電気的、光学的性質 - 東北大学 金属材料研究所

࠙◊✲㒊ࠚ
◊ ✲ ㄢ 㢟 ྡ
↓ᶵᒙ≧໬ྜ≀ࡢບ㉳ᏊⓎග࡟ࡼࡿࢩࣥࢳ࣮ࣞࢱᮦᩱࡢ᥈⣴
◊✲௦⾲⪅ྡ
Ⲷ㔝 ᣅ
◊✲ศᢸ⪅ྡ
ྜྷᕝᙲ
ᮾ໭኱Ꮫ㔠ᒓᮦᩱ◊✲ᡤ
㸯㸬ࡣࡌࡵ࡟
㝧㟁Ꮚ᩿ᒙ᧜ീ⿦⨨ࡸ X ⥺ CT ࡢ᳨▱㒊ࠊ✵ ࡢᡭⲴ≀᳨ᰝᶵ࡞࡝࡟
⏝࠸ࡽࢀࡿᨺᑕ⥺᳨ฟჾࡣࠊᨺᑕ⥺ࢆ⣸እ㹼ྍどග࡟ኚ᥮ࡍࡿࢩࣥࢳ࣮ࣞ
Se
ࢱ࡜ࠊࡑࡢගࢆ㟁Ẽಙྕ࡟ኚ᥮ࡍࡿཷග⣲Ꮚ࡜࠿ࡽ࡞ࡗ࡚࠾ࡾࠊࡑࡢᛶ⬟
Ag
ࡣࢩࣥࢳ࣮ࣞࢱࡢ≉ᛶ࡟኱ࡁࡃ౫Ꮡࡍࡿࠋࢩࣥࢳ࣮ࣞࢱࡣᛂ⏝ୖ㧗Ⓨග㔞
Ba
࠿ࡘ▷ᑑ࿨࡛࠶ࡿࡇ࡜ࡀᮃࡲࡋ࠸ࡀࠊ⌧≧ࡢᕼᅵ㢮Ⓨග୰ᚰࢆ⏝࠸ࡿࢩࣥ
ࢳ࣮ࣞࢱࡣ᣺ືᏊᙉᗘࡢไ⣙࠿ࡽࠊࡇࢀ௨ୖࡢ≉ᛶࡢྥୖࡣ㞴ࡋ࠸ࠋࡑࡇ
࡛Ⓨගཎ⌮࡜ࡋ࡚༙ᑟయࡢບ㉳ᏊⓎගࢆ⏝࠸ࡿࡇ࡜ࡀヨࡳࡽࢀ࡚࠾ࡾࠊ
ZnO ࡸ PbI2 ࡞࡝࠸ࡃࡘ࠿ࡢ໬ྜ≀࡛ᐊ ࡛ࡢⓎග㔞ࡣ㠀ᖖ࡟ప࠸ࡶࡢ
RE
ࡢࠊ▷ᑑ࿨࡞ࢩࣥࢳ࣮ࣞࢩࣙࣥ≉ᛶࡀሗ࿌ࡉࢀ࡚࠸ࡿࠋ୍᪉༢⣧࡞༙ᑟయ
O
࡛ࡣ࡞ࡃ᭷ᶵ⤯⦕య㸫↓ᶵ༙ᑟయᒙࢆ✚ᒙࡉࡏࡿࡇ࡜࡛ࠊ㔞Ꮚ㛢ࡌ㎸ࡵຠ
ᯝ࡟ࡼࡾᐊ ࡛ࡶ▷ᑑ࿨࠿ࡘẚ㍑ⓗ㧗࠸Ⓨග㔞ࢆ♧ࡍ໬ྜ≀ࡀⓎぢࡉࢀ
ࡓ[1]ࠋࡇࡢ≀㉁ࡣ᭷ᶵᒙࢆྵࡴࡇ࡜࠿ࡽᨺᑕ⥺㜼Ṇ⬟ࡀ㠀ᖖ࡟పࡃࠊ≀ᛶ
ホ౯ࡶ㟁Ꮚ⥺↷ᑕ࡟ࡼࡿࡶࡢࡢࡳ࡟␃ࡲࡗ࡚࠸ࡿࡀࠊྠᵝࡢᵓ㐀ࢆ↓ᶵ໬
ྜ≀࡛ᐇ⌧࡛ࡁࢀࡤ᪤Ꮡࢩࣥࢳ࣮ࣞࢱ࡟ᑐࡍࡿ኱ࡁ࡞ඃ఩ᛶࢆ᭷ࡍࡿࡇ
࡜ࡀᮇᚅ࡛ࡁࡿࠋ⏦ㄳ⪅ࡣࡈࡃ᭱㏆ࠊ㓟⣲࡜◲㯤࣭㓟⣲࡜◉⣲࡞࡝」ᩘࡢ
Fig. 1 Crystal structure of
࢔ࢽ࢜ࣥࢆྵࡴ⣔㸦௨ୗࠊᒙ≧」ྜ࢔ࢽ࢜ࣥ໬ྜ≀࡜࿧⛠㸧࡟࠾࠸࡚ࠊ㉸
(Ag2Se2)(Ba3RE2O5)
ఏᑟᒙࡀᩘ nm ࡢ㠀ᖖ࡟ཌ࠸⤯⦕ᒙ࡛㝸࡚ࡽࢀࡓ໬ྜ≀ࡀ⏕ᡂࡍࡿࡇ࡜
ࢆⓎぢࡋࡓࠋࡑࡇ࡛ࠊࡇࡢ≉␗࡞ᒙ≧ᵓ㐀ࢆ฼⏝ࡋ࡚⤯⦕య㸫༙ᑟయᒙࡀ✚ᒙࡋࡓ໬ྜ≀ࢆྜᡂࡋࠊᒙ≧
↓ᶵࢩࣥࢳ࣮ࣞࢱ࡜ࡋ࡚ࡢྍ⬟ᛶࢆ᥈ࡿࡇ࡜ࢆ௻ᅗࡋࡓࠋ
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1114
200
RE = Sm
Intensity / arb. units
㸱㸬◊✲ᡂᯝ
Ag, Se, Ba, BaO2, RE2O3(RE = Sc, Y, Sm ~ Lu)➼ࡢཎᩱࢆ
໬Ꮫ㔞ㄽẚ࡜࡞ࡿࡼ࠺⛗㔞ࡋࠊᅛ┦཯ᛂἲ࡟࡚ 900 ~ 1100Υ
࡛ 24 h ↝ᡂࡍࡿࡇ࡜࡛ከ⤖ᬗヨᩱࢆྜᡂࡋࡓࠋヨᩱࡣ⢊ᮎ
X ⥺ᅇᢡἲ࡟ࡼࡿ┦ࡢྠᐃ࡜᱁Ꮚᐃᩘࡢホ౯ࠊSQUID ☢᮰
ィ࡟ࡼࡿ☢໬⋡ࡢ ᐃཬࡧᣑᩓ཯ᑕ⋡ ᐃࢆ⾜ࡗࡓࠋ
⣔ ⤫ ⓗ ࡞ ≀ ㉁ ᥈ ⣴ ࡢ ⤖ ᯝ ࠊ Fig. 2 ࡢ ࡼ ࠺ ࡟
(Ag2Se2)(Ba3RE2O5) (RE = Sc, Y, Sm ~ Lu)ࡢ 12 ✀㢮ࡢ᪂つ
໬ྜ≀ࡢྜᡂ࡟ᡂຌࡋࡓࠋࡇࢀࡽࡢ໬ྜ≀ࡣ࠸ࡎࢀࡶ Fig. 1
࡟♧ࡍࡼ࠺࡟ Ag2Se2 ᒙ࡜ Ba3RE2O5 ᒙࡀ✚ᒙࡋࡓᵓ㐀ࢆ᭷
ࡋ࡚࠾ࡾࠊࡇࡢ࠺ࡕᕼᅵ㢮ඖ⣲ࡣ࣌ࣟࣈࢫ࢝࢖ࢺᒙࡢ 6 㓄఩
ࢧ࢖ࢺࢆ༨᭷ࡋ࡚࠸ࡿࠋ༢⣧࣌ࣟࣈࢫ࢝࢖ࢺ㓟໬≀࡟࠾࠸࡚
RE3+࢖࢜ࣥࡀ 6 㓄఩ࢧ࢖ࢺࢆ᏶඲࡟༨ࡵࡿ౛ࡣ࡞࠸ࡀࠊᮏ໬
ྜ≀୰࡛ࡣ࣌ࣟࣈࢫ࢝࢖ࢺᒙࡀ Ag2Se2 ᒙ࡜✚ᒙࡍࡿࡇ࡜࡛ࠊ
107
116
110
㸰㸬◊✲⤒㐣
ᒙ≧」ྜ࢔ࢽ࢜ࣥ໬ྜ≀ࡢ࠺ࡕࠊLaCuSO࣭LaCuSeO ࡣ༙ᑟయ㸫⤯⦕యᒙࡀ➨୍✀㔞Ꮚ஭ᡞ࡜ྠᵝࡢ
ᵓ㐀ࢆᙧᡂࡋࠊບ㉳ᏊⓎගࢆ♧ࡍࡇ࡜ࡀሗ࿌ࡉࢀ࡚࠸ࡿ[2]ࠋ⏦ㄳ⪅ࡽࡣ᭱㏆ࠊ㓟໬≀㸫◉໬≀ᒙࡀ✚ᒙࡋ
ࡓᒙ≧」ྜ࢔ࢽ࢜ࣥ໬ྜ≀࡟࠾࠸࡚ࠊ㉸ఏᑟᒙࡀ㠀ᖖ࡟ཌ࠸⤯⦕యᒙ࡟㝸࡚ࡽࢀࡓᒙ≧໬ྜ≀ࢆከᩘぢฟ
ࡋࡓ[3]ࠋ᭦࡟ࡇࡢ▱ぢࢆ༙ᑟయ㸫⤯⦕యᒙ࡜࡞ࡿ⣔࡟㐺⏝ࡋࡓ⤖ᯝࠊ༙ᑟయ㸫⤯⦕యᒙࡀ✚ᒙࡋࡓᵓ㐀ࢆ
᭷ࡍࡿ᪂≀㉁࡛࠶ࡿ(Cu2S2)(Sr3Sc2O5)ཬࡧ(Cu2S2)(Sr4Sc2O6)ࢆⓎぢࡋࠊࡇࡢ໬ྜ≀ࡀᐊ ࡛ບ㉳ᏊⓎගࢆ
♧ࡍ໬ྜ≀࡛࠶ࡿࡇ࡜ࠊ⤖ᬗᵓ㐀࡟ࡼࡾ≉ᛶࢆไᚚ࡛ࡁࡿࡇ࡜ࢆ᫂ࡽ࠿࡟ࡋࡓ[4]ࠋࡑࡇ࡛௒ᖺᗘࡣࠊྠᵝ
࡟༙ᑟయᒙ㸫⤯⦕యᒙࡀ✚ᒙࡋࡓ໬ྜ≀ࡢ᥈⣴ࢆ㐍ࡵࠊ≉࡟ AgSe ᒙ࡜࣌ࣟࣈࢫ࢝࢖ࢺᆺ㓟໬≀ᒙࡀ✚ᒙ
ࡋࡓ໬ྜ≀ࢆ᥈⣴ࡋࠊⓎぢࡋࡓ໬ྜ≀࡟ࡘ࠸࡚ࡣ☢ᛶࡸගᏛ
≉ᛶࡢホ౯ࢆ⾜ࡗࡓࠋ
RE = Gd
RE = Y
RE = Lu
RE = Sc
2T / deg.(Cu-KD)
Fig. 2 Powder XRD patterns of
(Ag2Se2)(Ba3RE2O5).
12 㓄఩ࡢ㔠ᒓࢧ࢖ࢺ࡟࢖༙࢜ࣥᚄࡢ኱ࡁ࠸ Ba2+ࢆ⏝࠸ࡿࡇ࡜ࡀ࡛ࡁࡿࡓࡵ᏶඲࡞༨᭷ࡀྍ⬟࡜࡞ࡗ࡚࠸
ࡿࠋࡲࡓ RE ࡢ✀㢮࡟ࡼࡾࠊ᱁Ꮚᐃᩘࡣ a = 4.22, c = 28.66 Å(RE = Sc)࠿ࡽ a = 4.49, c = 28.53 Å(RE = Sm)
ࡲ࡛ኚ໬ࡋࡓࠋࡇࢀࡽࡢ໬ྜ≀ࡢ☢໬⋡ࢆ ᐃࡋࡓ࡜ࡇࢁࠊ࠸ࡎࢀࡢ໬ྜ≀ࡶᣲືࡣᖖ☢ᛶⓗ࡛ࠊRE3+ࡢ
✀㢮࡟ࡼࡗ࡚☢໬ࡢ⤯ᑐ್ࡀኚ໬ࡋࠊ㍍ᕼᅵ㢮࠿ࡽ୰ᕼᅵ㢮࡛☢໬ࡀቑ኱ࠊ㔜ᕼᅵ㢮࡛ࡣῶᑡࡍࡿࡇ࡜ࡀ
ศ࠿ࡗࡓ(Fig.3)ࠋAgSe ᒙࡣ☢໬࡟࡯࡜ࢇ࡝ᙳ㡪ࡋ࡞࠸ࡓࡵࠊ࣌ࣟࣈࢫ࢝࢖ࢺᒙࡢ RE3+ࡢ☢໬ࡢࡳࡀほ ࡉࢀ࡚࠸ࡿࡇ࡜࡟࡞ࡿࡀࠊࡇࢀࡣᐃᛶⓗ࡟ࡣᕼᅵ㢮ࡢ඲ゅ㐠ື㔞㔞Ꮚᩘ J ࡟౫Ꮡࡋ࡚࠸ࡿ࡜⪃࠼ࡽࢀࡿࠋ
(Ag2Se2)(Ba3Lu2O5)ࡢᣑᩓ཯ᑕ⋡ ᐃ࠿ࡽࠊࡇࡢ໬ྜ≀ࡣࣂࣥࢻࢠࣕࢵࣉࡀ⣙ 2.5 eV ࡢ┤᥋㑄⛣ᆺ༙ᑟ
య࡛࠶ࡿࡇ࡜ࡀศ࠿ࡗࡓࠋࡇࢀࡣ Ag2Se ࡢࣂࣥࢻࢠࣕࢵࣉ࡜ࡋ࡚ሗ࿌ࡉࢀ࡚࠸ࡿ್㸦Eg = 0.15 eV[2]㸧ࡼ
ࡾࡶ࠿࡞ࡾ኱ࡁ࠸ࠋࡇࢀࡽࡢ໬ྜ≀࡟ࡘ࠸࡚ࠊᘬࡁ⥆ࡁගᏛ≉ᛶࡢホ౯ࢆ⾜ࡗ࡚࠸ࡃணᐃ࡛࠶ࡿࠋ
2
4
0.2
3
FC
0.1
2
ZFC
1
0
0
0
100
0
100
200
T / K H = 1000 Oe
T/K
200
300
1
0
0
RE = Ho ~ Lu
Ho
Er
Tm
Yb
Lu
0.3
M / emu mol-1Oe-1
3
Dy
Tb
Gd
Eu
Sm
Y
5
0.3
M / emu mol-1Oe-1
M / emu mol-1Oe-1
4
RE = Y, Sm ~ Dy
M / emu mol-1Oe-1
5
0.2
FC
ZFC
0.1
0
0
100
100
T/K
T/K
200
Fig. 3 Temperature dependence of magnetization for (Ag2Se2)(Ba3RE2O5)
References
[1] K. Shibuya et al., Jpn. J. Appl. Phys. 43 (2004) L1333-L1336
[2] K. Ueda et al., Appl. Phys. Lett. 78 (2001) 2333
[3] H. Ogino et al., Appl. Phys. Lett. 97 (2010) 072506
[4] H. Ogino et al., Appl. Phys. Lett. 101 (2012) 191901
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