Related Experiment Video
Updated: May 11, 2026

From Molecules to Materials: Engineering New Ionic Liquid Crystals Through Halogen Bonding
Published on: March 24, 2018
Dynamics behind the long-lived coherences of I2 in solid Xe
Johan Lindgren1, Eero Hulkko, Tiina Kiviniemi
1Nanoscience Center, Department of Chemistry, P. O. Box 35, FI-40014 University of Jyväskylä, Finland.
Iodine molecules in solid xenon exhibit distinct vibrational coherences on the X-state, differing between double and triple substitution sites. These differences in molecular dynamics provide insights into solvated potentials and interactions.
Area of Science:
- Physical Chemistry
- Spectroscopy
- Condensed Matter Physics
Background:
- The B←X transition of I2 in solid xenon exhibits complex spectral features, including zero-phonon lines and phonon side bands.
- Understanding molecular coherence and dephasing dynamics in solid matrices is crucial for characterizing solute-solvent interactions.
Purpose of the Study:
- To investigate the vibrational coherence and electronic dephasing times of I2 in solid xenon.
- To characterize the solvated B- and X-state potentials of I2 by analyzing resonance Raman spectra.
- To elucidate the role of molecular site occupancy and dynamics in spectral properties.
Main Methods:
- Resonance Raman (RR) spectroscopy was employed to observe vibrational coherences.
- Time-resolved coherent anti-Stokes Raman scattering (TR-CARS) was used to probe vibrational coherences on the X-state.
- Molecular dynamics (MD) simulations were performed to assign spectral features and understand site-specific dynamics.
Main Results:
- Two distinct RR progressions were observed, attributed to I2 molecules in double-substitution (sharp overtones, T2 > 21 ps) and triple-substitution (T2 = 6-0.6 ps) sites.
- Vibrationally unrelaxed fluorescence in RR spectra indicates long-lived |B⟩⟨X| coherence (T2 = 600 fs).
- Electronic dephasing time (T2) of 150 fs was measured upon excitation in the continuum.
- MD simulations accurately reproduced relative dephasing rates and clarified the role of rotation-translation dynamics.
Conclusions:
- The study successfully characterized the solvated B- and X-state potentials of I2 in solid xenon.
- Distinct vibrational coherence dynamics were observed for I2 in different substitutional sites.
- Molecular dynamics simulations provide a powerful tool for interpreting complex spectroscopic data in condensed phases.
More Related Videos
Related Concept Videos
Molecular and Ionic Solids
Molecular Solids
Molecular crystalline solids, such as ice, sucrose (table sugar), and iodine, are solids that are composed of neutral molecules as their constituent units. These molecules are held together by weak intermolecular forces such as London dispersion forces, dipole-dipole interactions, or hydrogen bonds, which...
Trends in Lattice Energy: Ion Size and Charge
Lattice Energies of Ionic Crystals
Crystal Field Theory - Octahedral Complexes
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
X-ray Crystallography
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...
Crystal Field Theory - Tetrahedral and Square Planar Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...

