Optical Based Line of Sight Voice Communication
Circuits for Optical Based Line of Sight Voice Communication
journalBEEI
 

Similar to Optical fibers and Integrated optics (20)

Integrated ring resonator system analysis to Optimize the soliton transmission
Integrated ring resonator system analysis to Optimize the soliton transmissionIntegrated ring resonator system analysis to Optimize the soliton transmission
Integrated ring resonator system analysis to Optimize the soliton transmission
 
Laser lecture 09 (applications, fiber optics)
Laser lecture 09 (applications, fiber optics)Laser lecture 09 (applications, fiber optics)
Laser lecture 09 (applications, fiber optics)
 
OTDR-OPTICAL TIME DOMAIN REFLECTOMETER
OTDR-OPTICAL TIME DOMAIN REFLECTOMETEROTDR-OPTICAL TIME DOMAIN REFLECTOMETER
OTDR-OPTICAL TIME DOMAIN REFLECTOMETER
 
Parra - Ultrashort Pulse (USP) Laser -- Matter Interactions - Spring Review 2013
Parra - Ultrashort Pulse (USP) Laser -- Matter Interactions - Spring Review 2013Parra - Ultrashort Pulse (USP) Laser -- Matter Interactions - Spring Review 2013
Parra - Ultrashort Pulse (USP) Laser -- Matter Interactions - Spring Review 2013
 
Polarisation non-reciprocity cancelling in Sagnac fibre ring interferometer: ...
Polarisation non-reciprocity cancelling in Sagnac fibre ring interferometer: ...Polarisation non-reciprocity cancelling in Sagnac fibre ring interferometer: ...
Polarisation non-reciprocity cancelling in Sagnac fibre ring interferometer: ...
 
743046
743046743046
743046
 
Transmission Characteristics of optical fiber
Transmission Characteristics of optical fiberTransmission Characteristics of optical fiber
Transmission Characteristics of optical fiber
 
Dispersion-Management-of-Optical-Fiber-Presented-by-Titas-Sarker
Dispersion-Management-of-Optical-Fiber-Presented-by-Titas-SarkerDispersion-Management-of-Optical-Fiber-Presented-by-Titas-Sarker
Dispersion-Management-of-Optical-Fiber-Presented-by-Titas-Sarker
 
Circuits for Optical Based Line of Sight Voice Communication
Circuits for Optical Based Line of Sight Voice CommunicationCircuits for Optical Based Line of Sight Voice Communication
Circuits for Optical Based Line of Sight Voice Communication
 
Fso
FsoFso
Fso
 
FOURIER -TRANSFORM INFRARED SPECTROMETER [FTIR]
FOURIER -TRANSFORM INFRARED SPECTROMETER [FTIR]	FOURIER -TRANSFORM INFRARED SPECTROMETER [FTIR]
FOURIER -TRANSFORM INFRARED SPECTROMETER [FTIR]
 
A method for controlling the bandwidth of high energy, fewoptical-cycle
A method for controlling the bandwidth of high energy, fewoptical-cycleA method for controlling the bandwidth of high energy, fewoptical-cycle
A method for controlling the bandwidth of high energy, fewoptical-cycle
 
09-Luna-Fiber-Optic-Test-Measurement-final.pptx
09-Luna-Fiber-Optic-Test-Measurement-final.pptx09-Luna-Fiber-Optic-Test-Measurement-final.pptx
09-Luna-Fiber-Optic-Test-Measurement-final.pptx
 
Introduction to Fourier Transfer Infrared Spectroscopy
Introduction to Fourier Transfer Infrared SpectroscopyIntroduction to Fourier Transfer Infrared Spectroscopy
Introduction to Fourier Transfer Infrared Spectroscopy
 
7 4-1-7-11
7 4-1-7-117 4-1-7-11
7 4-1-7-11
 
Testing effectiveness of the splice through otdr and power meter tests
Testing effectiveness of the splice through otdr and  power meter testsTesting effectiveness of the splice through otdr and  power meter tests
Testing effectiveness of the splice through otdr and power meter tests
 
Laser comm.
Laser comm.Laser comm.
Laser comm.
 
The control of scattered radiation
The control of scattered radiationThe control of scattered radiation
The control of scattered radiation
 
Laser ii 3 ppt
Laser ii 3 pptLaser ii 3 ppt
Laser ii 3 ppt
 
V4102176181
V4102176181V4102176181
V4102176181
 

Optical fibers and Integrated optics

  • 1. UEF // University of Eastern Finland Characterization of a ring resonator Advanced Laboratory Practices, 26th May 2016 Atri Halder Optical fibers and Integrated optics
  • 2. Resonance 2 Guiding 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) = 1 π 2𝑎 (λ−λ0)2+𝑎2
  • 3. Resonator 3 Guiding in optical fibers / Atri Halder, 26.05.2016 A B
  • 4. Ring Resonator 4 Guiding in optical fibers / Atri Halder, 26.05.2016 Resonance condition: L × 𝑛 𝑒𝑓𝑓 = N. λ 𝑑 where, L = 2πR R is the radius of the ring resonator. λ 𝑑 is the wavelength of light coupled to the input. 𝑛 𝑒𝑓𝑓 is the effective refractive index of the waveguide.
  • 5. Full width at half maxima (FWHM) 5 Guiding in optical fibers / Atri Halder, 26.05.2016 where 𝑛 𝑔 is the group index of the medium, r is the self coupling coefficient, a is the resonator round trip loss coefficient and λ 𝑟𝑒𝑠 is the resonance wavelength. FWHM = (1−𝑟𝑎)λ 𝑟𝑒𝑠 2 π𝑛 𝑔 𝐿 𝑟𝑎
  • 6. Free Spectral Range (FSR) 6 Guiding in optical fibers / Atri Halder, 26.05.2016 FSR = λ 𝑟𝑒𝑠 2 𝑛 𝑔 𝐿
  • 7. Finesse 7 Guiding in optical fibers / Atri Halder, 26.05.2016 Finesse = 𝐹𝑆𝑅 𝐹𝑊𝐻𝑀
  • 8. Quality Factor (Q-factor) 8 Guiding 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 = λ 𝑟𝑒𝑠 𝐹𝑊𝐻𝑀
  • 9. Micro ring resonator 9 Guiding in optical fibers / Atri Halder, 26.05.2016
  • 10. 10 Specification of the ring resonator Guiding in optical fibers / Atri Halder, 26.05.2016
  • 11. Experimental setup 11 Guiding in optical fibers / Atri Halder, 26.05.2016
  • 12. Result: Reference 12 Guiding in optical fibers / Atri Halder, 26.05.2016
  • 13. 13 Guiding in optical fibers / Atri Halder, 26.05.2016 Transmission spectrum of through port for a gap 300 nm.
  • 14. Guiding in optical fibers / Atri Halder, 26.05.2016 Enhanced resonance for a gap of 300 nm.
  • 15. Guiding in optical fibers / Atri Halder, 26.05.2016 Transmission spectrum of through port for a gap 400 nm.
  • 16. Guiding in optical fibers / Atri Halder, 26.05.2016 Enhanced resonance for a gap of 400 nm.
  • 17. 17 Guiding in optical fibers / Atri Halder, 26.05.2016 Transmission spectrum of drop port for a gap 400 nm.
  • 18. 18 Guiding in optical fibers / Atri Halder, 26.05.2016 Transmission spectrum of through and drop port for a gap 400 nm.
  • 19. Comparison 19 Guiding in optical fibers / Atri Halder, 26.05.2016
  • 20. Comparison 20 Guiding 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
  • 21. Conclusion 21 Guiding 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.