David Shelton

Email: shelton@physics.unlv.edu
Phone: (702) 895-3564
Fax: (702) 895-0804

Nonlinear Optics


The subject of nonlinear optics is concerned with the effects arising from the nonlinear response of a medium to electric fields, at least one of which is in the optical frequency range. Lasers are needed to produce the intense optical fields needed to reveal the nonlinear properties of most atoms and molecules. The applications of nonlinear optics can be broadly classified as frequency conversion and signal processing. In this laboratory we investigate gas, liquid and solid nonlinear optical materials. Gases are studied because they are the easiest to understand, and liquids and solids are studied because they are closer to practical applications.

CURRENT RESEARCH

Are dipolar liquids ferroelectric?

The electrostatic dipole interaction between polar molecules in liquids such as water is strong enough to drive long-range orientation ordering of the molecules. The first evidence for the existence such orientation order comes from recent hyper-Rayleigh scattering (HRS) experiments. The HRS spectrum for dipolar liquids contains an extremely sharp peak, with the polarization signature of a longitudinal polar collective mode, which disappears when the mean dipole coupling strength is reduced below a threshold value. This peak is interpreted as HRS from long-lived domains with ferroelectric order. These domains are of nanometer size and persist for 100 ns or longer. The observations are consistent with theoretical models predicting predominantly toroidal order for the dipoles, where each domain is a planar vortex with the dipoles in the vortex core pointing along the axis.





EXPERIMENTS

1. Hyper-Rayleigh Light Scattering in Liquids and Gases.

This is a second harmonic generation experiment in which the light is scattered in all directions rather that as a narrow coherent beam. The technique can be easily applied to study a very wide range of materials because electrostatic fields and phase matching are not required. Other advantages are that polarization analysis gives information about the tensor properties, and spectral analysis of the scattered light gives information about the dynamics. The main disadvantage is that the signal tends to be much weaker than in coherent harmonic generation experiments.

In this experiment the infrared light beam from a pulsed Nd:YAG laser is sharply focused inside the sample cell, and the green light scattered from the focal spot is collected by a camera lens and passed through a spectrometer. In a typical experiment the focal intensity is 1 GW/cm2, and the detected signal is 100 photons/second. The molecules studied range from water to large organic dyes.

2. Photochromic Signal Processing with Bacteriorhodopsin Films.

Bacteriorhodopsin is a protein which undergoes a reversible color change when it absorbs a photon. Bacteriorhodopsin and its various mutants have been investigated for photonics applications including signal processing, 3-D data storage, holographic storage, and spatial light modulators. The work in this laboratory is aimed at producing an optically configurable spatial light modulator suitable for optoelectronic neural network applications. Large scale neural networks require the massive parallelism that optics can provide.

Bacteriorhodopsin has several features which make it an attractive starting point for designing a "smart" material, a material in which significant information processing capability is built into the molecular structure. The protein part ensures switching between states of the chromophore with high quantum efficiency and without side reactions, and genetic engineering allows one to introduce controllable changes at the molecular scale. Presently, we are investigating the effects of environmental parameters (temperature, electric field) on the transitions between molecular states.

3. Electric Field Induced Second Harmonic Generation in Gases.

The simplest example of frequency conversion is Second Harmonic Generation, where a laser beam propagating through a nonlinear optical medium generates a beam of light at twice the original optical frequency (for example, an invisible infrared laser beam is converted into a beam of green light). In such "parametric" processes, the nonlinear optical medium responds on a time scale as short as femtoseconds, but large effects often require light intensities greater than 1 MW/cm2.

In the present experiments, the quadratic and cubic nonlinearities of isolated molecules are determined from measurements of the intensity of the frequency-doubled light beam, produced when a strong electric field is applied to a gas sample through which a laser beam passes. This experiment gives very accurate measurements of the nonlinear optical properties of small molecules. These measurements are important because they are a direct test of theoretical calculations for the same molecules.

This unique research facility uses periodic phase matching in a periodic electrode array to permit accurate gas phase hyperpolarizability measurements for a wide range of molecules, using cw and pulsed lasers, with wavelengths over the near-infrared and visible. The experiment currently uses a Nd:YAG laser which emits infrared light pulses with a power of 10 kW. The strength of the second harmonic signal generated in the sample is increased up to 10,000 times by using an electrode array in which the field periodically changes sign. The sample cell and sample handling apparatus is constructed to operate at temperatures up to 200 C. This allows gas phase measurements of molecules such as para-nitroaniline, which are closely related to chromophores of immediate practical interest.

4. Electric Field Induced Birefringence (Kerr Effect) in Gases.

The cubic nonlinearity of isolated molecules is determined from measurements of the depolarization of a laser beam as it propagates through a sample to which a transverse electric field has been applied. When the results of this experiment are combined with the results of the electric-field-induced second harmonic generation experiment, they allow one to clearly distinguish the nuclear and electronic contributions to the nonlinear optical response of a molecule (effects of the motion of the atomic nuclei as compared to effects of the motion of the electrons around the nuclei). The experiment uses argon-ion, dye, and He-Ne lasers producing continuous low power light beams in the near infrared and visible. The apparatus measures birefringent phase shift with nanoradian sensitivity.

5. Laser Cooling and Trapping of Atoms.

A wide range of coherent and nonlinear interactions occur when laser light is resonant with strong optical transitions in atoms. Laser sources and spectroscopic techniques for cooling and trapping rubidium atoms in a magneto-optic trap are being developed for the production and study of cold atoms. Much of the development work in this project has been done by undergraduate students in the Research Experience for Undergraduates program supported by the National Science Foundation.







SELECTED RECENT PUBLICATIONS

  • D. P. Shelton, Ferroelectric domains measured in nitrobenzene-nitromethane solutions by hyper-Rayleigh scattering, J. Chem. Phys. 124, 124509 (2006).
  • D. P. Shelton, Hyper-Rayleigh scattering spectrum of liquid nitromethane, J. Chem. Phys. 123, 111103 (2005).
  • D. P. Shelton, Are dipolar liquids ferroelectric? J. Chem. Phys. 123, 084502 (2005).
  • D. P. Shelton, Slow polarization relaxation in water observed by hyper-Rayleigh scattering, Phys. Rev. B 72, 020201 (2005).
  • D. P. Shelton, Collective molecular rotation in D2O, J. Chem. Phys. 117, 9374-9382 (2002).
  • R. D. Pyatt and D. P. Shelton, Hyper-Rayleigh scattering from CH4, CD4, CF4, and CCl4, J. Chem. Phys. 114, 9938-9946 (2001).
  • D.P. Shelton and P. Kaatz, Librons observed in liquid acetonitrile by hyper-Rayleigh scattering, Phys. Rev. Lett. 84, 1224-1227 (2000).
  • P. Kaatz, E.A. Donley and D.P. Shelton, A comparison of molecular hyperpolarizabilities from gas and liquid phase measurements, J. Chem. Phys. 108, 849-856 (1998).
  • D.P. Shelton, Bacteriorhodopsin optoelectronic synapses, Opt. Lett. 22, 1728-1730 (1997).
  • P. Kaatz and D.P. Shelton, Polarized hyper-Rayleigh light scattering measurements of nonlinear optical chromophores, J. Chem. Phys. 105, 3918-3929 (1996).
  • P. Kaatz and D.P. Shelton, Collision induced hyper-Rayleigh scattering in CCl4, Mol. Phys. 88, 683-691 (1996).
  • P. Kaatz and D.P. Shelton, Spectral measurements of hyper-Rayleigh light scattering, Rev. Sci. Instrum. 67, 1438-1444 (1996).
  • D.P. Shelton and J.J. Palubinskas, Vibrational hyperpolarizabilities and the Kerr effect in CH4, CF4 and SF6, J. Chem. Phys. 104, 2482-2487 (1996).
  • D.P. Shelton and J.E. Rice, Measurements and calculations of the hyperpolarizabilities of atoms and molecules in the gas phase, Chem. Rev. 94, 3-29 (1994).
  • D.P. Shelton, Nonlinear-optical susceptibilties of gases measured at 1064 and 1319 nm, Phys. Rev. A 42, 2578-2592 (1990).

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