Japan Atomic Energy Research Institute

Mitsubishi Chemical Industries Limited

Kyocera Corporation

Takashi Arisawa

Yoichiro Maruyama

Masaaki Kato

Kyoichi Deki

Fumiaki Matsuoka

Masaharu Kaneko

Akira Ohzu

Koreyuki Shiba

Youji Suzuki

Hitoshi Ono

Toshio Niwa

Seiichi Imahori

Hideaki Sakai

Kenji Ogura

Hiromitsu Kiriyama

Shigeki Kitamura

Kazumi Iwamoto

Katsuaki Akaoka

Masahiko Nishide

Tsuyoshi Nakayama

Akira Sugiyama

Yoji Suzuki

Toku Shimizu

Koji Tamura

Hitohsi Ono

A liquid crystal display device includes first and second substrates; a liquid crystal layer placed between the first and second substrates; gate lines; source lines; a first insulation film covering the gate lines and the source lines; a light-shielding film covering the source lines; a second insulation film covering the gate lines, the source lines, and the light-shielding film; a signal electrode disposed on the second insulation film; and a common electrode disposed on the second insulation film, a shield electrode being placed so as to lie between the signal electrode and the source line as seen in a plan view, as well as to lie between the first insulation film and the light-shielding film as seen in a sectional view, and a third insulation film being placed between the shield electrode and the light-shielding film.

Liquid crystal display device comprising voltage fluctuations

A method for generating ultra-short pulse amplified Raman laser light. Short pulse laser light is amplified, and a portion thereof is introduced into a Raman oscillator to produce compressed laser light. The compressed light is introduced to a first Raman amplifier. The remainder of the short pulse laser light is introduced to a polarizer, and the reflected light is introduced into the first Raman amplifier to pump it. The light transmitted through the first Raman amplifier that has not contributed to pumping is introduced to a beam splitter to produce a second reflected light that is passed to a second Raman amplifier to pump that amplifier. The compressed light is amplified in the first Raman amplifier and introduced to the second Raman amplifier to further amplify it. This further amplified radiation is passed through delay lines to the beam splitter, which passes only first Stokes radiation to generate ultra-short pulse amplified Raman laser light.

Systems for generating high-power short-pulse laser light

Short-pulse Raman laser is used to perform precision working of a substance without causing thermal effects on it or examine the interior of the skin or process the interior of a transparent material such as glass. By typically choosing a suitable Raman medium to be illuminated with a pump laser, the short-pulse Raman laser can have a wavelength that matches the wavelength of absorption by the substance of interest.

Method of processing substances by short-pulse, wavelength tunable raman laser

Systems for generating short-pulse laser light

The efficiency of wavelength conversion of laser light can be improved by allowing incident laser light to pass through nonlinear optical crystals a multiple of times. In converting the wavelength of laser light to generate second- and higher harmonic waves, a returning mirror, a polarizer and nonlinear optical crystals are combined and the rotation of polarized light is utilized to allow the incident laser light to undergo multiple passes through the nonlinear optical crystals so that it can be converted in wavelength with higher efficiency.

Method for changing a wavelength of a laser light

The wavefront of laser light as it propagates through a medium is controlled so that not only the inherent aberrations in the wavefront of the laser light itself but also the aberrations that are progressively caused by passage of laser light through the medium are effectively corrected to achieve long-distance propagation of the laser light through the medium.

Method of enabling laser light to propagate through a medium over long distance by means of controlling its wavefront

The compensation amount of the pressure for keeping the index of refraction of the gas constant is calculated on the basis of the pressures and the temperatures that have been measured at different time. Only the pressure of the gas will be varied in accordance with the calculated compensation value of the pressure, whereby the index of the gas can be maintained constant and the oscillation frequency can be kept constant as the consequence. The pressure corresponding to a desired sweeping oscillation frequency is also calculated using the measured pressures and temperatures. The pressure of the gas is varied on the basis of the result of calculation. Synchronously with the variation of the pressure of the gas, the cavity length and the angle of the frequency selecting element are compensated.

Apparatus and method of stabilizing oscillation frequency for single

The improved metal vapor laser capable of cold operation performs plasma etching on a vaporizing metal within a laser tube in the presence of a reactive gas so that the metal is vaporized at temperatures below its boiling point to effect laser oscillation. The laser can be operated at much lower temperatures than a conventional hot-operating version which produces metal vapors by thermal evaporation; in addition, the laser will experience a smaller heat loss while undergoing limited thermal damage to its structural members; further, laser light can be oscillated to produce high output power and, at the same time, the warmup time can be shortened significantly.

Metal vapor laser capable of cold operation

A method of producing a small expansion of laser light, in a pulse laser apparatus, including producing a small preliminary laser light by pumping a laser medium, and then, after an appropriate time lag, then pumping the preliminary laser medium at a higher intensity than the first pumping, thereby producing a laser light which is smaller in beam expansion than in the case where a preliminary pumping is not performed. The laser light which is smaller in beam expansion is due to the population inversion occurring in a small beam expansion part of pulse laser light obtained by the preliminary pumping.

Method of producing a small beam expansion of laser light

A solid state tunable laser resonator having a laser element, an excitation light source for outputting a pumping light, and elements for selecting a wavelength of the pumping light and directing the wavelength of the pumping light onto the laser element at a first point thereof on a first axis substantially parallel to an axis of oscillation light emitted by the laser element. The laser resonator may also include elements for directing the pumping light onto the laser element at a second additional point thereof. The laser resonator can be used as a laser light source having a wide tunable range with a narrow line width.

Solid-state tunable laser resonator

A method is, herein, disclosed for separating a specific isotope from a mixture of isotopes by first irradiating the isotope mixture with a highly monochromatic laser light that resonates only with the energy level of the specific isotope so as to increase its chemical activity and then bombarding said specific isotope with a molecule containing highly reactive atoms so as to form a spatially separated compound rich in the specific isotope.

Method of separating isotopes

There is herein, disclosed a dye laser including a container for a dye solution and a pumping energy source coupled thereto, said dye solution containing a perimidone dye formula (I): ##STR1## wherein R.sup.1 is a hydrogen atom, an alkyl group, a trifluoromethyl group, an alkoxycarbonyl group, an alkoxycarbonylalkyl group, an aralkyl group or a phenyl group; R.sup.2 is an optionally substituted alkoxycarbonyl group, a cyclohexyloxycarbonyl group, tetrahydrofurfuryloxycarbonyl group, an aryloxycarbonyl group, a benzyloxycarbonyl group, an acyl group, a cyano group or an optionally substituted carbamoyl group; R.sup.3 and R.sup.4 which may be the same or different are each a hydrogen atom, an alkyl group, an alkoxyalkyl group, an aralkyl group or an aryl group.

Dye laser

A process is, herein, disclosed for separating a particular isotope from a mixture of different isotopes by selective excitation and ionization of the particular isotope with a single laser beam, said process comprising heating the mixture, converting the resulting atomic vapor to a highly directional atomic beam by suitable means, causing said atomic beam to travel through a vacuum, crossing the atomic beam with a high-intensity laser beam having a specific wavelength, selectively exciting the particular isotope with a first photon having that specific wavelength while the other isotopes remaining in the ground state, allowing the excited isotope to absorb a second photon to be excited to a virtual energy level, causing the so excited isotope to absorb a third photon to ionize said isotope, and recovering the ionized isotope by use of an electric or electromagnetic field.

Process for separating an isotope from a mixture of different isotopes

A dye laser comprising a container retaining a dye solution for laser and an energy source for pumping connected to the container, the dye solution containing a pyrazoloazaxanthenoisoquinolinone dye.

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Kyoto, Japan

Takashi Arisawa