イオン性高分子ポルフィリン金属錯体およびポリビピリジン
|
|
- きゅういち そめや
- 5 years ago
- Views:
Transcription
1 2007 Excited State Properties of A Pyrene Derivative Containing Donor- and Acceptor- Functional Groups and Its Application as Photosensitizer
2 2
3 CH 3 N CH 3 H C C C 2 H 5 OOC COOC 2 H 5 3
4 Scheme 1 CH 3 N CH 3 Reaction Temp : Benzene reflux CH 3 N CH 3 + CH 2 (COOC 2 H 5 ) 2 NH piperidine : 4 drops AcOH : 2 drops : 30 ml HC O 460 mg (1.68 mmol) 222 mg (1.68 mmol) molecular sieve : 5g HC C C 2 H 5 OOC COOC 2 H 5 Yield ca 80% by NMR 4
5 Fig.1 5
6 CH 3 N c CH 3 a b H H 3 CH 2 COOC H 3 CH 2 COOC C C c CD 3 CN H 2 O b a 6
7 CH 3 N CH 3 H C C C 2 H 5 OOC COOC 2 H 5 7
8 2 17 CH 3 1 N 1 18 CH H 14 C19 15 C 20 C 2 H 5 OOC COOC 2 H 5 Fig.4 8
9 Solvent Heptane 1,4-Dioxane Toluene Diethyl Ether THF Dichloromethane Methanol Acetonitrile DMF N-Methyl formamide max 401nm 409nm 411nm 408nm 411nm 410nm 411nm 412nm 418nm 418nm Table.1 10 Max Absorbance Wavelength(nm) Fig.5 9
10 Solvent Heptane 1,4-Dioxane Toluene Diethyl Ether THF Dichloromethane Methanol Acetonitrile DMF N-Methyl formamide max 511nm 577nm 558nm 564nm 595nm 616nm 678nm 657nm 655nm 669nm Table.2 10 Max 10
11 Fluorescence Intensity Wavelength(nm) Fig
12 B3LYP/6-31+G(d) X f 2 = ( ε 1) /(2ε) ( n 1) / 2(2n 1) 2 f 12
13 1/cm Solvatochromic shift on the emission maxima Heptane 1,4-Dioxane Toluene Diethyl Ether THF Dichloromethane Methanol Acetonitrile DMF N-Methyl formamide f Fig ν max 3 = 1.2 / hcρ µ ( µ µ ) fconst 2 e e g 13
14 (Fig8)(Fig9) Absorbance 3 3 PMMA 2.5 AbsorptionSpectra in Polymer Films PMMA PS PSPE 2 PEPVA 1.5 PVA PA PAPVP PVP PEG PEG Absorbance Fluorescence Intensity Emission Spectra in Polymer Films PMMA PST PE PVA PA PVP PEG Wavelength(nm) 14
15 TRITONNX-100SDSCTAB) Absorbance Absorption Spectra in Micellar Solutions TRITONX-100 SDS CTAB Fig,9 sion Intensity EmissionSpectrain Micellar Solutions 15
16 Fig.10 Fig.11 AMP-CHO 16
17 ( I ph / e) IPCE( ) = 100 W /( hc / ) ph 17
18 Tris(2,2 -bipyridine)ru() AMP N3dye IPCE/% Wavelength/nm Fig.12 IPCE 5 AMP-Ester AMP-Ester IPCE 18
19 AMP-Ester X Table3,4 (Table5) (Table6)(Table6)AMP-Ester ORTEP Fig.13 Data Collection A reddish_yellow rod crystal of H 25 NO 4 C 26 having approximate dimensions of 0.25 x 0.25 x 0.25 mm was mounted on a glass fiber. All measurements were made on a Rigaku AFC7R diffractometer with graphite monochromated Mo-Kα radiation and a rotating anode generator. Cell constants and an orientation matrix for data collection, obtained from a least-squares refinement using the setting angles of 25 carefully centered reflections in the range < 2θ < o corresponded to a primitive monoclinic cell with dimensions: a = 9.148(4) Å b = 7.199(2) Å β = 96.63(2) o c = (4) Å V = (12) Å 3 For Z = 4 and F.W. = , the calculated density is g/cm 3. The systematic absences of: h0l: l ± 2n 0k0: k ± 2n uniquely determine the space group to be: P2 1 /c (#14) 19
20 The data were collected at a temperature of o C using the ω scan technique to a maximum 2θ value of 55.0 o. Omega scans of several intense reflections, made prior to data collection, had an average width at half-height of 0.28 o with a take-off angle of 6.0 o. Scans of ( tan θ) o were made at a speed of 8.0 o /min (in ω). The weak reflections (I < 10.0σ(I)) were rescanned (maximum of 5 scans) and the counts were accumulated to ensure good counting statistics. Stationary background counts were recorded on each side of the reflection. The ratio of peak counting time to background counting time was 2:1. The diameter of the incident beam collimator was 0.5 mm and the crystal to detector distance was 235 mm. The computer-controlled slits were set to 3.0 mm (horizontal) and 3.0 mm (vertical). Data Reduction Of the 5341 reflections that were collected, 5029 were unique (R int = 0.120). The intensities of three representative reflections were measured after every 0 reflections. No decay correction was applied. The linear absorption coefficient, µ, for Mo-Kα radiation is cm -1. The data were corrected for Lorentz and polarization effects. Structure Solution and Refinement The structure was solved by direct methods 1 and expanded using Fourier techniques 2. The non-hydrogen atoms were refined anisotropically. Hydrogen atoms were refined using the riding model. The final cycle of full-matrix least-squares refinement 3 on F 2 was based on 2044 observed reflections and 305 variable parameters and converged (largest parameter shift was 0.00 times its esd) with unweighted and weighted agreement factors of: R1 = Σ Fo - Fc / Σ Fo =
21 wr2 = [ Σ ( w (Fo 2 - Fc 2 ) 2 )/ Σ w(fo 2 ) 2 ] 1/2 = The standard deviation of an observation of unit weight 4 was A Sheldrick weighting scheme was used. Plots of Σ w ( Fo - Fc ) 2 versus Fo, reflection order in data collection, sin θ/λ and various classes of indices showed no unusual trends. The maximum and minimum peaks on the final difference Fourier map corresponded to 0.23 and e - /Å 3, respectively. Neutral atom scattering factors were taken from Cromer and Waber 5. Anomalous dispersion effects were included in Fcalc 6 ; the values for f' and f" were those of Creagh and McAuley7. The values for the mass attenuation coefficients are those of Creagh and Hubbell 8. All calculations were performed using the CrystalStructure 9,10 crystallographic software package. Table 3. Atomic coordinates and B iso /B eq atom x y z B eq O(1) (3) (5) (9) 6.87(8) O(2) (3) (6) (8) 7.50(9) O(3) (3) (5) (8) 6.82(8) O(4) (3) (4) (7) 5.11(6) N(1) (4) (5) (10) 5.42(8) C(1) (4) (5) (11) 4.42(8) C(2) (4) (5) (11) 4.64(9) C(3) (4) (5) (10) 4.58(9) C(4) (4) (5) (10) 3.91(7) C(5) (4) (4) (10) 3.52(7) C(6) (4) (4) (10) 3.83(7) C(7) (4) (5) (11) 4.28(8) C(8) (4) (5) (11) 4.11(8) C(9) (3) (5) (10) 3.65(7) 21
22 C(10) (3) (4) (10) 3.45(7) C(11) (4) (5) (10) 3.86(8) C(12) (4) (5) (11) 4.51(9) C(13) (4) (5) (11) 4.47(9) C(14) (3) (4) (10) 3.74(7) C(15) (4) (5) (11) 4.41(9) C(16) (4) (5) (11) 4.51(9) C(17) (6) (7) (13) 6.86(12) C(18) (4) (7) (13) 5.92(11) C(19) (4) (5) (10) 4.02(7) C(20) (4) (5) (11) 4.31(8) C(21) (4) (6) (11) 4.90(9) C(22) (4) (6) (11) 4.44(8) C(23) (6) (15) (17) 12.7(2) C(24) (9) (11) (2) 12.9(2) C(25) (5) (8) (14) 7.21(14) C(26) (7) (10) (18) 11.2(2) Beq = 8/3 π 2 (U11(aa*) 2 + U22(bb*) 2 + U33(cc*) 2 + 2U12(aa*bb*)cos γ + 2U13(aa*cc*)cos β + 2U23(bb*cc*)cos α) 22
23 Table 4. Atomic coordinates and B iso involving hydrogens/b eq atom x y z B eq H(1) H(2) H(3) H(4) H(5) H(6) H(7) H(8) H(9) H(10) H(11) H(12) H(13) H(14) H(15) H(16) H(17) H(18) H(19) H(20) H(21) H(22) H(23) H(24) H(25) Beq = 8/3 π 2 (U11(aa*) 2 + U22(bb*) 2 + U33(cc*) 2 + 2U12(aa*bb*)cos γ + 2U13(aa*cc*)cos β + 2U23(bb*cc*)cos α) 23
24 Table 5. Bond lengths (Å) atom atom distance atom atom distance O(1) C(21) 1.187(5) O(2) C(21) 1.334(4) O(2) C(23) 1.445(6) O(3) C(22) 1.201(5) O(4) C(22) 1.321(5) O(4) C(25) 1.456(6) N(1) C(1) 1.422(5) N(1) C(17) 1.479(5) N(1) C(18) 1.462(6) C(1) C(2) 1.392(6) C(1) C(6) 1.420(4) C(2) C(3) 1.377(5) C(3) C(4) 1.399(4) C(4) C(5) 1.421(5) C(4) C(7) 1.414(5) C(5) C(6) 1.416(4) C(5) C(10) 1.438(4) C(6) C(13) 1.431(5) C(7) C(8) 1.352(5) C(8) C(9) 1.425(5) C(9) C(10) 1.421(4) C(9) C(14) 1.423(4) C(10) C(11) 1.422(5) C(11) C(12) 1.424(5) C(11) C(16) 1.396(4) C(12) C(13) 1.357(5) C(14) C(15) 1.394(5) C(14) C(19) 1.450(4) C(15) C(16) 1.367(5) C(19) C(20) 1.350(4) C(20) C(21) 1.497(5) C(20) C(22) 1.493(5) 24
25 C(23) C(24) 1.351(9) C(25) C(26) 1.433(9) Table 6. Bond angles ( o ) atom atom atom angle atom atom atom angle C(21) O(2) C(23) 116.5(4) C(22) O(4) C(25) 116.9(3) C(1) N(1) C(17) 115.3(3) C(1) N(1) C(18) 115.5(3) C(17) N(1) C(18) 111.5(3) N(1) C(1) C(2) 122.6(3) N(1) C(1) C(6) 118.3(3) C(2) C(1) C(6) 119.1(3) C(1) C(2) C(3) 121.6(3) C(2) C(3) C(4) 121.3(3) C(3) C(4) C(5) 118.0(3) C(3) C(4) C(7) 122.8(3) C(5) C(4) C(7) 119.2(3) C(4) C(5) C(6) 120.9(3) C(4) C(5) C(10) 118.7(3) C(6) C(5) C(10) 120.5(3) C(1) C(6) C(5) 119.0(3) C(1) C(6) C(13) 122.7(3) C(5) C(6) C(13) 118.3(3) C(4) C(7) C(8) 122.0(3) C(7) C(8) C(9) 121.5(3) C(8) C(9) C(10) 118.0(3) C(8) C(9) C(14) 123.1(3) C(10) C(9) C(14) 118.9(3) C(5) C(10) C(9) 120.7(3) C(5) C(10) C(11) 119.0(2) C(9) C(10) C(11) 120.3(3) C(10) C(11) C(12) 119.3(3) C(10) C(11) C(16) 118.9(3) C(12) C(11) C(16) 25
26 121.8(3) C(11) C(12) C(13) 121.2(3) C(6) C(13) C(12) 121.6(3) C(9) C(14) C(15) 118.8(3) C(9) C(14) C(19) 119.4(3) C(15) C(14) C(19) 121.8(3) C(14) C(15) C(16) 122.4(3) C(11) C(16) C(15) 120.6(3) C(14) C(19) C(20) 128.4(3) C(19) C(20) C(21) 117.8(3) C(19) C(20) C(22) 125.3(3) C(21) C(20) C(22) 116.9(3) O(1) C(21) O(2) 124.2(3) O(1) C(21) C(20) 124.8(3) O(2) C(21) C(20) 110.9(3) O(3) C(22) O(4) 124.6(3) O(3) C(22) C(20) 123.9(4) O(4) C(22) C(20) 111.5(3) O(2) C(23) C(24) 112.4(5) O(4) C(25) C(26) 108.9(4) Table 7. Torsion Angles( o ) atom1 atom2 atom3 atom4 angle atom1 atom2 atom3 atom4 angle C(21) O(2) C(23) C(24) (6) C(23) O(2) C(21) O(1) -0.4(7) C(23) O(2) C(21) C(20) (5) C(22) O(4) C(25) C(26) (4) C(25) O(4) C(22) O(3) -3.6(5) C(25) O(4) C(22) C(20) 174.5(3) C(17) N(1) C(1) C(2) 21.1(5) C(17) N(1) C(1) C(6) (3) C(18) N(1) C(1) C(2) (4) C(18) N(1) C(1) C(6) 68.7(4) 26
27 N(1) C(1) C(2) C(3) 177.9(3) N(1) C(1) C(6) C(5) (3) N(1) C(1) C(6) C(13) 5.6(5) C(2) C(1) C(6) C(5) 3.5(5) C(2) C(1) C(6) C(13) (3) C(6) C(1) C(2) C(3) -2.0(5) C(1) C(2) C(3) C(4) -0.6(6) C(2) C(3) C(4) C(5) 1.5(5) C(2) C(3) C(4) C(7) (3) C(3) C(4) C(5) C(6) 0.1(3) C(3) C(4) C(5) C(10) 179.5(3) C(3) C(4) C(7) C(8) 178.5(3) C(5) C(4) C(7) C(8) -1.0(5) C(7) C(4) C(5) C(6) 179.6(3) C(7) C(4) C(5) C(10) -1.0(5) C(4) C(5) C(6) C(1) -2.6(5) C(4) C(5) C(6) C(13) 175.5(3) C(4) C(5) C(10) C(9) 1.9(4) C(4) C(5) C(10) C(11) (3) C(6) C(5) C(10) C(9) (3) C(6) C(5) C(10) C(11) 1.2(4) C(10) C(5) C(6) C(1) 178.0(3) C(10) C(5) C(6) C(13) -3.9(5) C(1) C(6) C(13) C(12) (3) C(5) C(6) C(13) C(12) 2.9(5) C(4) C(7) C(8) C(9) 2.0(6) C(7) C(8) C(9) C(10) -1.1(5) C(7) C(8) C(9) C(14) (3) C(8) C(9) C(10) C(5) -0.9(5) C(8) C(9) C(10) C(11) 179.2(3) C(8) C(9) C(14) C(15) (3) C(8) C(9) C(14) C(19) -0.8(5) C(10) C(9) C(14) C(15) 2.0(5) C(10) C(9) C(14) C(19) (3) C(14) C(9) C(10) C(5) 177.2(3) C(14) C(9) C(10) C(11) -2.7(5) 27
28 C(5) C(10) C(11) C(12) 2.5(5) C(5) C(10) C(11) C(16) (3) C(9) C(10) C(11) C(12) (3) C(9) C(10) C(11) C(16) 0.5(5) C(10) C(11) C(12) C(13) -3.5(5) C(10) C(11) C(16) C(15) 2.5(5) C(12) C(11) C(16) C(15) (3) C(16) C(11) C(12) C(13) 178.5(3) C(11) C(12) C(13) C(6) 0.8(6) C(9) C(14) C(15) C(16) 1.0(5) C(9) C(14) C(19) C(20) 153.3(4) C(15) C(14) C(19) C(20) -27.5(6) C(19) C(14) C(15) C(16) (3) C(14) C(15) C(16) C(11) -3.3(6) C(14) C(19) C(20) C(21) 179.2(3) C(14) C(19) C(20) C(22) -2.0(6) C(19) C(20) C(21) O(1) -5.5(6) C(19) C(20) C(21) O(2) 172.2(3) C(19) C(20) C(22) O(3) 109.9(4) C(19) C(20) C(22) O(4) -68.2(5) C(21) C(20) C(22) O(3) -71.3(5) C(21) C(20) C(22) O(4) 110.6(3) C(22) C(20) C(21) O(1) 175.6(4) C(22) C(20) C(21) O(2) -6.7(5) The sign is positive if when looking from atom 2 to atom 3 a clock-wise motion of atom 1 would superimpose it on atom 4. 28
29 Fig.13 ORTEP 29
30 1. Alan R Katritzky, Dong-Wei Zhu, and Kirk S. Schanze:Intramolecular Charge Transfer Properties of Dicyanovinyl-Substltuted Aromatics,J.Phys.Chem. 1991, 95, Paul Liska, Nick Vlachopoulos, Mohammad K. Nazeeruddin, Pascal Comte, and Michael Gratzel : cis-diaquabis(2,2 -bpyridyl-4,4 -dicarboxylate)-ruthenium( ) Sensitizes Wide band Gap Oxide Semiconductors Very Efficiently over a Broad Spectral Range in the Visible, J. Am. Chem. Soc. 1988, 110, M. K. Nazeeruddin, A. Kay, I.Rodicio, R. Humphry-Baker, E. Muller, P. Liska, N. Vlachopoulos, and M. Gratzel : Conversion of Light to Electricity by cis-x2bis(2,2 -bipyridyl-4,4 -dicarboxylate)ruthenium( ) Charge-Transfer Sensitizers (X=Cl -, Br -, I -, CN -, and SCN - ) on Nanocrystalline TiO2 Electrodes, J. Am. Chem. Soc. 1993, 115, Yuji Kawanishi, Noboru Kitamura, and Shingo Tazuke : Dependence of Spectroscopic, Electrochemical, and Excitd-State Properties of Tris Chelate Ruthenium() Complexes on Ligand Structure, Inorg. Chem. 1989, 28,
31
Isogai, T., Building a dynamic correlation network for fat-tailed financial asset returns, Applied Network Science (7):-24, 206,
H28. (TMU) 206 8 29 / 34 2 3 4 5 6 Isogai, T., Building a dynamic correlation network for fat-tailed financial asset returns, Applied Network Science (7):-24, 206, http://link.springer.com/article/0.007/s409-06-0008-x
More informationMikio Yamamoto: Dynamical Measurement of the E-effect in Iron-Cobalt Alloys. The AE-effect (change in Young's modulus of elasticity with magnetization
Mikio Yamamoto: Dynamical Measurement of the E-effect in Iron-Cobalt Alloys. The AE-effect (change in Young's modulus of elasticity with magnetization) in the annealed state of iron-cobalt alloys has been
More informationX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 informationStudy on Application of the cos a Method to Neutron Stress Measurement Toshihiko SASAKI*3 and Yukio HIROSE Department of Materials Science and Enginee
Study on Application of the cos a Method to Neutron Stress Measurement Toshihiko SASAKI*3 and Yukio HIROSE Department of Materials Science and Engineering, Kanazawa University, Kakuma-machi, Kanazawa-shi,
More information1. 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 informationLAGUNA LAGUNA 10 p Water quality of Lake Kamo, Sado Island, northeast Japan, Katsuaki Kanzo 1, Ni
LAGUNA10 47 56 2003 3 LAGUNA 10 p.47 56 2003 1997 2001 1 2 2 Water quality of Lake Kamo, Sado Island, northeast Japan, 1997 2001 Katsuaki Kanzo 1, Niigata Prefectural Ryotsu High School Science Club, Iwao
More informationStudies of Foot Form for Footwear Design (Part 9) : Characteristics of the Foot Form of Young and Elder Women Based on their Sizes of Ball Joint Girth
Studies of Foot Form for Footwear Design (Part 9) : Characteristics of the Foot Form of Young and Elder Women Based on their Sizes of Ball Joint Girth and Foot Breadth Akiko Yamamoto Fukuoka Women's University,
More informationMott散乱によるParity対称性の破れを検証
Mott Parity P2 Mott target Mott Parity Parity Γ = 1 0 0 0 0 1 0 0 0 0 1 0 0 0 0 1 t P P ),,, ( 3 2 1 0 1 γ γ γ γ γ γ ν ν µ µ = = Γ 1 : : : Γ P P P P x x P ν ν µ µ vector axial vector ν ν µ µ γ γ Γ ν γ
More information技術研究所 研究所報 No.80
Calculating Temperatures in Concrete Elements Exposed to Fire by Hideto Saito and Takeshi Morita Abstract Six concrete-filled steel tube column specimens without fire protection measures were subjected
More information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 informationVisual Evaluation of Polka-dot Patterns Yoojin LEE and Nobuko NARUSE * Granduate School of Bunka Women's University, and * Faculty of Fashion Science,
Visual Evaluation of Polka-dot Patterns Yoojin LEE and Nobuko NARUSE * Granduate School of Bunka Women's University, and * Faculty of Fashion Science, Bunka Women's University, Shibuya-ku, Tokyo 151-8523
More informationFig. 1 Flow diagram of experimental apparatus employed Fig. 2 Porosity change during sulfurization of reduced sample pellets
Fig. 1 Flow diagram of experimental apparatus employed Fig. 2 Porosity change during sulfurization of reduced sample pellets Fig. 4 Simultaneous reduction-sulfurization and direct sulfurization of iron
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 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土木学会構造工学論文集(2011.3)
Vol.57A (11 3 ) RC Consecutve falling-weight impact test of large-scale RC girders under specified total input-impact energy * ** *** **** ***** Norimitsu Kishi, Hisashi Konno, Satoru Yamaguchi, Hiroshi
More informationJan THE JAPANESE JOURNAL OF ANTIBIOTICS XL-1 Table 1. Outline of administering doses, routes and sampling times *: 4 ml/hr/kg Bacillus subtilis
THE JAPANESE JOURNAL OF ANTIBIOTICS XL-1 Jan. 1987 Jan. 1987 THE JAPANESE JOURNAL OF ANTIBIOTICS XL-1 Table 1. Outline of administering doses, routes and sampling times *: 4 ml/hr/kg Bacillus subtilis
More informationJFE.dvi
,, Department of Civil Engineering, Chuo University Kasuga 1-13-27, Bunkyo-ku, Tokyo 112 8551, JAPAN E-mail : atsu1005@kc.chuo-u.ac.jp E-mail : kawa@civil.chuo-u.ac.jp SATO KOGYO CO., LTD. 12-20, Nihonbashi-Honcho
More informationThe 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塗装深み感の要因解析
17 Analysis of Factors for Paint Depth Feeling Takashi Wada, Mikiko Kawasumi, Taka-aki Suzuki ( ) ( ) ( ) The appearance and quality of objects are controlled by paint coatings on the surfaces of the objects.
More informationudc-2.dvi
13 0.5 2 0.5 2 1 15 2001 16 2009 12 18 14 No.39, 2010 8 2009b 2009a Web Web Q&A 2006 2007a20082009 2007b200720082009 20072008 2009 2009 15 1 2 2 2.1 18 21 1 4 2 3 1(a) 1(b) 1(c) 1(d) 1) 18 16 17 21 10
More informationA Nutritional Study of Anemia in Pregnancy Hematologic Characteristics in Pregnancy (Part 1) Keizo Shiraki, Fumiko Hisaoka Department of Nutrition, Sc
A Nutritional Study of Anemia in Pregnancy Hematologic Characteristics in Pregnancy (Part 1) Keizo Shiraki, Fumiko Hisaoka Department of Nutrition, School of Medicine, Tokushima University, Tokushima Fetal
More information0801297,繊維学会ファイバ11月号/報文-01-青山
Faculty of Life Environment, Kinjogakuin University, Moriyama-ku, Nagoya 463-8521, Japan Faculty of Home Economics, Japan Women s University, Bunkyo-ku, Tokyo 112-8681, Japan AStudy on Easing by a Variable
More informationEstimation of Photovoltaic Module Temperature Rise Motonobu Yukawa, Member, Masahisa Asaoka, Non-member (Mitsubishi Electric Corp.) Keigi Takahara, Me
Estimation of Photovoltaic Module Temperature Rise Motonobu Yukawa, Member, Masahisa Asaoka, Non-member (Mitsubishi Electric Corp.) Keigi Takahara, Member (Okinawa Electric Power Co.,Inc.) Toshimitsu Ohshiro,
More information製紙用填料及び顔料の熱分解挙動.PDF
Thermogravimetric analysis of pigments and fillers for papermaking Toshiharu Enomae Graduate School of Agricultural and Life Sciences Contact e-mail address: enomae@psl.fp.a.u-tokyo.ac.jp A2 350 450 A2
More information42 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 informationFig. 1. Schematic drawing of testing system. 71 ( 1 )
1850 UDC 669.162.283 : 669.162.263.24/. 25 Testing Method of High Temperature Properties of Blast Furnace Burdens Yojiro YAMAOKA, Hirohisa HOTTA, and Shuji KAJIKAWA Synopsis : Regarding the reduction under
More informationContinuous Cooling Transformation Diagrams for Welding of Mn-Si Type 2H Steels. Harujiro Sekiguchi and Michio Inagaki Synopsis: The authors performed
Continuous Cooling Transformation Diagrams for Welding of Mn-Si Type 2H Steels. Harujiro Sekiguchi and Michio Inagaki Synopsis: The authors performed a series of researches on continuous cooling transformation
More information474 Nippon Shokuhin Kagaku Kogaku Kaishi Vol. /-, No.3,.1..2* (,**0) 24 Measurement of Deterioration of Frying Oil Using Electrical Properties Yoshio
474 Nippon Shokuhin Kagaku Kogaku Kaishi Vol. / No.3.1..2 (0) 24 Measurement of Deterioration of Frying Oil Using Electrical Properties Yoshio Hagura Yoshihiro Sasaki and Kanichi Suzuki Graduate School
More informationCMP Technical Report No. 4 Department of Computational Nanomaterials Design ISIR, Osaka University 2 2................................. 2.2......................... 2 3 3 3................................
More informationEvaluation of Anisotropy and Preferred Orientation of Carbon and Graphite Materials Yoshihiro Hishiyama Fig.1 Diffraction condition in Fourier space.
Evaluation of Anisotropy and Preferred Orientation of Carbon and Graphite Materials Yoshihiro Hishiyama Fig.1 Diffraction condition in Fourier space. Corresponding Author, E-mail: yhishiya@eng.musashi-tech.ac.jp
More information4/15 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 informationuntitled
2017 5 26 350 Restek time time time increasing time μ = = k = t r t o t o = t r ' t o van Deemter Equation H A B H = height equivalent theoretical plate (HETP) A = Eddy diffusion term B = Molecular diffusion
More informationalternating current component and two transient components. Both transient components are direct currents at starting of the motor and are sinusoidal
Inrush Current of Induction Motor on Applying Electric Power by Takao Itoi Abstract The transient currents flow into the windings of the induction motors when electric sources are suddenly applied to the
More informationStudy on Throw Accuracy for Baseball Pitching Machine with Roller (Study of Seam of Ball and Roller) Shinobu SAKAI*5, Juhachi ODA, Kengo KAWATA and Yu
Study on Throw Accuracy for Baseball Pitching Machine with Roller (Study of Seam of Ball and Roller) Shinobu SAKAI*5, Juhachi ODA, Kengo KAWATA and Yuichiro KITAGAWA Department of Human and Mechanical
More informationweak ferromagnetism observed on Shimotokuyama and Ayumikotan natural crystals behaves as pre dicted by Dzyaloshinsky and Moriya, while Wagasennin and
Magnetic Behavior of a-fe2o3, I. Origin of Weak Ferromagnetism and Magnetic Characteristics Masako IWATA (The Research Institute for Iron, Steel and Other Metals, Tohoku University, Katahiracho, Sendai)
More informationTemperature Rise in a Birefringent Substrate by RF Discharge Plasma Koichi Takaki, Member, Kunioh Sayama, Student Member, Atsushi Takahashi, Student M
Temperature Rise in a Birefringent Substrate by RF Discharge Plasma Koichi Takaki, Member, Kunioh Sayama, Student Member, Atsushi Takahashi, Student Member, Tamiya Fujiwara, Member (Iwate University),
More information日立金属技報 Vol.34
Influence of Misorientation Angle between Adjacent Grains on Magnetization Reversal in Nd-Fe-B Sintered Magnet Tomohito Maki Rintaro Ishii Mitsutoshi Natsumeda Takeshi Nishiuchi Ryo Uchikoshi Masaaki Takezawa
More information28 Horizontal angle correction using straight line detection in an equirectangular image
28 Horizontal angle correction using straight line detection in an equirectangular image 1170283 2017 3 1 2 i Abstract Horizontal angle correction using straight line detection in an equirectangular image
More information(1.2) T D = 0 T = D = 30 kn 1.2 (1.4) 2F W = 0 F = W/2 = 300 kn/2 = 150 kn 1.3 (1.9) R = W 1 + W 2 = = 1100 N. (1.9) W 2 b W 1 a = 0
1 1 1.1 1.) T D = T = D = kn 1. 1.4) F W = F = W/ = kn/ = 15 kn 1. 1.9) R = W 1 + W = 6 + 5 = 11 N. 1.9) W b W 1 a = a = W /W 1 )b = 5/6) = 5 cm 1.4 AB AC P 1, P x, y x, y y x 1.4.) P sin 6 + P 1 sin 45
More information75 unit: mm Fig. Structure of model three-phase stacked transformer cores (a) Alternate-lap joint (b) Step-lap joint 3 4)
3 * 35 (3), 7 Analysis of Local Magnetic Properties and Acoustic Noise in Three-Phase Stacked Transformer Core Model Masayoshi Ishida Kenichi Sadahiro Seiji Okabe 3.7 T 5 Hz..4 3 Synopsis: Methods of local
More informationFig. 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宇宙環境利用蛋白質結晶生成応用利用実証プロジェクトのご案内
16 8 23 1. 14 17 ISS JEM (JAXA) 2. JAXA 14 6 1 4 1 02/02/2003 29/08/2003 29/01/2004 11/08/2004 Baikonur Kazakhstan Progress 03/05/2003 28/10/2003 29/04/2004 19/10/2004 Kazakhstan Soyuz 13 weeks 9 weeks
More informationEVALUATION OF NOCTURNAL PENILE TUMESCENCE (NPT) IN THE DIFFERENTIAL DIAGNOSIS OF IMPOTENCE Masaharu Aoki, Yoshiaki Kumamoto, Kazutomi Mohri and Kazunori Ohno Department of Urology, Sapporo Medical College
More information*1 *2 *1 JIS A X TEM 950 TEM JIS Development and Research of the Equipment for Conversion to Harmless Substances and Recycle of Asbe
*1 *2 *1 JIS A 14812008X TEM 950 TEM 1 2 3 4 JIS Development and Research of the Equipment for Conversion to Harmless Substances and Recycle of Asbestos with Superheated Steam Part 3 An evaluation with
More informationInfluences of mortality from main causes of death on life expectancy. \ An observation for the past 25 years, 1950-1975, in Japan \ Takao SHIGEMATSU* and Zenji NANJO** With the Keyfitz-Nanjo method an
More informationAD8212: 高電圧の電流シャント・モニタ
7 V typ 7 0 V MSOP : 40 V+ V SENSE DC/DC BIAS CIRCUIT CURRENT COMPENSATION I OUT COM BIAS ALPHA 094-00 V PNP 0 7 V typ PNP PNP REV. A REVISION 007 Analog Devices, Inc. All rights reserved. 0-9 -- 0 40
More informationBUNSEKI KAGAKU Vol. 34 (1985) Fig. 1 Diagram of anti-stokes delayed fluorescence (ASDF) by the mixed triplet mechanism (the numbered transitions refer to the equations) BUNSEKI KAGAKU Vol. 34 (1985) Fig.
More information19 σ = P/A o σ B Maximum tensile strength σ % 0.2% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional
19 σ = P/A o σ B Maximum tensile strength σ 0. 0.% 0.% proof stress σ EL Elastic limit Work hardening coefficient failure necking σ PL Proportional limit ε p = 0.% ε e = σ 0. /E plastic strain ε = ε e
More informationLaser Ablation Dynamics of Amorphous Film of a Cu-Phthalocyanine Derivative Masahiro HOSODA*,**, Hiroshi FURUTANI*,**. Hiroshi FUKUMURA*,** Hiroshi MASUHARA*, Masanobu NISHII*** Nobuyuki ICHINOSE**,***,
More informationFrom Evans Application Notes
3 From Evans Application Notes http://www.eaglabs.com From Evans Application Notes http://www.eaglabs.com XPS AES ISS SSIMS ATR-IR 1-10keV µ 1 V() r = kx 2 = 2π µν x mm 1 2 µ= m + m 1 2 1 k ν = OSC 2
More informationNuclear Magnetic Resonance 1 H NMR spectrum PPM
Nuclear Magnetic Resonance 1 NMR spectrum PPM PPM X: X X: 1.5 1.5 1 1 1 1 : 1: 1 : 1.5 : 1.5 2 : 2 : 2 : 3 : 3 1 13 NMR spectrum BM PPM BM 13 NMR spectrum DEPT OSY a b c d a c 1 NMR spectrum PPM a-c a
More informationNote; a: Pressure sensor, b: Semi-permeable membrane, c: O-ring, d: Support screen, e: Solution, f: Solvent. Fig. 2. Osmometer cell. Fig. 1. Schematic
Studies on Collapse of Wood Cells and Negative Pressure in Cell Lumen by Yoshiaki HATTORI* and Yasushi KANAGAWA** The negative pressure, that is liquid-tension, to cause cell-collapse was estimated with
More information(43) Vol.33, No.6(1977) T-239 MUTUAL DIFFUSION AND CHANGE OF THE FINE STRUCTURE OF WET SPUN ANTI-PILLING ACRYLIC FIBER DURING COAGULATION, DRAWING AND
(43) Vol.33, No.6(1977) T-239 MUTUAL DIFFUSION AND CHANGE OF THE FINE STRUCTURE OF WET SPUN ANTI-PILLING ACRYLIC FIBER DURING COAGULATION, DRAWING AND DRYING PROCESSES* By Hiroshi Aotani, Katsumi Yamazaki
More information[Ver. 0.2] 1 2 3 4 5 6 7 1 1.1 1.2 1.3 1.4 1.5 1 1.1 1 1.2 1. (elasticity) 2. (plasticity) 3. (strength) 4. 5. (toughness) 6. 1 1.2 1. (elasticity) } 1 1.2 2. (plasticity), 1 1.2 3. (strength) a < b F
More information放射線化学, 97, 29 (2014)
20 5 Absorption spectra of biomolecules over wide energy range are very important to study their radiation effects in terms of the optical approximation proposed by Platzman. Using synchrotron radiation
More information2 94
32 2008 pp. 93 106 1 Received October 30, 2008 The purpose of this study is to examine the effects of aerobics training class on weight loss for female students in HOKURIKU UNIVERSITY. Seventy four female
More informationUDC : ' : '24' : '24'26' : : A Study of Condition of Pits Formation and Their Fe
UDC 620.193: 669.15'26-194.3: 669.15'24'26-194.3: 669.15'24'26'28-194.3: 669.141.24: 621.385.833.2 A Study of Condition of Pits Formation and Their Features in Chloride Solution Norio FUKASAKO, Hirokazu
More informationRate of Oxidation of Liquid Iron by Pure Oxygen Shiro BAN-YA and Jae-Dong SHIM Synopsis: The rate of oxidation of liquid iron by oxygen gas has been s
Rate of Oxidation of Liquid Iron by Pure Oxygen Shiro BAN-YA and Jae-Dong SHIM Synopsis: The rate of oxidation of liquid iron by oxygen gas has been studied using a volume constant technique. The process
More information1 1 1 1-1 1 1-9 1-3 1-1 13-17 -3 6-4 6 3 3-1 35 3-37 3-3 38 4 4-1 39 4- Fe C TEM 41 4-3 C TEM 44 4-4 Fe TEM 46 4-5 5 4-6 5 5 51 6 5 1 1-1 1991 1,1 multiwall nanotube 1993 singlewall nanotube ( 1,) sp 7.4eV
More informationFig. 3 Coordinate system and notation Fig. 1 The hydrodynamic force and wave measured system Fig. 2 Apparatus of model testing
The Hydrodynamic Force Acting on the Ship in a Following Sea (1 St Report) Summary by Yutaka Terao, Member Broaching phenomena are most likely to occur in a following sea to relative small and fast craft
More information0810_UIT250_soto
UIT UNIMETER SERIES 250 201 Accumulated UV Meter Digital UV Intensity Meter Research & Development CD Medical Biotech Sterilization Exposure Bonding Manufacturing Curing Production Electronic Components
More informationδδ 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 informationSafety Performance of Steel Deck Plate (Flat Decks) Used for Concrete Slab Moulding CONTENTS 1. Introduction ---------------------------------------------------------------- (2) 2. Flat Decks ------------------------------------------------------------------
More informationThe Evaluation on Impact Strength of Structural Elements by Means of Drop Weight Test Elastic Response and Elastic Limit by Hiroshi Maenaka, Member Sh
The Evaluation on Impact Strength of Structural Elements by Means of Drop Weight Test Elastic Response and Elastic Limit by Hiroshi Maenaka, Member Shigeru Kitamura, Member Masaaki Sakuma Genya Aoki, Member
More information強相関電子系ペロブスカイト遷移金属酸化物による光エレクトロニクス 平成 12 年 11 月 ~ 平成 18 年 3 月 研究代表者 : 花村榮一 ( 千歳科学技術大学光科学部 教授 )
強相関電子系ペロブスカイト遷移金属酸化物による光エレクトロニクス 平成 12 年 11 月 ~ 平成 18 年 3 月 研究代表者 : 花村榮一 ( 千歳科学技術大学光科学部 教授 ) χ αβγω χ αβγωβγ αχ χ -1 - ω ω Γ ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω ω -2 - -3 - BO 2 (Rutile) TiO 2
More informationTable 1 Experimental conditions Fig. 1 Belt sanded surface model Table 2 Factor loadings of final varimax criterion 5 6
JSPE-54-04 Factor Analysis of Relationhsip between One's Visual Estimation and Three Dimensional Surface Roughness Properties on Belt Sanded Surface Motoyoshi HASEGAWA and Masatoshi SHIRAYAMA This paper
More informationnews
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 informationpp * Yw; Mq 1. 1L 20 cc [1] Sonoluminescence: Light emission from acoustic cavitation bubble. Pak-Kon Choi (Departm
73 7 2017 pp. 447 454 447 * 43.25.Yw; 78.60.Mq 1. 1L 20 cc [1] Sonoluminescence: Light emission from acoustic cavitation bubble. Pak-Kon Choi (Department of Physics, Meiji University, Kawasaki, 214 8571)
More informationCHEMOTHERAPY APR Fig. 1 Chemical structure of cefotetan (CTT, YM09330)
CHEMOTHERAPY APR. 1982 Fig. 1 Chemical structure of cefotetan (CTT, YM09330) VOL.30 S-1 CHEMOTHERAPY Fig. 2 Comparison of standard curves of CTT on various test organisms by cylinder plate method Column
More information電子部品はんだ接合部の熱疲労寿命解析
43 Evaluation for Thermal Fatigue Life of Solder Joints in Electronic Components Haruhiko Yamada, Kazuyoshi Ogawa 2 63Sn- 37Pb 95Pb-5Sn Si Cu Si 63Sn-37Pb Since automotive electronic components are used
More informationIntroduction ur company has just started service to cut out sugar chains from protein and supply them to users by utilizing the handling technology of
Standard PA-Sugar Chain Catalogue Masuda Chemical Industries Co., LTD. http://www.mc-ind.co.jp Introduction ur company has just started service to cut out sugar chains from protein and supply them to users
More informationDegradation 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 informationOn the Wireless Beam of Short Electric Waves. (VII) (A New Electric Wave Projector.) By S. UDA, Member (Tohoku Imperial University.) Abstract. A new e
On the Wireless Beam of Short Electric Waves. (VII) (A New Electric Wave Projector.) By S. UDA, Member (Tohoku Imperial University.) Abstract. A new electric wave projector is proposed in this paper. The
More informationJFE(和文)No.4-12_下版Gのコピー
JFE No. 4 245 p. 6358 Electrical Steels for Advanced Automobiles Core Materials for Motors, Generators, and High-frequency Reactors SENDA Kunihiro JFE NAMIKAWA JFEMisao HAYAKAWA JFEYasuyuki JNE JNEH JGE
More information02-量子力学の復習
4/17 No. 1 4/17 No. 2 4/17 No. 3 Particle of mass m moving in a potential V(r) V(r) m i ψ t = 2 2m 2 ψ(r,t)+v(r)ψ(r,t) ψ(r,t) Wave function ψ(r,t) = ϕ(r)e iωt steady state 2 2m 2 ϕ(r)+v(r)ϕ(r) = εϕ(r)
More informationFig. 3 Flow diagram of image processing. Black rectangle in the photo indicates the processing area (128 x 32 pixels).
Fig. 1 The scheme of glottal area as a function of time Fig. 3 Flow diagram of image processing. Black rectangle in the photo indicates the processing area (128 x 32 pixels). Fig, 4 Parametric representation
More informationCaloric Behavior of Chemical Oscillation Reactions Shuko Fujieda (Received December 16, 1996) Chemical oscillation behavior of Belousov- Zhabotinskii
Caloric Behavior of Chemical Oscillation Reactions Shuko Fujieda (Received December 16, 1996) Chemical oscillation behavior of Belousov- Zhabotinskii (BZ) and Briggs- Rauscher (BR) reactions was followed
More informationStereoelectronic Effect
node anti bonding M ( σ* ) A A : bonding M ( σ ) A: atomic orbital M: molecular orbital node anti bonding M filled orbital of molecular 1 M bonding M vacant orbital of molecular 2 LUM LUM (lowest unoccupied
More information1) 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 informationperature was about 2.5 Ž higher than that of the control irrespective of wind speed. With increasing wind speeds of more than 1m/s, the leaf temperatu
Studies on the Row Covering Methods of Vinylon Cheesecloth to Prevent Cold Injury in Cabbage Daizou IGARASHI*, Masumi OKADA** and Keiichl NAKAYAMA*** *Miura Branch, Kanagawa Horticultural Experiment Station,
More information1) T. L. Cottrel, A. J. Matheson, Trans. Farad. Soc., 58, 2336(1962). 2) E. N. Chesnokov, V. N. Panfilov, Teor. Eksp. Khimiya, 17, 699(1981). 3) M. Ko
1) T. L. Cottrel, A. J. Matheson, Trans. Farad. Soc., 58, 2336(1962). 2) E. N. Chesnokov, V. N. Panfilov, Teor. Eksp. Khimiya, 17, 699(1981). 3) M. Koshi, M. Yoshimura, K. Koseki, H. Matsui, "Photoacoustic
More informationuntitled
SPring-8 RFgun JASRI/SPring-8 6..7 Contents.. 3.. 5. 6. 7. 8. . 3 cavity γ E A = er 3 πε γ vb r B = v E c r c A B A ( ) F = e E + v B A A A A B dp e( v B+ E) = = m d dt dt ( γ v) dv e ( ) dt v B E v E
More informationuntitled
20 * Re-Evaluation of Isoseismal Maps and Magnitudes from Two Big Earthquakes along the Subduction Zone of Kyushu and Ryukyu Islands Early in the 20th Century Masayuki TAKEMURA, Katsuhisa KANDA Kobori
More informationTitle 混合体モデルに基づく圧縮性流体と移動する固体の熱連成計算手法 Author(s) 鳥生, 大祐 ; 牛島, 省 Citation 土木学会論文集 A2( 応用力学 ) = Journal of Japan Civil Engineers, Ser. A2 (2017), 73 Issue
Title 混合体モデルに基づく圧縮性流体と移動する固体の熱連成計算手法 Author(s) 鳥生, 大祐 ; 牛島, 省 Citation 土木学会論文集 A2( 応用力学 ) = Journal of Japan Civil Engineers, Ser. A2 (2017), 73 Issue Date 2017 URL http://hdl.handle.net/2433/229150 Right
More information報告書 H22-2A-09
061-0293 1757 TEL 0133-23-1211 2.0% 0.5% in vitro QOL Quality of Life 1 MCE-400 400 mpa s Duck Algin 350M M/G 0.8 70 80 C 20% 50 C 1.0% 5 C SV-10 5 C 10 ml E TV 20H model E 1 34 R24 1 ml 5 C 30 6 12 30
More information[1] 2 キトラ古墳天文図に関する従来の研究とその問題点 mm 3 9 mm cm 40.3 cm 60.6 cm 40.5 cm [2] 9 mm [3,4,5] [5] 1998
18 1 12 2016 キトラ古墳天文図の観測年代と観測地の推定 2015 5 15 2015 10 7 Estimating the Year and Place of Observations for the Celestial Map in the Kitora Tumulus Mitsuru SÔMA Abstract Kitora Tumulus, located in Asuka, Nara
More information304 Nippon Shokuhin Kagaku Kogaku Kaishi Vol. /., No.0, -*. -*3 (,**1) 58 * ** *** : * : ** *** Development of Sorting System Based on Potato Starch C
304 Nippon Shokuhin Kagaku Kogaku Kaishi Vol. /., No.0, -*. -*3 (,**1) 58 * ** *** : * : ** *** Development of Sorting System Based on Potato Starch Content Using Visible and Near-Infrared Spectroscopy
More informationFundamental 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 informationDISTRIBUTION OF NEUROPEPTIDES IN THE INFERIOR NASAL TURBINATE MUCOSA OF PATIENTS WITH ALLERGIC RHINITIS KAZUHIRO YAMAMOTO. M.D. Department of Otolaryngology, School of Medicine, Kitasato University, Sagamihara
More information07_学術.indd
Arts and Sciences computed radiography CRpresampled MTF Measurement of presampled MTFs with computed radiography (CR) by contrast method using smoothed square-wave. 1 16813 1, 2 1 1 1 2 Key words: contrast
More informationTable 1. Shape and smelting properties of chrome ores as delivered. Table 2. Chemical composition of chrome ores (%). Table 3. Chemical composition of
UDC 669.263.1: 669.046.462 The Reduction Process and Reducibility of Chromite with Carbon Hiroshi G. KATAYAMA and Akihiko TANAKA Synopsis: In the present work, various chrome ores and relatively pure chromites
More information(check matrices and minimum distances) H : a check matrix of C the minimum distance d = (the minimum # of column vectors of H which are linearly depen
Hamming (Hamming codes) c 1 # of the lines in F q c through the origin n = qc 1 q 1 Choose a direction vector h i for each line. No two vectors are colinear. A linearly dependent system of h i s consists
More informationrcnp01may-2
E22 RCP Ring-Cyclotron 97 953 K beam K-atom HF X K, +,K + e,e K + -spectroscopy OK U U I= First-order -exchange - coupling I= U LS U LS Meson-exchange model /5/ I= Symmetric LS Anti-symmetric LS ( σ Λ
More informationuntitled
JIS A 12190000 Method for standard penetration test 2005 1 ISO 22476-3:2005 J J 1 SPTSPT 63.5 kg 760 mm SPT N SPT 300 mm N A 2 ISO 22475-1,Geotechnical investigation and testing Sampling methods and groundwater
More informationA comparison of abdominal versus vaginal hysterectomy for leiomyoma and adenomyosis Kenji ARAHORI, Hisasi KATAYAMA, Suminori NIOKA Department of Obstetrics and Gnecology, National Maizuru Hospital,Kyoto,
More informationELECTRONIC IMAGING IN ASTRONOMY Detectors and Instrumentation 5 Instrumentation and detectors
ELECTRONIC IMAGING IN ASTRONOMY Detectors and Instrumentation 5 Instrumentation and detectors 4 2017/5/10 Contents 5.4 Interferometers 5.4.1 The Fourier Transform Spectrometer (FTS) 5.4.2 The Fabry-Perot
More information揃 24 1681 0 20 40 60 80 100 0 21 42 63 84 Lag [hour] Lag [day] 35
Forecasting Model for Electricity Consumption in Residential House Based on Time Series Analysis * ** *** Shuhei Kondo Nobayasi Masamori Shuichi Hokoi ( 2015 7 3 2015 12 11 ) After the experience of electric
More informationuntitled
9118 154 B-1 B-3 B- 5cm 3cm 5cm 3m18m5.4m.5m.66m1.3m 1.13m 1.134m 1.35m.665m 5 , 4 13 7 56 M 1586.1.18 7.77.9 599.5.8 7 1596.9.5 7.57.75 684.11.9 8.5 165..3 7.9 87.8.11 6.57. 166.6.16 7.57.6 856 6.6.5
More information九州大学学術情報リポジトリ Kyushu University Institutional Repository 看護師の勤務体制による睡眠実態についての調査 岩下, 智香九州大学医学部保健学科看護学専攻 出版情報 : 九州大学医学部保健学
九州大学学術情報リポジトリ Kyushu University Institutional Repository 看護師の勤務体制による睡眠実態についての調査 岩下, 智香九州大学医学部保健学科看護学専攻 https://doi.org/10.15017/4055 出版情報 : 九州大学医学部保健学科紀要. 8, pp.59-68, 2007-03-12. 九州大学医学部保健学科バージョン : 権利関係
More informationS-5.indd
Development and pplication of Ultrasonic Noise B-scan nalysis ( I-CLT ) Creep Damage ssessment for Fossil-Fuel Boiler Piping precise creep damage assessment method has been required for boiler plants using
More information