• 검색 결과가 없습니다.

X Øy ¢Ñ ÷  ¹ Œ ½; c  \ ¥ 7 _T $ [ T ~ ¾© Ž8 ý ® oà à ŠX ê s — ¤V R ËÊ Ý Nd:YAG 7 _T $ [8 ý û s ÚI í Ä ì Å× D; c å ¾ ˔ X ¢ Ž ì ŏ Œ

N/A
N/A
Protected

Academic year: 2021

Share "X Øy ¢Ñ ÷  ¹ Œ ½; c  \ ¥ 7 _T $ [ T ~ ¾© Ž8 ý ® oà à ŠX ê s — ¤V R ËÊ Ý Nd:YAG 7 _T $ [8 ý û s ÚI í Ä ì Å× D; c å ¾ ˔ X ¢ Ž ì ŏ Œ"

Copied!
8
0
0

로드 중.... (전체 텍스트 보기)

전체 글

(1)

Æ

X Øy ¢Ñ ÷  ¹ Œ ½; c   \ ¥ 7 _T $ [  T ~ ¾© Ž8 ý ®  oà à ŠX ê s — ¤V R ËÊ Ý Nd:YAG 7 _T $ [8 ý û s ÚI í Ä  ì Å× D; c å ¾ ˔ X ¢ Ž ì ŏ Œ

™ »   · ™ »# Ü  ‘ ž · ~ ç ¡¹ ÿ › G ž B · © ¼U ] 8 ; · ™ »' Ö <4 w H · ™ » ÷ 7 BM 

/ B

N Å Ò@ /† < Ɠ § Ó ü t o † < Æõ , / B N Å Ò 314-701

ƒ

‘

š ø ¶ B] 8 ; ·  ™ »0 ï FŒ ‰ x

ô

 Dz D G…  ;ë  Hƒ  ½ ¨" é ¶, @ /„   305-764

™ »%  g ` @

ô

 ǵ 1 ×@ /† < Ɠ § “ §€ ª œ† < ÆÂ Ò, 305-719

(2008¸   7 Z 4 21{ 9  ~ à Î6 £ §, þ j7 á x‘ : r 2008¸   9 Z 4 19{ 9  ~ à Î6 £ §)

Nd:YAG “ ¦^ ‰Y Us $ _  # Œl  F g Ü ¼– Ð æ ¼s   H Y Us $   s š ¸× ¼ (Laser diode;LD)_  1 l x  Œ • “ : r • ¸ü < “  

„  À Ó\    É r # Œl   © œ_  : £ ¤$ í `  ¦ S X ‰ “   % i  . Nd:YAG   & ñ _  Å Ò f  ¨ à º  © œ“   808 nm\  ¦ ×  æd ” Ü ¼– Ð y

Œ

•y Œ •_  “  „  À Ó\ " f Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸\    É r ¨ î ç  H  © œ    oÖ  ¦“ É r 0.31 nm/

C s “ ¦, Y U s

$   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ 25

C \ " f_  “  „  À Ó\    É r  © œ    oÖ  ¦“ É r 0.22 nm/Ae ” `  ¦ S X ‰ “   % i 



. s    õ  Y Us $   s š ¸× ¼_  “  „  À Ó\     1 l x  Œ • “ : r • ¸\  ¦    or &  Y Us $   s š ¸× ¼_  # Œl  ×  æ d ”

  © œ`  ¦ 808 nm – Ð › ¸] X ½ + É Ã º e ” % 3  . s \  ¦  „ ½ ÓÜ ¼– Ð # Œl  F g _   © œ\    É r 7 á x # Œl  Nd:YAG Y Us $  _

 Ø  ¦§ 4 : £ ¤$ í `  ¦ · ú ˜  ‘ : r   õ  # Œl  F g _   © œ`  ¦ 808 nm – Ð # Œ Nd:YAG   & ñ `  ¦ # Œl  % i `  ¦ M :_  Ø  ¦§ 4  s

 808 nm     # Œl c ”  ˜ Ð  0.2 ∼ 0.5 W& ñ • ¸  H  כ `  ¦ S X ‰ “   % i  . 7 á x # Œl  Nd:YAG Y Us $ _  ë  H )

3

 Ø  ¦§ 4 “ É r 808 nm – Ð # Œl  % i `  ¦ M : 808 nm     # Œl c ”  ˜ Ð  €  • 1.3 W& ñ • ¸ ± ú “ É r  כ `  ¦ S X ‰ “   % i 



. ‘ : r ƒ  ½ ¨\  ¦ : Ÿ x K  “ ¦^ ‰ Y Us $ _  î ß –& ñ & h s “ ¦ & ñ S X ‰ ô  Ç ½ ¨1 l x`  ¦ 0 AK " f  H Y Us $   s š ¸× ¼_  # Œl  



© œs  808 nm ÷ &• ¸2 Ÿ ¤ Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸\  ¦ › ¸] X    H  כ s  Nd:YAG Y Us $ _  Ø  ¦§ 4 `  ¦ ´ ò Ö 

¦& h Ü ¼– Ð  6   x ½ + É Ã º e ”   H ~ ½ ÓZ O e ” `  ¦ z  ´+ « >& h Ü ¼– Ð ˜ Ð% i  .

PACS numbers: 42.55.Px, 42.55.Xi, 42.60.Lh

Keywords: Y Us $   s š ¸× ¼, Nd:YAG Y Us $ , 7 á x # Œl , “ : r • ¸ü < „  À Ó\    É r Û ¼& 7 ˜à Ô! 3     o,  © œ    oÖ  ¦

I. " e  ] Ø

‰

&

³F  “ ¦^ ‰ Y Us $   H _ « Ñü < í ß –\ O , † ½ Ó/ B N Ä ºÅ Ò 1 p x _  ì  r  

\

 ¦  Å  [ þ t # Q  € ª œ >  6 £ x6   x ÷ &“ ¦ e ”  . “ ¦^ ‰Y Us $ _   

€

ª œô  Ç 6 £ x6   x \     # Œl  F g _  7 á x À Óü < + þ AI  ¢ ¸ô  Ç  € ª œ o ÷ &

%

3 l \  “ ¦^ ‰ Y Us $ \  ¦ ] j Œ • “ ¦ > hµ 1 Ï   H X < e ” # Q 6   x • ¸

\

 ´ ú   H & h ] X ô  Ç # Œl  F g _  ‚  × þ ˜s  F g  © œy  ×  æ כ ¹  . s 

\

    7 á x # Œl    H “ ¦^ ‰ Y Us $ \ " f כ ¹½ ¨÷ &  H # Œl  F g _

 : £ ¤$ í \  @ /ô  Ç ƒ  ½ ¨ ‚  ' Ÿ & h Ü ¼– Ð Ã º' Ÿ ÷ &% 3 Ü ¼ 9 [1, 2]

#

Œl  F g ×  æ \   “   Y Us $   s š ¸× ¼ (Laser diode; LD)

\

 ¦ 7 á x # Œl  ~ ½ Ód ” _  “ ¦^ ‰ Y Us $ \  ŠҖ Ð s 6   x “ ¦ e ”  . Y U s

$   s š ¸× ¼\  ¦ “ ¦^ ‰ Y Us $ _  # Œl  F g Ü ¼– Ð s 6   x ½ + É  â Ä

º “ ¦^ ‰ Y Us $  r Û ¼% 7 ›_  ´ òÖ  ¦`  ¦ Z  } s “ ¦ à º" î `  ¦ Z þ tw n = à º

E-mail: [email protected]

e ”

`  ¦ ÷  r ë ß –  m   c ”  | 9 `  ¦ a % ~ >  ½ + É Ã º e ”  . ¢ ¸ô  Ç ` O Û ¼ ì ø Í 4

Ÿ

¤Ò  ¦`  ¦ 7 £ x r ~  ´ à º e ” # Q e  ¦ A r Ï þ ›á Ô\  ¦ # Œl  F g Ü ¼– Ð   6

 

x ô  Ç Y Us $  ˜ Ð  “ ¦ì ø Í4 Ÿ ¤Ö  ¦ _  ` O Û ¼ Y Us $ \  ¦ ] j Œ •   H X

< 6   x s  “ ¦ ™ è+ þ A o ] j Œ •s  / '0 > Y Us $  “  / B N 0 A$ í Æ Ò& h  r

Û ¼% 7 › (Satellite Laser Ranging; SLR) 1 p x  € ª œô  Ç Y Us $  r

Û ¼% 7 ›Ü ¼– Ð_  6 £ x6   x s  0 p x   [3–8]. s  Qô  Ç  © œ& h [ þ t`  ¦

t   H Y Us $   s š ¸× ¼\  ¦ s 6   x ô  Ç “ ¦^ ‰ Y Us $ [ þ t s  Y U s

$  r  © œ\ " f y Œ • F g ~ à Γ ¦ e ” # Q Y Us $   s š ¸× ¼\  ¦ “ ¦^ ‰ Y

Us $ _  # Œl  F g Ü ¼– Ð  6   x “ ¦  ½ + É M : Õ ª : £ ¤$ í `  ¦ ¸ ú ˜ s  K

 “ ¦ € Œ •   H  כ s  B Ä º ×  æ כ ¹  . s \  ¦ : Ÿ x K " f Y Us 

$

 “  / B N 0 A$ í Æ Ò& h l Õ ü t 1 p x Y Us $ \  ¦ > hµ 1 Ï   H l d  ¦`  ¦   º

  “ ¦  ô  Ç .

III-V7 á ¤  o½ + ËÓ ü t ì ø ͕ ¸^ ‰– Ð s À Ò# Q”   Y Us $   s š ¸× ¼  H 1

l

x  Œ • “ : r • ¸\      € ª œô  Ç µ 1 ϔ   : £ ¤$ í [ þ t`  ¦    · p . \ V\  ¦

-261-

(2)



s š ¸× ¼_  \ P & h  : £ ¤$ í `  ¦ ½ ©" î  9  H ´ ú §“ É r ƒ  ½ ¨[ þ t s  à º '

Ÿ ÷ &% 3   [11–14]. t F K  t  à º' Ÿ  ) a ƒ  ½ ¨  H Y Us $   s 

š

¸× ¼\  ¦ s À ҍ  H ì ø ͕ ¸^ ‰ Ó ü t| 9 õ  Y Us $   s š ¸× ¼_  ½ ¨› ¸ ü

< › ' aº   # Œ Õ ª\    É r \ P & h “   : £ ¤$ í `  ¦ S X ‰ “  ô  Ç  כ s  @ /Â Ò ì

 r s  . s   H # Œ Q + þ AI ü < ½ ¨› ¸\  ¦ t   H Y Us $   s š ¸

×

¼_  \ P & h “   : £ ¤$ í `  ¦ € Œ • “ ¦    H  כ Ü ¼– Ð Y Us $    s

š ¸× ¼_  î ß –& ñ & h “    © œ6   x  o\  e ” # Q" f • ¸¹ ¡ § s  ÷ &t ë ß – Y U s

$   s š ¸× ¼ “ ¦^ ‰ Y Us $ _  # Œl  F g Ü ¼– Ð  6   x ÷ &% 3 `  ¦ M

: Y Us $  µ 1 ϔ  \  p u   H % ò † ¾ Ó t   H “ ¦ 9 t  3 l w ô  Ç .



 " f “ ¦^ ‰ Y Us $ _  ] j Œ •õ  > hµ 1 Ï\  · ú ¡" f Y Us $   s 

š

¸× ¼_  \ P & h  : £ ¤$ í \  › ' a ô  Ç ƒ  ½ ¨ { 9  & h Ü ¼– Ð Ã º' Ÿ ÷ &# Q



  9 z  ´] j– Ð Y Us $   s š ¸× ¼\  ¦ “ ¦^ ‰ Y Us $ _  # Œl  F

g Ü ¼– Ð  6   x % i `  ¦ M : Y Us $   s š ¸× ¼_  \ P & h  : £ ¤$ í s  Y

Us $  µ 1 ϔ  \  p u   H % ò † ¾ Ó`  ¦ S X ‰ “  ½ + É € 9 כ ¹ e ”  . s  õ 

&

ñ \ " f Y Us $   s š ¸× ¼_  1 l x  Œ •“ : r • ¸\    É r  © œ   o\  ¦ é

ß –í  H y  › ' a ¹ 1 Ï   H  כ s      \ V8 £ ¤ ½ + É Ã º e ”   H à ºd ” `  ¦  Ž 7 £ x

# Œ  “ ¦ s \  ¦ : Ÿ x ô  Ç Y Us $   s š ¸× ¼_  ˜ Ð  ´ òÖ  ¦& h 

“

   6   x Ü ¼– Ð “ ¦^ ‰ Y Us $ _  Ø  ¦§ 4 7 £ x \  ¦ s = å J # Q ? / ô  Ç



.

‘

: r ƒ  ½ ¨\ " f  H 808 nm \ " f f  ¨ à º\  ¦   H Nd:YAG   & ñ _

 # Œl  F g " é ¶ Ü ¼– Ð  6   x| ¨ c Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ ü

< “  „  À Ó\    É r µ 1 ϔ   Û ¼& 7 ˜à Ô! 3 _  : £ ¤$ í `  ¦  [ jy  ¶ ú ˜ (

R˜ Г ¦ Õ ª : £ ¤$ í `  ¦ ƒ  ½ ¨ % i  . ¢ ¸ô  Ç Nd:YAG Y Us $ _  ]

j Œ •\  e ” # Q # Œl  F g " é ¶ Ü ¼– Ð  6   x ÷ &  H Y Us $   s š ¸× ¼_ 

#

Œl  ×  æd ”   © œs  “ : r • ¸ü < „  À Ó_     o\     808 nm– Ð

#

Œl    H  â Ä ºü < 808 nm  u  ´  â Ä º\  7 á x # Œl  Nd:YAG Y

Us $ _  Ø  ¦§ 4  : £ ¤$ í \  # Qb  G>  % ò † ¾ Ó`  ¦ p u   H t \  @ / 

#

Œ ƒ  ½ ¨ % i  .

II. ÷ m Ç] M ö õ m Í • ¤X N Ë

Y

Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ü < “  „  À Ó\    É r # Œ l

 Û ¼& 7 ˜à Ô! 3  : £ ¤$ í `  ¦ · ú ˜ ˜ Ðl  0 Aô  Ç z  ´+ « > © œu   H Fig. 1 õ 

° ú

  . ‘ : r z  ´+ « >\   6   x ) a Y Us $   s š ¸× ¼  H THALES   _

 TH-C1722-F6— ¸4 S qs  9 ³ ðï  r  © œ“ É r 808 nm s “ ¦ Û ¼& 7 ˜ à

Ô! 3 _  ; Ÿ ¤ (Full Width at Half Maximum; FWHM)“ É r 3

Fig. 1. The experimental setup for the measurement of the laser diode spectrum.

nm s  s  . Y Us $   s š ¸× ¼\  _ K  µ 1 ϔ   ) a c ” “ É r 1.5m U

 ´s _  F g$ 3 Ä »\  ¦ : Ÿ x K  y n Cs  „  5 Å x ÷ & 9, Y Us $   s š ¸× ¼

?

/ Ò\  “ : r • ¸ y Œ ™t \  ¦ 0 Aô  Ç \ P „  t  (thermocouple)  © œ‚ à Ì

÷

&# Q e ”  . Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ 25

C \ " f ƒ   5

Å q` O Û ¼_  Ø  ¦§ 4 “ É r 20 W s  9 f ”  â s  600 µm, ½ ¨ â (Nu- merical Aperture; NA) s  0.22“   F g$ 3 Ä »ü < ƒ    ÷ &# Q e ” 



. Y Us $   s š ¸× ¼_  “ : r • ¸  H ? / Ò_  \ P „  t _  $ † ½ Ó ° ú כ

`

 ¦ { 9 # Q 8 £ ¤& ñ % i “ ¦, 25

C \ " f 10 kΩ_  $ † ½ Ó`  ¦ t  9 Í ‰

ty Œ •l \  _ K  í  H¨ 8 Š   H Í ‰ ty Œ •à º\  ¦ s 6   x # Œ “ : r • ¸\  ¦ › ¸ ] X

 % i  . Í ‰ ty Œ •l – Ѝ  H SPEED Engineering  _  SPEED- 650L — ¸4 S q`  ¦  6   x % i Ü ¼ 9 Í ‰ ty Œ •à º– Ѝ  H œ íí  H à º\  ¦  6   x 

%

i  . Y Us $   s š ¸× ¼– Ð_  „  À ÓÅ Ò{ 9 `  ¦ 0 AK  Agilent  _

 — ¸4 S q" î 6651A]J03“   f ” À Ó „  " é ¶/ B N/ å L l \  ¦  6   x % i “ ¦ 0 V ∼ 6 V, 0 A ∼ 60 A _  „  " é ¶`  ¦ / B N/ å L ½ + É Ã º e ”  . ì  rF g l

  H Princeton Instruments  _  SP-306— ¸4 S q`  ¦  6   x 

%

i “ ¦ s M : 8 £ ¤& ñ \   6   x ô  Ç      H 1200 groove/mm s  9 Û

¼& 7 ˜à Ô! 3  8 £ ¤& ñ # 3 0 A  H 780 nm \ " f 820 nms  .

Y

Us $   s š ¸× ¼_  Û ¼& 7 ˜à Ô! 3  : £ ¤$ í `  ¦ · ú ˜ ˜ Ðl  0 Aô  Ç z  ´ +

«

>“ É r  6 £ § õ  ° ú  s  ¿ º t – Ð  ¾ º# Q ”  ' Ÿ  % i  . ' Í P :, Y

Us $   s š ¸× ¼_  ? /Â Ò “ : r • ¸    o\    É r # Œl  Û ¼& 7 ˜à Ô

! 3

 : £ ¤$ í `  ¦ · ú ˜ ˜ Ðl  0 Aô  Ç z  ´+ « >Ü ¼– Ð Y Us $   s š ¸× ¼_ 

?

/Â Ò “ : r • ¸\  ¦ 15

C \ " f 35

C  t  2

C ç ß –  Ü ¼– Ð    o r

(  Ü ¼ 9, s  M : Y Us $   s š ¸× ¼\  K ï  r „  À Ӎ  H 5 A, 10 A, 20 A, 30 A, 40 A – Ð y Œ • “  „  À Ó\ " f Ø  ¦§ 4  c ” _  Û

¼& 7 ˜à Ô! 3 `  ¦ 8 £ ¤& ñ % i  . Ñ ü t P :, Y Us $   s š ¸× ¼\  K  ï

 r „  À Ó_     o\    É r # Œl  Û ¼& 7 ˜à Ô! 3  : £ ¤$ í `  ¦ · ú ˜ ˜ Ðl  0

AK  Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸\  ¦ 25

C – Ð “ ¦& ñ r v 

“

¦ Y Us $   s š ¸× ¼\  “  K ï  r „  À Ó\  ¦ 10 A \ " f 40 A



t  2 A ç ß –  Ü ¼– Ð    or &  # Œl  Û ¼& 7 ˜à Ô! 3 `  ¦ 8 £ ¤& ñ % i 



. s  Qô  Ç — ¸Ž  H Y Us $   s š ¸× ¼_  # Œl  Û ¼& 7 ˜à Ô! 3 _  8 £ ¤

(3)

Fig. 2. The experimental setup for the measurement of output power of the Nd:YAG laser.

&

ñ “ É r Í ‰ ty Œ •l \  ¦ s 6   x ô  Ç  s š ¸× ¼ Ø  ¦§ 4  c ” s  Ø  æì  r ô  Ç î ß –& ñ



o s À Ò# Q”    6 £ § \  z  ´r  % i  .

0

A z  ´+ « >`  ¦  „ ½ ÓÜ ¼– Ð Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ü <

„

 À Ó\  ¦    or &  µ 1 ϔ   Û ¼& 7 ˜à Ô! 3 _  ×  æd ”   © œs  808 nm“  

 â

Ä ºü < 808 nm      â Ä º– Ð Nd:YAG Y Us $ \  ¦ µ 1 ϔ  r 

&

 Ø  ¦§ 4 _  : £ ¤$ í `  ¦ · ú ˜ ˜ Ѐ Œ ¤ . # Œl  F g`  ¦ 808 nm – Ð µ 1 ϔ  

½

+ É  â Ä º\   H Y Us $   s š ¸× ¼\  „  À Ó\  ¦ 14 A \ " f 42 A  t

 2 Aç ß –  Ü ¼– Ð K ŠҀ  " f y Œ • “  „  À Ó\  K { © œ   H Y U s

$   s š ¸× ¼_  & h & ñ 1 l x  Œ • “ : r • ¸\  ¦ [ O & ñ # Œ 808 nm\  ¦ µ

1 ϔ  r &  z  ´+ « >`  ¦ z  ´' Ÿ  % i Ü ¼ 9, # Œl  F g s  808 nm  



   â Ä º\   H Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸\  ¦ 25

C – Ð

“

¦& ñ “ ¦ “  „  À Óë ß – 14 A\ " f 42 A t  2 Aç ß –  Ü ¼– Ð



  or &  z  ´' Ÿ  % i  . # Œl  F g \    É r Nd:YAG Y Us $ _  Ø

 ¦§ 4  : £ ¤$ í `  ¦ · ú ˜ ˜ Ѝ  H z  ´+ « >  © œu   H Fig. 2 ü < ° ú   . YAG

 

& ñ \  @ /ô  Ç Nd_  • ¸i ç 0 l x • ¸  H 1 % s  9, ¿ º> h_  r ï  rE $ ™ Ý

¼ (collimation lens)ü < œ í& h  o  35 mm“   | 9 5 Å qE $ ™Ý ¼ (focusing lens)\  ¦  6   x # Œ Nd:YAG   & ñ \  c ” `  ¦ | 9 5 Å q r  ( 

“ ¦ Ø  ¦§ 4  ⠓ É r ì ø Í Ö  ¦ s  70 %“    כ `  ¦  6   x % i  . / B N”   l

_   o \  ¦ 30 mm, 50 mm, 70 mm, 100 mm – Ð # Œ y Œ • y

Œ

•_  / B N”  l \ " f # Œl  F g _  ×  æd ”   © œs  808 nm“    © œõ  808 nm       © œÜ ¼– Ð Nd:YAG Y Us $ \  ¦ µ 1 ϔ  r &  Ø  ¦

§

4 _     o\  ¦ 8 £ ¤& ñ % i “ ¦ / B N”  l _   o \    É r Ø  ¦§ 4 _ 



  o• ¸ · ú ˜ ˜ Ѐ Œ ¤ . # Œl \ " f „   ì ø Í  â õ  Nd:YAG   

&

ñ  s _   o   H 34 mm – Ð “ ¦& ñ r v “ ¦ Nd:YAG   & ñ _

 ¢ ¸   É r €   = å Q \ " f Ø  ¦§ 4  â  t _   o \  ¦    or &  / B N

”

 l _   o \  ¦ › ¸] X  % i  .

III. + s ÇÊ Ý õ m Í À X Ø8 ý

1. 7 _T $ [  T ~ ¾© Ž8 ý Ž Ò ÞX c l Æ X Øy ¢; c   \ ¥ X ê s8 ý

 ì Å× D

Fig. 3“ É r Y Us $   s š ¸× ¼_  “  „  À Ó 30 A{ 9  M : Y U s

$   s š ¸× ¼_  1 l x  Œ • “ : r • ¸    o\    É r # Œl   © œ_  Û ¼

Fig. 3. The emission spectra of the laser diode as a func- tion of operating temperature at 30 A injection current.

&

7 ˜à Ô! 3 `  ¦    · p  כ s  . Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸

 16

C \ " f 35

C  t  Z  }  f ” \     # Œl  Û ¼& 7 ˜à Ô! 3  _

 ×  æd ”   © œs   © œs  |   A á ¤ Ü ¼– Ð s 1 l x “ ¦ e ” 6 £ §`  ¦ · ú ˜ à º e ”

 . s ü < ° ú  “ É r  © œ_  „  s ‰ & ³ © œ“ É r Y Us $   s š ¸× ¼\  /

B

N/ å L   H   É r “  „  À Ó\ " f• ¸ 1 l x{ 9  >  Y Us $   s š ¸

×

¼_  1 l x  Œ • “ : r • ¸ Z  }  f ” \     ×  æd ”   © œs  |   A á ¤ Ü ¼– Ð s

1 l x † < Ê`  ¦ S X ‰ “   % i  .

Fig. 3 \ " f Y Us $   s š ¸× ¼_  “  „  À Ó 30 A{ 9  M : Nd:YAG   & ñ _  þ j@ / f  ¨ à º  © œ“   808 nm_  # Œl  F g µ 1 ϔ  

\

  H Y Us $   s š ¸× ¼_  1 l x  Œ •“ : r • ¸ 30

C   © œ & h ½ + Ë

†

< Ê`  ¦ · ú ˜ à º e ”  . Y Us $   s š ¸× ¼_  µ 1 ϔ    © œs  “ ¦ · ú ˜



9”   808 nm\  ¦ l ï  r Ü ¼– Ð “  „  À Ó\    É r  © œ_  s 1 l x

&

ñ • ¸ (∆λ)\  ¦ “ : r • ¸_  † < Êà º– Ð ³ ð‰ & ³ # Œ 8 £ ¤& ñ ô  Ç  כ s  Fig.

4 s  . s  Õ ªa Ë >\ " f f ” ‚  _  l Ö  ¦ l  (slope)  H y Œ • “  „   À

Ó\ " f_   © œ„  s Ö  ¦ s  9, Õ ª ° ú כ“ É r 5 A, 10 A, 20 A, 30 A, 40 A \ " f y Œ •y Œ • 0.3 nm/

C, 0.30 nm/

C, 0.31 nm/

C, 0.32 nm/

C, 0.32 nm/

C – Ð Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r

•

¸   o\    É r ¨ î ç  H  © œ„  s Ö  ¦“ É r 0.31 nm/

C – Ð y Œ • “  

„  À Ó\ " f_   © œ„  s Ö  ¦ s   _  { 9 & ñ † < Ê`  ¦ S X ‰ “   % i  .

‚ Ã

Г ¦ë  H‰  ³ [6]\   Ø Ô€   808 nm_  ×  æd ”   © œ`  ¦ t   H AlGaAs ½ ¨› ¸_  Y Us $   s š ¸× ¼_   © œ„  s Ö  ¦“ É r 0.3 nm/

C  “ ¦ " î r ÷ &# Q e ”   H X <, ‘ : r ƒ  ½ ¨_  8 £ ¤& ñ ° ú כs  s ü <

¸ ú

˜ { 9 u  % i 6 £ §`  ¦ S X ‰ “   % i  . ¢ ¸ô  Ç { 9 & ñ ô  Ç “ : r • ¸ 25

C

\

" f “  „  À Ó_     o\    É r Y Us $   s š ¸× ¼_  Û ¼& 7 ˜ à

Ô! 3  : £ ¤$ í `  ¦ 8 £ ¤& ñ ô  Ç   õ  “  „  À Ó\  _ ô  Ç  © œ„  s Ö  ¦

“

É r 0.22 nm/Ae ” `  ¦ S X ‰ “   % i “ ¦, “ : r • ¸\  _ ô  Ç  © œ„  s Ö  ¦ 0.31 nm/

C ü < q “ § % i `  ¦ M : Y Us $   s š ¸× ¼_  µ 1 ϔ   Û

¼& 7 ˜à Ô! 3     o\  p u   H % ò † ¾ ӓ É r Y Us $   s š ¸× ¼_  1 l x



Œ

• “ : r • ¸\  _ ô  Ç  כ s  “  „  À Ó\  _ ô  Ç  כ ˜ Ð   p u`  ¦ · ú ˜ à º

(4)

Fig. 4. The wavelength shift ratio of the laser diode as a function of operating temperature at each injection current.

e ”

% 3  . Y Us $   s š ¸× ¼ µ 1 ϔ   Û ¼& 7 ˜à Ô! 3 _  FWHM ; Ÿ ¤`  ¦ 8

£ ¤& ñ ô  Ç   õ  µ 1 ϔ   Û ¼& 7 ˜à Ô! 3 _  FWHM ; Ÿ ¤ • ¸ “ : r • ¸ü < „  À Ó _

 % ò † ¾ Ó`  ¦ ~ à ΍  H  כ Ü ¼– Ð   z Œ ¤ . Y Us $   s š ¸× ¼_  1 l x



Œ

• “ : r • ¸   o\    É r µ 1 ϔ   Û ¼& 7 ˜à Ô! 3 _  FWHM ; Ÿ ¤“ É r    o

t ë ß – ½ ©g Ë :$ í `  ¦ { t   H · ú §€ Œ ¤“ ¦ “  „  À Ó_     o\   

 É

r µ 1 ϔ   Û ¼& 7 ˜à Ô! 3 _  FWHM ; Ÿ ¤“ É r “  „  À Ó Z  }  f ” \ 



  Û ¼& 7 ˜à Ô! 3 _  FWHM ; Ÿ ¤ s  & t   H  כ `  ¦ S X ‰ “   % i  .

“

 „  À Ó 5 A\ " f_  Y Us $   s š ¸× ¼_  Û ¼& 7 ˜à Ô! 3 `  ¦ ˜ Ð

€

  FWHM ; Ÿ ¤ s  ¨ î ç  H 15.59 nm – Ð   É r “  „  À Ó\ " f_  FWHM ; Ÿ ¤ ˜ Ð  €  • 14 nm& ñ • ¸ V , “ É r  כ Ü ¼– Ð S X ‰ “  ÷ &% 3  .

s

  H “  „  À Ó 5 A\ " f Y Us $   s š ¸× ¼_  c ”  | 9 s  Ä ºÃ º

t  · ú §6 £ §`  ¦   ? /“ ¦ s X O >  ± ú “ É r # Œl „  À Ó\ " f_    s

š ¸× ¼ # Œl   H “ ¦^ ‰ Y Us $ _  # Œl  F g Ü ¼– Ð & h ½ + Ë t  · ú § 6

£

§`  ¦ · ú ˜ à º e ”  .

2. 7 _T $ [  T ~ ¾© Ž8 ý ß Ã Å ¹ Œ ½; c   \ ¥ X ê s8 ý

 ì Å× D

Fig. 5  H Y Us $   s š ¸× ¼_  1 l x  Œ •“ : r • ¸ 25

C \ " f “  

„  À Ó\    É r # Œl   © œ_  Û ¼& 7 ˜à Ô! 3 `  ¦    · p . “  

„

 À Ó Z  }  f ” \     # Œl  Û ¼& 7 ˜à Ô! 3 _  ×  æd ”   © œs  |   A

á

¤ Ü ¼– Ð s 1 l x   H  כ s  S X ‰ “  ÷ &% 3 “ ¦ FWHM ; Ÿ ¤ ¢ ¸ô  Ç V , 

#

Qt   H  כ `  ¦ S X ‰ “   % i  . y Œ • “   „  À Ó 10 A, 20 A, 30 A, 40 A \ " f 8 £ ¤& ñ ô  Ç ×  æd ”   © œ“ É r y Œ •y Œ • 802.60 nm, 804.69 nm, 806.75 nm, 809.30 nm s  9 36 A\ " f_  ×  æd ”   © œ“ É r 808.25 nm – Ð 808 nm\   © œ ¾ ú š .   " f Y Us $   s 

š

¸× ¼_  1 l x  Œ • “ : r • ¸ 25

C \ " f 36 A_  „  À Ó\  ¦ f  Ë  9Å Ò% 3 `  ¦ M

: 808 nm\   © œ  î  r y n Cs  µ 1 ϔ  † < Ê`  ¦ · ú ˜ à º e ”  . z  ´

Fig. 5. Dependence of the laser diode spectra as a func- tion of injection current at 25

C operating temperature.

Fig. 6. The wavelength shift ratio of the laser diode as a function of injection current at 25

C operating temper- ature.

+

« >\   6   x  ) a Y Us $   s š ¸× ¼\  ¦ 7 á x # Œl  Nd:YAG Y Us 

$

_  # Œl  F g Ü ¼– Ð  6   x ½ + É  â Ä º & h # Q• ¸ 807 nm\ " f 809 nm _  ×  æd ”   © œ`  ¦ t   H y n C`  ¦ µ 1 ϔ  r &     H X < s   H Y

Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ 25

C{ 9  M : Y Us $    s

š ¸× ¼\  32 A\ " f 40 A  s _  „  À Ó\  ¦ f  Ë  9Å Ò# Q  † < Ê

`

 ¦ ´ ú ˜ô  Ç . “  „  À Ó\  _ ô  Ç Y Us $   s š ¸× ¼_   © œ„   s

Ö  ¦“ É r # Œl  Û ¼& 7 ˜à Ô! 3 _  ×  æd ”   © œ\  @ /ô  Ç „  À Ó_  † < Êà º

–

Ð ³ ð‰ & ³ # Œ Fig. 6\  ˜ Ð% i Ü ¼ 9, Õ ª l Ö  ¦ l   – Ð  © œ

„

 s Ö  ¦ s  . 8 £ ¤& ñ ô  Ç “  „  À Ó\  _ ô  Ç  © œ„  s Ö  ¦“ É r 0.22 nm/A s % 3  .

0

A_    õ \ " f Nd:YAG   & ñ _  f  ¨ à º  © œ“   808 nm\  ¦ µ

1 ϔ  r v   H Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸\  ¦ “  „  À Ó\ 



 É r † < Êà º– Ð ³ ð‰ & ³ # Œ Fig. 7\    ? /% 3  . “  „  À Ó 5

A ü < 10 A\ " f Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ 35

C s 

(5)

Fig. 7. The optimum laser diode operating temperature for 808 nm center wavelength LD output.



© œ{ 9  M : 808 nm_   © œ`  ¦ µ 1 ϔ  r v  9 1 l x  Œ • “ : r • ¸\    É r

¨ î

ç  H  © œ„  s Ö  ¦ 0.31 nm/

C\  ¦ s 6   x # Œ Õ ª ° ú כ`  ¦ > í ß –

½

+ É Ã º e ”  . s  > í ß –\  s 6   x ) a à ºd ”  T

opt

  H Y Us $   s š ¸

×

¼_  “  „  À Ó\    É r þ j& h  1 l x  Œ •“ : r • ¸\  ¦   ? / 9, Fig.

7`  ¦ s 6   x # Œ ½ ¨ô  Ç   õ   6 £ § õ  ° ú  s  ½ ¨ # Œ& ’  .

T

opt

= −0.77C

A

+ 52.47 (1) s

 d ” \ " f C

A

  H “  „  À Ó\  ¦    · p . à ºd ”  (1)`  ¦ s 6   x

# Œ > í ß –ô  Ç   õ  “  „  À Ó 5 A\ " f  H 50.5

C, “  „   À

Ó 10 A\ " f  H 43.7

C _  ° ú כ`  ¦ ”   . “  „  À Ó 15 A\ 

"

f Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ ¢ ¸ô  Ç z  ´+ « >° ú כÜ ¼– Ð > í ß –

# Œ    · p ° ú כs  9 40

C& ñ • ¸\ " f 808 nm_   © œ`  ¦ µ 1 Ï

”

 r †   . y Œ • “  „  À Ó 20 A, 30 A, 36 A, 40 A\ " f  H 35

C, 30

C, 25

C, 22

C \  K { © œ   H Y Us $   s š ¸× ¼_  1

l

x  Œ • “ : r • ¸ ° ú כ`  ¦ t  9 s M : 808 nm_   © œ`  ¦ µ 1 ϔ  r †  



.

3. # bM ° Ë Ñ8 ý X ê s; c  Â \ ¥ Nd:YAG 7 _T $ [8 ý û s ÚI í Ä

— ¤V R Ë

Y

Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸ü < “  „  À Ó\  ¦    or & 



s š ¸× ¼ # Œl  Û ¼& 7 ˜à Ô! 3 _  ×  æd ”   © œs  808 nm{ 9  M :ü <

808 nm   u  ´ M : (Fig. 8\ " f “ : r • ¸\  ¦ 25

C – Ð “ ¦& ñ ô  Ç

 â

Ä º)– Ð Nd:YAG   & ñ `  ¦ 7 á x # Œl  r (  `  ¦ M : z  ´] j 1064 nm Y Us $ _  Ø  ¦§ 4 `  ¦ y Œ • / B N”  l  U  ´s \        · p  כ s

 Fig. 8s  . # Œl " f 808 nm      â Ä º  H Y Us $ 



s š ¸× ¼_  “  „  À Ó\  › ' a > \ O s  1 l x  Œ •“ : r • ¸\  ¦ 25

C – Ð

“

¦& ñ ô  Ç  â Ä º\  ¦ ´ ú ˜   H  כ s  . s   â Ä º Y Us $   s š ¸

Fig. 8. The output power of the end-pumped Nd:YAG laser by pumping ‘808 nm’ center wavelength and ‘non- 808 nm (25

C)’ center wavelength LD emission.

×

¼_  µ 1 ϔ   Û ¼& 7 ˜à Ô! 3 “ É r { © œƒ  y  “  „  À Ó_  % ò † ¾ ÓÜ ¼– Ð ×  æ d ”

 µ 1 ϔ    © œs     >   ) a  . Fig. 8`  ¦ ˜ Ѐ   / B N”  l _  U  ´ s

    o\   © œ › ' a\ O s  ×  æd ”   © œs  808 nm“   # Œl  F g Ü ¼– Ð Nd:YAG   & ñ `  ¦ # Œl  % i `  ¦ M :_  Ø  ¦§ 4 s  é ß –í  H y  Y Us 

$

  s š ¸× ¼_  1 l x  Œ • “ : r • ¸\  ¦ 25

C – Ð “ ¦& ñ r †   G  1 l x  Œ •r 

&

 808 nm      © œÜ ¼– Ð # Œl  % i `  ¦ M :_  Ø  ¦§ 4 ˜ Ð  Z

 } >   š ¸  H  כ `  ¦ · ú ˜ à º e ”  . Nd:YAG Y Us $  / B N”  l  _

 U  ´s  U  ´# Q| 9 à º2 Ÿ ¤ Z  }“ É r { 9 § 4 Ø  ¦§ 4  (input power)\ " f Ø

 ¦§ 4 _  ° ú כs  Ô  ¦ î ß –& ñ K  t   H  כ `  ¦ · ú ˜ à º e ” % 3  . s   H Y U s

$ _  / B N”  % ò % i s  / B N”  l _  U  ´s  U  ´# Q| 9 à º2 Ÿ ¤ Ô  ¦ î ß –& ñ K

 t   H ‰ & ³ © œs   Nd:YAG   & ñ _  \ P œ í& h  ‰ & ³ © œ (thermal lensing effect) \  _ ô  Ç  כ Ü ¼– Ð Ò q ty Œ •  ) a  . „  ^ ‰& h Ü ¼– Ð Y U s

$   s š ¸× ¼_  1 l x  Œ • “ : r • ¸\  ¦ › ¸] X  # Œ 808 nm_   © œ Ü

¼– Ð Nd:YAG Y Us $ \  ¦ 7 á x # Œl ô  Ç  â Ä º\  1 l x{ 9 ô  Ç / B N”  l  U

 ´s \ " f  8 Z  }“ É r Y Us $  Ø  ¦§ 4 `  ¦ ˜ Ðe ” `  ¦ · ú ˜ à º e ”  .

Fig. 9  H Nd:YAG Y Us $ _  / B N”  l  U  ´s  50 mm{ 9  M

:_  Ø  ¦§ 4 `  ¦    · p  כ Ü ¼– Ð ×  æd ”   © œs  808 nm“   F g " é ¶ Ü

¼– Ð Nd:YAG   & ñ `  ¦ # Œl ô  Ç  â Ä º\  8 £ ¤& ñ ô  Ç ë  H) 3 Ø  ¦§ 4 s  2.3 W s  9 # Œl  F g " é ¶ _  ×  æd ”   © œs  808 nm  u  ´ M : 8 £ ¤

&

ñ ô  Ç ë  H) 3 Ø  ¦§ 4 “ É r Õ ª˜ Ð  1.3 W  H 3.6 W – Ð   z Œ ¤ . Y U s

$ _  Ø  ¦§ 4 “ É r Y Us $ _  / B N”  % ò % i s  î ß –& ñ ½ + É M : þ j@ / 0.5 W& ñ • ¸ s  è ß – .

Fig. 10“ É r / B N”  l _  U  ´s \    É r 1064 nm Nd:YAG Y U s

$  Ø  ¦§ 4 _     o\  ¦ ˜ Г    כ s  . { 9 § 4 Ø  ¦§ 4 s  9.1 W{ 9  M

: y Œ • / B N”  l  U  ´s \ " f_  Ø  ¦§ 4 `  ¦    · p  כ Ü ¼– Ð Y Us $ 



s š ¸× ¼_  ×  æd ”   © œs  808 nm“   # Œl  F g Ü ¼– Ð Nd:YAG

 

& ñ `  ¦ 7 á x # Œl ô  Ç  â Ä º 808 nm      © œÜ ¼– Ð # Œl  ô

 Ç  â Ä º˜ Ð  Y Us $ _  Ø  ¦§ 4 s  þ j@ / 0.2 W& ñ • ¸ Z  } >    6

Ÿ

§`  ¦ S X ‰ “  ½ + É Ã º e ”  .

(6)

Fig. 9. Comparison of the Nd:YAG laser output power dependence on the 808 nm centered LD emission and non-808 nm (25

C) centered LD emission.

Fig. 10. The output power of the end-pumped Nd:YAG laser by pumping ‘808 nm’ center wavelength and ‘non- 808 nm’ center wavelength at each cavity length with a 9.1 W input power.

IV. + s Ç Â ] Ø

z 

´+ « >  õ  Y Us $   s š ¸× ¼\  ¦ “  „  À Ó 5 A, 10 A, 20 A, 30 A, 36 A, Y Us $   s š ¸× ¼_  þ j@ /Ø  ¦§ 4 `  ¦ % 3 l  0 A ô

 Ç 40 A\ " f 1 l x  Œ • r  ×  æd ”   © œs  808 nm“   y n C`  ¦ µ 1 ϔ  r  v

  H Y Us $   s š ¸× ¼_  & h & ñ 1 l x  Œ • “ : r • ¸  H y Œ •y Œ • 50.5

C, 43.7

C, 35

C, 30

C, 25

C, 22

C – Ð “  „  À Ó\    

&

h

] X ô  Ç Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸      H  כ `  ¦ · ú ˜ Ã

º e ”  .   " f ] j Œ • \ " f כ ¹½ ¨   H 25

C \ " f_  { 9 ~ ½ Ó

&

h “   1 l x  Œ •“ É r & h ] X  t  · ú §Ü ¼ 9, Y Us $   s š ¸× ¼\  “  

K

Šҍ  H „  À Ó\     Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸\  ¦ › ¸ ] X

 # Œ ×  æd ”   © œs  808 nm“   y n C`  ¦ µ 1 ϔ  r v   H  כ s  ×  æ Ä

º ×  æ כ ¹† < Ê`  ¦ · ú ˜ à º e ” % 3  .

‘

: r ƒ  ½ ¨\  ¦ : Ÿ x K  “ ¦^ ‰ Y Us $ _  î ß –& ñ & h s “ ¦ & ñ S X ‰ ô  Ç ½ ¨ 1

l

x`  ¦ 0 AK " f  H Y Us $   s š ¸× ¼_  î ß –& ñ & h “   “ : r • ¸Ä »t ü <

&

h

] X ô  Ç „  À Ó_  Å Ò{ 9 s  B Ä º ×  æ כ ¹† < Ê`  ¦ S X ‰ “   % i  . ¢ ¸ô  Ç Y

Us $   s š ¸× ¼_  # Œl  ×  æd ”   © œs  Nd:YAG   & ñ \  þ j

@

/ô  Ç f  ¨ à º÷ &>  l  0 AK " f  H Y Us $   s š ¸× ¼_  # Œl 

 © œs  808 nm ÷ &• ¸2 Ÿ ¤ Y Us $   s š ¸× ¼_  1 l x  Œ • “ : r • ¸

\

 ¦ › ¸] X    H  כ s  Nd:YAG Y Us $ _  Ø  ¦§ 4 `  ¦ ´ òÖ  ¦& h Ü ¼– Ð



6   x ½ + É Ã º e ”   H ~ ½ ÓZ O e ” `  ¦ z  ´+ « >& h Ü ¼– Ð 7 £ x" î # Œ ˜ Ð% i  .

P

c p 8 ý ò k >

‘

: r ƒ  ½ ¨  H ô  Dz D G…  ;ë  Hƒ  ½ ¨" é ¶ _  2008¸  • ¸ { 9 ì ø ̓  ½ ¨ \ O  0

A„ à ̃  ½ ¨õ ] j_  t " é ¶ \  _  # Œ ƒ  ½ ¨ s À Ò# Q& ’ 6 £ §`  ¦ µ 1 ß y

 9 Õ ª t " é ¶ \  y Œ ™ × ¼ 2 ; .

Y

c p w Š à U Ø ”  ô

[1] T. Y. Fan and Antonio Sanchez, IEEE J. Quantum Electron. 26, 311 (1990).

[2] Y. F. Chen, T. S. Liao, C. F. Kao, T. M. Huang, K.

H. Lin and S. C. Wang, IEEE J. Quantum Electron.

32, 2010 (1996).

[3] D. L. Sipes, Appl. Phys. Lett. 47, 74 (1985).

[4] Josef Berger, David F. Welch, Don R. Scifres, William Streifer and Peter S. Cross, Appl. Phys.

Lett. 51, 1212 (1987).

[5] William Streifer, Donald R. Scifres, Gary L. Har- nagel, David F. Welch, Josef Berger and Masamichi Sakamoto, IEEE J. Quantum Electron. 24, 883 (1988).

[6] Walter Koechner, Solid-State Laser Engineering (Springer, Berlin Heidelberg, 1999), Chap. 6.

[7] Y. A. Tarakanov, D. S. IIyushenkov, V. M.

Chistyakov, M. A. Odnoblyudoy and S. A. Gure-

vich, J. Appl. Phys. 95, 1 (2004).

(7)

[8] L. Borruel, I. Esquivias, P. Moreno, M. Krakowski, S. C. Auzanneau, M. Calligaro, O. Parillaud, M.

Lecomte, S. Sujecki, J. Wykes and E. C. Larkins, Appl. Phys. Lett. 87, 101 (2005).

[9] Jacques I. Pankove, IEEE J. Quantum Electron. 4, 119 (1968).

[10] Masahiko Kondow, Takeshi Kitatani, Kouji Naka- hara and Toshiaki Tanaka, IEEE Photonics Technol.

Lett. 12, 777 (2000).

[11] Minoru Ito and Tatsuya Kimura, IEEE J. Quantum Electron. 17, 787 (1981).

[12] Donal M. Byrne and Brian A. Keating, IEEE Pho- tonics Technol. Lett. 1, 356 (1989).

[13] J. ´ OGorman, A. F. J. Levi, T. Tanbun-Ek, D. L.

Coblentz and R. A. Logan, Appl. Phys. Lett. 60, 1058 (1992).

[14] Jae-Ho Han and Sung-Woong Park, Appl. Phys. 7,

6 (2007).

(8)

Jong-Uk Park and Hyung-Chul Im

Korea Astronomy and Space Science Institute, Daejeon 305-764

Duk-Hyun Kim

Cultural Studies, Hanbat National University, Daejen 305-719 (Received 21 July 2008, in final form 19 September 2008)

The effects of laser-diode (LD) operating temperature and injection current on the LD emission spectra and the lasing threshold have been studied for effective pumping of a Nd:YAG laser. A red shift was observed in the center wavelength of the LD emission for increasing LD operating temperature and injection current. The average wavelength shift ratio was 0.31 nm/

C at each operating temperature, and 0.22 nm/A at each injection current. The LD injection-current-based adjustment of the LD operating temperature enabled us to control the 808 nm center wavelength of LD emission for efficient pumping of a Nd:YAG crystal. When the center wavelength of the LD emission was 808 nm, the output power of the end-pumped Nd:YAG laser was up to 0.5 W higher than that of the non-808-nm center wavelength emission. A 1.3-W lower threshold input power was found with a 808-nm centered LD pump spectrum compared with a non-808-nm pump spectrum.

Tailor-controlling the LD operating temperature for emission of an 808-nm centered LD spectrum proved to be not only an effective method for maximizing the LD’s output power but also a stable condition for operating a Nd:YAG laser.

PACS numbers: 42.55.Px, 42.55.Xi, 42.60.Lh

Keywords: Laser diode, Nd:YAG laser, End-pumping, LD emission spectra, Wavelength shift ratio

E-mail: [email protected]

수치

Fig. 1. The experimental setup for the measurement of the laser diode spectrum.
Fig. 2. The experimental setup for the measurement of output power of the Nd:YAG laser.
Fig. 5. Dependence of the laser diode spectra as a func- func-tion of injecfunc-tion current at 25 ◦ C operating temperature.
Fig. 7. The optimum laser diode operating temperature for 808 nm center wavelength LD output.
+2

참조

관련 문서

and an improvement set of extragradient-type iteration methods in [5], we in- troduce new iteration algorithms for finding a common of the solution set of an equilibrium problem

A substance as germanium or silicon whose electrical conductivity is intermediate between that of a metal (like copper) and an insulator (like rubber); More importan t of

일반세제를 사용하면 거품이 많이 발생되어 감전, 고장 및 화재의 원인이 됩니다.. 칼 등 날카로운 기구는 손잡이가 위를

 äM EEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEEE F s  Ċ äM ¾Œ 

Although this energy can be released in the form of an emitted photon (X-ray fluorescence), the energy can also be transferred to another electron, which is ejected from

We study the relationship between Independent variables such as the V/T(Vibration Time), V/T movement, expansion height, curing time, placing temperature, Rising and C/S ratio

자동차용 GFRP( Gl as s Fi be rRe i nf or c ed Pl as t i c )복합재료로 실용화되어 폭 넓게 이용되고 있는 복합판재는 모재( Mat r i x) 를 플라스틱, 강화재 ( Rei nf or ce

XAFS: X-ray absorption fine structure XES: X-ray emission spectroscopy XRF: X-ray fluorescence.. Use of x-rays; a probe based