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 4 Z 4, pp. 373∼378

Er 3+ Ê Ý Yb 3+ T Æ X Øù p § Y 8 È” X ¢ ZrO 2  x ¢] k ù° Ë Ñ= k8 ý Upconversion ] k ù° Ë Ñ — ¤V R ˎ ì ŏ Œ

) ç

„ ‘ ž  ™ ¸ · ™ »( å V  œ · L |A j* å  · ™ »^ ï BZ 9 

1 l

x _ @ /† < Ɠ § Ó ü t o † < Æõ ,  Òí ß – 614-714

{

¡g ` @Q  · ' Ö <( å M  · + ä ^ ï Bg ` @

Â

Ò â @ /† < Ɠ § Ó ü t o † < Æõ ,  Òí ß – 608-737

(2011¸   2 Z 4 16{ 9  ~ à Î6 £ §, 2011¸   2 Z 4 28{ 9  à º& ñ ‘ : r ~ à Î6 £ §, 2011¸   3 Z 4 27{ 9  > F  S X ‰& ñ )

3 mol% _  Er

3+

ü < x mol% (x = 0, 5, 10, 15) _  Yb

3+

s “ : r`  ¦ ' ‘ ô  Ç ZrO

2

 ” ¸+ þ AF g ^ ‰\  ¦ à º\ P ½ + Ë$ í Z O

Ü ¼– Ð ½ + Ë$ í # Œ Yb

3+

s “ : r s  upconversion(UC) + þ AF g \  p u   H % ò † ¾ Ó`  ¦ › ¸  % i  . SEM(scanning electron microscopy)  ”  õ  X-‚    r] X  © œ`  ¦ ì  r$ 3  # Œ ZrO

2

:Er

3+

,Yb

3+

 ” ¸ + þ AF g ^ ‰  H ½ ¨+ þ As  9 & ñ

~

½ Ó+ þ A_    & ñ ½ ¨› ¸\  ¦ s À ғ ¦ e ” 6 £ §`  ¦ S X ‰ “   % i  . 1 W, 975 nm & h ü @‚   Y Us $   s š ¸× ¼– Ð # Œl  # Œ y

© œô  Ç 0 l qÒ  oõ  & h Ò  o_  UC + þ AF g`  ¦ 8 £ ¤& ñ % i Ü ¼ 9 Yb

3+

s “ : r _  0 l x • ¸\  ¦ 7 £ x r ( ” \     0 l qÒ  o + þ AF g \  q  K

  © œ@ /& h Ü ¼– Ð & h Ò  o + þ AF g _  [ jl  ß ¼>  7 £ x ÷ &% 3  . 0 l qÒ  oõ  & h Ò  o UC + þ AF g _  * 3 á Ô F g [ jl  _ ” > r`  ¦ 8 £ ¤

&

ñ # Œ q “ §ô  Ç   õ  Yb

3+

s “ : r _  ' ‘ – Ð “  ô  Ç Er

3+

s “ : r s  ~ ½ ÓØ  ¦   H & h Ò  o UC + þ AF g _  7 £ x   H   H] X ô  Ç Er

3+

ü < Yb

3+

s “ : r  s \  µ 1 ÏÒ q tô  Ç energy back transfer(

4

S

3/2

(Er

3+

) +

2

F

7/2

(Yb

3+

) →

4

I

13/2

(Er

3+

) +

2

F

5/2

(Yb

3+

)) õ & ñ \  l “   “ ¦ e ” 6 £ §`  ¦ S X ‰ “   % i  .

Ù þ

˜d ” # Q: t Ø Ô ïm  , upconversion, + þ AF g,  ” ¸+ þ AF g ^ ‰, # Q Ó% 3 

Upconversion Photoluminescence in ZrO 2 :Er 3+ ,Yb 3+ Nanophosphors

Samsik Sung · Byoung Kuk Kim · Haeyoung Choi · Jung Hwan Kim

Department of Physics, Dongeui University, Busan 614-714

Hyeon Mi Noh · Byung Ki Moon · Jung Hyun Jeong

Department Physics, Pukyong National University, Busan 608-737 (Received 16 February 2011 : revised 28 February 2011 : accepted 27 March 2011)

Upconversion photoluminescence (UCPL) is investigated in ZrO

2

:Er

3+

, Yb

3+

nanophosphors at different Yb

3+

concentrations. The nanophosphors were synthesized by using the solvothermal method. The lattice structure for the tetragonal phase and the spherical shape of the nanophosphors were confirmed by using X-ray diffraction and scanning electron microscopy, respectively. The red UCPL under an excitation of 975 nm increased significantly with increasing Yb

3+

concentration at room temperature. The pump-power dependence of the green and the red UCPL leads us to conclude that the red UCPL is enhanced by the energy back-transfer between Er

3+

and Yb

3+

ions (

4

S

3/2

(Er

3+

) +

2

F

7/2

(Yb

3+

) →

4

I

13/2

(Er

3+

) +

2

F

5/2

(Yb

3+

)).

PACS numbers: 78.51.-m

Keywords: ZrO

2

, Upconversion, Luminescence, Er

3+

, Yb

3+

, Nanophosphor

E-mail: [email protected] -373-

(2)

I. " e  ] Ø



 H& h ü @‚  % ò % i _  µ 1 ϔ    © œ`  ¦ ° ú   H Y Us $   s š ¸× ¼\  ¦ Er 3+ s “ : r s  ' ‘   ) a Ó ü t| 9 \  q Æ Ò# Q 0 l qÒ  o x 9 & h Ò  o_  + þ AF g

`

 ¦ ~ ½ ÓØ  ¦   H upconversion photoluminescence(UCPL) \ 

@

/ô  Ç ƒ  ½ ¨  € ª œ >  s À Ò# Q4 R M ® o   [1–3]. Er 3+ s “ : r“ É r



€ ª œô  Ç \  -t ï  r 0 A\  ¦ t  9 s [ þ t ï  r 0 A ×  æ \   H / B N" î ¢ ¸



 H ï  r / B N" î › ¸| \   ҽ + Ë   H ï  r 0 A_  Š © œ[ þ t s  e ” “ ¦, s  Q ô

 Ç Š © œ  s \  energy transfer upconversion(ETU) õ & ñ s  { 9

# Qè ß – . ï  r / B N" î › ¸| \   ҽ + Ë   H ï  r 0 A Š © œ  s _  \  - t

 s  €  •ç ß –ë ß – ² ú ˜ t  8 • ¸ ETU_     o  H ß ¼>  { 9 

#

Q  9, „   -Ÿ í 7 H  © œ  ñ Œ •6   x Ü ¼– Ð ETU\  ‚ à Ð# Œ   H ï  r 0 A _

 à º" î \     o Ò q t|   .   " f — ¸^ ‰_  7 á x À Ó\    " f Er 3+ s “ : r _  & h Ò  o x 9 0 l qÒ  o UCPL_   1 l x s  ² ú ˜ ”   . s 



Qô  Ç UC õ & ñ _  B j& m 7 £ §“ É r * 3 á Ô F g [ jl \  @ /ô  Ç UCPL _

    o\  ¦ 8 £ ¤& ñ † < ÊÜ ¼– Ð+ ‹ [ O " î ½ + É Ã º e ”  .

UCPL“ É r UC laser, 3D display, upconversion F g$ 3 Ä »

‰

&

³p  â x 9 I € ª œ„  t _  ´ òÖ  ¦7 £ x  ƒ  ½ ¨ 1 p x \  6 £ x6   x ÷ &“ ¦ e ” 



 [4–6]. z  ´o – B H I € ª œ„  t \ " f  6   x 0 p x ô  Ç I € ª œÛ ¼& 7 ˜à Ô

! 3

% ò % i “ É r 400 ∼ 1100 nm & ñ • ¸s  9 s ˜ Ð  |   & h ü @‚  % ò

%

i \  y n C“ É r ™ èz  ´ ) a  . I € ª œ„  t  ³ ð€  \  UC Ó ü t| 9 `  ¦ & h 8 £ x Ü

¼– Ð { 9 ) €" f & h ü @‚  % ò % i _  y n C`  ¦ r  F g‚  % ò % i Ü ¼– Ð   ¨ 8 Š r

v €   I € ª œ„  t _  ´ òÖ  ¦`  ¦ † ¾ Ó © œr ~  ´ à º e ”  . Õ ªo “ ¦ Ò q t

^

‰F « э  H l œ íƒ  ½ ¨ü < 6 £ x6   xƒ  ½ ¨_  ¿ º › ' a& h \ " f F « Ñõ † < Æ _

  © œ B § 4 & h “   ƒ  ½ ¨ ì  r   ×  æ  – Ð+ ‹, þ j   H ƒ  ½ ¨   õ

\   Ø Ô€   Ò q t^ ‰ì  r   ? /\  Å Ò{ 9  ) a ZrO 2 :Er 3+  ” ¸ì  r ´ ú ˜

\

" f upconversion + þ AF g`  ¦  Ž Ø  ¦ † < ÊÜ ¼– Ð+ ‹ D h– Ðî  r ƒ  ½ ¨\ 

@

/ô  Ç  Œ ™F § 4 `  ¦ S X ‰ “  ô  Ç   e ”   [7–10]. UCPL`  ¦ _ † < Æ6   x Ü

¼– Ð  6   x ½ + É  â Ä º & h ü @‚  `  ¦  6   x l  M :ë  H \   © œ@ /& h Ü ¼

–

Ð \  -t  Z  }“ É r ~ ½ Ó ‚  s   X-‚  \  q K  “  ^ ‰  H W =  ’ < H



© œ`  ¦ ~ à ΍  H s & h s  e ”  .

þ

j   H s ü < ° ú  “ É r  € ª œô  Ç ì  r  _  6 £ x6   x`  ¦ 0 A # Œ Er`  ¦ ' ‘ 

ô  Ç í ß – oÓ ü t  ” ¸+ þ AF g ^ ‰\  @ /ô  Ç ƒ  ½ ¨  € ª œ >  ”  ' Ÿ 

÷

&# Q M ® o Ü ¼  [11–13] l ” > r \  ƒ  ½ ¨÷ &# Q“ : r Ô  ¦  oÓ ü t upcon- version Ó ü t| 9 \  q K  F g † < Ɵ í 7 H \  -t  Z  }   # Œl ï  r 0 A_  Ã

º" î `  ¦  ú ª t >  Ù ¼– Ð upconversion\  & h 6   x l \   

™

è Ô  ¦ o ô  Ç › ¸| [ þ t`  ¦ t “ ¦ e ”  . t Ø Ô ïm  (ZrO 2 )  H



© œ@ /& h Ü ¼– Ð ± ú “ É r þ j@ / F g † < Ɵ í 7 H \  -t (∼470 cm −1 )\  ¦  t

“ ¦ e ” # Q" f Z  }“ É r upconversion   ¨ 8 Š ´ òÖ  ¦`  ¦ l @ /½ + É Ã º e ” 



 [14, 15]. Õ ªo “ ¦ 2680 C s  © œ_  Z  }“ É r Ö 6 x& h `  ¦ t  9

\ P

 Ø  æ  $ † ½ Ó$ í õ  ? / o† < Æ$ í s  Ä ºÃ º # Œ ? / o F « Ñ  ½ ¨

›

¸F « Ñ ÷  r  m   ± ú “ É r F g „    ’ < Hz  ´, Z  }“ É r Ï ã J] X Ò  ¦ 1 p x F g

†

< Æ F « і Е ¸  H › ' a d ” `  ¦ — ¸Ü ¼“ ¦ e ”   H Ó ü t| 9 s   [16].

‘

: r ƒ  ½ ¨\ " f  H t Ø Ô ïm  \  F g  Ö ¸$ í ^ ‰– Ð Er 3+ s “ : r _  0

l

x • ¸\  ¦ 3 mol% – Ð “ ¦& ñ r v “ ¦, F gf  ¨ à º´ òÖ  ¦`  ¦ † ¾ Ó © œr v  l

 0 AK  Yb 3+ s “ : r _  0 l x • ¸(0, 5, 10, 15 mol%)\  ¦  Ø Ô>  '

‘  # Œ à º\ P ½ + Ë$ í Z O Ü ¼– Ð ½ + Ë$ í % i  . s  r « Ñ[ þ t \  @ /ô  Ç UCPL Û ¼& 7 ˜à Ô! 3 `  ¦ 8 £ ¤& ñ “ ¦, * 3 á Ô F g [ jl \  @ /ô  Ç UCPL [

jl _     o\  ¦ 8 £ ¤& ñ # Œ & h Ò  o x 9 0 l qÒ  o upconversion + þ A F

g _  B j& m 7 £ §`  ¦ › ¸  % i  .

II. ÷ m Ç ] M ö



” ¸ ì  r ´ ú ˜“ É r @ /^ ‰– Ð _ þ vd ” ~ ½ ÓZ O Ü ¼– Ð ] j› ¸÷ & 9, @ /³ ð& h “   _

þ vd ” ~ ½ ÓZ O \   H / B Ng Ë >Z O  [17], a % ¦ 0 qZ O  [18], ƒ  ™ èZ O  [19], à º

\ P

½ + Ë$ í Z O  [20]1 p x s  e ”  . s  ×  æ \ " f à º\ P ½ + Ë$ í Z O “ É r ± ú “ É r

“

: r • ¸\ " f ½ + Ë$ í s  0 p x “ ¦ { 9  \  ¦ ç  H| 9  >  ë ß –[ þ t à º e ” 



 H  © œ& h `  ¦ t “ ¦ e ”  . ‘ : r z  ´+ « >\ " f  H ZrOý \  Er 3+ s 

“

: r õ  Yb 3+ s “ : r`  ¦ ' ‘ ô  Ç + þ AF g ^ ‰\  ¦ à º\ P ½ + Ë$ í Z O Ü ¼– Ð ½ + Ë

$ í

% i  . Er 3+ s “ : r 0 l x • ¸\  ¦ 3 mol% – Ð “ ¦& ñ “ ¦ Yb 3+ s 

“

: r 0 l x • ¸\  ¦ 0, 5, 10, 15 mol% – Ð ² ú ˜o ô  Ç r « Ñ[ þ t`  ¦ ] j› ¸  l

 0 AK " f  6 £ § õ  ° ú  “ É r õ & ñ `  ¦  ' ¬ I . — ¸^ ‰\  ¦ ½ ¨$ í   H

„

 ½ ¨^ ‰– Ð zirconium propoxide [Zr(OH), 99 % Aldrich]\  ¦



6   x % i “ ¦,  Ö ¸$ í ^ ‰\  ¦ ½ ¨$ í   H „  ½ ¨^ ‰– Ѝ  H erbium ni- trate pentahydrate [(Er(NO 3 ) 3 5H 2 O, 99.99 % Aldrich] ü <

ytterbium nitrate pentahydrate [Yb(NO 3 ) 3 5H 2 O, 99.99

% Aldrich]\  ¦  6   x % i  .  Ö ¸$ í ^ ‰\  ¦ d  ¦ À Ò ' p 25 ml\  6   x K

r & " f 6 f$ Ü ¼€  " f 3r ç ß –1 l x î ß – ¸ ú ˜ ™ D ¥ ½ + Ër (  “ ¦ # Œl \ 

—

¸^ ‰ zirconium propoxide [Zr(OH), 99 % Aldrich]\  ¦ ™ D ¥

½

+ Ë # Œ 24r ç ß – 1 l x î ß – 6 f$ Ü ¼€  " f ¸ ú ˜ ™ D ¥ ½ + Ër (   . s  6   x Ó 

o`  ¦ autoclaveV , “ ¦ 250 C  t  …  ;…  ;y  “ : r • ¸\  ¦  © œ5 p x r 

† 

 Ê ê 72 r ç ß – 1 l x î ß – Ä »t  r (   . g Ë >„   ì ø Í6 £ x s  { 9 # Q €   autoclave \ " f 50 C\  ¦ Ä »t  €  " f | › ¸r (   .



” ¸+ þ AF g ^ ‰_  ½ ¨› ¸\  ¦ S X ‰ “   l  0 AK  X‚    r] X 



© œ(XRD, X’Pert-MPD diffraction system, Philips)`  ¦ 8 £ ¤

&

ñ % i Ü ¼ 9, Field Emission Scanning Electron Micro- scope(FESEM, JSM-6700F, JEP) – Ð  ” ¸ + þ AF g ^ ‰_  — ¸

€

ª œõ  ß ¼l \  ¦ S X ‰ “   % i  . XRD 8 £ ¤& ñ   õ   H JCPDS 

×

¼ü < q “ § # Œ Yb 3+ 0 l x • ¸    o\    É r ½ ¨› ¸_     o\  ¦ ì  r

$

3  % i  . Õ ªo “ ¦ PL 8 £ ¤& ñ `  ¦ 0 AK  [ þ t> p u F g " é ¶ Ü ¼– Ð 975 nm Y Us $   s š ¸× ¼\  ¦  6   x % i “ ¦, r « Ñ\ " f µ 1 ÏÒ q tô  Ç + þ A F

g`  ¦ monochromator(Spectra Pro-300, Acton Research Corporation) \  { 9   “ ¦, F g„    7 £ x C  › ' a \ " f  Ž Ø  ¦ ) a ’    

ñ  H n t _ O  š ¸z  ´– ÐÛ ¼ ïá Ԗ Ð 8 £ ¤& ñ % i  .

III. + s ÇÊ Ý õ m Í w в  o

Figure 1“ É r 1300 C \ " f ™ è  ô  Ç ZrO 2 :Er 3 mol%, Yb

x mol% + þ AF g ^ ‰(x = 0, 5, 10, 15)_  X-‚    r] X  © œs  .

(3)

Fig. 1. (Color online) X-ray diffraction patterns of ZrO 2 :Er 3+ , Yb 3+ nanophosphors for different Yb 3+ con- centration with a fixed Er 3+ concentration (3 mol%).

The samples were annealed at 1300 C. The diffraction peaks are indexed to the JCPDS card for pure tetragonal ZrO 2 crystal.

Fig. 2. SEM photography of ZrO 2 :Er 3+ (3 mol%), Yb 3+ (5 mol%) nanophosphors annealed at 1300 C.

s

  r] X  © œ“ É r JCPDS × ¼ (24-1164)ü < @ /^ ‰– Ð { 9 u  # Œ

&

ñ ~ ½ Ó& ñ >    & ñ ½ ¨› ¸\  ¦ t “ ¦ e ” 6 £ §`  ¦ · ú ˜ à º e ”  .  Bž ÐÀ Ó s

“ : r _  0 l x • ¸ Z  }“ É r r « э  H ¢ - a„  ô  Ç & ñ ~ ½ Ó& ñ >  ½ ¨› ¸\  ¦ s  À

ғ ¦ e ” Ü ¼ , ' ‘   ) a  Bž ÐÀ Ó s “ : r _  0 l x • ¸ ± ú Ü ¼€   (# Œ l

" f  H Er 3+ s “ : r ë ß – 3 mol% ' ‘   ) a r « Ñü < Er 3+ s “ : r 5 mol% ü < Yb 3+ s “ : r s  5 mol% ' ‘   ) a r « Ñ) { 9 Â Ò é ß – & ñ

>

   & ñ ½ ¨› ¸(JCPDS 37-1484)\  ¦ Ÿ í† < Ê “ ¦ e ” 6 £ §`  ¦ · ú ˜ à º e ”

 . Õ ªa Ë >\  ³ ðr  t  · ú §€ Œ ¤t ë ß – Er 3+ s “ : r ë ß – 3 mol% ' ‘ 

  ) a t Ø Ô ïm    ” ¸   & ñ “ É r as-grown  © œI \ " f { 9 ~ ½ Ó

½

¨› ¸\  ¦ s À ғ ¦ e ” % 3 Ü ¼ 9, 800 C s  _  ™ è  “ : r • ¸\ " f



 H & ñ ~ ½ Ó& ñ > \  ¦ s À ғ ¦, { 9  _  ß ¼l   H 12 ∼ 25 nm s % 3 



. ™ è  “ : r • ¸ Z  }  | 9 à º2 Ÿ ¤ { 9  â s  & t €  " f é ß – & ñ > 

Fig. 3. (Color online) Upconversion photoluminescence spectra of ZrO 2 :Er 3+ ,Yb 3+ with different concentration of Yb 3+ under the excitation of 975 nm laser diode.

Fig. 4. (Color online) Energy level diagram of Er 3+ and Yb 3+ ions. The upconversion processes(excitation, emis- sion, and energy transfer) under 975 nm excitation are indicated by arrows.

    l  r  Œ • % i  . { 9 ì ø Í& h Ü ¼– Ð Ô  ¦í  HÓ ü t s  ' ‘ ÷ &

t

 · ú §“ É r t Ø Ô ïm    ” ¸  & ñ “ É r 600 ∼ 800 C ™ è  “ : r

•

¸\ " f & ñ ~ ½ Ó& ñ > – РÒ'  é ß – & ñ > – Ð  © œ  s  { 9 # Qè ß – .

Õ

ª Q  MgO, Y 2 O 3 , CaO x 9  Bž ÐÀ ÓF K5 Å q s “ : r 1 p x s  ' ‘ 

€   & ñ ~ ½ Ó& ñ >   © œs  î ß –& ñ  o÷ &“ ¦, Ô  ¦í  HÓ ü t _  0 l x • ¸ 7 £ x 

½

+ Éà º2 Ÿ ¤ î ß –& ñ  o 8 ú ¤”  ÷ &# Q & ñ ~ ½ Ó& ñ > \ " f é ß – & ñ > – Ð „   s

   H  © œ  s “ : r • ¸ 7 £ x    H  כ Ü ¼– Ð · ú ˜ 94 R e ”   [21, 22]. Fig. 1 \ " f ˜ Ѝ  H  ü < ° ú  s   Bž ÐÀ Ó s “ : r _  † < Ê| ¾ Ós 

´ ú

§“ É r r « Ñ\ " f & ñ ~ ½ Ó& ñ >   © œs  î ß –& ñ  o÷ &# Q e ” 6 £ §`  ¦ S X ‰ “  

½

+ É Ã º e ”  .

(4)

Fig. 5. (Color online) Pump power dependence of the green and red upconversion luminescence of ZrO 2

:Er 3+ (3 mol%), Yb 3+ (x mol%) for x = 0 (a) and x = 10 (b).

1300 C \ " f ™ è  ô  Ç r « Ñ_  X‚    r] X  © œÜ ¼– РÒ'  ½ ¨ô  Ç þ

j@ / x ß ¼_   r] X y Œ • θü < ì ø Íu ; Ÿ ¤(full width at half maxi- mum) β x 9 X-‚    © œ λ\  ¦ Scherrer ~ ½ Ó& ñ d ” (D = β cos θ 0.89λ ) \ 

@

/{ 9  # Œ > í ß –ô  Ç   & ñ _  ß ¼l   H €  • 0.6 ∼ 0.9 µms % 3  .

Figure 2  H 1300 C \ " f ™ è  ô  Ç 3 mol% Er 3+ ü < 5 mol% Yb 3+ s “ : r`  ¦ ' ‘ ô  Ç r « Ñ_  SEM  ”  s  9, s 

 כ

Ü ¼– РÒ'  ½ ¨ô  Ç { 9  _  ß ¼l   H €  • 0.8 ∼ 1.2 µm s % 3 



. Õ ªa Ë >\ " f ˜ Ð1 p w s  + þ AF g ^ ‰– Ð+ ‹ þ j& h + þ AI “   ½ ¨+ þ A_  { 9 



[ þ t s  “ ¦À Ò ì  r Ÿ í “ ¦ e ” 6 £ §`  ¦ S X ‰ “  ½ + É Ã º e ”  .

Figure 3 \  975 nm Y Us $   s š ¸× ¼– Ð [ þ t ä ¼>  # Œ % 3 

“

É r ZrO 2 :Er 3+ ,Yb 3+ + þ AF g ^ ‰_  UCPL Û ¼& 7 ˜à Ô! 3 `  ¦   ? /

%

3  . Õ ªa Ë >\ " f 550 nm Â Ò   H \ " f Er 3+ s “ : r _  4 H 11/2 ,

4 S 3/24 I 15/2 „  s \  _ ô  Ç 0 l qÒ  o+ þ AF g õ  660 nm Â Ò   H \ 

"

f 4 F 9/24 I 15/2 „  s \  _ ô  Ç & h Ò  o+ þ AF g`  ¦ ^  ¦ à º e ”  .

Õ

ªo “ ¦ Yb 3+ _  0 l x • ¸ 7 £ x † < Ê\     + þ AF g _  „  ^ ‰ [ jl 



 H 7 £ x  “ ¦, Yb 3+ 0 l x • ¸ 10 mol%\  s Ø Ô€   0 l qÒ  o+ þ AF g

“ É

r ‰ & ³$ y  ×  ¦ # Q[ þ t “ ¦ Õ ª @ /’   & h Ò  o+ þ AF g s  ß ¼>  7 £ x † < Ê`  ¦

^

 ¦ à º e ”  .

Figure 4  H ZrO 2 :Er 3+ ,Yb 3+ _  upconversion õ & ñ `  ¦ [ O

" î l  0 Aô  Ç \  -t  ï  r 0 A³ ðs  . LD\ " f ~ ½ ÓØ  ¦   H 975 nm y n C_  \  -t   H Er 3+ s “ : r _  4 I 15/24 I 11/2 „   s

ü < Yb 3+ s “ : r _  2 F 7/22 F 5/2 „  s  \  -t ü <   _

 ° ú   . Er 3+ s “ : r ë ß – ' ‘   ) a r « Ñ\ " f ~ ½ ÓØ  ¦ ÷ &  H 0 l qÒ  o UCPL“ É r excited state absorption(ESA: 4 I 15/24 I 11/2

4 F 7/2 ) õ & ñ õ  ETU õ & ñ \ ( 4 I 11/24 I 15/2 : 4 I 11/2

4 F 7/2 ) l “  ô  Ç . ô  Ǽ # , Er 3+ ü < Yb 3+ s “ : r s  † < Êa  ' ‘ 

 )

a r « Ñ\ " f  H Yb 3+ s “ : r _  f  ¨ à ºé ß –€  & h s  Er 3+ \  q K 

 s

`›   ß ¼Ù ¼– Ð [ þ t> p uF g _  @ / Òì  r`  ¦ Yb 3+ s “ : r s  f  ¨ à º “ ¦ Er 3+ s “ : r Ü ¼– Ð \  -t \  ¦ „  ² ú ˜ô  Ç .   " f Yb 3+ _  0 l x • ¸

 & t €   + þ AF g _  [ jl   H & t >   ) a  . & h Ò  o+ þ AF g“ É r 0 l q Ò 

o+ þ AF gï  r 0 A“   2 H 11/2 < ʓ É r 4 S 3/2 ï  r 0 A\ " f & h Ò  o+ þ AF gï  r 0

A“   4 F 9/2 ï  r 0 A– Ð „  s ÷ &  H  ×  æ Ÿ í 7 H s  ¢ - a õ & ñ Ü ¼– Ð [ O " î

½

+ É Ã º e ” Ü ¼ , 4 S 3/2 ü < 4 F 9/2 ï  r 0 A  s _  \  -t  Ì “ ss  €  • 3,060 cm −1 – Ð ZrO 2 _  þ j@ / F g † < Ɵ í 7 H \  -t (470 cm −1 ) _  6 C  s  © œ ß ¼Ù ¼– Ð  ×  æ Ÿ í 7 H s  ¢ - a s  { 9 # Q± ú ˜ S X ‰Ò  ¦“ É r B Ä º

± ú

 . ë ß –{ 9  4 I 13/2 ï  r 0 A G 0 >4 R e ” Ü ¼€  , 975 nm Â Ò   H _

 [ þ t> p u F g " é ¶ s  Er 3+ s “ : r`  ¦ & h Ò  oµ 1 Ï F gï  r 0 A– Ð * 3 i ç ( 4 I 13/2

4 F 9/2 ) # Œ y © œô  Ç & h Ò  o+ þ AF g`  ¦ % 3 `  ¦ à º e ”  . Er 3+ s 

“

: r _  0 l x • ¸ 7 £ x  €   Er 3+ s “ : r ç ß –_   o   0 >

t

€  " f Er 3+ s “ : r  s \  { 9 # Q   H “ § s  ¢ - a õ & ñ (cross- relaxation: 4 F 7/24 I 9/2 : 4 I 15/24 I 13/2 ) s   Ö ¸$ í  o ÷ &

Ù

¼– Ð 4 I 13/2 ï  r 0 A_  x 9 • ¸\  ¦ Z  }{ 9  à º e ”  .   " f Er 3+ s 

“

: r _  0 l x • ¸ 7 £ x  €   & h Ò  o+ þ AF g s    l  r  Œ • “ ¦, s 



Qô  Ç ‰ & ³ © œ“ É r “ § s  ¢ - a õ & ñ \  l “  ô  Ç  כ Ü ¼– Ð ˜ Г ¦÷ &# Qe ” 



 [23]. Fig. 3\ " f Er 3+ s “ : r ë ß – 3 mol% ' ‘   ) a r « Ñ\ 

"

f & h Ò  o+ þ AF g s   _     t  · ú §  H  כ “ É r “ § s  ¢ - a õ & ñ s  { 9

# Q± ú ˜ ë ß –  p u s “ : r  s _   o  ¾ ú št  3 l w l  M :ë  H s 



. Er 3+ s “ : r _  0 l x • ¸\  ¦ 3 mol% – Ð “ ¦& ñ r v “ ¦, Yb 3+ s 

“

: r _  0 l x • ¸\  ¦ 8 £ § 7 £ x r v €   „  ^ ‰ + þ AF g _  [ jl  7 £ x 

½

+ É ÷  r  m   0 l qÒ  o+ þ AF g _  [ jl   H ×  ¦ # Q[ þ t€  " f & h Ò  o+ þ AF g s  ß

¼>    z Œ ™`  ¦ ^  ¦ à º e ”  . Yb 3+ s “ : r _  0 l x • ¸ 10 mol%

s

 © œs  ÷ &€   0 l qÒ  o+ þ AF g“ É r  _    t “ ¦ & h Ò  o+ þ AF g ë ß – z Œ ™



 H  . Y 2 O 3  ” ¸+ þ AF g ^ ‰\ " f { 9 # Qè ß – s ü < ° ú  “ É r ‰ & ³ © œ`  ¦ [ O

" î l  0 AK " f Song 1 p x“ É r Er 3+ \ " f Yb 3+ s “ : r Ü ¼– Ð % i 

\

 -t  „  ² ú ˜, 7 £ ¤ energy back transfer (EBT: 4 S 3/2 (Er 3+ ) + 2 F 7/2 (Yb 3+ ) → 4 I 13/2 (Er 3+ ) + 2 F 5/2 (Yb 3+ )) — ¸+ þ A`  ¦ ]

jr ô  Ç   e ”   [24].

EBT õ & ñ `  ¦ S X ‰ “   l  0 AK  * 3 á Ô F g [ jl \    É r UCPL _

 [ jl \  ¦ 8 £ ¤& ñ % i  . Fig. 5  H Er 3+ ë ß – ' ‘   ) a ZrO 2 ü <

Er 3+ ü < Yb 3+  ° ú  s  ' ‘   ) a ZrO 2  ” ¸+ þ AF g ^ ‰\  @ /ô  Ç * 3 

(5)

á

Ô F g [ jl \    É r 0 l qÒ  o x 9 & h Ò  o UCPL_  [ jl \  ¦ log-log Õ

ªA á Ԗ Ð    · p  כ s  . { 9 ì ø Í& h Ü ¼– Ð * 3 á Ô F g _  [ jl  P  B

Ä º ß ¼t  · ú §Ü ¼€   UCPL_  [ jl   H P n \  q Y Vô  Ç . # Œl 

"

f n“ É r UCPL \  › ' a # Œô  Ç # Œl  F g  _  > hà ºs  9 * 3 á Ô F g \ 

@

/ô  Ç + þ AF g [ jl _  log-log Õ ªA á Ô_  l Ö  ¦ l – РÒ'  ½ ¨½ + É Ã º e ”

 . Er 3+  3 mol% ' ‘   ) a ZrO 2  ” ¸+ þ AF g ^ ‰\ " f 8 £ ¤& ñ ô

 Ç 0 l qÒ  o+ þ AF g _  l Ö  ¦ l   H 1.6 s  9 & h Ò  o_  l Ö  ¦ l   H 2.1 s 

%

3  . Õ ªo “ ¦ 3 mol% Er 3+ ü < 10 mol% Yb 3+  ' ‘   ) a ZrO 2 \ " f 8 £ ¤& ñ ô  Ç 0 l qÒ  o+ þ AF g _   â Ä º l Ö  ¦ l  1.5– Ð Õ ª   



o  Œ •€ Œ ¤Ü ¼ , & h Ò  o+ þ AF g _  l Ö  ¦ l   H 1.3 Ü ¼– Ð ß ¼>  ×  ¦% 3 



. · ú ¡\ " f  7 H _ ô  Ç  ü < ° ú  s  Er 3+ s “ : r ë ß – ' ‘   ) a r « Ñ

\

" f ~ ½ ÓØ  ¦   H & h Ò  o UCPL“ É r — ¸^ ‰   & ñ _  F g † < Ɵ í 7 H \  - t

_  ß ¼l \  _ ” > r   H  ×  æ Ÿ í 7 H s  ¢ - a õ & ñ õ  Er 3+ s “ : r _  0

l

x • ¸\  _ ” > r   H “ § s  ¢ - a õ & ñ \  l “  ô  Ç .  ×  æ Ÿ í 7 H s 

¢ -

a õ & ñ “ É r s  F g  (two photon, n = 2)s “ ¦, “ § s  ¢ - a õ & ñ

“ É

r # Œl ï  r 0 A 4 I 13/2 _  Ÿ í o– Ð “   # Œ { 9 F g  (one photon, n = 1)f  ¨ à ºõ & ñ s Ù ¼– Ð Er 3+  3 mol% ' ‘   ) a ZrO 2  

”

¸+ þ AF g ^ ‰\ " f µ 1 ÏÒ q t   H & h Ò  o UCPL“ É r  ×  æ Ÿ í 7 H s  ¢ - a õ 

&

ñ s  t C & h e ” `  ¦ r  ô  Ç . Õ ªo “ ¦ Yb 3+ s “ : r s  † < Êa  ' ‘ 

  ) a r « Ñ\ " f EBT µ 1 ÏÒ q t €   4 I 13/2 ï  r 0 A_  x 9 • ¸ &  t

“ ¦, s  ï  r 0 A_  + þ AF g à º" î “ É r B Ä º U  ´# Q" f(€  • 3 ms) ô  Ç > h _

 [ þ t> p u F g  – Ð & h Ò  oï  r 0 A“   4 F 9/2 ï  r 0 A\  ¦ G Ö  ¦ à º e ”  .  



" f Yb 3+ s “ : r _  0 l x • ¸ 7 £ x ½ + Éà º2 Ÿ ¤ EBT õ & ñ s   Ö ¸ µ 1 Ï K

4 R 0 l qÒ  oï  r 0 A“   4 S 3/2 (Er 3+ ) x 9 • ¸  H ×  ¦ # Q[ þ t “ ¦ 4 I 13/2 ï  r 0

A_  x 9 • ¸ 7 £ x ÷ &# Q { 9 F g   õ & ñ \  _ ô  Ç & h Ò  o UCPL _

 [ jl  & t   H ‰ & ³ © œ`  ¦ [ O " î ½ + É Ã º e ”  .

IV. + s Ç Â ] Ø

Ã

º\ P ½ + Ë$ í Z O Ü ¼– Ð Ô  ¦í  HÓ ü t – Ð ' ‘ ô  Ç Er 3+ _  0 l x • ¸\  ¦ 3 mol% – Ð “ ¦& ñ r v “ ¦ Yb 3+ _  0 l x • ¸\  ¦ 0, 5, 10, 15 mol% – Ð

# Œ ZrO 2 :Er 3+ ,Yb 3+ + þ AF g ^ ‰\  ¦ ] j› ¸ % i  . 1300 C \ 

"

f ™ è  ô  Ç r « Ñ_  X‚    r] X  © œÜ ¼– РÒ'  ZrO 2 :Er 3+ ,Yb 3+

+ þ

AF g ^ ‰  H ' ‘  s “ : r _  0 l x • ¸ 7 £ x  ½ + Éà º2 Ÿ ¤ & ñ ~ ½ Ó& ñ > 

½

¨› ¸– Ð î ß –& ñ ÷ &“ ¦ 0 l x • ¸ ± ú `  ¦ M :  H é ß – & ñ >  { 9  Ò



 z Œ ¤ . 1 W, 975 nm Y Us $   s š ¸× ¼– Ð [ þ t> p u F g

"

é

¶ Ü ¼– Ð  6   x # Œ 550 nm Â Ò   H _  0 l qÒ  oõ  660 nm Â Ò   H _

 & h Ò  o UCPL`  ¦ › ' a ¹ 1 Ï % i  . Yb 3+ s “ : r 0 l x • ¸ 7 £ x

 €   0 l qÒ  o + þ AF g“ É r ×  ¦ # Q[ þ t “ ¦ & h Ò  o + þ AF g _  [ jl   H 7 £ x

 % i  . Er 3+  3 mol% ' ‘   ) a ZrO 2  ” ¸+ þ AF g ^ ‰\ 

"

f µ 1 ÏÒ q t   H & h Ò  o UCPL“ É r  ×  æ Ÿ í 7 H s  ¢ - a õ & ñ s  t C 

&

h s % 3 Ü ¼ 9, Yb 3+ s “ : r _  0 l x • ¸ 7 £ x ½ + Éà º2 Ÿ ¤ ETU õ 

&

ñ s ( 4 S 3/2 (Er 3+ ) + 2 F 7/2 (Yb 3+ ) → 4 I 13/2 (Er 3+ ) +

2 F 5/2 (Yb 3+ ))  Ö ¸ µ 1 ÏK 4 R" f 4 I 13/2 ï  r 0 A_  x 9 • ¸ 7 £ x ÷ &# Q { 9

F g   õ & ñ \  _ ô  Ç & h Ò  o UCPL_  [ jl  & & ’  .

P

c p 8 ý ò k >

s

  7 Hë  H“ É r 2010 † < Ƹ  • ¸ 1 l x _ @ /† < Ɠ § “ §? /ƒ  ½ ¨q \  _ K 

ƒ

 ½ ¨÷ &% 3 6 £ § (2010AA092).

Y

c p w Š à U Ø ”  ô

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수치

Fig. 3. (Color online) Upconversion photoluminescence spectra of ZrO 2 :Er 3+ ,Yb 3+ with different concentration of Yb 3+ under the excitation of 975 nm laser diode.
Fig. 5. (Color online) Pump power dependence of the green and red upconversion luminescence of ZrO 2

참조

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