Decay and cooling of biomolecules in an electrostatic storage ring S. Tomita Department of Physics and Astronomy University of Aarhus DK-8000 Aarhus C,

Slides:



Advertisements
Similar presentations
Department für Physik Michael Sewtz Quantum Heavies From Hot Fusion to Ultracold Ions M. Block 1, M. Drewsen 2, S. Fritzsche 1, D. Habs 3, Y.T. Oganessian.
Advertisements

Evolving Role of Mass Spectrometry in Bioanalytical Analysis Daniel Pentek February 1, UCONN Bioanalytical Chem 395.
FC-MS from Teledyne Isco CombiFlash ® a Name You Can Rely On.
Characterization of Structural Motifs for CO 2 Accommodation in Two Model Ionic Liquid Systems Using Cryogenic Ion Vibrational Predissociation Spectroscopy.
outline introduction experimental setup & status
Vibrational Spectroscopy of Cold Molecular Ions Ncamiso Khanyile Ken Brown Lab School of Chemistry and Biochemistry June 2014.
Water Solvation of Copper Hydroxide Brett Marsh-UW Madison.
O BSERVATION OF ULTRAFAST CHARGE MIGRATION IN AN AMINO ACID SDG, Durham, January 2013 L OUISE B ELSHAW Observation of Ultrafast.
Groups: WA 2,4,5,7. History  The electron microscope was first invented by a team of German engineers headed by Max Knoll and physicist Ernst Ruska in.
X-rays & LASERs Section 31-7 Physics 1161: Lecture 24.
Dehydrogenation of nucleobases upon electron attachment to isolated nucleotides Steen Brøndsted Nielsen Department of Physics and Astronomy University.
AA and Atomic Fluorescence Spectroscopy Chapter 9
Electromagnetic Radiation Electromagnetic radiation - all E-M waves travel at c = 3 x 10 8 m/s. (Slower in water, glass, etc) Speed of light is independent.
Spectrophotometers Nucleic Acids and Proteins. Nucleic Acids and Spectrophotometer The rings of the bases (A, C, G, T, U) are made up of alternating single.
Intense Field Femtosecond Laser Interactions AMP TalkJune 2004 Ultrafast Laser Interactions with atoms, molecules, and ions Jarlath McKenna Supervisor:
Lecture 14 LC-MS Ionization. GC Computer MS GC-MS.
Luminescence (Miklós Nyitrai; 27 th of February, 2007)
Phys 102 – Lecture 25 The quantum mechanical model of light.
Motivation for using Radiation Chemistry to Study Free Radicals.
Thermo & Stat Mech - Spring 2006 Class 21 1 Thermodynamics and Statistical Mechanics Blackbody Radiation.
Basic Chemistry for Biology Water and Solutions. Water’s Life Supporting Properties Important to all living things 1.Moderation of temperature 2.Lower.
Common types of spectroscopy
Fluorescence Spectroscopy Part I. Background. Perrin-Jablonski diagram.
Fluorescence Spectroscopy 1Dr. Nikhat Siddiqi. Principles Interaction of photons with molecules results in promotion of valence electrons from ground.
Fluorescence and Absorption Spectroscopy of Bio-molecules
Magnetic Pulsed Valve 1.The valve opens and shuts Rotating Disk He Pulsed Valve Lens to focus the laser beam.
IPC Friedrich-Schiller-Universität Jena 1 6. Fluorescence Spectroscopy.
New LEIF I3 Transnational access to ELISA
Determination of fundamental constants using laser cooled molecular ions.
Bios 532 Fluorescence. Vocabulary Fluorophore - molecule that emits fluorescence. Excitation - absorption of a photon. Emission - release of a photon.
Instrumentation in the Molecular Physics Group Presented by: Mats Larsson.
A3: DESIREE Design and examples of planned experiments Belfast, July 1, 2003 Henning Schmidt, Stockholm University ( D ouble E lectro S tatic I on R ing.
DESIREE D ouble E lectro- S tatic I on R ing E xp- E riment Albanova Instrumentation Seminar Henning Schmidt.
Chemistry of Life Chapter 3 Pg Section 1: Matter and Substances Key Ideas:  What makes up matter?  Why do atoms form bonds?  What are some.
’High quality sources for complex ions’ 4 th Annual LEIF Meeting Belfast, July 1, 2003 Coordinator: Henrik Cederquist, Physics Department, Stockholm University.
A. Doyuran, L. DiMauro, W. Graves, R. Heese, E. D. Johnson, S. Krinsky, H. Loos, J.B. Murphy, G. Rakowsky, J. Rose, T. Shaftan, B. Sheehy, Y. Shen, J.
Chapter 15 Molecular Luminescence Spectrometry Three types of Luminescence methods are: (i) molecular fluorescence (ii) phosphorescence (iii) chemiluminescence.
1. Principles  Interaction of photons with molecules results in promotion of valence electrons from ground state orbitals to high energy levels.  The.
Christopher Leavitt Yale University Vibrational spectra of cryogenic peptide ions using H 2 predissociation spectroscopy.
Direct Measurement of Weak Collisions and Collision Rates using High-Resolution Transient IR Absorption Spectroscopy Daniel K. Havey, Qingnan Liu, Amy.
Spectroscopy of Multiply Charged Metal Ions: IR Study of Mn 2+ (18-crown-6 ether)(MeOH) 1-3 Jason D. Rodriguez and James M. Lisy Department of Chemistry,
Robert C. Dunbar Case Western Reserve University Jeffrey D. Steill FOM Institute for Plasma Physics Jos Oomens FOM Institute for Plasma Physics and University.
ANALYTICAL CHEMISTRY CHEM 3811 CHAPTER 23 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state university.
UV Photodissociation of cyclic ketones in the gas phase and cold inert gas matrixes Anamika Mukhopadhyay, Moitrayee Mukherjee, Amit K. Samanta and Tapas.
Chap 6. Practical Methods for Kinetics and Equilibria
Ultrafast Spectroscopic and ab initio Computational Investigations on Solvation Dynamics of Neutral and Deprotonated Tyrosine 70 th ISMS TI03 Champaign,
L. Maunoury 4 rd Annual LEIF Meeting June 27th - July 2rd 2003, Belfast, Ireland Status of the ARIBE project L. Maunoury, B. Huber, T.Been, P. Guinement,
Chemistry of Life Section 1 Section 4
Relaxation methods A chemical equilibrium is thrown off-balance, and we measure the rate of reaching the new equilibrium. E.g.: temperature jump,
Fluorescence spectroscopy, Einstein’s coefficients Consider a molecule with two energy levels S a and S b The rate of transition.
Cavity Ringdown Spectroscopy of Molecular Ions in a Fast Ion Beam Susanna L. Widicus Weaver, Andrew A. Mills, and Benjamin J. McCall Departments of Chemistry.
From the Bottom Up: Hydrogen Bonding in Ionic Liquids 6/19/2014 Olga Gorlova, Conrad Wolke, Joseph Fournier, Christopher Johnson and Mark Johnson.
Introduction to Physics and Astronomy (1) 2-1. Light and Black Body Radiation.
Yonsei Proteome Research Center Peptide Mass Finger-Printing Part II. MALDI-TOF 2013 생화학 실험 (1) 6 주차 자료 임종선 조교 내선 6625.
The Double ElectroStatic Ion-Ring ExpEriment, DESIREE The other end of the scale from ESS!
SCRIBES Sensitive Cooled Resolved Ion BEam Spectroscopy
Dissociation of Molecular Ions Studied by
Same chromophore – different absorption maximum
C70 and C60 colliding with slow highly charged ions – a comparison
Summary of activities of the pellet target development
Fluorescence Spectroscopy
Electronic Spectrum of Cryogenic Ruthenium-Tris-Bipyridine Dications
Lecture 14 LC-MS Ionization.
Fluorescence Lifetimes
Biophysical Approaches
Chemistry Vocab Quiz.
Volume 89, Issue 4, Pages (October 2005)
Lecture 14 LC-MS Ionization.
5.2 Properties of Light Our goals for learning What is light?
Mass Spectrometry THE MAIN USE OF MS IN ORG CHEM IS:
Presentation transcript:

Decay and cooling of biomolecules in an electrostatic storage ring S. Tomita Department of Physics and Astronomy University of Aarhus DK-8000 Aarhus C, Denmark June 27 -July 2, rth annual LEIF meeting - Belfast, N. Ireland4rth annual LEIF meeting

Ubiquitin 76 amino acid protein 8.6 k amu 40 Å Helical structure:  helix Sheet structure:  sheets

Common amino acids

Photo absorption in solution Photo absorption Tryptophan Tyrosine Phenylalanine Absorption Wavelength Tryptophan280 nm Tyrosine274 nm Phenylalanine257 nm

Molecules investigated Lys-Trp-LysTrp

Electrospray J.B. Fenn (1988) Nobel Prize in Chemistry (2002) ~3kV ~1cm ~10  M/L ~1  L/min

Electrospray Source 1 mbar mbar10 -5 mbar10 -6 mbar Rotary pump Turbo pump Turbo pump Heated capillary ESI needle 4kV Fused silica capillary 22 pole Ion trap Tube lens Skimmer Octapole Lenses Acceleration tube

ELISA 1 m Detector for neutrals Laser Accelerator with electrospray ion source Magnet Laser power meter Injection Channeltron t Counts Pulsed Alexandrite Laser nm (3 rd harmonic) Pulsed NdYAG Laser 266nm (4 th harmonic)

Photo absorption in solution Heating by photo absorption h TrTr

1/t decay law Distribution at time t Yield of decay Maximum at E m (t) 1/k = t at E m (t)

[Lys-Trp-Lys+H] + 266nm Injection Laser

[Lys-Trp-Lys+H] + 243nm  E = 5.10 eV  = 0.48ms 260nm  E = 4.77 eV  = 0.86ms Lower photon energy Longer life time Higher photon energy Shorter life time

Arrhenius plot We can determine pre-exponential factor and dissociation energy. 243nm 260nm

Dependence on temperature of ion trap HOT COLD Temperature of ion trap

[Trp+H] nm InjectionLaser 1/t

Fluorescence

Quantum yield Solvent Amino AcidPolypeptide EmissionQuantumEmissionQuantum PhenylalanineDMSO TyrosineDMSO TyrosineH20H TryptophanDMSO TryptophanH20H Quantum yield is very sensitive to the environment. (Amino Acid) > (Polypeptide) DMSO > H 2 0

Summary Lys-Trp-Lys Narrow internal energy distribution Exponential decay after photo absorption Statistical decay through ergonic process Determination of dissociation energy Trp 1/t Decay Due to high fluorescence quantum yield?

Collaborators Stockholm H. Cederquist H.T. Schmidt J. Jensen H. Zettergren CAEN B.A. Huber B. Manil L. Maunoury Canada J.S. Forstar Group at Univ. of Aarhus P. Hvelplund J.U. Andersen S.B. Nielsen J. Rangama B. Liu