Photosalient 7 図 Å 2 HOMO 5d z 2 図 2 HOMO dσ dσ* 図 2 HOMO dσ* 図 2 HOMO 7 HOMO 1 図 2 8 Au CN nm 2.0 ns 図 3 Au CN 2 3 図 2 Schematic repr

Size: px
Start display at page:

Download "Photosalient 7 図 Å 2 HOMO 5d z 2 図 2 HOMO dσ dσ* 図 2 HOMO dσ* 図 2 HOMO 7 HOMO 1 図 2 8 Au CN nm 2.0 ns 図 3 Au CN 2 3 図 2 Schematic repr"

Transcription

1 最近の研究から 金属間相互作用の増強が鍵となる光誘起結晶相転移と Photosalient 効果 Tomohiro SEKI and Hajime ITO: Photoinduced Crystalline Structure Change and Photosalient Effect through Strengthening Metallophilic Interaction We report the first photoinduced single-crystal-to-single-crystal SCSC phase transition of a gold complex 1 that involves strengthening of intermolecular aurophilic interactions. This is also the first solid state photochromism of gold complexes. Upon UV irradiation, blue-emitting crystals 1B of aryl gold I isocyanide complex 1 transform into the weakly yellow-emitting crystals 1Y. X-ray diffraction analyses exhibit that the phase transition proceeds in an SCSC manner. After phase transition from 1B to 1Y, the intermolecular Au Au separation decreases from to Å, resulting in a red-shifted emission. The photoinduced strengthening of the aurophilic interactions in the excited state initiates the change in the crystal structure from 1B to 1Y. Moreover, crystal 1B showed a photosalient effect: the 1B crystals jump upon irradiation with strong UV light owing to the phase transition into 1Y. The photoinduced strengthening of aurophilic interactions in the crystal generate the sudden mechanical movement of the crystal. 1. はじめに 1 1 Nature 図 1 2 図 1 Photochromism of the crystal of diarylethene derivative. 365 nm 金原子間相互作用とその光応答特性

2 Photosalient 7 図 Å 2 HOMO 5d z 2 図 2 HOMO dσ dσ* 図 2 HOMO dσ* 図 2 HOMO 7 HOMO 1 図 2 8 Au CN nm 2.0 ns 図 3 Au CN 2 3 図 2 Schematic representation of aurophilic bonds and their simplified orbital levels. dσ dσ* dσ* HOMO 1 Au CN Au CN I 1 図 4 図 3 Au CN 2 3 Schematic representation of the relaxation pathway upon photoirradiation of Au CN 2 3 complexes 図 Structures of

3 3. 金イソシアニド錯体 1の光誘起結晶相転移 3.1 アリール金イソシアニド錯体 Photosalient 3.2 金イソシアニド錯体 1の紫外光照射に伴う結晶相転移 1 1B 図 5 1B Φ em nm 図 6 λ em,max 448 nm 450 nm 371 nm 400 nm 1B X _ P1 R wr GOF a Å b Å c Å α β γ Z 4 V Å 3 d g cm 3 図 7 1B R 1 wr 2 X 1Y X 1 H NMR 図 6 1B 1Y Excitation and emission spectra of 1B and 1Y. 1B 450 nm 1Y 590 nm 1B 370 nm 1Y 390 nm Inset 1Y. τ av 34.2 μs 590 nm 1B 図 5 1B 1Y A series of photographs of the SCSC phase transition from 1B to 1Y induced by strong photoirradiation 367 nm, approx. 100 mw cm 2 taken under excitation at 365 nm. 図 7 1B The single-crystal structure of 1B. a ORTEP b ORTEP c CPK ORTEP

4 Photosalient Head-to-tail Å 1B 1Y 図 nm 100 mw cm 2 60 s 1B 図 5 1Y 5 mw cm 2 1B 10 1Y Φ em 0.5 λ em, max 580 nm 図 6 1B 132 nm 図 6 23 nm580 nm τ av μs 1B τ av 50 1Y X 1B 1B 1Y X 1B 1Y _ 1Y P1 R wr GOF a Å b Å c Å α β γ Z 2 V Å 3 d g cm 3 図 8 1 H NMR 1Y Head-to-tail 1B B 1Y 2 1Y 図 8 1Y The single-crystal structure of 1Y. a ORTEP b ORTEP c CPK ORTEP Å 1B 0.2 Å 3.3 励起状態における金原子間相互作用の増強を利用した光誘起結晶相転移 1 1B 1Y 1B 1B 1Y 1B 1Y 120 DSC B 1Y nm 200 mw cm 2 1B 1B 1Y 1B 1B 1Y 229

5 1B DFT PBEPBE/ SDD 1B 図 9 HOMO 図 2 1B 1B 1B 3 1T Opt 1B 1T Opt 図 9 Head-to-tail 2.86 Å 1B 3 図 2 HOMO 1T Opt 1Y 図 9 1B 1B 1Y 1B 1Y 3.4 Photosalient 効果 1 Photosalient Salient 図 Salient Thermosalient Photosalient Salient Photosalient 1 Photosalient mw cm nm Photosalient 図 mw cm 2 図 10 Salient Schematic representation of salient effect. 図 9 1B 1T Opt 1Y Comparison of the structures and frontier orbital levels and the corresponding molecular orbitals of 1B, 1T Opt, and 1Y. 図 11 1 Photosalient A series of photographs of the photosalient effect of 1B through the transformation into 1Y induced by strong photoirradiation 367 nm, approx. 400 mw cm 2. d

6 Photosalient 1B 5 図 11a b 1B 1Y 図 11c 21 図 11d 1 1B Photosalient 1B Salient 16 1 Photosalient Photosalient Photosalient1 Salient 1 Photosalient 1B 1Y Salient Naumov Salient 16 Salient Thermosalient X Salient Salient 1 V/Z Δ V/Z Δ V/Z 25 Å 3 1 Naumov Salient _ P1 Δ V/Z 6.8 Å Photosalient Naumov Salient 1 4. おわりに 1 1B Photosalient 1 Photosalient 5 文献 1 a J. Zhang, Q. Zou and H. Tian: Adv. Mater. 25, ; b M. Irie, T. Fukaminato, K. Matsuda and S. Kobatake: Chem. Rev. 114, S. Kobatake, S. Takami, H. Muto, T. Ishikawa and M. Irie: Nature 446, O. S. Bushuyev, A. Tomberg, T. Friscic and C. J. Barrett: J. Am. Chem. Soc. 135, J. W. Chung, S.-J. Yoon, B.-K. An and S. Y. Park: J. Phys. Chem. C 117, S. Iyengar and M. C. Biewer: Cryst. Growth Des. 5, N. K. Nath, L. Pejov, S. M. Nichols, C. Hu, N. Saleh, B. Kahr and P. Naumov: J. Am. Chem. Soc. 136, a A. L. Balch: Gold Bull. 37, ; b P. Pyykko: Angew. Chem., Int. Ed. 43, ; c V. W. Yam and E. C. Cheng: Chem. Soc. Rev. 37, a G. Cui, X. Y. Cao, W. H. Fang, M. Dolg and W. Thiel: Angew. Chem., Int. Ed. 52, ; b H. H. Patterson, S. M. Kanan and M. A. Omary: Coord. Chem. Rev. 208, a M. Iwamura, K. Nozaki, S. Takeuchi and T. Tahara, J. Am. Chem. Soc. 135, ; b K. H. Kim, J. G. Kim, S. Nozawa, T. Sato, K. Y. Oang, T. W. Kim, H. Ki, J. Jo, S. Park and C. Song: Nature 518, a K. Haldrup, T. Harlang, M. Christensen, A. Dohn, T. B. van Driel, K. S. Kjaer, N. Harrit, J. Vibenholt, L. Guerin, M. Wulff and M. M. Nielsen: Inorg. Chem. 50, ; b R. M. van der Veen, C. J. Milne, A. El Nahhas, F. A. Lima, V. T. Pham, J. Best, J. A. Weinstein, C. N. Borca, R. Abela, C. Bressler and M. Chergui: Angew. Chem., Int. Ed. 48, H. Ito, T. Saito, N. Oshima, N. Kitamura, S. Ishizaka, Y. Hinatsu, 231

7 M. Wakeshima, M. Kato, K. Tsuge and M. Sawamura: J. Am. Chem. Soc. 130, a Y. Sagara and T. Kato: Nat. Chem. 1, ; b A. L. Balch: Angew. Chem. Int. Ed. 48, ; c C. Jobbágy and A. Deák, Eur. J. Inorg. Chem. 2014, a K. Kawaguchi, T. Seki, T. Karatsu, A. Kitamura, H. Ito and S. Yagai: Chem. Commun. 49, ; b T. Seki, T. Ozaki, T. Okura, K. Asakura, A. Sakon, H. Uekusa and H. Ito: Chem. Sci. 6, a T. Seki, K. Sakurada and H. Ito: Angew. Chem., Int. Ed. v52, ; b H. Ito, M. Muromoto, S. Kurenuma, S. Ishizaka, N. Kitamura, H. Sato and T. Seki: Nat. Commun. 4, T. Seki, K. Sakurada, M. Muromoto and H. Ito: Chem. Sci. 6, a N. K. Nath, M. K. Panda, S. C. Sahoo and P. Naumov: CrystEngComm 16, ; b S. C. Sahoo, M. K. Panda, N. K. Nath and P. Naumov: J. Am. Chem. Soc. 135, a M. C. Etter and A. R. Siedle: J. Am. Chem. Soc. 105, ; b I. Colombier, S. Spagnoli, A. Corval, P. Baldeck, M. Giraud, A. Léaustic and P. Yu: Mol. Cryst. Liq. Cryst. 431, プロフィール Tomohiro SEKI Faculty of Engineering, Frontier Chemistry Center, Hokkaido University Kita 13 Nishi 8 Kita-ku, Sapporo, Hokkaido , Japan seki@eng.hokudai.ac.jp Hajime ITO Faculty of Engineering, Frontier Chemistry Center, Hokkaido University Kita 13 Nishi 8 Kita-ku, Sapporo, Hokkaido , Japan hajito@eng.hokudai.ac.jp

1

1 4 Nano Device Technologies From New Functions of Extreme Substances to Telecommunication Technologies 4-1 Controlling Intermolecular Interactions using Nano- Structural Molecules OTOMO Akira, YOKOYAMA

More information

X線分析の進歩45

X線分析の進歩45 Advances in X-Ray Chemical Analysis, Japan, 45 (2014) ISSN 0911-7806 NaCl Color Center in NaCl Takuya TSUJI, Hiroyuki IWASAKI and Jun KAWAI NaCl Color Center in NaCl Takuya TSUJI, Hiroyuki IWASAKI and

More information

Degradation Mechanism of Ethylene-propylene-diene Terpolymer by Ozone in Aqueous Solution Satoshi MIWA 1 *, 2, Takako KIKUCHI 1, 2, Yoshito OHTAKE 1 a

Degradation Mechanism of Ethylene-propylene-diene Terpolymer by Ozone in Aqueous Solution Satoshi MIWA 1 *, 2, Takako KIKUCHI 1, 2, Yoshito OHTAKE 1 a Degradation Mechanism of Ethylene-propylene-diene Terpolymer by zone in Aqueous Solution Satoshi MIWA 1, 2, Takako KIKUCHI 1, 2, Yoshito TAKE 1 and Keiji TANAKA 2 ( 1 Chemicals Evaluation and Research

More information

X X 1. 1 X 2 X 195 3, 4 Ungár modified Williamson-Hall/Warren-Averbach 5-7 modified modified Rietveld Convolutional Multiple Whole Profile CMWP 8 CMWP

X X 1. 1 X 2 X 195 3, 4 Ungár modified Williamson-Hall/Warren-Averbach 5-7 modified modified Rietveld Convolutional Multiple Whole Profile CMWP 8 CMWP X X a a b b c Characterization of dislocation evolution during work hardening of stainless steels by using XRD line-profile analysis Tomoaki KATO a, Shigeo SATO a, Yoichi SAITO b, Hidekazu TODOROKI b and

More information

1 2 2 (Dielecrics) Maxwell ( ) D H

1 2 2 (Dielecrics) Maxwell ( ) D H 2003.02.13 1 2 2 (Dielecrics) 4 2.1... 4 2.2... 5 2.3... 6 2.4... 6 3 Maxwell ( ) 9 3.1... 9 3.2 D H... 11 3.3... 13 4 14 4.1... 14 4.2... 14 4.3... 17 4.4... 19 5 22 6 THz 24 6.1... 24 6.2... 25 7 26

More information

untitled

untitled 3 4 4 2.1 4 2.2 5 2.3 6 6 7 4.1 RC 7 4.2 RC 8 4.3 9 10 5.1 10 5.2 10 11 12 13-1 - Bond Behavior Between Corroded Rebar and Concrete Ema KATO* Mitsuyasu IWANAMI** Hiroshi YOKOTA*** Hajime ITO**** Fuminori

More information

Laser Ablation Dynamics of Amorphous Film of a Cu-Phthalocyanine Derivative Masahiro HOSODA*,**, Hiroshi FURUTANI*,**. Hiroshi FUKUMURA*,** Hiroshi MASUHARA*, Masanobu NISHII*** Nobuyuki ICHINOSE**,***,

More information

The Phase Behavior of Monooleoylglycerol-Water Systems Mivoshi Oil & Fat Co.. Ltd. Faculty of Science and Technology, Science University of Tokyo Inst

The Phase Behavior of Monooleoylglycerol-Water Systems Mivoshi Oil & Fat Co.. Ltd. Faculty of Science and Technology, Science University of Tokyo Inst The Phase Behavior of Monooleoylglycerol-Water Systems Mivoshi Oil & Fat Co.. Ltd. Faculty of Science and Technology, Science University of Tokyo Institute of Colloid and Interface Science, Science University

More information

LLG-R8.Nisus.pdf

LLG-R8.Nisus.pdf d M d t = γ M H + α M d M d t M γ [ 1/ ( Oe sec) ] α γ γ = gµ B h g g µ B h / π γ g = γ = 1.76 10 [ 7 1/ ( Oe sec) ] α α = λ γ λ λ λ α γ α α H α = γ H ω ω H α α H K K H K / M 1 1 > 0 α 1 M > 0 γ α γ =

More information

Fundamental Study on the SOX Gas Sensor Utilizing Beta-Alumina with Sputtered Praseodymium Oxide Thin Films by Shinya YAO1*, Kenji MIYAGAWA1, Shigeru

Fundamental Study on the SOX Gas Sensor Utilizing Beta-Alumina with Sputtered Praseodymium Oxide Thin Films by Shinya YAO1*, Kenji MIYAGAWA1, Shigeru Fundamental Study on the SOX Gas Sensor Utilizing Beta-Alumina with Sputtered Praseodymium Oxide Thin Films by Shinya YAO1*, Kenji MIYAGAWA1, Shigeru IIJIMA2 and Zensaku KOZUKA1 1. Faculty of Engineering,

More information

薄膜結晶成長の基礎3.dvi

薄膜結晶成長の基礎3.dvi 3 464-8602 1 [1] 2 3 (epitaxy) (homoepitaxy) (heteroepitaxy) 1 Makio Uwaha. E-mail:uwaha@nagoya-u.jp; http://slab.phys.nagoya-u.ac.jp/uwaha/ 2 3.1 [2] (strain) r u(r) ɛ αγ (r) = 1 ( uα + u ) γ (3.1) 2

More information

<966B91E58C6F8DCF8A77959493AF918B89EF89EF95F18E8F5F8DC58F495F8B5E8E9790462E696E6464>

<966B91E58C6F8DCF8A77959493AF918B89EF89EF95F18E8F5F8DC58F495F8B5E8E9790462E696E6464> 1 Hokkaido University Faculty of Economics ;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;; 2 Hokkaido University Faculty of Economics ;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;; 3 Hokkaido University Faculty of Economics ;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;;

More information

寄稿論文 規則性無機ナノ空間が創り出す新しい触媒能 | 東京化成工業

寄稿論文 規則性無機ナノ空間が創り出す新しい触媒能 | 東京化成工業 MCM-41 M41 MCM-41 M41 2 3 m 2 /g nm nm Mn Ti Ti H N 2 S Ti-MCM-41, H H N H H 2 2 -Urea, CH 2 Cl 2, H 2 S + S 1b 2b 3b 54%, 58% ee Ti M41 H 2 As 4 ZP 4 ZP ZS ZS 5 Me Me Me Me M41 / 15 mg MeH 1.0 mmol 89%

More information

X線分析の進歩36 別刷

X線分析の進歩36 別刷 X X X-Ray Fluorescence Analysis on Environmental Standard Reference Materials with a Dry Battery X-Ray Generator Hideshi ISHII, Hiroya MIYAUCHI, Tadashi HIOKI and Jun KAWAI Copyright The Discussion Group

More information

結晶成長学からの提案

結晶成長学からの提案 Vol.No. 2003 1 Abstract µ 1 Vol.No. 2003 1 σ = µ / k B T = ln(c / C e ) µ k B 2 Vol.No. 2003 1 Fig. 1. Protein crystals and their surfaces observed in various size scales. (a) An optical micrograph of

More information

Molecule tomic rbital bridied tomic rbital Valence Shell Electron Pair Repulsion Rule Molecular rbital 2 1+ + 1+ 1+ 1+ 2 9+ + 9+ 9+ 9+ 2 1+ 1+ 1s 1s 2 9+ 9+ 2p 2p 9+ () 2 (2p ) 2 (2p ) 2 (2p ) 1 Energ

More information

C-2 NiS A, NSRRC B, SL C, D, E, F A, B, Yen-Fa Liao B, Ku-Ding Tsuei B, C, C, D, D, E, F, A NiS 260 K V 2 O 3 MIT [1] MIT MIT NiS MIT NiS Ni 3 S 2 Ni

C-2 NiS A, NSRRC B, SL C, D, E, F A, B, Yen-Fa Liao B, Ku-Ding Tsuei B, C, C, D, D, E, F, A NiS 260 K V 2 O 3 MIT [1] MIT MIT NiS MIT NiS Ni 3 S 2 Ni M (emu/g) C 2, 8, 9, 10 C-1 Fe 3 O 4 A, SL B, NSRRC C, D, E, F A, B, B, C, Yen-Fa Liao C, Ku-Ding Tsuei C, D, D, E, F, A Fe 3 O 4 120K MIT V 2 O 3 MIT Cu-doped Fe3O4 NCs MIT [1] Fe 3 O 4 MIT Cu V 2 O 3

More information

研修コーナー

研修コーナー l l l l l l l l l l l α α β l µ l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l l

More information

1) Y. Kobuke, K. Hanji, K. Horiguchi, M. Asada, Y. Nakayama, J. Furukawa, J. Am. Chem. Soc., 98, 7414(1976). 2) S. Yoshida, S. Hayano, J. Memb. Sci.,

1) Y. Kobuke, K. Hanji, K. Horiguchi, M. Asada, Y. Nakayama, J. Furukawa, J. Am. Chem. Soc., 98, 7414(1976). 2) S. Yoshida, S. Hayano, J. Memb. Sci., 1) Y. Kobuke, K. Hanji, K. Horiguchi, M. Asada, Y. Nakayama, J. Furukawa, J. Am. Chem. Soc., 98, 7414(1976). 2) S. Yoshida, S. Hayano, J. Memb. Sci., 11, 157(1982). 3) J. D. Lamb, J. J. Christensen, J.

More information

2 FIG. 1: : n FIG. 2: : n (Ch h ) N T B Ch h n(z) = (sin ϵ cos ω(z), sin ϵ sin ω(z), cos ϵ), (1) 1968 Meyer [5] 50 N T B Ch h [4] N T B 10 nm Ch h 1 µ

2 FIG. 1: : n FIG. 2: : n (Ch h ) N T B Ch h n(z) = (sin ϵ cos ω(z), sin ϵ sin ω(z), cos ϵ), (1) 1968 Meyer [5] 50 N T B Ch h [4] N T B 10 nm Ch h 1 µ : (Dated: February 5, 2016), (Ch), (Oblique Helicoidal) (Ch H ), Twist-bend (N T B ) I. (chiral: ) (achiral) (n) (Ch) (N ) 1996 [1] [2] 2013 (N T B ) [3] 2014 [4] (oblique helicoid) 2016 1 29 Electronic

More information

δδ 1 2 δ δ δ δ μ H 2.1 C 2.5 N 3.0 O 3.5 Cl 3.0 S μ

δδ 1 2 δ δ δ δ μ H 2.1 C 2.5 N 3.0 O 3.5 Cl 3.0 S μ 1961. (Received January 15, 2013) 1) 1. 2. ph 2) 3) 2) 2) 2001 4 6) 7) ph ph ph 1961 1962 1. 2 1 1 δδ 1 2 δ δ δ δ μ 1 1 1 1. H 2.1 C 2.5 N 3.0 O 3.5 Cl 3.0 S 2.5 1 1. μ 1 3. 1 2. 1963 1,4- δ δ 1 3 2 δ

More information

untitled

untitled E-mail: khatano@fms.saitama-u.ac.jp Tel & Fax: 048-858-3535 Toxin Virus Bacterium Glycolipid Glycoprotein Vero toxin (Stx1 and Stx2) Side view Bottom view H H H H N H Grobotriaosyl Ceramide (Gb 3 : Galα1-4Galβ1-4Glcβ-Cer)

More information

1 2 LDA Local Density Approximation 2 LDA 1 LDA LDA N N N H = N [ 2 j + V ion (r j ) ] + 1 e 2 2 r j r k j j k (3) V ion V ion (r) = I Z I e 2 r

1 2 LDA Local Density Approximation 2 LDA 1 LDA LDA N N N H = N [ 2 j + V ion (r j ) ] + 1 e 2 2 r j r k j j k (3) V ion V ion (r) = I Z I e 2 r 11 March 2005 1 [ { } ] 3 1/3 2 + V ion (r) + V H (r) 3α 4π ρ σ(r) ϕ iσ (r) = ε iσ ϕ iσ (r) (1) KS Kohn-Sham [ 2 + V ion (r) + V H (r) + V σ xc(r) ] ϕ iσ (r) = ε iσ ϕ iσ (r) (2) 1 2 1 2 2 1 1 2 LDA Local

More information

Fig. 3. Morse curves for the ground ( a ) and excited state ( b ) of a diatomic molecule2) Fig. 2. The various modes of energy dissipation from electr

Fig. 3. Morse curves for the ground ( a ) and excited state ( b ) of a diatomic molecule2) Fig. 2. The various modes of energy dissipation from electr Color and Constitution of Organic Colorants, and Some Approach to New Chromophore Masaru MATSUOKA Fig. 3. Morse curves for the ground ( a ) and excited state ( b ) of a diatomic molecule2) Fig. 2. The

More information

a L = Ψ éiγ c pa qaa mc ù êë ( - )- úû Ψ 1 Ψ 4 γ a a 0, 1,, 3 {γ a, γ b } η ab æi O ö æo ö β, σ = ço I α = è - ø çèσ O ø γ 0 x iβ γ i x iβα i

a L = Ψ éiγ c pa qaa mc ù êë ( - )- úû Ψ 1 Ψ 4 γ a a 0, 1,, 3 {γ a, γ b } η ab æi O ö æo ö β, σ = ço I α = è - ø çèσ O ø γ 0 x iβ γ i x iβα i 解説 4 matsuo.mamoru jaea.go.jp 4 eizi imr.tohoku.ac.jp 4 maekawa.sadamichi jaea.go.jp i ii iii i Gd Tb Dy g khz Pt ii iii Keywords vierbein 3 dreibein 4 vielbein torsion JST-ERATO 1 017 1. 1..1 a L = Ψ

More information

nsg02-13/ky045059301600033210

nsg02-13/ky045059301600033210 φ φ φ φ κ κ α α μ μ α α μ χ et al Neurosci. Res. Trpv J Physiol μ μ α α α β in vivo β β β β β β β β in vitro β γ μ δ μδ δ δ α θ α θ α In Biomechanics at Micro- and Nanoscale Levels, Volume I W W v W

More information

薄膜結晶成長の基礎4.dvi

薄膜結晶成長の基礎4.dvi 4 464-8602 1 [1] 2 (STM: scanning tunneling microscope) (AFM: atomic force microscope) 1 ( ) 4 LPE(liquid phase epitaxy) 4.1 - - - - (Burton Cabrera Frank) BCF [2] P f = (4.1) 2πmkB T 1 Makio Uwaha. E-mail:uwaha@nagoya-u.jp;

More information

( ) 1 1.1? ( ) ( ) ( ) 1.1(a) T m ( ) 1.1(a) T g ( ) T g T g 500 74% ( ) T K ( 1.1(b) 15 T g T g 10 13 T g T g T g [ ] A ( ) exp (1.1) T T 0 Vogel-Fulcher T 0 T 0 T K T K Ortho-Terphenil (OTP) SiO 2 (1.1)

More information

1) K. J. Laidler, "Reaction Kinetics", Vol. II, Pergamon Press, New York (1963) Chap. 1 ; P. G. Ashmore, "Catalysis and Inhibition of Chemical Reactio

1) K. J. Laidler, Reaction Kinetics, Vol. II, Pergamon Press, New York (1963) Chap. 1 ; P. G. Ashmore, Catalysis and Inhibition of Chemical Reactio 1) K. J. Laidler, "Reaction Kinetics", Vol. II, Pergamon Press, New York (1963) Chap. 1 ; P. G. Ashmore, "Catalysis and Inhibition of Chemical Reactions", Butterworths, London (1963) Chap. 7, p. 185. 2)

More information

I II III IV V

I II III IV V I II III IV V N/m 2 640 980 50 200 290 440 2m 50 4m 100 100 150 200 290 390 590 150 340 4m 6m 8m 100 170 250 µ = E FRVβ β N/mm 2 N/mm 2 1.1 F c t.1 3 1 1.1 1.1 2 2 2 2 F F b F s F c F t F b F s 3 3 3

More information

O x y z O ( O ) O (O ) 3 x y z O O x v t = t = 0 ( 1 ) O t = 0 c t r = ct P (x, y, z) r 2 = x 2 + y 2 + z 2 (t, x, y, z) (ct) 2 x 2 y 2 z 2 = 0

O x y z O ( O ) O (O ) 3 x y z O O x v t = t = 0 ( 1 ) O t = 0 c t r = ct P (x, y, z) r 2 = x 2 + y 2 + z 2 (t, x, y, z) (ct) 2 x 2 y 2 z 2 = 0 9 O y O ( O ) O (O ) 3 y O O v t = t = 0 ( ) O t = 0 t r = t P (, y, ) r = + y + (t,, y, ) (t) y = 0 () ( )O O t (t ) y = 0 () (t) y = (t ) y = 0 (3) O O v O O v O O O y y O O v P(, y,, t) t (, y,, t )

More information

磁気測定によるオーステンパ ダクタイル鋳鉄の残留オーステナイト定量

磁気測定によるオーステンパ ダクタイル鋳鉄の残留オーステナイト定量 33 Non-destructive Measurement of Retained Austenite Content in Austempered Ductile Iron Yoshio Kato, Sen-ichi Yamada, Takayuki Kato, Takeshi Uno Austempered Ductile Iron (ADI) 100kg/mm 2 10 ADI 10 X ADI

More information

9 Nippon Shokuhin Kagaku Kogaku Kaishi Vol. /,, No.0,,/+,/0 (,**/) 251 * * E#ects of Microbial Transglutaminase on Melting Point and Gel property of G

9 Nippon Shokuhin Kagaku Kogaku Kaishi Vol. /,, No.0,,/+,/0 (,**/) 251 * * E#ects of Microbial Transglutaminase on Melting Point and Gel property of G 9 Nippon Shokuhin Kagaku Kogaku Kaishi Vol. /,, No.0,,/+,/0 (,**/) 251 * * E#ects of Microbial Transglutaminase on Melting Point and Gel property of Gelatins Takahiko Soeda, Tomoko Kaneko*, Akiko Hokazono,

More information

untitled

untitled 254nm UV TiO 2 20nm :Sr 5 Ta 4 O 15 3 4 KEY-1 KEY-2 (Ti,Nb,Ta) 5 KEY-1 KEY-2 6 7 NiO/ Sr 2 Ta 2 O 7 mmol h -1 g -1 20 15 10 5 H 2 O 2 H 2 O 2 0 0 2 4 6 8 10 12 NiO/Sr 2 Ta 2 O 7 The synthesis of photocatalysts

More information

d (i) (ii) 1 Georges[2] Maier [3] [1] ω = 0 1

d (i) (ii) 1 Georges[2] Maier [3] [1] ω = 0 1 16 5 19 10 d (i) (ii) 1 Georges[2] Maier [3] 2 10 1 [1] ω = 0 1 [4, 5] Dynamical Mean-Field Theory (DMFT) [2] DMFT I CPA [10] CPA CPA Σ(z) z CPA Σ(z) Σ(z) Σ(z) z - CPA Σ(z) DMFT Σ(z) CPA [6] 3 1960 [7]

More information

Microsoft Excelを用いた分子軌道の描画の実習

Microsoft Excelを用いた分子軌道の描画の実習 J. Comput. Chem. Jpn.,Vol.9, No.4, pp.177 182 (2010) 2010 Society of Computer Chemistry, Japan Microsoft Excel a*, b, c a, 790-8577 2-5 b, 350-0295 1-1 c, 305-8568 1-1-1 *e-mail: nagaoka@ehimegw.dpc.ehime-u.ac.jp

More information

news

news ETL NEWS 1999.9 ETL NEWS 1999.11 Establishment of an Evaluation Technique for Laser Pulse Timing Fluctuations Optoelectronics Division Hidemi Tsuchida e-mail:tsuchida@etl.go.jp A new technique has been

More information

カイラル結晶化ver3pp.dvi

カイラル結晶化ver3pp.dvi 464-8602 (Dated: March 14, 2008) Abstract () PACS numbers: 81.10.-h, 64.60.Qb, 82.20.-w Electronic address: uwaha@nagoya-u.jp 1 I. [1] [2] 20 L [3] D D D BCF Frank [4] D L [5] 2 D L D L [6] D L [7] SiO

More information

Table 1 Type of polymeric coating materials Fig. 2 Results of suppressive effects of polymeric coating materials on the progress of neutralization of concrete. Table 2 Evaluation of the suppressive effects

More information

SAXS Table 1 DSC POM SAXSSAXS PF BL-10C BL-15A Fig. 2 LC12 DSC SAXS 138 C T iso T iso SAXS q=1.4 nm -1 q=(4π/λ)sin(θ/2), λ:, θ: Fig. 3 LC12 T iso Figu

SAXS Table 1 DSC POM SAXSSAXS PF BL-10C BL-15A Fig. 2 LC12 DSC SAXS 138 C T iso T iso SAXS q=1.4 nm -1 q=(4π/λ)sin(θ/2), λ:, θ: Fig. 3 LC12 T iso Figu 1 1 1 1,2 1,2 1 2 Correlation between Microphase Separation and Liquid Crystallization in Structure Formation of Liquid Crystalline Block Copolymers Shin-ichi TANIGUCHI 1, Hiroki TAKESHITA 1, Masamitsu

More information

陽電子科学 第4号 (2015) 3-8

陽電子科学 第4号 (2015) 3-8 4 (2015) 3 8 Japanese Positron Science Society Positron annihilation age momentum correlation (AMOC) measurement Abstract: Positron annihilation Age-MOmentum Correlation (AMOC) measurement is the coincidence

More information

1 M = (M, g) m Riemann N = (N, h) n Riemann M N C f : M N f df : T M T N M T M f N T N M f 1 T N T M f 1 T N C X, Y Γ(T M) M C T M f 1 T N M Levi-Civi

1 M = (M, g) m Riemann N = (N, h) n Riemann M N C f : M N f df : T M T N M T M f N T N M f 1 T N T M f 1 T N C X, Y Γ(T M) M C T M f 1 T N M Levi-Civi 1 Surveys in Geometry 1980 2 6, 7 Harmonic Map Plateau Eells-Sampson [5] Siu [19, 20] Kähler 6 Reports on Global Analysis [15] Sacks- Uhlenbeck [18] Siu-Yau [21] Frankel Siu Yau Frankel [13] 1 Surveys

More information

光学

光学 Control of Refractive Indices of Optical Polymers: Theoretical Prediction and Molecular Design Method Shinji ANDO The fundamental theory and a method to predict the refractive indices and dispersions of

More information

1 9 v.0.1 c (2016/10/07) Minoru Suzuki T µ 1 (7.108) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1)

1 9 v.0.1 c (2016/10/07) Minoru Suzuki T µ 1 (7.108) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1) 1 9 v..1 c (216/1/7) Minoru Suzuki 1 1 9.1 9.1.1 T µ 1 (7.18) f(e ) = 1 e β(e µ) 1 E 1 f(e ) (Bose-Einstein distribution function) *1 (8.1) (9.1) E E µ = E f(e ) E µ (9.1) µ (9.2) µ 1 e β(e µ) 1 f(e )

More information

(Compton Scattering) Beaming 1 exp [i (k x ωt)] k λ k = 2π/λ ω = 2πν k = ω/c k x ωt ( ω ) k α c, k k x ωt η αβ k α x β diag( + ++) x β = (ct, x) O O x

(Compton Scattering) Beaming 1 exp [i (k x ωt)] k λ k = 2π/λ ω = 2πν k = ω/c k x ωt ( ω ) k α c, k k x ωt η αβ k α x β diag( + ++) x β = (ct, x) O O x Compton Scattering Beaming exp [i k x ωt] k λ k π/λ ω πν k ω/c k x ωt ω k α c, k k x ωt η αβ k α x β diag + ++ x β ct, x O O x O O v k α k α β, γ k γ k βk, k γ k + βk k γ k k, k γ k + βk 3 k k 4 k 3 k

More information

Hideki MATSUOKA: An Introduction to Small-angle Scattering Fundamental aspects of small-angle scattering technique are duly explained from the very ba

Hideki MATSUOKA: An Introduction to Small-angle Scattering Fundamental aspects of small-angle scattering technique are duly explained from the very ba Hideki MATSUOKA: An Introduction to Small-angle Scattering Fundamental aspects of small-angle scattering technique are duly explained from the very basic points for the beginners and newcommers of this

More information

放射線化学, 92, 39 (2011)

放射線化学, 92, 39 (2011) V. M. S. V. 1 Contents of the lecture note by Prof. V. M. Byakov and Dr. S. V. Stepanov (Institute of Theoretical and Experimental Physics, Russia) are described in a series of articles. The first article

More information

Movement of Population and Structure of 'Buraku' in the Edo Period Akira FUKUYAMA Section of Economics, Osaka Kyoiku University, Kashiwara, Osaka 582, Japan That goes without saying now, historical study

More information

Surface Morphology for Poly-L-lactide Fibers Subjected to Hydrolysis Suong-Hyu Hyon Institute for Frontier Medical Sciences, Kyoto University 53, Shog

Surface Morphology for Poly-L-lactide Fibers Subjected to Hydrolysis Suong-Hyu Hyon Institute for Frontier Medical Sciences, Kyoto University 53, Shog Surface Morphology for Poly-L-lactide Fibers Subjected to Hydrolysis Suong-Hyu Hyon Institute for Frontier Medical Sciences, Kyoto University 53, Shogoin Kawaharacho, Sakyo-ku, Kyoto, 606-8507 Japan Abstract:

More information

(1) 1.1

(1) 1.1 1 1 1.1 1.1.1 1.1 ( ) ( ) ( ) { ( ) ( ) { ( ) ( ) { ( ) ( ) { ( ) ( ) { ( ) ( ) ( ) ( ) ( ) 2 1 1.1.2 (1) 1.1 1.1 3 (2) 1.2 4 1 (3) 1.3 ( ) ( ) (4) 1.1 5 (5) ( ) 1.4 6 1 (6) 1.5 (7) ( ) (8) 1.1 7 1.1.3

More information

Journal of the Combustion Society of Japan Vol.58 No.185 (2016) ORIGINAL PAPER 火災旋風近傍の流れに関する研究 Flow Around a Fire Whirl *

Journal of the Combustion Society of Japan Vol.58 No.185 (2016) ORIGINAL PAPER 火災旋風近傍の流れに関する研究 Flow Around a Fire Whirl * 58 185 2016 167-171 Journal of the Combustion Society of Japan Vol.58 No.185 (2016) 167-171 ORIGINAL PAPER 火災旋風近傍の流れに関する研究 Flow Around a Fire Whirl * ONISHI, Hiroyuki and KUWANA, Kazunori 992-8510 4-3-16

More information

(a) (b) (c) (d) 1: (a) (b) (c) (d) (a) (b) (c) 2: (a) (b) (c) 1(b) [1 10] 1 degree k n(k) walk path 4

(a) (b) (c) (d) 1: (a) (b) (c) (d) (a) (b) (c) 2: (a) (b) (c) 1(b) [1 10] 1 degree k n(k) walk path 4 1 vertex edge 1(a) 1(b) 1(c) 1(d) 2 (a) (b) (c) (d) 1: (a) (b) (c) (d) 1 2 6 1 2 6 1 2 6 3 5 3 5 3 5 4 4 (a) (b) (c) 2: (a) (b) (c) 1(b) [1 10] 1 degree k n(k) walk path 4 1: Zachary [11] [12] [13] World-Wide

More information

無電解めっきとレーザー照射による有機樹脂板上へのCuマイクロパターン形成

無電解めっきとレーザー照射による有機樹脂板上へのCuマイクロパターン形成 Title 無電解めっきとレーザー照射による有機樹脂板上への Cu マイクロパターン形成 Author(s) 菊地, 竜也 ; 和智, 悠太 ; 坂入, 正敏 ; 高橋, 英明 ; 飯野, 潔 ; 片山, 直樹 Citation 表面技術, 59(8): 555-561 Issue Date 2008-08 Doc URL http://hdl.handle.net/2115/36647 Type

More information

明治期の新聞における「鶏姦」報道の特徴 : 『読売新聞』と『朝日新聞』の分析から

明治期の新聞における「鶏姦」報道の特徴 : 『読売新聞』と『朝日新聞』の分析から Title 明治期の新聞における 鶏姦 報道の特徴 : 読売新聞 と 朝日新聞 の分析から Author(s) 斉藤, 巧弥 国際広報メディア 観光学ジャーナル = The Journal of International Med Citation24: 21-38 Issue Date 2017-03-24 Doc URL http://hdl.handle.net/2115/64760 Type

More information

20 4 20 i 1 1 1.1............................ 1 1.2............................ 4 2 11 2.1................... 11 2.2......................... 11 2.3....................... 19 3 25 3.1.............................

More information

,, Andrej Gendiar (Density Matrix Renormalization Group, DMRG) 1 10 S.R. White [1, 2] 2 DMRG ( ) [3, 2] DMRG Baxter [4, 5] 2 Ising 2 1 Ising 1 1 Ising

,, Andrej Gendiar (Density Matrix Renormalization Group, DMRG) 1 10 S.R. White [1, 2] 2 DMRG ( ) [3, 2] DMRG Baxter [4, 5] 2 Ising 2 1 Ising 1 1 Ising ,, Andrej Gendiar (Density Matrix Renormalization Group, DMRG) 1 10 S.R. White [1, 2] 2 DMRG ( ) [3, 2] DMRG Baxter [4, 5] 2 Ising 2 1 Ising 1 1 Ising Model 1 Ising 1 Ising Model N Ising (σ i = ±1) (Free

More information

4/15 No.

4/15 No. 4/15 No. 1 4/15 No. 4/15 No. 3 Particle of mass m moving in a potential V(r) V(r) m i ψ t = m ψ(r,t)+v(r)ψ(r,t) ψ(r,t) = ϕ(r)e iωt ψ(r,t) Wave function steady state m ϕ(r)+v(r)ϕ(r) = εϕ(r) Eigenvalue problem

More information

2014Vol.63No.4p.383393 Thermal environment for health and safety Hirohumi HAYAMA Masaya SAITO Haruka MIKAMI Faculty of Engineering, Hokkaido University School of Design, Sapporo City University Graduate

More information

Activation and Control of Electron-Transfer Reactions by Noncovalent Bond

Activation and Control of Electron-Transfer Reactions by Noncovalent Bond 2 + 4e- + 4 + hν 2 2 1 2 20 J. Am. Chem. oc. Angew. Chem. Int. Ed. umber of Papers 15 10 5 0 1998 1999 2000 2001 2002 2003 Year : J. Am. Chem. oc. (Trost, B. M.; tanford University, UA) 3 π 1/2 k ET =

More information

Fig. ph Si-O-Na H O Si- Na OH Si-O-Si OH Si-O Si-OH Si-O-Si Si-O Si-O Si-OH Si-OH Si-O-Si H O 6

Fig. ph Si-O-Na H O Si- Na OH Si-O-Si OH Si-O Si-OH Si-O-Si Si-O Si-O Si-OH Si-OH Si-O-Si H O 6 NMR ESR NMR 5 Fig. ph Si-O-Na H O Si- Na OH Si-O-Si OH Si-O Si-OH Si-O-Si Si-O Si-O Si-OH Si-OH Si-O-Si H O 6 Fig. (a) Na O-B -Si Na O-B Si Fig. (b) Na O-CaO-SiO Na O-CaO-B -Si. Na O-. CaO-. Si -. Al O

More information

液晶の物理1:連続体理論(弾性,粘性)

液晶の物理1:連続体理論(弾性,粘性) The Physics of Liquid Crystals P. G. de Gennes and J. Prost (Oxford University Press, 1993) Liquid crystals are beautiful and mysterious; I am fond of them for both reasons. My hope is that some readers

More information

XFEL/SPring-8

XFEL/SPring-8 DEVELOPMENT STATUS OF RF SYSTEM OF INJECTOR SECTION FOR XFEL/SPRING-8 Takao Asaka 1,A), Takahiro Inagaki B), Hiroyasu Ego A), Toshiaki Kobayashi A), Kazuaki Togawa B), Shinsuke Suzuki A), Yuji Otake B),

More information

研究室ガイダンス(H28)福山研.pdf

研究室ガイダンス(H28)福山研.pdf 1 2 3 4 5 4 He M. Roger et al., JLTP 112, 45 (1998) A.F. Andreev and I.M. Lifshitz, Sov. Phys. JETP 29, 1107 (1969) Born in 2004 (hcp 4 He) E. Kim and M.H.W. Chan, Nature 427, 225 (2004); Science 305,

More information

研究室ガイダンス(H29)福山研v2.pdf

研究室ガイダンス(H29)福山研v2.pdf J.M. Kosterlitz and D.J. Thouless, Phys. 5, L124 (1972); ibid. 6, 1181 (1973) David J. Thouless J. Michael Kosterlitz + ρ T s KT D.J. Bishop and J.D. Reppy, PRL 40, 1727 (1978) ( ) = 2k B m2 T KT π 2 T

More information

‚åŁÎ“·„´Šš‡ðŠp‡¢‡½‹âfi`fiI…A…‰…S…−…Y…•‡ÌMarkovŸA“½fiI›ð’Í

‚åŁÎ“·„´Šš‡ðŠp‡¢‡½‹âfi`fiI…A…‰…S…−…Y…•‡ÌMarkovŸA“½fiI›ð’Í Markov 2009 10 2 Markov 2009 10 2 1 / 25 1 (GA) 2 GA 3 4 Markov 2009 10 2 2 / 25 (GA) (GA) L ( 1) I := {0, 1} L f : I (0, ) M( 2) S := I M GA (GA) f (i) i I Markov 2009 10 2 3 / 25 (GA) ρ(i, j), i, j I

More information

E 1/2 3/ () +3/2 +3/ () +1/2 +1/ / E [1] B (3.2) F E 4.1 y x E = (E x,, ) j y 4.1 E int = (, E y, ) j y = (Hall ef

E 1/2 3/ () +3/2 +3/ () +1/2 +1/ / E [1] B (3.2) F E 4.1 y x E = (E x,, ) j y 4.1 E int = (, E y, ) j y = (Hall ef 4 213 5 8 4.1.1 () f A exp( E/k B ) f E = A [ k B exp E ] = f k B k B = f (2 E /3n). 1 k B /2 σ = e 2 τ(e)d(e) 2E 3nf 3m 2 E de = ne2 τ E m (4.1) E E τ E = τe E = / τ(e)e 3/2 f de E 3/2 f de (4.2) f (3.2)

More information

O1-1 O1-2 O1-3 O1-4 O1-5 O1-6

O1-1 O1-2 O1-3 O1-4 O1-5 O1-6 O1-1 O1-2 O1-3 O1-4 O1-5 O1-6 O1-7 O1-8 O1-9 O1-10 O1-11 O1-12 O1-13 O1-14 O1-15 O1-16 O1-17 O1-18 O1-19 O1-20 O1-21 O1-22 O1-23 O1-24 O1-25 O1-26 O1-27 O1-28 O1-29 O1-30 O1-31 O1-32 O1-33 O1-34 O1-35

More information

(2) N elec = D p,q p,q χ q χ p dr = p,q D p,q S q,p Mulliken PA D Mull p = p = group A D p,p 1 + D p,q S q,p p q p [ r A D Mull p ] group χ p G Mull A

(2) N elec = D p,q p,q χ q χ p dr = p,q D p,q S q,p Mulliken PA D Mull p = p = group A D p,p 1 + D p,q S q,p p q p [ r A D Mull p ] group χ p G Mull A 7 - (Electron-Donor Acceptor) : Charge-Transfer ( CT) ( (Charge-Transfer) - (electron donor-electron acceptor) [1][2][3][4] Van der Waals CT [5] Population Analysis population analysis ( ), observable

More information

第86回日本感染症学会総会学術集会後抄録(I)

第86回日本感染症学会総会学術集会後抄録(I) κ κ κ κ κ κ μ μ β β β γ α α β β γ α β α α α γ α β β γ μ β β μ μ α ββ β β β β β β β β β β β β β β β β β β γ β μ μ μ μμ μ μ μ μ β β μ μ μ μ μ μ μ μ μ μ μ μ μ μ β

More information

596 Dementia Japan 29 : , 2015 原著 1,2 1,2 1,3 1,4 1,4 1,5 1,5 1,6 1,7 1,8 要 旨 Activity of Initial - phase Intensive Support Team for Dementia o

596 Dementia Japan 29 : , 2015 原著 1,2 1,2 1,3 1,4 1,4 1,5 1,5 1,6 1,7 1,8 要 旨 Activity of Initial - phase Intensive Support Team for Dementia o 596 Dementia Japan 29 : 596-604, 2015 原著 1,2 1,2 1,3 1,4 1,4 1,5 1,5 1,6 1,7 1,8 要 旨 Activity of Initial - phase Intensive Support Team for Dementia of Kobe City Hiroyuki Kajita 1,2, Kiyoshi Maeda 1,2,

More information

1. Precise Determination of BaAl2O4 Cell and Certification of the Formation of Iron Bearing Solid Solution. By Hiroshi UCHIKAWA and Koichi TSUKIYAMA (

1. Precise Determination of BaAl2O4 Cell and Certification of the Formation of Iron Bearing Solid Solution. By Hiroshi UCHIKAWA and Koichi TSUKIYAMA ( 1. Precise Determination of BaAl2O4 Cell and Certification of the Formation of Iron Bearing Solid Solution. By Hiroshi UCHIKAWA and Koichi TSUKIYAMA (Central Research Laboratory, Onoda Cement Co., Ltd.,

More information

newmain.dvi

newmain.dvi 数論 サンプルページ この本の定価 判型などは, 以下の URL からご覧いただけます. http://www.morikita.co.jp/books/mid/008142 このサンプルページの内容は, 第 2 版 1 刷発行当時のものです. Daniel DUVERNEY: THÉORIE DES NOMBRES c Dunod, Paris, 1998, This book is published

More information

42 1 Fig. 2. Li 2 B 4 O 7 crystals with 3inches and 4inches in diameter. Fig. 4. Transmission curve of Li 2 B 4 O 7 crystal. Fig. 5. Refractive index

42 1 Fig. 2. Li 2 B 4 O 7 crystals with 3inches and 4inches in diameter. Fig. 4. Transmission curve of Li 2 B 4 O 7 crystal. Fig. 5. Refractive index MEMOIRS OF SHONAN INSTITUTE OF TECHNOLOGY Vol. 42, No. 1, 2008 Li 2 B 4 O 7 (LBO) *, ** * ** ** Optical Scatterer and Crystal Growth Technology of LBO Single Crystal For Development with Optical Application

More information

T g T 0 T 0 fragile * ) 1 9) η T g T g /T *1. τ τ η = Gτ. G τ

T g T 0 T 0 fragile * ) 1 9) η T g T g /T *1. τ τ η = Gτ. G τ 615-851 ryoichi@chemekyoto-uacjp 66-852 onuki@scphyskyoto-uacjp 1 T g T T fragile *2 1 11) 1 9) η T g T g /T *1 τ 198 τ η = Gτ G τ T c η τ 12) strong fragile T c strong η η exp(e/k B T ) 1 2/3 E SiO 2

More information

Black-Scholes [1] Nelson [2] Schrödinger 1 Black Scholes [1] Black-Scholes Nelson [2][3][4] Schrödinger Nelson Parisi Wu [5] Nelson Parisi-W

Black-Scholes [1] Nelson [2] Schrödinger 1 Black Scholes [1] Black-Scholes Nelson [2][3][4] Schrödinger Nelson Parisi Wu [5] Nelson Parisi-W 003 7 14 Black-Scholes [1] Nelson [] Schrödinger 1 Black Scholes [1] Black-Scholes Nelson [][3][4] Schrödinger Nelson Parisi Wu [5] Nelson Parisi-Wu Nelson e-mail: takatoshi-tasaki@nifty.com kabutaro@mocha.freemail.ne.jp

More information

06’ÓŠ¹/ŒØŒì

06’ÓŠ¹/ŒØŒì FD. FD FD FD FD FD FD / Plan-Do-See FD FD FD FD FD FD FD FD FD FD FD FD FD FD JABEE FD A. C. A B .. AV .. B Communication Space A FD FD ES FD FD The approach of the lesson improvement in Osaka City University

More information

微粒子合成化学・講義

微粒子合成化学・講義 http://www.tagen.tohoku.ac.jp/labo/muramatsu/mura/main.html E-mail: mura@tagen.tohoku.ac.jp 1 2 3 1m 10cm 1cm 1mm 100 m 10 m 1 m 100nm 10nm 1nm 1 100 m 10 m 1 m 1nm 100nm 10nm 4 5 6 7 1m 10cm 1cm 1mm 100

More information

Fig. la PL spectra of PSL prepared on Si specimen (p = 1 k Q m) with electrochemical etching in HF solution (26wt %) under galvanostatic conditions of

Fig. la PL spectra of PSL prepared on Si specimen (p = 1 k Q m) with electrochemical etching in HF solution (26wt %) under galvanostatic conditions of Vol.47,No.11,1996 Influence of Electrochemical Etching Current Density on Porous Si Luminescence Properties and Microstructure Kazuhiro SHIGYO *, Masahiro SEO *, Kazuhlsa AZUMI * and Hideaki TAKAHASHI

More information