Shape measuring apparatus and shape measuring method

3:

• The shape measuring apparatus according to claim 1,
• wherein the shape measuring device includes
• an A surface detector that detects light intensity signals of the A surface measuring interference light and the A surface reference interference light in the A surface interference unit,
• a B surface detector that detects light intensity signals of the B surface measuring interference light and the B surface reference interference light in the B surface interference unit,
• an A surface lock-in amplifier and a B surface lock-in amplifier that detect phases of a measurement signal and a reference signal, respectively, when a phase difference between the measurement signal and the reference signal is represented by θ and output two output signals of cos θ and sin θ, respectively, and
• a thickness arithmetic unit that obtains a variation in the thickness of the object to be measured based on the output signals from the A surface lock-in amplifier and the B surface lock-in amplifier,
• wherein the A surface lock-in amplifier receives the light intensity signal of the A surface measuring interference light and the light intensity signal of the A surface reference interference light detected by the A surface detector, as the measurement signal and the reference signal,
• wherein the B surface lock-in amplifier receives the light intensity signal of the B surface measuring interference light and the light intensity signal of the B surface reference interference light detected by the B surface detector, as the measurement signal and the reference signal, and
• wherein the thickness arithmetic unit obtains a variation in the thickness of the object to be measured based on addition of a phase obtained as the first phase based on a result of dividing the output signal of sin θ by the output signal of cos θ, both the signals being output from the A surface lock-in amplifier, and a phase obtained as the second phase based on a result of dividing the output signal of cos θ by the output signal of sin θ, both the signals being output from the B surface lock-in amplifier, or based on addition of a phase obtained as the first phase based on a result of dividing the output signal of cos θ by the output signal of sin θ, both the signals being output from the A surface lock-in amplifier, and a phase obtained as the second phase based on a result of dividing the output signal of sin θ by the output signal of cos θ, both the signals being output from the B surface lock-in amplifier.

5:

• A shape measuring method comprising:
• branching a measuring light into an A surface measuring light and a B surface measuring light;
• generating an A surface measuring interference light and an A surface reference interference light, the A surface measuring interference light being generated by further branching the A surface measuring light branched in the branching into a first A surface measuring light and a second A surface measuring light and by causing a first post-emission A surface measuring light emitted to and reflected from a portion of a first measurement position on one surface of an object to be measured in the first A surface measuring light to interfere with the second A surface measuring light through optical heterodyne interference, the A surface reference interference light being generated by causing a first pre-emission A surface measuring light before emission to the portion of the first measurement position in the first A surface measuring light to interfere with the second A surface measuring light through the optical heterodyne interference;
• generating a B surface measuring interference light and a B surface reference interference light, the B surface measuring interference light being generated by further branching the B surface measuring light branched in the branching into a first B surface measuring light and a second B surface measuring light and by causing a first post-emission B surface measuring light emitted to and reflected from a portion of a second measurement position, opposing the portion of the first measurement position, on the other surface of the object to be measured in the first B surface measuring light to interfere with the second B surface measuring light through the optical heterodyne interference, the B surface reference interference light being generated by causing a first pre-emission B surface measuring light before emission to the portion of the second measurement position in the first B surface measuring light to interfere with the second B surface measuring light through the optical heterodyne interference;
• and
• obtaining a variation in a thickness of the object to be measured based on a first phase obtained by detecting phases of the A surface measuring interference light and the A surface reference interference light that has been generated and a second phase obtained by detecting phases of the B surface measuring interference light and the B surface reference interference light that has been generated,
• wherein in the generation of the A surface measuring interference light and the A surface reference interference light and the generation of the B surface measuring interference light and the B surface reference interference light, when the optical heterodyne interference is performed, the first A surface measuring light and the second B surface measuring light are made to be equal in frequency, and the first B surface measuring light and the second A surface measuring light are made to be equal in frequency.