Mass spectrometer performing mass spectrometry for sample with laser irradiation
View Patent ↗A mass spectrometer includes a beam radiator radiating a beam to a sample. A laser radiator radiates laser light onto an irradiation surface of a surface of the sample irradiated with the beam or above the irradiation surface. The laser radiator splits the laser light into at least first light and second light. The laser radiator adjusts a polarization state, a length of an optical path, or a direction of the optical path of at least either the first light or the second light to condense the first light and the second light onto the irradiation surface or above the irradiation surface. A detector detects particles discharged from the sample.
1. A mass spectrometer comprising:
a beam radiator radiating a beam to a sample;
a laser radiator radiating laser light onto an irradiation surface of a surface of the sample irradiated with the beam or above the irradiation surface, the laser radiator splitting the laser light into at least first light and second light and adjusting a polarization state, a length of an optical path, or a direction of the optical path of at least either the first light or the second light to condense the first light and the second light onto the irradiation surface or above the irradiation surface; and
a detector detecting particles discharged from the sample, wherein:
the laser radiator is capable of switching a difference between a length of an optical path of the first light and that of the second light being condensed by a condenser lens on a same position as the first light, between a value smaller than a coherence length and a value equal to or larger than the coherence length,
at least a part of the first light in the first condition and at least a part of the second light in the first condition are condensed to a same position,
the first light in the first condition and the first light in the second condition are condensed to a same position, and
the second light in the first condition and the second light in the second condition are condensed to a same position.
2. The mass spectrometer of claim 1 , wherein
the laser radiator includes
a splitter splitting the laser light into the first light and the second light,
a changer provided in the optical path of the first light or the second light to be capable of changing the polarization state, the length of the optical path, or the direction of the optical path of the at least either the first light or the second light, and
the condenser lens condensing one of the first light and the second light and the other of the first light and the second light having passed through the changer onto the irradiation surface or above the irradiation surface.
3. The mass spectrometer of claim 2 , wherein the changer is a birefringence modulator.
4. The mass spectrometer of claim 2 , wherein the laser radiator includes optical-path adjusting mirrors lengthening the optical path of the first light or the second light.
5. The mass spectrometer of claim 2 , wherein the changer is an acoustic cell.
6. The mass spectrometer of claim 2 , wherein
the splitter is a half mirror.
7. The mass spectrometer of claim 3 , wherein
the splitter is a half mirror.
8. The mass spectrometer of claim 1 , further comprising a particle controller directing particles to the detector, the particles being discharged from the sample by the beam and being ionized by the laser light.
9. The mass spectrometer of claim 2 , further comprising a particle controller directing particles to the detector, the particles being discharged from the sample by the beam and being ionized by the laser light.
10. The mass spectrometer of claim 3 , further comprising a particle controller directing particles to the detector, the particles being discharged from the sample by the beam and being ionized by the laser light.
11. The mass spectrometer of claim 1 , wherein the laser light is infrared laser light.
12. The mass spectrometer of claim 1 , wherein the laser radiator is capable of switching a difference between a polarization direction of the first light and that of the second light, between a first condition and a second condition, the second condition being different from the first condition in the difference of the polarization direction.