原子・分子架橋系の量子輸送の理論 現状と展望

outline SPM,

AFM WPI-Advanced Institute for Materials Research 167 67 2012.. (NIMS) outline 1. 2. SPM, 3. 4. 5. 6. STM/STS, AFM KPFM, SNOM,. What and how Does SPM see the sample??? 2004~2007, 2009~2011 1. AFM 1A. 1B.

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

chap1_MDpotentials.ppt

simplest Morse : simplest (1 Well-chosen functional form is more useful than elaborate fitting strategies!! Phys. Rev. 34, 57 (1929 ( 2 E ij = D e 1" exp("#(r ij " r e 2 r ij = r i " r j r ij =r e E ij

燃焼圧センサ

49 Combustion Pressure Sensor Kouji Tsukada, Masaharu Takeuchi, Sanae Tokumitsu, Yoshiteru Ohmura, Kazuyoshi Kawaguchi π 1000N 150 225N 1 F.S Abstract A new combustion pressure sensor capable of measuring

スライド 1

Matsuura Laboratory SiC SiC 13 2004 10 21 22 H-SiC ( C-SiC HOY Matsuura Laboratory n E C E D ( E F E T Matsuura Laboratory Matsuura Laboratory DLTS Osaka Electro-Communication University Unoped n 3C-SiC

02-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)

Influence of Material and Thickness of the Specimen to Stress Separation of an Infrared Stress Image Kenji MACHIDA The thickness dependency of the temperature image obtained by an infrared thermography

untitled

213 74 AlGaN/GaN Influence of metal material on capacitance for Schottky-gated AlGaN/GaN 1, 2, 1, 2, 2, 2, 2, 2, 2, 2, 1, 1 1 AlGaN/GaN デバイス ① GaNの優れた物性値 ② AlGaN/GaN HEMT構造 ワイドバンドギャップ半導体 (3.4eV) 絶縁破壊電界が大きい

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

T05_Nd-Fe-B磁石.indd

Influence of Intergranular Grain Boundary Phases on Coercivity in Nd-Fe-B-based Magnets Takeshi Nishiuchi Teruo Kohashi Isao Kitagawa Akira Sugawara Hiroyuki Yamamoto To determine how to increase the coercivity

1 1.1,,,.. (, ),..,. (Fig. 1.1). Macro theory (e.g. Continuum mechanics) Consideration under the simple concept (e.g. ionic radius, bond valence) Stru

1. 1-1. 1-. 1-3.. MD -1. -. -3. MD 1 1 1.1,,,.. (, ),..,. (Fig. 1.1). Macro theory (e.g. Continuum mechanics) Consideration under the simple concept (e.g. ionic radius, bond valence) Structural relaxation

Input image Initialize variables Loop for period of oscillation Update height map Make shade image Change property of image Output image Change time L

1,a) 1,b) 1/f β Generation Method of Animation from Pictures with Natural Flicker Abstract: Some methods to create animation automatically from one picture have been proposed. There is a method that gives

weak 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)

untitled

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

28 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

将来（２０１０年前後を想定）の研究目標とスーパーコンピューティング環境について(物質・材料研究機構)

(2010 2 1 NEC-SX4 16cpu x 2GFLOPS/cpu 1996 42000 3 2 NEC-SX5 32cpu x 8GFLOPS/cpu 2000 42004 3 90% MD 99% 1cpu cpu 3 cpu 99% MPI, OpenMP 4 or 3 HITACHI-SR11000 64node x 16cpu/node x 6.8GFLOPS/cpu 2004 4

Fig. 1 Schematic construction of a PWS vehicle Fig. 2 Main power circuit of an inverter system for two motors drive

An Application of Multiple Induction Motor Control with a Single Inverter to an Unmanned Vehicle Propulsion Akira KUMAMOTO* and Yoshihisa HIRANE* This paper is concerned with a new scheme of independent

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

OPA134/2134/4134('98.03)

OPA OPA OPA OPA OPA OPA OPA OPA OPA TM µ Ω ± ± ± ± + OPA OPA OPA Offset Trim Offset Trim Out A V+ Out A Out D In +In V+ Output In A +In A A B Out B In B In A +In A A D In D +In D V NC V +In B V+ V +In

SiC SiC QMAS(Quantum MAterials Simulator) VASP(Vienna Ab-initio Simulation Package) SiC 3C, 4H, 6H-SiC EV VASP VASP 3C, 4H, 6H-SiC (0001) (11 20) (1 1

QMAS SiC 7661 24 2 28 SiC SiC QMAS(Quantum MAterials Simulator) VASP(Vienna Ab-initio Simulation Package) SiC 3C, 4H, 6H-SiC EV VASP VASP 3C, 4H, 6H-SiC (0001) (11 20) (1 100) MedeA SiC QMAS - C Si (0001)

PowerPoint プレゼンテーション

Drain Voltage (mv) 4 2 0-2 -4 0.0 0.2 0.4 0.6 0.8 1.0 Gate Voltage (V) Vds [V] 0.2 0.1 0.0-0.1-0.2-10 -8-6 -4-2 0 Vgs [V] 10 1000 1000 1000 1000 (LSI) Fe Catalyst Fe Catalyst Carbon nanotube 1~2 nm

食糧　その科学と技術　No.43( )

17 DNA SEM, Scanning electron microscope TEM, transmission electron microscope X NMR AFM, atomic force microscopy SPM, scanning probe microscopy 1 SPM SPM AFM SNOM NSOM, Scanning near-field optical microscope

THE INSTITUTE OF ELECTRONICS, INFORMATION AND COMMUNICATION ENGINEERS TECHNICAL REPORT OF IEICE.

THE INSTITUTE OF ELECTRONICS, INFORMATION AND COMMUNICATION ENGINEERS TECHNICAL REPORT OF IEICE. E-mail: {ytamura,takai,tkato,tm}@vision.kuee.kyoto-u.ac.jp Abstract Current Wave Pattern Analysis for Anomaly

PowerPoint Presentation

2010 KEK (Japan) (Japan) (Japan) Cheoun, Myun -ki Soongsil (Korea) Ryu,, Chung-Yoe Soongsil (Korea) 1. S.Reddy, M.Prakash and J.M. Lattimer, P.R.D58 #013009 (1998) Magnetar : ~ 10 15 G ~ 10 17 19 G (?)

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

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

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

LC304_manual.ai

Stick Type Electronic Calculator English INDEX Stick Type Electronic Calculator Instruction manual INDEX Disposal of Old Electrical & Electronic Equipment (Applicable in the European Union

Study 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,

BH BH BH BH Typeset by FoilTEX 2

GR BH BH 2015.10.10 BH at 2015.09.07 NICT 2015.05.26 Typeset by FoilTEX 1 BH BH BH BH Typeset by FoilTEX 2 1. BH 1.1 1 Typeset by FoilTEX 3 1.2 2 A B A B t = 0 A: m a [kg] B: m b [kg] t = t f star free

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.

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

Microsoft PowerPoint - 山形大高野send ppt [互換モード]

, 2012 10 SCOPE, 2012 10 2 CDMA OFDMA OFDM SCOPE, 2012 10 OFDM 0-20 Relative Optical Power [db] -40-60 10 Gbps NRZ BPSK-SSB 36dB -80-20 -10 0 10 20 Relative Frequency [GHz] SSB SSB OFDM SSB SSB OFDM OFDM

vdw-df vdw-df vdw-df 2

WPI-AIMR ikutaro@wpi-aimr.tohoku.ac.jp 1 vdw-df vdw-df vdw-df 2 (Semi-)local approximation in density-functional theory - Local density approximation (LDA) Good structural and dynamical properties of solids

1

2-2 Atom Optics and Atom Lithography OHMUKAI Ryuzo and WATANABE Masayoshi High-resolution atomic channeling using velocity-selected atoms may be able to overcome precision limitations of the conventional

音響部品アクセサリ本文(AC06)PDF (Page 16)

Guide for Electret Condenser Microphones A microphone as an audio-electric converting device, whose audio pickup section has a structure of a condenser consisting of a diaphragm and a back plate opposite

25 Removal of the fricative sounds that occur in the electronic stethoscope

25 Removal of the fricative sounds that occur in the electronic stethoscope 1140311 2014 3 7 ,.,.,.,.,.,.,.,,.,.,.,.,,. i Abstract Removal of the fricative sounds that occur in the electronic stethoscope

[ 30 p. 1-8 (2012)] / ** *** Numerical Analysis of Metal Transfer Phenomena - critical condition between globular and spray transfer mode - by KADOTA

[ 30 p. 1-8 (2012)] / ** *** Numerical Analysis of Metal Transfer Phenomena - critical condition between globular and spray transfer mode - by KADOTA Keiji and HIRATA Yoshinori Metal transfer modes in

Mikio 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

Developement of Plastic Collocation Method Extension of Plastic Node Method by Yukio Ueda, Member Masahiko Fujikubo, Member Masahiro Miura, Member Sum

Developement of Plastic Collocation Method Extension of Plastic Node Method by Yukio Ueda, Member Masahiko Fujikubo, Member Masahiro Miura, Member Summary Previously, the authors developed the plastic

第3節

Prolith 3.1 Post Exposure Bake PEB PC 1970 F.H.Dill [1-2] PC Aerial Image Image in Resist Latent Image before PEB Resist Profile Develop Time Contours Latent Image after PEB 1 NA PEB [3-4] NA Cr 2 3 (b)

080906_…o…−…^…b…vVSCW

Thyristor Type Single-Phase Power Regulator 2030 A 6A 150200A TOKYO RIKOSHA CO., LTD Latest VARITAP VSCW Series Achieved 1/2 the width (our company comparison). Free Power source of 100 to 240V specification.cover-type

189 2015 1 80

189 2015 1 A Design and Implementation of the Digital Annotation Basis on an Image Resource for a Touch Operation TSUDA Mitsuhiro 79 189 2015 1 80 81 189 2015 1 82 83 189 2015 1 84 85 189 2015 1 86 87

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),

WATOC2005 Best Poster Diamond Certificate α -(BEDT-TTF) 2 IBr 2 H.turkmenica X H C H O Brønsted Al K Electronic structure of CeNiGe 2 x Si x studied by Ce 4d-4f resonant and angleresolved photoemission

The Effect of the Circumferential Temperature Change on the Change in the Strain Energy of Carbon Steel during the Rotatory Bending Fatigue Test by Ch

The Effect of the Circumferential Temperature Change on the Change in the Strain Energy of Carbon Steel during the Rotatory Bending Fatigue Test by Chikara MINAMISAWA, Nozomu AOKI (Department of Mechanical

OPA277/2277/4277 (2000.1)

R OPA OPA OPA OPA OPA OPA OPA OPA OPA µ µ ± ± µ OPA ±± ±± ± µ Offset Trim Offset Trim In OPA +In -Pin DIP, SO- Output NC OPA Out A In A +In A A D Out D In D +In D Out A In A +In A A B Out B In B +In B

75 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

The 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

Table 1. Assumed performance of a water electrol ysis plant. Fig. 1. Structure of a proposed power generation system utilizing waste heat from factori

Proposal and Characteristics Evaluation of a Power Generation System Utilizing Waste Heat from Factories for Load Leveling Pyong Sik Pak, Member, Takashi Arima, Non-member (Osaka University) In this paper,

PDF

1 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

(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

Spacecraft Propulsion Using Solar Energy Spacecraft with Magnetic Field Light from the Sun Solar Wind Thrust Mirror Solar Sail Thrust production by li

2004.3.28 物理学会シンポジウム 磁気プラズマセイル の可能性と 深宇宙探査への挑戦 宇宙航空研究開発機構 船木一幸 Spacecraft Propulsion Using Solar Energy Spacecraft with Magnetic Field Light from the Sun Solar Wind Thrust Mirror Solar Sail Thrust production

技術研究報告第２６号

1) 2) 3) 250Hz 500Hz RESEARCH ON THE PHYSICAL VOLUME OF THE DYNAMIC VIBRATION RESPONSE AND THE REDUCTION OF THE FLOOR IMPACT SOUND LEVEL IN FLOORS OF RESIDENTIAL HOUSING Hideo WATANABE *1 This study was

Jan 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

Fig. 1. Relation between magnetron anode current and anode-cathod voltage. Fig. 2. Inverter circuit for driving a magnetron. 448 T. IEE Japan, Vol. 11

High Frequency Inverter for Microwave Oven Norikazu Tokunaga, Member, Yasuo Matsuda, Member, Kunio Isiyama, Non-member (Hitachi, Ltd.), Hisao Amano, Member (Hitachi Engineering, Co., Ltd.). Recently resonant

200708_LesHouches_02.ppt

Numerical Methods for Geodynamo Simulation Akira Kageyama Earth Simulator Center, JAMSTEC, Japan Part 2 Geodynamo Simulations in a Sphere or a Spherical Shell Outline 1. Various numerical methods used

PFニュース indd

最近の研究から Ｘ線回折法による Si(111) 表面における Ag の超構造および薄膜結晶配向性の研究 高橋敏男 1 * 田尻寛男 1 隅谷和嗣 1 秋本晃一 2 1 東京大学物性研究所 2 名古屋大学大学院工学研究科 Structural studies on superstructures and thin films of Ag on Si(111) by X-ray diffraction

pp * 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)

研究成果報告書(基金分)

(DMS) 1 3 DMS 2 4 DMS II-VI CdTe ZnTe 2 4 DMS 2 4 DMS II-VI 2 3d 4 3d (MBE) II-VI ZnTe CdTe 3d Mn, Cr, Fe 2 4 DMS MBE X (XRD)X (XAFS) II (SQUID) (a) 4 DMS (Cd,Mn,Cr)Te 4 DMS II-VI CdTe 2 Mn, Cr (Cd,Mn,Cr)Te

橡最終原稿.PDF

GIS Simulation analysis of disseminate of disaster information using GIS * ** *** Toshitaka KATADAJunsaku ASADA and Noriyuki KUWASAWA GIS GIS AbstractWe have developed the simulation model expressing the

1. 2. 3. 2010-02- 22-24 1.1 1.1.1 1.1.2 1.1.3 F10.7 1.2 1.2.1 1.2.2 1.2.3 14 C 1.2.4 10 Be 1.2.5 14 C 10 Be 1.1 太陽放射とその変動 20100223-24森羅万象学校 1.1.1 (from Encyclopedia of Earth) op1cal depth (Lean et al.,

IPSJ SIG Technical Report Vol.2014-EIP-63 No /2/21 1,a) Wi-Fi Probe Request MAC MAC Probe Request MAC A dynamic ads control based on tra

1,a) 1 1 2 1 Wi-Fi Probe Request MAC MAC Probe Request MAC A dynamic ads control based on traffic Abstract: The equipment with Wi-Fi communication function such as a smart phone which are send on a regular

EQUIVALENT TRANSFORMATION TECHNIQUE FOR ISLANDING DETECTION METHODS OF SYNCHRONOUS GENERATOR -REACTIVE POWER PERTURBATION METHODS USING AVR OR SVC- Ju

EQUIVALENT TRANSFORMATION TECHNIQUE FOR ISLANDING DETECTION METHODS OF SYNCHRONOUS GENERATOR -REACTIVE POWER PERTURBATION METHODS USING AVR OR SVC- Jun Motohashi, Member, Takashi Ichinose, Member (Tokyo

AD8212: 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

LM6172 デュアル高速低消費電力、低歪み電圧帰還アンプ

Dual High Speed, Low Power, Low Distortion, Voltage Feedback Amplifiers Literature Number: JAJS854 100MHz 3000V/ s 50mA 2.3mA/ 15V ADSL 5V VIP III (Vertically Integrated PNP) LM6171 Dual High Speed, Low

note4.dvi

10 016 6 0 4 (quantum wire) 4.1 4.1.1.6.1, 4.1(a) V Q N dep ( ) 4.1(b) w σ E z (d) E z (d) = σ [ ( ) ( )] x w/ x+w/ π+arctan arctan πǫǫ 0 d d (4.1) à ƒq [ƒg w ó R w d V( x) QŽŸŒ³ džq x (a) (b) 4.1 (a)

特-3.indd

Development of Automation Technology for Precision Finishing Works Employing a Robot Arm There is demand for the automation of finishing processes that require technical skills in the manufacturing of

1

5-3 Photonic Antennas and its Application to Radio-over-Fiber Wireless Communication Systems LI Keren, MATSUI Toshiaki, and IZUTSU Masayuki In this paper, we presented our recent works on development of

(Jackson model) Ziman) (fluidity) (viscosity) (Free v

1) 16 6 10 1) e-mail: nishitani@ksc.kwansei.ac.jp 0. 1 2 0. 1. 1 2 0. 1. 2 3 0. 1. 3 4 0. 1. 4 5 0. 1. 5 6 0. 1. 6 (Jackson model) 8 0. 1. 7 10. 1 10 0. 1 0. 1. 1 Ziman) (fluidity) (viscosity) (Free volume)(

RTM RTM Risk terrain terrain RTM RTM 48

Risk Terrain Model I Risk Terrain Model RTM,,, 47 RTM RTM Risk terrain terrain RTM RTM 48 II, RTM CSV,,, RTM Caplan and Kennedy RTM Risk Terrain Modeling Diagnostics RTMDx RTMDx RTMDx III 49 - SNS 50 0

Fig. 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

September 9, 2002 ( ) [1] K. Hukushima and Y. Iba, cond-mat/ [2] H. Takayama and K. Hukushima, cond-mat/020

mailto:hukusima@issp.u-tokyo.ac.jp September 9, 2002 ( ) [1] and Y. Iba, cond-mat/0207123. [2] H. Takayama and, cond-mat/0205276. Typeset by FoilTEX Today s Contents Against Temperature Chaos in Spin Glasses

Fig. 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

IntroductionToQuantumComputer

http://quantphys.org/wp/keisukefujii/?p=433 Twitter Keisuke Fujii@fgksk ? 1687: () Isaac Newton (1642-1727) http://www.newton.cam.ac.uk/art/portrait.html Equation of motion ? 1687: () 1873: () James C.

LM837 Low Noise Quad Operational Amplifier (jp)

Low Noise Quad Operational Amplifier Literature Number: JAJSBB7 600 Low Noise Quad Operational Amplifier 2000 8 Converted to nat2000 DTD ds009047tl/h/9047 33020 19860602 10 V/ s ( ); 8 V/ s ( ) 25 MHz

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

rcnp01may-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

LMV851/LMV852/LMV854 8 MHz Low Power CMOS, EMI Hardened Operational Amplifi(jp)

LMV851,LMV852,LMV854 LMV851/LMV852/LMV854 8 MHz Low Power CMOS, EMI Hardened Operational Amplifiers Literature Number: JAJSAM3 LMV851/LMV852/LMV854 8MHz CMOS EMI LMV851/LMV852/LMV854 CMOS IC 40 125 LMV851/

Mｏｔｔ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

Frontier Simulation Software for Industrial Science

PACS-CS FIRST 2005 2005 2 16 17 2 28 2 17 2 28 3 IT IT H14~H16 CHASE CHASE-3PT Protein Protein-DF ABINIT-MP 17 2 28 4 CMOS Si-CMOS CMOS-LSI CMOS ATP 10nm 17 2 28 5 17 2 28 6 CMOS CMOS-LSI LSI 90nm CMOS

Google Social Influences and Legal Issues of Google Street View Hiroshi Takada

Social Influences and Legal Issues of Google Street View Hiroshi Takada Sanno University Bulletin Vol. No. September Social Influences and Legal Issues of Google Street View Hiroshi Takada In this paper,

i

009 I 1 8 5 i 0 1 0.1..................................... 1 0.................................................. 1 0.3................................. 0.4........................................... 3

Fig. 1. Horizontal displacement of the second and third order triangulation points accompanied with the Tottori Earthquake of (after SATO, 1973)

Journal of the Geodetic Society of Japan Vol. 27, No. 3, (1981), pp. 183-191 Research on Fault Movement by means of Aero-Triangulation ( T) (An experiment on the earthquake fault of the Izu-Oshima Kinkai

Huawei G6-L22 QSG-V100R001_02

G6 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 1 2 3 17 4 5 18 UI 100% 8:08 19 100% 8:08 20 100% 8:08 21 100% 8:08 22 100% 8:08 ********** 23 100% 8:08 Happy birthday! 24 S S 25 100% 8:08 26 http://consumer.huawei.com/jp/

PowerPoint プレゼンテーション

実空間差分法に基づく 第一原理電子構造 量子輸送特性計算 09/05/15 大阪大学大学院工学研究科小野倫也 Real-space first-principles calculation code The grand-state electronic structure is obtained by solving the Schrödinger (Kohn-Sham) equation 1 2

RIBF

MEASUREMENT OF ISOCHRONISM OF RIBF CYCLOTRONS Ryo Koyama 1, A), B), Masaki Fujimaki A), Nobuhisa Fukunishi A), Akira Goto A), Masatake Hemmi A), Masayuki Kase A), Naruhiko Sakamoto A), Tamaki Watanabe

IPSJ SIG Technical Report Vol.2016-CE-137 No /12/ e β /α α β β / α A judgment method of difficulty of task for a learner using simple

1 2 3 4 5 e β /α α β β / α A judgment method of difficulty of task for a learner using simple electroencephalograph Katsuyuki Umezawa 1 Takashi Ishida 2 Tomohiko Saito 3 Makoto Nakazawa 4 Shigeichi Hirasawa

I N S T R U M E N T A T I O N & E L E C T R I C A L E Q U I P M E N T STW Symbol Symbol otary switch) 05 otary switch Symbol angle of notch 181

These items are using an aluminum alloy cast, so the weight is corrosion-resistant and excel halo tolerance and is light-weight and it's about 1/3 compared with conventional cast iron and made of steel

DPA,, ShareLog 3) 4) 2.2 Strino Strino STRain-based user Interface with tacticle of elastic Natural ObjectsStrino 1 Strino ) PC Log-Log (2007 6)

1 2 1 3 Experimental Evaluation of Convenient Strain Measurement Using a Magnet for Digital Public Art Junghyun Kim, 1 Makoto Iida, 2 Takeshi Naemura 1 and Hiroyuki Ota 3 We present a basic technology

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

1 Fig. 1 Extraction of motion,.,,, 4,,, 3., 1, 2. 2.,. CHLAC,. 2.1,. (256 ).,., CHLAC. CHLAC, HLAC. 2.3 (HLAC ) r,.,. HLAC. N. 2 HLAC Fig. 2

CHLAC 1 2 3 3,. (CHLAC), 1).,.,, CHLAC,.,. Suspicious Behavior Detection based on CHLAC Method Hideaki Imanishi, 1 Toyohiro Hayashi, 2 Shuichi Enokida 3 and Toshiaki Ejima 3 We have proposed a method for

24 Depth scaling of binocular stereopsis by observer s own movements

24 Depth scaling of binocular stereopsis by observer s own movements 1130313 2013 3 1 3D 3D 3D 2 2 i Abstract Depth scaling of binocular stereopsis by observer s own movements It will become more usual

Postoperative Assessment by Using a Torque Machine (BIODEX) and MRIs in Patients treated for a Recurrent Anterior Dislocation or Subluxation of the Sh

Postoperative Assessment by Using a Torque Machine (BIODEX) and MRIs in Patients treated for a Recurrent Anterior Dislocation or Subluxation of the Shoulder by HATA Yukihiko MURAKAMI Narumichi Department

2

8 23 26A800032A8000 31 37 42 51 2 3 23 37 10 11 51 4 26 7 28 7 8 7 9 8 5 6 7 9 8 17 7 7 7 37 10 13 12 23 21 21 8 53 8 8 8 8 1 2 3 17 11 51 51 18 23 29 69 30 39 22 22 22 22 21 56 8 9 12 53 12 56 43 35 27

2

8 22 19A800022A8000 30 37 42 49 2 3 22 37 10 11 49 4 24 27 7 49 7 8 7 9 8 5 6 7 9 8 16 7 7 7 37 10 11 20 22 20 20 8 51 8 8 9 17 1 2 3 16 11 49 49 17 22 28 48 29 33 21 21 21 21 20 8 10 9 28 9 53 37 36 25

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

A Feasibility Study of Direct-Mapping-Type Parallel Processing Method to Solve Linear Equations in Load Flow Calculations Hiroaki Inayoshi, Non-member

A Feasibility Study of Direct-Mapping-Type Parallel Processing Method to Solve Linear Equations in Load Flow Calculations Hiroaki Inayoshi, Non-member (University of Tsukuba), Yasuharu Ohsawa, Member (Kobe

δf = δn I [ ( FI (N I ) N I ) T,V δn I [ ( FI N I ( ) F N T,V ( ) FII (N N I ) + N I ) ( ) FII T,V N II T,V T,V ] ] = 0 = 0 (8.2) = µ (8.3) G

8 ( ) 8. 1 ( ) F F = F I (N I, T, V I ) + F II (N II, T, V II ) (8.1) F δf = δn I [ ( FI (N I ) N I 8. 1 111 ) T,V δn I [ ( FI N I ( ) F N T,V ( ) FII (N N I ) + N I ) ( ) FII T,V N II T,V T,V ] ] = 0

CMP Technical Report No. 4 Department of Computational Nanomaterials Design ISIR, Osaka University 2 2................................. 2.2......................... 2 3 3 3................................