Proton Conduction Mechanism in Water Nanotube of New Molecular Porous Crystal

Size: px
Start display at page:

Download "Proton Conduction Mechanism in Water Nanotube of New Molecular Porous Crystal"

Transcription

1 Proton Conduction Mechanism in Water anotube of ew Molecular Porous Crystal Tohoku Univ.. Matsui Tokyo Univ. of Science M. Tadokoro Structure and dynamics of confined water in nanospace the present water network (water nanotube) in the nanochannel Quasi one-dimensional high proton conductor Infrared spectra + microwave conductivity the motif of hydrated proton (estimation of the mobility) SSPC16

2 ~1.5 nm c axis Water network is formed inside the hydrophilic nanochannel. TMA 3- trimesic acid 2,2 -biinidazole cobalt(iii) complex M. Tadokoro et al. Chem. Commun. (2006) 1274; J. Phys. Chem. B 114 (2010) 2091.

3 DSC experiment IT WT melting of bulk water Water nanotube (WT) X-ray crystal structural analysis Ice nanotube (IT) melting! Primary hydration layer (eutron exp.)

4

5 Infrared Spectroscopy + Microwave conductivity on-contact cavity perturbation technique c axis. Matsui et al. J. Phys. Soc. Jpn. 79 (2010) ; J. Chem. Phys. to be published.

6 TE 011 mode resonating at 16.3 Gz Transmitted wave Incident wave Coupling hole Resonance curve : Lorentzian Transmission intensity Resonance width : Γ s, Γ 0 Resonance frequency : f s, f 0 S : sample installed in the cavity 0 : empty cavity f Maximum electric field E ac Scheme of a depolarization regime

7 Microwave conductivity (real part) along c axis under R ~ 100 % σ 1 (Ωcm) (E g ~ 0.3 ev) 2 -WT D 2 -WT 246K 240K Vacuum R ~ 100% E K 242K T (K)

8 Microwave conductivity (real part) along c axis under R ~ 100 % Anisotropic conduction is remarkable in WT state. σ 1 (Ωcm) (E g ~ 0.3 ev) 2 -WT D 2 -WT 246K 240K Vacuum R ~ 100% E K 242K T (K) σ 1 T ( (Ωcm) -1 K ) c // c R ~ 80% E g ~ 0.3eV Long-range proton transfer is available along c. Rotational motions of water molecule? /T (K -1 )

9 ~1700cm -1 bending ~2160cm -1 Additional Band 3000~4000cm -1 stretching Spectra of WT above 240K A (arb. unit) K 234K 100K 6K Spectra of IT below 240K dynamically fluctuating - distance in WT is identical to one in IT Wavenumber (cm -1 ) WT possesses regulated structure as well as IT!

10 at 293 K under R ~100 % A (arb. unit) Parallel to c axis Long range proton transfer occurs along c direction (microwave exp.) A = A para -A perp hydrated protons! Parpendicular to c axis Wavenumber (cm -1 ) emergence of hydrated protons transferable along c direction Resonant wavenumber relating to - distance c axis

11 ovak s correlation Additional band ~2200 cm -1 - distance ~ 2.56 Å much shorter than dominant - distance 2.7~ 2.9 Å Fig. 8 in Chem. Mat. 8 (1996) 610, K.D. Kreuer. - distance ~ 1.03 Å distance ~ 1.53 Å

12 R Asymmetric coordinate : δ = R > Experimentally categorized as an Eigen-like motif! The transfer of protons accompanies a local distortion! 2.7~ 2.9 Å ~ 2.56 Å hopping distorted Eigen complex in Cl solution J. Xu, Y. Zhang and G. A. Voth, J. Phys. Chem. Lett. 2, 81 (2011).

13 WT = Quasi one-dimensional high proton conductor dynamically fluctuating in the vicinity of the regulated positions in IT with maintaining the - distance The additional band (~2200 cm -1 ) indicating polarization effect the - distance around protonated site shrinks to ~ 2.56 Å Mobile hydrated proton = Eigen-like motif Proton-lattice coupling plays significant role! reminiscent of Polaron

14 dissociation occurs in the water molecule just contacting to carboxylate oxygen atoms of TMA 3- carrier density : = 2.3 x (cm -3 ) Mobile protons are released in WT Co Co + σ 1 ~ 0.03 (Ωcm) -1 mobility = 2.6 x 10-2 (cm 2 /Vs) ice: 8 x 10-2 (cm 2 /Vs) > water: 3.6 x 10-3 (cm 2 /Vs) < The carrier density is not large, but high mobility yields the high conductivity! eutron Crystal structural analysis

The Initial Process of Photoinduced Phase Transition in an Organic Electron-Lattice Correlated System using 10-fs Pulse

The Initial Process of Photoinduced Phase Transition in an Organic Electron-Lattice Correlated System using 10-fs Pulse The Initial Process of Photoinduced Phase Transition in an Organic Electron-Lattice Correlated System using 1-fs Pulse S. Koshihara, K. Onda, Y. Matsubara, T. Ishikawa, Y. Okimoto, T. Hiramatsu, G. Saito,

More information

TEMPERATURE DEPENDENCE OF CURRENT CARRIER S SPIN RELAXATION IN GRAPHITE

TEMPERATURE DEPENDENCE OF CURRENT CARRIER S SPIN RELAXATION IN GRAPHITE TEMPERATURE DEPENDENCE OF CURRENT CARRIER S SPIN RELAXATION IN GRAPHITE A.M. Ziatdinov and V.V. Kainara Institute of Chemistry, Far Eastern Branch of the Russian Academy of Sciences 159, Prosp. 1-letiya,

More information

2) Atom manipulation. Xe / Ni(110) Model: Experiment:

2) Atom manipulation. Xe / Ni(110) Model: Experiment: 2) Atom manipulation D. Eigler & E. Schweizer, Nature 344, 524 (1990) Xe / Ni(110) Model: Experiment: G.Meyer, et al. Applied Physics A 68, 125 (1999) First the tip is approached close to the adsorbate

More information

Surface Transfer Doping of Diamond by Organic Molecules

Surface Transfer Doping of Diamond by Organic Molecules Surface Transfer Doping of Diamond by Organic Molecules Qi Dongchen Department of Physics National University of Singapore Supervisor: Prof. Andrew T. S. Wee Dr. Gao Xingyu Scope of presentation Overview

More information

CHAPTER 5 FTIR STUDIES

CHAPTER 5 FTIR STUDIES CHAPTER 5 FTIR STUDIES 5.1 Introduction Fourier transform infrared spectroscopy is employed to investigate interactions between the polymers chitosan and PVA, the polymer blend and salt, the salt and plasticizer

More information

Asymmetric transport efficiencies of positive and negative ion defects in amorphous ice

Asymmetric transport efficiencies of positive and negative ion defects in amorphous ice Asymmetric transport efficiencies of positive and negative ion defects in amorphous ice E.-S. Moon, Y. Kim, S. Shin, H. Kang Phys. Rev. Lett. 2012, 108, 226103 Soumabha Bag CY08D021 18-08-12 Introduction:

More information

Chapter 6 ELECTRICAL CONDUCTIVITY ANALYSIS

Chapter 6 ELECTRICAL CONDUCTIVITY ANALYSIS Chapter 6 ELECTRICAL CONDUCTIVITY ANALYSIS CHAPTER-6 6.1 Introduction The suitability and potentiality of a material for device applications can be determined from the frequency and temperature response

More information

PAPER No. : 8 (PHYSICAL SPECTROSCOPY) MODULE No. : 5 (TRANSITION PROBABILITIES AND TRANSITION DIPOLE MOMENT. OVERVIEW OF SELECTION RULES)

PAPER No. : 8 (PHYSICAL SPECTROSCOPY) MODULE No. : 5 (TRANSITION PROBABILITIES AND TRANSITION DIPOLE MOMENT. OVERVIEW OF SELECTION RULES) Subject Chemistry Paper No and Title Module No and Title Module Tag 8 and Physical Spectroscopy 5 and Transition probabilities and transition dipole moment, Overview of selection rules CHE_P8_M5 TABLE

More information

MS482 Materials Characterization ( 재료분석 ) Lecture Note 2: UPS

MS482 Materials Characterization ( 재료분석 ) Lecture Note 2: UPS 2016 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 2: UPS Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1 lecture)

More information

CO 2 molecule. Morse Potential One of the potentials used to simulate chemical bond is a Morse potential of the following form: O C O

CO 2 molecule. Morse Potential One of the potentials used to simulate chemical bond is a Morse potential of the following form: O C O CO 2 molecule The aim of this project is a numerical analysis of adsorption spectra of CO2 molecule simulated by a double Morse potential function. In the project you should achieve following tasks: 1.

More information

Spectroscopy in Inorganic Chemistry. Vibration and Rotation Spectroscopy

Spectroscopy in Inorganic Chemistry. Vibration and Rotation Spectroscopy Spectroscopy in Inorganic Chemistry Symmetry requirement for coupling combination bands and Fermi resonance 2 3 V 3 1505 cm -1 (R, IR) E' stretches v 1 888 cm -1 (R) A 1 ' stretch V 2 718 cm -1 (IR) A

More information

Angle-Resolved Two-Photon Photoemission of Mott Insulator

Angle-Resolved Two-Photon Photoemission of Mott Insulator Angle-Resolved Two-Photon Photoemission of Mott Insulator Takami Tohyama Institute for Materials Research (IMR) Tohoku University, Sendai Collaborators IMR: H. Onodera, K. Tsutsui, S. Maekawa H. Onodera

More information

ORIGINAL PROPERTIES OF WATER

ORIGINAL PROPERTIES OF WATER ORIGINAL PROPERTIES OF WATER IN NANOCHANNELS Pascale Launois Laboratoire de Physique des Solides, CNRS, Université Paris Sud, Université Paris Saclay, Orsay, France pascale.launois@u-psud.fr https://www.equipes.lps.u-psud.fr/launois/

More information

Spectroscopy: The Study of Squiggly Lines. Reflectance spectroscopy: light absorbed at specific wavelengths corresponding to energy level transi8ons

Spectroscopy: The Study of Squiggly Lines. Reflectance spectroscopy: light absorbed at specific wavelengths corresponding to energy level transi8ons Spectroscopy: The Study of Squiggly Lines Reflectance spectroscopy: light absorbed at specific wavelengths corresponding to energy level transi8ons Interaction of Radiant Energy and Matter What causes

More information

Infrared Spectroscopy: Identification of Unknown Substances

Infrared Spectroscopy: Identification of Unknown Substances Infrared Spectroscopy: Identification of Unknown Substances Suppose a white powder is one of the four following molecules. How can they be differentiated? H N N H H H H Na H H H H H A technique that is

More information

Energy Spectroscopy. Ex.: Fe/MgO

Energy Spectroscopy. Ex.: Fe/MgO Energy Spectroscopy Spectroscopy gives access to the electronic properties (and thus chemistry, magnetism,..) of the investigated system with thickness dependence Ex.: Fe/MgO Fe O Mg Control of the oxidation

More information

Review of Optical Properties of Materials

Review of Optical Properties of Materials Review of Optical Properties of Materials Review of optics Absorption in semiconductors: qualitative discussion Derivation of Optical Absorption Coefficient in Direct Semiconductors Photons When dealing

More information

Chemistry 2. Assumed knowledge

Chemistry 2. Assumed knowledge Chemistry 2 Lecture 8 IR Spectroscopy of Polyatomic Molecles Assumed knowledge There are 3N 6 vibrations in a non linear molecule and 3N 5 vibrations in a linear molecule. Only modes that lead to a change

More information

compound Cs 2 Cu 2 Mo 3 O 12

compound Cs 2 Cu 2 Mo 3 O 12 133 Cs-NMR study on aligned powder of competing spin chain compound A Yagi 1, K Matsui 1 T Goto 1, M Hase 2 and T Sasaki 3 1 2 Sophia University, Physics Division, Tokyo, 102-8554, Japan National Institute

More information

Phases of Na x CoO 2

Phases of Na x CoO 2 Phases of Na x CoO 2 by Aakash Pushp (pushp@uiuc.edu) Abstract This paper deals with the various phases of Na x CoO 2 ranging from charge ordered insulator to Curie-Weiss metal to superconductor as the

More information

Defense Technical Information Center Compilation Part Notice

Defense Technical Information Center Compilation Part Notice UNCLASSIFIED Defense Technical Information Center Compilation Part Notice ADP013264 TITLE: I Absorption Spectra of Liquid Crystals Confined in the Channels f Macroporous Silicon DISTIBUTION: Approved for

More information

Surface atoms/molecules of a material act as an interface to its surrounding environment;

Surface atoms/molecules of a material act as an interface to its surrounding environment; 1 Chapter 1 Thesis Overview Surface atoms/molecules of a material act as an interface to its surrounding environment; their properties are often complicated by external adsorbates/species on the surface

More information

Synthesis of a Radical Trap

Synthesis of a Radical Trap Chemistry Catalyzed oxidation with hydrogen peroxide Trapping of a free radical (spin trapping) Technique Acquisition and interpretation of ESR spectra Radical trap molecule that reacts with short-lived

More information

Vibrational Spectroscopy

Vibrational Spectroscopy Vibrational Spectroscopy In this part of the course we will look at the kind of spectroscopy which uses light to excite the motion of atoms. The forces required to move atoms are smaller than those required

More information

Lecture 8. Assumed knowledge

Lecture 8. Assumed knowledge Chemistry 2 Lecture 8 IR Spectroscopy of Polyatomic Molecles Assumed knowledge There are 3N 6 vibrations in a non linear molecule and 3N 5 vibrations in a linear molecule. Only modes that lead to a change

More information

Electrical conductivity in new imidazolium salts of dicarboxylic acids

Electrical conductivity in new imidazolium salts of dicarboxylic acids Materials Science-Poland, Vol. 24, No. 1, 2006 Electrical conductivity in new imidazolium salts of dicarboxylic acids K. POGORZELEC-GLASER 1, J. GARBARCZYK 1*, CZ. PAWLACZYK 2, E. MARKIEWICZ 2 1 Poznan

More information

Optics of complex micro structures

Optics of complex micro structures Optics of complex micro structures dielectric materials λ L disordered partially ordered ordered random multiple scattering liquid crystals quasi crystals (Fibonacci) photonic crystals Assembly of photonic

More information

Supporting Information

Supporting Information Supporting Information Enhanced thermoelectricity in High-temperature β-phase Copper (I) Selenides embedded with Cu 2 Te nanoclusters Sajid Butt, a,b, * Wei Xu, c,f, * Muhammad U. Farooq, d Guang K. Ren,

More information

6.5 mm. ε = 1%, r = 9.4 mm. ε = 3%, r = 3.1 mm

6.5 mm. ε = 1%, r = 9.4 mm. ε = 3%, r = 3.1 mm Supplementary Information Supplementary Figures Gold wires Substrate Compression holder 6.5 mm Supplementary Figure 1 Picture of the compression holder. 6.5 mm ε = 0% ε = 1%, r = 9.4 mm ε = 2%, r = 4.7

More information

Workshop on Nanoscience for Solar Energy Conversion October Charge Transport in Metal Oxides: Multi-scale Studies

Workshop on Nanoscience for Solar Energy Conversion October Charge Transport in Metal Oxides: Multi-scale Studies 1938-6 Workshop on Nanoscience for Solar Energy Conversion 27-29 October 2008 Charge Transport in Metal Oxides: Multi-scale Studies Michel DUPUIS Pacific Northwest National Laboratory P.O. Box 999 Richland

More information

Spectroscopy at nanometer scale

Spectroscopy at nanometer scale Spectroscopy at nanometer scale 1. Physics of the spectroscopies 2. Spectroscopies for the bulk materials 3. Experimental setups for the spectroscopies 4. Physics and Chemistry of nanomaterials Various

More information

SPECTRAL AND THERMODYNAMIC PROPERTIES OF CHOLESTERYL MYRISTATE IN THE REGION OF PHASE TRANSITION

SPECTRAL AND THERMODYNAMIC PROPERTIES OF CHOLESTERYL MYRISTATE IN THE REGION OF PHASE TRANSITION SPECTRAL AND THERMODYNAMIC PROPERTIES OF CHOLESTERYL MYRISTATE IN THE REGION OF PHASE TRANSITION V. DANCHUK 1, A. KRAVCHUK 1, G. PUCHKOVSKA 2, A. YAKUBOV 3 1 National Transport University, 1 Suvorova str.,

More information

The Role of Oxygen during Thermal Reduction of Graphene Oxide Studied by Infrared Absorption Spectroscopy

The Role of Oxygen during Thermal Reduction of Graphene Oxide Studied by Infrared Absorption Spectroscopy SUPPLEMENTARY INFORMATION The Role of Oxygen during Thermal Reduction of Graphene Oxide Studied by Infrared Absorption Spectroscopy Muge Acik, 1 Geunsik Lee, 1 Cecilia Mattevi, ǂ2 Adam Pirkle, 1 Robert

More information

Infrared Spectroscopy An Instrumental Method for Detecting Functional Groups

Infrared Spectroscopy An Instrumental Method for Detecting Functional Groups Infrared Spectroscopy An Instrumental Method for Detecting Functional Groups 1 The Electromagnetic Spectrum Infrared Spectroscopy I. Physics Review Frequency, υ (nu), is the number of wave cycles that

More information

Influence of Dilution with Methanol on Fermi's Resonance inccl 4 Vibrational Spectra

Influence of Dilution with Methanol on Fermi's Resonance inccl 4 Vibrational Spectra International Journal of ChemTech Research CODEN( USA): IJCRGG ISSN : 0974-4290 Vol.6, No.1, pp 521-526, Jan-March 2014 Influence of Dilution with Methanol on Fermi's Resonance inccl 4 Vibrational Spectra

More information

XANES spectra of Bulk Water (Ph. Wernet, A. Nilsson, et al. Science 304, 995 (2004)) Pre-edge peak Post-edge

XANES spectra of Bulk Water (Ph. Wernet, A. Nilsson, et al. Science 304, 995 (2004)) Pre-edge peak Post-edge XANES spectra of Bulk Water (Ph. Wernet, A. Nilsson, et al. Science 304, 995 (2004)) Pre-edge peak Post-edge Transition State Potential Method Consider an electronic transition: Initial state Final state

More information

Supporting Information

Supporting Information Supporting Information Ultrathin Spinel-Structured Nanosheets Rich in Oxygen Deficiencies for Enhanced Electrocatalytic Water Oxidation** Jian Bao, Xiaodong Zhang,* Bo Fan, Jiajia Zhang, Min Zhou, Wenlong

More information

Synthesis, characterization and crystal structure of a new supramolecular system containing triorganotin(iv) and 1,3,5- Benzenetricarboxylic acid

Synthesis, characterization and crystal structure of a new supramolecular system containing triorganotin(iv) and 1,3,5- Benzenetricarboxylic acid Synthesis, characterization and crystal structure of a new supramolecular system containing triorganotin(iv) and 1,3,5- Benzenetricarboxylic acid Azadeh Tadjarodi*, Homayoun Gholipour Research Laboratory

More information

Supporting Information. for. Angew. Chem. Int. Ed. Z Wiley-VCH 2003

Supporting Information. for. Angew. Chem. Int. Ed. Z Wiley-VCH 2003 Supporting Information for Angew. Chem. Int. Ed. Z52074 Wiley-VCH 2003 69451 Weinheim, Germany Kinetic and Thermodynamic Control via Chemical Bond Rearrangement on Si(001) Surface Chiho Hamai, Akihiko

More information

Physics of Semiconductors

Physics of Semiconductors Physics of Semiconductors 9 th 2016.6.13 Shingo Katsumoto Department of Physics and Institute for Solid State Physics University of Tokyo Site for uploading answer sheet Outline today Answer to the question

More information

CHEM 3.2 (AS91388) 3 credits. Demonstrate understanding of spectroscopic data in chemistry

CHEM 3.2 (AS91388) 3 credits. Demonstrate understanding of spectroscopic data in chemistry CHEM 3.2 (AS91388) 3 credits Demonstrate understanding of spectroscopic data in chemistry Spectroscopic data is limited to mass, infrared (IR) and 13 C nuclear magnetic resonance (NMR) spectroscopy. Organic

More information

Q. Shen 1,2) and T. Toyoda 1,2)

Q. Shen 1,2) and T. Toyoda 1,2) Photosensitization of nanostructured TiO 2 electrodes with CdSe quntum dots: effects of microstructure in substrates Q. Shen 1,2) and T. Toyoda 1,2) Department of Applied Physics and Chemistry 1), and

More information

Supplementary Information

Supplementary Information Supplementary Information Supplementary Figure 1. Photographs show the titration experiments by dropwise adding ~5 times number of moles of (a) LiOH and LiOH+H 2 O, (b) H 2 O 2 and H 2 O 2 +LiOH, (c) Li

More information

Functional Group Adsorption on Calcite: I. Oxygen Containing and Nonpolar Organic Molecules

Functional Group Adsorption on Calcite: I. Oxygen Containing and Nonpolar Organic Molecules SUPPORTING INFORMATION Functional Group Adsorption on Calcite: I. Oxygen Containing and Nonpolar Organic Molecules E. Ataman*, M. P. Andersson, M. Ceccato, N. Bovet, S. L. S. Stipp Nano-Science Center,

More information

Absorption and scattering

Absorption and scattering Absorption and scattering When a beam of radiation goes through the atmosphere, it encounters gas molecules, aerosols, cloud droplets, and ice crystals. These objects perturb the radiation field. Part

More information

Mutual transparency of coherent laser beams through a terahertz-field-driven quantum well

Mutual transparency of coherent laser beams through a terahertz-field-driven quantum well A. Maslov and D. Citrin Vol. 19, No. 8/August 2002/J. Opt. Soc. Am. B 1905 Mutual transparency of coherent laser beams through a terahertz-field-driven quantum well Alexey V. Maslov and D. S. Citrin School

More information

Modeling Electron Emission From Diamond-Amplified Cathodes

Modeling Electron Emission From Diamond-Amplified Cathodes Modeling Electron Emission From Diamond-Amplified Cathodes D. A. Dimitrov Tech-X Corporation, Boulder, CO I. Ben-Zvi, T. Rao, J. Smedley, E. Wang, X. Chang Brookhaven National Lab, NY This work is funded

More information

Quantum Phenomena & Nanotechnology (4B5)

Quantum Phenomena & Nanotechnology (4B5) Quantum Phenomena & Nanotechnology (4B5) The 2-dimensional electron gas (2DEG), Resonant Tunneling diodes, Hot electron transistors Lecture 11 In this lecture, we are going to look at 2-dimensional electron

More information

Molecular energy levels and spectroscopy

Molecular energy levels and spectroscopy Molecular energy levels and spectroscopy 1. Translational energy levels The translational energy levels of a molecule are usually taken to be those of a particle in a three-dimensional box: n x E(n x,n

More information

Ion Conducting Behaviour of Nano Dispersed Polymer Gel Electrolytes Containing NH 4 PF 6

Ion Conducting Behaviour of Nano Dispersed Polymer Gel Electrolytes Containing NH 4 PF 6 Portugaliae Electrochimica Acta 26/6 (2008) 493-501 PORTUGALIAE ELECTROCHIMICA ACTA ISSN 1647-1571 Ion Conducting Behaviour of Nano Dispersed Polymer Gel Electrolytes Containing NH 4 PF 6 Jitender P. Sharma

More information

Advanced Photon-In Photon-Out Hard X-ray Spectroscopy

Advanced Photon-In Photon-Out Hard X-ray Spectroscopy FLS 2010, ICFA Beam Dynamics Workshop, SLAC, Menlo Park, CA, March 2, 2010 ħω ħω e - Advanced Photon-In Photon-Out Hard X-ray Spectroscopy Uwe Bergmann Linac Coherent Light Source SLAC National Accelerator

More information

X-ray Absorption Spectroscopy

X-ray Absorption Spectroscopy X-ray Absorption Spectroscopy Matthew Newville Center for Advanced Radiation Sources University of Chicago 12-Sept-2014 SES VI SES VI 12-Sept-2014 SES VI What Is XAFS? X-ray Absorption Fine-Structure (XAFS)

More information

High-Performance Flexible Asymmetric Supercapacitors Based on 3D. Electrodes

High-Performance Flexible Asymmetric Supercapacitors Based on 3D. Electrodes Supporting Information for: High-Performance Flexible Asymmetric Supercapacitors Based on 3D Porous Graphene/MnO 2 Nanorod and Graphene/Ag Hybrid Thin-Film Electrodes Yuanlong Shao, a Hongzhi Wang,* a

More information

Recent results in microwave and rf spectroscopy of two-dimensional electron solids

Recent results in microwave and rf spectroscopy of two-dimensional electron solids J. Phys. IV France 131 (2005) 241 245 C EDP Sciences, Les Ulis DOI: 10.1051/jp4:2005131061 Recent results in microwave and rf spectroscopy of two-dimensional electron solids R.M. Lewis 1,2, Y.P. Chen 1,2,

More information

Homework Assignment #3

Homework Assignment #3 Chemistry 12600 Spring 2016 Homework Assignment #3 1. Determine whether each of the following statements is true or false. If the statement is false, modify and rewrite it so that it is a true statement.

More information

kev e - and H + ECR source Shock wave Molecular ices 3 C 2 H 2 C 6 H 6 2 C 3 H 3 Dust impact Europa

kev e - and H + ECR source Shock wave Molecular ices 3 C 2 H 2 C 6 H 6 2 C 3 H 3 Dust impact Europa B Sivaraman kev e - and H + Shock wave Molecular ices ECR source 3 C 2 H 2 C 6 H 6 Europa Dust impact 2 C 3 H 3 C 6 H 6 Temperature, K 273 K 70 / 80 90 K 50 60 K < 20 K New molecules (ISM) C 60 - C 70

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION Coexistence of superconductivity and antiferromagnetism in (Li 0.8 Fe 0.2 )OHFeSe superconductor X. F. Lu 1,2, N. Z. Wang 1,2, H. Wu 3,7, Y. P. Wu 1,2, D. Zhao 1,2, X. Z. Zeng 1,2, X. G. Luo 1,2,8, T.

More information

Supporting Information

Supporting Information Electronic Supplementary Material (ESI) for Nanoscale. This journal is The Royal Society of Chemistry 2015 Supporting Information Single Layer Lead Iodide: Computational Exploration of Structural, Electronic

More information

Hole-concentration dependence of band structure in (Bi,Pb) 2 (Sr,La) 2 CuO 6+δ determined by the angle-resolved photoemission spectroscopy

Hole-concentration dependence of band structure in (Bi,Pb) 2 (Sr,La) 2 CuO 6+δ determined by the angle-resolved photoemission spectroscopy Journal of Electron Spectroscopy and Related Phenomena 137 140 (2004) 663 668 Hole-concentration dependence of band structure in (Bi,Pb) 2 (Sr,La) 2 CuO 6+δ determined by the angle-resolved photoemission

More information

Atomic Level Analysis of SiC Devices Using Numerical Simulation

Atomic Level Analysis of SiC Devices Using Numerical Simulation Atomic Level Analysis of Devices Using Numerical mulation HIRSE, Takayuki MRI, Daisuke TERA, Yutaka ABSTRAT Research and development of power semiconductor devices with (silicon carbide) has been very

More information

Influence of excitation frequency on Raman modes of In 1-x Ga x N thin films

Influence of excitation frequency on Raman modes of In 1-x Ga x N thin films Influence of excitation frequency on Raman modes of In 1-x Ga x N thin films A. Dixit 1,, J. S. Thakur 2, V. M. Naik 3, R. Naik 2 1 Center of Excellence in Energy & ICT, Indian Institute of Technology

More information

Supplementary information

Supplementary information Supplementary information Electrochemical synthesis of metal and semimetal nanotube-nanowire heterojunctions and their electronic transport properties Dachi Yang, ab Guowen Meng,* a Shuyuan Zhang, c Yufeng

More information

V( x) = V( 0) + dv. V( x) = 1 2

V( x) = V( 0) + dv. V( x) = 1 2 Spectroscopy 1: rotational and vibrational spectra The vibrations of diatomic molecules Molecular vibrations Consider a typical potential energy curve for a diatomic molecule. In regions close to R e (at

More information

Chapter 9. Electromagnetic waves

Chapter 9. Electromagnetic waves Chapter 9. lectromagnetic waves 9.1.1 The (classical or Mechanical) waves equation Given the initial shape of the string, what is the subsequent form, The displacement at point z, at the later time t,

More information

Optical Science of Nano-graphene (graphene oxide and graphene quantum dot) Introduction of optical properties of nano-carbon materials

Optical Science of Nano-graphene (graphene oxide and graphene quantum dot) Introduction of optical properties of nano-carbon materials Optical Science of Nano-graphene (graphene oxide and graphene quantum dot) J Kazunari Matsuda Institute of Advanced Energy, Kyoto University Introduction of optical properties of nano-carbon materials

More information

Verwey transition in magnetite (Fe3O4), unveiled?

Verwey transition in magnetite (Fe3O4), unveiled? Verwey transition in magnetite (Fe3O4), unveiled? J.E. Lorenzo Keywords: Charge, orbital orderings; lattice distortion; spin reorientation; resonant X ray scattering S. Grenier N. Jaouen Y. Joly D. Mannix

More information

Chapter 5. Effects of Photonic Crystal Band Gap on Rotation and Deformation of Hollow Te Rods in Triangular Lattice

Chapter 5. Effects of Photonic Crystal Band Gap on Rotation and Deformation of Hollow Te Rods in Triangular Lattice Chapter 5 Effects of Photonic Crystal Band Gap on Rotation and Deformation of Hollow Te Rods in Triangular Lattice In chapter 3 and 4, we have demonstrated that the deformed rods, rotational rods and perturbation

More information

Bi-Axial Growth Mode of Au-TTF Nanowires. Induced by Tilted Molecular Column Stacking

Bi-Axial Growth Mode of Au-TTF Nanowires. Induced by Tilted Molecular Column Stacking Supporting Information Bi-Axial Growth Mode of Au-TTF Nanowires Induced by Tilted Molecular Column Stacking Yanlong Xing Eugen Speiser * Dheeraj K. Singh Petra S. Dittrich and Norbert Esser Leibniz-Institut

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION DOI: 1.138/NNANO.211.214 Control over topological insulator photocurrents with light polarization J.W. McIver*, D. Hsieh*, H. Steinberg, P. Jarillo-Herrero and N. Gedik SI I. Materials and device fabrication

More information

24 Introduction to Spectrochemical Methods

24 Introduction to Spectrochemical Methods 24 Introduction to Spectrochemical Methods Spectroscopic method: based on measurement of the electromagnetic radiation produced or absorbed by analytes. electromagnetic radiation: include γ-ray, X-ray,

More information

Ultra-fast response of nano-carbons under dynamical strong electric field

Ultra-fast response of nano-carbons under dynamical strong electric field Ultra-fast response of nano-carbons under dynamical strong electric field Yoshiyuki Miyamoto NEC Nano Electronics Res. Labs. Acknowledgements Dr. Nakamura (RIST, Tokyo) Prof. Tománek (Michigan Univ.) Prof.

More information

Solid State Device Fundamentals

Solid State Device Fundamentals Solid State Device Fundamentals ENS 345 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 Office 4N101b 1 Outline - Goals of the course. What is electronic device?

More information

Local Electronic Structures and Chemical Bonds in Zr-Based Metallic Glasses

Local Electronic Structures and Chemical Bonds in Zr-Based Metallic Glasses Materials Transactions, Vol. 45, No. 4 (2004) pp. 1172 to 1176 Special Issue on Bulk Amorphous, Nano-Crystalline and Nano-Quasicrystalline Alloys-V #2004 The Japan Institute of Metals Local Electronic

More information

NANOGRAPHITES AND THEIR COMPOUNDS

NANOGRAPHITES AND THEIR COMPOUNDS NANOGRAPHITES AND THEIR COMPOUNDS Albert M. Ziatdinov Institute of Chemistry, Far Eastern Branch of the Russian Academy of Sciences. Vladivostok, Russia E-mail: albert_ziatdinov@mail.primorye.ru Introduction

More information

Supporting Information for. Dynamics of Architecturally Engineered All- Polymer Nanocomposites

Supporting Information for. Dynamics of Architecturally Engineered All- Polymer Nanocomposites Supporting Information for Dynamics of Architecturally Engineered All- Polymer Nanocomposites Erkan Senses,,,,* Madhusudan Tyagi,, Madeleine Pasco, Antonio Faraone,* NIST Center for Neutron Research, National

More information

Supplementary Figure 1

Supplementary Figure 1 Supplementary Figure 1 XRD patterns and TEM image of the SrNbO 3 film grown on LaAlO 3(001) substrate. The film was deposited under oxygen partial pressure of 5 10-6 Torr. (a) θ-2θ scan, where * indicates

More information

Supplementary Figure 1 Comparison between normalized and unnormalized reflectivity of

Supplementary Figure 1 Comparison between normalized and unnormalized reflectivity of Supplementary Figures Supplementary Figure 1 Comparison between normalized and unnormalized reflectivity of bulk SrTiO 3. The normalized high-energy reflectivity (0.5 35 ev) of SrTiO 3 is compared to the

More information

Interaction between Single-walled Carbon Nanotubes and Water Molecules

Interaction between Single-walled Carbon Nanotubes and Water Molecules Workshop on Molecular Thermal Engineering Univ. of Tokyo 2013. 07. 05 Interaction between Single-walled Carbon Nanotubes and Water Molecules Shohei Chiashi Dept. of Mech. Eng., The Univ. of Tokyo, Japan

More information

Fermi polaron-polaritons in MoSe 2

Fermi polaron-polaritons in MoSe 2 Fermi polaron-polaritons in MoSe 2 Meinrad Sidler, Patrick Back, Ovidiu Cotlet, Ajit Srivastava, Thomas Fink, Martin Kroner, Eugene Demler, Atac Imamoglu Quantum impurity problem Nonperturbative interaction

More information

Some properties of water

Some properties of water Some properties of water Hydrogen bond network Solvation under the microscope 1 Water solutions Oil and water does not mix at equilibrium essentially due to entropy Substances that does not mix with water

More information

The Electromagnetic Properties of Materials

The Electromagnetic Properties of Materials The Electromagnetic Properties of Materials Electrical conduction Metals Semiconductors Insulators (dielectrics) Superconductors Magnetic materials Ferromagnetic materials Others Photonic Materials (optical)

More information

CHEM 301: Homework assignment #12

CHEM 301: Homework assignment #12 CHEM 301: Homework assignment #12 Solutions 1. Let s practice converting between wavelengths, frequencies, and wavenumbers. (10%) Express a wavelength of 442 nm as a frequency and as a wavenumber. What

More information

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations

Lecture 1. OUTLINE Basic Semiconductor Physics. Reading: Chapter 2.1. Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations Lecture 1 OUTLINE Basic Semiconductor Physics Semiconductors Intrinsic (undoped) silicon Doping Carrier concentrations Reading: Chapter 2.1 EE105 Fall 2007 Lecture 1, Slide 1 What is a Semiconductor? Low

More information

CHEM Atomic and Molecular Spectroscopy

CHEM Atomic and Molecular Spectroscopy CHEM 21112 Atomic and Molecular Spectroscopy References: 1. Fundamentals of Molecular Spectroscopy by C.N. Banwell 2. Physical Chemistry by P.W. Atkins Dr. Sujeewa De Silva Sub topics Light and matter

More information

Carrier dynamics of rubrene single-crystals revealed by transient broadband terahertz

Carrier dynamics of rubrene single-crystals revealed by transient broadband terahertz Supplemental Material Carrier dynamics of rubrene single-crystals revealed by transient broadband terahertz spectroscopy H. Yada 1, R. Uchida 1, H. Sekine 1, T. Terashige 1, S. Tao 1, Y. Matsui 1, N. Kida

More information

Vibrational Spectroscopy

Vibrational Spectroscopy Vibrational Spectroscopy Keith Refson STFC Rutherford Appleton Laboratory August 28, 2009 Density Functional Methods for Experimental Spectroscopy 2009: Oxford 1 / 22 Two similar structures Zincblende

More information

Optical Vibration Modes in (Cd, Pb, Zn)S Quantum Dots in the Langmuir Blodgett Matrix

Optical Vibration Modes in (Cd, Pb, Zn)S Quantum Dots in the Langmuir Blodgett Matrix Physics of the Solid State, Vol. 44, No. 0, 2002, pp. 976 980. Translated from Fizika Tverdogo Tela, Vol. 44, No. 0, 2002, pp. 884 887. Original Russian Text Copyright 2002 by Milekhin, Sveshnikova, Repinskiœ,

More information

Role of Salts in Phase Transformation of Clathrate Hydrates under Brine Environments

Role of Salts in Phase Transformation of Clathrate Hydrates under Brine Environments Supporting Information for Role of Salts in Phase Transformation of Clathrate Hydrates under Brine Environments Donghoon Shin, Jong-Won Lee, Yesol Woo, Minjun Cha, Yongjae Lee, Seen Ae Chae, Sun Ha Kim,

More information

Probing Wigner Crystals in the 2DEG using Microwaves

Probing Wigner Crystals in the 2DEG using Microwaves Probing Wigner Crystals in the 2DEG using Microwaves G. Steele CMX Journal Club Talk 9 September 2003 Based on work from the groups of: L. W. Engel (NHMFL), D. C. Tsui (Princeton), and collaborators. CMX

More information

X-ray diffraction and Crystal Structure Solutions from Thin Films

X-ray diffraction and Crystal Structure Solutions from Thin Films X-ray diffraction and Crystal Structure Solutions from Thin Films Ingo Salzmann Humboldt-Universität zu Berlin Institut für Physik Overview Experimental technique X-ray diffraction The principal phenomenon

More information

Simple strategy for enhancing terahertz emission from coherent longitudinal optical phonons using undoped GaAs/n-type GaAs epitaxial layer structures

Simple strategy for enhancing terahertz emission from coherent longitudinal optical phonons using undoped GaAs/n-type GaAs epitaxial layer structures Presented at ISCS21 June 4, 21 Session # FrP3 Simple strategy for enhancing terahertz emission from coherent longitudinal optical phonons using undoped GaAs/n-type GaAs epitaxial layer structures Hideo

More information

7a. Structure Elucidation: IR and 13 C-NMR Spectroscopies (text , , 12.10)

7a. Structure Elucidation: IR and 13 C-NMR Spectroscopies (text , , 12.10) 2009, Department of Chemistry, The University of Western Ontario 7a.1 7a. Structure Elucidation: IR and 13 C-NMR Spectroscopies (text 11.1 11.5, 12.1 12.5, 12.10) A. Electromagnetic Radiation Energy is

More information

Energy Spectroscopy. Excitation by means of a probe

Energy Spectroscopy. Excitation by means of a probe Energy Spectroscopy Excitation by means of a probe Energy spectral analysis of the in coming particles -> XAS or Energy spectral analysis of the out coming particles Different probes are possible: Auger

More information

ELEMENTARY BAND THEORY

ELEMENTARY BAND THEORY ELEMENTARY BAND THEORY PHYSICIST Solid state band Valence band, VB Conduction band, CB Fermi energy, E F Bloch orbital, delocalized n-doping p-doping Band gap, E g Direct band gap Indirect band gap Phonon

More information

Spin transport and relaxation mechanism in disordered organic film

Spin transport and relaxation mechanism in disordered organic film pin transport and relaxation mechanism in disordered organic film Motoi Kimata 1, Daisuke Nozaki 1, Yasuhiro Niimi 1, Hiroyui Tajima 2, YoshiChika Otani 1, 3 1 Institute for olid tate Physics, University

More information

QENS in the Energy Domain: Backscattering and Time-of

QENS in the Energy Domain: Backscattering and Time-of QENS in the Energy Domain: Backscattering and Time-of of-flight Alexei Sokolov Department of Polymer Science, The University of Akron Outline Soft Matter and Neutron Spectroscopy Using elastic scattering

More information

Quantum Condensed Matter Physics Lecture 12

Quantum Condensed Matter Physics Lecture 12 Quantum Condensed Matter Physics Lecture 12 David Ritchie QCMP Lent/Easter 2016 http://www.sp.phy.cam.ac.uk/drp2/home 12.1 QCMP Course Contents 1. Classical models for electrons in solids 2. Sommerfeld

More information

Andrea Morello. Nuclear spin dynamics in quantum regime of a single-molecule. magnet. UBC Physics & Astronomy

Andrea Morello. Nuclear spin dynamics in quantum regime of a single-molecule. magnet. UBC Physics & Astronomy Nuclear spin dynamics in quantum regime of a single-molecule magnet Andrea Morello UBC Physics & Astronomy Kamerlingh Onnes Laboratory Leiden University Nuclear spins in SMMs Intrinsic source of decoherence

More information

Experimental and Quantum Investigation on Ice Surface Structure and Reactivity

Experimental and Quantum Investigation on Ice Surface Structure and Reactivity Experimental and Quantum Investigation on Ice Surface Structure and Reactivity A.Allouche J.P.Aycard F.Borget T.Chiavassa I.Couturier C.Manca F.Marinelli C.Martin S.Raunier P.Roubin Physique des Interactions

More information

Lecture 3: Light absorbance

Lecture 3: Light absorbance Lecture 3: Light absorbance Perturbation Response 1 Light in Chemistry Light Response 0-3 Absorbance spectrum of benzene 2 Absorption Visible Light in Chemistry S 2 S 1 Fluorescence http://www.microscopyu.com

More information