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Title
高性能磁気熱変換材料の開発を目指して
Author(s)
戎, 修二; 阿波加, 淳司; 藤, 耕一郎
Citation
室蘭工業大学紀要 Vol.63, pp.33-36, 2014
Issue Date
2014-03-18
URL
http://hdl.handle.net/10258/2827
Rights
- 33 - ᐊᕤ⣖せ➨63 ྕ㸦2013㸧 33㹼36
- 33 -
㧗ᛶ⬟☢Ẽ⇕ኚᮦᩱࡢ㛤Ⓨࢆ┠ᣦࡋ࡚
ᡁ
ಟ
*1, *2㸪㜿Ἴຍ
῟ྖ
*2㸪⸨
⪔୍㑻
*3Aiming for High Performance Magnetocaloric Materials
Shuji EBISU
*1, *2, Junji AWAKA
*2, and Koichiro FUJI
*3㸦ཎ✏ཷ᪥ ᖹᡂ
25 ᖺ 9 ᭶ 30 ᪥ ㄽᩥཷ⌮᪥ ᖹᡂ 26 ᖺ 1 ᭶ 24 ᪥㸧
Abstract
Specific heat measurements on single crystals of rare-earth sesquisulfide α-R2S3 (R = Pr, Nd, Sm, Gd,
Tb and Dy) have been performed under applied magnetic fields in the range between 0 and 5 T. Any compound shows one or two peak(s) at magnetic transition temperature(s) in the temperature dependence of the specific heat. The values of the specific heat below the temperature of 10 K for
α-Gd2S3 are considerably larger than those for other α-R2S3 and comparable to those for other cold
storage materials. Application of magnetic field perpendicular to the b-axis of α-Dy2S3 single crystal
shifts the antiferromagnetic transition temperature TN1 toward higher temperature and decreases
magnetic entropy. In this case, adiabatic demagnetization after isothermal magnetization at 12 K with a magnetic field of 5 T yields a magnetic refrigeration effect of Tad= 5.8 K.
Keywords : Rare-earth sesquisulfide, Magnetocaloric effect, Magnetic refrigeration, Cold storage material, Specific heat
1 ࡣࡌࡵ ᐊ⹒ᕤᴗᏛ➨㸰ᮇ୰ᮇ┠ᶆᮇ㛫࠾ࡅࡿ㔜Ⅼ ◊✲ࣉࣟࢪ࢙ࢡࢺ㸸ࠕᕼᅵ㢮㛵㐃ࡋࡓ⏕ྍ⬟࢚ ࢿࣝࢠ࣮ᮦᩱ⛉Ꮫ࠾ࡼࡧࢧࢫࢸࢼࣈࣝᮦᩱ㛤 Ⓨࠖ䠄␎⛠㸸ᕼᅵ㢮ࣉࣟࢪ࢙ࢡࢺ䠅ࡀᖹᡂ22 ᖺⓎ ㊊ࡋࠊᙜึ❧ࡕୖࡀࡗࡓ㸱ࢱࢫࢡ◊✲ࡢ࠺ࡕࡢ㸯 ࡘࡀࠊ䛂㧗ᛶ⬟☢Ẽ⇕ኚᮦᩱࡢ㛤Ⓨ䛃ࢱࢫࢡ࡛࠶ ࡿࠋ ࡼࡃ▱ࡽࢀࡿ☢ᛶᮦᩱࡢᛂ⏝ࡣࠊ☢ሙࡼࡿᛂ ⟅࡛࠶ࡿ☢ࢆ⏝ࡍࡿࡶࡢࡸࠊ㟁Ẽ☢Ẽࡢ┦ స⏝ࢆ⏝ࡍࡿࡶࡢࡀ༙࡛࠶ࡿࠋ୍᪉࡛ࠊእ 㒊☢ሙࡣ☢ᛶయෆ㒊ࡢ☢Ẽ࣮࣓ࣔࣥࢺస⏝ࡋࠊ ☢Ẽ࢚ࣥࢺࣟࣆ࣮ኚࢆࡋ࡚⇕ࡢ⛣ືࡶ㛵㐃 ࡍࡿࠋࡇࡢࡼ࠺☢Ẽ⇕㔞ࡀ⤖ྜࡍࡿ⌧㇟ࢆ☢ Ẽ⇕㔞ຠᯝ䠄MCE; Magnetocaloric Effect䠅࠸࠺ࠋ *1 ᐊ⹒ᕤᴗᏛ ࡋࡃࡳሗ⣔㡿ᇦ *2 ᐊ⹒ᕤᴗᏛ ⎔ቃㄪᮦᩱᕤᏛ◊✲ࢭࣥࢱ࣮ *3 ᐊ⹒ᕤᴗᏛ ᛂ⏝⌮Ꮫ⣔ᑓᨷ ☢ሙࡣ☢࢚ࢿࣝࢠ࣮ⓗඹᙺࡢ㛵ಀ࠶ࡾࠊ ࡇࢀࡣ⇕ຊᏛⓗẼయࡢᅽຊ࣭య✚ࡢ㛵ಀྠ➼ ࡛࠶ࡿࠋࡋࡓࡀࡗ࡚ࠊ୍⯡ࡢ෭ᶵࡀẼయࡢᅽ⦰࣭ ⭾ᙇࡼࡾ෭༷ຠᯝࢆᚓࡿࡢᑐᛂࡋ࡚ࠊ࠶ࡿ✀ ࡢ☢ᛶయ☢ሙࢆບ☢࣭ᾘ☢ࡍࡿࡇࡼࡾ෭༷ ࡍࡿࡇࡀྍ⬟࡛࠶ࡾࠊࡇࢀࢆ☢Ẽ෭䠄Magnetic Refrigeration䠅࠸࠺ࠋࡲࡓࠊMCE ࡼࡾ୍⯡ⓗ ☢ᛶయࡣ☢Ẽ┦㌿⛣Ⅼ䠄 ᗘ䠅࠾࠸࡚ẚ⇕ࡀඛ 㗦࡞ᴟࢆ♧ࡍࡢ࡛ࠊ☢Ẽ┦㌿⛣Ⅼࢆ㊬ࡄ ᗘୖ ᪼ࢆࡶࡓࡽࡍࡓࡵࡣ㠀ᖖࡁ࡞⇕㔞ࡀᚲせ ࡞ࡿࠋࡇࡢຠᯝࡀࡁ࠸≀㉁ࡣ䇾෭䇿ࢆ࠼ࡿ෭ ᮦࡋ࡚⏝࡛ࡁࠊ෭ᶵሸࡍࡿ➼ࡋ࡚෭༷ ຠ⋡ࢆྥୖࡉࡏࡿࡇࡀ࡛ࡁࡿࠋᮏࢱࢫࢡ◊✲࡛ ࡣ☢Ẽ෭ᮦࡸ෭ᮦࡢ㛤Ⓨࢆᣦྥࡋ࡚࠸ࡿࠋ 2 ⫼ᬒ◊✲ᣦ㔪 ෭ᮦࡋ࡚ࡣࠊ☢Ẽ㌿⛣➼ࡢ┦㌿⛣కࡗ࡚ ࡁ࡞ẚ⇕ࣆ࣮ࢡࢆ⏕ࡌࡿࡶࡢࡀ㐺ࡋ࡚࠾ࡾࠊ 室工大紀要第63 号(2013) 33~36
特 集
- 34 - 㧗ᛶ⬟☢Ẽ⇕ኚᮦᩱࡢ㛤Ⓨࢆ┠ᣦࡋ࡚
- 35 -
ࡿ㢮᥎ࡉࢀࡿࠋ୍᪉࡛୰ᛶᏊᅇᢡᐇ㦂(20)ࡸ࢚ࣥ ࢺࣟࣆ࣮ኚ(21)ࡽ☜ㄆࡉࢀࡿࡼ࠺ࠊα-Gd2S3ࡣ 㸯ẁࡢ㌿⛣࡛Gd1, Gd2 ࡀᙉ☢ᛶ⛛ᗎࡍࡿࠋ 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0 5 10 15 20C
/ J
K
-1c
m
-3T / K
-
R
2S
3 R = Gd Tb Dy Pr Nd Sm ᅗ1 α-R2S3༢⤖ᬗࡢẚ⇕ࡢ ᗘ౫Ꮡᛶ ᅗ1 ࡽ᫂ࡽ࡞ࡼ࠺ࠊα-Gd2S3ࡢẚ⇕ࣆ࣮ࢡ ࡣࢆᅽಽࡋ࡚ࡁ࠸ࠋከ㔜㡯ᇶᗏ≧ែ࠾࠸࡚ Gd3+ࡢゅ㐠ື㔞J ࡣ 7/2 ẚ㍑ⓗࡁ࠸ࡀࠊTb3+ (J = 6)ࡸ Dy3+ (J = 15/2)ࡢ᪉ࡀࡉࡽࡁ࠸ࠋࡋࡋࠊ Gd ⣔௨እࡢ J ከ㔜㡯ࡣ⤖ᬗሙࡼࡗ࡚࢚ࢿࣝࢠ࣮ ‽ศࡋࠊᇶᗏ㡯ࡢከ㔜ᗘࡣపࡃ࡞ࡿࠋ୍᪉Gd ⣔࡛ࡣ㌶㐨ゅ㐠ື㔞ࡀ 0 ࡛࠶ࡿࡓࡵ⤖ᬗሙࡢᙳ 㡪ࢆཷࡅࡎࠊᇶᗏࡀࢫࣆࣥ 8 㔜㡯࡛࠶ࡿࡇ㉳ ᅉࡋ࡚ẚ⇕ࣆ࣮ࢡࡀࡁࡃ࡞ࡗ࡚࠸ࡿࠋࡉࡽGd ⣔࡛ࡣ㌿⛣ࡼࡾప ࡛ẚ⇕ࡀ⫪ࢆࡶࡗ࡚࠸ࡿࠋࡇ ࢀࡣᗄఱᏛⓗࣇࣛࢫࢺ࣮ࣞࢩࣙࣥࢆ᭷ࡍࡿGd2 ࡢ ⛛ᗎࡀGd1 ࡢ⮬Ⓨ⛛ᗎࡼࡿศᏊሙࡢᙳ㡪࡛ࠊ ᗘపୗకࡗ࡚ᚎࠎ㐍⾜ࡋ࡚࠸ࡿࡇ㉳ᅉ ࡋ࡚࠸ࡿ⪃࠼ࡽࢀࡿ(21)ࠋࡇࡢࡓࡵࠊα-Gd2S3ࡣᗈ ࠸ ᗘ⠊ᅖ࡛ࡁ࡞ẚ⇕ࢆࡶࡘࠋ༢య✚࠶ࡓࡾ ࡢẚ⇕ࡢ್᭱0.63 J K-1cm-3 (T = 9.8 K)ࡣ෭ᮦ ࡋ ࡚ ᮇ ᚅ ࡉ ࢀ ࡚ ࠸ ࡿ Gd2O2S (GOS) ࡢ 1.1 J K-1cm-3 (T = 5.2 K)ࡼࡾࡶప࠸ࡀࠊᐇ⏝ࡉࢀ࡚࠸ ࡿEr3Ni ࡸ HoCu2ࢆ㥙ࡋ࡚࠸ࡿࠋHoCu2ࡀࢲࣈࣝ ࣆ࣮ࢡ࡛ࡼ࠸ᛶ⬟ࢆ♧ࡍ ᗘᇦ࡛ࡣ್ࡀୗᅇࡿࡀ α-Gd2S3ࡢᖜᗈࡢ⫪ࡣⰋ࠸≉ᚩ࡛࠶ࡿࠋࡲࡓࠊࡼࡾ ࡁ࡞ẚ⇕ࣆ࣮ࢡࢆࡶࡘᙉ☢ᛶయ ErNi ࡛ࡣ࡞ࡃ Er3Ni ࡀᐇ⏝ࡉࢀ࡚࠸ࡿ⌮⏤ࡣᚋ⪅ࡀᙉ☢ᛶయ ࡛࠶ࡾ㉸ఏᑟ࣐ࢢࢿࢵࢺࡽࡢ₃ࢀ☢ሙࡢᙳ㡪ࢆ ཷࡅࡃ࠸ࡓࡵ࡛࠶ࡿࡀࠊࡑࡢⅬ࡛ࡶᙉ☢ᛶయ α-Gd2S3ࡣ㐺ࡋ࡚࠸ࡿࠋࡁ࡞ẚ⇕ࢆ♧ࡍ ᗘᇦࡀ ␗࡞ࡿ෭ᮦࢆ⤌ࡳྜࢃࡏ࡚෭ᶵ➼ሸࡍࡿ ࡇࡼࡾ㧗ຠ⋡ࡀᅗࢀࡿࡓࡵࠊࢲࣈࣝࣆ࣮ࢡ ࢆ♧ࡍࡢ α-R2S3ࡶྵࡵࠊẚ⇕≉ᛶⓗࡣ෭ᮦ ࡋ࡚ࡢྍ⬟ᛶࡣ࠶ࡿࠋࡋࡋᐇᮦᩱࡋ࡚ࡣࠊ ⌫≧ከ⤖ᬗヨᩱࡢసᡂྍ⬟ᛶࠊࡑࡢሙྜࡢẚ⇕≉ ᛶࡸ⇕ఏᑟ⋡ࠊ⇕ࢧࢡࣝࢆྵࡵࡓ⪏⎔ቃᛶࠊࢥ ࢫࢺ➼ࡢ᳨ウࡍࡁㄢ㢟ࡣᩘከࡃᏑᅾࡍࡿࠋ 4.2 ☢ሙ୰ẚ⇕ ᅗ2 α-Dy2S3ࡢb ㍈ᑐࡋ࡚ᆶ┤☢ሙࢆ༳ຍ ࡋࡓሙྜࡢ(a)☢Ẽẚ⇕ Cm࠾ࡼࡧ(b)☢Ẽ࢚ࣥࢺࣟ ࣆ࣮Smࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋ㧗 ഃ㌿⛣ⅬTN1ࡀ☢ ሙ༳ຍࡼࡾ㢧ⴭ㧗 ഃࢩࣇࢺࡋࠊప ഃ㌿ ⛣ࡀᾘኻࡋ࡚࠸ࡿᵝᏊࡀࢃࡿࠋᙉ☢ᛶ㌿⛣ࡀ☢ ሙ༳ຍࡼࡾ㧗 ഃࢩࣇࢺࡍࡿࡇࡣࡼࡃぢࡽ ࢀࡿࡇ࡛ࠊࡇࡢഴྥࡣ☢Ẽ෭ࡗ࡚ࡣ㒔ྜ ࡀⰋ࠸ࠋࡋࡋࠊᙉ☢ᛶ㌿⛣ࡣ☢ሙ༳ຍࡼࡾ ప ഃࢩࣇࢺࡍࡿࡢࡀ୍⯡ⓗ࡛࠶ࡿࠋ⌧ࡢ α-R2S3࡛ࡣ☢ሙࡢ༳ຍ᪉ྥࡼࡽࡎ㌿⛣ࡢప ࢩ ࣇࢺࡀほ ࡉࢀࡿࡋࠊα-Dy2S3ࡢb ㍈ᖹ⾜࡞☢ሙ ༳ຍ࡛ࡶྠᵝࡢഴྥࡀぢࡽࢀࡿࠋα-Dy2S3ࡣ㏲ḟ ᙉ☢ᛶ㌿⛣Ⅼࡢ㛫TN1-TN2࡛✀ࠎࡢ≉␗࡞⌧㇟ࢆ♧ ࡍ(13)(14)ࡀࠊb ㍈ᆶ┤࡞☢ሙᑐࡍࡿᛂ⟅ࡀ㗦ᩄ ࡛࠶ࡿࡇࡶࡑࡢ୍ࡘ࡛࠶ࡿࠋDy1 ࡀᙉ☢ᛶ⛛ ᗎࡍࡿࡇࡼࡾࠊDy2 ࡢ☢ሙᑐࡍࡿᛂ⟅ᛶ ࡀࡼࡃ࡞ࡾࠊ☢ሙࡼࡿࢮ࣮࣐࢚ࣥࢿࣝࢠ࣮పୗ ࡀ࠶ࡿࡓࡵࠊTN1ࡀ㧗 ࢩࣇࢺࡍࡿ⪃࠼ࡽࢀࡿࠋ 0 10 20 30 40 50-
Dy
2S
3C
m/ J
K
-1mol
-1Hԋb
0 T 1 T2 T 3 T 5 T(a)
0 5 10 15 20 0 5 10 15 20-
Dy
2S
3S
m/ J
K
-1mol
-1Hԋb
0 T1 T 2 T 5 T 3 T(b)
T / K
ᅗ2 α-R2S3༢⤖ᬗࡢ☢ሙ୰࡛ࡢ(a)☢Ẽẚ⇕ (b)☢Ẽ࢚ࣥࢺࣟࣆ࣮ࡢ ᗘ౫Ꮡᛶ TN1ࡢ㧗 ࢩࣇࢺప ഃTN2࡛ࡢ㌿⛣ࡢᾘኻࡀ ࡶຠ࠸࡚ࠊᅗ2(b)♧ࡍࡼ࠺ Cm/T ࢆ ᐃ᭱ ప ᗘ 0.4 K ࡽ ᗘ࡛✚ศࡋࡓ☢Ẽ࢚ࣥࢺࣟࣆ ࣮ࡣ☢ሙ༳ຍࡼࡾῶᑡࡋ࡚࠸ࡿ㸦|Sm| < 0㸧ࠋບ ☢Ọஂ☢▼ࡢ⏝ࢆᐃࡋࡓ☢ሙ 2 T ࡛ࡢ|Sm| ᡁ ಟ㸪㜿Ἴຍ ῟㸪⸨ ⪔୍㑻- 34 -
ࡁ࡞ゅ㐠ື㔞㔞Ꮚᩘࢆࡶࡘ㔜ᕼᅵ㢮ඖ⣲ࢆྵࡴ ≀㉁ࡀೃ⿵࡞ࡾᚓࡿࠋ10 K ⛬ᗘ࡛☢Ẽ┦㌿⛣ࢆ ࡶࡘα ኚែᕼᅵ㢮୕◲≀ α-R2S3䠄R㸸ᕼᅵ㢮ඖ ⣲䠅ࡸᕼᅵ㢮࣍࢘≀╔┠ࡋࠊ⣔⤫ⓗ࡞ẚ⇕ ᐃ ࢆ⾜ࡗࡓࠋ ☢Ẽ෭ᮦ㛵ࡋ࡚ࡣືస ᗘࢆ⪃៖ࡍࡿࡇ ࡀ㔜せ࡛࠶ࡾࠊᮏࢱࢫࢡ࣓ࣥࣂ࣮ࡀࡶࡘࢩ࣮ࢬࢆ ㋃ࡲ࠼ࠊ(1)ᐊ ᇦࠊ(2)ᾮయ❅⣲ ᗘᇦࠊ(3)10 K ᗘᇦ࡛ࡢ᳨ウࢆ⾜ࡗࡓࠋ (1)ᐊ ᇦ㸸ᐊ ᇦ࠾ࡅࡿ☢Ẽ෭ᶵࡣࠊࣇࣟ ࣥ࢞ࢫࡼࡿ࢜ࢰࣥᒙࡢ◚ቯࠊ௦᭰ࣇࣟࣥ࢞ࢫ ࡼࡿᆅ⌫ ᬮࡢಁ㐍ࢆ㜼ࡴࡶࡢࡋ࡚ᮇᚅࡉࢀ ࡚࠸ࡿࠋࡇࡢ ᗘᇦ࠾࠸࡚ࡣࠊᐊ ㏆ᙉ☢ ᛶ㌿⛣ ᗘ䠄࣮࢟ࣗࣜⅬ䠅TC ࢆࡶࡘᕼᅵ㢮ඖ⣲ Gd ࡀึᮇࡢ㡭ࡼࡾὀ┠ࡉࢀ࡚ᐇᶵ࡛ࡶホ౯ࡉࢀࠊᐊ ☢Ẽ෭ࢩࢫࢸ࣒ࡢⓎᒎࡁ࡞ᙺࢆᢸࡗ࡚ ࡁࡓࠋ㧗ຠ⋡࣭㧗ᛶ⬟ࡢࡓࡵ✀ࠎࡢGd ྜ≀ࠊ ࠼ࡤGd5Si2Ge2(1)(2)ࡸࠊ㠀☢ᛶࡢᕼᅵ㢮ඖ⣲La ࢆ ྵࡴ La(Fe1-xSix)13Hy(3)(4)࠶ࡿ࠸ࡣᕼᅵ㢮ඖ⣲ࢆྵࡲ ࡞࠸Mn(As1-xSbx)(5)ࡸ MnFe(P1-xAsx)(6)࡞ࡀὀ┠ࢆ 㞟ࡵ࡚┒ࢇ◊✲ࡉࢀࠊᐇ⏝㏆࡙࠸࡚࠸ࡿࠋ ᕼᅵ㢮ඖ⣲ࢆ⏝࠸ࡎࡶࠊ୍ḟ┦㌿⛣ࡢࡁ࡞࢚ ࣥࢺࣟࣆ࣮ኚࢆ⏝ࡍࢀࡤ㧗ᛶ⬟ࡢ෭ᶵࢆᐇ ⌧࡛ࡁࡿྍ⬟ᛶࡀ♧ࡉࢀࠊ⌧ᅾࡢ୍ࡘࡢ₻ὶ࡞ ࡾࡘࡘ࠶ࡿࠋᚋⓎࡢᮏࢱࢫࢡ࡛ࡣࠊ⌧᭷ࡢࢩ࣮ࢬ ࡛࠶ࡿᐊ ᇦ࡛␗ᖖࡁ࡞⇕⭾ᙇ⋡䠄ẚ⇕ᐦ ᥋㛵㐃ࡍࡿ≀⌮㔞䠅ࢆ♧ࡍᕼᅵ㢮ඖ⣲ Ce ࢆྵࡴ ᵓ㐀つ๎⣔ྜ㔠(7)-(9)ࡢᇶ♏◊✲ࢆ㐍ࡵࡓࠋ (2)ᾮయ❅⣲ ᗘᇦ㸸㖡㓟≀㧗 ㉸ఏᑟయࢆ⏝ ࠸ࡓ✀ࠎࡢࢹࣂࢫࡀ⏝ࡉࢀ࡚ࡁ࡚࠸ࡿࡀࠊࡇ ࡢᏳ ᐃືసࡢ ࡓࡵࡣ ᾮయ❅ ⣲ ᗘ 䠄❅⣲ࡢ Ἓ Ⅼ㸸77 K䠅ࡼࡾᩘ༑ K ప࠸ ᗘࡀᚲせ࡛࠶ࡾࠊࡇࢀ ࢆᐇ⌧ࡍࡿపࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢᑠᆺ☢Ẽ ෭ᶵࡀᮃࡲࢀࡿࠋࡑࡢᙧᡂࣃࢱ࣮ࣥࡽࢫࢺࣛ ࣉ⛛ᗎࡤࢀࡿ㟁Ⲵ⛛ᗎࢆ㉸ఏᑟ㌿⛣కࡗ ࡚㉳ࡇࡍ㖡㓟≀㧗 ㉸ఏᑟయ㛵ࡍࡿ◊✲ࢩ࣮ ࢬ(10)ࡀ࠶ࡾࠊࡇࡢ㌿⛣క࠺࢚ࣥࢺࣟࣆ࣮ኚࢆ ྵࡵࡓᇶ♏◊✲ྲྀࡾ⤌ࢇࡔࠋ (3)10 K ᗘᇦ㸸ࢡ࣮࢚ࣜࣥࢿࣝࢠ࣮ࡋ࡚ᮇᚅ ࡉࢀࡿỈ⣲⇞ᩱࢆ㈓ⶶ࣭㍺㏦ࡍࡿࡓࡵࡣỈ⣲ࢆ ᾮࡍࡿࡢࡀຠ⋡ⓗ࡛࠶ࡾࠊ10 K ⛬ᗘࡢ ᗘࢆᐇ ⌧ࡍࡿᚲせࡀ࠶ࡿࠋᾮయ࣒࣊ࣜ࢘ࢆ⏝ࡍࢀࡤࠊ ᾐₕࡍࡿࡔࡅ࡛࣒࣊ࣜ࢘ࡢἛⅬ 4.2 K ㏆ࡃࡲ࡛෭ ༷ࡍࡿࡇࡀྍ⬟࡛࠶ࡿࡀࠊ࣒࣊ࣜ࢘ࡣᕼᑡ㈨※ ࡛࠶ࡾࠊ♫ໃࡼࡗ࡚ࡣ☜ಖࡀࡁࢃࡵ࡚ᅔ㞴 ࡶ࡞ࡾᚓࡿࠋࡇࡢࡓࡵࠊ࣒࣊ࣜ࢘ࣇ࣮࡛ࣜྠ➼ ࡢ ᗘࢆᚓࡿᑠᆺ࣭పࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢ ☢Ẽ෭ᶵࡢ㛤Ⓨࡀᮇᚅࡉࢀ࡚࠸ࡿࠋࡇࢀࡲ࡛ⴭ ⪅ࡣ๓㏙ࡢα-R2S3ࡀ10 K ㏆ࡢ ᗘ࡛㏲ḟ☢Ẽ┦ ㌿⛣ࢆ㉳ࡇࡋࠊࡑࢀకࡗ࡚✀ࠎࡢ≉␗࡞≀ᛶᛂ ⟅ࢆ♧ࡍࡇࢆぢฟࡋ࡚ࡁࡓ(11)-(18)ࠋࡇࡢ◊✲ࢩ࣮ ࢬࢆάࡋࠊα-R2S3ࡢ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࢆ ᥈ࡗࡓࠋ α-R2S3ࡣᩳ᪉ᬗ⣔⤖ᬗᵓ㐀䠄✵㛫⩌㸸Pnma䠅୰ ⤖ᬗᏛⓗ⊂❧࡞ࡘࡢᕼᅵ㢮ࢧࢺ㸦R1, R2㸧ࢆ ᭷ࡋ࡚࠸ࡿ(11)ࠋࡇࢀࡲ࡛ᚓࡽࢀࡓᐇ㦂ᐇࢆ⥲ ᣓࡍࡿࠊR1 ࡣ b ㍈᪉ྥ୍ḟඖ㙐ෆ࡛ᙉ☢ᛶⓗࠊa ㍈᪉ྥࢪࢢࢨࢢ㙐ෆ࡛ᙉ☢ᛶⓗ⛛ᗎࡍࡿഴ ྥࡀᙉࡃࠊR1 ᙅࡃ⤖ྜࡋࡓ R2 ࡣ㊥㞳ⓗࡣࡸ ࡸ㐲࠸㞄᥋ R2 」㞧స⏝ࡋྜ࠺⪃ᐹࡉࢀࡿࠋ ࡇࡢR1-R2, R2-R2 㛫ࡢ」㞧࡞☢Ẽⓗ┦స⏝ࡀ➇ ྜࡋࠊ ᗘࡸ☢ሙᑐࡋ࡚࣐ࢡࣟ≀ᛶࡀ≉␗࡞ᛂ ⟅ࢆ♧ࡍ⪃࠼ࡽࢀࡿࠋᮏሗ࿌࡛ࡣࠊα-R2S3ࡢ↓☢ ሙୗ࠾ࡼࡧ☢ሙ୰࡛ࡢẚ⇕ࡢ ᐃ⤖ᯝ෭ᮦ࣭ ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࡘ࠸࡚㆟ㄽࡍࡿࠋ 3 ᐇ㦂 ᕷ㈍ࡢᕼᅵ㢮㓟≀ࢆ CS2Ẽὶ୰࡛ຍ⇕ࡍࡿࡇ ࡛ α-R2S3⢊ᮎヨᩱࢆᚓࠊࡇࢀࢆཎᩱࡋ࡚ࣚ࢘ ⣲ࢆ㍺㏦ࡋࡓẼ┦Ꮫ㍺㏦ἲࡼࡾ༢⤖ᬗヨ ᩱࢆ⫱ᡂࡋࡓࠋẚ⇕ࡣ⡿ᅜQuantum Design ♫〇≀ ⌮≉ᛶ ᐃࢩࢫࢸ࣒ PPMS ࢆ⏝ࡋࠊ5 T ࡲ࡛ࡢ ✀ࠎࡢ☢ሙ୰࡛⦆ἲࡼࡾ ᐃࡋࡓࠋ 4 ⤖ᯝ⪃ᐹ 4.1 ↓☢ሙୗẚ⇕ ᅗ1 α-R2S3䠄R㸸Pr, Nd, Sm, Gd, Tb, Dy䠅༢⤖ᬗ ࡢ↓☢ሙୗ࡛ࡢẚ⇕ࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋGd, Pr ⣔௨እࡢ α-R2S3࡛ࡣ㸰ẁࡢ☢Ẽ┦㌿⛣క࠺ඛ㗦 ࡞ࣆ࣮ࢡࡀ☜ㄆࡉࢀࡿࠋTb, Dy ⣔㛵ࡋ࡚ࡣ☢ ᐃ(12)(14)ࡸ୰ᛶᏊᅇᢡᐇ㦂(19)ࡢ⤖ᯝࡽࠊ㸰ẁࡢ ᙉ☢ᛶ㌿⛣ࡀ㉳ࡁ࡚࠸ࡿ⪃࠼ࡽࢀࡿࠋNd ⣔ࡢ ᑡ࡞ࡃࡶ㧗 ഃࣆ࣮ࢡࡣࡸࡣࡾᙉ☢ᛶ㌿⛣ ࡼࡿࡶࡢ࡛࠶ࡿࠋࡇࢀᑐࡋ࡚Sm ⣔࡛ࡢ㌿⛣ࡣ㸰 ẁࡢ䠄ᙅ䠅ᙉ☢ᛶ㌿⛣࡛࠶ࡿ⪃࠼ࡽࢀࡿ(16)ࠋPr ⣔ ࡛ࡣ᭱ప ࡢ0.36 K ࡲ࡛➨ࡢࣆ࣮ࢡࡣ☜ㄆࡉࢀ ࡞࠸ࡶࡢࡢࠊప ࡛ࡢ᫂ࡽ࡞ẚ⇕ࡢୖ᪼ࡽ㏲ ḟⓗ┦㌿⛣ࡀ࠶ࡿ⪃࠼ࡽࢀࡿࠋα-Tb2S3࡛ࡢ☢Ẽ ᵓ㐀ゎᯒ⤖ᯝ(19)ࡢᐇ㦂ᐇࡽࠊࡇࢀࡽࡢ㧗 ഃ㌿⛣࡛ࡣ R1ࠊప ഃ㌿⛣࡛ࡣ R2 ࡀ⛛ᗎࡍ ᡁ ಟ㸪㜿Ἴຍ ῟㸪⸨ ⪔୍㑻- 34 -
ࡁ࡞ゅ㐠ື㔞㔞Ꮚᩘࢆࡶࡘ㔜ᕼᅵ㢮ඖ⣲ࢆྵࡴ ≀㉁ࡀೃ⿵࡞ࡾᚓࡿࠋ10 K ⛬ᗘ࡛☢Ẽ┦㌿⛣ࢆ ࡶࡘα ኚែᕼᅵ㢮୕◲≀ α-R2S3䠄R㸸ᕼᅵ㢮ඖ ⣲䠅ࡸᕼᅵ㢮࣍࢘≀╔┠ࡋࠊ⣔⤫ⓗ࡞ẚ⇕ ᐃ ࢆ⾜ࡗࡓࠋ ☢Ẽ෭ᮦ㛵ࡋ࡚ࡣືస ᗘࢆ⪃៖ࡍࡿࡇ ࡀ㔜せ࡛࠶ࡾࠊᮏࢱࢫࢡ࣓ࣥࣂ࣮ࡀࡶࡘࢩ࣮ࢬࢆ ㋃ࡲ࠼ࠊ(1)ᐊ ᇦࠊ(2)ᾮయ❅⣲ ᗘᇦࠊ(3)10 K ᗘᇦ࡛ࡢ᳨ウࢆ⾜ࡗࡓࠋ (1)ᐊ ᇦ㸸ᐊ ᇦ࠾ࡅࡿ☢Ẽ෭ᶵࡣࠊࣇࣟ ࣥ࢞ࢫࡼࡿ࢜ࢰࣥᒙࡢ◚ቯࠊ௦᭰ࣇࣟࣥ࢞ࢫ ࡼࡿᆅ⌫ ᬮࡢಁ㐍ࢆ㜼ࡴࡶࡢࡋ࡚ᮇᚅࡉࢀ ࡚࠸ࡿࠋࡇࡢ ᗘᇦ࠾࠸࡚ࡣࠊᐊ ㏆ᙉ☢ ᛶ㌿⛣ ᗘ䠄࣮࢟ࣗࣜⅬ䠅TC ࢆࡶࡘᕼᅵ㢮ඖ⣲ Gd ࡀึᮇࡢ㡭ࡼࡾὀ┠ࡉࢀ࡚ᐇᶵ࡛ࡶホ౯ࡉࢀࠊᐊ ☢Ẽ෭ࢩࢫࢸ࣒ࡢⓎᒎࡁ࡞ᙺࢆᢸࡗ࡚ ࡁࡓࠋ㧗ຠ⋡࣭㧗ᛶ⬟ࡢࡓࡵ✀ࠎࡢGd ྜ≀ࠊ ࠼ࡤGd5Si2Ge2(1)(2)ࡸࠊ㠀☢ᛶࡢᕼᅵ㢮ඖ⣲La ࢆ ྵࡴ La(Fe1-xSix)13Hy(3)(4)࠶ࡿ࠸ࡣᕼᅵ㢮ඖ⣲ࢆྵࡲ ࡞࠸Mn(As1-xSbx)(5)ࡸ MnFe(P1-xAsx)(6)࡞ࡀὀ┠ࢆ 㞟ࡵ࡚┒ࢇ◊✲ࡉࢀࠊᐇ⏝㏆࡙࠸࡚࠸ࡿࠋ ᕼᅵ㢮ඖ⣲ࢆ⏝࠸ࡎࡶࠊ୍ḟ┦㌿⛣ࡢࡁ࡞࢚ ࣥࢺࣟࣆ࣮ኚࢆ⏝ࡍࢀࡤ㧗ᛶ⬟ࡢ෭ᶵࢆᐇ ⌧࡛ࡁࡿྍ⬟ᛶࡀ♧ࡉࢀࠊ⌧ᅾࡢ୍ࡘࡢ₻ὶ࡞ ࡾࡘࡘ࠶ࡿࠋᚋⓎࡢᮏࢱࢫࢡ࡛ࡣࠊ⌧᭷ࡢࢩ࣮ࢬ ࡛࠶ࡿᐊ ᇦ࡛␗ᖖࡁ࡞⇕⭾ᙇ⋡䠄ẚ⇕ᐦ ᥋㛵㐃ࡍࡿ≀⌮㔞䠅ࢆ♧ࡍᕼᅵ㢮ඖ⣲ Ce ࢆྵࡴ ᵓ㐀つ๎⣔ྜ㔠(7)-(9)ࡢᇶ♏◊✲ࢆ㐍ࡵࡓࠋ (2)ᾮయ❅⣲ ᗘᇦ㸸㖡㓟≀㧗 ㉸ఏᑟయࢆ⏝ ࠸ࡓ✀ࠎࡢࢹࣂࢫࡀ⏝ࡉࢀ࡚ࡁ࡚࠸ࡿࡀࠊࡇ ࡢᏳ ᐃືసࡢ ࡓࡵࡣ ᾮయ❅ ⣲ ᗘ 䠄❅⣲ࡢ Ἓ Ⅼ㸸77 K䠅ࡼࡾᩘ༑ K ప࠸ ᗘࡀᚲせ࡛࠶ࡾࠊࡇࢀ ࢆᐇ⌧ࡍࡿపࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢᑠᆺ☢Ẽ ෭ᶵࡀᮃࡲࢀࡿࠋࡑࡢᙧᡂࣃࢱ࣮ࣥࡽࢫࢺࣛ ࣉ⛛ᗎࡤࢀࡿ㟁Ⲵ⛛ᗎࢆ㉸ఏᑟ㌿⛣కࡗ ࡚㉳ࡇࡍ㖡㓟≀㧗 ㉸ఏᑟయ㛵ࡍࡿ◊✲ࢩ࣮ ࢬ(10)ࡀ࠶ࡾࠊࡇࡢ㌿⛣క࠺࢚ࣥࢺࣟࣆ࣮ኚࢆ ྵࡵࡓᇶ♏◊✲ྲྀࡾ⤌ࢇࡔࠋ (3)10 K ᗘᇦ㸸ࢡ࣮࢚ࣜࣥࢿࣝࢠ࣮ࡋ࡚ᮇᚅ ࡉࢀࡿỈ⣲⇞ᩱࢆ㈓ⶶ࣭㍺㏦ࡍࡿࡓࡵࡣỈ⣲ࢆ ᾮࡍࡿࡢࡀຠ⋡ⓗ࡛࠶ࡾࠊ10 K ⛬ᗘࡢ ᗘࢆᐇ ⌧ࡍࡿᚲせࡀ࠶ࡿࠋᾮయ࣒࣊ࣜ࢘ࢆ⏝ࡍࢀࡤࠊ ᾐₕࡍࡿࡔࡅ࡛࣒࣊ࣜ࢘ࡢἛⅬ 4.2 K ㏆ࡃࡲ࡛෭ ༷ࡍࡿࡇࡀྍ⬟࡛࠶ࡿࡀࠊ࣒࣊ࣜ࢘ࡣᕼᑡ㈨※ ࡛࠶ࡾࠊ♫ໃࡼࡗ࡚ࡣ☜ಖࡀࡁࢃࡵ࡚ᅔ㞴 ࡶ࡞ࡾᚓࡿࠋࡇࡢࡓࡵࠊ࣒࣊ࣜ࢘ࣇ࣮࡛ࣜྠ➼ ࡢ ᗘࢆᚓࡿᑠᆺ࣭పࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢ ☢Ẽ෭ᶵࡢ㛤Ⓨࡀᮇᚅࡉࢀ࡚࠸ࡿࠋࡇࢀࡲ࡛ⴭ ⪅ࡣ๓㏙ࡢα-R2S3ࡀ10 K ㏆ࡢ ᗘ࡛㏲ḟ☢Ẽ┦ ㌿⛣ࢆ㉳ࡇࡋࠊࡑࢀకࡗ࡚✀ࠎࡢ≉␗࡞≀ᛶᛂ ⟅ࢆ♧ࡍࡇࢆぢฟࡋ࡚ࡁࡓ(11)-(18)ࠋࡇࡢ◊✲ࢩ࣮ ࢬࢆάࡋࠊα-R2S3ࡢ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࢆ ᥈ࡗࡓࠋ α-R2S3ࡣᩳ᪉ᬗ⣔⤖ᬗᵓ㐀䠄✵㛫⩌㸸Pnma䠅୰ ⤖ᬗᏛⓗ⊂❧࡞ࡘࡢᕼᅵ㢮ࢧࢺ㸦R1, R2㸧ࢆ ᭷ࡋ࡚࠸ࡿ(11)ࠋࡇࢀࡲ࡛ᚓࡽࢀࡓᐇ㦂ᐇࢆ⥲ ᣓࡍࡿࠊR1 ࡣ b ㍈᪉ྥ୍ḟඖ㙐ෆ࡛ᙉ☢ᛶⓗࠊa ㍈᪉ྥࢪࢢࢨࢢ㙐ෆ࡛ᙉ☢ᛶⓗ⛛ᗎࡍࡿഴ ྥࡀᙉࡃࠊR1 ᙅࡃ⤖ྜࡋࡓ R2 ࡣ㊥㞳ⓗࡣࡸ ࡸ㐲࠸㞄᥋ R2 」㞧స⏝ࡋྜ࠺⪃ᐹࡉࢀࡿࠋ ࡇࡢR1-R2, R2-R2 㛫ࡢ」㞧࡞☢Ẽⓗ┦స⏝ࡀ➇ ྜࡋࠊ ᗘࡸ☢ሙᑐࡋ࡚࣐ࢡࣟ≀ᛶࡀ≉␗࡞ᛂ ⟅ࢆ♧ࡍ⪃࠼ࡽࢀࡿࠋᮏሗ࿌࡛ࡣࠊα-R2S3ࡢ↓☢ ሙୗ࠾ࡼࡧ☢ሙ୰࡛ࡢẚ⇕ࡢ ᐃ⤖ᯝ෭ᮦ࣭ ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࡘ࠸࡚㆟ㄽࡍࡿࠋ 3 ᐇ㦂 ᕷ㈍ࡢᕼᅵ㢮㓟≀ࢆ CS2Ẽὶ୰࡛ຍ⇕ࡍࡿࡇ ࡛ α-R2S3⢊ᮎヨᩱࢆᚓࠊࡇࢀࢆཎᩱࡋ࡚ࣚ࢘ ⣲ࢆ㍺㏦ࡋࡓẼ┦Ꮫ㍺㏦ἲࡼࡾ༢⤖ᬗヨ ᩱࢆ⫱ᡂࡋࡓࠋẚ⇕ࡣ⡿ᅜQuantum Design ♫〇≀ ⌮≉ᛶ ᐃࢩࢫࢸ࣒ PPMS ࢆ⏝ࡋࠊ5 T ࡲ࡛ࡢ ✀ࠎࡢ☢ሙ୰࡛⦆ἲࡼࡾ ᐃࡋࡓࠋ 4 ⤖ᯝ⪃ᐹ 4.1 ↓☢ሙୗẚ⇕ ᅗ1 α-R2S3䠄R㸸Pr, Nd, Sm, Gd, Tb, Dy䠅༢⤖ᬗ ࡢ↓☢ሙୗ࡛ࡢẚ⇕ࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋGd, Pr ⣔௨እࡢ α-R2S3࡛ࡣ㸰ẁࡢ☢Ẽ┦㌿⛣క࠺ඛ㗦 ࡞ࣆ࣮ࢡࡀ☜ㄆࡉࢀࡿࠋTb, Dy ⣔㛵ࡋ࡚ࡣ☢ ᐃ(12)(14)ࡸ୰ᛶᏊᅇᢡᐇ㦂(19)ࡢ⤖ᯝࡽࠊ㸰ẁࡢ ᙉ☢ᛶ㌿⛣ࡀ㉳ࡁ࡚࠸ࡿ⪃࠼ࡽࢀࡿࠋNd ⣔ࡢ ᑡ࡞ࡃࡶ㧗 ഃࣆ࣮ࢡࡣࡸࡣࡾᙉ☢ᛶ㌿⛣ ࡼࡿࡶࡢ࡛࠶ࡿࠋࡇࢀᑐࡋ࡚Sm ⣔࡛ࡢ㌿⛣ࡣ㸰 ẁࡢ䠄ᙅ䠅ᙉ☢ᛶ㌿⛣࡛࠶ࡿ⪃࠼ࡽࢀࡿ(16)ࠋPr ⣔ ࡛ࡣ᭱ప ࡢ0.36 K ࡲ࡛➨ࡢࣆ࣮ࢡࡣ☜ㄆࡉࢀ ࡞࠸ࡶࡢࡢࠊప ࡛ࡢ᫂ࡽ࡞ẚ⇕ࡢୖ᪼ࡽ㏲ ḟⓗ┦㌿⛣ࡀ࠶ࡿ⪃࠼ࡽࢀࡿࠋα-Tb2S3࡛ࡢ☢Ẽ ᵓ㐀ゎᯒ⤖ᯝ(19)ࡢᐇ㦂ᐇࡽࠊࡇࢀࡽࡢ㧗 ഃ㌿⛣࡛ࡣ R1ࠊప ഃ㌿⛣࡛ࡣ R2 ࡀ⛛ᗎࡍ 㧗ᛶ⬟☢Ẽ⇕ኚᮦᩱࡢ㛤Ⓨࢆ┠ᣦࡋ࡚- 35 -
ࡿ㢮᥎ࡉࢀࡿࠋ୍᪉࡛୰ᛶᏊᅇᢡᐇ㦂(20)ࡸ࢚ࣥ ࢺࣟࣆ࣮ኚ(21)ࡽ☜ㄆࡉࢀࡿࡼ࠺ࠊα-Gd2S3ࡣ 㸯ẁࡢ㌿⛣࡛Gd1, Gd2 ࡀᙉ☢ᛶ⛛ᗎࡍࡿࠋ 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0 5 10 15 20C
/ J
K
-1c
m
-3T / K
-
R
2S
3 R = Gd Tb Dy Pr Nd Sm ᅗ1 α-R2S3༢⤖ᬗࡢẚ⇕ࡢ ᗘ౫Ꮡᛶ ᅗ1 ࡽ᫂ࡽ࡞ࡼ࠺ࠊα-Gd2S3ࡢẚ⇕ࣆ࣮ࢡ ࡣࢆᅽಽࡋ࡚ࡁ࠸ࠋከ㔜㡯ᇶᗏ≧ែ࠾࠸࡚ Gd3+ࡢゅ㐠ື㔞J ࡣ 7/2 ẚ㍑ⓗࡁ࠸ࡀࠊTb3+ (J = 6)ࡸ Dy3+ (J = 15/2)ࡢ᪉ࡀࡉࡽࡁ࠸ࠋࡋࡋࠊ Gd ⣔௨እࡢ J ከ㔜㡯ࡣ⤖ᬗሙࡼࡗ࡚࢚ࢿࣝࢠ࣮ ‽ศࡋࠊᇶᗏ㡯ࡢከ㔜ᗘࡣపࡃ࡞ࡿࠋ୍᪉Gd ⣔࡛ࡣ㌶㐨ゅ㐠ື㔞ࡀ 0 ࡛࠶ࡿࡓࡵ⤖ᬗሙࡢᙳ 㡪ࢆཷࡅࡎࠊᇶᗏࡀࢫࣆࣥ 8 㔜㡯࡛࠶ࡿࡇ㉳ ᅉࡋ࡚ẚ⇕ࣆ࣮ࢡࡀࡁࡃ࡞ࡗ࡚࠸ࡿࠋࡉࡽGd ⣔࡛ࡣ㌿⛣ࡼࡾప ࡛ẚ⇕ࡀ⫪ࢆࡶࡗ࡚࠸ࡿࠋࡇ ࢀࡣᗄఱᏛⓗࣇࣛࢫࢺ࣮ࣞࢩࣙࣥࢆ᭷ࡍࡿGd2 ࡢ ⛛ᗎࡀGd1 ࡢ⮬Ⓨ⛛ᗎࡼࡿศᏊሙࡢᙳ㡪࡛ࠊ ᗘపୗకࡗ࡚ᚎࠎ㐍⾜ࡋ࡚࠸ࡿࡇ㉳ᅉ ࡋ࡚࠸ࡿ⪃࠼ࡽࢀࡿ(21)ࠋࡇࡢࡓࡵࠊα-Gd2S3ࡣᗈ ࠸ ᗘ⠊ᅖ࡛ࡁ࡞ẚ⇕ࢆࡶࡘࠋ༢య✚࠶ࡓࡾ ࡢẚ⇕ࡢ್᭱0.63 J K-1cm-3 (T = 9.8 K)ࡣ෭ᮦ ࡋ ࡚ ᮇ ᚅ ࡉ ࢀ ࡚ ࠸ ࡿ Gd2O2S (GOS) ࡢ 1.1 J K-1cm-3 (T = 5.2 K)ࡼࡾࡶప࠸ࡀࠊᐇ⏝ࡉࢀ࡚࠸ ࡿEr3Ni ࡸ HoCu2ࢆ㥙ࡋ࡚࠸ࡿࠋHoCu2ࡀࢲࣈࣝ ࣆ࣮ࢡ࡛ࡼ࠸ᛶ⬟ࢆ♧ࡍ ᗘᇦ࡛ࡣ್ࡀୗᅇࡿࡀ α-Gd2S3ࡢᖜᗈࡢ⫪ࡣⰋ࠸≉ᚩ࡛࠶ࡿࠋࡲࡓࠊࡼࡾ ࡁ࡞ẚ⇕ࣆ࣮ࢡࢆࡶࡘᙉ☢ᛶయ ErNi ࡛ࡣ࡞ࡃ Er3Ni ࡀᐇ⏝ࡉࢀ࡚࠸ࡿ⌮⏤ࡣᚋ⪅ࡀᙉ☢ᛶయ ࡛࠶ࡾ㉸ఏᑟ࣐ࢢࢿࢵࢺࡽࡢ₃ࢀ☢ሙࡢᙳ㡪ࢆ ཷࡅࡃ࠸ࡓࡵ࡛࠶ࡿࡀࠊࡑࡢⅬ࡛ࡶᙉ☢ᛶయ α-Gd2S3ࡣ㐺ࡋ࡚࠸ࡿࠋࡁ࡞ẚ⇕ࢆ♧ࡍ ᗘᇦࡀ ␗࡞ࡿ෭ᮦࢆ⤌ࡳྜࢃࡏ࡚෭ᶵ➼ሸࡍࡿ ࡇࡼࡾ㧗ຠ⋡ࡀᅗࢀࡿࡓࡵࠊࢲࣈࣝࣆ࣮ࢡ ࢆ♧ࡍࡢ α-R2S3ࡶྵࡵࠊẚ⇕≉ᛶⓗࡣ෭ᮦ ࡋ࡚ࡢྍ⬟ᛶࡣ࠶ࡿࠋࡋࡋᐇᮦᩱࡋ࡚ࡣࠊ ⌫≧ከ⤖ᬗヨᩱࡢసᡂྍ⬟ᛶࠊࡑࡢሙྜࡢẚ⇕≉ ᛶࡸ⇕ఏᑟ⋡ࠊ⇕ࢧࢡࣝࢆྵࡵࡓ⪏⎔ቃᛶࠊࢥ ࢫࢺ➼ࡢ᳨ウࡍࡁㄢ㢟ࡣᩘከࡃᏑᅾࡍࡿࠋ 4.2 ☢ሙ୰ẚ⇕ ᅗ2 α-Dy2S3ࡢb ㍈ᑐࡋ࡚ᆶ┤☢ሙࢆ༳ຍ ࡋࡓሙྜࡢ(a)☢Ẽẚ⇕ Cm࠾ࡼࡧ(b)☢Ẽ࢚ࣥࢺࣟ ࣆ࣮Smࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋ㧗 ഃ㌿⛣ⅬTN1ࡀ☢ ሙ༳ຍࡼࡾ㢧ⴭ㧗 ഃࢩࣇࢺࡋࠊప ഃ㌿ ⛣ࡀᾘኻࡋ࡚࠸ࡿᵝᏊࡀࢃࡿࠋᙉ☢ᛶ㌿⛣ࡀ☢ ሙ༳ຍࡼࡾ㧗 ഃࢩࣇࢺࡍࡿࡇࡣࡼࡃぢࡽ ࢀࡿࡇ࡛ࠊࡇࡢഴྥࡣ☢Ẽ෭ࡗ࡚ࡣ㒔ྜ ࡀⰋ࠸ࠋࡋࡋࠊᙉ☢ᛶ㌿⛣ࡣ☢ሙ༳ຍࡼࡾ ప ഃࢩࣇࢺࡍࡿࡢࡀ୍⯡ⓗ࡛࠶ࡿࠋ⌧ࡢ α-R2S3࡛ࡣ☢ሙࡢ༳ຍ᪉ྥࡼࡽࡎ㌿⛣ࡢప ࢩ ࣇࢺࡀほ ࡉࢀࡿࡋࠊα-Dy2S3ࡢb ㍈ᖹ⾜࡞☢ሙ ༳ຍ࡛ࡶྠᵝࡢഴྥࡀぢࡽࢀࡿࠋα-Dy2S3ࡣ㏲ḟ ᙉ☢ᛶ㌿⛣Ⅼࡢ㛫TN1-TN2࡛✀ࠎࡢ≉␗࡞⌧㇟ࢆ♧ ࡍ(13)(14)ࡀࠊb ㍈ᆶ┤࡞☢ሙᑐࡍࡿᛂ⟅ࡀ㗦ᩄ ࡛࠶ࡿࡇࡶࡑࡢ୍ࡘ࡛࠶ࡿࠋDy1 ࡀᙉ☢ᛶ⛛ ᗎࡍࡿࡇࡼࡾࠊDy2 ࡢ☢ሙᑐࡍࡿᛂ⟅ᛶ ࡀࡼࡃ࡞ࡾࠊ☢ሙࡼࡿࢮ࣮࣐࢚ࣥࢿࣝࢠ࣮పୗ ࡀ࠶ࡿࡓࡵࠊTN1ࡀ㧗 ࢩࣇࢺࡍࡿ⪃࠼ࡽࢀࡿࠋ 0 10 20 30 40 50-
Dy2S
3C
m/ J
K
-1mol
-1Hԋb
0 T 1 T2 T 3 T 5 T(a)
0 5 10 15 20 0 5 10 15 20-
Dy2S
3S
m/ J
K
-1mol
-1Hԋb
0 T1 T 2 T 5 T 3 T(b)
T / K
ᅗ2 α-R2S3༢⤖ᬗࡢ☢ሙ୰࡛ࡢ(a)☢Ẽẚ⇕ (b)☢Ẽ࢚ࣥࢺࣟࣆ࣮ࡢ ᗘ౫Ꮡᛶ TN1ࡢ㧗 ࢩࣇࢺప ഃTN2࡛ࡢ㌿⛣ࡢᾘኻࡀ ࡶຠ࠸࡚ࠊᅗ2(b)♧ࡍࡼ࠺ Cm/T ࢆ ᐃ᭱ ప ᗘ 0.4 K ࡽ ᗘ࡛✚ศࡋࡓ☢Ẽ࢚ࣥࢺࣟࣆ ࣮ࡣ☢ሙ༳ຍࡼࡾῶᑡࡋ࡚࠸ࡿ㸦|Sm| < 0㸧ࠋບ ☢Ọஂ☢▼ࡢ⏝ࢆᐃࡋࡓ☢ሙ 2 T ࡛ࡢ|Sm|- 35 - 㧗ᛶ⬟☢Ẽ⇕ኚᮦᩱࡢ㛤Ⓨࢆ┠ᣦࡋ࡚
- 35 -
ࡿ㢮᥎ࡉࢀࡿࠋ୍᪉࡛୰ᛶᏊᅇᢡᐇ㦂(20)ࡸ࢚ࣥ ࢺࣟࣆ࣮ኚ(21)ࡽ☜ㄆࡉࢀࡿࡼ࠺ࠊα-Gd2S3ࡣ 㸯ẁࡢ㌿⛣࡛Gd1, Gd2 ࡀᙉ☢ᛶ⛛ᗎࡍࡿࠋ 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0 5 10 15 20C
/ J
K
-1c
m
-3T / K
-
R
2S
3 R = Gd Tb Dy Pr Nd Sm ᅗ1 α-R2S3༢⤖ᬗࡢẚ⇕ࡢ ᗘ౫Ꮡᛶ ᅗ1 ࡽ᫂ࡽ࡞ࡼ࠺ࠊα-Gd2S3ࡢẚ⇕ࣆ࣮ࢡ ࡣࢆᅽಽࡋ࡚ࡁ࠸ࠋከ㔜㡯ᇶᗏ≧ែ࠾࠸࡚ Gd3+ࡢゅ㐠ື㔞J ࡣ 7/2 ẚ㍑ⓗࡁ࠸ࡀࠊTb3+ (J = 6)ࡸ Dy3+ (J = 15/2)ࡢ᪉ࡀࡉࡽࡁ࠸ࠋࡋࡋࠊ Gd ⣔௨እࡢ J ከ㔜㡯ࡣ⤖ᬗሙࡼࡗ࡚࢚ࢿࣝࢠ࣮ ‽ศࡋࠊᇶᗏ㡯ࡢከ㔜ᗘࡣపࡃ࡞ࡿࠋ୍᪉Gd ⣔࡛ࡣ㌶㐨ゅ㐠ື㔞ࡀ 0 ࡛࠶ࡿࡓࡵ⤖ᬗሙࡢᙳ 㡪ࢆཷࡅࡎࠊᇶᗏࡀࢫࣆࣥ 8 㔜㡯࡛࠶ࡿࡇ㉳ ᅉࡋ࡚ẚ⇕ࣆ࣮ࢡࡀࡁࡃ࡞ࡗ࡚࠸ࡿࠋࡉࡽGd ⣔࡛ࡣ㌿⛣ࡼࡾప ࡛ẚ⇕ࡀ⫪ࢆࡶࡗ࡚࠸ࡿࠋࡇ ࢀࡣᗄఱᏛⓗࣇࣛࢫࢺ࣮ࣞࢩࣙࣥࢆ᭷ࡍࡿGd2 ࡢ ⛛ᗎࡀGd1 ࡢ⮬Ⓨ⛛ᗎࡼࡿศᏊሙࡢᙳ㡪࡛ࠊ ᗘపୗకࡗ࡚ᚎࠎ㐍⾜ࡋ࡚࠸ࡿࡇ㉳ᅉ ࡋ࡚࠸ࡿ⪃࠼ࡽࢀࡿ(21)ࠋࡇࡢࡓࡵࠊα-Gd2S3ࡣᗈ ࠸ ᗘ⠊ᅖ࡛ࡁ࡞ẚ⇕ࢆࡶࡘࠋ༢య✚࠶ࡓࡾ ࡢẚ⇕ࡢ್᭱0.63 J K-1cm-3 (T = 9.8 K)ࡣ෭ᮦ ࡋ ࡚ ᮇ ᚅ ࡉ ࢀ ࡚ ࠸ ࡿ Gd2O2S (GOS) ࡢ 1.1 J K-1cm-3 (T = 5.2 K)ࡼࡾࡶప࠸ࡀࠊᐇ⏝ࡉࢀ࡚࠸ ࡿEr3Ni ࡸ HoCu2ࢆ㥙ࡋ࡚࠸ࡿࠋHoCu2ࡀࢲࣈࣝ ࣆ࣮ࢡ࡛ࡼ࠸ᛶ⬟ࢆ♧ࡍ ᗘᇦ࡛ࡣ್ࡀୗᅇࡿࡀ α-Gd2S3ࡢᖜᗈࡢ⫪ࡣⰋ࠸≉ᚩ࡛࠶ࡿࠋࡲࡓࠊࡼࡾ ࡁ࡞ẚ⇕ࣆ࣮ࢡࢆࡶࡘᙉ☢ᛶయ ErNi ࡛ࡣ࡞ࡃ Er3Ni ࡀᐇ⏝ࡉࢀ࡚࠸ࡿ⌮⏤ࡣᚋ⪅ࡀᙉ☢ᛶయ ࡛࠶ࡾ㉸ఏᑟ࣐ࢢࢿࢵࢺࡽࡢ₃ࢀ☢ሙࡢᙳ㡪ࢆ ཷࡅࡃ࠸ࡓࡵ࡛࠶ࡿࡀࠊࡑࡢⅬ࡛ࡶᙉ☢ᛶయ α-Gd2S3ࡣ㐺ࡋ࡚࠸ࡿࠋࡁ࡞ẚ⇕ࢆ♧ࡍ ᗘᇦࡀ ␗࡞ࡿ෭ᮦࢆ⤌ࡳྜࢃࡏ࡚෭ᶵ➼ሸࡍࡿ ࡇࡼࡾ㧗ຠ⋡ࡀᅗࢀࡿࡓࡵࠊࢲࣈࣝࣆ࣮ࢡ ࢆ♧ࡍࡢ α-R2S3ࡶྵࡵࠊẚ⇕≉ᛶⓗࡣ෭ᮦ ࡋ࡚ࡢྍ⬟ᛶࡣ࠶ࡿࠋࡋࡋᐇᮦᩱࡋ࡚ࡣࠊ ⌫≧ከ⤖ᬗヨᩱࡢసᡂྍ⬟ᛶࠊࡑࡢሙྜࡢẚ⇕≉ ᛶࡸ⇕ఏᑟ⋡ࠊ⇕ࢧࢡࣝࢆྵࡵࡓ⪏⎔ቃᛶࠊࢥ ࢫࢺ➼ࡢ᳨ウࡍࡁㄢ㢟ࡣᩘከࡃᏑᅾࡍࡿࠋ 4.2 ☢ሙ୰ẚ⇕ ᅗ2 α-Dy2S3ࡢb ㍈ᑐࡋ࡚ᆶ┤☢ሙࢆ༳ຍ ࡋࡓሙྜࡢ(a)☢Ẽẚ⇕ Cm࠾ࡼࡧ(b)☢Ẽ࢚ࣥࢺࣟ ࣆ࣮Smࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋ㧗 ഃ㌿⛣ⅬTN1ࡀ☢ ሙ༳ຍࡼࡾ㢧ⴭ㧗 ഃࢩࣇࢺࡋࠊప ഃ㌿ ⛣ࡀᾘኻࡋ࡚࠸ࡿᵝᏊࡀࢃࡿࠋᙉ☢ᛶ㌿⛣ࡀ☢ ሙ༳ຍࡼࡾ㧗 ഃࢩࣇࢺࡍࡿࡇࡣࡼࡃぢࡽ ࢀࡿࡇ࡛ࠊࡇࡢഴྥࡣ☢Ẽ෭ࡗ࡚ࡣ㒔ྜ ࡀⰋ࠸ࠋࡋࡋࠊᙉ☢ᛶ㌿⛣ࡣ☢ሙ༳ຍࡼࡾ ప ഃࢩࣇࢺࡍࡿࡢࡀ୍⯡ⓗ࡛࠶ࡿࠋ⌧ࡢ α-R2S3࡛ࡣ☢ሙࡢ༳ຍ᪉ྥࡼࡽࡎ㌿⛣ࡢప ࢩ ࣇࢺࡀほ ࡉࢀࡿࡋࠊα-Dy2S3ࡢb ㍈ᖹ⾜࡞☢ሙ ༳ຍ࡛ࡶྠᵝࡢഴྥࡀぢࡽࢀࡿࠋα-Dy2S3ࡣ㏲ḟ ᙉ☢ᛶ㌿⛣Ⅼࡢ㛫TN1-TN2࡛✀ࠎࡢ≉␗࡞⌧㇟ࢆ♧ ࡍ(13)(14)ࡀࠊb ㍈ᆶ┤࡞☢ሙᑐࡍࡿᛂ⟅ࡀ㗦ᩄ ࡛࠶ࡿࡇࡶࡑࡢ୍ࡘ࡛࠶ࡿࠋDy1 ࡀᙉ☢ᛶ⛛ ᗎࡍࡿࡇࡼࡾࠊDy2 ࡢ☢ሙᑐࡍࡿᛂ⟅ᛶ ࡀࡼࡃ࡞ࡾࠊ☢ሙࡼࡿࢮ࣮࣐࢚ࣥࢿࣝࢠ࣮పୗ ࡀ࠶ࡿࡓࡵࠊTN1ࡀ㧗 ࢩࣇࢺࡍࡿ⪃࠼ࡽࢀࡿࠋ 0 10 20 30 40 50-
Dy
2S
3C
m/ J
K
-1mol
-1Hԋb
0 T 1 T2 T 3 T 5 T(a)
0 5 10 15 20 0 5 10 15 20-
Dy
2S
3S
m/ J
K
-1mol
-1Hԋb
0 T1 T 2 T 5 T 3 T(b)
T / K
ᅗ2 α-R2S3༢⤖ᬗࡢ☢ሙ୰࡛ࡢ(a)☢Ẽẚ⇕ (b)☢Ẽ࢚ࣥࢺࣟࣆ࣮ࡢ ᗘ౫Ꮡᛶ TN1ࡢ㧗 ࢩࣇࢺప ഃTN2࡛ࡢ㌿⛣ࡢᾘኻࡀ ࡶຠ࠸࡚ࠊᅗ2(b)♧ࡍࡼ࠺ Cm/T ࢆ ᐃ᭱ ప ᗘ 0.4 K ࡽ ᗘ࡛✚ศࡋࡓ☢Ẽ࢚ࣥࢺࣟࣆ ࣮ࡣ☢ሙ༳ຍࡼࡾῶᑡࡋ࡚࠸ࡿ㸦|Sm| < 0㸧ࠋບ ☢Ọஂ☢▼ࡢ⏝ࢆᐃࡋࡓ☢ሙ 2 T ࡛ࡢ|Sm| ᡁ ಟ㸪㜿Ἴຍ ῟㸪⸨ ⪔୍㑻- 34 -
ࡁ࡞ゅ㐠ື㔞㔞Ꮚᩘࢆࡶࡘ㔜ᕼᅵ㢮ඖ⣲ࢆྵࡴ ≀㉁ࡀೃ⿵࡞ࡾᚓࡿࠋ10 K ⛬ᗘ࡛☢Ẽ┦㌿⛣ࢆ ࡶࡘα ኚែᕼᅵ㢮୕◲≀ α-R2S3䠄R㸸ᕼᅵ㢮ඖ ⣲䠅ࡸᕼᅵ㢮࣍࢘≀╔┠ࡋࠊ⣔⤫ⓗ࡞ẚ⇕ ᐃ ࢆ⾜ࡗࡓࠋ ☢Ẽ෭ᮦ㛵ࡋ࡚ࡣືస ᗘࢆ⪃៖ࡍࡿࡇ ࡀ㔜せ࡛࠶ࡾࠊᮏࢱࢫࢡ࣓ࣥࣂ࣮ࡀࡶࡘࢩ࣮ࢬࢆ ㋃ࡲ࠼ࠊ(1)ᐊ ᇦࠊ(2)ᾮయ❅⣲ ᗘᇦࠊ(3)10 K ᗘᇦ࡛ࡢ᳨ウࢆ⾜ࡗࡓࠋ (1)ᐊ ᇦ㸸ᐊ ᇦ࠾ࡅࡿ☢Ẽ෭ᶵࡣࠊࣇࣟ ࣥ࢞ࢫࡼࡿ࢜ࢰࣥᒙࡢ◚ቯࠊ௦᭰ࣇࣟࣥ࢞ࢫ ࡼࡿᆅ⌫ ᬮࡢಁ㐍ࢆ㜼ࡴࡶࡢࡋ࡚ᮇᚅࡉࢀ ࡚࠸ࡿࠋࡇࡢ ᗘᇦ࠾࠸࡚ࡣࠊᐊ ㏆ᙉ☢ ᛶ㌿⛣ ᗘ䠄࣮࢟ࣗࣜⅬ䠅TC ࢆࡶࡘᕼᅵ㢮ඖ⣲ Gd ࡀึᮇࡢ㡭ࡼࡾὀ┠ࡉࢀ࡚ᐇᶵ࡛ࡶホ౯ࡉࢀࠊᐊ ☢Ẽ෭ࢩࢫࢸ࣒ࡢⓎᒎࡁ࡞ᙺࢆᢸࡗ࡚ ࡁࡓࠋ㧗ຠ⋡࣭㧗ᛶ⬟ࡢࡓࡵ✀ࠎࡢGd ྜ≀ࠊ ࠼ࡤGd5Si2Ge2(1)(2)ࡸࠊ㠀☢ᛶࡢᕼᅵ㢮ඖ⣲La ࢆ ྵࡴ La(Fe1-xSix)13Hy(3)(4)࠶ࡿ࠸ࡣᕼᅵ㢮ඖ⣲ࢆྵࡲ ࡞࠸Mn(As1-xSbx)(5)ࡸ MnFe(P1-xAsx)(6)࡞ࡀὀ┠ࢆ 㞟ࡵ࡚┒ࢇ◊✲ࡉࢀࠊᐇ⏝㏆࡙࠸࡚࠸ࡿࠋ ᕼᅵ㢮ඖ⣲ࢆ⏝࠸ࡎࡶࠊ୍ḟ┦㌿⛣ࡢࡁ࡞࢚ ࣥࢺࣟࣆ࣮ኚࢆ⏝ࡍࢀࡤ㧗ᛶ⬟ࡢ෭ᶵࢆᐇ ⌧࡛ࡁࡿྍ⬟ᛶࡀ♧ࡉࢀࠊ⌧ᅾࡢ୍ࡘࡢ₻ὶ࡞ ࡾࡘࡘ࠶ࡿࠋᚋⓎࡢᮏࢱࢫࢡ࡛ࡣࠊ⌧᭷ࡢࢩ࣮ࢬ ࡛࠶ࡿᐊ ᇦ࡛␗ᖖࡁ࡞⇕⭾ᙇ⋡䠄ẚ⇕ᐦ ᥋㛵㐃ࡍࡿ≀⌮㔞䠅ࢆ♧ࡍᕼᅵ㢮ඖ⣲ Ce ࢆྵࡴ ᵓ㐀つ๎⣔ྜ㔠(7)-(9)ࡢᇶ♏◊✲ࢆ㐍ࡵࡓࠋ (2)ᾮయ❅⣲ ᗘᇦ㸸㖡㓟≀㧗 ㉸ఏᑟయࢆ⏝ ࠸ࡓ✀ࠎࡢࢹࣂࢫࡀ⏝ࡉࢀ࡚ࡁ࡚࠸ࡿࡀࠊࡇ ࡢᏳ ᐃືసࡢ ࡓࡵࡣ ᾮయ❅ ⣲ ᗘ 䠄❅⣲ࡢ Ἓ Ⅼ㸸77 K䠅ࡼࡾᩘ༑ K ప࠸ ᗘࡀᚲせ࡛࠶ࡾࠊࡇࢀ ࢆᐇ⌧ࡍࡿపࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢᑠᆺ☢Ẽ ෭ᶵࡀᮃࡲࢀࡿࠋࡑࡢᙧᡂࣃࢱ࣮ࣥࡽࢫࢺࣛ ࣉ⛛ᗎࡤࢀࡿ㟁Ⲵ⛛ᗎࢆ㉸ఏᑟ㌿⛣కࡗ ࡚㉳ࡇࡍ㖡㓟≀㧗 ㉸ఏᑟయ㛵ࡍࡿ◊✲ࢩ࣮ ࢬ(10)ࡀ࠶ࡾࠊࡇࡢ㌿⛣క࠺࢚ࣥࢺࣟࣆ࣮ኚࢆ ྵࡵࡓᇶ♏◊✲ྲྀࡾ⤌ࢇࡔࠋ (3)10 K ᗘᇦ㸸ࢡ࣮࢚ࣜࣥࢿࣝࢠ࣮ࡋ࡚ᮇᚅ ࡉࢀࡿỈ⣲⇞ᩱࢆ㈓ⶶ࣭㍺㏦ࡍࡿࡓࡵࡣỈ⣲ࢆ ᾮࡍࡿࡢࡀຠ⋡ⓗ࡛࠶ࡾࠊ10 K ⛬ᗘࡢ ᗘࢆᐇ ⌧ࡍࡿᚲせࡀ࠶ࡿࠋᾮయ࣒࣊ࣜ࢘ࢆ⏝ࡍࢀࡤࠊ ᾐₕࡍࡿࡔࡅ࡛࣒࣊ࣜ࢘ࡢἛⅬ 4.2 K ㏆ࡃࡲ࡛෭ ༷ࡍࡿࡇࡀྍ⬟࡛࠶ࡿࡀࠊ࣒࣊ࣜ࢘ࡣᕼᑡ㈨※ ࡛࠶ࡾࠊ♫ໃࡼࡗ࡚ࡣ☜ಖࡀࡁࢃࡵ࡚ᅔ㞴 ࡶ࡞ࡾᚓࡿࠋࡇࡢࡓࡵࠊ࣒࣊ࣜ࢘ࣇ࣮࡛ࣜྠ➼ ࡢ ᗘࢆᚓࡿᑠᆺ࣭పࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢ ☢Ẽ෭ᶵࡢ㛤Ⓨࡀᮇᚅࡉࢀ࡚࠸ࡿࠋࡇࢀࡲ࡛ⴭ ⪅ࡣ๓㏙ࡢα-R2S3ࡀ10 K ㏆ࡢ ᗘ࡛㏲ḟ☢Ẽ┦ ㌿⛣ࢆ㉳ࡇࡋࠊࡑࢀకࡗ࡚✀ࠎࡢ≉␗࡞≀ᛶᛂ ⟅ࢆ♧ࡍࡇࢆぢฟࡋ࡚ࡁࡓ(11)-(18)ࠋࡇࡢ◊✲ࢩ࣮ ࢬࢆάࡋࠊα-R2S3ࡢ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࢆ ᥈ࡗࡓࠋ α-R2S3ࡣᩳ᪉ᬗ⣔⤖ᬗᵓ㐀䠄✵㛫⩌㸸Pnma䠅୰ ⤖ᬗᏛⓗ⊂❧࡞ࡘࡢᕼᅵ㢮ࢧࢺ㸦R1, R2㸧ࢆ ᭷ࡋ࡚࠸ࡿ(11)ࠋࡇࢀࡲ࡛ᚓࡽࢀࡓᐇ㦂ᐇࢆ⥲ ᣓࡍࡿࠊR1 ࡣ b ㍈᪉ྥ୍ḟඖ㙐ෆ࡛ᙉ☢ᛶⓗࠊa ㍈᪉ྥࢪࢢࢨࢢ㙐ෆ࡛ᙉ☢ᛶⓗ⛛ᗎࡍࡿഴ ྥࡀᙉࡃࠊR1 ᙅࡃ⤖ྜࡋࡓ R2 ࡣ㊥㞳ⓗࡣࡸ ࡸ㐲࠸㞄᥋ R2 」㞧స⏝ࡋྜ࠺⪃ᐹࡉࢀࡿࠋ ࡇࡢR1-R2, R2-R2 㛫ࡢ」㞧࡞☢Ẽⓗ┦స⏝ࡀ➇ ྜࡋࠊ ᗘࡸ☢ሙᑐࡋ࡚࣐ࢡࣟ≀ᛶࡀ≉␗࡞ᛂ ⟅ࢆ♧ࡍ⪃࠼ࡽࢀࡿࠋᮏሗ࿌࡛ࡣࠊα-R2S3ࡢ↓☢ ሙୗ࠾ࡼࡧ☢ሙ୰࡛ࡢẚ⇕ࡢ ᐃ⤖ᯝ෭ᮦ࣭ ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࡘ࠸࡚㆟ㄽࡍࡿࠋ 3 ᐇ㦂 ᕷ㈍ࡢᕼᅵ㢮㓟≀ࢆ CS2Ẽὶ୰࡛ຍ⇕ࡍࡿࡇ ࡛ α-R2S3⢊ᮎヨᩱࢆᚓࠊࡇࢀࢆཎᩱࡋ࡚ࣚ࢘ ⣲ࢆ㍺㏦ࡋࡓẼ┦Ꮫ㍺㏦ἲࡼࡾ༢⤖ᬗヨ ᩱࢆ⫱ᡂࡋࡓࠋẚ⇕ࡣ⡿ᅜQuantum Design ♫〇≀ ⌮≉ᛶ ᐃࢩࢫࢸ࣒ PPMS ࢆ⏝ࡋࠊ5 T ࡲ࡛ࡢ ✀ࠎࡢ☢ሙ୰࡛⦆ἲࡼࡾ ᐃࡋࡓࠋ 4 ⤖ᯝ⪃ᐹ 4.1 ↓☢ሙୗẚ⇕ ᅗ1 α-R2S3䠄R㸸Pr, Nd, Sm, Gd, Tb, Dy䠅༢⤖ᬗ ࡢ↓☢ሙୗ࡛ࡢẚ⇕ࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋGd, Pr ⣔௨እࡢ α-R2S3࡛ࡣ㸰ẁࡢ☢Ẽ┦㌿⛣క࠺ඛ㗦 ࡞ࣆ࣮ࢡࡀ☜ㄆࡉࢀࡿࠋTb, Dy ⣔㛵ࡋ࡚ࡣ☢ ᐃ(12)(14)ࡸ୰ᛶᏊᅇᢡᐇ㦂(19)ࡢ⤖ᯝࡽࠊ㸰ẁࡢ ᙉ☢ᛶ㌿⛣ࡀ㉳ࡁ࡚࠸ࡿ⪃࠼ࡽࢀࡿࠋNd ⣔ࡢ ᑡ࡞ࡃࡶ㧗 ഃࣆ࣮ࢡࡣࡸࡣࡾᙉ☢ᛶ㌿⛣ ࡼࡿࡶࡢ࡛࠶ࡿࠋࡇࢀᑐࡋ࡚Sm ⣔࡛ࡢ㌿⛣ࡣ㸰 ẁࡢ䠄ᙅ䠅ᙉ☢ᛶ㌿⛣࡛࠶ࡿ⪃࠼ࡽࢀࡿ(16)ࠋPr ⣔ ࡛ࡣ᭱ప ࡢ0.36 K ࡲ࡛➨ࡢࣆ࣮ࢡࡣ☜ㄆࡉࢀ ࡞࠸ࡶࡢࡢࠊప ࡛ࡢ᫂ࡽ࡞ẚ⇕ࡢୖ᪼ࡽ㏲ ḟⓗ┦㌿⛣ࡀ࠶ࡿ⪃࠼ࡽࢀࡿࠋα-Tb2S3࡛ࡢ☢Ẽ ᵓ㐀ゎᯒ⤖ᯝ(19)ࡢᐇ㦂ᐇࡽࠊࡇࢀࡽࡢ㧗 ഃ㌿⛣࡛ࡣ R1ࠊప ഃ㌿⛣࡛ࡣ R2 ࡀ⛛ᗎࡍ ᡁ ಟ㸪㜿Ἴຍ ῟㸪⸨ ⪔୍㑻- 34 -
ࡁ࡞ゅ㐠ື㔞㔞Ꮚᩘࢆࡶࡘ㔜ᕼᅵ㢮ඖ⣲ࢆྵࡴ ≀㉁ࡀೃ⿵࡞ࡾᚓࡿࠋ10 K ⛬ᗘ࡛☢Ẽ┦㌿⛣ࢆ ࡶࡘα ኚែᕼᅵ㢮୕◲≀ α-R2S3䠄R㸸ᕼᅵ㢮ඖ ⣲䠅ࡸᕼᅵ㢮࣍࢘≀╔┠ࡋࠊ⣔⤫ⓗ࡞ẚ⇕ ᐃ ࢆ⾜ࡗࡓࠋ ☢Ẽ෭ᮦ㛵ࡋ࡚ࡣືస ᗘࢆ⪃៖ࡍࡿࡇ ࡀ㔜せ࡛࠶ࡾࠊᮏࢱࢫࢡ࣓ࣥࣂ࣮ࡀࡶࡘࢩ࣮ࢬࢆ ㋃ࡲ࠼ࠊ(1)ᐊ ᇦࠊ(2)ᾮయ❅⣲ ᗘᇦࠊ(3)10 K ᗘᇦ࡛ࡢ᳨ウࢆ⾜ࡗࡓࠋ (1)ᐊ ᇦ㸸ᐊ ᇦ࠾ࡅࡿ☢Ẽ෭ᶵࡣࠊࣇࣟ ࣥ࢞ࢫࡼࡿ࢜ࢰࣥᒙࡢ◚ቯࠊ௦᭰ࣇࣟࣥ࢞ࢫ ࡼࡿᆅ⌫ ᬮࡢಁ㐍ࢆ㜼ࡴࡶࡢࡋ࡚ᮇᚅࡉࢀ ࡚࠸ࡿࠋࡇࡢ ᗘᇦ࠾࠸࡚ࡣࠊᐊ ㏆ᙉ☢ ᛶ㌿⛣ ᗘ䠄࣮࢟ࣗࣜⅬ䠅TC ࢆࡶࡘᕼᅵ㢮ඖ⣲ Gd ࡀึᮇࡢ㡭ࡼࡾὀ┠ࡉࢀ࡚ᐇᶵ࡛ࡶホ౯ࡉࢀࠊᐊ ☢Ẽ෭ࢩࢫࢸ࣒ࡢⓎᒎࡁ࡞ᙺࢆᢸࡗ࡚ ࡁࡓࠋ㧗ຠ⋡࣭㧗ᛶ⬟ࡢࡓࡵ✀ࠎࡢGd ྜ≀ࠊ ࠼ࡤGd5Si2Ge2(1)(2)ࡸࠊ㠀☢ᛶࡢᕼᅵ㢮ඖ⣲La ࢆ ྵࡴ La(Fe1-xSix)13Hy(3)(4)࠶ࡿ࠸ࡣᕼᅵ㢮ඖ⣲ࢆྵࡲ ࡞࠸Mn(As1-xSbx)(5)ࡸ MnFe(P1-xAsx)(6)࡞ࡀὀ┠ࢆ 㞟ࡵ࡚┒ࢇ◊✲ࡉࢀࠊᐇ⏝㏆࡙࠸࡚࠸ࡿࠋ ᕼᅵ㢮ඖ⣲ࢆ⏝࠸ࡎࡶࠊ୍ḟ┦㌿⛣ࡢࡁ࡞࢚ ࣥࢺࣟࣆ࣮ኚࢆ⏝ࡍࢀࡤ㧗ᛶ⬟ࡢ෭ᶵࢆᐇ ⌧࡛ࡁࡿྍ⬟ᛶࡀ♧ࡉࢀࠊ⌧ᅾࡢ୍ࡘࡢ₻ὶ࡞ ࡾࡘࡘ࠶ࡿࠋᚋⓎࡢᮏࢱࢫࢡ࡛ࡣࠊ⌧᭷ࡢࢩ࣮ࢬ ࡛࠶ࡿᐊ ᇦ࡛␗ᖖࡁ࡞⇕⭾ᙇ⋡䠄ẚ⇕ᐦ ᥋㛵㐃ࡍࡿ≀⌮㔞䠅ࢆ♧ࡍᕼᅵ㢮ඖ⣲ Ce ࢆྵࡴ ᵓ㐀つ๎⣔ྜ㔠(7)-(9)ࡢᇶ♏◊✲ࢆ㐍ࡵࡓࠋ (2)ᾮయ❅⣲ ᗘᇦ㸸㖡㓟≀㧗 ㉸ఏᑟయࢆ⏝ ࠸ࡓ✀ࠎࡢࢹࣂࢫࡀ⏝ࡉࢀ࡚ࡁ࡚࠸ࡿࡀࠊࡇ ࡢᏳ ᐃືసࡢ ࡓࡵࡣ ᾮయ❅ ⣲ ᗘ 䠄❅⣲ࡢ Ἓ Ⅼ㸸77 K䠅ࡼࡾᩘ༑ K ప࠸ ᗘࡀᚲせ࡛࠶ࡾࠊࡇࢀ ࢆᐇ⌧ࡍࡿపࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢᑠᆺ☢Ẽ ෭ᶵࡀᮃࡲࢀࡿࠋࡑࡢᙧᡂࣃࢱ࣮ࣥࡽࢫࢺࣛ ࣉ⛛ᗎࡤࢀࡿ㟁Ⲵ⛛ᗎࢆ㉸ఏᑟ㌿⛣కࡗ ࡚㉳ࡇࡍ㖡㓟≀㧗 ㉸ఏᑟయ㛵ࡍࡿ◊✲ࢩ࣮ ࢬ(10)ࡀ࠶ࡾࠊࡇࡢ㌿⛣క࠺࢚ࣥࢺࣟࣆ࣮ኚࢆ ྵࡵࡓᇶ♏◊✲ྲྀࡾ⤌ࢇࡔࠋ (3)10 K ᗘᇦ㸸ࢡ࣮࢚ࣜࣥࢿࣝࢠ࣮ࡋ࡚ᮇᚅ ࡉࢀࡿỈ⣲⇞ᩱࢆ㈓ⶶ࣭㍺㏦ࡍࡿࡓࡵࡣỈ⣲ࢆ ᾮࡍࡿࡢࡀຠ⋡ⓗ࡛࠶ࡾࠊ10 K ⛬ᗘࡢ ᗘࢆᐇ ⌧ࡍࡿᚲせࡀ࠶ࡿࠋᾮయ࣒࣊ࣜ࢘ࢆ⏝ࡍࢀࡤࠊ ᾐₕࡍࡿࡔࡅ࡛࣒࣊ࣜ࢘ࡢἛⅬ 4.2 K ㏆ࡃࡲ࡛෭ ༷ࡍࡿࡇࡀྍ⬟࡛࠶ࡿࡀࠊ࣒࣊ࣜ࢘ࡣᕼᑡ㈨※ ࡛࠶ࡾࠊ♫ໃࡼࡗ࡚ࡣ☜ಖࡀࡁࢃࡵ࡚ᅔ㞴 ࡶ࡞ࡾᚓࡿࠋࡇࡢࡓࡵࠊ࣒࣊ࣜ࢘ࣇ࣮࡛ࣜྠ➼ ࡢ ᗘࢆᚓࡿᑠᆺ࣭పࢥࢫࢺ࣭పື࣭ప㦁㡢ࡢ ☢Ẽ෭ᶵࡢ㛤Ⓨࡀᮇᚅࡉࢀ࡚࠸ࡿࠋࡇࢀࡲ࡛ⴭ ⪅ࡣ๓㏙ࡢα-R2S3ࡀ10 K ㏆ࡢ ᗘ࡛㏲ḟ☢Ẽ┦ ㌿⛣ࢆ㉳ࡇࡋࠊࡑࢀకࡗ࡚✀ࠎࡢ≉␗࡞≀ᛶᛂ ⟅ࢆ♧ࡍࡇࢆぢฟࡋ࡚ࡁࡓ(11)-(18)ࠋࡇࡢ◊✲ࢩ࣮ ࢬࢆάࡋࠊα-R2S3ࡢ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࢆ ᥈ࡗࡓࠋ α-R2S3ࡣᩳ᪉ᬗ⣔⤖ᬗᵓ㐀䠄✵㛫⩌㸸Pnma䠅୰ ⤖ᬗᏛⓗ⊂❧࡞ࡘࡢᕼᅵ㢮ࢧࢺ㸦R1, R2㸧ࢆ ᭷ࡋ࡚࠸ࡿ(11)ࠋࡇࢀࡲ࡛ᚓࡽࢀࡓᐇ㦂ᐇࢆ⥲ ᣓࡍࡿࠊR1 ࡣ b ㍈᪉ྥ୍ḟඖ㙐ෆ࡛ᙉ☢ᛶⓗࠊa ㍈᪉ྥࢪࢢࢨࢢ㙐ෆ࡛ᙉ☢ᛶⓗ⛛ᗎࡍࡿഴ ྥࡀᙉࡃࠊR1 ᙅࡃ⤖ྜࡋࡓ R2 ࡣ㊥㞳ⓗࡣࡸ ࡸ㐲࠸㞄᥋ R2 」㞧స⏝ࡋྜ࠺⪃ᐹࡉࢀࡿࠋ ࡇࡢR1-R2, R2-R2 㛫ࡢ」㞧࡞☢Ẽⓗ┦స⏝ࡀ➇ ྜࡋࠊ ᗘࡸ☢ሙᑐࡋ࡚࣐ࢡࣟ≀ᛶࡀ≉␗࡞ᛂ ⟅ࢆ♧ࡍ⪃࠼ࡽࢀࡿࠋᮏሗ࿌࡛ࡣࠊα-R2S3ࡢ↓☢ ሙୗ࠾ࡼࡧ☢ሙ୰࡛ࡢẚ⇕ࡢ ᐃ⤖ᯝ෭ᮦ࣭ ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࡘ࠸࡚㆟ㄽࡍࡿࠋ 3 ᐇ㦂 ᕷ㈍ࡢᕼᅵ㢮㓟≀ࢆ CS2Ẽὶ୰࡛ຍ⇕ࡍࡿࡇ ࡛ α-R2S3⢊ᮎヨᩱࢆᚓࠊࡇࢀࢆཎᩱࡋ࡚ࣚ࢘ ⣲ࢆ㍺㏦ࡋࡓẼ┦Ꮫ㍺㏦ἲࡼࡾ༢⤖ᬗヨ ᩱࢆ⫱ᡂࡋࡓࠋẚ⇕ࡣ⡿ᅜQuantum Design ♫〇≀ ⌮≉ᛶ ᐃࢩࢫࢸ࣒ PPMS ࢆ⏝ࡋࠊ5 T ࡲ࡛ࡢ ✀ࠎࡢ☢ሙ୰࡛⦆ἲࡼࡾ ᐃࡋࡓࠋ 4 ⤖ᯝ⪃ᐹ 4.1 ↓☢ሙୗẚ⇕ ᅗ1 α-R2S3䠄R㸸Pr, Nd, Sm, Gd, Tb, Dy䠅༢⤖ᬗ ࡢ↓☢ሙୗ࡛ࡢẚ⇕ࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋGd, Pr ⣔௨እࡢ α-R2S3࡛ࡣ㸰ẁࡢ☢Ẽ┦㌿⛣క࠺ඛ㗦 ࡞ࣆ࣮ࢡࡀ☜ㄆࡉࢀࡿࠋTb, Dy ⣔㛵ࡋ࡚ࡣ☢ ᐃ(12)(14)ࡸ୰ᛶᏊᅇᢡᐇ㦂(19)ࡢ⤖ᯝࡽࠊ㸰ẁࡢ ᙉ☢ᛶ㌿⛣ࡀ㉳ࡁ࡚࠸ࡿ⪃࠼ࡽࢀࡿࠋNd ⣔ࡢ ᑡ࡞ࡃࡶ㧗 ഃࣆ࣮ࢡࡣࡸࡣࡾᙉ☢ᛶ㌿⛣ ࡼࡿࡶࡢ࡛࠶ࡿࠋࡇࢀᑐࡋ࡚Sm ⣔࡛ࡢ㌿⛣ࡣ㸰 ẁࡢ䠄ᙅ䠅ᙉ☢ᛶ㌿⛣࡛࠶ࡿ⪃࠼ࡽࢀࡿ(16)ࠋPr ⣔ ࡛ࡣ᭱ప ࡢ0.36 K ࡲ࡛➨ࡢࣆ࣮ࢡࡣ☜ㄆࡉࢀ ࡞࠸ࡶࡢࡢࠊప ࡛ࡢ᫂ࡽ࡞ẚ⇕ࡢୖ᪼ࡽ㏲ ḟⓗ┦㌿⛣ࡀ࠶ࡿ⪃࠼ࡽࢀࡿࠋα-Tb2S3࡛ࡢ☢Ẽ ᵓ㐀ゎᯒ⤖ᯝ(19)ࡢᐇ㦂ᐇࡽࠊࡇࢀࡽࡢ㧗 ഃ㌿⛣࡛ࡣ R1ࠊప ഃ㌿⛣࡛ࡣ R2 ࡀ⛛ᗎࡍ 㧗ᛶ⬟☢Ẽ⇕ኚᮦᩱࡢ㛤Ⓨࢆ┠ᣦࡋ࡚- 35 -
ࡿ㢮᥎ࡉࢀࡿࠋ୍᪉࡛୰ᛶᏊᅇᢡᐇ㦂(20)ࡸ࢚ࣥ ࢺࣟࣆ࣮ኚ(21)ࡽ☜ㄆࡉࢀࡿࡼ࠺ࠊα-Gd2S3ࡣ 㸯ẁࡢ㌿⛣࡛Gd1, Gd2 ࡀᙉ☢ᛶ⛛ᗎࡍࡿࠋ 0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0 5 10 15 20C
/ J
K
-1c
m
-3T / K
-
R
2S
3 R = Gd Tb Dy Pr Nd Sm ᅗ1 α-R2S3༢⤖ᬗࡢẚ⇕ࡢ ᗘ౫Ꮡᛶ ᅗ1 ࡽ᫂ࡽ࡞ࡼ࠺ࠊα-Gd2S3ࡢẚ⇕ࣆ࣮ࢡ ࡣࢆᅽಽࡋ࡚ࡁ࠸ࠋከ㔜㡯ᇶᗏ≧ែ࠾࠸࡚ Gd3+ࡢゅ㐠ື㔞J ࡣ 7/2 ẚ㍑ⓗࡁ࠸ࡀࠊTb3+ (J = 6)ࡸ Dy3+ (J = 15/2)ࡢ᪉ࡀࡉࡽࡁ࠸ࠋࡋࡋࠊ Gd ⣔௨እࡢ J ከ㔜㡯ࡣ⤖ᬗሙࡼࡗ࡚࢚ࢿࣝࢠ࣮ ‽ศࡋࠊᇶᗏ㡯ࡢከ㔜ᗘࡣపࡃ࡞ࡿࠋ୍᪉Gd ⣔࡛ࡣ㌶㐨ゅ㐠ື㔞ࡀ 0 ࡛࠶ࡿࡓࡵ⤖ᬗሙࡢᙳ 㡪ࢆཷࡅࡎࠊᇶᗏࡀࢫࣆࣥ 8 㔜㡯࡛࠶ࡿࡇ㉳ ᅉࡋ࡚ẚ⇕ࣆ࣮ࢡࡀࡁࡃ࡞ࡗ࡚࠸ࡿࠋࡉࡽGd ⣔࡛ࡣ㌿⛣ࡼࡾప ࡛ẚ⇕ࡀ⫪ࢆࡶࡗ࡚࠸ࡿࠋࡇ ࢀࡣᗄఱᏛⓗࣇࣛࢫࢺ࣮ࣞࢩࣙࣥࢆ᭷ࡍࡿGd2 ࡢ ⛛ᗎࡀGd1 ࡢ⮬Ⓨ⛛ᗎࡼࡿศᏊሙࡢᙳ㡪࡛ࠊ ᗘపୗకࡗ࡚ᚎࠎ㐍⾜ࡋ࡚࠸ࡿࡇ㉳ᅉ ࡋ࡚࠸ࡿ⪃࠼ࡽࢀࡿ(21)ࠋࡇࡢࡓࡵࠊα-Gd2S3ࡣᗈ ࠸ ᗘ⠊ᅖ࡛ࡁ࡞ẚ⇕ࢆࡶࡘࠋ༢య✚࠶ࡓࡾ ࡢẚ⇕ࡢ್᭱0.63 J K-1cm-3 (T = 9.8 K)ࡣ෭ᮦ ࡋ ࡚ ᮇ ᚅ ࡉ ࢀ ࡚ ࠸ ࡿ Gd2O2S (GOS) ࡢ 1.1 J K-1cm-3 (T = 5.2 K)ࡼࡾࡶప࠸ࡀࠊᐇ⏝ࡉࢀ࡚࠸ ࡿEr3Ni ࡸ HoCu2ࢆ㥙ࡋ࡚࠸ࡿࠋHoCu2ࡀࢲࣈࣝ ࣆ࣮ࢡ࡛ࡼ࠸ᛶ⬟ࢆ♧ࡍ ᗘᇦ࡛ࡣ್ࡀୗᅇࡿࡀ α-Gd2S3ࡢᖜᗈࡢ⫪ࡣⰋ࠸≉ᚩ࡛࠶ࡿࠋࡲࡓࠊࡼࡾ ࡁ࡞ẚ⇕ࣆ࣮ࢡࢆࡶࡘᙉ☢ᛶయ ErNi ࡛ࡣ࡞ࡃ Er3Ni ࡀᐇ⏝ࡉࢀ࡚࠸ࡿ⌮⏤ࡣᚋ⪅ࡀᙉ☢ᛶయ ࡛࠶ࡾ㉸ఏᑟ࣐ࢢࢿࢵࢺࡽࡢ₃ࢀ☢ሙࡢᙳ㡪ࢆ ཷࡅࡃ࠸ࡓࡵ࡛࠶ࡿࡀࠊࡑࡢⅬ࡛ࡶᙉ☢ᛶయ α-Gd2S3ࡣ㐺ࡋ࡚࠸ࡿࠋࡁ࡞ẚ⇕ࢆ♧ࡍ ᗘᇦࡀ ␗࡞ࡿ෭ᮦࢆ⤌ࡳྜࢃࡏ࡚෭ᶵ➼ሸࡍࡿ ࡇࡼࡾ㧗ຠ⋡ࡀᅗࢀࡿࡓࡵࠊࢲࣈࣝࣆ࣮ࢡ ࢆ♧ࡍࡢ α-R2S3ࡶྵࡵࠊẚ⇕≉ᛶⓗࡣ෭ᮦ ࡋ࡚ࡢྍ⬟ᛶࡣ࠶ࡿࠋࡋࡋᐇᮦᩱࡋ࡚ࡣࠊ ⌫≧ከ⤖ᬗヨᩱࡢసᡂྍ⬟ᛶࠊࡑࡢሙྜࡢẚ⇕≉ ᛶࡸ⇕ఏᑟ⋡ࠊ⇕ࢧࢡࣝࢆྵࡵࡓ⪏⎔ቃᛶࠊࢥ ࢫࢺ➼ࡢ᳨ウࡍࡁㄢ㢟ࡣᩘከࡃᏑᅾࡍࡿࠋ 4.2 ☢ሙ୰ẚ⇕ ᅗ2 α-Dy2S3ࡢb ㍈ᑐࡋ࡚ᆶ┤☢ሙࢆ༳ຍ ࡋࡓሙྜࡢ(a)☢Ẽẚ⇕ Cm࠾ࡼࡧ(b)☢Ẽ࢚ࣥࢺࣟ ࣆ࣮Smࡢ ᗘ౫Ꮡᛶࢆ♧ࡍࠋ㧗 ഃ㌿⛣ⅬTN1ࡀ☢ ሙ༳ຍࡼࡾ㢧ⴭ㧗 ഃࢩࣇࢺࡋࠊప ഃ㌿ ⛣ࡀᾘኻࡋ࡚࠸ࡿᵝᏊࡀࢃࡿࠋᙉ☢ᛶ㌿⛣ࡀ☢ ሙ༳ຍࡼࡾ㧗 ഃࢩࣇࢺࡍࡿࡇࡣࡼࡃぢࡽ ࢀࡿࡇ࡛ࠊࡇࡢഴྥࡣ☢Ẽ෭ࡗ࡚ࡣ㒔ྜ ࡀⰋ࠸ࠋࡋࡋࠊᙉ☢ᛶ㌿⛣ࡣ☢ሙ༳ຍࡼࡾ ప ഃࢩࣇࢺࡍࡿࡢࡀ୍⯡ⓗ࡛࠶ࡿࠋ⌧ࡢ α-R2S3࡛ࡣ☢ሙࡢ༳ຍ᪉ྥࡼࡽࡎ㌿⛣ࡢప ࢩ ࣇࢺࡀほ ࡉࢀࡿࡋࠊα-Dy2S3ࡢb ㍈ᖹ⾜࡞☢ሙ ༳ຍ࡛ࡶྠᵝࡢഴྥࡀぢࡽࢀࡿࠋα-Dy2S3ࡣ㏲ḟ ᙉ☢ᛶ㌿⛣Ⅼࡢ㛫TN1-TN2࡛✀ࠎࡢ≉␗࡞⌧㇟ࢆ♧ ࡍ(13)(14)ࡀࠊb ㍈ᆶ┤࡞☢ሙᑐࡍࡿᛂ⟅ࡀ㗦ᩄ ࡛࠶ࡿࡇࡶࡑࡢ୍ࡘ࡛࠶ࡿࠋDy1 ࡀᙉ☢ᛶ⛛ ᗎࡍࡿࡇࡼࡾࠊDy2 ࡢ☢ሙᑐࡍࡿᛂ⟅ᛶ ࡀࡼࡃ࡞ࡾࠊ☢ሙࡼࡿࢮ࣮࣐࢚ࣥࢿࣝࢠ࣮పୗ ࡀ࠶ࡿࡓࡵࠊTN1ࡀ㧗 ࢩࣇࢺࡍࡿ⪃࠼ࡽࢀࡿࠋ 0 10 20 30 40 50-
Dy2S
3C
m/ J
K
-1mol
-1Hԋb
0 T 1 T2 T 3 T 5 T(a)
0 5 10 15 20 0 5 10 15 20-
Dy2S
3S
m/ J
K
-1mol
-1Hԋb
0 T1 T 2 T 5 T 3 T(b)
T / K
ᅗ2 α-R2S3༢⤖ᬗࡢ☢ሙ୰࡛ࡢ(a)☢Ẽẚ⇕ (b)☢Ẽ࢚ࣥࢺࣟࣆ࣮ࡢ ᗘ౫Ꮡᛶ TN1ࡢ㧗 ࢩࣇࢺప ഃTN2࡛ࡢ㌿⛣ࡢᾘኻࡀ ࡶຠ࠸࡚ࠊᅗ2(b)♧ࡍࡼ࠺ Cm/T ࢆ ᐃ᭱ ప ᗘ 0.4 K ࡽ ᗘ࡛✚ศࡋࡓ☢Ẽ࢚ࣥࢺࣟࣆ ࣮ࡣ☢ሙ༳ຍࡼࡾῶᑡࡋ࡚࠸ࡿ㸦|Sm| < 0㸧ࠋບ ☢Ọஂ☢▼ࡢ⏝ࢆᐃࡋࡓ☢ሙ 2 T ࡛ࡢ|Sm|α
α
- 36 - ᡁ ಟ㸪㜿Ἴຍ ῟㸪⸨ ⪔୍㑻
- 36 -
ࡣᑠࡉ࠸ࡀࠊ㉸ఏᑟ࣐ࢢࢿࢵࢺࡢ⏝ࢆᐃࡋࡓ5 T ࡛ࡣࡁ࡞|Sm|ࡀ☜ㄆࡉࢀࡿࠋ12 K ࡢ➼ ≧ែ ࡛5 T ࡢ☢ሙࢆ༳ຍࡋࠊ᩿⇕≧ែ࡛ᾘ☢ࡋࡓሙྜࡢ ᗘῶᑡࡣࠊᅗ2(b)ࡽTad= 5.8 K ぢ✚ࡶࡽࢀ ࡿࠋ☢Ẽ෭ᮦࡋ࡚᥋ࡍࡿ≀㉁ࡽ⇕ࢆዣ࠺ࡓ ࡵࡣࠊ༢య✚࠶ࡓࡾࡢ࢚ࣥࢺࣟࣆ࣮ῶᑡࡀ ࡁ࠸ᚲせࡀ࠶ࡿࡀࠊᮏ⣔ࡣDy2S3࠸࠺Ꮫᘧࡽ ࢃࡿࡼ࠺ᕼᅵ㢮ᐦᗘࡀప࠸ศ࡛࠶ࡿࠋࡋ ࡋࠊα-R2S3ࡢእሙᑐࡍࡿ≉␗࡞≀ᛶᛂ⟅ࢆ⏝ ࡋࠊ☢Ẽ⇕㔞ຠᯝࢆไᚚࡋᚓࢀࡤࠊእሙไᚚ࠸ ࠺ຍ౯್ࢆࡶࡗࡓ☢Ẽ෭ᮦࡀᐇ⌧ࡋᚓࡿࡢ࡛ ࡣ࡞࠸࠸࠺ほⅬ࡛ᇶ♏≀ᛶ◊✲ࢆ㐍ࡵ࡚࠸ࡿࠋ 5 ࡲࡵ ᕼᅵ㢮◲≀ α-R2S3༢⤖ᬗࡢ↓☢ሙୗ࠾ࡼࡧ☢ ሙ୰ẚ⇕ࢆ ᐃࡋࠊα-Gd2S3ࡢ෭ᮦࡋ࡚ࡢྍ⬟ ᛶࠊα-Dy2S3ࡢ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࢆぢฟࡋ ࡓࠋࡋࡋᐇᮦᩱࡋ࡚ࡢඃᛶࡘ࠸࡚ࡣࠊከ ࡃࡢ᳨ウࡍࡁㄢ㢟ࡀṧࡉࢀ࡚࠸ࡿࠋα-R2S3ࡢ☢Ẽ ⇕㔞ຠᯝࢆእሙไᚚࡍࡿྍ⬟ᛶࡘ࠸࡚ࡶࠊᚋ ࡉࡽ᳨ウࡋ࡚࠸ࡃࠋ ㅰ㎡ ᮏ◊✲ࡢ୍㒊ࡣJSPS ⛉◊㈝ 23540384 ࡢຓᡂࢆ ཷࡅ࡚࡞ࡉࢀࡲࡋࡓࠋ ཧ⪃ᩥ⊩(1) V. K. Pecharsky and K. A. Gschneidner, Jr., Giant Magnetocaloric Effect in Gd5(Si2Ge2), Phys. Rev. Lett.,
76 (1997) p4494-4497.
(2) V. K. Pecharsky and K. A. Gschneidner, Jr., Tunable magnetic regenerator alloys with a giant magnetocaloric effect for magnetic refrigeration from ~20 to ~290̴K, Appl. Phys. Lett., 70 (1997) p3299-3301.
(3) A. Fujita, S. Fujieda, Y. Hasegawa, and K. Fukamichi, Itinerant-electron metamagnetic transition and large magnetocaloric effects in La(FexSi1-x)13 compounds and
their hydrides, Phys. Rev. B, 67 (2003) 104416(12 pages).
(4) A. Fujita, S. Fujieda, K. Fukamichi, Y. Yamazaki, and Y. Iijima, Giant Magnetic Entropy Change in Hydrogenated La(Fe0.88Si0.12)13Hy Compounds, Mater. Trans., 43 (2002)
p653-655.
(5) H. Wada, and Y. Tanabe, Giant magnetocaloric effect of MnAs1−xSbx, Appl. Phys. Lett., 79 (2001) p3302- 3304.
(6) O. Tegus, E. Brück, K. H. J. Buschow, and F. R. de Boer, Transition-metal-based magnetic refrigerants for room- temperature applications, Nature, 415 (2002) p150- 152.
(7) S. Kikegawa, T. Matsumura, S. Murayama, H. Takano, and Y. Obi, Magnetic properties of amorphous Mn100_xCex alloys, Physica B, 329–333 (2003)
p1074–1076.
(8) S. Kikegawa, Y. Amakai, K. Asano, S. Murayama, H. Takano, and Y. Obi, Specific heat of amorphous Mn100-xCex alloys, J. Magn. Mag. Mater., 272-276 (2004)
p72-74.
(9) Y. Amakai, S. Murayama, Y. Obi, H. Takano, N. Momono, and K. Takanashi, Thermal expansion of structure-disordered heavy-fermion Ce alloys, J. Phys. Soc. Jpn., 80 (2011) SA057 (3 pages).
(10) N. Momono, S. Kuribayashi, Y. Amakai, S. Murayama, S Torii, and H. Takano, Stripe order and supercon- ductivity in the mechanically milled La1.6-xNd0.4SrxCuO4,
J. Phys.: Conf. Ser., 400 (2012) 022077 (4 pages). (11) S. Ebisu, Y. Iijima, T. Iwasa, and S. Nagata,
Antiferromag- netic transition and electrical conductivity in -Gd2S3, J. Phys. Chem. Solids, 65 (2004)
p1113-1120.
(12) S. Ebisu, M. Gorai, K. Maekawa, and S. Nagata, Highly Anisotropic Properties of Antiferromagnetic -Tb2S3
Single Crystal, AIP Conf. Proc., 850 (2006), p1237-1238.
(13) S. Ebisu, M. Narumi, and S. Nagata, Anomalous enlarge- ment of electrical resistivity between successive mag- netic transitions in -Dy2S3, J. Phys. Soc. Jpn., 75
(2006) 085002 (2 pages).
(14) S. Ebisu, M. Narumi, M. Gorai, S. Nagata, Successive magnetic phase transitions in -Dy2S3 single crystal, J.
Magn. Magn. Mater., 310 (2007) p1741-1743.
(15) S. Ebisu, K. Koyama, H. Omote, and S. Nagata, High field magnetization processes in single crystals of -Tb2S3 and -Dy2S3., J. Phys.: Conf. Ser., 150 (2009)
042027(4 pages).
(16) S. Ebisu, H. Omote, and S. Nagata, Drastic change of the electrical resistivity related to the novel magnetic phase transition in -Sm2S3, J. Phys.: Conf. Ser., 200 (2010)
092005(4 pages).
(17) S. Ebisu, K. Koyama, T. Horikoshi, M. Kokita and S. Nagata, Extremely broad hysteresis in the magnetization process of -Dy2S3 single crystal induced by high field
cooling, J. Phys.: Conf. Ser., 400 (2012), 032010 (4 pages).
(18) S. Ebisu, Y. Ushiki, and S. Takahashi, Specific-heat Study on Successive Magnetic Transitions in -Dy2S3
Single Crystals under Magnetic Fields, J. Kor. Phys. Soc., 63 (2013) p571-574.
(19) M. Matsuda, K. Kakurai, S. Ebisu, and S. Nagata, Succes- sive Magnetic Phase Transitions in -Tb2S3
Studied by Neutron Diffraction Technique, J. Phys. Soc. Jpn., 75 (2006) 074710 (4 pages).
(20) M. Matsuda, A. Kikkawa, K. Katsumata, S. Ebisu, and S. Nagata, Neutron Diffraction Study of -Gd2S3, J. Phys.
Soc. Jpn., 74 (2005) p1412-1415.
(21) A. Kikkawa, K. Katsumata, S. Ebisu, and S. Nagata, Phase transition of a frustrated -Gd2S3, J. Phys. Soc.
Jpn., 73 (2004) p2955-2958. ᡁ ಟ㸪㜿Ἴຍ ῟㸪⸨ ⪔୍㑻
- 36 -
ࡣᑠࡉ࠸ࡀࠊ㉸ఏᑟ࣐ࢢࢿࢵࢺࡢ⏝ࢆᐃࡋࡓ5 T ࡛ࡣࡁ࡞|Sm|ࡀ☜ㄆࡉࢀࡿࠋ12 K ࡢ➼ ≧ែ ࡛5 T ࡢ☢ሙࢆ༳ຍࡋࠊ᩿⇕≧ែ࡛ᾘ☢ࡋࡓሙྜࡢ ᗘῶᑡࡣࠊᅗ2(b)ࡽTad= 5.8 K ぢ✚ࡶࡽࢀ ࡿࠋ☢Ẽ෭ᮦࡋ࡚᥋ࡍࡿ≀㉁ࡽ⇕ࢆዣ࠺ࡓ ࡵࡣࠊ༢య✚࠶ࡓࡾࡢ࢚ࣥࢺࣟࣆ࣮ῶᑡࡀ ࡁ࠸ᚲせࡀ࠶ࡿࡀࠊᮏ⣔ࡣDy2S3࠸࠺Ꮫᘧࡽ ࢃࡿࡼ࠺ᕼᅵ㢮ᐦᗘࡀప࠸ศ࡛࠶ࡿࠋࡋ ࡋࠊα-R2S3ࡢእሙᑐࡍࡿ≉␗࡞≀ᛶᛂ⟅ࢆ⏝ ࡋࠊ☢Ẽ⇕㔞ຠᯝࢆไᚚࡋᚓࢀࡤࠊእሙไᚚ࠸ ࠺ຍ౯್ࢆࡶࡗࡓ☢Ẽ෭ᮦࡀᐇ⌧ࡋᚓࡿࡢ࡛ ࡣ࡞࠸࠸࠺ほⅬ࡛ᇶ♏≀ᛶ◊✲ࢆ㐍ࡵ࡚࠸ࡿࠋ 5 ࡲࡵ ᕼᅵ㢮◲≀ α-R2S3༢⤖ᬗࡢ↓☢ሙୗ࠾ࡼࡧ☢ ሙ୰ẚ⇕ࢆ ᐃࡋࠊα-Gd2S3ࡢ෭ᮦࡋ࡚ࡢྍ⬟ ᛶࠊα-Dy2S3ࡢ☢Ẽ෭ᮦࡋ࡚ࡢྍ⬟ᛶࢆぢฟࡋ ࡓࠋࡋࡋᐇᮦᩱࡋ࡚ࡢඃᛶࡘ࠸࡚ࡣࠊከ ࡃࡢ᳨ウࡍࡁㄢ㢟ࡀṧࡉࢀ࡚࠸ࡿࠋα-R2S3ࡢ☢Ẽ ⇕㔞ຠᯝࢆእሙไᚚࡍࡿྍ⬟ᛶࡘ࠸࡚ࡶࠊᚋ ࡉࡽ᳨ウࡋ࡚࠸ࡃࠋ ㅰ㎡ ᮏ◊✲ࡢ୍㒊ࡣJSPS ⛉◊㈝ 23540384 ࡢຓᡂࢆ ཷࡅ࡚࡞ࡉࢀࡲࡋࡓࠋ ཧ⪃ᩥ⊩(1) V. K. Pecharsky and K. A. Gschneidner, Jr., Giant Magnetocaloric Effect in Gd5(Si2Ge2), Phys. Rev. Lett.,
76 (1997) p4494-4497.
(2) V. K. Pecharsky and K. A. Gschneidner, Jr., Tunable magnetic regenerator alloys with a giant magnetocaloric effect for magnetic refrigeration from ~20 to ~290̴K, Appl. Phys. Lett., 70 (1997) p3299-3301.
(3) A. Fujita, S. Fujieda, Y. Hasegawa, and K. Fukamichi, Itinerant-electron metamagnetic transition and large magnetocaloric effects in La(FexSi1-x)13 compounds and
their hydrides, Phys. Rev. B, 67 (2003) 104416(12 pages).
(4) A. Fujita, S. Fujieda, K. Fukamichi, Y. Yamazaki, and Y. Iijima, Giant Magnetic Entropy Change in Hydrogenated La(Fe0.88Si0.12)13Hy Compounds, Mater. Trans., 43 (2002)
p653-655.
(5) H. Wada, and Y. Tanabe, Giant magnetocaloric effect of MnAs1−xSbx, Appl. Phys. Lett., 79 (2001) p3302- 3304.
(6) O. Tegus, E. Brück, K. H. J. Buschow, and F. R. de Boer, Transition-metal-based magnetic refrigerants for room- temperature applications, Nature, 415 (2002) p150- 152.
(7) S. Kikegawa, T. Matsumura, S. Murayama, H. Takano, and Y. Obi, Magnetic properties of amorphous Mn100_xCex alloys, Physica B, 329–333 (2003)
p1074–1076.
(8) S. Kikegawa, Y. Amakai, K. Asano, S. Murayama, H. Takano, and Y. Obi, Specific heat of amorphous Mn100-xCex alloys, J. Magn. Mag. Mater., 272-276 (2004)
p72-74.
(9) Y. Amakai, S. Murayama, Y. Obi, H. Takano, N. Momono, and K. Takanashi, Thermal expansion of structure-disordered heavy-fermion Ce alloys, J. Phys. Soc. Jpn., 80 (2011) SA057 (3 pages).
(10) N. Momono, S. Kuribayashi, Y. Amakai, S. Murayama, S Torii, and H. Takano, Stripe order and supercon- ductivity in the mechanically milled La1.6-xNd0.4SrxCuO4,
J. Phys.: Conf. Ser., 400 (2012) 022077 (4 pages). (11) S. Ebisu, Y. Iijima, T. Iwasa, and S. Nagata,
Antiferromag- netic transition and electrical conductivity in -Gd2S3, J. Phys. Chem. Solids, 65 (2004)
p1113-1120.
(12) S. Ebisu, M. Gorai, K. Maekawa, and S. Nagata, Highly Anisotropic Properties of Antiferromagnetic -Tb2S3
Single Crystal, AIP Conf. Proc., 850 (2006), p1237-1238.
(13) S. Ebisu, M. Narumi, and S. Nagata, Anomalous enlarge- ment of electrical resistivity between successive mag- netic transitions in -Dy2S3, J. Phys. Soc. Jpn., 75
(2006) 085002 (2 pages).
(14) S. Ebisu, M. Narumi, M. Gorai, S. Nagata, Successive magnetic phase transitions in -Dy2S3 single crystal, J.
Magn. Magn. Mater., 310 (2007) p1741-1743.
(15) S. Ebisu, K. Koyama, H. Omote, and S. Nagata, High field magnetization processes in single crystals of -Tb2S3 and -Dy2S3., J. Phys.: Conf. Ser., 150 (2009)
042027(4 pages).
(16) S. Ebisu, H. Omote, and S. Nagata, Drastic change of the electrical resistivity related to the novel magnetic phase transition in -Sm2S3, J. Phys.: Conf. Ser., 200 (2010)
092005(4 pages).
(17) S. Ebisu, K. Koyama, T. Horikoshi, M. Kokita and S. Nagata, Extremely broad hysteresis in the magnetization process of -Dy2S3 single crystal induced by high field
cooling, J. Phys.: Conf. Ser., 400 (2012), 032010 (4 pages).
(18) S. Ebisu, Y. Ushiki, and S. Takahashi, Specific-heat Study on Successive Magnetic Transitions in -Dy2S3
Single Crystals under Magnetic Fields, J. Kor. Phys. Soc., 63 (2013) p571-574.
(19) M. Matsuda, K. Kakurai, S. Ebisu, and S. Nagata, Succes- sive Magnetic Phase Transitions in -Tb2S3
Studied by Neutron Diffraction Technique, J. Phys. Soc. Jpn., 75 (2006) 074710 (4 pages).
(20) M. Matsuda, A. Kikkawa, K. Katsumata, S. Ebisu, and S. Nagata, Neutron Diffraction Study of -Gd2S3, J. Phys.
Soc. Jpn., 74 (2005) p1412-1415.
(21) A. Kikkawa, K. Katsumata, S. Ebisu, and S. Nagata, Phase transition of a frustrated -Gd2S3, J. Phys. Soc.
Jpn., 73 (2004) p2955-2958.
ᐊᕤ⣖せ➨63 ྕ㸦2013㸧 37㹼40
- 37 -
ᵓ㐀౫Ꮡᕼᅵ㢮ྜ㔠ࡢ㛤Ⓨ☢Ẽ⇕㔞࣭⇕ᙎᛶᮦᩱࡢᒎ㛤
㞵ᾏ
᭷భ
*1, *2㸪ሷᑼ
Ὀᗈ
*3㸪㕥ᮌ
ᣅஓ
*3㸪▼ཎ
ᆂ
*3㸪ᮧᒣ
ⱱᖾ
*1, *2Development of Magnetocaloric and Thermoelastic Materials in
Structure-dependent Rare-earth Alloys
Yusuke AMAKAI
*1, *2, Yasuhiro SHIOJIRI
*3, Takuya SUZUKI
*3Kei ISHIHARA
*3, and Shigeyuki MURAYAMA
*1, *2㸦ཎ✏ཷ᪥ ᖹᡂ
25 ᖺ 9 ᭶ 30 ᪥ ㄽᩥཷ⌮᪥ ᖹᡂ 26 ᖺ 1 ᭶ 24 ᪥㸧
Abstract
This study aims to develop next-generation high-performance materials with utilizing the strongly correlated electronic properties in amorphous Ce-alloys. We have focused amorphous Ce-Mn alloys consisting of the rare-earth metal cerium and the transition metal manganese. We have measured the magnetostriction for amorphous Ce-Mn alloys where a large thermal expansion and anomalous temperature dependence observed. The thermal expansion of the low temperature for amorphous Ce-Mn alloys has been found to be controlled by a magnetic field. In the future, we aim at development of the drive actuator element under the control of the temperature and magnetic field. Keywords : Strongly correlated electron, Amorphous alloys, Thermal expansion, Magnetostriction
1 ࡣࡌࡵ ᕼᅵ㢮ඖ⣲ࢆྵࡴ㔠ᒓ㛫ྜ≀ࡸྜ㔠ࡣ㸪ᕼᅵ 㢮ࡢ㟁Ꮚࡀ≉ᐃࡢ㌶㐨㸦4f ㌶㐨㸧᮰⦡ࡉࢀࡿࡓ ࡵᒁᅾᛶࡀᙉࡃ㸪㟁Ꮚྠኈࡢࢡ࣮ࣟࣥ┦స⏝ࡀ ↓ど࡛ࡁ࡞࠸ࡓࡵ㸪ᙉ࠸㟁Ꮚ┦㛵㸦ᙉ┦㛵㟁Ꮚ≧ ែ㸧ࢆᐇ⌧ࡍࡿ㸬ࡇࡢᙉ┦㛵㟁Ꮚ≧ែࡣ㸪ᕧ⇕ ᐜ㔞࣭ወጁ࡞☢Ẽ┦㌿⛣࣭ᕧ☢Ẽᢠ࣭␗ᖖ⇕ ⭾ᙇ࣭⇕㟁ኚ≉ᛶ࣭㠀ᚑ᮶ᆺ㉸ఏᑟ࡞ከᙬ࡛ 㨩ຊⓗ࡞≀ᛶࢆ♧ࡍࡇࡀ▱ࡽࢀ࡚࠸ࡿࠋࡇࢀࡽ ࡢ≉ᛶࡣ㸪⤖ᬗᵓ㐀ࡸእሙ㸦☢ሙ࣭ ᗘ࣭ᅽຊ࣭ 㟁ሙ➼㸧ࡼࡗ࡚ࡁࡃ≉ᛶࢆኚࡉࡏࡿ㸬ᚑࡗ ࡚ᕼᅵ㢮ࢆྵࡴ㔠ᒓ㛫ྜ≀ࡸྜ㔠ࡣ㸪ࡕࡻࡗ ࡋࡓࢳ࣮ࣗࢽࣥࢢࡼࡗ࡚᭷ᮃ࡞ḟୡ௦ࡢ㧗ᶵ⬟ ᮦᩱࡋ࡚᭷ຊ࡞ྍ⬟ᛶࢆ⛎ࡵ࡚࠸ࡿ㸬 *1 ᐊ⹒ᕤᴗᏛ ࡋࡃࡳሗ⣔㡿ᇦ *2 ᐊ⹒ᕤᴗᏛ ⎔ቃㄪᮦᩱᕤᏛ◊✲ࢭࣥࢱ࣮ *3 ᐊ⹒ᕤᴗᏛ ᛂ⏝⌮Ꮫ⣔ᑓᨷ ᡃࠎࡣ㸪ᕼᅵ㢮ඖ⣲ࡢࢭ࣒ࣜ࢘㸦Ce㸧ࢆྵ ࡴ㸪༢⤖ᬗࡽᵓ㐀つ๎㸦ࣔࣝࣇࢫ㸧࡞ ࡢᵝࠎ࡞ᵓ㐀ࢆᣢࡘᕼᅵ㢮ྜ≀࠾ࡼࡧྜ㔠ࡢ㛤 Ⓨ㟁Ꮚ≀ᛶࡘ࠸࡚◊✲ࢆ⾜ࡗ࡚ࡁࡓ㸬ࡇࢀࡲ ࡛ࡢᡂᯝࡽ㸪ᙉ┦㛵㟁Ꮚࡀ㛵ࡋࡓᵝࠎ࡞㟁Ẽ ఏᑟᛶࡸ⇕≉ᛶࢆぢฟࡋ࡚ࡁࡓࡀ㸪≉㸪ࣔࣝ ࣇࢫ(a-)Ce ྜ㔠㛵ࡋ࡚㸪つ๎࡞ᵓ㐀࠾࠸࡚ ࡶᙉ┦㛵㟁Ꮚ≧ែࡀᐇ⌧ࡍࡿࡇࢆึࡵ࡚ぢฟࡋ ࡓ㸬ࡑࡇ࡛㸪≉ࣔࣝࣇࢫྜ㔠ࢆ◊✲ᑐ㇟ ࡋ࡚㸪≀㉁㛤Ⓨࢆ⾜࠸᪂ࡓ࡞ᶵ⬟ᛶᮦᩱࡋ࡚ࡢ ྍ⬟ᛶࢆ᥈ࡗࡓ㸬ࣔࣝࣇࢫྜ㔠ࡢ◊✲ࡢⅬ ࡣ㸪ձ⤖ᬗྜ≀ࡋ࡚Ꮡᅾࡋ࡞࠸ඖ⣲ᵓᡂࡢྜ 㔠స〇ࡀྍ⬟㸪ղ௵ពࡢ⤌ᡂẚ࡛ไᚚࡋࡓヨᩱస 〇ࡀྍ⬟㸪ճ☢Ẽ␗᪉ᛶࡀ࡞࠸࡞ࡢ≉㛗ࢆᣢࡘ ࡓࡵ㸪≀㉁㛤Ⓨࡢ⮬⏤ᗘࡀ㠀ᖖ㧗࠸㸬ࡉࡽ㸪 ࣐ࢡࣟᆒ㉁࡞≉ᛶࡀᚓࡽࢀࡿࡇࡽ㸪ᮦᩱ≀ ᛶࡢほⅬࡽࡶ᭷࡛࠶ࡿゝ࠼ࡿ㸬ࡑࡇ࡛ᮏࢱ ࢫࢡࣇ࢛࣮ࢫ◊✲࡛ࡣ㸪ᕼᅵ㢮ඖ⣲ࡢCe ࢆ୰ᚰ ࡋࡓࣔࣝࣇࢫ࡞ࡢᵝࠎ࡞ᵓ㐀ࢆᣢࡘ㔠ᒓ㛫