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Page 1: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM
Page 2: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Robert:•Motivation•Principles of Optics•Applications •Optimization

Andy:Materials

Loss vs. amplification

Theoretical problems

Overview

2 + 2 = 4WM

Page 3: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Motivation

1. Internet relies on fiber optics.

2. Amplification needed.

Current technology inadequate:

Limited amplification bandwidth

Limited internet speed

Page 4: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Linear OpticsLow intensity light in transparent media.

•Refraction

•Dispersion

Light slows down in transparent media.

Refractive index is function of frequency.

Page 5: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Propagation constantBeta (propagation constant) very useful.

Expressible as power series.

Coefficient critical to optimizing FWM.

Page 6: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Limitations1. Photons do not interact.

2. No new frequencies are created.

3. Too simple for our purposes.

But nonlinear optics provides uswith great possibilities…

Page 7: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Nonlinear Optics•Kerr effect: refractive index depends on

intensity of light.

•Nonlinearity causes complex behavior.

•Nonlinear Schrödinger Equation

Photons can mix and change their frequencies!

Nonlinear Term

Page 8: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Four-wave Mixing

Signal

Pump Lasers Photons added to signal

Photons added to idler

Idler(createdto conserve energy)

(Amplified through FWM)2 + 2=4WM

Frequency (ω)/100THz

Log

(In

tensi

ty)

Pump photons mix to form signal and idler photons.

Page 9: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Elastic Collision Analogy

Energy Conservation:

MomentumConservation:

Pump energies

Energies of signal and idler

Pump momenta

Momenta of signal and idler

Page 10: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

ApplicationsWhat can we use it for?

•Amplification and Frequency conversion.

•Solves world hunger (for internet speed)

Optimization:•How do we turn ideas into high performance technology?

mathematical analysis and approximation.

Page 11: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Amplification Optimization•Amplification depends on only one number.

•Must be close to –γP for maximum gain.

•Complexity of β solved by quartic approximation.

Page 12: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Conditions for Maximum Flat Gain

1. Average pump frequency at zero dispersion point ω00.

Where:

2. β4 4 must be positive.

3. And lastly, regarding the pumps:

Page 13: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Before and After Optimization

Signal Frequency Offset

Gain

Inferior bandwidth

Optimized bandwidth

Page 14: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Frequency Conversion OptimizationIdler photons used as new signal:

Useful since different frequencies needed in fiber.

Problem: pumps: same average frequency as “a” and “b.”

Stuck with bandwidth we’re given…

Page 15: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Dispersion Engineering•Optical fibers:

Total internal reflection

•Light strays into cladding.

•Samples 2 refractive indices.

•We can engineer β22, , β3, 3, β4 etc.4 etc.

n22n11

Page 16: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Frequency Conversion OptimizationIdler photons used as new signal:

Useful since different frequencies needed.

Problem: pumps: same average frequency as “a” and “b.”

Stuck with bandwidth we’re given…

Solution: dispersion engineering: minimize β44 Make β3 3 and β4 4 into “magic ratio.”

Creates greater bandwidth.

Page 17: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Summary

Page 18: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Optical Fiber

Nonlinear effect ∝ γPL

Silica Low loss Low nonlinearity γ

High P and L needed for FWM

Page 19: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Silica V.S. Chalcogenide

Silica Chalcogenide

Made of

SiO2 S, Se, Te+others

γ Low High

Used in Optical Fiber Optical Chip

Loss Low High

Page 20: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Nonlinear Schrodinger Equation (NLS)

uiuut

u

z

ui

2

2

2

)(2

1

Linear loss coefficient

Numerically solve NLS with loss(Split step Fourier method)

How loss affects gains

Page 21: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

1 pump case

Signal GainIdler Gain

γ+γ- INPUTOUTPUT

Page 22: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

1 pump case

INPUTOUTPUT

Page 23: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Gain curve – 1 pump

Page 24: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Gain curve – 1 pump

α = (dB/m) 0 20 40 60 80 100

Chalcogenide

Page 25: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Peak Gain– 1 pump

loss ∝ e-αL

(dB/m)

Page 26: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

2 pump case INPUTOUTPUT

Signal Gain

Idler Gain

2 pump case

Page 27: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Gain curve - 2 pump case

Signal Gain Idler Gain

Page 28: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Asymmetry Problem

Page 29: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Conclusion FWM : nonlinear optical effect

Parametric amplifications

Conditions for greater bandwidth

How loss affects gain curves— unexpected!!

Page 30: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

Future Work

Asymmetry Problem

Coping with loss

Page 31: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

References

• C. J. McKinstrie, S. Radic and A. R. Chraplyvy. Parametric Amplifiers Driven by Two Pump Waves. IEEE J. Quantum Electron., vol.QE-8, pp. 538–547, 2002.

• G. P. Agrawal (2001). Nonlinear Fiber Optics. Orlando: Academic Press.

• M. R. Lamont, T. T. Kuhlmey and C. M. de Sterke. Multi-order dispersion engineering for optimal four-wave mixing. Optics Express, vol.16, pp. 7551–7563, 2008.

Page 32: Robert: Motivation Principles of Optics Applications Optimization Andy: Materials Loss vs. amplification Theoretical problems Overview 2 + 2 = 4WM

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