1:30 pm
The Formation of Three Dimensional Bud-Like Structures in Various Tri-Octyl Phosphine Oxide and 1,2-Dipalmitoyl–sn-Glycero-3-Phosphocholine Mixtures
Eric A. Tong* and Bret N. Flanders, Department of Physics, Oklahoma State University, Stillwater, OK 74078.
Abstract
The surface pressure-area isotherms of different tri-octyl phosphine oxide (TOPO) and 1,2-dipalmitoyl–sn-glycero-3-phosphocholine (DPPC) mixture monolayers were collected on the air-water interface. Most of these isotherms exhibited a plateau at a surface pressure between 30mN/m and 40mN/m, similar to the plateau of pure TOPO monolayer isotherms. However, after continual compression, these isotherms also showed a secondary liftoff which do not exist in the pure TOPO case. The lengths of the plateaus on these isotherms are dependent on the mole percent of the mixtures; as the mole percent of TOPO increases, the plateau length also increases. Through AFM microscopy, small bud-like structures were observed on pure TOPO monolayer at surface pressures in its plateau region. These behaviors suggest that both the mixtures of DPPC and TOPO and pure TOPO form these bud-like structures under the two dimensional monolayer in order to undergo compression without increasing the surface pressure of the interface.
*Department of Physics, Duke University, Durham, North Carolina
1:50 pm
Hydrogen Bonding Interactions Between Amino Acid Side Chains and Isotopic Labeling of Tyrosine for Infrared Spectroscopy
David Paige, Beining Nie and Aihua Xie, Department of Physics, Oklahoma State University, Stillwater, Oklahoma 74078.
Abstract
Infrared Spectroscopy is an important technique for studying protein structure and dynamics. Fourier Transform Infrared Spectroscopy (or FTIR) is a form of infrared spectroscopy which has several key advantages. First it has high wavenumber accuracy and allows the creation of very high-resolution instruments. Secondly, the Jacquinot advantage arises from the circular apertures used in FTIR apparatuses, which have larger areas than the corresponding linear apertures in traditional spectrometers. Finally, the use of a Michelson interferometer allows very good time resolutions, essential to any detailed study of protein dynamics.1 Tyrosine (Tyr) and aspartic acid (Asp) are two amino acids which play an important role in many protein structures. Theoretical ab initio calculations of frequency are important in determining the interaction of these two amino acids with other side chains so that protein structure can be better understood. Finally, isotopic labeling of tyrosine can provide important clues for the deduction of protein function.
2:10 pm
Photorefractive Evaluation of LiNbO3 Co-doped with Fe and Ni
Rebekah Esmaili, Joel J. Martin, and Walid Hikal,
Department of Physics,
Oklahoma State University,
Stillwater, OK 74078.
Abstract
The photorefractive properties of LiNbO3 (LN) improve when doped with certain transition metals, in particular iron and nickel. LN doped with Fe and co-doped with Fe and Ni were measured at three different wavelengths in the visible and near-infrared. The three crystals that showed improved optical performance were LN:0.1%Fe, LN:0.05%Fe + 0.1%Ni, and LN:0.2% Fe + 0.1% Ni. The photorefractive response was measured by writing a simple holographic grating with two crossed laser beams; one beam was interrupted periodically to read the Bragg reflected signal of the other beam. At 514 nm LN:0.2% Fe + 0.1% Ni had a slightly faster rise time but the magnitudes of gratings for all three samples were about the same. Diffraction efficiency at 633 nm light improved with increased percentages of iron. However, at 784 nm LN:0.2% Fe + 0.1% Ni showed a significantly improved performance over the other two samples. At 784 nm the excitation is into a broad Ni2+ internal transition. It appears that this excitation may couple to the Fe and free charge necessary for the photorefractive effect.
This research was supported by the National Science Foundation-Research Experience for Undergraduates, the Air Force Research Laboratory, WPAFB, and the Anteon Corporation.
2:30 – 2:50 pm Intermission
2:50 pm
Force Measurement with Optical Tweezers
Matt Andrews, Emanuela Ene, Jerry Morgan, Electrical Engineering and Physics Departments, Oklahoma State University, Stillwater, OK 74078.
Abstract
This experiment is designed to calibrate an optical trap for the purpose of SERS tweezing. In order for this to be done, one must know the forces that are: 1) Being exerted by the tweezers upon the particle, and 2) exerted by the fluid upon the particle. Previously this has been done in order to view biological samples. In this case we are trapping polystyrene spheres in the order of 0.1 to 6.4 microns. Some of the particles have had carbon nano tubes attached to them. The particles are captured because light carries momentum, which is similar to stopping a train with about one trillion ping pong balls. Trapping is accomplished by expanding the laser beam to the size of the objectives first lens and the radius of curvature set to the objective. Force calculations are made by finding the maximum speed one can move the particle while holding the particle in the trap. With this and knowledge of the solution that the particle is submersed in, stokes force can then be calculated.
3:10 pm
Frequency Stabilizing using the DAVLL Technique
Jonathan White, Gil Summy, Ghazal Behin-Aein, and Peyman Ahmadi, Department of Physics,
Oklahoma State University,
Stillwater, OK 74078.
Abstract
In laser cooling and laser trapping experiments it is very important to have the laser locked to specific frequency without drifting more than 1 MHz. The DAVLL technique, which we have set up, utilizes the dichroic properties of Rb vapor in a magnetic field. The left- and right- circular polarizations are only absorbed by the ml=-1 and the ml=+1 hyperfine transitions respectively. By then separating these polarizations an error signal can be obtained whose locking slope depends on the magnitude of the hyperfine separation (about 500 MHz). We send a 785nm diode laser, reflected off of a diffraction grating, into a Rb vapor cell, which is in a magnetic field of about 100 gauss. The two polarization beams are divided using a quarter wave plate and a polarizing beam splitter, and they are then sent into photodiodes. Through these techniques, we were able to observe the DAVLL signal in the experimental setup.
3:30 pm
Experimental Investigation of Diffraction by Multiple Gratings for use in Quantum Chaos Experiments
Jason Cartwright and G. S. Summy, Department of Physics, Oklahoma State University, Stillwater, Oklahoma 74078.
Abstract
We investigate the spread of momentum in the spatial frequency band due to several diffraction gratings of uniform grating period that are separated by variable distances. The incident plane wave undergoes an evolution by the grating potential, which is affected by the phase modulation depth. The wave then undergoes a second evolution by the different phases from the grating, which depend on grating separation and increase quadratically with increasing diffraction order. Additionally, we note how varying the grating separation effects the positioning of intensity maxima. Finally we discuss the relevance of this work to the study of quantum chaos.
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