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11/25/2011 1 4 Power Launching and Coupling Th l b d Ch 5GK This lecture is based on Chapter 5, G. Keiser [email protected] Topics in this lecture Launching optical power into a fiber Fiber-to-Fiber coupling Fiber Splicing and connectors 2 Fiber Splicing and connectors

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Page 1: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

1

4Power Launching and

CouplingTh l b d Ch 5 G KThis lecture is based on Chapter 5, G. Keiser

[email protected]

Topics in this lecture

Launching optical power into a fiber

Fiber-to-Fiber coupling

Fiber Splicing and connectors

2

Fiber Splicing and connectors

Page 2: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

2

Coupling Efficiency

s

F

PP

==soursethefromemittedpower fiber theinto coupledpower η

sp

3

Source Optical FibersP

FP

Radiance (Brightness) of the sourceOptical power coupled into the fiber depends upon the radiance of optical source rather than total output power. (Optical power radiated from a unit area of the source into a unit solid angle) (watts/cm2/steradian)a unit solid angle) (watts/cm2/steradian)→ [spatial distribution of the

optical power of the source]

4

Page 3: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

3

Source output pattern

θφθ cos),( 0BB =For surface emitting LEDs

B0 is the radiance along the normal to the radiating surface

For Edge emitting LEDs and lasers

φφ cossin1 22+=

5

θθφθ LT BBB coscos),( 00+

Integers T and L are the transverse and lateral power distribution coefficients

For edge emitting LEDs, L = 1

Power Coupled from source to the fiber

rdrdddB

dAdABP

r

sA

sssF

m

f f

θφθθφθθππ

⎥⎤

⎢⎡

=

⎥⎥⎥

⎢⎢⎢

⎡ΩΩ=

∫∫∫∫

∫ ∫Ω

max022

sin)(

),(

6

rdrdddB sθφθθφθ⎥⎥

⎦⎢⎢

⎣= ∫∫∫∫

0000

sin),(

source theof angleemission solid and area : and ssA Ωfiber of angle acceptance solid and area : and ffA Ω

Page 4: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

4

Example: Power coupled from LED to the Step Index Fiber

rdrddBP s

rs

θθθθππ θ

∫ ∫∫ ⎟⎟⎠

⎞⎜⎜⎝

⎛=

2

0 sincos2max0

For rs < a (fiber radius)

rdrdB

rdrdB

s

r

s

r

s

s

θπ

θθπ

π

π

∫∫

∫∫

∫ ∫∫

=

=

⎟⎠

⎜⎝

2

0

2

00

2

0max0

2

00

0 00

NA

sin

7

00

Δ≈= 210

2220

22stepLED, 2)NA( nBrBrP ss ππ

Total optical power from LED:

sin),(2

0

2/

0∫ ∫=ππ

ϕθθϕθ ddBAP ss

sincos2 2/

00

220

2 ∫ ==π

πθθθππ BrdBrP sss

⎪⎬

⎪⎨

≥⎟⎟⎞

⎜⎜⎛

=arPa

arP

Pss

if)NA(

if )NA(

22

2

stepLED,

8

⎪⎭

⎪⎩

≥⎟⎟⎠

⎜⎜⎝

arPr ss

s

if )NA(

Derive equations 5.5 and 5.8 (Assignment)

Page 5: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

5

Equilibrium Numerical ApertureNon propagating modes will scatter out within a short distance (~ 50 m) and equilibrium is establishedSurface emitting LEDs have max of non propagating modesFl l d l d l l t thi ff tFly–lead coupled lasers are less prone to this effect

eric

al A

pertu

re NA in

NA eq

2

50 ⎟⎟⎠

⎞⎜⎜⎝

⎛=

in

eqeq NA

NAPP

P50 = Power expected 50

9

Fiber Length

Num

e

0 50 100 150 meters

at z = 50 m

Examples of possible lensing schemes used to improve optical source-to-fiber coupling efficiency

Collimating

Focuses light onto a line

10

Page 6: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

6

LED to Fiber Coupling as a function of Emitting Diameter

In case of:

Fiber NA = 0.2Core Radius ‘a’ = 25 μm

uplin

g E

ffici

ency

(%)

11

& Emitting Dia = 25 μmCoupling Efficiency = ….

Cou

Emitting Diameter (μm)

Fiber-to-Fiber Joint

Low loss fiber-fiber joints are either:1 – Splice (permanent bond)p (p )2 – Connector (demountable connection)Fiber-to-Fiber coupling loss LF (dB) = − 10 log ηF

where ηF = Mcomm / ME

12

Page 7: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

7

Different modal distributions of the optical beam emerging from a fiber, lead to different degrees of coupling loss

When all modes are equally excited, the output beam fills the entire output NA

13

For a steady state modal distribution, only the equilibrium NA is filled by the output beam

Mechanical Misalignment Losses

14

Page 8: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

8

Lateral (Axial) Misalignment Losses

2step, =Acomm

Dominant Mechanical loss

2/12

2p,

21

2arccos2

⎥⎥⎦

⎢⎢⎣

⎡⎟⎠⎞

⎜⎝⎛−−=

ad

ad

ad

a

ππ

π

15

Dominant Mechanical loss

Derive the similar expression for GI Fiber (Assignment)

Losses due to differences in the geometry and waveguide characteristics of the fibers 1. Radius

2. Numerical Aperture3 R f ti I d P fil

( ) ( )ER

ERE

RF

ERE

RF

NAL

aaaaaL

αα +

≤⎟⎠⎞⎜

⎝⎛−=

≤⎟⎠⎞⎜

⎝⎛−=

2

NANAfor NANAlog10)(

for log10)(

2

23. Refractive Index Profile

16

( ) ( )( ) ER

RE

ERFL αα

αααα

α ≤++

−= for 22log10

E & R subscripts refer to emitting and receiving fibers

Page 9: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

9

Connector Return Loss

17

Important characteristics of few connectors

18

Page 10: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

10

Write a brief report on theWrite a brief report on the

Connector parameters

19

Experimental comparison of Losses as a function of mechanical misalignment

20

Page 11: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

11

Connectors CharacteristicsSome of the principal requirements of a good connector design are as follows:1 l li l1- low coupling losses 2- Interchangeability3- Ease of assembly4- Low environmental sensitivity5- Low-cost and reliable construction

21

5 Low cost and reliable construction6- Ease of connection

Fiber End Face

22

Fiber end defects

Page 12: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

12

Fiber Splicing

23

Fusion Splicing

V-groove Optical Fiber Splicing

24

Page 13: Power Launching and Coupling - University of Engineering ...web.uettaxila.edu.pk/CMS/AUT2011/eeOCms/notes/4 - Power launchi… · Equilibrium Numerical Aperture Non propagating modes

11/25/2011

13

Exercises

25