• 검색 결과가 없습니다.

-Substitution on the Ferroelectric and Piezoelectric Properties of BiFeO

N/A
N/A
Protected

Academic year: 2021

Share "-Substitution on the Ferroelectric and Piezoelectric Properties of BiFeO"

Copied!
5
0
0

로드 중.... (전체 텍스트 보기)

전체 글

(1)

Effects of Bi(Zn

2/3

Ta

1/3

)O

3

-Substitution on the Ferroelectric and Piezoelectric Properties of BiFeO

3

-BaTiO

3

Ceramics

Jin Su Park · Myang Hwan Lee · Da Jeong Kim · Myong-Ho Kim · Tae Kwon Song

School of Materials Science and Engineering, Changwon National University, Changwon 641-773, Korea

Sung Jin Han · Won-Jeong Kim

Department of Physics, Changwon National University, Changwon 641-773, Korea

Dalhyun Do

Department of Advanced Materials Engineering, Keimyung University, Daegu 704-701, Korea (Received 20 April 2015 : revised 7 June 2015 : accepted 23 June 2015)

Lead-free ceramics with compositions of (1-x)[0.67Bi1.05FeO3-0.33BaTiO3]-xBi(Zn2/3Ta1/3)O3(x

=0.00, 0.01, 0.02, 0.03, 0.04 and 0.05) [BF-BT-BZTx] were prepared through a conventional solid- state reaction method. The effects of BZT substitution on the crystal structural, microstructural, piezoelectric and electrical properties of the ceramics were investigated. The X-ray diffraction patterns showed that all ceramics were crystallized with the perovskite phase. The grain size decreased with increasing BZT content. For x = 0.02, good ferroelectric and piezoelectric properties were observed: 2Pr= 42 µC/cm2and 2Ec= 55 kV/cm. The static- and the dynamic-piezoelectric constants were observed to be 130 pC/N and 290 pm/V, respectively.

PACS numbers: 77.65.-j, 77.65.Ly, 77.80.-e, 77.84.Dy

Keywords: Piezoelectric, Ferroelectric, Lead-free, BiFeO3, BaTiO3

Bi(Zn

2/3

Ta

1/3

)O

3

V ò ÿT &  BiFeO

3

-BaTiO

3

: g à k Ä­ Ž8 ý P ê s– ¥ ¹ Å õ m Í ° q  ¹ Å — ¤V R Ë; c Q

V À W ¥ W _ Ë] ‚ §

ƒ

‘

š . > ¬ £ · T ' å Z 9  · ™ » + ä  · ™ »' å ‡ Ú · ö ¶ B? - ! H

‚

½Ó"é¶@/†<Ɠ§ ’™èF /BN†<ÆÂÒ, ‚½Ó"é¶ 641-773

 6

Ò) ç  . > · ™ » 4 w H+ ä 

‚

½Ó"é¶@/†<Ɠ§ Ótüo†<Æõ, ‚½Ó"é¶ 641-773

|

¡î m g ` @

>

"î@/†<Ɠ§ ’™èF/BN†<ÆÂÒ, @/½¨ 704-701

(2015¸ 4Z4 20{9 ~ÃÎ6§, 2015¸£  6Z4 7{9 ú&ñ‘:r~ÃÎ6£§, 2015¸ 64 23{Z 9 >FSX‰&ñ)

q

±úš> [jb” (1-x)[0.67Bi1.05FeO3-0.33BaTiO3]-xBi(Zn2/3Ta1/3)O3 (x = 0.00, 0.01, 0.02, 0.03, 0.04 and 0.05) [BF-BT-BZTx]`¦ {9ìøÍ&h“ “¦©œìøÍ6£xZO`¦6s x #Œ ]j›¸ %i. BZT u¨8Š`¦ :Ÿx #Œ



&ñ½¨›¸, p½¨›¸, ·úš„$, „í l&h :£¤$í`¦›¸ %i. X-‚ r]X J‡ õ —¸ŽH[jb”\"f s 

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)



©œ \Os `…–ÐÚÔÛ¼sàÔ ½¨›¸\¦þA$+í Hכ `¦a›'¹1Ï %i. p½¨›¸ ±ú ·ú˜_ ß¼lH BZT€ªœs 7£x

½

+Éú2Ÿ¤ yŒ™™è %i. x = 0.02 \"f a%~“Ér y©œÄ»„ :¤$£õí ·úš„ :£¤$ísa8›'£¤÷&%3: 2Pr = 42 µC/cm2 Õ

ªo“¦ 2Ec= 55 kV/cm. &ñ·úš„õ %i·úš„©œÃºHyŒ•yŒ• 130 pC/N ü< 290 pm/V–Ða8›'£¤÷&%3.

PACS numbers: 77.65.-j, 77.65.Ly, 77.80.-e, 77.84.-s Keywords:·úš„^‰, y©œÄ»„^‰, qúš>[jb”, BiFeO3, BaTiO3

I. " e  ] Ø

q

±úš> qÛ¼ÁºÛ¼\¦l‘:r¼–ÜÐ ôÇ `…–ÐÚÔÛ¼sàÔ ·úš„ [

jb”“Ér Pb(Zr,Ti)O3 (PZT)\¦ @/^‰½+É Óüt|9–Ð"f ÅÒ3lq

~ Ã

Γ¦ e”. PZTH ĺúôÇ ·úš„ :£¤$í`¦ °úl M:ëH\ yŒ• 7

áx G'p"f x9 "loÆÓ\s'–Ð"f V,o 6 x÷&“¦ e”. ÕªQ



 ±úš“Ér “^‰\ u"î&h“ ׿1q ël H]j\¦ÏÒµ1qt rv 9, ]j

›

¸õ&ñ\"f ´ú§“rÉ Ä»KÓüt|9s µ1ÏÒqt÷&#Q ¨8Š⚸%i`¦ Ä» µ

1Ͻ+É Ãº e”H ëH]j&h`¦ t“¦ e” [1–3]. s ëH]j

&

hܼ–Ð ±úš`¦ Ÿí†<Ê t ·ú§Ü¼€"f a%~“Ér ·úš„:£¤$í`¦ t



H F«Ñ_ >hµ1Ïs €9כ¹ . ‰&³F, ´ú§s ƒ½¨ ÷&“¦ e”H q

±úš> ·úš„ F«Ñ_ Êê˜Ð–Ð"f, (Bi0.5K0.5)TiO3 (BKT), (Bi,Na)TiO3 (BNT), (K0.5Na0.5)NbO3 (KNN) 1pxs a%~

“ É

r š„·ú:£¤$`í¦ tH Üכ¼–Ð ˜Ð“¦ ÷&“¦ e”. ÕªX<

BiFeO3 (BF)H Z}“Ér œ„©s Ç©o “:r•¸ (Tc ∼ 1,103 K) ü

< a%~“Éry©œÄ»„$í`¦t“¦ e” [4–6]. tëߖ BF\¦ 6£x 6

 

x l 0AK"fH Z }“Ér ¾º[O„ÀÓ\¦ tH ëH]j&hs e”



. ¾º[O„ÀÓ\¦ צsl 0A #Œ ±“úÉr¾º[O„ÀÓü< a%~“Ér·úš

„

:£¤$í`¦ tH BaTiO3 (BT)< “ü ¦6 x^‰\¦ ëߖ[þt#Q ¾º [O

„ÀÓ x9 †¾Ó©œ)a ·úš„:£¤$í`¦ ئ “¦ e” [7–9]. y©œ Ä

»„:£¤$í“Ér ïߖÀÓ ìrFG (Pr)s 15 ∼ 22 µC/cm2, &ñ·úš

„

 :£¤$í>ú d33H 43 ∼ 116 pC/N, %·iúš„:£¤$í 0AH 0.12 ∼ 0.14%`¦›¸$ís x = 0.3 ∼ 0.4\"f ˜Ð“¦÷&“¦ e”



 [10,11]. #Œl\ Bi\¦l‘:rܼ–Ð ôÇ Bi(Mg1/2Ti1/2)O3 ü< Bi(Ni1/2Ti1/2)O3 ¦ (1-x)BiFeO\ 3-xBaTiO3ü< Œ™$í ì

r> “¦6 x^‰\¦ –[ßëþt#Q 8¹¡¤ Ó†¾©œ)a :£¤$í`¦ ˜Ðs“¦ e”



 [12–14]. þjH 0.71BF-0.29BT[jb”\"f Bo\ (Mg1/3Nb2/3)4+\¦u¨8Š# Œ €• 158 pC/N _ †¾Ó©œ)a·úš

„

 :£¤$í`¦ ˜Ð“¦ %i [15]. ‘r: ƒ½¨\"fH ©œâ>%ò

%

iܼ–Ð ·ú˜94R e”H 0.67Bi 1.05FeO3-0.33BaTiO3 [jb”

\

 (Mg1/3Nb2/3)4+ü< °ú “Ér „ú\¦ t“¦ e”H Znõ Ta\¦ ‚×þ˜ #Œ Bi\¦ l‘r:ܼ–Ð ôÇ (Zn2/3Ta1/3)3+ u¨8Š

#Œ “¦6 x^‰\¦ –[ßëþt âĺ †¾Ó©œ)a ·úš„ :¤$£í`¦ l@/½+É Ã

º e”#Q ƒ½¨ %i. (1-x)[0.67Bi1.05FeO3-0.33BaTiO3]- xBi(Zn2/3Ta1/3)O3(x = 0.00, 0.01, 0.02, 0.03, 0.04, 0.05, BF-BT-BZTx)_ ›¸$íܼ–Ð &½ñ¨›¸, p½¨›¸, y©œÄ»„

, ·úš„ :£¤$í\ @/ôÇ ƒ½¨\¦ ”'Ÿ %i.

E-mail: [email protected]

II. ÷ m Ç] M ö U ê s0 n É

BF-BT-BZTx (x = 0.00, 0.01, 0.02, 0.03, 0.04, 0.05) [

jb”“Ér {9ìøÍ&h“ “¦œ ì© øÍ6£xZOܼ–Ð Bi2O3, Fe2O3, BaCO3, TiO2, ZnO Õªo“¦ Ta2O5 (>99.9%, Sigma- Aldrich) ìr´ú˜`¦ s6 x #Œ ]j›¸ %i. tØÔïm ^¦

`

¦s6 x #Œ ›¸$í\  gA|¾ÓôÇ ìr´ú˜`¦˜ú·ï`¦õ †<Êa 12rçߖ 1lx– ™ßîD¥½+Ë x9 ìrW %i. |› ¸ Êê\ 700C\"f 2rçߖ 1lxîߖ 1  ™è (calcination) “¦, ìr´ú˜_ çH|9$í`¦ Z

}sl 0AK _þvd” x9aAõ |› ¸\¦ìøÍ4¤ŸÊê 800C\"f 2r ç

ߖ 1lxîߖ 2  ™è %i. þj7áx ™èôÇ ìr´ú˜`¦+$íþA`¦0A ô

Ç ½+Ë]j–Ð 5 wt% e¦o qu´ ·ú˜ï`¦`¦'‘ #Œ }Œ•  µ

1Ï\"f “¦ÀÒ [O“ÉrÊê 150 µm ^‰–Ð ^‰2£§ %i. r¼#_

+þA“Ér {9»¡¤·úš $í+AZþOܼ–Ð ·úš§4`¦K, t2£§ 10 mm,

¿

ºa 0.6 mm_ "é¶óøÍ+þAI–Ð r¼`#¦]j›¸ %i. —¸ŽH›¸

_ r¼#“Ér 1,000C \"f ™è %i“¦, ©œ“:rt /åL͉t y

Œ

• ~½ÓZO`¦s6 x #Œ [jb”`¦]j›¸ %i [16]. [jb”_

½

¨›¸H X-‚ r]X ìr$3l (XRD, Miniflex II, Rigaku)\¦ s

6 x #Œ ©œ“:r\"f ›¸ %i. [jb”_ ³ð€ p½¨

›

¸HÅÒ „‰&³pâ (SEM, JSM-5610, Jeol)`¦s6 x 

#

Œ ¶ú˜(R ˜Ð€Œ¤. „l&h :£¤$`í¦ 8£¤&ñ l 0A #Œ [jb”

³

ð€\ Û¼('aA`¦s6 x #Œ Ñþ˜FK~ÃÌ}Œ•`¦ ïhAôÇ Êê Õª 0

A\ “Ér`…sÛ¼àÔ\¦ s6 x #Œ „FG`¦ {9+ÀI. y©œÄ»„ s

§ 4

/BG‚“Ér Radiant_ Precision LC œq©\¦s6 x #Œ 10 Hz_ ÅÒ ú\"f 8£¤&ñ %i. ·úš„:£¤$í`¦ 8£¤&ñ l 0A

#Œ, z´o–BHš¸{9\ 30ìr1lxîߖ 66 kV/cm f”ÀÓ „l©œ`¦

 #Œ ìrFG%ƒo (poling) %i. &·ñúš„©œÃºH d33-p '

 (ZJ-6B, HC Materials)\¦s6 x #Œ 8¤&£ñ %i. %i·úš

„

´òõH]X8ú¤d” 0A 8£¤&ñ G'p"f (LVDT, Millimar 1240, Mahr)\¦s6 x #Œ 50 mHz_ ÅÒ ú\"f 8£¤&ñ %i. e” x

~Û¼ ìr$3l (HP 4192A)\¦6 x #Œ “:r•¸ o\ 

 É

rÄ»„©œÃº\¦ 8£¤&ñ %i.

III. + s ÇÊ Ý õ m Í À X Ø8 ý

Fig. 1“Ér BF-BT-BZTx[jb”_ X-‚ r]X J‡`¦˜Ð

#

ŒÅғ¦ e”. 8£¤&ñ õ&ñ\"f µÏÒ1qt H š¸ \¦þj™èo  l

 0A #Œ z´o–BH (99.999%) ìr´ú˜`¦s6 x #Œ r]X yŒ••¸

(3)

Fig. 1. (Color online) X-ray diffraction patterns of BF- BT-BZTx ceramics.

Fig. 2. SEM microstructure images of (a) BF-BT- BZT0.00, (b) BF-BT-BZT0.01, (c) BF-BT-BZT0.02, (d) BF-BT-BZT0.03, (e) BF-BT-BZT0.04, and (f) BF-BT- BZT0.05.

\

¦ ˜Ð&ñ %i. —¸ŽH ›¸$í\"f `…–ÐÚÔÛ¼sàÔ ½¨›¸\¦

˜

Ðs“¦ e”ܼ 9, 0x€p&ñ>õ &ñ~½Ó&ñ>_ ™D¥Ë+½)a ½¨›¸\¦

˜

Ðs“¦ e”ܼ 9, s ©œ“ÉrÏ|1µ÷&t ·ú§€Œ¤. BZT u¨8Š

€

ªœ_ 7£x\  (110) xß¼ ±ú“Ér yŒ• Aá¤Ü¼–Ð ›¸FK ¹¡§ f”

sHכ `¦›'a¹1Ï½É Ã+º e”. (110)xß¼_ s1lx“Ér B-o s

“:r Fe(0.645 nm), Ti(0.605 nm)_ ß¼l\ q #Œ u¨8Š

)

as“:r Zn(0.74 nm), Ta(0.64 nm)_ ß¼l &"f (110) x

ß¼ ±ú“ÉryŒ• Aá¤Ü¼–Ð s1lxôÇ כ ܼ–Ð ˜Ð“.

Fig. 2H BZT€ªœ\ Ér³ð€ p½¨›¸ ”s. „

^

‰&hܼ–Ð ˜ÐsH ux9ôÇ p½¨›¸\¦ :Ÿx #Œ ™è õ&ñ

×

æ ux9o ¸ú˜ ”'Ÿ ÷&%36£§`¦·ú˜ ú e”%3. BZT\¦u

¨8

Š H€ªœs 7£x†<Ê\ , ±ú ·ú˜_ ß¼lH&h  yŒ™™è 



H↾Ó`¦˜Ðs“¦ e”. ± ·úú˜_ ß¼l yŒ™™è HsÄ»H u

¨8ŠôÇ Zns“:rõ Ta s“:rs ± ·úú˜_ $큩œ`¦%3]j %il M

:ëHܼ–Ð ˜Ð“.

Fig. 3(a)H©œ“:r\"f 8£¤&ñôÇ %i·úš„ ´òõ“ 0A-„l



©œ (S−E) /BG‚`¦˜Ð#ŒÅғ¦ e”ܼ 9, Fig. 3(b)Hs–ÐÂÒ'

½

¨ôÇ %i·úš„ >ú (d33)ü< d33-p'\¦s6 x #Œ 8£¤&ñôÇ

Fig. 3. (Color online) (a) Bipolar strain vs. electric field (S − E) loops BF-BT-BZTx ceramics and (b) static piezoelectric constant (d33) and dynamic piezoelectric constant (d33 ) of BF-BT-BZTx ceramics.

&

ñ·úš„>ú (d33) X<s's. Fig. 3(a)_ %i·úš„ ´òõ



H BF-BT-BZT0.01 ∼ 0.05 ›¸$í\"f 60 kV/cmt „ l

©œ`¦ #Œ 8£¤&`ñ¦ %i. tëߖ, BF-BT-BZT0.00

›

¸$í\"fH ©œ@/&hܼ–Ð ¾º[O„ÀÓ Z} 55 kV/cm \

"

f 8£¤&ñ %i. BF-BT-BZTx[jb”“rÉ ¸ú˜ µ1ϲú˜)a q

—

¸€ªœ_ /BG‚`¦ ˜Ðs 9 þj@/ 0A (Sm)ü< 6£§_ 0A (- Sn)\¦ ¸ú˜ ˜Ðs“¦ e”. íHúôÇ BF-BT_ r¼#“Ér„+þA&h

“

 q—¸€ªœ_ y©œÄ»„^‰ :£¤$í /BG‚`¦ ¸ú˜ ˜Ðs“¦ e”.

Õ

ªo“¦ „l©œs †½Ó„l©œ (Ec)\ •¸²ú˜Ùþ¡`¦ M:  



H 6£§_ 0A (-Sn) €• -0.15% &ñ•¸–Ð Hכ `¦·ú˜ ú e”



 [17]. tëߖ BZT 0.01 mol '‘ ÷&€"f 6£§_ 0A

 ß¼> yŒ™™è %“i¦ 0.01 molÂÒ' 0.05 molt '‘ 

% i

`¦ M: q5pwôÇ 6£§_ 0A °úכ`¦ ˜Ðs“¦ e”. ÕªQÙ¼–Ð BZT_ €ªœs 7£x ½+Éú2Ÿ¤ Sn °úכs yŒ™™è H `כ¦ ›'a¹1Ï

½

+É Ãº e”. Õªo“¦ BZT €ªœs 7x£ ½+Éú2Ÿ¤ Sm °úכ“Ér

"

f"fy 7£x H↾Ó`¦˜Ðs“¦, 0.02 (Sm= ∼0.18%)\

"

f ©œ Z}“Ér°úכ`¦˜Ðs“¦ e”. tëߖ, BF-BT\ BZT u

¨8Š€ªœs 0.02 mol˜Ð 7£x½É +âĺ Sm °úכs yŒ™™è H

†¾Ó`¦˜Ð%i. ©œ a~“%Ér0A °úכ“Ér BF-BT-BZT0.02\

"

f d33= 290 pm/Vܼ–Ð 8£¤& ÷ñ&%3. BF-BT [jb”\ BZT€ªœs 7£x½+Éú2Ÿ¤ ²DI“rÉ+þAI_ S − E /BG‚s ÁºÉr+þA I

_ S −E /BG‚ܼ–Ð o %i. íHúôÇ BF-BT\ q 

(4)

Fig. 4. (Color online) Room-temperature P − E hystere- sis loops of BF-BT-BZTx ceramics.

#

Œ 0.02 mol BZT\¦'‘ %i`¦M: ýaĺ @/gA&hs 9 Z}

“ É

r °úכ`¦ l M:ëH\ íߖ\O\"f ´ú§s 6£x6x ÷&HӐoÆÒ

\

s'–Ð &h6 xs|¨c âĺ 6£x6x 0px$ís Z}“¦ ÒqtyŒ•)a



. Fig. 3(b)H BF-BT-BZTx [jb”\ BZT €ªœ\ Ér d33õ d33_ o\¦˜Ð#ŒÅғ¦ e”. BF-BT-BZT0.02\

"

f &ñ·úš„ :£¤$ís œ Z© }“Ér d33 °úכs €• 130 pC/N–Ð 8

£¤&ñ÷&%3. Õªo“¦ x 0.02s©œ 7£x ½+Éú2Ÿ¤ d33°úכ“Ér y

Œ

™™è H כ ܼ–Ð ›'aÏ ÷1¹ &%3. Õªo“¦ d33 °úכ“Ér BZT

ۻ

œs 0.02 molt 7£x½+Éú2Ÿ¤ 7£x H↾Ós ˜Ð%i“¦ 0.02 mols©œ uŠ8¨ ÷&%3`¦ M:\H r yŒ™™è H â†¾Ó s

 ˜Ð%i. BNT [jb”\"f q5wpôÇ o\¦ Jo 1px [18]õ Hussain 1px [19]_ 7HëH\"f ¸˜ ˜ú Ðs“¦ e”. 0A °úכ`¦ q

“§K ˜Ð€Œ¤`¦M: íHúBF-BT_ d33 °úכ“Ér 180 pm/Vs

%

3ܼ, BZT 0.02 mol`¦u¨8Š %i`¦M: 290 pm/V–Ð $í 0

p

xs †¾Ó©œ÷&H `כ¦ ^¦Ãº e” [11].

Fig. 4H BF-BT-BZTx [jb”_ 65 kV/cm „l©œ\

"

f 10 Hz_ ÅÒ ú–Ð 8£¤&ñôÇ yœÄ©»„ s§4 /BG‚ s. BF- BT-BZT[jb”“Ér¸ú˜ Ÿío)a§s4/BG‚`¦˜Ð#ŒÅғ¦ e”.

BF-BT-BZT0.02\"f ©œ HïߖÀÓìrFG°úכ(2Pr)“ €• 42 µC/cm2 °úכ`¦ ?/“¦ e”. Fig. 4_ '‘ÂÒ ÕªaË>“Ér BF- BT-BZT [jb”_ ü@ÂÒ „lœ\© Ér Prõ Ec_ o

\

¦  ·p כ s. ÕªaË>\"f ˜Ð1pws 2Pr_ âĺ BZT_

€

ªœs x = 0.02t 7£x  x = 0.03ÂÒ'H›¸FKm” y

Œ

™™è %i.

Fig. 5H BF-BT [jb”\ BZT_ '‘\  “:r•¸

\

 ÉrÄ»„ ©œÃº_ o\¦ ·p כ s. íHúôÇ BF- BTH ©œâ>%ò%isÙ¼–Ð Ä»„©œÃº þj@/°úכ`¦  ?/

“

¦, BZT '‘|¾Ós 7£x†<Ê\  TcH ?/9€"f Ä»

„

©œÃº•¸ yŒ™™è H ↾Ó`¦ ˜Ð“. [jb_” Ä»„Ö¦\

†¾Ó`¦puH “–ЍH ·ú±ú˜_ ß¼l, ™èx9•¸, ½¨

Fig. 5. (Color online) Temperature dependent dielectric constants of BF-BT-BZTx ceramics at a frequency of 10 kHz.

›

¸ü< °ú “Ér &ñ½¨›¸_ "é¶s“ e”`¦ ú e”ܼ 9, ±ú ·ú˜_ ß

¼l &t“¦ x9•¸ Z}|9ú2Ÿ¤Ä»„©œÃº &”“¦

· ú

˜94R e” [20]. Ä»„©œÃº °úכ_ yŒ™™è HsÄ»H íHú ô

Ç BF-BT [jb”\"f BZT u¨8Š\  Œ•tHp

½

¨›¸ü< XRD ©œ\"f  èߖ  °úכ_ 7£x "鶓“ כ Ü

¼–Ð ÒqtyŒ•)a.

IV. + s Ç Â ] Ø

‘

:r ƒ½¨\"fH (1-x)BiFeO 3-xBaTiO3 (BF-BT) ›¸$í

`

¦l‘:rܼ–Ð #Œ Bi(Zn2/3Ta1/3)O3›¸$í`¦Œ™$íìr>–Ð u

¨8Š #Œ “¦œ ì©øÍ6£xZO`¦6s x #Œ [jb`”¦]j›¸ %i.

BF-BT-BZTx[jb” ±ú ·ú˜_ ß¼lH x_ €ªœs 7£x†<Ê\



"f yŒ™™è Hכ `¦ a›'¹1Ͻ+É Ãº e”%3. BF-BT-BZTx [

jb”_ XRD J‡“Ér `…–ÐÚÔÛ¼sàÔ ½¨›¸\¦ tH J

‡`¦˜Ð#ŒÅғ¦ e”“¦, íHúôÇ BF-BT [jb”_ âĺ 0px

€

&ñ>ü< &ñ~½Ó&ñ> ½¨›¸ ™D¥Ë½+)aJ‡`¦ ˜Ð#Œ Åғ¦ e”



 BZT€ªœs Zþt#Q ±ú˜Ãº2Ÿ¤ßx¼_ 0Au ±ú“ÉryŒ•ܼ–Ð s

1xl H‰&³©œ`¦a›'¹1Ͻ+É Ãº e”%3. BF-BT-BZT0.02 [j



b”\"f 2Pr“Ér 42 µC/cm2Õªo“¦ 2Ec H 55 kV/cm–Ð 8

£¤&ñ ÷&%3. Õªo“¦ &·ñúš„ >ú“ d33 = 126 pC/Nܼ

–

Ð 8£¤&ñ ÷&%3. ¢¸ôÇ, BF-BT-BZT0.02[ jb”\"f %i·úš

„

 0A°úכ“r 60 kV/cmÉ \"f 0.17% (d33= 290 pm/V)–Ð 8

£¤&ñ ÷&%3.

P

c p 8 ý ò k >

s

 7HëH“Ér 2011¸•¸ &ñÂÒ (pA‚½Ó›¸õ†<ÆÂÒ)_ F"é¶Ü¼

–

Ð ôDzDGƒ½¨Féߖ_ t"é¶`¦ ~ÃÎ ú'Ÿ)a ƒ½¨s 9 (No.

(5)

2011-0030058), &ñÂÒ (“§¹¢¤ÂÒ)_ F"¶éܼ–Ð ôDzDGƒ½¨F é

ߖ_ @/†<Æ×æ&hƒ½¨™è t"é¶\Oܼ–Ð ú'Ÿa)ƒ½¨{9m (No. 2012-045424, 2013R1A1A4A01010612). Õªo“¦ í

ߖ\O:Ÿx©œ"é¶ÂÒ lÕüt+À:’\Oܼ–Ð t"鶝)a ƒ½¨{9m (No. 10047914).

REFERENCES

[1] D. Lin, D. Xiao, J. Zhu and P. Yu, Appl. Phys. Lett.

88, 062901 (2006).

[2] K. G. Webber, Y. Zhang, W. Jo, J. E. Daniels and J. R¨odel, J. Appl. Phys. 108, 014101 (2010).

[3] R. Zuo and J. Fu, J. Am. Ceram. Soc. 94, 1467 (2011).

[4] A. Hussain, C. W. Ahn, A. Ullah, J. S. Lee and I.

W. Kim, Jpn. J. Appl. Phys. 49, 041504 (2010).

[5] W. Jo and J. Rodel, Appl. Phys. Lett. 99, 042901 (2011).

[6] V. D. N. Tran, A. Hussain, H.-S. Han, T. H. Dinh and J-S. Lee et al., Jpn. J. Appl. Phys. 51, 09MD02 (2012).

[7] T-H. Wang, C-S. Tu, Y. Ding, T-C. Lin and C-S.

Ku et al., Curr. Appl. Phys. 11, S240 (2011).

[8] Z. Cen, H. Yang, C. Zhou, Q. Zhou and J. Cheng et al., J. Electroceram. 31, 15 (2013).

[9] H. Deng, M. Zhang, Z. Hu, Q. Xie and Q. Zhong et al., J. Alloys. Compd. 582, 273 (2014).

[10] H. Zhang, W. Jo, K. Wang and K. G. Webber, Ce- ram. Int. 40, 4759 (2014).

[11] S. O. Leontsev and R. E. Eitel, J. Am. Ceram. Soc.

92, 2957 (2009).

[12] Q. Zhou, C. Zhou, H. Yang, G. Chen and W. Li et al., J. Am. Ceram. Soc. 95, 3889 (2012).

[13] C. Zhou, A. Feteira, X. Shan, H. Yang and Q. Zhou et al., Appl. Phys. Lett. 101, 032901 (2012).

[14] I. Fujii, R. Mitsui, K. Nakashima, N. Kumada and M. Shimada, Jpn. J. Appl. Phys. 50, 09ND07 (2011).

[15] X. Zhou, C. Zhou, Q. Zhou, H. Yang and Z. Cen et al. J. Electron. Mater. 43, 755 (2014).

[16] M. H. Lee, J. S. Park, D. J. Kim, R. C. Kambale and M-H. Kim et al., Ferroelectrics 452, 7 (2013).

[17] J. S. Park, K. T. Lee, J. H. Cho, Y. H. Jeong and J.

H. Paik et al., J. Kor. Ceram. Soc. 51, 527 (2014).

[18] W. Jo, R. Dittmer, M. Acosta, J. Zang and C. Groh et al., J. Electroceram. 29, 71 (2012).

[19] A. Hussain, C. W. Ahn, A. Ullah, J. S. Lee and I.

W. Kim, Jpn. J. Appl. Phys. 49, 041504 (2010).

[20] H. W. Kim, S. C. Kim, B. M. Jin, C. W. Ahn and I. W. Kim et al., Sae Mulli 53, 56 (2006).

수치

Fig. 2. SEM microstructure images of (a) BF-BT- BF-BT-BZT0.00, (b) BF-BT-BZT0.01, (c) BF-BT-BZT0.02, (d) BZT0.03, (e) BZT0.04, and (f)  BF-BT-BZT0.05
Fig. 4. (Color online) Room-temperature P − E hystere- hystere-sis loops of BF-BT-BZTx ceramics.

참조

관련 문서

The purpose of this study is to evaluate the effects of heat treatment on the load-deflection properties and transitional temperature range(TTR) of

Temperature distribution of cold region between thermoelectric cooling system and piezoelectric actuator was visualized without and with the piezoelectric

웹 표준을 지원하는 플랫폼에서 큰 수정없이 실행 가능함 패키징을 통해 다양한 기기를 위한 앱을 작성할 수 있음 네이티브 앱과

_____ culture appears to be attractive (도시의) to the

 When the price of an item declines, the substitution effect always leads to an increase in the quantity demanded of the good.. Income

intensive properties are available. • The calculation of these properties from measurable ones depends on the availability of simple and accurate relations between the two

– A collection of molecules (or atoms) in continuous random motion – Average speeds increases as T is raised.. – The molecules of a gas are widely separated (negligible

1 John Owen, Justification by Faith Alone, in The Works of John Owen, ed. John Bolt, trans. Scott Clark, &#34;Do This and Live: Christ's Active Obedience as the