• 검색 결과가 없습니다.

Structure and Magnetic Properties of

N/A
N/A
Protected

Academic year: 2021

Share "Structure and Magnetic Properties of"

Copied!
6
0
0

로드 중.... (전체 텍스트 보기)

전체 글

(1)

Structure and Magnetic Properties of

(Ru

1−y

Nb

y

)Sr

2

(Nd

0.67

Tb

0.67

Ce

0.66

)Cu

2

O

z

: Effect of Nb and Tb Substitutions

H. K. Lee · G. W. Kim

Department of Physics, Kangwon National University, Chuncheon 200-701, Korea (Received 1 August 2014 : revised 4 August 2014 : accepted 4 August 2014)

Polycrystalline samples of (Ru0.9Nb0.1)Sr2(Nd 1−x/2Tb1−x/2Cex)Cu2Oz (0.5 ≤ x ≤ 1.0) and (Ru1−yNby)Sr2(Nd0.67Tb0.67Ce0.66)Cu2Oz (0 ≤ y ≤ 1.0) were synthesized by using a solid-state reaction method. The structure and the magnetic properties were investigated by means of X-ray diffraction (XRD) and magnetization measurements. XRD data revealed that almost single-phase samples could be obtained for x = 0.66 - 0.8. Nb substitution was also found to result in a reduction of the weak-ferromagnetic component of the field-cooled (FC) magnetization and a reduction in the magnetic-ordering temperature. Based on the results of a Rietveld refinement of the XRD data, we discuss the structure and the magnetic behaviors induced by Nb doping and the local structural changes in the Ru sublattice.

PACS numbers: 74.72.-h, 74.72.Jt, 74.62.Bf, 74.25.Ha

Keywords: (Ru,Nb)Sr2(Nd,Tb,Ce)Cu2Oz, Nb doping, Structure, Magnetic property

Nb õ m Í TbV ò & ÿ; c  Â \ ¥ (Ru

1−y

Nb

y

)Sr

2

(Nd

0.67

Tb

0.67

Ce

0.66

)Cu

2

O

z

4 8 ý  Œ º õ m Í



M X ì Ä — ¤V R Ë

T

‡Ú£Ó · ™»4wH

y©

œ"é@<Ɠ§ Óüto<Æõ, ð; 200-701

(2014¸ 8Z4 1{9 ~ÃÎ6£§, 2014¸ 8Z4 4{9 ú&ñ‘:r~ÃÎ6£§, 2014¸ 8Z4 4{9 >FSX‰&ñ)

(Ru0.9Nb0.1)Sr2(Nd1−x/2Tb1−x/2Cex)Cu2Oz (0.5 ≤ x ≤ 1.0)õ (Ru1−yNby)Sr2(Nd0.67Tb0.67

Ce0.66)Cu2Oz (0 ≤ y ≤ 1.0)›¸$í_ &ñ r#`¦ “¦©œ ìøÍ6£xZO¼–Ð ½+Ë$í ¦ Õª ½¨›¸ü< l&h :

£¤$í`¦ X-‚ r]X (XRD) x9 ¸ :£¤$í 8£¤&ñ`¦ :ŸxK ƒ¨Ùþ¡. XRD ìr$3 H x = 0.66 - 0.8 {9 M

: _ éߖ{9©œ r#s ½+Ë$íH†d`¦˜Ð#Œ ÅÒ%3. ¢¸ôÇ Nb_ u¨8Š|¾Ós 7£x ls “:r•¸ ÷rm



 field-cooled (FC) 8£¤&ñZO¼–Ð 8£¤&ñ)a €•ôÇ y©œ$í $íìr_ ß¼l¸ yŒ™™èH†ds›'a8£¤÷&%3. Nb u¨8Š Ü

¼–Ð l)a ½¨›¸ x9 l&h :£¤$í\¦ XRDX<s'_ Rietveld ìr$3¼–Ð %3# Ru ÅÒ0A_ ²DG™è½¨›¸



< ƒ> #Œ 7H_&%3.

PACS numbers: 74.72.-h, 74.72.Jf, 74.62.Bf, 74.25.Ha

Keywords:(Ru,Nb)Sr2(Nd,Tb,Ce)Cu2Oz, Nb•¸iç, ½¨›¸, l&h :£¤$í

E-mail: [email protected]

952

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)

I. "e Â]Ø

CuBa2RCu2O7 (Cu-1212, R = Y ¢¸H ÐÀÓ "é™è)

>

 œí„¸^‰_ µ1Ï| [1] Êê u¨8Š\ @Ç ´ú§“Ér ƒ¨ ú '

Ÿ÷&%3¼ 9, Õª Bauernfeind 1px [2]“Ér Cu-1212 œí„

•

¸^‰_ Cu-O ^‰“o Cu @ Ru \¦u¨8Š ¦ Ba @/

’

 Sr`¦u¨8ŠôÇ RuSr2RCu2O8(Ru-1212)œí„¸^‰\¦%ƒ 6

£

§Ü¼–Ð ½+Ë$íÙþ¡. Õª[þÉr¢¸ôÇ RuSr2(R2−xCex)Cu2O10

(Ru-1222) > œí„¸^‰•¸ ½+Ë$íÙþ¡Ü¼ 9, s[þÉr Ru> œí

„

¸^‰–Ð Ô¦oº 9, R s Sm, Eu, x9 Gd {9 âĺ\ëߖ éߖ {9

©œs +þA$íH†ds ·ú˜94R e”. s[þt Ru > œí„¸^‰H

>

5Åq&h ƒ¨\ _K 1997¸ Ru-1222 >_ âĺ e”>

“

:r•¸ (Tc)€• 50 K s _ œí„¸ :£¤$íõ ls “:r•¸ (Tm) 100 - 180 K “ €•ôÇ y©œ$í:£¤$ís /B>r†<Ê [3]s

˜

Г¦÷&%3¼ 9, s#Q"f 1999 ¸\ Ru-1212> [4]\"¸ Ä»



Ç œí„¸ :£¤$íõ y©œ$í :£¤$ís /B>rôÇHƒ¨  õ

¸ ·ú˜9t"f s[þt$í œí„¸^‰\ @ǁָµ1ÏôÇ ƒ

½

¨ ú'Ÿ÷&#¸“¦ e”. s[þt $í œí„¸^‰_ Rux9 Cuo u¨8Š ƒ¨ Hs >\"f›'a8£¤÷Hy©œ$í“Ér RuO28£x\, Õªo¦ œí„¸ :£¤$í“Ér CuO2 8£x\ l H

כ

ܼ–Ð ·ú˜9t¦ e”. "f Ru 8£x_ l¨›¸ :£¤$í_ s

K ׿כ¹ > ÷&%3. l ½¨›¸ :£¤$í“Ér ׿$ír]X z

´+«¼–Ð ©œ "îSX‰y µ1߁n= ú e”¼ Ru >_ âĺ Õª

½

¨$í"é™è“ ÐÀÓ "é™è ׿$í f¨Ãº>º Bº H Sm, Eu, Gd 1px {9 Mߖ _ éߖ{9©œs ½+Ë$í÷&#Q Õª ƒ

½

¨ Ö¸µ1Ï t 3lþ¡. Õª!3\•¸ Ô¦½¨ ¦ ׿$í f¨Ãº

>

º &hÉr°úכqߖ 1lx0A"é™è\¦6 xK Ru-1212_ l

½

¨›¸ƒ¨ ú'Ÿ÷&%3 [5,6]. Õª  l:£¤$íܼ–Ð ìr

$

3H y©œ$í½¨›¸ m ìøÍy©œ$í_ Û¼—2; l ½¨

›

¸\¦ °úHכ ܼ–Ð ìr$3&%3. Õªo #Œ l&h¼–Л'a 8

£

¤÷H €•ôÇ y©œ$í :£¤$í“Ér RuÛ¼—2; l¸F'Ô l¦

#

Q4R (canting) Dzyaloshinsky-Moriya +þA ìøÍy©œ$í “§¨8Š



©œ ñŒ•6 xܼ–Ð €•ôÇ y©œ$ís Ä»•¸÷Hכ ܼ–Ð [O"î÷¦ e”

. ôǼ# Ru-1222>_ âĺH Ru-1212>< Ä» > RuÛ¼—2;\ _Ç ìøÍy©œ$í_ l¨›¸ ”>rFÇH [7]ü< ÕªÇ l¨›¸›'a8£¤÷&t ·ú§HH©œìøÍ÷H õ

 [8] ˜Ð“¦÷¦ e”. Õª¼–Ð Ru-1222>_ l¨›¸ :

£¤$í_ sKH Ru>_ œí„¸ x9 y©œ$í :£¤$í_ /B>r :£¤

$í

`¦ sK l 0AK Bº ׿כ¹ ¦ ^¦ ú e”. l

½

¨›¸ :£¤$í`¦sK l 0AK"H :£¤y ׿$ír]Xz´+«>s כ

¹½¨÷& 9 "f ׿$í f¨Ãº>º &hÉrÐÀÓ "é™è\¦ s

6 xôÇ Ru-1222 > éߖ{9©œ r#`¦ ½+Ë$í H כ s Ö¸µ1Ï ô

Ç ƒ¨\¦Ãº'Ÿ l 0AK"HBº |¹ . sÇ 3lq

&

h¼–Ð ĺoHþjH ׿$í f¨Ãº>º &hÉr Nd\H ô

Ç Ru-1222> ½+Ë$í`¦ƒ¨ #Œ Ruo\ Cu\¦ {9Ò u

¨8

ŠôÇ (Ru1−xCux)(Sr,Ba,Nd)(Nd,Ce)Cu2Oz(0.25 ≤ x ≤ 0.5)›¸$í\"f éߖ{9©œ`¦½+Ë$í½+É Ãº e”6£§`¦µ1Ï| [9,10] 

“

¦ ׿$ír]X z´+«>`¦Ãº'ŸÙþ¡. ÕªX< s âĺ ¸ 8

£¤&ñ Ru-1222 >\"f›'a8£¤÷&#:r€•ôÇ y©œ$í :£¤$í s

 ›'a8£¤÷&t ·ú§€Œ¤Ü¼ 9, Õª "é“s Nd “¦Ä»_ :£¤$í“t Ruo Cu u¨8ŠÜ¼–Ð Ru B$3 (dilution)÷&#Q Ruçߖ ¨î ç

Ho YO#Q4R {9#ߖ ‰&³©œ“t ·ú˜ ú \O%3. ‘:rƒ

½

¨\"H sÇ ƒ¨\ s#Q ׿$í r]Xz´+«>s 0px

 9, €•ôÇ y©œ$í :£¤$ís ›'a8£¤÷HDÐîr Ru-1222> _

 ½+Ë$í`¦ 3lq³ð–Ð ×æ$í f¨Ãº>º &hÉr Tb`¦ Nd o

\ {9Ò u¨8ŠôÇ r#_ ½+Ë$íõ Õª ½¨›¸&h Õªo¦ l

&

h

 :£¤$í ƒ¨\¦Ãº'ŸÙþ¡.

II. ÷mÇ ]Mö

r

#Ér “¦©œìøÍ6£xZO¼–Ð ½+Ë$íÙþ¡Ü¼ 9, ½+Ë$í M: íH•¸ 99.9% s©œ_ RuO2, Nb2O5, SrCO3, Nd2O3, Tb4O7, CeO2x9 CuO ìr´ú˜s s6 x÷&%3. r#Ér 1010 C\"f 7 ∼ 10 rߖ |9è ìr0Al\"f \P%ƒo ÷&%3¼ 9, s Êê í

ߖ™èÛ¼\¦ fËo 91050 C\"f 12 rߖ è ¦ s#Q

"

f 1060C\"f 15rߖ ™è Êê ©œ“:rܼ–Ð "‰þ¡. B

\P

%ƒo ׿çߖ\ r#Ér ìrW x9 $í+þ&ñ`¦'¬I. r# _

 ½¨›¸ ìr$3Ér Cu K±‚`¦ s6 xôÇ X’pert-pro MPD x9 Rigaku, Dmax 2200 X-‚ r]XlÐ 8£¤&ñ)aX<s'\¦

„

½Óܼ–Ð sÒ#Q&’¼ 9, ²DG™è½¨›¸ ìr$3 RIETAN-2000áÔ

–

ÐÕªÏþ›`¦s6 þ¡ [11]. r#_ ¸H Quantum De- sign _ SQUID©œuÐ 8£¤&ñ÷&%3¼ 9, 8£¤&ñ l©œ“Ér 20 Oe %i.

‘

:r ƒ¨\"H Nd\ HÇ Ru-1222 > +ËÓüt\

"

f Nd @ Tb_ u¨8Š ´òõ\¦ ›¸ l 0AK, \V q

&h¼–Ð (Ru0.5Nb0.5)Sr2(Nd1.34−xTbxCe0.66)Cu2Oz›¸

$í

ܼ–Ð r#`¦ ½+Ë$í ¦ ©œ_ íH•¸\¦ ›¸þ¡. sM: Ru @ Nb\¦ {9Ò u¨8ŠôÇ s»H Nb {9Ò u¨8Š

÷

 ©œ_ íH•¸ †¾Ó©œ÷H 7á_ ƒ¨ [12]\



H #Œ ú'Ÿ÷&%3. s z´+«>_  ĺoH Nbü<

Tb_ u¨8Š|¾Ós °ú `¦ M: ©œ_ íH•¸ ©œ Z}> ›'a8£¤

÷

&%3. s \Vq&h \¦ ½Óܼ–Ð ‘:r ƒ¨\"H (Ru0.9Nb0.1)Sr2(Nd1−x/2Tb1−x/2Cex)Cu2Oz(0.5 ≤ x ≤ 1.0)õ (Ru1−yNby)Sr2(Nd0.67Tb0.67Ce0.66)Cu2Oz (0 ≤ y ≤ 1.0)›¸$í_ r#\ @/K Õª :£¤$í`¦ƒ¨Ùþ¡.

(3)

Fig. 1. XRD patterns for (Ru0.9Nb0.1)Sr2(Nd1−x/2 Tb1−x/2Cex)Cu2Oz(0.5 ≤ x ≤ 1.0) samples. Peaks due to impurity phases are denoted by asterisk.

III. ÷mÇ]Mö+sÇÊÝ õmÍ ‚º8ý

Figure 1“Ér (Ru0.9Nb0.1)Sr2(Nd1−x/2Tb1−x/2Cex)Cu2Oz

(0.5 ≤ x ≤ 1.0) ›¸$í r#_ X-‚ r]X (XRD) X<s'

\

¦ ˜Ð#Œïr. Figure 1\ ³ðr)a < °ú s @Òìr_ r ]X

 xs¼H Ru-1222½¨›¸_ ©œÜ¼–Ð x9Qtº B^” ½+É Ã

º e”%3¼ 9, ©œ_ íH•¸H x 0.5 x9 0.6 {9 M: Û¼ Ð

³

ðr)a Ô¦íüts ›'a8£¤÷&%3. s Ô¦íüt xs¼H x 0.66- 0.8 %ò%i\"H _ ›'a8£¤÷&t ·ú§Ü¼ x 0.9 x9 1.0 {9 M: r›'a8£¤H†d`¦˜Ð#Œïr. sÐ"f ĺoH&h{©œ ô

Ç Ce_ u¨8Š ›¸| \"f (Nd,Tb)\HÇ DÐîréߖ{9



©œ_ Ru-1222 +ËÓüts ½+Ë$í|¨cú e”6£§`¦·ú˜ ú e”.

Figure 2H Fig. 1_ \¦½Óܼ–Ð (Ru1−yNby)Sr2 (Nd0.67Tb0.67Ce0.66)Cu2Oz(0 ≤ y ≤ 1.0)›¸$íܼ–Ð ½+Ë$í

)

a r#_ ¸ 8£¤&ñ\¦˜Ð#Œïr. ÕªaË>\"f ZFC (zero-field-cooled) 8£¤&ñ“Érl©œ`¦ t ·ú§“Ér©œI\

"

f “:r•¸\¦ €• 4 K t ±úðr Êê l©œ`¦  #Œ “:r•¸

\

¦ `¦o 9 8£¤&ñ÷&%3¼ 9, FC (field-cooled) 8£¤&ñ\"H



©œ“:r\"f €$ l©œ`¦ #Œ “:r•¸\¦€• 4 K t ±ú ð

rÊê Õª ©œIÐ “:r•¸\¦ `¦o 9 8£¤&ñôÇ s. Figure 2_ H Nbs u¨8Š÷&t ·ú§“Érr#_ âĺ ZFCü< FC 8

£¤&ñ  €• 110 K \"f t Òqtl 9 º#Qf”`¦ ^¦ Ã

º e”¼ 9, FC 8£¤&ñ H€•ôÇ y©œ$í :£¤$í`¦˜Ð#Œïr



. ZFC 8£¤&ñ H€• 30 K s \"f ìøÍ$í :£¤$ís›'a 8

£

¤÷&%3. Nb_ u¨8Š|¾Ó y°úכs 7£x > ÷ t Òqt

Fig. 2. Temperature dependences of zero-field- cooled (ZFC) and field-cooled (FC) dc magnetiza- tion measured at 20 Oe for the (Ru1−yNby)Sr2(Nd0.67

Tb0.67Ce0.66)Cu2Oz (0 ≤ y ≤ 1.0) samples.

l

H “:r•¸ yŒ™™è > ÷& 9 y°úכs 0.5 s©œs ÷ t

›'a8£¤÷&t ·ú§“¦ ZFC 8£¤&ñõ FC 8£¤&ñs _ 5gf”`¦

˜

Г. :£¤y Nb u¨8Š|¾Ó y 7£x > ÷ FC –Ð 8£¤&ñ

÷

Hy©œ$í ¸ /åLy yŒ™™è , s y©œ$í o

•

¸ :£¤$í“Ér y = 0.25 {9 M¸›'a8£¤H†d`¦˜Ð#Œïr. s 



H 7áxA_ (Ru1−xCux)(Sr1.47Ba0.2Nd0.33)(NdCe)Cu2Oz

>

 [10]_ âĺ x = 0.25 {9 M: €•ôÇ y©œ$í :£¤$ís›'a8£¤

÷

&t ·ú§H z´õ @/q& 9, s >\"f €•ôÇ y©œ$í :£¤

$í

s›'a8£¤÷&t ·ú§“Érכ “Ér Ruo u¨8Š\ _Ç Ru "é Ã

º_ yŒ™™è\ _Ç éߖíHôÇ B$3òõ(dilution effect)ëߖ“Ér



_”`¦trÇ. ©œl ¿º >_ âĺ ©œÃº_ s

e”

%3¼ 9, Ru o\ Cu\¦u¨8ŠôÇ âĺ Ru o\ °ú 

“ É

r|¾Ó_ Nb`¦ u¨8Š_ âĺ\ qK a »¡¤ U´sH 8 ß¼ 9 (3.8641 ˚A → 3.8565 ˚A), c »¡¤_ U´sH©œ@/&h¼–Ð Œ•€Œ¤



 (28.565 ˚A → 28.594 ˚A). Figure 2\"f FC –Ð 8£¤&ñ)a

€



•ôÇ y©œ$í :£¤$í_ ¸ “:r•¸ ±ú|9 M: /åLy 7

£

x H “:r•¸\¦ ls:r•¸ (Tm)ܼ–Ð çߖÅÒ½+É Ãº e” Ü

¼ 9, prܼ–Ð ìr$3)als:r•¸H y = 0 x9 0.25“

â

ĺ yŒ•yŒ• 110 K x9 70 K %i.

Nb u¨8Š\ Ér l&h :£¤$í< ²DG™è½¨›¸



<_ ›'a>\¦ sK l 0AK (Ru1−yNby)Sr2(Nd0.67 Tb0.67Ce0.66)Cu2Oz (0 ≤ y ≤ 1.0) ›¸$í r#_ XRD X

<s \¦ Rietveld ZO¼–Ð ìr$3 [13]ôÇ  Table 1\



  e”. Figure 3\H y = 0.25 “ r#_ XRD J

수치

Fig. 1. XRD patterns for (Ru 0.9 Nb 0.1 )Sr 2 (Nd 1−x/2 Tb 1−x/2 Ce x )Cu 2 O z (0.5 ≤ x ≤ 1.0) samples
Table 1. Refined structural parameters for the (Ru 1−y Nb y )Sr 2 (Nd 0.67 Tb 0.67 Ce 0.66 )Cu 2 O z (y = 0, 0.25, 0.5, 1.0) samples obtained from X-ray Rietveld analysis

참조

관련 문서

¾ Ferromagnetism ‰ Explanation of Ferromagnetism - Spontaneous magnetization: • the spins of unfilled d-band spontaneously aligned parallel to each other below TC within magnetic

Measured rock-magnetic properties including magnetic susceptibility χ, Anhysteretic remanent magnetization ARM, saturation remanent magnetization SIRM and S300 = -IRM-300mT / SIRM for

Room temperature magnetic hysteresis (M-H) curve showed an obvious ferromagnetic behavior and the magnetic moment per Fe atom under the applied of 0.8 T was estimated to be about

simply controlling the temperature, the micron-sized FeCo grains embedded FeCo film was synthesized where the large grains allow high magnetization originated from larger

The magnetic properties including saturation magnetization and coercivity at room temperature were measured in a maximum applied field of 20,000 Oe by using a vibrating

The strong dependence of torque on the magnetic field revealed that the magnetic easy axis is along the in-plane direction, and that the observed field-induced weak ferromagnetic

Short-range ferromagnetic interaction, in other words, a bound magnetic polaron, was revealed along the c axis by the small upturn of χ(T ) at low temperature, the deviation from

부산대학교 재료공학부 [Hysteresis Loop] 계면공학 연구실 Hysteresis loop: Magnetization [demagnetization] in materials  Hard magnetic- : permanent magnet  Soft magnetic- : recording materials