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PREDICTION METHODS OF RAYLEIGH
SCATTERING LOSSESPREPARED BY
DARSHAN BHATT(150320705001)
INTRODUCTION■ Scattering losses in glass arise from microscopic variation in material
density, from structural decomposition and structural inhomogeinity.
SCATTERING LOSSES
Stimulated Brillouin
Scattering(SBS)
Stimulated Raman
Scattering(SRS)
Non-Linear Scattering Losses
RayleighScattering
Linear Scattering Losses
Mie Scattering
RAYLEIGH SCATTERING IN OPTICAL FIBER
• Rayleigh scattering named after the British physicist Lord Rayleigh.
• Also known as elastic scattering.
• It is a linear type of scattering mechanism.
• It is a parametric process.
• It is the reason for blue color of sky. Figure 1 : Lord Rayleigh [1]
Why the sky is blue..................?
FIGURE 2 – RAY LEIGH SCATTERING PHENOMENA
Expression for Rayleigh Scattering Coefficient
■ Rayleigh scattering is an important component of the scattering of optical
signals in optical fibers.
■ Microscopic variations of density and refractive index: These give rise
to energy losses due to the scattered light, with the following coefficient -
Prediction Methods for Rayleigh Scattering Losses■ To reduce the attenuation losses due to Rayleigh scattering in optical
fibers –
1. Improved Fabrication Processes
2. Thermal Treatment of glass fibers■ Fabrication processes – OVPO, MCVD, VAD■ Better Fabrication process – Vapor-Phase Axial Deposition (VAD)■ The Rayleigh scattering coefficient is strictly dependent on fictive
temperature (TF) and it is inversely proportional to the 4th power of the wavelength.
■ If fictive temperature (TF) ↓ γR↓
Rayleigh Scattering Reduction Method using VAD Technique
■ Effect of temperature on Rayleigh Scattering : γR ↑ (5 to 10%) at 1800 deg. C
■ To reduce γR drawing the fiber at low temperature.
Consideration:
■ GeO2 doped Silica core SMF with minimum loss 0.16 dB/km at 1.55 μm.
Reduction Method :
Vapor Phase Axial Deposition (VAD) which is developed by Izawa.
Sub Processes in VADFour processes in VAD technique :
1. Consolidation - Process of uniting or unification of two or more components
2. Annealing – Heating than cooling
3. Air cooling
4. Re-heating
To reduce scattering losses – ■ Consolidation – At 1400 deg. C■ Annealing – At 1250 to 1400 deg C■ Cooling Rate – 5 deg C / min■ Air cooling – At room temp.
Thermal Treatment Diagram
Expression for R.S.C for GeO2 and F doped fiber
■Rayleigh scattering coefficient of GeO2 and F doped Silica fiber is
given by –
■Here, [GeO2] and [F] are the refractive index differences, AGeO2-F and
ASiO2 are Rayleigh scattering co-efficients for GeO2 & F doped Silica
fiber and SiO2 doped glass fiber.
Overall Spectral Loss
■ By analysis of loss components in fiber the total spectral loss is expressed by α of an optical fiber is expanded as –
■ Here A = Rayleigh scattering coefficient, αIM = Imperfection loss
αIR = Infrared Absorption loss,
αOH = OH Absorption loss
Generalized form of R.S.C
■ In general the Rayleigh scattering coefficient ‘A’ is expressed by the equation –
■ Here Ad = density fluctuations and Ac = Concentration fluctuations
where Ad is defined by -
Relation between Rayleigh scattering
coefficient and drawing
temperature
Conclusion■The Rayleigh scattering coefficients of the glasses increased 5–
10% by heating them to 1800 C.
■A method for reducing the Rayleigh scattering of silica-based optical fibers by drawing them slowly at low temperatures.
■This is because the fictive temperature of the fiber decreased as the drawing temperature decreased.
References[1]. https://en.wikipedia.org/wiki/John_William_Strutt,_3rd_Baron_Rayleigh
[2]. www.slideshare.net
[3]. K.T.Katsuske, Member IEEE, K Shiraki, I Sankawa, “Method for predicting Rayleigh scattering loss of silica based optical fiber”, vol. 25, no.8, Aug 2007.
[4]. K Tsujikawa, K Tajima, M. Ohashi, Senior member IEEE, “Rayleigh scattering reduction method for silica based optical fiber”, vol 18, no 11, Nov 2000.
[5] Book – John M Senior, Optical fiber communications, Principles & practice, second edition
THANK YOU