TEMPERATURE-INDUCED VALENCE AND STRUCTURAL INSTABILITY OF DMTTF-CA Paolo Ranzieri, Alberto Girlando Matteo Masino Università degli studi di Parma INSTM.

Slides:



Advertisements
Similar presentations
Valence instabilities of gold in perovskite structures The relativistic effects in gold stabilizes enormously the 6s level and destabilizes the 5d levels.
Advertisements

APRIL 2010 AARHUS UNIVERSITY Simulation of probed quantum many body systems.
Mechanism of the Verwey transition in magnetite Fe3O4
Zero-Phonon Line: transition without creation or destruction of phonons Phonon Wing: at T = 0 K, creation of one or more phonons 7. Optical Spectroscopy.
Vibrational Spectroscopy of Cold Molecular Ions Ncamiso Khanyile Ken Brown Lab School of Chemistry and Biochemistry June 2014.
Emergent Majorana Fermion in Cavity QED Lattice
Soft bend elastic constant and transition to a modulated nematic phase Alenka Mertelj, 1 Martin Čopič, 1,* Geoffrey R. Luckhurst 2, R. P. Tuffin 3, and.
ISCOM2009 International symposium on crystalline organic metals, superconductors, ferromagnets announcement At Niseko in Hokkaido, Japan On Sep. 12 – 17,
C Cl: CH 3 H.. S N 2 ANIMATION ENERGY PROFILE R. C Cl: CH 3 H :Br:.. S N 2 ANIMATION ENERGY PROFILE R.
Interpretation of the Raman spectra of graphene and carbon nanotubes: the effects of Kohn anomalies and non-adiabatic effects S. Piscanec Cambridge University.
Subir Sachdev arXiv: Subir Sachdev arXiv: Loss of Neel order in insulators and superconductors Ribhu Kaul Max Metlitski Cenke Xu.
Heat conduction by photons through superconducting leads W.Guichard Université Joseph Fourier and Institut Neel, Grenoble, France M. Meschke, and J.P.
Surface Enhanced Infrared Absorption (SEIRA) Spectroscopy
Infrared and Raman study of the charge-density-wave state in the rare-earth polychalcogenides RTe n Leonardo Degiorgi Laboratorium für Festkörperphysik.
Lattice Vibrations – Phonons in Solids Alex Mathew University of Rochester.
Chem 440/540 Advanced Organic Spectroscopy Introduction What spectroscopic techniques would be useful in determining the structure of this compound? H-1.
5. ATOMIC DYNAMICS IN AMORPHOUS SOLIDS Crystalline solids  phonons in the reciprocal lattice.
Spectroscopy of Hybrid Inorganic/Organic Interfaces Vibrational Spectroscopy Dietrich RT Zahn.
IV. Electronic Structure and Chemical Bonding J.K. Burdett, Chemical Bonding in Solids Experimental Aspects (a) Electrical Conductivity – (thermal or optical)
Ionic Compounds What holds them together?.
Lattice Vibrations Part II
Structures and Spin States of Transition-Metal Cation Complexes with Aromatic Ligands Free Electron Laser IRMPD Spectra Robert C. Dunbar Case Western Reserve.
Nanoclusters in model ferroelastics Hg 2 Hal 2 E.M.Roginskii A.F.Ioffe Physical-Technical Institute, Russia.
Aloke Das Indian Institute of Science Education and Research, Pune Mimicking trimeric interactions in the aromatic side chains of the proteins: A gas phase.
Conformational Analysis of R-(+)-3-Methylcyclopentanone by IR Spectroscopy in Para-Hydrogen Crystal Watheq Al-Basheer 1,2, Shin Y. Toh 2, Jun Miyazaki.
In-situ Photolysis of Methyl Iodide in Solid Para-hydrogen and Solid Ortho-deuterium Yuki Miyamoto 1, Mizuho Fushitani 2, Hiromichi Hoshina 3, and Takamasa.
Charge transport in DNA molecules: Structural and dynamical disorder 张伟 北京应用物理与计算研究所 2007 年 10 月.
Ultrafast Carrier Dynamics in Graphene M. Breusing, N. Severin, S. Eilers, J. Rabe and T. Elsässer Conclusion information about carrier distribution with10fs.
University of Wisconsin-Madison Department of Materials Science and Engineering Opportunities for Coherent Scattering in Ferroelectrics and Multiferroics.
Phonons & electron-phonon coupling Claudia Ambrosch-Draxl Department für Materialphysik, Montanunversität Leoben, Austria Institut für Physik, Universität.
Manifestation of Nonadiabatic Effects in the IR Spectrum of para-Benzoquinone Radical Cation Krzysztof Piech, Thomas Bally Department of Chemistry, University.
441 Chem Introduction to Spectroscopy CH-1 1. Introduction to Spectroscopy Set of methods where interaction of electromagnetic radiation with chemical.
Jeroen van den Brink Bond- versus site-centred ordering and possible ferroelectricity in manganites Leiden 12/08/2005.
- 1 - 有機導電体における分子自由度 ・分子性導体の歴史 ・ (EDO-TTF) 2 PF 6 の多重不安定性 超高速・高効率光誘起相転移・分子の化学修飾と錯体の物性変化 低温物質科学研究センター 矢持 秀起.
SPECTROSCOPY OF AND PHOTOINDUCED ELECTRON TRANSFER IN THE COMPLEXES OF C 2 H 4 WITH I AND I 2 Lisa George, Aimable Kalume, and Scott A. Reid Department.
From molecules to materials: the crucial role of supramolecular interactions Anna Painelli Francesca Terenziani INSTM-Parma Parma University.
Materials 286K Class 09. VO 2, V 2 O 3 Morin reported on TiO, VO, Ti 2 O 3, V 2 O 3, and VO 2 Morin, Phys. Rev. Lett. 3 (1959) 34–36.
Resonant SFG Line Shapes on Single Crystal Surfaces Scott K. Shaw, A. Laguchev, D. Dlott, A. Gewirth Department of Chemistry University of Illinois at.
NANO 225 Intro to Nano/Microfabrication
J. Phys. Chem. Lett., 2010, 1, Introduction Electron transfer (ET) processes and charge transfer (CT) states are involved in photosynthesis utilized.
Summary of Collaborative Investigation – Na 5 ACu 4 (AsO 4 ) 4 Cl 2 (A = Rb, Cs) Jeffrey Clayhold, Miami University, USA Shiou-Jyh Hwu, Clemson University,
Title: Multiferroics 台灣大學物理系 胡崇德 (C. D. Hu) Abstract
Electronic Raman Spectroscopy in a Nut Shell (I) Yu He SC Meeting Oct 10, 2013 Raman and History Experimental Setup Geometry in Raman Position Raman among.
Using gate-modulated Raman scattering and electron-phonon interactions to probe single layer graphene: A new technique to assign phonon combination modes.
Introduction to Molecular Magnets Jason T. Haraldsen Advanced Solid State II 4/17/2007.
P. D. CARNEGIE, B. BANDYOPADHYAY AND M. A. DUNCAN
Infrared Spectra of Chloride- Fluorobenzene Complexes in the Gas Phase: Electrostatics versus Hydrogen Bonding Holger Schneider OSU International Symposium.
Helical Spin Order in SrFeO 3 and BaFeO 3 Zhi Li Yukawa Institute for Theoretical Physics (YITP) Collaborator: Robert Laskowski (Vienna Univ.) Toshiaki.
From quasi-2D metal with ferromagnetic bilayers to Mott insulator with G-type antiferromagnetic order in Ca 3 (Ru 1−x Ti x ) 2 O 7 Zhiqiang Mao, Tulane.
Transverse optical mode for diatomic chain
Electronic Properties of Glassy Metals MSE 410 Rochan Mehta.
Cavity-Enhanced Direct Frequency Comb Velocity Modulation Spectroscopy Laura Sinclair William Ames, Tyler Coffey, Kevin Cossel Jun Ye and Eric Cornell.
Development of a cavity ringdown spectrometer for measuring electronic states of Be clusters JACOB STEWART, MICHAEL SULLIVAN, MICHAEL HEAVEN DEPARTMENT.
Tunable Electron-Phonon Coupling in Carbon Nanotubes Moonsub Shim, University of Illinois, DMR EFEF K. Nguyen, A. Gaur, & M. Shim, Phys. Rev. Lett.
Low-temperature properties of the t 2g 1 Mott insulators of the t 2g 1 Mott insulators Interatomic exchange-coupling constants by 2nd-order perturbation.
Institute of Chemical Sciences, School of Engineering and Physical Sciences, Heriot-Watt University Dipole Aligned Solids A Metastable Phase of Molecular.
Infrared Spectra of Anionic Coinage Metal-Water Complexes J. Mathias Weber JILA and Department of Chemistry and Biochemistry University of Colorado at.
Antiferromagnetic Resonances and Lattice & Electronic Anisotropy Effects in Detwinned La 2-x Sr x CuO 4 Crystals Crystals: Yoichi Ando & Seiki Komyia Adrian.
Study of Compositional Intermixing in GaAs/AlAs Superlattices using Raman Spectroscopy MASc. Project Philip Scrutton.
Vibrationally Driven Hydrogen Abstraction Reaction of Bromine Radical in Solution Jae Yoon Shin, Michael A. Shalowski, F. Fleming Crim OSU International.
modes Atomic Vibrations in Crystals = Phonons Hooke’s law: Vibration frequency   f = force constant, M = mass Test for phonon effects by using isotopes.
Lecture 8: Volume Interactions Thursday, 28 January 2010 Ch 1.8 Major spectral features of minerals (p. xiii-xv), from Infrared.
Photoinduced nano and micron structures K. Nasu Solid state theory division, Institute of materials structure science, High energy accelerator research.
Eeee.
Ionic and Metallic Bonding
On the collapses and revivals in the Rabi Hamiltonian
O 96 pm 104.5o H H Fig. 1. A Model for the Water Molecule.
Phonons in Crystal Structures
6.4 Covalent Bonding.
Instrumental Analysis
Presentation transcript:

TEMPERATURE-INDUCED VALENCE AND STRUCTURAL INSTABILITY OF DMTTF-CA Paolo Ranzieri, Alberto Girlando Matteo Masino Università degli studi di Parma INSTM Parma University

Charge-Transfer (CT) crystals eeee D-----A 0<  <1

Neutral-Ionic Transition eeee eeee eeee D  D  D ..... D  A  D  A  D  A ..... COLLECTIVE CHARGE-TRANSFER D  D  D  D .... A  D  A  D  A  D  A  D  Stack dimerization and ferroelectricity

TTF-CA derivatives AcceptorDonor X=Cl, Br DMTTF-CA crystal

Vibrational Spectroscopy Ionicity variation

Infrared activation of the totally-symmetric molecular vibrations Spectroscopic effects of the stack distorsion

65 K X-ray data E. Collet at al. Phys. Rev. B 63, (2001) Dimerization and cell doubling

DMTTF - CA Temperature-induced transition

Pretransitional phenomena  IR =  Raman ±  lattice  lattice =  Peierls M.Masino, A. Girlando, Z. G. Soos Chem. Phys. Lett. 369, 428 (2003)

Low-temperature phase Raman-active lattice modes

Many coupled modes contribute to the effective Peierls mode

Competition between the energy required for the formation of D + A - pair and the Madelung energy Conclusions Overlap between D-A modulated by Peierls phonons DMTTF-CA: transition driven by electron-phonon coupling followed by an electronic rearrangement Complex interaction among electronic, spin and vibrational degrees of freedom TTF-CA : transition driven by electronic interactions