34 results about "Argon ion laser" patented technology

Disclosed is a mixed carbon material for use in an electrode of a non-aqueous secondary battery showing excellent characteristics having rapid charge-discharge characteristics and high cycle characteristics. More particularly, disclosed is a negative electrode material for non-aqueous electrolyte secondary battery comprising the following carbon material A and carbon material B, wherein the carbon material A is a multilayer-structured carbon material which contains graphite particles and amorphous carbon covering the surfaces of the particles, and in which a 002 plane spacing (d002) measured by X-ray wide angle diffraction is 3.37Angstrom or less, Lc is 900Angstrom or more, a tap density is 0.8 g / cm<3> or more, and a Raman R value, which is the ratio of a peak intensity at around 1360 cm<-1> to a peak intensity at around 1580 cm<-1> in an argon ion laser Raman spectrum, is 0.25 to 0.6; and the carbon material B is graphite particles in which a 002 plane spacing (d002) measured by X-ray wide angle diffraction is 3.37Angstrom or less, Lc is 900Angstrom or more, a tap density is 0.8 g / cm<3> or more, a Raman R value, which is the ratio of a peak intensity at around 1360 cm<-1> to a peak intensity at around 1580 cm<-1> in an argon ion laser Raman spectrum, is 0.2 to 0.5, and an average circularity measured by a flow-type particle analyzer is 0.9 or more.

A method for producing low-noise laser output at various wavelengths and / or in various operation modes in a monolithic microchip laser comprises schemes of generating two fundamental beams in separate cavities, precise intracavity beam combination based on the walk-off effect in birefringent crystal, and wavelength conversion in nonlinear optical crystals. The fundamental beams are produced from light sources selected upon the desired wavelengths, polarizations, and other features related to the laser output. Low-noise laser devices operated in SLM or with spectra of flat-top or desired bandwidths are constructed according to the method. High-volume fabrication is feasible. Apparatus of compact size and efficient frequency conversion is demonstrated with various configurations including those for generating low-noise 491 nm laser, as a replacement of Argon ion laser.

The invention discloses a controllable terahertz wave attenuator device and a method. The device is that a computer is connected respectively with a D / A converter and a two-dimensional moving platform, the D / A converter is connected with a direct current high voltage amplifier, a terahertz wave source device, a chopper, a piece of focusing lens, a high resistance silicon, a piece of focusing lens, a terahertz wave detector, a locking phase amplifier, an A / D converter, and the computer, the high-resistance silicon is connected respectively with an argon ion laser and the two-dimensional moving platform. The method is that lasers which are issued by the argon ion laser are used by the controllable terahertz wave attenuator device to excite photo-generated carriers; terahertz waves can be decreased through the absorbing effect of the photo-generated carriers to the terahertz waves. The controllable terahertz wave attenuator device of the invention has large decrement, smooth attenuating spectra ray, compact structure, convenient adjustment, low cost, and can satisfy the requirements of the terahertz waves for applying in the fields of imaging, medical diagnosis, safety check, information communication, space astronomy, and the like.

The electrochemical device of the present invention comprises a positive electrode (2), a negative electrode (1), a nonaqueous electrolyte and a separator (3). The separator (3) includes a porous layer (I) composed of a microporous film composed predominantly of a thermoplastic resin and a porous layer (II) containing a filler having a heat-resistant temperature of 150° C. or higher as the main component. The negative electrode (1) contains graphite having an R value of 0.1 to 0.5 and d002 of 0.338 nm or less as a negative electrode active material, where the R value is a ratio of a peak intensity at 1360 cm−1 to a peak intensity at 1580 cm−1 in an argon ion laser Raman spectrum and the d002 is a lattice spacing between 002 planes. The ratio of the graphite to the negative electrode active material is 30 mass % or more, and the nonaqueous electrolyte contains vinyl ethylene carbonate or a derivative thereof, or a dinitrile compound or acid anhydride.

To provide a mixed carbon material used for an electrode of a nonaqueous secondary battery with excellent characteristics satisfying both rapid charge-discharge characteristics and high cycle characteristics. A negative electrode material for nonaqueous electrolyte secondary battery, comprising the following carbon material A and carbon material B: (Carbon material A) a multilayer-structure carbon material containing a graphitic particle and an amorphous carbon covering the surface of the graphitic particle, which is a carbon material where the interplanar spacing (d002) of 002 planes by the wide-angle X-ray diffraction method is 3.37 Å or less, Lc is 900 Å or more, the tap density is 0.8 g / cm 3 or more, and the Raman R value that is a ratio of the peak intensity near 1,360 cm -1 to the peak intensity near 1,580 cm -1 in the argon ion laser Raman spectrum, is from 0.25 to 0.6, (Carbon material B) a graphitic particle where the interplanar spacing (d002) of 002 planes by the wide-angle X-ray diffraction method is 3.37 Å or less, Lc is 900 Å or more, the tap density is 0.8 g / cm 3 or more, the Raman R value that is a ratio of the peak intensity near 1,360 cm -1 to the peak intensity near 1,580 cm -1 in the argon ion laser Raman spectrum, is from 0.2 to 0.5, and the average degree of circularity as determined by a flaw-type particle analyzer is 0.9 or more.

A vertical magnetic recording disc (100) includes a base (10), a magnetic recording layer (22), and a medium protection layer (26). The magnetic recording layer (22) is a ferromagnetic layer having a granular structure where a granular portion is formed. The medium protection layer (26) contains nitrogen (N) atoms and carbon (C) atoms with a number ratio (N / C) in a range from 0.050 to 0.150. In a Raman spectrum obtained by exciting the medium protection layer (26) by argon ion laser light of wavelength 514.5 nm, from which a fluorescence is removed, the peak ratio Dh / Gh is in a range from 0.70 to 0.95, when a D peak Dh appearing in the vicinity of 1350 cm−1 is separated from G peak Gh appearing in the vicinity of 1520 cm−1 by the Gauss function.

To provide a negative electrode carbon material capable of suppressing capacity degradation which will occur due to repetition of a charge / discharge cycle, storage under a charged state, float charging, or the like. An artificial graphite for a negative electrode of a lithium secondary battery having a c-axis crystallite size L (112) of from 2.0 to 4.2 nm as calculated from a (112) diffraction line obtained by X-ray wide-angle diffractometry and having a half-value width ΔνG of from 15 to 19 cm−1 for a peak appearing in a wavelength region of from 1580 cm−1±100 cm−1 in the Raman spectroscopy using an argon ion laser light having a wavelength of 5145 angstrom.

The laser sheet light source system of the present invention comprises: a first reflector, a second reflector, a Fresnel lens, a grid fine-tuning device, an argon ion laser, a heat exchanger and a cooling tower. One end of the heat exchanger forms an outer circulation loop with the cooling tower, and the other end of the heat exchanger forms an inner circulation loop with the resonant cavity cooling chamber of the argon ion laser, and the cooling water circulates in the outer circulation loop and the inner circulation loop respectively. The laser beam emitted by the argon ion laser passes through the grid fine-tuning device, the Fresnel lens, the second reflector and the first reflector in sequence. The grid fine-tuning device, the argon ion laser, the Fresnel lens, the second reflector and the first reflector are respectively installed on the sheet light turning device. The heat exchange system of the present invention ensures the safe operation of the laser; the grid fine-tuning device can flexibly adjust the transmission orientation of the high-power laser beam, and at the same time, the sheet light steering device can flexibly adjust the transmission height and orientation of the sheet light, which greatly facilitates users Change the measurement section.

Provided is a synthetic graphite material, in which a size L (112) of a crystallite in a c-axis direction as calculated from a (112) diffraction line obtained by an X-ray wide angle diffraction method is in a range of 4 to 30 nm, a surface area based on a volume as calculated by a laser diffraction type particle size distribution measuring device is in a range of 0.22 to 1.70 m2 / cm3, an oil absorption is in a range of 67 to 147 mL / 100 g, and a half width ΔvG of a peak present in a wavelength range of 1580 cm−1±100 cm−1 is in a range of 19 to 24 cm−1 in Raman spectrum analysis using argon ion laser light having a wavelength of 514.5 nm.

A lithium cell includes a positive electrode, a negative electrode employing a carbon material as an active material, and a non-aqueous electrolyte including a solute dissolved in a non-aqueous solvent, and is characterized in that the carbon material in the negative electrode has an RA value (IA / IG) of 0.05 or more, the RA value calculated from a peak intensity (IA) of a broad peak PA having a full width at half maximum of 100 cm<-1 >or more and a peak intensity (IG) in the vicinity of 1580 cm<-1 >as determined by laser Raman spectroscopy using an argon ion laser having a wavelength of 514.5 nm, the peak intensity (IA) determined from a peak PD in the vicinity of 1360 cm<-1>, as determined by the aforesaid laser Raman spectroscopy, which is separated into the broad peak PA having the full width at half maximum of 100 cm<-1 >or more and a peak PB having a full width at half maximum of less than 100 cm<-1>.

The invention discloses a measuring device and method for a two-phase flow system internal particle motion trajectory. The measuring device comprises a laser emission system and a photovoltaic conversion detection system, wherein the laser emission system is composed of an argon ion laser, a first cylindrical lens, a second cylindrical lens and a reactor, and the photovoltaic conversion detection system is composed of three optical receivers, three photomultiplier tubes, a filter and a computer. The three optical receivers are evenly arranged around the peripheral side of the reactor by using the reactor as a circle center. According to the measuring method, non-immersive measurement is included, the measuring device does not need to be placed into the reactor, the influence of the measuring device on two-phase flow inside the reactor is avoided, measuring accuracy is improved, and the measuring result is precise and reliable; the argon ion laser is used as a light source and replaces an X-ray source, the cost of an X-ray detector is omitted, and the measuring device is economical, practical, safe and reliable.

A synthetic graphite material wherein the crystal grain size L(112) in the c-axis direction as calculated from a (112) diffraction line obtained by wide-angle X-ray diffraction is 4-30 nm, the surface area based on volume as calculated by a laser diffraction-type particle size distribution measurement device is 0.22-1.70 m2 / cm3, the oil absorption is 67-147 mL / 100g, and the half-value width [delta][nu]G is 19-24 cm-1 for a peak appearing in the wavelength region of 1580 cm-1+ / -100 cm-1 in Raman spectroscopy using argon ion laser light having a wavelength of 514.5 nm.

Disclosed is a carbon material for electrode. The carbonaceous material has a plane space d002 of a (002) plane less than 0.337 nm in an X-ray wide angle diffraction method, a crystallite size (Lc) of 90 nm or higher, an R value, as a peak intensity ratio of a peak intensity of 1360 cm<-1> to a peak intensity of 1580 cm<-1> in a Raman spectrum in use of an argon ion laser, of 0.20 or higher, and a tap density of 0.75 g / cm<3> or higher. Also disclosed is a multilayer structure carbonaceous material for electrode, which is manufactured by carbonizing some organic compounds where the carbonaceous material for electrode is mixed with the organic compounds. The battery using the carbonaceous material for electrode or the multilayer structure carbonaceous material for electrode has a large capacity, a small irreversible capacity admitted in the initial cycle, excellent capacity maintaining rate of the cycle, and particularly, largely improved quick charging and discharging characteristics.