towards a spectroscopically flexible water dimer potential energy surface ross e. a. kelly, and...
TRANSCRIPT
![Page 1: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/1.jpg)
Towards a Spectroscopically Towards a Spectroscopically Flexible Water Dimer Potential Flexible Water Dimer Potential
Energy SurfaceEnergy Surface
Ross E. A. KellyRoss E. A. Kelly, and Jonathan Tennyson, and Jonathan TennysonDepartment of Physics & AstronomyDepartment of Physics & Astronomy
University College LondonUniversity College London
Gerrit C. Groenenboom and Ad van der Avoird Gerrit C. Groenenboom and Ad van der Avoird Theoretical Chemistry, Institute for Molecules and Theoretical Chemistry, Institute for Molecules and
Materials, Materials, Radboud University, Nijmegen.Radboud University, Nijmegen.
Imperial College, December 2008
![Page 2: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/2.jpg)
OutlineOutline
I. MotivationsI. Motivations II. The Water DimerII. The Water Dimer III. Vibration-Rotation TunnellingIII. Vibration-Rotation Tunnelling IV. Dimer PotentialsIV. Dimer Potentials V. Theoretical MethodV. Theoretical Method VI. VRT StatesVI. VRT States VII. Monomer Band OriginsVII. Monomer Band Origins VIII. Monomer Corrected SurfaceVIII. Monomer Corrected Surface IX. Conclusions & Further WorkIX. Conclusions & Further Work
![Page 3: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/3.jpg)
I. MotivationsI. Motivations to understand to understand water dimer absorption water dimer absorption
throughout visible and IR region in the throughout visible and IR region in the atmosphere.atmosphere.
To create a To create a high accuracy water dimer high accuracy water dimer spectraspectra in agreement with in agreement with experimentsexperiments..
To create a To create a linelistlinelist of all possible of all possible water water dimer transitionsdimer transitions..
![Page 4: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/4.jpg)
• To get all Vibration Rotation Energy Levels To get all Vibration Rotation Energy Levels Calculations require:Calculations require:
1. Some theoretical methodology for solving 1. Some theoretical methodology for solving the Hamiltonianthe Hamiltonian 2. High accuracy Potential Energy Surface2. High accuracy Potential Energy Surface
Preferably fully flexible (12D)Preferably fully flexible (12D)
•4 O-H distances4 O-H distances•2 H-O-H Angles2 H-O-H Angles•O-O distanceO-O distance•5 Euler Angles5 Euler Angles
II. Water DimerII. Water Dimer
![Page 5: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/5.jpg)
Extremely Complex LandscapeExtremely Complex Landscape
X. Huang, B. J. Braams, J. M. Bowman, J. Phys. Chem. A 110, 445 (2006).
II. Water DimerII. Water Dimer
![Page 6: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/6.jpg)
Complicated further by tunnelling effects!Complicated further by tunnelling effects! Tunnelling between eqiulavent states in the PES is Tunnelling between eqiulavent states in the PES is
feasible!feasible! Acceptor Tunnelling:Acceptor Tunnelling:
No bond breaking hereNo bond breaking hereLowest tunnelling barrier Lowest tunnelling barrier
Also, by breaking the Hydrogen bond, other tunnelling Also, by breaking the Hydrogen bond, other tunnelling paths possible: paths possible: Donor-Acceptor interchangeDonor-Acceptor interchangeDonor Bifurcation TunnellingDonor Bifurcation Tunnelling
III. Vibration-Rotation TunnellingIII. Vibration-Rotation Tunnelling
![Page 7: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/7.jpg)
Can be represented by Permutation-Inversion Group GCan be represented by Permutation-Inversion Group G1616..
1 1
1 1
5 5
5 5
2 2
2 2
6 6
6 6
6 6
6 6
5
5 5
5
4
4
4
4
3
3
3
3
3 3
3 3
4
4
4
4
1 1
1 1
2
2 2
2
Isomorphic to D4h
with Irreducible Elements:
A1
+, A2
+, A1
-, A2
-, B1
+, B2
+, B1
-, B2
-, E+, E-
-> Water Dimer Spectroscopic Labels
III. Labelling Water Dimer StatesIII. Labelling Water Dimer States
![Page 8: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/8.jpg)
[1] R. Bukowski, K. Szalewicz, G. C. Groenenboom, A. van der Avoird, Science 315, p1249-1252 (2007).
[2] X. Huang, B. J. Braams, J. M. Bowman, J. Phys. Chem. A 110, 445 (2006).
[3] X. Huang, B. J. Braams, J. M. Bowman, R. E. A. Kelly, J. Tennyson, G. C. Groenenboom, A. van der Avoird, J. Chem. Phys. 128,
034312 (2008)
Benchmark:Benchmark:●6D6D CC-polCC-pol Potential [1] - Potential [1] - Rigid MonomersRigid Monomers
New (2) New (2) 12D PESs12D PESs by Huang, Braams & Bowman by Huang, Braams & Bowman [2,3][2,3]
●HBB0HBB0 [2] [2] ●and and HBBHBB [3] – [3] – NEW 12D PESNEW 12D PES
- All completely - All completely ab initioab initio- Good agreement with experiment- Good agreement with experiment
Many PES’s available!Many PES’s available!
IV. Dimer Potentials AvailableIV. Dimer Potentials Available
![Page 9: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/9.jpg)
• 30 000 configurations. 30 000 configurations.
• Calculated at coupled-cluster, single and double and Calculated at coupled-cluster, single and double and
perturbative treatment of triple excitations method.perturbative treatment of triple excitations method.
• augmented, correlation consistent, polarized triple zeta augmented, correlation consistent, polarized triple zeta
basis set.basis set.
• Polynomial fit with 5227 coefficients.Polynomial fit with 5227 coefficients.
• However, compared to However, compared to CCpolCCpol potential (benchmark): potential (benchmark):● Lower relative grid coverage of the surface than Lower relative grid coverage of the surface than
benchmark 6D PES.benchmark 6D PES.● Not extrapolated to the complete basis set limit Not extrapolated to the complete basis set limit
(CBS)(CBS)● No bond functions in analytical fitNo bond functions in analytical fit● Dissociation less accurately describedDissociation less accurately described
12DIV. IV. HBBHBB PES for H PES for H
44OO22
[1] X. Huang, B. J. Braams, J. M. Bowman, R. E. A. Kelly, J. Tennyson, G. C. Groenenboom, A. van der Avoird, J. Chem. Phys. 128, 034312
(2008).
![Page 10: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/10.jpg)
• Dissociation Energy = 1665.82 cmDissociation Energy = 1665.82 cm-1-1 / 1757.90 cm / 1757.90 cm-1-1
• Other tests? Other tests?
• Compare with Low temperature high-resolution Compare with Low temperature high-resolution
Tetrahertz Spectroscopy (prepared in supersonic Tetrahertz Spectroscopy (prepared in supersonic
molecular beams), around 5 K.molecular beams), around 5 K.
• How can this be done theoretically?How can this be done theoretically?
IV. IV. HBBHBB PES for H PES for H44OO22
![Page 11: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/11.jpg)
Rigid monomer Hamiltonian [1]:
Only for the Intermolecular modes
Used for water dimer previously, detailed account [2]
Coupled product of Symmetric rotor functions (Wigner-D functions) for the Angular coordinates
Radial basis: sinc Discrete Variable Representation (DVR)
[1] G. Brocks, A. van der Avoird, B. T. Sutcliffe, J. Tennyson, Mol. Phys. 50, 1025 (1983).
[2] G. C. Groenenboom, et al., JCP 113, 6702 (2000).
V. Theoretical Method for VRT levelsV. Theoretical Method for VRT levels
![Page 12: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/12.jpg)
VI. Ground State VRT states for HVI. Ground State VRT states for H44OO22
[1] X. Huang, B. J. Braams, J. M. Bowman, R. E. A. Kelly, J. Tennyson, G. C. Groenenboom, A. van der Avoird, J. Chem. Phys. 128, 034312
(2008).
Very good agreement with:
Ground State Tunnelling splittings Rotational Constants
Not so good agreement with:
Acceptor Tunnelling
![Page 13: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/13.jpg)
Excellent agreement with:
Ground State Tunnelling splittings Rotational Constants
Not so good agreement with:
Acceptor Tunnelling
[1] X. Huang, B. J. Braams, J. M. Bowman, R. E. A. Kelly, J. Tennyson, G. C. Groenenboom, A. van der Avoird, J. Chem. Phys. 128, 034312
(2008).
VI. Ground State VRT for DVI. Ground State VRT for D44OO22
![Page 14: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/14.jpg)
In cm-1
Red – ab initio potential Black – experimental
GS – ground state
DT – donor torsion
AW – acceptor wag
AT – acceptor twist
DT2 – donor torsion overtone
VI. More low level VRT States for HVI. More low level VRT States for H44OO22
![Page 15: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/15.jpg)
In cm-1
Red – ab initio potential Black – experimental
GS – ground state
DT – donor torsion
AW – acceptor wag
AT – acceptor twist
DT2 – donor torsion overtone
VI. More low level VRT States for DVI. More low level VRT States for D44OO22
![Page 16: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/16.jpg)
VII. Monomer Band OriginsVII. Monomer Band Origins New 12D Huang New 12D Huang et al.et al. PES seems to work well: PES seems to work well:
– for low-level dimer VRT statesfor low-level dimer VRT states How about for H2O monomer energy levels?How about for H2O monomer energy levels? Use DVR3D [1] for Water monomer levels:Use DVR3D [1] for Water monomer levels:
ExciteExciteFixFix100 bohr
1. J. Tennyson et al., Comp. Phys. Comm. 2004, 163, 85-116.
![Page 17: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/17.jpg)
Comparison is not so good.Comparison is not so good.
VII. Monomer Band OriginsVII. Monomer Band Origins
Blue HBB dimerBlue HBB dimerGreen HBB0Green HBB0Red Shirin 2008.Red Shirin 2008.(Monomer).(Monomer).
![Page 18: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/18.jpg)
VIII. Adding Monomer CorrectionVIII. Adding Monomer Correction
)],,(),,([)](2)()([),( 21212121 eeecorr VVVVVV qqqqqqqqq
Correction for monomer modes:Correction for monomer modes:
New Potential Expression:New Potential Expression:
),(),,(),,(),,( 21212121 qqqqrqqrqq corrcorr VVVV
Tests for PotentialTests for Potential Evaluation of the saddle points.Evaluation of the saddle points. Evaluation of the monomer & dimer VRT states.Evaluation of the monomer & dimer VRT states.
![Page 19: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/19.jpg)
VIII. Monomer Corrected SurfaceVIII. Monomer Corrected SurfaceCharacteristicCharacteristic HBBHBB HBB+MCHBB+MC
DDee -1657.12-1657.12 -1665.82-1665.82
Point 2Point 2 198.47198.47 193.46193.46
Point 3Point 3 243.98243.98 241.09241.09
Point 4Point 4 340.60340.60 358.06358.06
Point 5Point 5 1178.921178.92 1181.761181.76
Point 6Point 6 588.19588.19 590.19590.19
Point 7Point 7 894.83894.83 898.27898.27
Not Particularly worse than HBB potential.
![Page 20: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/20.jpg)
Still a very good Still a very good agreement with agreement with exp.exp.
Nothing is Nothing is changed changed significantly.significantly.
VIII. Ground VIII. Ground State VRT State VRT
levels for Hlevels for H44OO22
![Page 21: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/21.jpg)
VIII. More VIII. More VRT States VRT States for HBB+MCfor HBB+MC
surfacesurface
Again, Again, agreement is agreement is not not significantly significantly worse.worse.
![Page 22: Towards a Spectroscopically Flexible Water Dimer Potential Energy Surface Ross E. A. Kelly, and Jonathan Tennyson Department of Physics & Astronomy University](https://reader036.vdocuments.mx/reader036/viewer/2022062511/5515fac055034694308b4913/html5/thumbnails/22.jpg)
IX. Conclusions & Further WorkIX. Conclusions & Further Work
Introduction of monomer correction makes PES Introduction of monomer correction makes PES more transferable for spectroscopic purposes.more transferable for spectroscopic purposes.
Little effect on dimer characteristics.Little effect on dimer characteristics. Monomer band origins significantly improved.Monomer band origins significantly improved. We are working towards a model which We are working towards a model which
incorporates monomer excitations into the dimer incorporates monomer excitations into the dimer states, so spectra can be produced.states, so spectra can be produced.