Abstract:
A method for monitoring the effects of a chemotherapeutic agent on a neoplasm medium. The method is premised on the discovery that chemotherapeutic agent, such as retinoic acid, affects the fluorescence spectroscopy of neoplasmic media and that such differences can be monitored, for example, by comparing the spectral profiles, spectral peaks, and spectral bandwidths of fluorescence at various wavelengths of the medium before and after administration of the chemotherapeutic agent. Differences in the excitation spectroscopy of the medium can also be used to monitor the effects of the agent.
Abstract:
A method of forming 2 dimensional image of a translucent object in or behind a turbid medium. In one embodiment, the method comprises the steps of illuminating the translucent object through one side of the turbid medium with an ultrafast pulse of light, the light emergent from the opposite side of the turbid medium consisting of a ballistic component, a snake-like component and a diffuse component. The emergent light is then temporally and spatially gated to preferentially pass the ballistic component and the snake-like component. Preferably, the temporal and spatial gating is achieved by positioning the Kerr cell of an optical Kerr gate at the 2F spectral plane of a 4F Kerr-Fourier imaging system. At the appropriate time, that portion of the Kerr cell located at the focal point of the 2F spectral plane is gated open, allowing predominantly ballistic and snake-like components of the transilluminated light to pass therethrough. A cooled CCD detector is positioned at the 4F spectral plane to form a 2-dimensional image of the temporally and spatially gated light.
Abstract:
A method for distinguishing between calcified atherosclerotic tissue and either fibrous atherosclerotic tissue or normal cardiovascular tissue. The present method is based on the discovery that, when irradiated with a beam of monochromatic infrared light, calcified atherosclerotic human aortic tissue produces a Fourier Transform Raman spectrum which is distinguishable from analagous spectra obtained from fibrous atherosclerotic human aortic tissue and normal human aortic tissue. Some salient differences in the respective Raman spectra are the presence of five Raman bands at Raman shifts of 957, 1071, 1262-1300, 1445, and 1659 cm.sup.-1 (.+-.4 cm.sup.-1 for all shifts) for the calcified tissue as compared to three Raman bands at Raman shifts of 1247-1270, 1453 and 1659 cm.sup.-1 (.+-.4 cm.sup.-1 for all shifts) for the fibrous tissue and three Raman bands at Raman shifts of 1247-1270, 1449 and 1651 cm.sup.-1 (.+-.4 cm.sup.-1 for all shifts) for the normal tissue. In addition, it was discovered that the ratios of intensities for the Raman bands at 1659 and 1453 cm.sup.-1 and at 1254 and 1453 cm.sup.-1 were 0.69 and 0.53, respectively, for the calcified tissue, 1.02 and 0.85, respectively, for the fibrous tissue and 1.2 and 0.83, respectively, for the normal tissue.
Abstract:
A trigger circuit for use in providing a trigger pulse to a sweep drive circuit in a streak camera. The trigger circuit comprises a low voltage DC power supply, a resistor, a charge line and a photodetector switch all connected in series. The photodetector switch includes a slab of a semi-insulating semiconductor material which becomes photoconductive when actuated by optical radiation. In use, the trigger circuit is coupled to the sweep drive circuit of the streak camera. In the absence of optical radiation, the switch is nonconducting and a voltage from the DC power supply builds up in the charge line. When the switch is actuated by optical radiation it becomes closed causing the voltage to be discharged to the sweep drive circuit. The switch returns to a nonconducting state (i.e. an open state) after about 1.5 nanoseconds.
Abstract:
A photomultiplier tube which may be used in time resolving a luminiscence profile emitted from a sample with picosecond resolution using short (picosecond) electrical pulses as a probe and in time resolving an electrical pulse profile produced by fast electronic or optoelectronic devices with femtosecond resolution, using short (femtosecond) laser pulses as the probe is disclosed. The photomultiplier tube includes a photocathode for receiving light and producing emission of electrons in proportion to the intensity of the light, said photocathode having a transmission strip line configuration, accellerating means for accellerating electrons emitted by said photocathode, electron multiplication means for performing electron multiplication on the electrons emitted from the accellerating means, anode means for receiving electrons from the electron multiplication means and producing an analog electrical signal output, means for causing electrons emitted by the photocathode to move through the accellerating means and the electron multiplication means and then impinge on the anode means, and means connected to said photocathode for receiving an ultrafast voltage signal.
Abstract:
An electrical device for use in delaying the time of arrival of an electrical signal with fixed increments of delay in the picosecond range and having a minimum delay time in picoseconds is disclosed. In one embodiment of the invention, the device comprises a plurality of small T shaped RF coaxial connectors fixedly coupled together in series with the connectors themselves serving as delay elements. One of the unconnected (open) ports of the connector at one end of the series is used as the entrance port for the device and the other unconnected ports of the connectors in the series are used as exit ports for the device. An electrical signal introduced into the device through the entrance port and then exiting through one of the exit ports is delayed according to the total path length travelled by the signal in passing from the entrance port to the particular exit port selected to be used as the exit port, each port in the path travelled by the signal from the entrance port to the exit port producing a time delay in the order of picoseconds, the exact number of picoseconds for a port depending on the specific type of connector employed. In another embodiment of the invention, a plurality of transmission lines having different lengths between about 10 to 100 mm etched on a printed circuit board are connected to individual double pole double throw switches which are coupled together in series, each transmission line causing a time delay of a signal passing through it of a different number of picoseconds.
Abstract:
Method and device for detecting the threshold of generation of a non-visible laser beam, wherein a dark colored film, enclosed in a transparent container, is placed in the path of the laser beam to cause the dark film to burn when the laser beam impinges thereon and wherein the transparent container prevents the vaporized film particles from the area impinged upon by the laser beam from escaping into the atmosphere.
Abstract:
A method for obtaining a polarized orbital angular momentum Raman spectrum using vector vortex beams, includes the steps of emitting a polarized laser light from a laser source. The polarized laser light is passed through a narrow band filter that is then passed through a section of wave plates (quarter or half wave plate) to generate polarized light (linear, circular, radial and azimuthal), then through a q-plate (vortex retarder or spiral plate) to give a vortex structure topology carrying orbital angular momentum with a helical phase. The polarized vector vortex light is then directed to contact a sample, thereby producing a Raman scatter beam. The Raman scatter beam is passed back and collected into a spectrometer, thereby obtaining a Raman scattering spectrum of the sample to investigate the matching of the multipoles of the material and the multipoles of the light. A method for transmission with Multiple expansions of orbital angular momentum in rat cerebellum tissue is also disclosed. In general, we use polarized Laguerre-Gaussian vector vortex beams as a topology multipole model to describe and study the light matter interaction for Raman and transmission using the fact that the optical vortices and material can possess Multipoles denoted as L in form of monopole (L=0), dipole (L=1), quadrupole (L=2), octupole (L=3), hexidecapole (L=4) and higher orders. These multipoles can be involved with the matching up with the symmetry of the moments involved with vibrational states in Raman processes.
Abstract:
In this patent, we teach methods to generate coherent X-ray and UUV rays beams for X ray and UUV microscopes using intense femtosecond pulses resulting the Ultra-Supercontinuum (USC) and Higher Harmonic Generation (HHG) from χ3 and χ5 media produce from electronic and molecular Kerr effect. The response of n2 (χ3) and n4 (χ5) at the optical frequency from instantaneously response of carrier phase of envelope results in odd HHG and spectral broadening about each harmonic on the anti-Stokes side of the pump pulse at wo typically in the visible, NIR, and MIR. From the slower molecular Kerr response on femtosecond to picosecond from orientation and molecular motion on n2 and n4 which follow the envelope of optical field of the laser gives rise to extreme broadening without HHG. The resulting spectra extend on the Stokes side towards the IR, RF to DC covering most of the electromagnetic spectrum. These HHG and Super broadening covering UUV to X rays and possibly to gamma ray regime for microscopes.