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(1)

 ƒ  ½ ¨ 7 Hë  H  Sae Mulli (The Korean Physical Society), Volume 56, Number 5, 2008¸   5 Z 4, pp. 418∼421

° Ë

ÑV Ȗ ¥ ß f Ä   ï " e8 ý ­ Žz ð ² Žâ ì È  © Žõ u §  › ͓ Ó Þ” X ¢  ú n Þ× D; c 6 ” X ¢ • ¤V A 0V Ä Ž ì ŏ Œ

)

í <® £a : @ · L |M ` 9 · ™ »£ Ó . > · T # Ü  , > · ƒ ‘ š ò 6 B* å  · * × << ) Ö < · Ù • v: c ø ¶ B ·  ™ »M Z Ì

„

 z Œ ™@ /† < Ɠ § Ó ü t o † < Æõ , F g Å Ò 500-757 (2008¸   3 Z 4 5{ 9  ~ à Î6 £ §)

F

g$ 3 Ä »     G ' p" f  ×  æ  o  H @ /+ þ A½ ¨› ¸Ó ü t õ  ° ú  s  > 8 £ ¤ # 3 0 A V , “ ¦ B Ä º ´ ú §“ É r G ' p" f € 9 כ ¹ô  Ç / B M \  ´ ò Ö 

¦& h “   l Õ ü t s  .  ×  æ F g$ 3 Ä »     G ' p" f r Û ¼% 7 ›`  ¦ 0 A # Œ ] jî ß –  ) a D h– Ðî  r Û ¼& 7 ˜à Ô! 3  I Õ ª ~ ½ ÓZ O “ É r 2 > h s

 © œ_  " f– Ð   É r Ú ÔA Õ ª    \  ¦  ï× ¼ o r &  y Œ •y Œ •_  G ' p" f\  C & ñ   H ~ ½ ÓZ O Ü ¼– Ð Â Ò& h “    © œu  \ O s 



×  æ  o 0 p x§ 4 `  ¦ † ¾ Ó © œr ~  ´ à º e ”  .   + þ A§ 4 \    É r  ×  æ Û ¼& 7 ˜à Ô! 3 _     o\  ¦ : Ÿ x K  G ' p" f_  0 Au ü <   + þ A

&

ñ • ¸\  ¦ 8 £ ¤& ñ l  0 A # Œ  ×  æ G ' p" f_  Û ¼& 7 ˜à Ô! 3   ï× ¼  s  ç ß –  “ É r 0.4 nm,    _  ì ø Í Ö  ¦“ É r 5 % _ 

° ú

כ\  @ /K  r Ó ý t Y Us ‚   % i  .

PACS numbers: 42.81.P, 42.79.D, 07.10.P

Keywords: F g$ 3 Ä » Ú ÔA Õ ª    , Û ¼& 7 ˜à Ô! 3  I Õ ª ~ ½ ÓZ O ,  © œì  r ½ + É ×  æ  o,   + þ A G ' p" f, Û ¼& 7 ˜à Ô! 3   ï× ¼

I. " e  ] Ø

F

g$ 3 Ä »     (Fiber Bragg Gratings)   H  € ª œô  Ç Ó ü t o 

&

h ,  o† < Æ& h  ¢ ¸  H Ò q tÓ ü t& h    à º\  › ' a ô  Ç ’    ñ\  ¦ 8 £ ¤& ñ l  0

Aô  Ç G ' p" f– Ð+ ‹ s 6   x ÷ &“ ¦ e ”   [1,2]. þ j   H Y > ¸   1 l x î ß – { 9 

§ 4

F g _  [ jl _     o\  % ò † ¾ Ó`  ¦ ~ à Ît  · ú §“ ¦  ×  æ  o 0 p x ô

 Ç F g$ 3 Ä »    \  ¦ s 6   x # Œ V , “ É r 8 £ ¤& ñ # 3 0 A\  ¦ ° ú   H 4 Ÿ ¤

½

+ Ë+ þ A @ /+ þ A ½ ¨› ¸Ó ü t _    + þ A ¢ ¸  H “ : r • ¸    o\  @ /ô  Ç z  ´r ç ß – 8

£ ¤& ñ s  B Ä º  H › ' a d ” _  @ / © œs  ÷ &“ ¦ e ”  . @ /+ þ A “ §| ¾ Ós 



 @ /+ þ A ž Ð3 l q ½ ¨› ¸Ó ü t õ  ° ú  s  ô  Ç { Œ •_  F g$ 3 Ä »\  ¦ : Ÿ x # Œ

#

Œ Q G ' p" f_  8 £ ¤& ñ ’    ñ\  ¦ ×  æ^ o ?r v   H f ” § > = C \ P s  Ô  ¦  x

½ + É  â Ä º 0 Au  “  d ”  0 p x ô  Ç G ' p" f_  Õ ü w  \  ¦ 7 £ x r v   H

´

òÖ  ¦& h “   ~ ½ ÓZ O s  € 9 כ ¹  . F g$ 3 Ä »     G ' p" f_   ×  æ  o

~

½ ÓZ O \   H ß ¼>  TDM (Time Division Multiplexing) [3]õ  WDM (Wavelength Division Multiplexing) [4,5] Ü ¼– Ð   Ð

ü

t à º e ”  . s  ×  æ WDM ~ ½ ÓZ O “ É r F g @ /% i  F g " é ¶ (broadband light source) _   © œ # 3 0 Aü < x 9 ] X  >  › ' aº  ÷ &# Q e ” l  M : ë

 H \  F g$ 3 Ä » G ' p" f_  Õ ü w  \  ¦ 7 £ x r v   H X < ô  Ç>  e ”  .

ì ø

Í • ¸ ± ú “ É r    \  ¦  6   x   H TDM ~ ½ ÓZ O  ¢ ¸ô  Ç SNR 1

p

x _  ë  H ] j& h `  ¦ t “ ¦ e ”  . s  Qô  Ç & h `  ¦ ˜ Ð ¢ - a l  0 AK  0

A_  TDMõ  WDM l Õ ü t`  ¦   ½ + Ë # Œ  6   x   H  כ s  



© œ { 9 ì ø Í& h “   ~ ½ ÓZ O s  . s  ƒ  ½ ¨\ " f Ä ºo   H WDM l Õ ü t

`

 ¦ s 6   x # Œ G ' p" f_  > hà º\  ¦ ´ òõ & h Ü ¼– Ð 7 £ x  l  0 A 

#

Œ y Œ •y Œ •_  F g$ 3 Ä »     G ' p" f\  ¿ º > h s  © œ_   ï× ¼ o  ) a Ú

ÔA Õ ª  © œ`  ¦ C \ P † < ÊÜ ¼– Ð+ ‹ # Œ Q > h_  “ ¦Ä »ô  Ç I Õ ª[ þ t

E-mail: [email protected]

`

 ¦ % 3   H ~ ½ ÓZ O  (spectral tag method) `  ¦ ] jî ß – % i Ü ¼ 9, ×  æ

^ o

? ) a ’    ñ[ þ t _  ç ß –[ O `  ¦ ] j  “ ¦ “    ) a   + þ A\    É r K  {

© œ G ' p" f_  Û ¼& 7 ˜à Ô! 3  s 1 l x`  ¦ r Ó ý t Y Us ‚  `  ¦ : Ÿ x # Œ \ V8 £ ¤

†

< ÊÜ ¼– Ð+ ‹ D h– Ðî  r  ×  æ  o l Õ ü t`  ¦ ƒ  ½ ¨Ù þ ¡ . y Œ • G ' p" f  H " f

–

Ð   É r Û ¼& 7 ˜à Ô! 3 `  ¦ ° ú “ ¦ e ” l  M :ë  H \  œ íl _   © œ 0 Au 

\

" f ×  ¦ # QŽ  H ì ø Í  x ß ¼ü < `  …  ç ß – 0 Au \ " f 7 £ x ô  Ç ì ø Í  x

ß ¼_  ’    ñ[ þ t`  ¦ ì  r$ 3 † < ÊÜ ¼– Ð+ ‹ # QÖ ¼ G ' p" f  Œ •1 l x ÷ &  H t 

· ú

˜ à º e ”  . 7 £ ¤ y Œ • F g$ 3 Ä »     G ' p" f\  " f– Ð   É r “  d ” ³ ð (identification tag) \  ¦  Ò# Œ† < ÊÜ ¼– Ð+ ‹ “ ¦Ä »ô  Ç Û ¼& 7 ˜à Ô! 3  6 £ x

² ú

š: £ ¤$ í `  ¦ % 3 `  ¦ à º e ”  .

II. T  Â ] Ø



×  æ FBG G ' p" f r Û ¼% 7 ›\  & h 6   x| ¨ c à º e ”   H ] jî ß –  ) a Û ¼& 7 ˜ à

Ô! 3  I Õ ª (spectral tag) ~ ½ ÓZ O _  > h| Ä Ì• ¸ Fig. 1\    



e ” Ü ¼ 9, y Œ • G ' p" f " f– Ð   É r Ú ÔA Õ ª  © œ`  ¦ ° ú   H ¿ º F

g$ 3 Ä »     (s ×  æ    ) – Ð ½ ¨$ í  ) a \ V\  ¦ ˜ Ð# Œï  r  . y Œ • G ' p

"

f  H ¿ º > h_  Û ¼& 7 ˜à Ô! 3   ï× ¼ (spectral code) \  ¦ ° ú   H I  Õ

ª (tag)   Ò# Œ  ) a    “ ¦ ³ ð‰ & ³½ + É Ã º e ”  . s M :\  G ' p" f

–

Ð s 6   x| ¨ c à º e ”   H þ j@ / Õ ü w   (n) “ É r d ”  (1) õ  ° ú  s  ³ ð‰ & ³

÷

&# Q| 9  à º e ”  .

n =

N

C

M

= N !

M !(N − M )! , M ≤ N

2 (1) s

 d ” \ " f N“ É r G ' p" f & ñ § > = ? /\  Ÿ í† < ʝ ) a " f– Ð   É r Ú ÔA Õ ª

 © œ (spectral code) _  > hà ºs “ ¦, M“ É r y Œ •y Œ •_  G ' p" f\ 

-418-

(2)

 ƒ  ½ ¨ 7 Hë  H  F g$ 3 Ä »     G ' p" f_  Û ¼& 7 ˜à Ô! 3   ï× ¼\  ¦  Ö ¸6   x ô  Ç  ×  æ  o\  @ /ô  Ç Ã ºu K $ 3  ƒ  ½ ¨ – ’ < H Š҃   1 p x -419-

Fig. 1. Multiple FBG sensor structure with two spectral codes.

Fig. 2. The result of simulation with Opti-Grating (a) and its average (b).

½

+ É{ © œ  ) a    _  > hà ºs  . s ü < ° ú  s   ×  æ  o  ) a FBG G ' p" f _

 Õ ü w  , n“ É r Y > > h_  Û ¼& 7 ˜à Ô! 3   ï× ¼  6   x ÷ &% 3 “ ¦ Å Ò# Q

”

  { 9 § 4  F g " é ¶ _  @ /% i ; Ÿ ¤ \  \ O    ´ ú §“ É r 1 l x{ 9 ô  Ç  ï× ¼ ×  æ

^ o

?÷ &# Q e ”   H t \       & ñ  ) a  . s  Qô  Ç  ×  æ  o  ) a F g$ 3  Ä

»     G ' p" f r Û ¼% 7 ›_  ì  r$ 3 `  ¦ 0 A # Œ F g$ 3 Ä »    _  Û ¼

&

7 ˜à Ô! 3  _ ” > r \  › ' aº   ) a € ª œ& h  & ñ ˜ Ð\  ¦ % 3   H X < Ä »6   x ô  Ç   ½ + Ë

—

¸× ¼s  : r (coupled-mode theory) `  ¦  6   x % i   [6]. Å Ò l

& h  ½ ¨› ¸\ " f é ß –{ 9  — ¸× ¼ F g$ 3 Ä »\  ¦ “ ¦ 9ô  Ç €  , „  l  © œ

“ É

r ~ E(z) = A(z) exp(−iβ

i

z) + B(z) exp(iβ

i

z) ü < ° ú  s  “ ¦ Ä

»ô  Ç — ¸× ¼[ þ t _  ‚  + þ A& h “     ½ + ËÜ ¼– Ð   è ­ q à º e ”  . > à º A(z) ü < B(z)  H y Œ •y Œ • ”  ' Ÿ  ü < ì ø Í  _  ”  ; Ÿ ¤`  ¦    · p



.   ½ + ˗ ¸× ¼ ~ ½ Ó& ñ d ” “ É r d ”  (2) ü < ° ú  s  æ ¼# Œ| 9  à º e ”  .

d

dz A + iδ · A = −iκ · B · e

−iθ

(2) d

dz B − iδ · B = iκ · A · e

−iθ

, δ = β − π Λ

δ  H 0 A © œ & ñ ½ + Ë   à º s “ ¦ κ  H & e  ¦a A  © œÃ ºs  . 0 A d ” _  K

  H z 0 Au \ " f_  „  l  © œõ  Z + ∆ 0 Au \ " f_  „  l  © œ

`

 ¦   ½ + Ër ( ” Ü ¼– Ð+ ‹ Å Òl & h     _  ì  r$ 3 \   © œ & h ½ + Ëô  Ç transfer matrix method [7]\  ¦  6   x # Œ ½ ¨½ + É Ã º e ”  .

Fig. 3. Calculated reflectance spectrums for 6 sensors of double gratings as they are installed successively.

Fig. 4. Simulated reflectance spectrums when the sensor with 1st and 3rd spectral code is strained.

III.  ¹ ō ˜ m { ¢8 ý

]

jî ß –  ) a f ” § > = ƒ    _   ×  æ      H Opti-Grating (Ver.

4.0) `  ¦  6   x # Œ r Ó ý t Y Us ‚   % i “ ¦ s  M :_     _  Ï ã J ] X

Ò  ¦ ì  r Ÿ í  H d ”  (3) ü < ° ú   .

n(z) = ¯ n(z) + δn(z) · sin  2π Λ z



(3) s

 d ” \ " f ¯n(z)  H ¨ î ç  HÏ ã J] X Ò  ¦, δn(z)  H Ï ã J] X Ò  ¦   › ¸ Õ ª o

“ ¦ ˍ  H    _  Å Òl \  ¦    · p . y Œ •y Œ •_  Û ¼& 7 ˜à Ô! 3   ï

×

¼  H “  ] X ô  Ç  ï× ¼\  % ò † ¾ Ó`  ¦ ~ à Ît  · ú §  H þ j™ è ç ß –  “   0.4 nm _  ç ß –  Ü ¼– Ð C u  % i Ü ¼ 9,  8 ´ ú §“ É r G ' p" f_  > hà º\  ¦ % 3  l

 0 AK " f  H  8 ´ ú §“ É r 1 l x{ 9   © œ_  ×  æ^ o ?`  ¦ € 9 כ ¹– Ð l  M : ë

 H \  5 % _  ± ú “ É r ì ø Í Ö  ¦ – Ð ´ ú Æ Ò# Q   + þ A§ 4 \    É r ì ø Í  Û

¼& 7 ˜à Ô! 3 _     o\  ¦ r Ó ý t Y Us ‚   % i  . s M : “  ] X ô  Ç  ï

×

¼  s _   o ü < ì ø Í • ¸  H y Œ •y Œ •    _  Å Òl ü < Ï ã J] X Ò  ¦



 › ¸• ¸ (δn)\  ¦    or &  º ¡ § Ü ¼– Ð+ ‹ › ¸] X ÷ &% 3  . “  ] X ô  Ç x

ß ¼_  ß ¼l \  % ò † ¾ Ó`  ¦ p u   H side lobe[ þ t`  ¦ \ O E l  0 AK 

"

f    _  Ï ã J] X Ò  ¦ ì  r Ÿ í\  d ”  (4) _  Ä ºr î ß – (Gaussian)

†

< ÊÃ º\  ¦  6   x % i  .

A(z) = exp



− ln 2 ·  2(z − L/2) s · L



2



(4) 0

A d ” \ " f  © œÃ º s (taper parameter)   H 0.4 s “ ¦     U  ´ s

 L “ É r 1 cm s  . y Œ •y Œ •_  G ' p" f  s _   o \  ¦ 10 m ç ß –  

(3)

-420- ô  Dz D GÓ ü t o † < Æ rt  “D hÓ ü t o ”, Volume 56, Number 5, 2008¸   5 Z 4

Ü

¼– Ð Ø  æì  r y  b  # Qä ¼§ 4 6 £ § \ • ¸ Ô  ¦ ½ ¨ “ ¦ r Ó ý t Y Us ‚     õ 

–

РÒ'      Š © œ\  _ ô  Ç ç ß –[ O ´ òõ       H  כ `  ¦ Fig.

2 (a) \  ¦ : Ÿ x K  ^  ¦ à º e ”  . s \  ¦ \ O E l  0 A # Œ optical spectrum analyzer _  þ j™ è ì  r K 0 p x õ  ° ú  “ É r 0.01 nm ç ß –  

?

/\ " f % 3 # Q”   — ¸Ž  H à ºu [ þ t`  ¦ ¨ î ç  H % i “ ¦ s   H Fig. 2 (b) \ " f ˜ Ð# Œï  r  . „  ^ ‰  6   x ) a Û ¼& 7 ˜à Ô! 3   ï× ¼_  Õ ü w   (N ) ü <  _  G ' p" f\  Ÿ í† < ʝ ) a    _  > hà º (M)   H y Œ •y Œ • 4 ü < 2 _  ° ú כ`  ¦ 2 [ # Œ r Ó ý t Y Us ‚   % i “ ¦ Fig. 3 \ " f

˜

Ð# Œ t   H  כ õ  ° ú  s  6 > h_  " f– Ð   É r Û ¼& 7 ˜à Ô! 3  I Õ ª[ þ t s

 “ ¦Ä » >  d ” Z > ÷ &# Q| 9  à º e ”  . s  M : y Œ •y Œ •_  x ß ¼  H 3

>

h_  Ú ÔA Õ ª  © œs  ×  æ^ o ?÷ &% 3 Ü ¼ 9 „  ^ ‰ ì ø Í • ¸  H Fig. 3 (f) \ " f ˜ Ð# Œt   H  כ % ƒ! 3  @ /| Ä Ì é ß –{ 9      ì ø Í • ¸_  3 C 

&

ñ • ¸  ) a  . Fig. 4   H G ' p" f 1   \  0 µε Ò'  3000 µε   t

   + þ A`  ¦ & h 6   xÙ þ ¡`  ¦ M :_  ì ø Í  Û ¼& 7 ˜à Ô! 3 s “ ¦, @ /6 £ x   H

¿

º > h_   ï× ¼  © œ  © œ A á ¤ Ü ¼– Ð s 1 l x ÷ &  H  כ `  ¦ S X ‰ “  ½ + É Ã º e ”

 .   + þ A§ 4 \    É r  ï× ¼[ þ t _  ¹ ¡ §f ” “   0 Au \  ¦ S X ‰ “   l  0

A # Œ   + þ As  “  ÷ &% 3 `  ¦ M :_  ì ø Í  Û ¼& 7 ˜à Ô! 3 `  ¦ œ íl  _

 ì ø Í  Û ¼& 7 ˜à Ô! 3 õ  q “ § % i “ ¦ Õ ª   õ   H Fig. 4 _  & h 

‚

 Ü ¼– Ð   Í Ç x . s \  ¦ : Ÿ x K  œ íl _   © œ 0 Au \ " f ×  ¦ # Q

Ž

 H ì ø Í  x ß ¼ü < `  …  ç ß – 0 Au \ " f 7 £ x ô  Ç ì ø Í  x ß ¼_  ’    

ñ[ þ t`  ¦ ì  r$ 3 † < ÊÜ ¼– Ð+ ‹ ' Í   P :ü < [ j   P : Û ¼& 7 ˜à Ô! 3   ï× ¼

\

 ¦ t “ ¦ e ”   H G ' p" f 1  \    + þ As  & h 6   x ÷ &% 3 6 £ §`  ¦ · ú ˜ à º e ”

 .

IV. + s Ç Â ] Ø

G '

p" f_  > hà º\  ¦ ´ òõ & h Ü ¼– Ð 7 £ x  l  0 A # Œ y Œ •y Œ •_  F

g$ 3 Ä »     G ' p" f\  ½ ¨Z >  0 p x ô  Ç Û ¼& 7 ˜à Ô! 3   ï× ¼[ þ t`  ¦ C 

\ P

   H Û ¼& 7 ˜à Ô! 3  I Õ ª ~ ½ ÓZ O `  ¦ ] jî ß – % i  . G ' p" f_  Õ ü w   n“ É r Û ¼& 7 ˜à Ô! 3  I Õ ª_  Õ ü w   Nõ  G ' p" f\  Ÿ í† < ʝ ) a     Õ ü w



 M\  _ K    & ñ  ) a  . 4 > h_  Ú ÔA Õ ª      © œ`  ¦ s 6   x

# Œ 6 > h_  G ' p" f\  ¦ ½ ¨‰ & ³ % i “ ¦, ×  æ^ o ? ) a  © œ_  ç ß –[ O  : £ ¤

$ í

õ  Û ¼à ÔY U“  \    É r  ï× ¼[ þ t _     o\  ¦ r Ó ý t Y Us ‚   † < ÊÜ ¼

–

Ð+ ‹ D h– Ðî  r  ×  æ  o l Õ ü t`  ¦ ƒ  ½ ¨Ù þ ¡ . s  Qô  Ç D h– Ðî  r Û ¼

&

7 ˜à Ô! 3  I Õ ª ~ ½ ÓZ O “ É r ] jô  ǝ ) a G ' p" f r Û ¼% 7 ›_  @ /% i ; Ÿ ¤ ? /\ 

"

f G ' p" f_  Õ ü w  \  ¦ 7 £ x  l  0 Aô  Ç  _  Ä »6   x ô  Ç @ /^ ‰ ~ ½ Ó Z O

s  | ¨ c à º e ” `  ¦  כ s  . ¿ º > h s  © œ_  G ' p" f\    + þ As  “  

÷ &% 3 `  ¦  â Ä º\ • ¸ > h> h_  G ' p" f\  ¦ d ” Z >    H ~ ½ ÓZ O \  @ / ô

 Ç ƒ  ½ ¨ü <  « Ñ% ƒo  · ú ˜“ ¦o 7 £ §`  ¦  Œ •$ í   H ƒ  ½ ¨ ”  ' Ÿ 

×

 æ s  .

P

c p 8 ý ò k >

s

  7 Hë  H“ É r F g ™ èF  Ҿ ¡ §ƒ  ½ ¨G ' p' _  ƒ  ½ ¨q  t " é ¶ \  _ K  Ã

º' Ÿ ÷ &% 3 _ þ v m  .

Y

c p w Š à U Ø ”  ô

[1] M. A. Davis and A. D. Kersey, Electronics Letters 31, 822 (1995).

[2] A. D. Kersey, M. A. Davis, H. J. Patrick, M. LeBlanc and K. P. Koo et al, J. Lightwave Technology 15, 1442 (1997).

[3] S. Liu, Y. Yu, J. Zhang and X. Chen, IEEE Photonics Technology Letters 19, 1493 (2007).

[4] P. K. C. Chan, W. Jin and M. S. Demokan, IEEE J. Selected Topics in Quantum Electronics 6, 756 (2000).

[5] Y. Yu, L. Lui, H. Tam and W. Chung, IEEE Photon- ics Technology Letters 13, 702 (2001).

[6] A. Yariv, IEEE Journal of Quantum Electronics QE- 9, 919 (1973).

[7] M. Yamada, K. Sakura, Applied Optics 26, 3474

(1987).

(4)

 ƒ  ½ ¨ 7 Hë  H  F g$ 3 Ä »     G ' p" f_  Û ¼& 7 ˜à Ô! 3   ï× ¼\  ¦  Ö ¸6   x ô  Ç  ×  æ  o\  @ /ô  Ç Ã ºu K $ 3  ƒ  ½ ¨ – ’ < H Š҃   1 p x -421-

Numerical Analysis on the Multiplexing of a Fiber Bragg Grating Employing a Spectral Code

Ju-Youn Son, Ki-Sun Choi, Geun-Jin Kim, Kyoung-Shin Lee, Dong-Young Park, Jae-Soon Youn, Se-Jong Baik and Kiegon Im

Department of Physics, Chonnam National University, Gwangju 500-757

(Received 5 March 2008)

A multiplexing technique for fiber Bragg grating sensors is required for multipoint measurements such as smart structure applications. The spectral tag method can enhance the multiplexing ca- pability in the Wavelength Division Multiplexing (WDM) approach without additional switching units. Each sensor is assigned with a unique spectral tag that represents a series of Bragg wave- lengths. The maximum number of sensors in a single optical fiber is determined by the number of employed spectral codes and the number of constituent gratings. With a 0.4-nm peak-to-peak separation and a 5 % reflectance of the grating, we simulated the change caused in the multiplexed spectrum by the strain to determine the position of the sensor and to measure the degree of its change.

PACS numbers: 42.81.P, 42.79.D, 07.10.P

Keywords: Fiber Bragg grating sensor array, Spectral tag method, Wavelength division multiplexing, Strain monitoring, Spectral code

E-mail: [email protected]

수치

Fig. 3. Calculated reflectance spectrums for 6 sensors of double gratings as they are installed successively.

참조

관련 문서

Modern Physics for Scientists and Engineers International Edition,

Five days later, on 15 January 1975, the Portuguese government signed an agreement with the MPLA, FNLA and UNITA providing for Angola to receive its independence on 11

What is the number of square units in the area of a triangle whose sides measure 5, 5 and

Usefulness of co-treatment with immunomodulators in patients with inflammatory bowel disease treated with scheduled infliximab maintenance therapy.. Oussalah A, Chevaux JB, Fay

Since every classical or virtual knot is equivalent to the unknot via a sequence of the extended Reidmeister moves together with the forbidden moves, illustrated in Section 2,

Inclusion and Inclusiveness: Shared Vision of Youth for Local, National, and Global Village Inclusion at large stands for embracing populations with disabilities and

A phylogenetic tree obtained by the neighbor-joining method revealed that five sequence (SMS-1, 2, 5, 6, 7) from the squirrel monkey and three sequences (NM6-4, 5, 9) from

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