Nonlinear Optical Effects in Fibers

Transcription

1 Nonlinear Optical Effects in Fibers NLO effects are manifested as attenuation, phase shifts, or wavelength conversion effects, and become stronger with increasing light intensity. The glass materials usually used for fibers exhibit very small intrinsic nonlinearities. Nevertheless, the magnitude with which a nonlinear effect manifests itself is proportional to 3 factors: the size of the nonlinearity, the intensity of the radiation (light), and the interaction length. Because of the latter 2 factors, esp. the interaction length (limited normally by focusing geometries and by attenuation), optical fibers can manifest extremely strong nonlinear behavior, which can limit the BL products for optical communication applications.

2 Dominant Nonlinear Optical Effects in Telecom Fibers Stimulated inelastic light scattering Stimulated Brillouin scattering Stimulated Raman scattering Nonlinear optical effects Nonlinear phase modulation Self-phase modulation Cross-phase modulation Four-wave mixing Note that all the above effects are due to 3 rd order nonlinearities, since 2 nd order NLs are negligible in centrosymmetric media (the glass materials used to make fibers are nearly-perfectly isotropic, thus they are centrosymmetric)

3 Stimulated Brillouin Scattering Energy conservation: Momentum conservation: Dispersion relation: Ω = Ω k A A = p Ω k p s k k = Ω / v s A k s k A θ k p Stokes scattering The acoustic frequency: Ω = k v = 2v k sin( θ / 2) A A A p θ = 0 : Ω = 0 θ = π : Ω = Ω B = 2v A k p The Brillouin shift: ν = Ω / 2π = 2nv / λ B B A p For n =1. 45 λ = p 1. 55µm v A = 5.96km / s ν =11. GHz B 1

4 Stimulated Brillouin Scattering Spontaneously Scattered waves (Ω B ) Pump (Ω p ) Scattered waves (Ω B ) Enhance Beating term (Ω A ) Enhance Sound waves (Ω A ) The feedback process is governed by: di p = g dz di s = g dz B B I I α I α I I p and I s are the intensity of the pump and Stokes fields, g B is the SBS gain, and α p and α s account for fiber losses p p I I s s p s p s If the acoustic waves decay as exp( t / T The Brillouin gain is frequency dependent g B g B ( Ω ( Ω) = 1+ ( Ω Ω B B ) 2 ) The peak value of Brillouin gain is depends on various material parameters such as the density and the elasto-optic coefficient. For Silica fibers T 2 B 11 g B 5 10 m / W B ),

5 Stimulated Brillouin Scattering SBS gain bandwidth of silica fiber is larger than that of bulk silica A part of this increase is due to the guided nature of acoustic modes in optical fibers Brillouin-gain spectra measured using a µm pump for three fibers with different germania doping: (a) silica-core fiber; (b) depressed-cladding fiber; (c) dispersion-shifted fiber. The threshold power: g BPthLeff / Aeff 21 L eff = [ 1 exp( α L)] /α 2 A eff = πw P th ~ 5mW Most of the increase can be attributed to variations in the core diameter along the fiber length. The difference of SBS gain bandwidth between fibers can exceed 100MHz Typical value ~50MHz for wavelength near 1.55 µm

6 Stimulated Raman Scattering Spontaneously Scattered waves (Ω R ) Pump (Ω p ) Scattered waves (Ω R ) Beating term (Ω O ) Enhance Molecular oscillations (Ω O ) Enhance The feedback process is governed by: di p = g dz di s = g dz R R I I p α I α I I p and I s are the intensity of the pump and Stokes fields, g R is the SRS gain, and α p and α s account for fiber losses p I I s s s p s p Energy levels participating in the SRS process For Silica fibers 13 g R 1 10 m / m 13 g R 6 10 m/ m

7 Stimulated Raman Scattering Raman gain spectrum of fused silica at λ p =1 µm The threshold power: g P L / A 16 R th eff eff SRS gain bandwidth of silica fiber exceeds 10 THz The broadband and multipeak nature of the spectrum is due to the amorphous nature of glass The maximum gain occurs when the Raman shift is about 13 THz. L eff = [ 1 exp( α L)] /α 2 A eff = πw P 16α ( πw ) / 2 th g R P th ~ 500mW

8 Stimulated Light Scattering Similarity: Difference: Inelastic scattering SBS and SRS Frequency shifted down (lower energy) Grows exponentially SBS occurs only in the backward direction whereas SRS can occurs in both directions Frequency shift about ~ 10 GHz for SBS, ~ 13 THz for SRS The Brillouin gain spectrum is extremely narrow (bandwidth < 100 MHz) compared with the Raman-gain spectrum (bandwidth > 20 THz) SBS acoustic phonon, SRS optical phonon

9 Self-Phase Modulation Physics origin of nonlinearity: n ' = n + n2( P / Aeff ) n2 is the nonlinear-index coefficient, ~ m / W The propagation constant is power dependent: Nonlinear phase shift: β = β + k n P / Aeff = β + γp ' 0 2 γ = L L ( β ' β ) dz = 0 0 2πn 2 /( A λ) φ NL = γpin exp( αz) dz = γp eff in L eff

10 Self-Phase Modulation In practice, time dependence of P in makes ф NL vary with time SPM leads to frequency chirping of optical pulses The frequency chirp is proportional to the derivative dp in /dt, and depends on the pulse shape SPM-induced frequency chirp for Gaussian (dashed curve) and super-gaussian (solide curve ) pulse

11 Cross-Phase Modulation In DWDM systems, the nonlinear phase shift for a specific channel depends not only on the power of that channel but also on the power of other channel, the phase shift for the jth channel: The worst case: φ NL j φ NL j = γl eff ( P + 2 j P m j m = ( γ / α)(2m 1) P ) j Enlarging A eff helps reduce the fiber nonlinearity considerably

12 Four-Wave Mixing If three optical fields with carrier frequencies ω 1, ω 2, and ω 3 copropagate inside the fiber simultaneously, χ (3) generates a fourth field whose frequency ω 4, is related to other frequencies: The most troublesome case: ω ± 4 = ω1 ± ω2 ω3 ω 4 = ω1 + ω2 ω3 The phase mismatch when four waves propagate in the same direction: = β ( ω3) + β ( ω4) β ( ω1) β ( ω2) Modern DWDM systems avoid FWM by using the technique of dispersion management

13 Birefringence Birefringence is acquired when the degeneracy between the orthogonally polarized fiber modes is removed The degree of birefringence is B = n x n y nx and ny are the mode indices for the orthogonally polarized fiber modes Birefringence leads to a periodic power exchange between the two polarization components. The period is called beat length: L B = λ / B nx and ny are the mode indices for the orthogonally polarized fiber modes

14 Birefringence Polarization state is arbitrary in a conventional fiber Polarization-preserving fiber is produced by intentionally introducing a large amount of birefringence. Typically, B~10-4 State of polarization in a birefringent fiber over one beat length. Input beam is linearly polarized at 45 o with respect to the slow and fast axes

15 Spot Size The field distribution is often approximated by a Gaussian function: E x = 2 Aexp( ρ 2 / ω )exp( iβz) Where,ω is the field radius and is referred to as the spot size ω/a depends on V parameter; the value for 1.2<V<2.4 can be determined by: Confinement factor: ω / a Γ = P P core total V = 3/ V ρdρ = 1 exp ρdρ 6 a 2 E 2 x 0 2a E x ω

16 Spot Size (a) Normalized spot size ω/a as a function of the V parameter obtained by fitting the fundamental fiber mode to a Gaussian distribution; (b) quality of fit for V=2.4 Most telecommunication single-mode fibers are designed to operate in the range 2<V<2.4

17 Fiber Loss Power attenuation inside an optical fiber is governed by The output power is determined dp / dz = αp Where,α is the field radius and P is the optical power Relation between units of db/km and 1/m Fiber loss: P out ( L) = P exp( αl) in 10 P out α( db / km) = log10 = α L Pin (1) Material Absorption (2) Rayleigh Scattering (3) Waveguide Imperfection (4) Bending

18 Spectral loss profile of a single-mode fiber. Wavelength dependence of fiber loss for several fundamental loss mechanisms is also shown Fiber Loss Two main sources: Material absorption Rayleigh scattering

19 Material Absorption Material absorption: (1) Intrinsic material absorption The electronic and vibrational resonances associated with SiO 2 (a) Electronic resonance λ < 0.4µm (b) Vibrational resonance λ > 7µm (2) Extrinsic material absorption The electronic and vibrational resonances associated with impurties (a) Transition-metal ( Fe, Cu, Co, Ni, Mn, and Cr) (b) OH ion (c ) Dopants ( GeO2, P2O5, and B2O3)

20 Rayleigh Scattering Rayleigh scattering is a fundamental loss mechanism arising from local microscopic fluctuations in density At 1.55µm, α R = db/km 4 α = R C / λ Where,C is in the range (dB/km)-µm 4,

21 Waveguide Imperfections Mie scattering induced by the imperfections at the core-cladding interface (random core-radius variations) In practice, such variation can be kept below 1%, and the resulting scattering loss is typically below 0.03 db/km

22 Bending Loss Bending is another source of scattering loss The bending loss is proportional to exp(-r/r c ) For single-mode fibers, R c = µm typically, and the bending loss is negligible (<0.01 db/km) for bend radii R > 5 mm Macrobending loss are negligible in practice since macroscopic bends exceed R = 5 mm Microbending loss could be large in the cable

23 Optical Fiber Manufacturing Fiber Materials Design Issues Fabrication Methods Cables and Connectors

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25 Fiber Materials Requirements in selecting materials for optical fibers: 1. It must be possible to make long, thin, flexible fibers from the material 2. The material must be transparent at a particular optical wavelength 3. Physically compatible materials that have slightly different refractive indices for the core and cladding must be available Oxide Glass Fibers Halide Glass Fibers Active Glass Fibers Chalcogenide Glass fibers Plastic Optical Fibers

26 Glass Fibers Glass is made by fusing mixtures of metal oxides, sulfides, or selenides Glass has a randomly connected molecular network Glasses do not have well-defined melting points

27 Oxide Glass Fibers The most common oxide glass fiber is silica (SiO 2 ) Its refractive index is 850nm Its refractive index can be easily modified by adding either fluorine or various oxides Examples of fiber compositions: (1) GeO 2 -SiO 2 core; SiO 2 cladding (2) P 2 O 5 -SiO 2 core; SiO 2 cladding (3) SiO 2 Core;cladding (4) Ge 2 O 5 -B 2 O 2 -SiO 2 core, P 2 O 5 -SiO 2 core cladding Variation in refractive index as function of doping concentration in silica glass

28 Halide Glass Fibers The most common halide glass fiber is ZBLAN (ZrF 4, BaF 4, LaF 3, AlF 3, NaF) A lower-refractive-index cladding (ZHBLAN)is produced by partially replacing ZrF 4 by HaF 4 Extremely low transmission losses at mid-infrared wavelengths (0.2-8µm) with the lowest loss being around 2.55 µm Potentially offers intrinsic minimum losses of dB/km

29 Active Glass Fibers Incorporating rare-earth elements (atomic numbers 57-71) into a normally passive glass gives the resulting materials new optical and magnetic properties Amplification, attenuation, and phase retardation can be performed in active glass fibers Commonly used materials for fiber lasers and amplifiers: Erbium, Neodymium, Ytterbium, Holmium,

30 Chalcogenide Glass Fibers Contain at least one chalcogen element (S, Se, or Te) and typically one other element such as P, I, Cl, Br, Cd, Ba, Si, or Tl for tailoring the thermal, mechanical, and optical properties of the glass High optical nonlinearity Long interaction length As 2 S 3 is one of the most well-known materials ( core: As 40 S 58 Se 2, cladding: As 2 S 3 ) Loss typically range around 1 db/m

31 Plastic Optical Fibers High-bandwidth graded-index polymer optical fibers (POFs) meet the growing demand for delivering high-speed services directly to the workstation The core of FOPs are either polymethylmethacrylate (PMMA POF) or perfluorinated polymer (PFP POF) Larger optical signal attenuations than glass fibers Tough and durable

32 Design Issues Several index profiles used in the design of single-mode fibers. Upper and lower rows correspond to standard and dispersion-shifted fibers, respectively

33 Fiber Fabrication Outside Vapor-Phase Oxidation Vapor-Phase Axial Deposition Modified Chemical Vapor Deposition Plasma-Activated Chemical Vapor Deposition Double-Crucible Method

34 Outside Vapor-Phase Oxidation Basic steps in preparing a preform by the OVPO process. (a) Bait rod rotates and moves back and forth under the burner to produce a uniform deposition of glass soot particles along the rod; (b) profiles can be step or graded index; (c ) following deposition, the soot preform is sintered into a clear glass preform; (d) fiber is drawn from the glass preform

35 Modified Chemical Vapor Deposition GeCl 4 4POCl + O O 2 GeO 2 2P O + 2Cl Cl 2 Schematic of MCVD

36 Plasma-Activated Chemical Vapor Deposition Schematic of PCVD process

37 Vapor-Phase Axial Deposition Apparatus for the VAD process

38 Double-Crucible Method Double-crucible arrangement for drawing fibers from molten glass

39 Fiber Drawing Schematic of a fiber-drawing apparatus Apparatus used for fiber drawing

40 Cables and Connectors Typical designs for light-duty fiber cables Typical designs for heavy-duty fiber cables

41 Birefringence Birefringence is acquired when the degeneracy between the orthogonally polarized fiber modes is removed The degree of birefringence is B = n x n y nx and ny are the mode indices for the orthogonally polarized fiber modes Birefringence leads to a periodic power exchange between the two polarization components. The period is called beat length: L B = λ / B nx and ny are the mode indices for the orthogonally polarized fiber modes

42 Birefringence Polarization state is arbitrary in a conventional fiber Polarization-preserving fiber is produced by intentionally introducing a large amount of birefringence. Typically, B~10-4 State of polarization in a birefringent fiber over one beat length. Input beam is linearly polarized at 45 o with respect to the slow and fast axes

43 Spot Size The field distribution is often approximated by a Gaussian function: E x = 2 Aexp( ρ 2 / ω )exp( iβz) Where,ω is the field radius and is referred to as the spot size ω/a depends on V parameter; the value for 1.2<V<2.4 can be determined by: Confinement factor: ω / a Γ = P P core total V = 3/ V ρdρ = 1 exp ρdρ 6 a 2 E 2 x 0 2a E x ω

44 Spot Size (a) Normalized spot size ω/a as a function of the V parameter obtained by fitting the fundamental fiber mode to a Gaussian distribution; (b) quality of fit for V=2.4 Most telecommunication single-mode fibers are designed to operate in the range 2<V<2.4

45 Fiber Loss Power attenuation inside an optical fiber is governed by The output power is determined dp / dz = αp Where,α is the field radius and P is the optical power Relation between units of db/km and 1/m Fiber loss: P out ( L) = P exp( αl) in 10 P out α( db / km) = log10 = α L Pin (1) Material Absorption (2) Rayleigh Scattering (3) Waveguide Imperfection (4) Bending

46 Spectral loss profile of a single-mode fiber. Wavelength dependence of fiber loss for several fundamental loss mechanisms is also shown Fiber Loss Two main sources: Material absorption Rayleigh scattering

47 Material Absorption Material absorption: (1) Intrinsic material absorption The electronic and vibrational resonances associated with SiO 2 (a) Electronic resonance λ < 0.4µm (b) Vibrational resonance λ > 7µm (2) Extrinsic material absorption The electronic and vibrational resonances associated with impurties (a) Transition-metal ( Fe, Cu, Co, Ni, Mn, and Cr) (b) OH ion (c ) Dopants ( GeO2, P2O5, and B2O3)

48 Rayleigh Scattering Rayleigh scattering is a fundamental loss mechanism arising from local microscopic fluctuations in density At 1.55µm, α R = db/km 4 α = R C / λ Where,C is in the range (dB/km)-µm 4,

49 Waveguide Imperfections Mie scattering induced by the imperfections at the core-cladding interface (random core-radius variations) In practice, such variation can be kept below 1%, and the resulting scattering loss is typically below 0.03 db/km

50 Bending Loss Bending is another source of scattering loss The bending loss is proportional to exp(-r/r c ) For single-mode fibers, R c = µm typically, and the bending loss is negligible (<0.01 db/km) for bend radii R > 5 mm Macrobending loss are negligible in practice since macroscopic bends exceed R = 5 mm Microbending loss could be large in the cable