초록 ▼

A laser oscillation frequency stabilizer including a laser light source portion having a laser light source whose oscillation frequency can be controlled and configured to emit a laser beam. The frequency stabilizer includes a polarized beam splitter configured to split a laser beam from the laser l

A laser oscillation frequency stabilizer including a laser light source portion having a laser light source whose oscillation frequency can be controlled and configured to emit a laser beam. The frequency stabilizer includes a polarized beam splitter configured to split a laser beam from the laser light source portion into laser beams having linearly polarized components. The frequency stabilizer includes a quarter wavelength plate converts the laser beams, split by the polarized beam splitters, into circularly polarized laser beams. Further, an absorption cell sealed with gaseous atoms or molecules having a certain absorption spectrum is disposed in an optical path of the circularly polarized laser beams, and has a uniform magnetic field applied thereto. A half mirror reflects partially each of the circularly polarized laser beams back through the absorption cell. A control portion controllably locks the oscillation frequency of the laser light source in accordance with transmitted light reception levels of laser light having passed in opposite directions through the absorption cell

대표청구항 ▼

1. A laser oscillation frequency stabilizer comprising:a laser light source portion including a laser light source configured to have a controlled oscillation frequency and to emit a laser beam; a polarized beam splitter portion configured to split the laser beam from said laser light source portion

1. A laser oscillation frequency stabilizer comprising:a laser light source portion including a laser light source configured to have a controlled oscillation frequency and to emit a laser beam; a polarized beam splitter portion configured to split the laser beam from said laser light source portion into two laser beams, each of said two laser beams having linearly polarized components orthogonal to each other; a quarter wavelength plate configured to form from the two laser beams, split by way of said polarized beam splitter portion, circularly polarized first and second laser beams, the circularly polarized first and second laser beams being polarized in an opposite direction to each other; an absorption cell disposed in an optical path of the circularly polarized first and second laser beams, sealed therein with gaseous atoms or molecules having a certain absorption spectrum, and configured to have a uniform magnetic field applied thereto; a half mirror disposed in the optical path of the circularly polarized first and second laser beams after the absorption cell, configured to reflect partially the circularly polarized first and second laser beams back in an opposite direction through said absorption cell and onto said quarter wavelength plate to form linearly polarized third and fourth laser beams, and configured to transmit partially the circularly polarized first and second laser beams; a first light-receiving portion configured to receive the partially transmitted circularly polarized first laser beam; a second light-receiving portion configured to receive the partially transmitted circularly polarized second laser beam; a third light-receiving portion configured to receive the linearly polarized third laser beam; a fourth light-receiving portion configured to receive the linearly polarized fourth laser beam; and a control portion configured to controllably lock the oscillation frequency of said laser light source to said absorption spectrum in accordance with transmitted light reception levels provided by said first to fourth light-receiving portions, said control portion configured to control said laser beam source so that a difference between a ratio of a light reception level of said first light-receiving portion to a light reception level of said third light-receiving portion and a ratio of a light reception level of said second light-receiving portion to a light reception level of said fourth light-receiving portion is substantially zero.