High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Raman Study of Amino Acids at High Pressures Alanine and its mutimer crystal Korea University.

Slides:



Advertisements
Similar presentations
Infrared spectroscopy of metal ion-water complexes
Advertisements

Complementary Use of Modern Spectroscopy and Theory in the Study of Rovibrational Levels of BF 3 Robynne Kirkpatrick a, Tony Masiello b, Alfons Weber c,
Raman Spectroscopy A) Introduction IR Raman
1 ( ).
Visible and IR Absorption Spectroscopy Andrew Rouff and Kyle Chau.
Raman Spectroscopy Laser 4880 Å. Raman Spectroscopy.
1 Raman spectra and X-ray diffraction of Boron Triiodide at high pressure SHIMIZU Group ONODA Suzue Ref: A. Anderson and L. Lettress J. Raman Spectrosc.
Helium Nanodroplet Isolation Spectroscopy of NO 2 and van der Waals Complexes Robert Fehnel Kevin Lehmann Department of Chemistry University of Virginia.
Specific heat Blue=olivine, green=MgO, orange=forsterite, black=Al2O3, brown=grossular, purple=pyrope, red=CaO.
Condensed phase vs. Isolated gas phase spectra Solution phase A A A A A A W W W W W WW W W W W W W W W W W W: water A: sample ( nm) ( nm) Isolated.
RAMAN SPECTROSCOPY Scattering mechanisms
Lecture 3 – 4. October 2010 Molecular force field 1.
Raman Spectroscopy Rayleigh Scattering ─ about 1 in 10,000 photons will scatter at an angle from a sample without being absorbed while keeping the same.
Raman Spectroscopy 1923 – Inelastic light scattering is predicted by A. Smekel 1928 – Landsberg and Mandelstam see unexpected frequency shifts in scattering.
Raman Spectroscopy Laser 4880 Å. Raman Spectroscopy.
On a FREE AMINO ACID, what functional groups will accept or donate protons at pH 7, and hence are normally charged in water? side chain groups -OH -CH.
Today: IR Next time: (see our website!) Partition coefficient and partition calculations Separations of mixtures.
Lecture 3 INFRARED SPECTROMETRY
Time out—states and transitions Spectroscopy—transitions between energy states of a molecule excited by absorption or emission of a photon h =  E = E.
Common types of spectroscopy
 PART Requirements for Spectroscopic Techniques for Polymers 1. High resolution 2. High sensitivity (>1%) 3. High selectivity between molecular.
Protein Structure Determination Part 2 -- X-ray Crystallography.
1 University of Petra Faculty of Science & Arts Department of Chemistry Seminar I.R Spectroscopy By Firas Al-ouzeh Supervisor : Nuha I. Swidan Summer 2007.
Investigation of fluid- fluid phase transition of hydrogen under high pressure and high temperature 2014/11/26 Shimizu laboratory SHO Kawaguchi.
RamanRaman. Scattering Tyndall scattering – if small particles are present During Rayleigh scattering (interaction of light with relatively small molecules)
INFRARED-ACTIVE VIBRON BANDS ASSOCIATED WITH RARE GAS SUBSTITUTIONAL IMPURITIES IN SOLID HYDROGEN PAUL L. RASTON and DAVID T. ANDERSON, Department of Chemistry,
Advanced Analytical Chemistry – CHM 6157® Y. CAIFlorida International University Updated on 9/18/2008Chapter 5Raman Spectrometry Chapter 5 Raman Spectrometry.
PROTON TRANSFER IN NEUTRAL PEPTIDES EXAMINED BY CONFORMATIONAL SPECIFIC IR/UV SPECTROSCOPY Sander Jaeqx 67th International Symposium on Molecular Spectroscopy.
States and transitions
A Protein Folding Nucleus in the Gas Phase Jessica Thomas and David Pratt University of Pittsburgh Michel Mons, François Piuzzi, Eric Gloaguen, and Benjamin.
Fukuoka Univ. A. Nishiyama, A. Matsuba, M. Misono Doppler-Free Two-Photon Absorption Spectroscopy of Naphthalene Assisted by an Optical Frequency Comb.
Investigation of the Amide I Band of N-Methylacetamide in Solid Parahydrogen using FTIR Spectroscopy Leif O. Paulson and David T. Anderson Department of.
Chapter 12 Infrared Spectroscopy Jo Blackburn Richland College, Dallas, TX Dallas County Community College District  2006,  Prentice Hall Organic Chemistry,
Chapter 2: IR Spectroscopy Paras Shah
Photosynthesis Research by Means of Optical Spectroscopy: Energy Transfer Charge Transfer Protein Dynamics Biosensors.
The Nb 5 Si 3 sample was prepared by Dr. Ravhi Kumar at the University of Nevada, Las Vegas. A stainless steel gasket with a 130 μm centered circular hole.
Electronic Transitions of Palladium Monoboride and Platinum Monoboride Y.W. Ng, H.F. Pang, Y. S. Wong, Yue Qian, and A. S-C. Cheung Department of Chemistry.
Spectrophotometry.
High Pressure study of Bromine Shimizu Lab M2 Hayashi Yuma.
Phase diagram of solid oxygen at low temperature and high pressure
Bonding & dynamics of CN-Rg and C 2 -Rg complexes Jiande Han, Udo Schnupf, Dana Philen Millard Alexander (U of Md)
NANO 225 Intro to Nano/Microfabrication
Water. Vibration Spectrum of Water Water The Water Molecule The occupied molecular orbitals (as electron probability distributions of the isolated molecule)
Frequency Calculations Lecture CompChem 3 Chemistry 347 Hope College.
POLAR (ACYCLIC) ISOMER OF FORMIC ACID DIMER: RAMAN SPECTROSCOPY STUDY
Structural Determination of Solid SiH 4 at High Pressure Russell J. Hemley (Carnegie Institution of Washington) DMR The hydrogen-rich solids are.
Ch 10 Pages ; Lecture 24 – Introduction to Spectroscopy.
Electron-phonon coupling in alpha-hexathiophene single crystals
A. Nishiyama a, K. Nakashima b, A. Matsuba b, and M. Misono b a The University of Electro-Communications b Fukuoka University High Resolution Spectroscopy.
High Resolution Electronic Spectroscopy of 9-Fluorenemethanol (9FM) in the Gas Phase Diane M. Mitchell, James A.J. Fitzpatrick and David W. Pratt Department.
Raman spectroscopy.
K.-X. AuYong, J.M. King, A.R.W. McKellar, & J.K.G. Watson
PhD Chemistry (Analytical) Area of Research Interest:
States and transitions
IR and Raman spectra of N2H2
Jacob T. Stewart and Bradley M
States and transitions
Time out—states and transitions
E. D. Pillai, J. Velasquez, P.D. Carnegie, M. A. Duncan
Water Structure around Hydrophobic Solutes
SPECTROSCOPIC STUDIES OF GREEN FLUORECENCE PROTEIN (GFP)
Raman Spectroscopy A) Introduction IR Raman
Volume 94, Issue 5, Pages (March 2008)
Instrumental Analysis
Hot Cold Molecules: Collisions at Astrophysical Temperatures
TIME RESOLVED SPECTROSCOPY [T.R.S.]:
Introduction During the last years the use of Fourier Transform Infrared spectroscopy (FTIR) to determine the structure of biological macromolecules.
Infrared Spectroscopy
Raman Spectroscopy A) Introduction IR Raman
Fig. 2 XRD spectra and molecular structures of tetragonal and monoclinic crystal phase KDP samples. XRD spectra and molecular structures of tetragonal.
Presentation transcript:

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Raman Study of Amino Acids at High Pressures Alanine and its mutimer crystal Korea University Div. of Chemistry & Molecular Engineering Seung-Joon Jeon

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon High Pressure Study Pressure Unit : 1 bar = 10 5 pascal(Pa) = atm 1 GPa = 10Kbar  10 4 atm Pressure Effect in Materials - Isolation of effect on interatomic and/or intermolecular interaction - Phase transtion - Insulator-metal transition Experimental techniques - Dynamic method : shock wave - Static method : pressure cell Diamond Anvil Cell(DAC)

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Diamond Anvil Cell(DAC) Sampling part

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Diamond Anvil Cell

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Pressure calibration with ruby fluorescence Doublet : R nm R nm Red Shift almost linearly with pressure up to 30 GPa P(GPa) = 380.8{(x/ ) 5 - 1} x: R 1 shift with nm Band width is sensitive to hydrostatic condition

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Ruby fluoresence shift with pressure Wavelength (A o )

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon L-Alanine - Simplest chiral amino acid - Molecular crystal with inter- and/or intra- hydrogen bonding molecule C 1 symmetry crystal orthorombic at 1 atm and room T space group P unit cell dimension : a= 6.032, b= , c=5.784 A Vibrational mode Internal mode: 33 fundamental molecular vibration modes Phonon mode: 6A + 5B(x) + 5B(y) + 5B(z) A sym -6 optical Raman active & IR inactive B sym -15 optical Raman & IR both active L-alanyl-L-alanine Crystal tetragonal space group, I4 unit cell : a=17.985, c= A molecular packing : 4-fold sym

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Tri-L-Alanine -Two different crystal form parallel-chain sheet arrangement(P) – platelet form Antiparallel-chain pleated sheet arrangement (AP)– needle form -Ala 3 (P) monoclinic, space group P21, unit cell : a=9.862Å, b=10.004Å, c= Å  =101.3°, Z=4

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Experimental Sample : Aldrich (99+%), powdered High pressure : DAC Gasket : thickness 250  m steinless steel 300  m diameter hole Pressure calibration : Ruby fluorescence Raman : Jovin-Yvon U m double monochromator PMT + photon counting Back scattering geometry IR : Bomem MB102 FT-IR with Spectra-Bench beam condenser

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Crystal structure L-alanine L-alanyl-L-alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Molecular structure L-alanine L-alanyl-L-alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Ackowlegement Coworker Prof. Hackjin Kim (Chungnam Univ) Prof. Hogyu Han (Korea Univ) Students - Hang Sun Ahn (Ph. D student) - Yong Ho Jung (MS student) Financial support - KOSEF - KOSEF-SRC(CMR-Korea Univ.)

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Conformation Change(or Phase transition) L-Alanine : GPa L-Alanyl-L-alanine : Gpa Tri-L-Alanine : 2.3-3GPa - No evidence of polymerization reaction - dimer : intermolecular H-bonding  intramolecular H-bonding with rotation of C-C and C-N maybe ruduce more in c-axis than in a-axis - The conformation changes shows hysteresis

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Raman spectrum of L-Alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon IR spectrum of L-alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon The d /dp of modes of L-alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon IR spectrum of L-Alanyl-L-Alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon IR spectrum of L-Alanyl-L-Alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon The d /dp of modes of L-Alanyl-L-alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Pressure induced frequency change of modes of L-Alanyl-L-Alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon The calculated frequency at different conformations L-Alanyl-L-Alanine : Amide III mode

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Ab initio calculation with conformations Basis set : 6-31G L-Alanyl-L-Alanine

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon The optimized dihedral angle of peptide bond

High Pressure Raman Korea Univ. Dept. of Chemistry Seung-Joon Jeon Raman Shift of Ala 3 (P)