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로드 중.... (전체 텍스트 보기)

전체 글

(1)

α-LiFeO

2

ì  r ´ ú ˜`  ¦ a % ¦ 0 qZ O `  ¦ s 6   x # Œ ] j› ¸ % i  .   & ñ † < Æ& h  x 9  l & h  $ í | 9 `  ¦ \ P ì  r$ 3  © œu , x-‚  



r] X ì  r$ 3 l , Å Ò „   ‰ & ³p  â , M¨ ossbauer ì  rF g l  x 9 ”  1 l x+ þ Ar « Ñ  oÖ  ¦8 £ ¤& ñ l \  ¦ s 6   x # Œ ƒ  ½ ¨ % i 



. α-LiFeO

2

é ß –{ 9  © œ“ É r 600

C \ " f 3r ç ß – 1 l x î ß – / B N l  ×  æ \ " f \ P % ƒo  # Œ % 3 `  ¦ à º e ” % 3 Ü ¼ 9, x-‚    r ] X

ì  r$ 3    õ  α-LiFeO

2

ì  r ´ ú ˜“ É r cubic ½ ¨› ¸\  ¦ & ’ Ü ¼ 9 s M :     © œÃ º a = 4.1610 ± 0.0005 ˚ A s % 3 



. M¨ossbauer Û ¼& 7 ˜à Ô! 3  ì  r$ 3   õ  α-LiFeO

2

_  Curie “ : r • ¸  H 90 ± 3 Ke ” `  ¦ · ú ˜ à º e ” % 3  .  © œ“ : r \ " f α-LiFeO

2

_  s $ í | 9 ^ ‰s 1 l x ° ú כ“ É r 0.24 mm/s ° ú כ`  ¦ & ’ Ü ¼ 9, s   H α-LiFeO

2

_  Fe s “ : r s  t   H s “ : r

  H Fe

3+

_  high spin  © œI e ” `  ¦ ˜ Ð# ŒÅ Ò% 3  . α-LiFeO

2

_  ¨ î ç  H œ íp [ j  l  © œ H

hf

(T )  H T /T

C

<0.7

% ò

% i \ " f [H

hf

(T ) − H

hf

(0)]/H

hf

(0) = −0.36(T /T

C

)

3/2

− 0.27(T /T

C

)

5/2

– Ð spin wave   & ñ ? /\ 

"

f ¸ ú ˜ # Œl  H † d`  ¦ · ú ˜ à º e ” % 3  .

PACS numbers: 74.25.Ha, 75.50.Gg, 76.80.+y Keywords: M¨ ossbauer Û ¼& 7 ˜à Ô! 3 , a % ¦ 0 q ] j› ¸Z O , LiFeO

2

I. " e  ] Ø

o

½ ¢ § s “ : r„  t   H \  -t x 9 • ¸ Z  } “ ¦  l  ~ ½ ӄ   Ö  ¦ s  ± ú  Ü

¼ 9 1 l x{ 9  ^ ‰& h , Á º>  { © œ 6   x | ¾ Ós   H  © œ& h `  ¦ t “ ¦ e ”  .

÷

 r ë ß –  m  , B j— ¸o  ´ òõ  \ O # Q" f  6   x  © œ ¼ # o  “ ¦ à º

"

î s  U  ´ . ” ¸à Ô· ¡ ¤, Ö  r ï 8, Ê ë@ /„   o 1 p x þ j   H ] j¾ ¡ § _  ™ è + þ

A o\     „  t  „  ^ ‰ ] j¾ ¡ § \  p u   H % ò † ¾ Ós  & & ’ Ü ¼ 9, Õ ª\      Ҿ ¡ § _   â | ¾ Ó oü < $  ™ èq „  § 4  oü <  8Ô  ¦

#

Q „  t _  ™ è+ þ A oü < é ß –0 A€  & h { © œ @ /6   x | ¾ Ó o ´ ú §“ É r › ' a d ”  s

 ÷ &“ ¦ e ”   [1,2]. : £ ¤ y , o ½ ¢ § (Li) õ  ^ o = (Fe) í ß – oÓ ü t“   LiFeO

2

ü < LiFe

5

O

8

\  @ /ô  Ç ƒ  ½ ¨  H o ½ ¢ § s “ : r„  t _  cath- ode Ó ü t| 9 – Ð_  6 £ x6   x õ   Å (garnet : Y

3

Fe

5

O

12

)`  ¦ @ /’   

#

Œ ˜ Ð  $ § 4 ô  Ç   _   s ß ¼– Ð  6 £ x6   x  Ҿ ¡ § > hµ 1 ϖ Ð “  

# Œ ´ ú §“ É r ƒ  ½ ¨ s À Ò# Qt “ ¦ e ”   [3,4]. LiFeO

2

  H ½ + Ë$ í

›

¸|  x 9 ~ ½ ÓZ O \     α-LiFeO

2

, β-LiFeO

2

, x 9 γ-LiFeO

2

_  3 t    & ñ ½ ¨› ¸\  ¦ t “ ¦ e ”  . α-LiFeO

2

  H €  d ”  { 9 ~ ½ Ó

&

ñ (fcc cubic) ½ ¨› ¸– Ð, Li

+

ü < Fe

3+

s “ : r“ É r Ô  ¦ ½ ©g Ë :& h Ü ¼– Ð

E-mail: [email protected] Tel: 02-910-4752, Fax: 02-910-5170

¼

1 π  ^ ‰  o \  ¦ & h Ä » “ ¦ e ” Ü ¼ 9, / B N ç ß –ç  H“ É r F m3m s  .

γ-LiFeO

2

(tetragonal, I41/amd)  H Li

+

ü < Fe

3+

s “ : r s  ¼ 1 Ï

€

 ^ ‰ ½ ¨› ¸\ " f ½ ©g Ë :& h “   | 9 " f\  ¦ f ” Ü ¼– Ð   & ñ     @ / g A$ í s  ×  ¦ # Q[ þ t # Q { 9 ~ ½ Ó& ñ ½ ¨• ¸\ " f  ~ ½ Ó& ñ ½ ¨› ¸– Ð    

€

 " f % 3 # Q”   . ¢ ¸ô  Ç, β-LiFeO

2

(monoclinic, C2c)  H α- LiFeO

2

\ " f γ-LiFeO

2

– Ð      H ×  æ ç ß –õ & ñ \ " f + þ A$ í  ) a   [5]. LiFeO

2

Ó ü t| 9 _  „  l & h  : £ ¤$ í “ É r ´ ú §“ É r ƒ  ½ ¨ s À Ò# Qt 

“

¦ e ” Ü ¼   l & h  $ í | 9 \  › ' a ô  Ç ƒ  ½ ¨  H ´ ú §s   Ò7 á ¤ ô  Ç z  ´& ñ s

 . s \  ‘ : r ƒ  ½ ¨\ " f  H a % ¦ 0 q ] j› ¸Z O Ü ¼– Ð LiFeO

2

\  ¦ ] j

›

¸ # Œ DTA/TGA, x-‚    r] X l , Å Ò „   ‰ & ³p  â (SEM)

`

 ¦ s 6   x # Œ \ P % ƒo › ¸| ,   & ñ ½ ¨› ¸ x 9 { 9  _  ß ¼l \  ¦ › ¸



 % i Ü ¼ 9, M¨ossbauer ì  rF g l , ”  1 l x r « Ñ  oÖ  ¦8 £ ¤& ñ l 

\

 ¦ : Ÿ x # Œ Li

+

, Fe

3+

s “ : r[ þ t _  site ì  r Ÿ í• ¸ x 9  l & h  $ í

| 9

`  ¦ › ¸  % i  .

II. ÷ m Ç] M ö U ê s0 n É

a

% ¦ 0 q ] j› ¸Z O Ü ¼– Ð LiFeO

2

ì  r ´ ú ˜`  ¦ ½ + Ë$ í l  0 Aô  Ç Ø  ¦ µ 1 Ï

"

é

¶ « і Ð" f  H í  H • ¸ 99.99 %_  iron nitrate (Fe(NO

3

)

3

-527-

(2)

Fig. 1. TGA/DTA curves of LiFeO

2

gel powder.

·9H

2

O) x 9 99.99 %_  lithium acetate (CH

3

CO

2

Li)\  ¦   6

 

x % i Ü ¼ 9, 6   x B – Ѝ  H distilled water (H

2

O), ethylene glycol (HOCH

2

CH

2

OH) x 9 acetic acid (CH

3

COOH)`  ¦ 1 : 7 : 2 _  q Ö  ¦ – Ð ™ D ¥ ½ + Ë # Œ  6   x % i “ ¦ ‚ à Ð] j– Ѝ  H ethanol (CH

3

CH

2

OH)`  ¦  6   x % i Ü ¼ 9, s M : stock solu- tion _  ]  t 0 l x • ¸  H 0.2 M – Ð ‚  × þ ˜ % i  . Ø  ¦ µ 1 Ï" é ¶ « Ñ\  ¦ ™ D ¥ ½ + Ë ô

 Ç 6   x B \  ¦ 60

C \ " f 12r ç ß – ì ø Í6 £ x`  ¦ r &  ¢ - a„  y  6   x K  r

(   . ì  r ´ ú ˜r « Ñ\  ¦ % 3 l  0 A # Œ ”  / B N 𠏑 É r \ " f 100

C

\

" f { 9 Å Ò{ 9 ç ß – | › ¸ # Œ œ íl  ì  r ´ ú ˜`  ¦ ] j› ¸ % i  . | › ¸ ì

 r ´ ú ˜\  @ /ô  Ç Ä »l Ó ü t _  ì  r K  x 9   & ñ  © œ_  Ò q t$ í [ þ t`  ¦ S X ‰ “  

“ ¦ \ P % ƒo  › ¸| `  ¦ · ú ˜ ˜ Ðl  0 A # Œ, TA Instruments  _

 SDT 2900— ¸4 S q`  ¦ s 6   x # Œ DTA/TGA`  ¦ à º' Ÿ  % i  .

|

› ¸  ) a ì  r ´ ú ˜`  ¦ DTA/TGA – РÒ'  % 3 “ É r   õ \  ¦  Ö ¸6   x # Œ

|

› ¸ô  Ç ì  r ´ ú ˜`  ¦ 600

C \ " f 3r ç ß – 1 l x î ß – / B N l  ×  æ \ " f \ P 

%

ƒo  # Œ r « Ñ\  ¦ ] j› ¸ % i  . \ P % ƒo ô  Ç ì  r ´ ú ˜_    & ñ $ í

`

 ¦ S X ‰ “   l  0 A # Œ, Philips _  X’pert PW 1827 x-‚  



r] X ì  r$ 3 l  (CuKα)\  ¦ s 6   x # Œ x-‚    r] X • ¸,     © œÃ º

\

 ¦ ½ ¨ % i  . ¢ ¸ô  Ç, \ P % ƒo ô  Ç ì  r ´ ú ˜_  { 9  ß ¼l  x 9 ç  H{ 9 

•

¸\  ¦ S X ‰ “   l  0 A # Œ JSM-6700F _  SEM`  ¦ 8 £ ¤& ñ 

%

i  . M¨ossbauer Û ¼& 7 ˜à Ô! 3 “ É r „  l % i † < Æ& h  1 p x 5 Å q • ¸+ þ A [6]

M¨ ossbauer ì  rF g l – Ð 2 [ % i Ü ¼ 9, ‚  " é ¶“ É r Dupont  r ] j

¾

¡

§ _  Rh F K5 Å q \  [ þ t # Qe ”   H z  ´“ : r  © œI _  40 mCi_  57Co é ß – { 9

 ‚  `  ¦  6   x % i  . r « Ñ_  € ª œ“ É r 40 mg Ü ¼– Ð % i “ ¦ r « Ñ _

 ç  H{ 9 ô  Ç ¿ ºa \  ¦ 0 AK  f ”  â s  1 “  u s “ ¦ ¿ ºa  0.005

“

 u _  Be ó ø Í`  ¦ € ª œ€  \  } Œ • " f  6   x % i  . $ “ : rz  ´+ « >`  ¦ 0

AK " f APD CS-202 displex  © œu ü < DMX-20 M¨ossbauer vacuum shroud\  ¦  6   x % i “ ¦, r « Ñ_  \ P „  ² ú ˜`  ¦ 0 AK  Í ‰ t B

– Ð He gas\  ¦ í  H¨ 8 Š r (  Ü ¼ 9 1 psi · ú š§ 4 `  ¦ Ä »t  • ¸2 Ÿ ¤ 

%

i  . “ : r • ¸8 £ ¤& ñ “ É r “ : r • ¸› ¸] X l  (Lake Shore  DRC-91C + þ

A)\  ¦ s 6   x # Œ 0.05 K_  “ : r • ¸ š ¸ _  & ñ x 9 • ¸ü < 10−6 torr s  © œ_  ”  / B N • ¸\  ¦ Ä »t  % i  . VSM“ É r Lake Shore

Fig. 2. X-ray diffraction pattern of α-LiFeO

2

at room temperature. Open circle represents the observed pat- tern; continuous lines represent calculated and difference obs-cal patterns. Ticks markers correspond to the posi- tion of the allowed Bragg reflections.

7300`  ¦ s 6   x # Œ # Œ Q “ : r • ¸\ " f ü @ Ò l  © œ`  ¦ 10 kOe

“

  # Œ  l & h  : £ ¤$ í `  ¦ 8 £ ¤& ñ % i  .

III. ÷ m Ç] M ö+ s ÇÊ Ý õ m Í w в  o

LiFeO

2

ì  r ´ ú ˜r « Ñ_    & ñ  o 0 p x ô  Ç \ P % ƒo “ : r • ¸\  ¦   

&

ñ “ ¦ ] j› ¸  ) a a % ¦ – РÒ'  Ä »• ¸  ) a  0 q_  Ä »l Ó ü t  1 l x`  ¦ › ¸



 l  0 A # Œ DTA/TGA z  ´+ « >`  ¦ ' Ÿ  % i Ü ¼ 9, Fig. 1\  LiFeO

2

 0 q_  DTA/TGA ì  r$ 3   õ \  ¦   ? /% 3  .

€



• 244

C Â Ò   H \ " f › ' a ¹ 1 Ï÷ &  H µ 1 Ï\ P  x ß ¼  H > 5 Å q ÷ &  H

à ºì  r K  x 9 ×  æ» ¡ ¤ ½ + Ëì ø Í6 £ x _   Òí ß –Ó ü t – Ð" f Ò q t$ í  ) a Ä »l Ó ü t _ 

ƒ

 ™ è\  _ ô  Ç  כ Ü ¼– Ð 55 %_  ×  æ | ¾ Óy Œ ™™ è\  ¦ à ºì ø Í “ ¦ e ” Ü ¼ 9, 550

C s  © œ_  “ : r • ¸\ " f_  | 9 | ¾ Ó y Œ ™™ è  H \ O % 3  . s 

“

: r • ¸ % ò % i \ " f LiFeO

2

 © œ_    & ñ Ò q t$ í s  r  Œ • H † d`  ¦ 0 p u

½

+ É Ã º e ”  . 0 A_    õ \  ¦ s 6   x # Œ 600

C \ " f LiFeO

2

ì

 r ´ ú ˜`  ¦ \ P % ƒo  % i Ü ¼ 9,  © œ“ : r \ " f 8 £ ¤& ñ ô  Ç x-‚    r] X  8 £ ¤

&

ñ   õ    É r ½ ¨› ¸_  + þ A © œ \ O s  í  H à ºô  Ç é ß –{ 9  © œ_  r « Ñ\  ¦

½

+ Ë$ í ½ + É Ã º e ” % 3 Ü ¼ 9, s \  ¦ Fig. 2 \    ? /% 3  . ½ + Ë$ í ô  Ç r

« Ñ_  € ª œs “ : r ì  r Ÿ í 1 p x`  ¦   & ñ l  0 A # Œ Rietveld ì  r

$ 3

Z O \  _ ô  Ç & ñ º  `  ¦ à º' Ÿ  % i  . ì  r$ 3  r  Fullprof á Ԗ Ð Õ

ªÏ þ ›`  ¦ s 6   x % i  . þ j7 á x& h Ü ¼– Ð   & ñ  ) a     © œÃ º  H a = 4.1610 ± 0.0005 ˚ A s % 3 Ü ¼ 9, ’  ø @• ¸\  ¦   ? /  H Bragg

“

   R

B

, R

F

  H y Œ •y Œ • 5.56, 3.79 %% i  . Fig. 2_  x-‚    r ] X

 ‚  `  ¦ ì  r$ 3 ô  Ç   õ   H F m3m _  / B N ç ß –ç  H`  ¦ ° ú   H { 9 ~ ½ Ó& ñ + þ

A ½ ¨› ¸ s ü @_   r] X  ‚  “ É r ˜ Ðs t  · ú §€ Œ ¤Ü ¼ 9 & ñ º  _    õ 

\

" f ˜ Ð1 p w s  z  ´+ « > u ü < s  : r u  ¸ ú ˜ { 9 u † < Ê`  ¦ ˜ Ðs “ ¦ e ” 



.

(3)

Fig. 3. SEM micrographs of α-LiFeO

2

annealed at 600

C.

Fig. 4. M¨ ossbauer spectra of α-LiFeO

2

at low tempera- ture.

Fig. 3“ É r α-LiFeO

2

   & ñ _  $ í  © œ — ¸€ ª œ`  ¦ ˜ Ðs   H SEM 8

£ ¤& ñ   õ – Ð, 6 £ x| 9  ) a Ñ ü æ  H — ¸€ ª œ“ É r €  • 110 nm_  ß ¼l \  ¦

t  9, a % ¦ 0 q ~ ½ Ód ” \  _  # Œ ] j Œ •  ) a r « Ñ[ þ t _  „  + þ A& h “   + þ

AI \  ¦ ˜ Ðs “ ¦ e ” 6 £ §`  ¦ · ú ˜ à º e ”   [7]. α-LiFeO

2

_  Curie

Fig. 5. M¨ ossbauer spectra of α-LiFeO

2

at high temper- ature.

“

: r • ¸ü < $ “ : r \ " f_  p r & h   $ í : £ ¤$ í `  ¦ › ¸  l  0 A 

#

Œ M¨ossbauer Û ¼& 7 ˜à Ô! 3 `  ¦ 4.2 K \ " f 295 K_  “ : r • ¸# 3 0 A

\

" f 2 [ % i Ü ¼ 9, @ /³ ð& h “    כ [ þ t`  ¦ Fig. 4, 5 \    ? /% 3 



.

Curie “ : r • ¸ s  _  “ : r • ¸\ " f  H 2 set(  ¾ ú  A á ¤;I-site, î ß – A

á ¤;II-site) _  / B N" î f  ¨ à º‚  Ü ¼– Ð K $ 3  % i   [8]. s  Qô  Ç Û ¼

&

7 ˜à Ô! 3 `  ¦  [ jy  ì  r$ 3  l  0 A # Œ Lorentzian ‚  + þ A`  ¦   6

 

x # Œ þ j™ è 5 p xZ O Ü ¼– Ð ì  r$ 3  % i Ü ¼ 9 [9] s X O >  ì  r$ 3 ô  Ç

 

õ \  ¦ Table 1 \  ˜ Ð# ŒÅ ғ ¦ e ”  .

α-LiFeO

2

_  M¨ossbauer Û ¼& 7 ˜à Ô! 3 “ É r  © œ“ : r \ " f 2 line_ 



×  æF G  ì  r\ P ° ú כ ë ß –`  ¦ & ’   H X < s   H α-LiFeO

2

_  Curie

“

: r • ¸  © œ“ : r s  e ” `  ¦   ? /  H  כ s  . Curie “ : r • ¸\  ¦ S X

‰ “   l  0 A # Œ M¨ossbauer Û ¼& 7 ˜à Ô! 3 “ É r 4.2 K \ " f 295 K  t  “ : r • ¸\  ¦ 7 £ x r v  9 8 £ ¤& ñ ô  Ç   õ  4.2 K\ " f 55 K



t   H 6 line _  / B N" î f  ¨ à º‚  s  › ' a8 £ ¤ ÷ &% 3 Ü ¼  Õ ª s  © œ _

 “ : r • ¸\ " f  H 6 line _  / B N" î f  ¨ à º‚  s  ™ èY >  “ ¦ î  r

(4)

Fig. 6. Reduced magnetic hyperfine field H

hf

(T )/H

hf

(0) against reduced temperature T /T

C

for α-LiFeO

2

. Points marked are the experimental values. The full curve is the Brillouin curve for S = 5/2.

X

< 2 line_  Û ¼& 7 ˜à Ô! 3 ë ß – › ' a8 £ ¤ ÷ &% 3 Ü ¼ 9, α-LiFeO

2

_  Curie

“

: r • ¸  H 90 ± 3 K – Ð   & ñ % i  . M¨ossbauer ì  r$ 3   õ  Table 1 \ " f% ƒ! 3   © œ“ : r \ " f α-LiFeO

2

_  s $ í | 9 ^ ‰s 1 l x ° ú כ

“

É r 0.24 mm/s ° ú כ`  ¦ & ’ Ü ¼ 9, s   H α-LiFeO

2

_  Fe s “ : r s

 t   H s “ : r   H Fe

3+

e ” `  ¦ ˜ Ð# ŒÅ ҍ  H  כ s   [8]. 8 £ ¤& ñ

“

: r • ¸ 4.2 K\ " f 7 £ x ½ + Éà º2 Ÿ ¤ œ íp [ j  l  © œ ° ú כ“ É r y Œ ™™ è

†

< Ê`  ¦ · ú ˜ à º e ” % 3 Ü ¼ 9 4.2 K\ " f_  œ íp [ j l  © œ ° ú כ“ É r I- site x 9 II-site\ " f 506, 478 kOe,  ×  æF G  ì  r\ P ° ú כ“ É r y Œ •y Œ • 0.02, −0.02 m/s – Ð  _  % ò \  ¾ ú š>    z Œ ¤Ü ¼ 9, s   H α-LiFeO

2

_    & ñ ½ ¨› ¸ { 9 ~ ½ Ó& ñ + þ A   & ñ ½ ¨› ¸e ” `  ¦ _ p ô  Ç



. ¢ ¸ô  Ç s $ í | 9 ^ ‰s 1 l x ° ú כ“ É r 0.37(I-site) ü < 0.36 mm/s(II- site) – Ð   z Œ ¤  H X < y Œ • site_  ^ o = s “ : r s  Fe

3+

– Ð ” > r F † < Ê`  ¦

· ú

˜ à º e ”   [10]. s M : 4.2 K\ " f_  I-siteü < II-site_  €  & h  q

  H 50 % : 50 % – Ð s   H α-LiFeO

2

_    & ñ ½ ¨› ¸ { 9 ~ ½ Ó

&

ñ + þ A ½ ¨› ¸e ” `  ¦ S X ‰ “  ½ + É Ã º e ”   H  כ s   [8].

Fig. 6“ É r α-LiFeO

2

_  œ íp [ j  © œ ° ú כ_  ¨ î ç  H ° ú כ`  ¦ “ : r

•

¸\    É r    o– Ð Curie “ : r • ¸ T

C

\  @ /ô  Ç ¨ 8 Š í ß –  ) a “ : r • ¸ T /T

C

\ " f_  ] X @ / % ò • ¸\ " f_  œ íp [ j l  © œ H

hf

(0) \ 

@

/ô  Ç ¨ 8 Š í ß –  ) a œ íp [ j l  © œ H

hf

(T )/H

hf

(0) _     o ° ú כ`  ¦



 ? /“ ¦ e ”  . " é ¶ Ü ¼– Ð ³ ðr   ) a & h [ þ t s  M¨ossbauer z  ´+ « >

° ú

כs  9 s \  @ /K  z  ´‚  Ü ¼– Ð ³ ðr   ) a  כ “ É r spin ° ú כs  S = 5/2“   Brillouin s  : r/ B G‚  Ü ¼– Ð+ ‹ š ¸  # 3 0 A ? /\ " f " î S X ‰

>  ¸ ú ˜  Ø Ô“ ¦ e ”  . Õ ª QÙ ¼– Ð α-LiFeO

2

? /_  Fe

3+

s 

“

: r[ þ t“ É r S = 5/2 – Ð high spin  © œI e ” `  ¦ · ú ˜ à º e ” % 3   [11].

Fig. 7“ É r spin wave theory \  _  # Œ α-LiFeO

2

_  T /T

C

<0.7 # 3 0 A? /_  “ : r • ¸% ò % i \ " f ¨ î ç  H œ íp [ j  l 



© œ ° ú כ_  “ : r • ¸\    É r    o\  ¦ ] X @ /% ò • ¸\  @ /ô  Ç ° ú כ\  @ / ô

 Ç q – Ð   ? /“ ¦ e ”  . “ : r • ¸\    É r œ íp [ j  l  © œ ° ú כ

Fig. 7. Fractional change of the average magnetic hyper- fine field, H

hf

, as a function of (T /T

C

)

3/2

for α-LiFeO

2

.

Fig. 8. Reverse magnetic susceptibility of α-LiFeO

2

.

“ É

r “ : r • ¸ 7 £ x † < Ê\     y Œ ™™ è   H X < Õ ª d ” “ É r  6 £ § õ  ° ú  



 [12].

H

hf

(T ) − H

hf

(0)

H

hf

(0) = −B

3/2

 T T

C



3/2

− C

5/2

 T T

C



5/2

(1)

#

Œl " f T

C

  H Curie “ : r • ¸s  9 H

hf

(T )  H “ : r • ¸ T \ " f_ 

œ

íp [ j l  © œ ° ú כs “ ¦, H

hf

(0)  H ] X @ /% ò • ¸\ " f_  œ íp [ j



l  © œ ° ú כs  . œ íp [ j  l  © œ z  ´ + « >° ú כ\  d ”  (1)`  ¦ þ j™ è



5 p x ° ú כÜ ¼– Ð > í ß –ô  Ç   õ  α-LiFeO

2

_   â Ä º spin wave  © œ Ã

º B

3/2

= 0.36 ± 0.05, C

5/2

= 0.27 ± 0.05 s % i Ü ¼ 9, s

 ° ú כ“ É r   & ñ $ í  $ í Ó ü t| 9 “   α-Feü < Ni_  0.11 x 9 0.12

˜

Ð   s `›    H ° ú כ`  ¦ t   H X < s   H  © œ  © œ_  spin wave

α-LiFeO

2

  & ñ ? /\ " f  8 ¸ ú ˜ # Œl  H † d`  ¦ · ú ˜ à º e ”   [13].

Fig. 8“ É r VSM`  ¦ s 6   x # Œ þ j@ / 10 kOe_  ü @ Ò l  © œ

`

 ¦ “   # Œ 8 £ ¤& ñ ô  Ç α-LiFeO

2

_  % i    oÖ  ¦`  ¦   ? /“ ¦ e ”

 .



© œ $ í \  K { © œ   H  Òì  r`  ¦ ‚  + þ A  H  Z O `  ¦  6   x # Œ ì  r

$

3 ô  Ç   õ  Curie-Weiss “ : r • ¸(θ

P

)  H @ /| Ä Ì −160 K s % i Ü ¼

(5)

%

i Ü ¼ 9, 4.2 K\ " f_  œ íp [ j l  © œ ° ú כ“ É r 506 kOe x 9 478 kOe, Curie “ : r • ¸  H 90 ± 3 K – Ð   & ñ % i  .  © œ“ : r \ " f s 

$ í

| 9 ^ ‰s 1 l x ° ú כ“ É r 0.24 mm/s – Ð ^ o = s “ : r _  „    © œI  +3

e ” `  ¦ · ú ˜€ Œ ¤Ü ¼ 9, Fe

3+

s “ : r[ þ t“ É r S = 5/2 – Ð high spin  © œ I

% i Ü ¼ 9 spin wave  © œÃ º  H B

3/2

= 0.36 ± 0.05, C

5/2

= 0.27 ± 0.05 – Ð 8 £ ¤& ñ ÷ &% 3  . ¢ ¸ô  Ç Curie-Weiss “ : r • ¸(θ

P

)  H

−160 K – Ð  l & h  : £ ¤$ í s  ì ø Íy © œ $ í : £ ¤f ç `  ¦   Í Ç x .

P

c p 8 ý ò k >

‘

: r ƒ  ½ ¨  H † < ÆÕ ü t”  < É ª F é ß –(KRF-2005-070-C00050)_  t 

"

é

¶  \ O \  _ ô  Ç  כ s  9 s \  y Œ ™ \  ¦ × ¼w n m  .

Y

c p w Š à U Ø ”  ô

[1] S. Y. An, I. B. Shim, C. S. Kim, J. Magn. Magn.

Mater. 290-291, 1551 (2005).

[2] X. Wang, L. Gao, F. Zhou, Z. Zhang, M. Ji, C. Tang,

(2005).

[7] P. Vaqueiro, M. P. Cosner-Lppez, and M. A. Lopez- Quintela, J. Solid State Chem. 126, 161 (1996).

[8] M. Tabuchi, S. Tsutsui, C. Masquelier, R. Kanno, K. Ado, I. Matsubara, S. Nasu, and H. Kageyama, J. Solid State Chem. 140, 159 (1998).

[9] S. J. Kim, K. W. Jung C. K. Kim, Hyperfine Inter- actions 156/157, 113 (2004).

[10] M. Tabuchi, C. Masquelier, T. Yakeuchi, K. Ado, I. Matsubara, T. Shirane, R. Kanno, S. Tsutsui, S.

Nasu, O. Nakamura, J. Solid State Ionics 90, 129 (1996).

[11] T. Matsumura, R. Kanno, Y. Inaba, Y. Kawamoto, and M. Takano, J. Electrochemical Soc. 149, A1509 (2002).

[12] S. Y. An, S. W. Lee, D. H. Choi, I. B. Shim, and C.

S. Kim, Phys. Stat. Sol.(c)1 12, 3310 (2004).

[13] C. S. Kim, S. Y. An, Y. R. Uhm, S. W. Lee, Y. B.

Kim and C. S. Kim, J. Appl. Phys. 83, 6929 (1998).

(6)

Magnetic Properties of LiFeO 2 Powders by a Sol-Gel Process

Seung Wha Lee

Department of Electronic Engineering Chungju National University, Chungju 380-702 Chul Sung Kim

Department of Physics, Kookmin University, Seoul 136-702 (Received 28 October 2005)

α-LiFeO

2

powders have been prepared by using a sol-gel method. The crystallographic and magnetic properties of the powders were investigated with DTA/TGA, XRD, SEM, M¨ ossbauer spectroscopy, and VSM. The α-LiFeO

2

single-phase is observed in the samples annealed at 600

C for 3 h in air. The crystal structure of α-LiFeO

2

is found to be cubic with a lattice of a = 4.1610 ± 0.0005 ˚ A. The Curie temperature of α-LiFeO

2

is found to be 90 ± 3 K. The isomer shift values at room temperature are found to be 0.24 mm/s relative to Fe metal, which is consistent with high- spin Fe

3+

charge states. The average hyperfine field H

hf

(T ) of the α-LiFeO

2

shows a temperature dependence of [H

hf

(T ) − H

hf

(0)]/H

hf

(0) = −0.36(T /T

C

)

3/2

− 0.27(T /T

C

)

5/2

for T /T

C

< 0.7, indicative of spin-wave excitation.

PACS numbers: 74.25.Ha, 75.50.Gg, 76.80.+y

Keywords: M¨ ossbauer spectroscopy, Sol-gel method, LiFeO

2

E-mail: [email protected]

수치

Fig. 1. TGA/DTA curves of LiFeO 2 gel powder.
Fig. 4. M¨ ossbauer spectra of α-LiFeO 2 at low tempera- tempera-ture.
Fig. 7. Fractional change of the average magnetic hyper- hyper-fine field, H hf , as a function of (T /T C ) 3/2 for α-LiFeO 2 .

참조

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