Water molecule first hyperpolarizability

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Discussion Overview

The discussion revolves around the first hyperpolarizability of the water molecule (H2O), specifically whether it has non-vanishing elements in its hyperpolarizability tensor. Participants explore theoretical calculations and properties related to the hyperpolarizability of H2O.

Discussion Character

  • Technical explanation
  • Exploratory
  • Debate/contested

Main Points Raised

  • One participant inquires about the existence of non-vanishing elements in the hyperpolarizability tensor of the isolated H2O molecule.
  • Another participant confirms that the hyperpolarizability tensor has non-vanishing elements and provides detailed calculations from a referenced study, including values for the dipole moment and hyperpolarizabilities.
  • A subsequent post references the same study and notes specific tensor elements (\beta_{zxx}, \beta_{zyy}, and \beta_{zzz}) mentioned in the literature.
  • Another participant proposes a reasoning approach to demonstrate why only these three tensor elements survive, discussing the symmetry properties of the tensor and the implications of polarization and electric field symmetry.

Areas of Agreement / Disagreement

While there is agreement on the existence of certain non-vanishing elements in the hyperpolarizability tensor, the discussion includes differing viewpoints on how to demonstrate which specific elements survive, indicating that multiple approaches and interpretations are present.

Contextual Notes

The discussion references specific calculations and theoretical frameworks, but does not resolve the underlying assumptions or the completeness of the arguments presented regarding the hyperpolarizability tensor.

Konte
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Hello everybody,

My question is about the water molecule. Is the isolated H2O molecule has a non-vanishing element [itex]\beta_{ijk}[/itex] in its first-order hyperpolarizability tensor [itex]\beta[/itex] ?

Thank you everybody.
 
Physics news on Phys.org
Yes.

A complete description of the electric dipole moment (μ), the dipole polarizability (α), the first dipole (β), and the second dipole (γ) hyperpolarizability tensors is reported for the ground state of the water molecule at its equilibrium geometry. Self‐consistent‐field (SCF) and complete fourth‐order many‐body perturbation theory (MP4) values of the independent components are calculated via a finite‐field method from the perturbed energies of the molecule in the presence of a homogeneous electric field. The dependence of the calculated values on the basis set is studied at both the SCF and the MP4 levels. Electron correlation has a strong effect on the hyperpolarizability. Our best SCF values are calculated with a large (13s10p6d2f/9s6p2d)[9s7p6d2f/6s5p2d] basis set comprising 136 contracted Gaussian‐type functions and are 0.7789 e a0 for the dipole moment and 8.531 e2a02 Eh−1, −10.86 e3 a03 Eh−2, and 979 e4 a04 Eh−3 for the mean dipole polarizability and first and second dipole hyperpolarizabilities, respectively. The electron correlation correction to these properties is estimated at −0.055±0.005 e a0, 1.11±0.14 e2 a02 Eh−1, −7.1±1.3 e3 a03 Eh−2, and 749±113 e4 a04 Eh−3. Agreement with experiment is very good for the dipole moment and mean dipole polarizability. As regards the hyperpolarizability, satisfactory agreement with the frequency‐dependent values of Ward and Miller may also be deduced, but further experimental and theoretical work on the dispersion of the hyperpolarizability is needed for an effective rapprochement of theory and experiment.
G. Maroulis, J. Chem. Phys. 94, 1182 (1991); http://dx.doi.org/10.1063/1.460025
 
DrClaude said:
Yes.G. Maroulis, J. Chem. Phys. 94, 1182 (1991); http://dx.doi.org/10.1063/1.460025

Thank you Dr Claude,

Indeed, they mention [itex]\beta_{zxx}[/itex], [itex]\beta_{zyy}[/itex] and [itex]\beta_{zzz}[/itex].

Does someone know how to demonstrate that only theses three tensor elements survive for the water molecule H2O ?

Thank you.
 
Handwaving maybe like this: The tensor is symmetric in the last two indices, so it can be brought to main axis form where only the xx, yy and zz components survive. The polarisation is antisymmetric while the square of the electric field is symmetric under reflections. Hence matrix elements where P is perpendicular to some symmetry plane must vanish. This leaves only zxx, zyy, and zzz.
 

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