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Dispersion (ps/km.nm) Dispersion (ps/km.nm)

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(1)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광통신

(Optical Communication)

(2)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광통신의 발전

- 봉화, 횃불, 등대

- 1870, J. Tyndall : 자유낙하 하는 물줄기에 빛이 가두어짐을 발견 - 1880, A.G. Bell : 태양광으로 213m 소리 전송

- 1962, T. Maiman : 반도체레이저 개발

- 1966, 영국 스탠더드통신연, K.C. Kao, Hockham : 광섬유 원거리 전송 제안 - 1970 초, 미국 코닝사, R.D. Maurer (20dB/km)

- 1979, 미국 벨연구소, 1.55 μm LD 개발, 저손실 광섬유 (0.2dB/km) - 1988, 태평양 횡단 해저 광케이블 설치

(3)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광통신의 장점

- Compact : 전선에 비해 가볍고 작음

- Low Cost : 같은 전송능력에서 전선보다 매우 저렴.

- No electrical connection (ground loop) - No EMI (electromagnetic interference)

- Transmission capacity : 10Gbps 상용, 100Gbps 연구중

- Long repeater spacing : 40km 상용, 120 km 가능 (전선 : 12km) - Better security : tapping 불가

(4)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광통신의 원리

core (n1)

cladding (n2) (n1 > n2) TIR(total internal reflection, 내부전반사)

core (n1)

cladding (n2) θ1

θ2

* critical angle (θ2=π/2) : θc1= sin-1(n2/n1) θ>θc1

<광섬유(optical fiber) 기본 구조>

<실제 광섬유 구조>

(5)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광통신의 제한점

- Optoelectric conversion efficiency Æ energy loss

- Difficulty in joining fiber cable : fusion splice, connector Æ transmission loss - Cable bending loss

- Relatively expensive components

- Difficulty in controlling optical signal

exceed the critical angle condition : bending loss

core

(6)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광통신 시스템의 개요

signal in

signal out transmitter

(laser/LED)

repeater

(photodiode/ laser/LED)

coupler receiver

(photodiode) splice

optical fiber

Main issues

- High quality fiber (low loss/dispersion)

- Efficient laser/LED (low power consumption /narrow single mode) - High speed switching (>100Gb rate)

(7)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광섬유 손실

(8)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

NA(numerical aperture) of optical fiber : light accepting capability

core (n1)

cladding (n2)

θ1

θ2 n0

θ0

NA = n0sinθ0= n1sinθ1 θ2= π/2 − θ1 = sin-1(n2/n1)

2 2 2

1

n

n

NA = −

Î

(9)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광섬유의 분산 특성

1. Modal dispersion

: multimode fiber(다중모드 광섬유)에서 고차 모드일수록 군속도가 느림.

Î optical pulse의 broadening

high order mode low order mode

1 ) ( 1

max , min

, g

g v

L v

= Δτ

(10)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Modal dispersion의 제거 - Single mode fiber 사용 - Graded-index fiber 사용

Higher order mode의 군속도가 빨라져, 펄스 확대가 줄게 됨.

(11)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

2. Intramodal dispersion : Material dispersion & waveguide dispersion

- Material dispersion : 단일 모드라도 일정 주파수폭을 가지므로, vg =vg(ω) : fiber material property

- Waveguide dispersion : Core와 cladding에서 광에너지 전파속도가 다르기 때문 : fiber geometrical (& doping) property

c n n

n c

d d

vg m w⎥ +

⎢ ⎤

⎡ ⎟

⎜ ⎞

∂ + ∂

⎟⎠

⎜ ⎞

− ∂

=

=

ω ω

λ ω

β

1

⎥ ⎦

⎢ ⎤

⎡ ⎟

⎜ ⎞

∂ + ∂

⎟ ⎠

⎜ ⎞

− ∂

=

w m

n n

D c

ω ω

λ

: group velocity dispersion

(12)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Intramodal dispersion의 제거 - Phase conjugation에 의한 보상 - Material, waveguide dispersion의 상쇄

fiber1 fiber1

phase conjugator

<Phase conjugation에 의한 보상>

EDFA1 EDFA2

DSF

Pump LD

(13)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

0 10 20

-20 -10

Dispersion (ps/km.nm)

1.1 1.2 1.3 1.4 1.5 1.6 1.7 Wavelength (μm)

waveguide dispersion material dispersion

<Material, waveguide dispersion의 상쇄>

0 10 20

-20 -10

Dispersion (ps/km.nm)

1.1 1.2 1.3 1.4 1.5 1.6 1.7

Wavelength (μm)

dispersion shifted dispersion flattened

(14)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광결정 (photonic crystals)

광자밴드갭(photonic bandgap)을 이용한 신개념 광섬유

(15)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광결정섬유 (photonic crystal fibers)와 도파로(waveguide)

(16)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

광통신용 레이저 광원

+

- p

n

LED(light emitting diode)

- forward-biased heavily doped p-n junction - pumping by injection current

=> Spontaneous emission

LD(laser diode)

- optical feedback by cleaved surface

=> Stimulated emission

LD(laser diode)

- small size, high efficiency, integrability with electronic components - ease of pumping and modulation by current injection

- spectral linewidth is larger than that of other lasers

(17)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

LED(light emitting diode)

- Display

- Traffic signal lamp - Memory

- Laser disk - Lighting

- GaN series Î Blue color

- OLED(organic LED) Î high efficiency Î

(18)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

<Characteristic optical properties of LDs> +

- elliptical beam

short cavity length Output power(P) & oscillation frequency(ν)

sensitively depend on temperature,

injection current and also feedback light.

polar

ization (TE)

LD(laser diode)

(19)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Differential responsibility of laser

0

24 . 1 ηd λ

o

d di

R = dP =

Overall efficiency

eV h i it

d

η ν

η

⎜ ⎞

⎝⎛ −

= 1

(above threshold)

Output power

(20)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Oscillation frequency

- Laser oscillation condition : γ0(ν) >αr

- Phase condition : νnqνF, (q =1,2,...)

- FWHM linewidth : δν ≈νFF where, : finesse of resonator

r r

= − 1

2 /

π 1

F where, : mode spacing

c nd

F

= 2 ν

Fig. 14.2-4

(21)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

example)

* Since the mode closest to the gain maximum Increases in power while the side peaks saturate, the number of modes decreases as the injection current increases.

InGaAsP laser(n = 3.5), d = 400 μm => νF~ 107 GHz λ0 ~ 1.3 μm => λF= λ02 νF/ ν = λ02 /2nd ~ 0.6 nm

Gain width ~ 7 nm => ~ 11 modes oscillation

InGaAsP laser, 1.3 μm / 1.5 μm

10Gbps DFB-LD/module

(22)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Internal feedback laser

- DBR(distributed Bragg reflector) - DFB(distributed feedback)

<DBR structure> <DFB structure>

(23)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Surface emitting laser

SEM image of a VCSEL

<Surface emitting LD> <Edge emitting LD>

(24)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Kwangju Institute of Science & Technology(K-JIST) Optoelectronics Lab.

Fabrication of oxide-confined VCSEL

Light output

QW

Polyimide(PI2555)

n- DBR

n- metal(Ni/Au/Ge/Ni/Au) Substrate

p- DBR P-metal(Ti/Pt/Au)

Oxide

aperture Output window

Pad metal

9Mesa diameter : 40μm

9Current aperture diameter : 5 μm

9Output window diameter : 20 μm

9Bonding pad : 200 X 120 μm2

Surface emitting laser (광주과기원)

(25)

Nonlinear Optics Lab

Nonlinear Optics Lab

. .

HanyangHanyang Univ.Univ.

Surface emitting laser (과기원 – science 게재)

광결정을 이용한 고효율 레이저 광원

참조

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