Ultrasonic Team (T. Yanagisawa, Hokkaido Univ,)    

研究日誌
2008-8/1「超音波装置セットアップ間近」

Aug 01, 2008

Rerearch Photo 20080801

2月に赴任してから着々と準備を進めてきた超音波装置のセットアップもいよいよ佳境にはいっています。
必要な機器と部品を全て揃え、近日中にキャリブレーションを兼ねた実験を行う予定です。
実験系研究室のセットアップには、お金がかかります。。。そのため中古機器や古い資産をうまく活用して、高精度の測定システムを組むべく知恵を絞っています。写真のネットワークアナライザHP8753Eは、10年前のヒューレットパッカード製の名機。当時の販売価格はなんと350万円(>_<)!ですが、秋葉原やWeb上をくまなく探して、価格は5分の1程度にもかかわらず質の良いリセール品を見つけることができました。まだまだ現役で使えます。

Start-up of the ultrasonic apparatus at our lab. is about to be completed, since it was prepared from Feb. when I have been started for my new post here. Now we are planning to perform preliminary experiment as system calibrations.
Generally, set upping an experimental laboratory has some costs of its own. We try to make a high-accuracy measurement system by utilize old equipments and secondhand equipment, sometimes. The top picture shows famous network analyzer HP8753E, which was selled a decade ago with list price of over $30000! Luckily, we could get a re-sell one with fifth list price due to all the effort for searching on Web and Akihabara. It’s still on active duty☺

研究日誌 2008-7/18「単結晶育成中」

Jul 18, 2008

Rerearch Photo 20080718

チョクラルスキー法とフラックス法を駆使して単結晶試料を鋭意育成中!
RA(リサーチアシスタント)の森下君とM1の真山君(共に 理学部 極低温研究室 所属)がサポートしてくれています。

Now we are start growing single x-tals of rare-earth compounds by using Czochralski- and molten flux-method.
Mr. Morishita (RA) and Mr. Mayama (Grad. Student from VLT Lab. at Grad. School of Science)are helping me out.


Topics: Discovery of Double Ultrasonic Dispersion due to Rattling in NdOs4Sb12

Jul 10, 2008

日本語解説 >> Topics「カゴ状化合物のラットリング

Ultrasonic investigation of the off-center rattling in the filled skutterudite compound NdOs4Sb12
Tatsuya Yanagisawa, Pei-Chun Ho, William M. Yuhasz, M. Brian Maple, Yuri Yasumoto, Hiromu Watanabe, Yuichi Nemoto, and Terutaka Goto

The off-center rattling of Nd rare-earth ions in the filled skutterudite compound NdOs4Sb12 has been investigated by ultrasonic measurement. The longitudinal C11 mode for frequencies between 34 and 253 MHz shows a marked frequency dependence in elastic constant and ultrasonic attenuations at two different temperatures centered at around 45 and 15 K. The relaxational frequency dependence of ultrasonic dispersion reveals a thermally activated Γ23-type off-center motion of Nd-ions, involving local charge fluctuations with Γ23 symmetry in the (OsSb3)4 cage. An attempt time τ0,(1)=7.5×10-12 s and an activation energy E1=337 K were obtained from fits to the dispersion at around 45 K. The presence of another dispersion at lower temperatures of around 15 K implies that the rattling in NdOs4Sb12 has an additional low-energy excitation characterized by a lower activation energy E2∼67 K with an attempt time τ0,(2)=5.1×10-11 s.

J. Phys. Soc. Jpn. 77 (2008) 074607.

NdOs_4Sb_12 Ultrasonic Dispersion

Figure (a) Relative change in elastic constant ΔC11/C11 as function of temperature at frequencies of 34, 108, 180, and 253 MHz. (b) Solid lines show calculations of ΔC11/C11 using Landau-Khalatnikov theory. Dotted lines indicate the higher-frequency limit of the elastic constant C and the low frequency limit C0. Arrows indicate the temperatures that satisfy the resonant condition of ω ∼ 1/τi. (c) Temperature dependence of ultrasonic attenuation coefficient α11 at frequencies of 34, 108, 180, and 253 MHz. Solid lines are theoretical fits using the parameters.

(*This research was performed at UC San Diego and Niigata University in 2006.)

「実験手法」 -Method-

Jul 07, 2008

 

図1 さまざまな極限環境(極低温・強磁場・高圧力)における物質中の電子の挙動を、超音波を使って調べています。

 

Q 電気四極子(でんきしきょくし)って何ですか?
A 原子の持つ異方的な電荷分布を表す物理量です。
 

  元素は原子核と電子から構成されており、電子は原子核の周りを公転運動しています。元素は固体中や水溶液中に入るとイオン化し、最も外側を回る電子をいくつか放出します。残りの電子は原子核に束縛されており、特に金属化合物を構成するような原子番号の大きな(電子を沢山持った)元素の持つ電子は原子核の周りに球状の電子雲を形成しています。その球状電子分布は、数学的にさまざまな形の電荷分布の重ね合わせとして理解できます。これを専門的に表現すると「イオンが持つ局在電子の異方的な静電ポテンシャルを高次展開する」となります。対称性を保つために、その次数は2・4・8・16…と2の指数になります。電気四極子(electric quadrupole クアドゥルポール)とは、そのうちの蝶のような形をした二次の成分で、電子の軌道自由度に由来する二階のテンソル量として表現されます。

この記事には続きがあります:続きを読む ...

Abstract

Apr 29, 2008
Thermodynamic and transport studies of the ferromagnetic filled skutterudite compound PrFe4As12
T. A. Sayles, W. M. Yuhasz, J. Paglione, T. Yanagisawa, J.R. Jeffries, M.B. Maple, Z. Henkie, A. Pietraszko, T. Cichorek, R. Wawryk, Y. Nemoto and T. Goto

A variety of thermodynamic and transport measurements were made on high-quality single crystals of the Pr-based filled skutterudite compound PrFe4As12. Abrupt features in magnetization, ac susceptibility, specific heat, resistivity, thermoelectric power, and ultrasonic velocity reveal the onset of long range ferromagnetic order below ThetaC=18 K. The low-temperature magnetic susceptibility is characterized by a Curie–Weiss law with an effective moment of 3.52µB/f.u. and a saturation magnetization of 2.3µB/f.u., which is consistent with a magnetic Γ5 triplet ground state. A gaplike reduction of the large electronic specific heat coefficient of 340 mJ/mol K2 and several other features point to a strongly correlated electron behavior that is likely coupled to a change in magnetic and/or structural order near T*~12 K. Furthermore, this complex magnetic state is found to be strongly field dependent, as evidenced by a change in the easy axis at low fields and an additional contribution to thermal conductivity appearing only at high fields.

Phys. Rev. B 77 (2008) 144432. (Editor's Suggested).

PrFe4As12 combinedfigure

Figure : A comparison of low-temperature specific heat, electrical resistivity, magnetization, ac susceptibility,
thermopower, and ultrasound data that are used to correlate features that are observed at the ferromagnetic ordering temperatureThetac = 18 K and the characteristic temperature T*= 12 K and T' = 10 K.

Upper: Temperature derivative of resistivity and electronic plus magnetic contributions to specific heat, which shows a striking resemblance of the temperature dependence of each throughout the entire range.

Middle: Low-field (5 mT) dc magnetization and the imaginary part of the ac susceptibility, highlighting the coincidence of both the irreversibility temperature in M(T) and the peak in Chi_ac(T) with T*.

Lower* Zero-field thermoelectric power and relative change in the elastic constant ΔC44/C44 as a function of temperature for PrFe4As12.

(* This research was performed at UC San Diego and Niigata University in 2006-2007)
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