Patent ID: 11921040
Assignee: SHIMADZU CORPORATION
Field: Measurement (Instruments)
Classification: CPC G  H | IPC G

Claim 1:
2. A gas absorption spectroscopic measurement device configured to acquire a component concentration of a gas to be measured by cavity ring-down absorption spectroscopy, the gas absorption spectroscopic measurement device comprising:
a laser irradiation unit;
an optical resonator configured to cause light emitted from the laser irradiation unit to resonate, the optical resonator including a measurement cell for accommodating the gas to be measured; and
a first detector configured to detect light taken out of the optical resonator,
wherein the laser irradiation unit includes:
a frequency adjustable laser light source;
a splitting unit splitter configured to split the laser light emitted from the laser light source into a plurality of laser light;
a frequency converter configured to output one of the plurality of laser light split by the splitter having a frequency of the frequency of the laser light source multiplied by a predetermined number of times;
a first frequency modulator configured to modulate a frequency of the laser light emitted from the frequency converter, using a first modulation signal;
a second frequency modulator configured to modulate a frequency of the other laser light split at the splitter, using a second modulation signal;
a combiner configured to cause first laser light modulated by the first frequency modulator and second laser light modulated by the second frequency modulator to be incident on the optical resonator in an optically separable manner; and
a second detector configured to independently detect returning light from the light resonator derived from the first laser light emitted to the optical resonator and returning light from the light resonator derived from the second laser light emitted to the light resonator; and
a feedback controller,
wherein the feedback controller is configured to:
generate a first error signal reflecting a difference between a frequency of the first laser light and a mode frequency of the optical resonator, based on a detection signal by the second detector and the first modulation signal;
perform feedback control of an oscillation frequency of the laser light source in response to the first error signal to thereby adjust the oscillation frequency to the mode frequency of the oscillation resonator; and thereafter
maintain a state of the feedback control, or
generate a second error signal reflecting a difference between a frequency of the second laser light and the mode frequency of the optical resonator, based on a detection signal by the second detector derived from returning light derived from the second laser light and the second modulation signal, and perform feedback control corresponding to the second laser light to continuously perform the control of the oscillation frequency of the laser light source.