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Upconversion Properties of Y 2 O 3 :Er 3+ , Yb 3+ Nanophosphors with Different Yb 3+ Concentrations

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Upconversion Properties of Y 2 O 3 :Er 3+ , Yb 3+ Nanophosphors with Different Yb 3+ Concentrations

Hyeon Mi Noh · Ju Hyun Oh · Jung Hyun Jeong

Department of Physics, Pukyong National University, Busan 608-737, Korea

Ha Ri Kang · Won Jong Kim · Chae Hyun Lee · Yong Rok Choi · Yong Dae Park

Haeundae High School, Busan 612-818, Korea

Jun Kyu Jang

Department of Ophthalmic Optics, Kaya University, Gimhae 621-748, Korea (Received 29 April 2015 : revised 1 June 2015 : accepted 1 June 2015)

Y

2

O

3

nanophosphors co-doped with 0.01 mol Er

3+

and various concentrations of Yb

3+

were synthesized by using the high-energy ball-milling method, and their upconversion properties were studied. The crystallinities and the surface morphologies of the nanophosphors that were investi- gated by using X-ray diffraction and scanning electron microscopy, respectively, and upconversion luminescence spectra were obtained by using a 975 nm laser diode (LD). According to the X- ray diffraction results, as the Yb

3+

concentration was increased, the crystallinity of the powder improved, and the powder tended to show a more cubic structure. The emission spectra of the Y

2

O

3

:Er

3+

, Yb

3+

nanophosphors showed green, red and blue UC emissions at 550, 660 and 410 nm, which could be assigned to the

2

H

11/2

,

4

S

3/2

5

I

15/2

,

4

F

9/2

5

I

15/2

and

4

G

11/2

5

I

15/2

of Er

3+

transitions, respectively. Also, their upconversion processes were explained by measuring the pump-power dependency of the upconversion luminescence spectra.

PACS numbers: 78.55.-m, 78.55.Hx, 78.66.Bf

Keywords: Upconversion, Y

2

O

3

:Er

3+

/Yb

3+

, Nanophosphors, Energy transfer

Yb 3+  Ò Þy ¢  ì Å× D; c   \ ¥ Y 2 O 3 :Er 3+ , Yb 3+  x ¢] k ù° Ë Ñ= k8 ý V ê sU ê s ¹ Åò & ÿ ] k ù° Ë Ñ— ¤V R Ë

{

¡g ` @Q  ·  ¡® £g ` @ · + ä ^ ï Bg ` @

Â

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

~ ç

¡ P  · ™ » 4 w Hø ¶ B · T = g ` @ · L | ÷ 7 B ó i ; · ƒ ‘ š ÷ 7 B6 0

K

î  r @ /“ ¦1 p x † < Ɠ §,  Òí ß – 612-818

† ç

¡+ Ö <¦ 

 @ /† < Ɠ § î ß – â F g † < Æõ , ^ ” K  621-748

(2015¸   4 Z 4 29{ 9  ~ à Î6 £ §, 2015¸   6 Z 4 1{ 9  à º& ñ ‘ : r ~ à Î6 £ §, 2015¸   6 Z 4 1{ 9  > F  S X ‰& ñ )

Er

3+

_  0 l x • ¸\  ¦ 0.01 mol – Ð “ ¦& ñ “ ¦ Yb

3+

0 l x • ¸\  ¦    or †   Y

2

O

3

:Er

3+

, Yb

3+

 ” ¸+ þ AF g ^ ‰\  ¦ “ ¦

\

 -t  ^  ¦ x 9 a A ~ ½ ÓZ O `  ¦ s 6   x # Œ ½ + Ë$ í “ ¦  © œ~ ½ ӄ  ¨ 8 Š + þ AF g: £ ¤$ í `  ¦ ƒ  ½ ¨ % i  . X-‚    r] X z  ´+ « >, Å Ò „  

This is an Open Access article distributed under the terms of the Creative Commons Attribution Non-Commercial License

(http://creativecommons.org/licenses/by-nc/3.0) which permits unrestricted non-commercial use, distribution, and reproduction in

any medium, provided the original work is properly cited.

(2)



‰ & ³p  â `  ¦ s 6   x # Œ ½ + Ë$ í  ) a ì  r ´ ú ˜_    & ñ $ í x 9 ³ ð€  + þ A © œ`  ¦ › ' a ¹ 1 Ï “ ¦, 975 nm Y Us $   s š ¸× ¼– Ð # Œ l

 # Œ  © œ~ ½ ӄ  ¨ 8 Š + þ AF g`  ¦ % 3 % 3  . X-‚    r] X 8 £ ¤& ñ `  ¦ : Ÿ x K  ½ + Ë$ í  ) a  ” ¸+ þ AF g ^ ‰  H { 9 ~ ½ Ó& ñ >  (cubic) ½ ¨› ¸ e ”

`  ¦ S X ‰ “   % i “ ¦, Yb

3+

_  0 l x • ¸ 7 £ x † < Ê\     ì  r ´ ú ˜_    & ñ $ í s  † ¾ Ó © œ H † d`  ¦ · ú ˜ à º e ” % 3  . 975 nm– Ð

#

Œl  # Œ % 3 “ É r Y

2

O

3

:Er

3+

, Yb

3+

 ” ¸+ þ AF g ^ ‰_  µ 1 Ï F g Û ¼& 7 ˜à Ô! 3 “ É r Yb

3+

_  0 l x • ¸ 7 £ x † < Ê\     550 nm Â Ò   H _  y © œô  Ç 0 l qÒ  o + þ AF g õ  660 nm_  & h Ò  o + þ AF g, Õ ªo “ ¦ €  •ô  Ç 410 nm_  ' õ AÒ  o + þ AF g`  ¦ ˜ Ð% i Ü ¼ 9 s 



 H y Œ •y Œ • Er

3+

s “ : r _ 

2

H

11/2

,

4

S

3/2

5

I

15/2

,

4

F

9/2

5

I

15/2

Õ ªo “ ¦

4

G

11/2

5

I

15/2

„  s \  l “  ô  Ç



. ¢ ¸ô  Ç  © œ~ ½ ӄ  ¨ 8 Š+ þ AF g _  õ & ñ `  ¦ + þ AF g Û ¼& 7 ˜à Ô! 3 õ  * 3 á Ô F g _ ” > r • ¸\  ¦ 8 £ ¤& ñ # Œ [ O " î % i  .

PACS numbers: 78.55.-m, 78.55.Hx, 78.66.Bf

Keywords:  © œ~ ½ ӄ  ¨ 8 Š+ þ AF g, Y

2

O

3

:Er

3+

/Yb

3+

,  ” ¸+ þ AF g ^ ‰, \  -t  „  ² ú ˜

I. " e  ] Ø

s

“ : r s   { Œ • © œI \ " f F g \  -t \  ¦ f  ¨ à º # Œ  r   { Œ •



© œI – Ð [  t  t  „  \  ¢ ¸   É r F g \  -t \  ¦ f  ¨ à º # Œ Z  }

“ É

r \  -t   © œI – Ð „  s    H õ & ñ `  ¦  © œ~ ½ ӄ  ¨ 8 Š (upconver- sion) õ & ñ s  “ ¦ ô  Ç .   H& h ü @‚  % ò % i _  µ 1 ϔ    © œ`  ¦ ° ú 



 H Y Us $   s š ¸× ¼\  ¦  Bž ÐÀ Ó " é ¶ ™ è ' ‘   ) a   & ñ s   Ä

»o \   e# Œ r  F g‚   % ò % i _  + þ AF g`  ¦ ~ ½ ÓØ  ¦   H  © œ~ ½ ӄ  

¨ 8

Š + þ AF g \  @ /ô  Ç ƒ  ½ ¨  H  € ª œ >  s À Ò# Q4 R M ® o Ü ¼ 9 [1–3], ( 

 Qn Û ¼e  ¦ Y Us , F g 7 £ x; Ÿ ¤  © œu , F g: Ÿ x’  , Ò q tÓ ü t _ † < Ɣ  é ß –, I 

€

ª œ„  t _  ´ òÖ  ¦ † ¾ Ó © œ 1 p x \  ´ ú §“ É r 6 £ x6   x 0 p x$ í `  ¦ t “ ¦ e ” 



 [4–6]. Õ ªo “ ¦  Bž ÐÀ Ó s “ : r`  ¦ ' ‘ ô  Ç   & ñ s   Ä »o \ 

"

f { 9 # Q   H  © œ~ ½ ӄ  ¨ 8 Š ‰ & ³ © œ“ É r & h ü @‚   8 £ ¤& ñ  © œu ,  © œ~ ½ ӄ  

¨ 8

Š Y Us $ ü < _ « Ñ6   x ”  é ß – © œu  1 p x _   € ª œô  Ç 6 £ x6   x 0 p x$ í

`

 ¦ t “ ¦ e ” # Q" f Ë ¨ï  r ô  Ç ƒ  ½ ¨ s À Ò# Q4 R M ® o  .

Er 3+ s “ : r“ É r  ü @‚  Ü ¼– РÒ'  r  F g‚  , & h ü @‚   % ò % i 

\

 s Ø Ôl  t  ´ ú §“ É r \  -t  ï  r 0 A\  ¦ t “ ¦ e ” “ ¦, / B N" î

<

ʓ É r ï  r / B N" î › ¸| `  ¦ ë ß –7 á ¤ r v   H ï  r 0 A_  Š © œ[ þ t s  e ” # Q" f



€ ª œô  Ç \  -t  „  ² ú ˜õ & ñ õ   © œ~ ½ ӄ  ¨ 8 Š + þ AF g s  { 9 # Q± ú ˜ à º e ”

  H › ¸| `  ¦ ° ú Æ ғ ¦ e ”  . ¢ ¸ô  Ç Yb 3+ s “ : r“ É r \  -t  ï  r 0

A é ß – ¿ º > h– Ð l $  © œI “   2 F 7/2 ï  r 0 Aü < # Œl  © œI “  

2 F 5/2 ï  r 0 Aë ß – t “ ¦ e ” # Q % 3 ! s sà Ô s “ : r Ü ¼– Ð ´ ú §s   6   x

÷

& 9,   É r  Bž ÐÀ Ó " é ¶ ™ èü < † < Êa  ' ‘  # Œ  € ª œô  Ç ƒ  ½ ¨

s

À Ò# Q4 R M ® o  . Yb 3+ s “ : r _  [ þ t›  H  © œI ü <  { Œ • © œI _  \ 



-t  s \  @ /6 £ x   H \  -t  ï  r 0 A\  ¦ ”   Eu 3+ , Tb 3+ , Er 3+ , Pr 3+ , Tm 3+ s “ : r 1 p x s  Yb 3+ s “ : r õ  † < Êa  ' ‘ ÷ &



 H s “ : r[ þ t s  9, s [ þ t  s \  { 9 # Q   H \  -t „  ² ú ˜– Ð “   ô

 Ç + þ AF g : £ ¤$ í ƒ  ½ ¨ ´ ú §s  s À Ò# Qt “ ¦ e ” “ ¦ [7–11], þ j   H

\

  H  © œ~ ½ ӄ  ¨ 8 Š ´ òÖ  ¦`  ¦ Z  } s l  0 A # Œ ± ú “ É r Ÿ í 7 H \  -t 

\

 ¦ t   H Ó ü t| 9 \ " f upconversion : £ ¤$ í s  ƒ  ½ ¨  ) a   e ” 



 [12–14]. Õ ª ×  æ Y 2 O 3   H q “ §& h  ± ú “ É r þ j@ / F g † < Æ Ÿ í 7 H \ 



-t  (597 cm −1 )\  ¦ t “ ¦ e ” “ ¦, Ó ü t o & h s    o† < Æ& h Ü ¼

E-mail: [email protected]

–

Ð î ß –& ñ  9 1 l q$ í s  \ O   H Ó ü t| 9 – Ð   ñÛ ¼à Ԗ Ð" f & h ½ + Ëô  Ç Ó ü t

| 9

s  .

{ 9

ì ø Í& h Ü ¼– Ð  © œ~ ½ ӄ  ¨ 8 Š + þ AF g“ É r @ / Òì  r # Œl  © œI f  ¨ à º (excited state absorption, ESA) õ & ñ õ    H] X ô  Ç s “ : r  s 

\

 { 9 # Q   H \  -t „  ² ú ˜  © œ~ ½ ӄ  ¨ 8 Š (energy transfer up- conversion, ETU) õ & ñ Ü ¼– Ð µ 1 ÏÒ q t “ ¦, # Œl  F g õ   Ö ¸$ í ^ ‰ s

“ : r _  0 l x • ¸ Õ ªo “ ¦ — ¸^ ‰_  $ í | 9 \  % ò † ¾ Ó`  ¦ ~ à ΍  H  .  Bž Ð À

Ó s “ : r“ É r   & ñ  © œ_  % ò † ¾ Ó`  ¦  Œ •>  ~ à Ît ë ß –, ï  r / B N" î › ¸| \  Â

Ò½ + Ë   H ï  r 0 A Š © œ  s _  \  -t  s  €  •ç ß –ë ß – ² ú ˜ t 



8 • ¸ ETU    o 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 { 9 # Q± ú ˜ à º e ”

 .   " f — ¸^ ‰_  7 á x À Ó\     Er 3+ s “ : r _   © œ~ ½ ӄ  

¨ 8

Š+ þ AF g _  [ jl  ´ ú §s  ² ú ˜ ”   . ¢ ¸ô  Ç „   -Ÿ í 7 H  © œ  ñ Œ • 6

 

x Ü ¼– Ð Ã ºÑ þ ˜ cm −1 \  -t  s     H ï  r 0 A[ þ t  s \   H



×  æ Ÿ í 7 H q ~ ½ Ó õ & ñ s  { 9 # Qè ß – . s  Qô  Ç כ ¹“  [ þ t õ  † < Ê a

 # Œl   © œ, power density, Ô  ¦í  HÓ ü t 0 l x • ¸, # Œl  © œI \ " f Er 3+ _  + þ AF g à º" î 1 p x _  ´ ú §“ É r כ ¹“  [ þ t s  Er 3+ s “ : r s  ' ‘ 

 )

a Z O ß ¼  & ñ [15–17] x 9  ” ¸  & ñ [18, 19]\ " f  © œ~ ½ ӄ  ¨ 8 Š + þ

AF g _   € ª œô  Ç B j m 7 £ § \  % ò † ¾ Ó`  ¦ p • 2 ; .

‘

: r ƒ  ½ ¨\ " f  H “ ¦\  -t  ^  ¦ x 9 a A ~ ½ ÓZ O Ü ¼– Ð 0.01 mol_  Er 3+ s “ : r õ  0 l x • ¸\  ¦    or †   Yb 3+ s “ : r s  4 Ÿ ¤ ½ + Ë' ‘   ) a Y 2 O 3  ” ¸+ þ AF g ^ ‰\  ¦ ½ + Ë$ í “ ¦ 975 nm Y Us $   s š ¸× ¼

–

Ð # Œl  # Œ  © œ~ ½ ӄ  ¨ 8 Š + þ AF g: £ ¤$ í `  ¦ › ¸  % i  . + þ AF g ^ ‰ _

   & ñ ½ ¨› ¸ü < { 9  _    & ñ $ í `  ¦ › ¸  l  0 A # Œ X-‚  



r] X  z  ´+ « >`  ¦ s 6   x % i “ ¦, { 9  _  + þ A © œõ  ç  H{ 9 $ í `  ¦ › ¸ 

l  0 AK  ³ ð€   p [ j½ ¨› ¸\  ¦ ì  r$ 3  % i  . ¢ ¸ô  Ç s  + þ AF g ^ ‰

\

 @ /ô  Ç  © œ~ ½ ӄ  ¨ 8 Š + þ AF g Û ¼& 7 ˜à Ô! 3 `  ¦ 8 £ ¤& ñ “ ¦, * 3 á Ô F g [ j l

\  @ /ô  Ç  © œ~ ½ ӄ  ¨ 8 Š + þ AF g [ jl     o\  ¦ 8 £ ¤& ñ # Œ  © œ~ ½ ӄ  

¨ 8

Š + þ AF g _  B j& m 7 £ §`  ¦ ƒ  ½ ¨ % i  .

II. ÷ m Ç] M ö U ê s0 n É

Er 3+ s “ : r _  0 l x • ¸  H 0.01 mol – Ð “ ¦& ñ “ ¦ Yb 3+ s 

“

: r _  0 l x • ¸\  ¦  € ª œ >     or †   Y 2 O 3  ” ¸+ þ AF g ^ ‰\  ¦

(3)

Fig. 1. (Color online) XRD patterns of Y 2 O 3 :Er 3+ , Yb 3+

nanophosphors with various sintering temperatures.

“

¦\  -t  ^  ¦ x 9 a A ~ ½ ÓZ O Ü ¼– Ð ½ + Ë$ í % i  . Ø  ¦ µ 1 ÏÓ ü t| 9 – Ѝ  H Y 2 O 3 (99.9%, Aldrich), Er 2 O 3 (99.99%, Aldrich), Yb 2 O 3

(99.99%, Aldrich)\  ¦ s 6   x % i “ ¦ — ¸Ž  H r « Ñ\  ¦  o† < ƀ ª œ : r Ü

¼– Ð > í ß – % i  .  o† < ƀ ª œ : r Ü ¼– Ð > | ¾ Ó  ) a Ø  ¦ µ 1 ÏÓ ü t| 9 `  ¦ ^  ¦ x 9

a A (ball milling)`  ¦ l 0 AK  e  ¦  Û ¼h Ë : ˜ ÐÖ  ¦ (bowl) \  ï

 r q ô  Ç r « Ñü < 10 mm ß ¼l _  ZrO ^  ¦`  ¦ ° ú  s  V , # Q €  • 350 rpm _   r„  5 Å q • ¸– Ð 50ì  r 1 l x î ß – ™ D ¥ ½ + Ëô  Ç Ê ê 10ì  r 1 l x î ß –

@

/l  r ç ß –`  ¦ ° ú   H  כ `  ¦ 10  r ì ø Í4 Ÿ ¤ # Œ ™ D ¥ ½ + Ë·ì  r  W # Œ ï  r q

 % i “ ¦, Õ ª Ê ê 1100 C _  “ : r • ¸\ " f 4r ç ß – 1 l x î ß – \ P % ƒo 

% i  .



” ¸+ þ AF g ^ ‰_    & ñ ½ ¨› ¸ ì  r$ 3 `  ¦ 0 AK  X-‚    r] X  (X- ray diffraction, XRD, Philips, X’Pert)`  ¦ 8 £ ¤& ñ % i Ü ¼ 9, X-‚  _  í ß –ê ø Íy Œ • (2Θ)“ É r 10 ∼ 70 % ò % i \ " f ì  r { © œ 0.02 _  Û

¼ ± p5 Å q • ¸– Ð 8 £ ¤& ñ % i  . Õ ªo “ ¦ Field Emission Scanning Electron Microscopy (FE-SEM, JSM-6700F, JEOL)`  ¦ s  6

 

x # Œ r « Ñ_  ³ ð€  ½ ¨› ¸ x 9 + þ A © œ`  ¦ ì  r$ 3  % i  .  © œ~ ½ ӄ  

¨ 8

Š + þ AF g`  ¦ 8 £ ¤& ñ l  0 AK  þ j@ / F gØ  ¦§ 4  1 W“   975 nm Y U s

$   s š ¸× ¼\  ¦ # Œl  F g Ü ¼– Ð  6   x % i Ü ¼ 9 + þ AF g ’    ñ  H é

ß –Ò  oF g  © œu \  ¦ : Ÿ x õ r &  F g„    7 £ x C l – Ð  Ž Ø  ¦ % i  .

III. ÷ m Ç] M ö+ s ÇÊ Ý õ m Í w в  o

Fig. 1“ É r “ ¦\  -t  ^  ¦ x 9 a A ~ ½ ÓZ O Ü ¼– Ð ½ + Ë$ í ô  Ç Y 2 O 3 :Er 3+ , Yb 3+  ” ¸+ þ AF g ^ ‰_  ½ + Ë$ í “ : r • ¸\    É r X-‚  



r] X  © œs  . 8 £ ¤& ñ  ) a X-‚    r] X  © œ“ É r ½ + Ë$ í “ : r • ¸ 7 £ x † < Ê

\

      É r Ô  ¦í  HÓ ü t x ß ¼ \ O s  { 9 ~ ½ Ó& ñ >  (cubic) ½ ¨› ¸

–

Ð — ¸¿ º ° ú  “ É r   õ \  ¦ ˜ Ð# ŒÅ ғ ¦ e ” “ ¦, s \  ¦ JCPDS 

×

¼ (88-1040)   õ ü < ¸ ú ˜ { 9 u † < Ê`  ¦ S X ‰ “   % i  . Õ ªo “ ¦ ½ + Ë

$ í

“ : r • ¸ 7 £ x ½ + Éà º2 Ÿ ¤  r] X  x ß ¼_  [ jl  7 £ x  “ ¦ Å Ò

Fig. 2. FE-SEM images of Y 2 O 3 :Er 3+ , Yb 3+ nanophos- phors sintered at (a) 800, (b) 900, (c) 1000 and (d) 1100

◦ C.

Fig. 3. FE-SEM images of Y 2 O 3 :Er 3+ , Yb 3+ nanophos- phors at (a) 0 mol and (b) 0.05 mol Yb 3+ sintered at 1100 C.

x

ß ¼_  ì ø Íu ; Ÿ ¤ (full with at half maximum, FWHM)“ É r Yb 3+ _  0 l x • ¸ 0\ " f 0.07 mol– Ð 7 £ x † < Ê\     0.226\ 

"

f 0.180Ü ¼– Ð y Œ ™™ è # Œ   & ñ $ í s  † ¾ Ó © œ÷ &% 3 6 £ §`  ¦ · ú ˜ à º e ” 



.

Fig. 2  H \ P % ƒo  “ : r • ¸ (a) 800, (b) 900, (c) 1000 Õ ªo 

“

¦ (d) 1100 C{ 9  M :_  FE-SEM  ”  s  . \ P % ƒo  “ : r • ¸

7

£

x ½ + Éà º2 Ÿ ¤ { 9  [ þ t _  ß ¼l  & t “ ¦  8¹ ¡ ¤ ç  H{ 9  >  + þ A

$ í

÷ &# Q { 9  [ þ t _  ì ø Í6 £ x s   Ö ¸ µ 1 Ïy  { 9 # Qz Œ ¤6 £ §`  ¦ · ú ˜ à º e ”  .

 

& ñ { 9  [ þ t s  & f ” Ü ¼– Ð" f Õ ªY U“  [ þ t _   â > x 9 • ¸  H ×  ¦ # Q [

þ

t >  ÷ &# Q + þ AF g _  ’ < Hz  ´s  ×  ¦ # Q[ þ t  כ e ” `  ¦ \ V © œ½ + É Ã º e ”  .

{ 9

 [ þ t s  ç  H{ 9  >  ì  r Ÿ í÷ &# Q e ”   H 1100 C \ " f Yb 3+ _  0

l

x • ¸\    É r FE-SEM  ”  `  ¦ Fig. 3 \    ? /% 3  . Yb 3+

s

“ : r`  ¦ ' ‘  t  · ú §€ Œ ¤`  ¦ M :  H  • 2 ; ³ ð€  _  { 9  [ þ t s  é

#

Qo – Ð Ó ü æ 5 ge ”   H — ¸_ þ v`  ¦ ˜ Ð% i “ ¦ 0.05 mol Yb 3+ s “ : r _ 

 â

Ä º €  • 90 nm_  ½ ¨+ þ A\   î  r  ” ¸ ß ¼l _  { 9  [ þ t s  “ ¦ Ø

Ô>  ì  r Ÿ í “ ¦ e ” 6 £ §`  ¦ S X ‰ “   % i  . Yb 3+ _  † < Ê| ¾ Ós  0.05 mol“   ì  r ´ ú ˜_   â Ä º { 9  [ þ t s   8¹ ¡ ¤ ç  H{ 9  >  ÷ &“ ¦ { 9   [

þ

t _  ì ø Í6 £ x s   Ö ¸ µ 1 Ïy  { 9 # Qz Œ ¤6 £ §`  ¦ · ú ˜ à º e ”  .

0.01 mol Er 3+ s “ : r õ  0 l x • ¸\  ¦ ² ú ˜o ô  Ç Yb 3+ s “ : r`  ¦ † < Ê a

 4 Ÿ ¤ ½ + Ë' ‘ ô  Ç Y 2 O 3 :Er 3+ , Yb 3+  ” ¸+ þ AF g ^ ‰_  Yb 3+ 0 l x

(4)

Fig. 4. (Color online) (a) Upconversion emission spectra of Y 2 O 3 :Er 3+ , Yb 3+ and (b) comparing the upconver- sion emission intensity with different Yb 3+ concentra- tions under 975 nm excitation.

•

¸\    É r  © œ~ ½ ӄ  ¨ 8 Š + þ AF g Û ¼& 7 ˜à Ô! 3 `  ¦ Fig. 4(a) \    ? /

%

3  . 550 nm Â Ò   H _  y © œô  Ç 0 l qÒ  o + þ AF g ( 2 H 11/2 , 4 S 3/25 I 15/2 ) õ  660 nm Â Ò   H _  & h Ò  o + þ AF g ( 4 F 9/2 → 5 I 15/2 ), Õ ª o

“ ¦ 410 nm Â Ò   H _  €  •ô  Ç ' õ AÒ  o + þ AF g ( 4 G 11/25 I 15/2 ) s 

› '

a ¹ 1 Ï÷ &% 3  . Yb 3+ 0 l x • ¸ 7 £ x † < Ê\     + þ AF g _  [ jl 

7

£

x    0.05 mol s  © œs  ÷ &€   0 l x • ¸™ è F g (concentra- tion quanching) ‰ & ³ © œÜ ¼– Ð  r  y Œ ™™ è   H — ¸_ þ v`  ¦ ˜ Ð% i 



. Yb 3+ s “ : r _  0 l x • ¸_     o\    É r + þ AF g [ jl     o\  ¦ Fig. 4(b) \  Õ ªA á Ԗ Ð   ? /% 3  .

Fig. 5  H Y 2 O 3 :Er 3+ , Yb 3+  ” ¸+ þ AF g ^ ‰_   © œ~ ½ ӄ  ¨ 8 Š + þ

AF g _  õ & ñ `  ¦ [ O " î l  0 Aô  Ç \  -t  ï  r 0 A³ ðs  . 975 nm _  # Œl  F g“ É r Er 3+ s “ : r _  4 I 15/2 \ " f 4 I 11/2 ï  r 0 A– Ð_ 

„

 s ü < Yb 3+ s “ : r _  2 F 7/2 \  2 F 5/2 ï  r 0 A– Ð_  „  s \  K  {

© œ  ) a  . Er 3+ \  q K  Yb 3+ s “ : r _  f  ¨ à º &  # Œl  F g _

 \  -t   H @ / Òì  r Yb 3+ s “ : r \ " f f  ¨ à º÷ &“ ¦ Er 3+ s “ : r

“

É r Yb 3+ \ " f Er 3+ s “ : r Ü ¼– Ð_  \  -t  „  ² ú ˜õ & ñ \  _ K 

#

Œl   ) a  . 0 l qÒ  o + þ AF g“ É r Er 3+ s “ : r \ " f_  # Œl ï  r 0 Af  ¨ à º õ

& ñ (ESA : 4 I 15/24 I 11/24 F 7/2 ) õ  \  -t  „  ² ú ˜



© œ~ ½ ӄ  ¨ 8 Š õ & ñ (ETU : 2 F 5/2 → 2 F 7/2 (Yb 3+ ): 4 I 11/2 → 4

Fig. 5. (Color online) Energy level diagram of Er 3+ and Yb 3+ ions under 975 nm excitation.

F 7/2 (Er 3+ )) \  _ K  µ 1 ÏÒ q t  9, & h Ò  o + þ AF g“ É r 0 l qÒ  oï  r 0 A“  

2 H 11/2 < ʓ É r 4 S 3/2 ï  r 0 A\ " f 4 F 9/2 – Ð q ~ ½ Ó „  s  # Œ µ 1 Ï Ò q

tô  Ç . s M : — ¸^ ‰ r « Ñ t   H Ÿ í 7 H \  -t _  ß ¼l 

q

~ ½ Ó „  s Ö  ¦`  ¦   & ñ   H  © œ ×  æ כ ¹ô  Ç כ ¹“  s   ) a  . { 9  ì

ø Í& h Ü ¼– Ð  Bž ÐÀ ÓF K5 Å q \ " f { 9 # Q   H q ~ ½ Ó „  s  S X ‰Ò  ¦“ É r

\

 -t  Ì “ s Z O g Ë :`  ¦ ë ß –7 á ¤ ô  Ç . — ¸^ ‰_  þ j@ / F g † < Æ Ÿ í 7 H \  - t

\  @ /ô  Ç “  ] X ô  Ç ï  r 0 A s _  \  -t  s  4C  s  © œs 

÷

&€   q ~ ½ Ó „  s  { 9 # Q± ú ˜ S X ‰Ò  ¦“ É r B Ä º  Œ • . Y 2 O 3 _  þ

j@ / F g † < Æ Ÿ í 7 H \  -t   H 597 cm −1 s “ ¦, 4 S 3/2 ü < 4 F 9/2 ï  r 0

A ç ß – \  -t   H €  • 3140 cm −1 s Ù ¼– Ð \  -t  s  €  • 5.3 s  .   " f q ~ ½ Ó „  s  õ & ñ Ü ¼– Ð 4 F 9/2 ï  r 0 A G  0

>| 9  S X ‰Ò  ¦“ É r B Ä º ± ú   & h Ò  o + þ AF g“ É r   É r B j m 7 £ §`  ¦ : Ÿ x K

      H  כ `  ¦ \ V © œ½ + É Ã º e ”  . Yb 3+ s “ : r _  0 l x • ¸

 & t €   2 H 11/24 I 15/2 : 4 I 9/24 I 13/2 _  “ § s 

¢ -

a (cross relaxation, CR) õ & ñ Ü ¼– Ð 4 I 13/2 ï  r 0 A G 0 >| 9  Ã

º e ” “ ¦ 4 I 13/2 ï  r 0 A_  „   [ þ t s  Yb 3+ s “ : r Ü ¼– РÒ'  \ 



-t \  ¦ „  ² ú ˜~ à Î  4 I 13/2 → 4 F 9/2 _  ETU õ & ñ s  { 9 # Q



 & h Ò  o + þ AF g s     >   ) a  . ¢ ¸ô  Ç 0 l qÒ  o + þ AF g _  [ jl 

 & 4 R 4 F 9/2 ï  r 0 A_  „   x 9 • ¸ Z  }  t €   Yb 3+ s “ : r \ 

"

f_  \  -t „  ² ú ˜õ & ñ ( 4 F 9/24 G 11/24 I 15/2 ) \  _  K

 4 F 9/2 ï  r 0 A\ " f 4 G 11/2 ï  r 0 A– Ð # Œl  0 p x K t “ ¦ ' õ A Ò 

o + þ AF g s    ± ú ˜ à º e ”  .

s

 Qô  Ç  © œ~ ½ ӄ  ¨ 8 Š + þ AF g _  B j m 7 £ §`  ¦ [ O " î l  0 AK 

*

3 á Ô F g [ jl \      © œ~ ½ ӄ  ¨ 8 Š + þ AF g [ jl _  _ ” > r • ¸\  ¦ 8 £ ¤

&

ñ % i  . { 9 ì ø Í& h Ü ¼– Ð * 3 á Ô F g _  [ jl  (P ) Õ ªo  ß ¼t 

· ú

§`  ¦ M : + þ AF g _  [ jl   H P n \  q Y V “ ¦ n“ É r + þ AF g \  › ' 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 ”  . Fig. 6“ É r

0.01 mol Er 3+ s “ : r õ  0.05 mol Yb 3+ s “ : r s  4 Ÿ ¤ ½ + Ë' ‘   ) a

(5)

Fig. 6. (Color online) Pump power dependence of green, red and blue upconversion emission.

Ó

ü t| 9 \ " f { 9   F g [ jl \    É r  © œ~ ½ ӄ  ¨ 8 Š + þ AF g _  [ jl \  ¦ log-log Õ ªA á Ԗ Ð    · p  כ s  . 0 l qÒ  o + þ AF g _  l Ö  ¦ l   H 1.903 Ü ¼– Ð 2\   î  r ° ú כ`  ¦ ˜ Ð% i “ ¦ s   H 0 l qÒ  o + þ AF g s  ¿ º

>

h_  # Œl  F g   › ' a # Œô  Ç { 9 ì ø Í& h “    © œ~ ½ ӄ  ¨ 8 Š + þ AF g “   s  F g



 õ & ñ (two-photon process)\  _ ô  Ç  כ e ” `  ¦    · p  כ s

 . & h Ò  o + þ AF g _   â Ä º l Ö  ¦ l  1.585– Ð { 9 F g   õ & ñ (one-photon process) Ü ¼– Ð      H X < s   H “ § s  ¢ - a‰ & ³



© œÜ ¼– Ð 4 I 13/2 ï  r 0 A_  x 9 • ¸ Ÿ í o÷ &# Q & h Ò  o+ þ AF g _  l Ö  ¦ l

 1\   0 >t l  M :ë  H s  . s  Qô  Ç   õ   H · ú ¡" f \  - t

 ï  r 0 A³ ð\ " f [ O " î ô  Ç  © œ~ ½ ӄ  ¨ 8 Š + þ AF g B j m 7 £ § õ  ¸ ú ˜ { 9  u

† < Ê`  ¦ · ú ˜ à º e ”  . ¢ ¸ô  Ç ' õ AÒ  o + þ AF g _  l Ö  ¦ l   H 2.603 Ü ¼

–

Ð 4 F 9/24 G 11/24 I 15/2 „  s \    É r  Œ ™ F g   õ & ñ (three-photon process) Ü ¼– Ð   z Œ ¤ .

IV. + s Ç Â ] Ø

‘

: r ƒ  ½ ¨\ " f  H “ ¦\  -t  ^  ¦ x 9 a A ~ ½ ÓZ O `  ¦ s 6   x # Œ Y 2 O 3 :Er 3+ , Yb 3+  ” ¸+ þ AF g ^ ‰\  ¦ ½ + Ë$ í “ ¦  © œ~ ½ ӄ  ¨ 8 Š + þ A F

g: £ ¤$ í `  ¦ ƒ  ½ ¨ % i  . XRD 8 £ ¤& ñ   õ   ” ¸ + þ AF g ^ ‰  H

Yb 3+ _  0 l x • ¸ 7 £ x ü < › ' a > \ O s  { 9 ~ ½ Ó& ñ >  (cubic) ½ ¨› ¸– Ð



 z Œ ¤“ ¦ Yb 3+ _  0 l x • ¸ 7 £ x ½ + Éà º2 Ÿ ¤ Å Ò x ß ¼_  [ jl 

&

t “ ¦ ì ø Íu ; Ÿ ¤ s  ×  ¦ # Q[ þ t # Q ì  r ´ ú ˜_    & ñ $ í s  † ¾ Ó © œ H † d`  ¦ · ú ˜ Ã

º e ” % 3  . 975nm Y Us $   s š ¸× ¼– Ð # Œl  # Œ 550 nm Â

Ò   H _  y © œô  Ç 0 l qÒ  o + þ AF g ( 2 H 11/2 , 4 S 3/25 I 15/2 ) õ  660 nm Â Ò   H _  & h Ò  o + þ AF g ( 4 F 9/25 I 15/2 ), Õ ªo “ ¦ 410 nm Â

Ò   H _  €  •ô  Ç ' õ AÒ  o + þ AF g ( 4 G 11/25 I 15/2 ) s  › ' a ¹ 1 Ï÷ &% 3  .

Yb 3+ s “ : r _  0 l x • ¸ 7 £ x † < Ê\     0 l qÒ  o + þ AF g“ É r Er 3+ s 

“

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

&

ñ ( 2 F 5/22 F 7/2 (Yb 3+ ): 4 I 11/24 F 7/2 (Er 3+ )) \  l 

“

   9 & h Ò  o + þ AF g“ É r 2 H 11/24 I 15/2 : 4 I 9/24 I 13/2 _  CR \  _ ô  Ç ETU õ & ñ , Õ ªo “ ¦ ' õ AÒ  o + þ AF g“ É r 4 G 11/25 I 15/2 „  s \  l “  ô  Ç . s  © œ_     : r“ É r * 3 á Ô F g _ ” > r • ¸\  ¦ :

£ ¤& ñ ô  Ç   õ \ " f• ¸ S X ‰ “   % i   H X < 0 l qÒ  o + þ AF g“ É r l Ö  ¦ l 

1.903“   s  F g   õ & ñ s  9 & h Ò  o + þ AF g“ É r l Ö  ¦ l  1.585“   { 9

F g   õ & ñ , Õ ªo “ ¦ ' õ AÒ  o + þ AF g“ É r l Ö  ¦ l  2.603“    Œ ™ F

g   õ & ñ Ü ¼– Ð [ O " î ½ + É Ã º e ”  .

P

c p 8 ý ò k >

‘

: r ƒ  ½ ¨  H  Ò â @ /† < Ɠ §ü < K î  r @ /“ ¦1 p x † < Ɠ §_  R&E á Ԗ Ð Õ

ªÏ þ › t " é ¶ Ü ¼– Ð s À Ò# Q& ’ _ þ v m  . Y 2 O 3 :Er 3+ , Yb 3+  ” ¸ + þ

AF g ^ ‰  H  Ò â @ /† < Ɠ § + þ AF g ™ èF “ É r' Ÿ _  ™ èF t " é ¶  \ O `  ¦ :

Ÿ

x K  à º' Ÿ ÷ &% 3 _ þ v m  .

REFERENCES

[1] F. Tong, W. P. Risk, R. M. Macfarlane and W.

Lenth, Electron. Lett. 25, 1391 (1989).

[2] R. Brede, E. Heumann, J. Kortke, T. Danger and G. Huber, Appl. Phys. Lett. 63, 1727 (1990).

[3] A. Silversmith, J. Lumin. 60, 636 (1994).

[4] A. Patra, S. Szha, M. Rakov and G. Naciel, Chem.

Phys. Lett. 407, 477 (2005).

[5] S. Heer, M. Wermuth, K. Kaamaer, D. Ehrentraut and H. Gudel, J. Lumin. 94, 337 (2001).

[6] N. J. Ekins-Daukes, K. Ballard, C. D. J. Calder, K.

W. J. Barnjanm and G. Hill et al., Appl. Phys. Lett.

82, 1974 (2003).

[7] D. C. Hanna, R. M. Percival, I. R. Perry, R. G.

Smart and J. E. Townsend et al., Opt. Commun.

78, 187 (1990).

[8] Y-M. Hua, Q. Li, Y-L. Chen and Y-X. Chen, Opt.

Commun. 88, 441 (1992).

(6)

[9] A. S. Oliveira, M. T. de Araujo, A. S. Gouveia-Neto, J. A. Medeiros Neto and A. S. B. Sombra et al., Appl. Phys. Lett. 72, 753 (1998).

[10] D. M. Baney, G. Rankin and K. W. Chang, Appl.

Phys. Lett. 69, 1662 (1996).

[11] T. R. Gosnell, Electron. Lett. 33, 411 (1997).

[12] R. Balda, A. J. Garcia-adeva, M. Voda and J.

Rern´ andez, Phys. Rev. B 69, 205203 (2004).

[13] A. M. Tkachuk, S. E. Ivanova, M.-F. Joubert, Y.Guyot and L. Il Lsaenko et al., J. Lumin. 125, 271 (2007).

[14] A. J. Garcia-Adeva, R. Balda, J. Fern´ andez, Ei Ei Nyein and U. H˝ ommerich, Phys. Rev. B 72, 165116 (2005).

[15] J. Wang and D. J. Simkin, Phys. Rev. B 52, 3309 (1995).

[16] H. Xu and Z. Jiang, Chem. Phys. 155, 287 (2003).

[17] S. Georgescu, O. Toma, C. Florea and C. Naud, J.

Lumin. 87, 101 (2003).

[18] F. Vetrone, J. C. Boyer, J. A. Capobianco, A. Spegh- ini and M. Bettinelli, J. Phys. Chem. B 106, 5622 (2002).

[19] J. A. Capobianco, F. Vetrone, J. C. Boyer, A. Spegh-

ini and M. Bettinelli, J. Phys. Chem. B 106, 1181

(2002).

참조

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