Modelling Water Dimer Band Intensities and Spectra Matt Barber Jonathan Tennyson University College London 10 th February 2011

Slides:



Advertisements
Similar presentations
Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University.
Advertisements

Progress Towards Theoretical Spectra of the Water Dimer Ross E. A. Kelly, Matt Barber, & Jonathan Tennyson Department of Physics & Astronomy University.
Simulating the spectrum of the water dimer in the far infrared and visible Ross E. A. Kelly, Matt J. Barber, Jonathan Tennyson Department of Physics and.
Contribution of water dimers in atmospheric absorption: methodology Ross E. A. Kelly, Matt J. Barber, Jonathan Tennyson Department of Physics and Astronomy,
Preliminary Results for Water Dimer Spectroscopy Simulations Ross E. A. Kelly, Matt J. Barber, and Jonathan Tennyson Department of Physics and Astronomy.
1 Formal definition of the water vapour continuum in CKD / MTCKD model The "25 cm-1 plinth" of Lorentzian WM lines is not subtracted from continuum in.
1 Water vapour self-continuum: Recent update from Reading/RAL Semi-annual CAVIAR meeting UCL, London Igor Ptashnik, Keith Shine, Andrey Vigasin.
1 Water vapour self-continuum: Recent interpretation Igor Ptashnik, Keith Shine, Andrey Vigasin University of Reading (UK) Zuev Institute of Atmospheric.
1 Annual CAVIAR meeting, , Imperial College London Water vapour continuum absorption in near- and middle-IR: Recent investigations Department.
Best spectral regions: ARIES & TAFTS Up-Down, at 4 km Downwelling, at 4 km 1) I err = I* ( I Lines *2 ) 0.5 W/(m 2 * cm -1 ) 2) Surface.
1 Analysis of BBCRDS Spectra: Inferred Upper Limits for Water Dimer Absorption A.J.L. Shillings 1, S.M. Ball 2 and R.L. Jones 1 1 University of Cambridge,
BBCRDS Measurements of Water Vapour: Inferred Upper Limits for Water Dimer Absorption in the 610 and 750 nm regions A.J.L. Shillings 1, S.M. Ball 2 and.
Molecular pairs in the atmosphere, the carriers of continuum-like absorption Andrei A. Vigasin General Physics & Atmospheric Physics Institutes, Russian.
1 CAVIAR science meeting 29 th Sept 2010 (National Physical Laboratory) Stephen Ball Leicester University.
Water monomer linelists Matt Barber Jonathan Tennyson Department of Physics and Astronomy University College London December 2009.
Vibrational averaging techniques to calculate the role of water dimers in atmospheric absorption Jonathan Tennyson, Matt J. Barber, Ross E. A. Kelly, Lorenzo.
Theoretical work on the water monomer and dimer Matt Barber Jonathan Tennyson University College London 13 th May 2010
Theoretical work on the water monomer and dimer Matt Barber Jonathan Tennyson University College London December 2008.
Infrared spectroscopy of metal ion-water complexes
Structures and spectroscopic properties calculated for C 6 H 7 + and its complexes with Ne, Ar, N 2, or CO 2 Peter Botschwina and Rainer Oswald Institute.
The role of asymptotic states in H 3 + Jonathan Tennyson Department of Physics and Astronomy Royal Society University College London Jan 2006 HPCx supercomputer:
NABIL F. FARUK, HUI LI, JING YANG, ROBERT J. LE ROY & PIERRE-NICHOLAS ROY Simulation Studies of the Vibrational Dynamics of para- Hydrogen Clusters 1.
Ivan Janeček, Daniel Hrivňák, and René Kalus Department of Physics, University of Ostrava, Ostrava, Czech Republic Supported by the Grant Agency of the.
Analysis of an 18 O and D enhanced lab water spectrum using variational calculations of HD 18 O and D 2 18 O spectra Michael J Down - University College.
Conformational isomerization of bis-(4-hydroxyphenyl)methane in a supersonic jet expansion. Part II: Internal mixing and low barrier potential energy surface.
A L INE L IST FOR H YDROGEN S ULPHIDE (H 2 S) Ala’a A. A. Azzam J. Tennyson and S. Yurchencko Department of Physics and Astronomy, University College London,
SOLVENT EFFECTS ON IR MODES OF (R)-3-METHYLCYCLOPENTANONE CONFORMERS: A COMPUTATIONAL INVESTIGATION Watheq Al-Basheer Physics Department - King Fahd University.
Photoelectron Spectroscopy Lecture 3: vibrational/rotational structure –Vibrational selection rules –Franck-Condon Effect –Information on bonding –Ionization.
Rotational Spectra Simplest Case: Diatomic or Linear Polyatomic molecule Rigid Rotor Model: Two nuclei joined by a weightless rod J = Rotational quantum.
Theoretical work on the water monomer and dimer Matt Barber Jonathan Tennyson University College London September 2009.
Modelling Water Dimer Band Intensities and Spectra Matt Barber Jonathan Tennyson University College London 29 th September 2010
Towards Theoretical Spectroscopy of the Water Dimer Ross E. A. Kelly, Matt J. Barber, and Jonathan Tennyson Department of Physics and Astronomy UCL Gerrit.
Simulating the spectrum of the water dimer in the far infrared and visible Ross E. A. Kelly, Matt J. Barber, Jonathan Tennyson Department of Physics and.
Theoretical work on the water monomer Matt Barber Jonathan Tennyson University College London
High-accuracy ab initio water line intensities Lorenzo Lodi University College London Department of Physics & Astronomy.
IR EMISSION SPECTROSCOPY OF AMMONIA: LINELISTS AND ASSIGNMENTS. R. Hargreaves, P. F. Bernath Department of Chemistry, University of York, UK N. F. Zobov,
Vibrational Spectroscopy
Vibrational and Rotational Spectroscopy
Rovibronic Analysis of the State of the NO 3 Radical Henry Tran, Terrance J. Codd, Dmitry Melnik, Mourad Roudjane, and Terry A. Miller Laser Spectroscopy.
Einstein A coefficients for vibrational-rotational transitions of NO
Calculation of rovibrational H 3 + lines. New level of accuracy Slides of invited talk at Royal Society conference on H 3 + Oleg L. Polyansky 1,2 1 Institute.
Towards perfect water line intensities Lorenzo Lodi University College London, Dept of physics & Astronomy, London, UK.
Modelling Metal Foam Formation in Helium Nanodroplets David McDonagh, The Centre for Interdisciplinary Science Project Supervisor: Professor Andrew Ellis,
1 B. RAM PRASAD, MANGALA SUNDER KRISHNAN Department of Chemistry, Indian Institute of Technology Madras, Chennai , India. AND E. ARUNAN Department.
Meng Huang and Anne B. McCoy Department of Chemistry and Biochemistry The Ohio State Univerisity.
Theoretical Modelling of the Water Dimer: Progress and Current Direction Ross E. A. Kelly, Matt Barber, & Jonathan Tennyson Department of Physics & Astronomy.
Praveenkumar Boopalachandran, 1 Jaan Laane 1 and Norman C. Craig 2 1 Department of Chemistry, Texas A&M University, College Station, Texas Department.
QED of H 3 + Oleg L. Polyansky 1,2 1 Institute of Applied Physics, Russian Academy of Sciences, Uljanov Street 46, Nizhnii Novgorod, Russia Department.
Electronic Spectroscopy of DHPH Revisited: Potential Energy Surfaces along Different Low Frequency Coordinates Leonardo Alvarez-Valtierra and David W.
DIMETHYL -ETHER THREE DIMENTIONAL SPECTRA M. VILLA U.A.M.-I. (México) and M. L. SENENT C.S.I.C. (Spain)
Bonding & dynamics of CN-Rg and C 2 -Rg complexes Jiande Han, Udo Schnupf, Dana Philen Millard Alexander (U of Md)
Rotationally-Resolved Spectroscopy of the Bending Modes of Deuterated Water Dimer JACOB T. STEWART AND BENJAMIN J. MCCALL DEPARTMENT OF CHEMISTRY, UNIVERSITY.
ENERGY LEVELS OF THE NITRATE RADICAL BELOW 2000 CM -1 Christopher S. Simmons, Takatoshi Ichino and John F. Stanton Molecular Spectroscopy Symposium, June.
Ohio State (Current and recent): Laura Dzugan Jason FordSamantha Horvath Meng Huang Zhou LinMelanie Marlett Bernice Opoku-AgyemanAndrew PetitBethany Wellen.
Chuanxi Duan (段传喜) Central China Normal University Wuhan, China
Manfred Birk, Georg Wagner Remote Sensing Technology Institute (IMF) Deutsches Zentrum für Luft- und Raumfahrt (DLR) Lorenzo Lodi, Jonathan Tennyson Department.
Development of a cavity ringdown spectrometer for measuring electronic states of Be clusters JACOB STEWART, MICHAEL SULLIVAN, MICHAEL HEAVEN DEPARTMENT.
Photoelectron Imaging of Vibrational Autodetachment from Nitromethane Anions Chris L. Adams, Holger Schneider, J. Mathias Weber JILA, University of Colorado,
Intermolecular Interactions between Formaldehyde and Dimethyl Ether and between Formaldehyde and Dimethyl Sulfide in the Complex, Investigated by Fourier.
Tao Peng and Robert J. Le Roy
Itaru KURUSU, Reona YAGI, Yasutoshi KASAHARA, Haruki ISHIKAWA Department of Chemistry, School of Science, Kitasato University ULTRAVIOLET AND INFRARED.
Laser spectroscopy of a halocarbocation: CH 2 I + Chong Tao, Calvin Mukarakate, and Scott A. Reid Department of Chemistry, Marquette University 61 st International.
The Rotational Spectrum of the Water–Hydroperoxy Radical (H 2 O–HO 2 ) Complex Kohsuke Suma, Yoshihiro Sumiyoshi, and Yasuki Endo Department of Basic Science,
Microwave Spectroscopic Investigations of the Xe-H 2 O and Xe-(H 2 O) 2 van der Waals Complexes Qing Wen and Wolfgang Jäger Department of Chemistry, University.
A New Potential Energy Surface for N 2 O-He, and PIMC Simulations Probing Infrared Spectra and Superfluidity How precise need the PES and simulations be?
EXPERIMENTAL LINE LISTS OF HOT METHANE Image credit: Mark Garlick MONDAY 22 nd JUNE 2015 ROBERT J. HARGREAVES MICHAEL DULICK PETER F.
~ ~ DETERMINATION OF THE TRANSITION DIPOLE MOMENT OF THE A - X
Jacob T. Stewart and Bradley M
The Atmosphere: Part 2: Radiative equilibrium
Vibrational Predissociation of the Methanol Dimer
Presentation transcript:

Modelling Water Dimer Band Intensities and Spectra Matt Barber Jonathan Tennyson University College London 10 th February 2011

Band Intensities Calculated using the forbidden J=0-0 transition. Water dimer is too complicated for full ro- vibrational modelling. However, we can model vibrations of monomers within dimer and simulate additional rotational structure. Need to use 1992 version of DVR –Band models subsequently superseded –Calculate monomer bands from recent line lists

Dimer band intensities Calculate from (perturbed) monomer vibrational wavefunctions Requires Eckart embedding of axis frame Use HBB 12 D dipole moment surface (DMS) corrected with accurate monomer DMS CVR: L. Lodi et al, J Chem Phys., 128, (2008) Issues: PES used to generate monomer wavefunctions Cut through 12 D DMS used

Perturbing the dimer configuration Many possible configurations Transition intensities vary considerably from small changes in geometry Equilibrium may not be best choice Pick to strengthen donor bound stretch

Estimating transition frequencies Band centre from monomer DVR3D calculation Blue/red shift from calculation on perturbed PES Vibrational fine structure from dimer dimer transitions Rotational structure simulated by overlaid Lorentzian

Partition function and equlibrium constant 800 vibrational energy levels J up to 5 calculated, extrapolated up to 50 Dissociation energy? Equilibrium constant at room temperature: –Around 0.03 to 0.05 for bound states –Possibly up to 0.08 for metastable

Simulate spectra at 296 K Assume equilibrium constant for typical atmospheric conditions Rotational band profile 30 cm -1 HWHM Vibrational fine structure mostly hidden beneath rotational structure But: Vibrational substructure still only for low T (8 J=0 states per symmetry) Possible contribution from metastable dimers

Further Work Preliminary spectra for up to 10,000 cm -1 produced. –Band profile comparisons show some encouraging signs. –Effects of the sampling of the potential being investigated. Need all states up to dissociation for RT spectra –Only 8 states per symmetry here –It is a challenge for a much higher number of states Improved band origins