Abstract: A gas measuring apparatus includes a cell portion, a light source portion, a detection portion, and a control portion. The cell portion includes a space into which a sample gas containing breath containing a first isotope of carbon dioxide and a second isotope of carbon dioxide is introduced. The light source portion changes a wavelength of the light in a band of 4.345 ?m or more and 4.384 ?m or less. The detection portion performs an operation including first detection of an intensity of the light passing through the space and second detection of an intensity of the light passing through the space into which the sample gas is not introduced. The control portion calculates a ratio of an amount of the second isotope to an amount of the first isotope based on a result of the first detection and a result of the second detection.

Abstract: A gas measuring apparatus of an embodiment includes a light source, a gas cell and a detection portion. The light source emits infrared light. Into the gas cell, gas containing 13CO2 and 12CO2 is introduced, and the gas cell includes an incident surface on which the infrared light is incident and an emission surface through which the infrared light is transmitted. The gas cell has a cell length of 2.5 cm or more and 20 cm or less. The detection portion measures a first transmittance of transmitted light from the emission surface at a first wavelength in wavelength range in an absorption line of the 13CO2 and a second transmittance of transmitted light from the emission surface at a second wavelength in the wavelength range in an absorption line of the 12CO2, and is capable of calculating a concentration of each of the 13CO2 and the 12CO2.

Abstract: According to one embodiment, a laser annealing method includes: detecting an intensity distribution of a laser light formed as a line beam by a line beam optical system; dividing width in short axis direction of the line beam in the detected intensity distribution by number of times of the irradiation per one site and partitioning the width; and calculating increment of crystal grain size of a non-crystalline thin film for energy density corresponding to wave height of the partitioned intensity distribution, and summing the increments by number of times of pulse irradiation, when energy density of the laser light is larger than a threshold, the crystal grain size of the non-crystalline thin film taking a downward turn at the threshold, the increment summed before the energy density exceeds the threshold being set to zero.

Abstract: According to one embodiment, a laser annealing method includes: detecting an intensity distribution of a laser light formed as a line beam by a line beam optical system; dividing width in short axis direction of the line beam in the detected intensity distribution by number of times of the irradiation per one site and partitioning the width; and calculating increment of crystal grain size of a non-crystalline thin film for energy density corresponding to wave height of the partitioned intensity distribution, and summing the increments by number of times of pulse irradiation, when energy density of the laser light is larger than a threshold, the crystal grain size of the non-crystalline thin film taking a downward turn at the threshold, the increment summed before the energy density exceeds the threshold being set to zero.

Abstract: A laser radiating apparatus controls an intensity of energy of a laser beam output from a laser generating device and radiates an object with the laser beam. The laser radiating apparatus includes an intensity homogenizer for substantially homogenizing distribution of the intensity of energy of the laser beam, an imaging lens for converging the laser beam substantially homogenized by the intensity homogenizer and radiating an object with the laser beam, a slit for removing a part of the converged laser beam and shaping it into a predetermined beam shape, a detector for detecting an intensity of energy of the part of the laser beam removed by the slit, and a control device for controlling the intensity of energy of the laser beam based on a detection signal output from the detector.