Digital signal processing (DSP) techniques for FT-IR multiple modulation measurements using a photoelastic modulator

Claim 2

In a step-scanning Fourier transform spectrometer comprising an interferometer, a detector, and a digital processor, a digital method for extracting a modulation phase and modulation frequency of a modulation signal, the method comprising: capturing a series of discrete digital values corresponding to an analog signal output from the detector, the series of discrete values having a time dependence over a sampling interval, which time dependence includes a component resulting from the modulation signal; using a nominal modulation signal at a nominal modulation frequency to process at least some of the discrete values to determine a first phase error; using the first phase error and the nominal modulation frequency to provide a first refined modulation frequency.

Claim 3

The method of claim 1, wherein the modulation signal is driving an element in the spectrometer optical train that modulates the polarization of a beam incident on the detector.

Claim 4

The method of claim 1, and further comprising adding a signal at the modulation frequency to the analog signal output from the detector before capturing the series of discrete digital values.

Claim 5

The method of claim 1, and further comprising: using the the first refined modulation frequency to process at least some of the discrete values to determine a second phase error; and using the second phase error to modify the first refined estimate of the modulation frequency to provide a second refined estimate of the modulation frequency.

Claim 6

In a step-scanning Fourier transform spectrometer comprising an interferometer, a detector, and a digital processor, a digital method for generating spectral data from a sample, the method comprising: passing a beam of analytic radiation through the interferometer and the sample to the detector; using a modulation signal to subject the beam to a modulation at a modulation frequency prior to the beam encountering the detector; for each of a plurality of retardation steps of the interferometer, capturing a series of discrete digital values corresponding to an analog signal output from the detector, the series of discrete values having a time dependence over a sampling interval, which time dependence includes a carrier component resulting from the modulation signal, extracting a modulation phase and modulation frequency of the carrier component from the series of discrete digital values, and using the modulation frequency and modulation phase extracted at that retardation step to demodulate the series of discrete digital values at that retardation step and provide at least one output value; assembling the output values from the plurality of retardation steps to provide an interferogram; and computing a spectrum based on the interferogram.

Claim 7

In a step-scanning Fourier transform spectrometer comprising an interferometer, a detector, and a digital processor, a digital method for generating spectral data from a sample, the method comprising: passing a beam of analytic radiation through the interferometer and the sample to the detector; using a modulation signal to subject the beam to a modulation at a modulation frequency prior to the beam encountering the detector; for each of a plurality of retardation steps of the interferometer, capturing a series of discrete digital values corresponding to an analog signal output from the detector, the series of discrete values having a time dependence over a sampling interval, which time dependence includes a carrier component resulting from the modulation signal, extracting a modulation phase and modulation frequency of the carrier component from the series of discrete digital values, and using the modulation frequency and modulation phase extracted at that retardation step to demodulate the series of discrete digital values at that retardation step and provide at least one output value; assembling the output values from the plurality of retardation steps to provide an interferogram; and computing a spectrum based on the interferogram.

Claim 8

The method of claim 5, wherein the modulation signal is driving an element in the spectrometer optical train that modulates the polarization of a beam incident on the detector.

Claim 9

The method of claim 5, and further comprising adding a signal at the modulation frequency to the analog signal output from the detector before capturing the series of discrete digital values.

Claim 10

In a step-scanning Fourier transform spectrometer comprising an interferometer, a detector, and a digital processor, a digital method for extracting a modulation phase and modulation frequency of a modulation signal, the method comprising: capturing a series of discrete digital values output from the detector, the series of discrete values having a time dependence over a sampling interval, which time dependence includes a component resulting from the modulation signal; using a nominal modulation signal at a nominal modulation frequency to process a first subset of the discrete values to determine a first phase error at a first particular point in the sampling interval; using the first phase error and the nominal modulation signal to generate a phase-shifted signal that is nominally in phase with the modulation signal at the first particular point in the sampling interval; using the phase-shifted signal to process a second subset of the discrete values to determine a second phase error at a second particular point in the sampling interval; and using the second phase error to modify the nominal modulation frequency to provide a first refined estimate of the modulation frequency.

Claim 11

In a step-scanning Fourier transform spectrometer comprising an interferometer, a detector, and a digital processor, a digital method for extracting a modulation phase and modulation frequency of a modulation signal, the method comprising: capturing a series of discrete digital values output from the detector, the series of discrete values having a time dependence over a sampling interval, which time dependence includes a component resulting from the modulation signal; using a nominal modulation signal at a nominal modulation frequency to process a first subset of the discrete values to determine a first phase error at a first particular point in the sampling interval; using the first phase error and the nominal modulation signal to generate a phase-shifted signal that is nominally in phase with the modulation signal at the first particular point in the sampling interval; using the phase-shifted signal to process a second subset of the discrete values to determine a second phase error at a second particular point in the sampling interval; and using the second phase error to modify the nominal modulation frequency to provide a first refined estimate of the modulation frequency.

Claim 12

The method of claim 8, and further comprising: using a signal at the first refined estimate of the modulation frequency to process the first subset of the discrete values to determine a first refined phase error; using the first refined phase error to generate a first refined phase-shifted signal; and using the first refined phase-shifted signal to process a subset of discrete values other than the first subset to determine a second refined phase error; and using the second refined phase error to modify the first refined modulation frequency to provide a second refined estimate of the modulation frequency.

Claim 13

In a step-scanning Fourier transform spectrometer comprising an interferometer, a detector, and a digital processor, a method for measuring a spectral response of a sample to multiple modulations, including a phase modulation, a polarization modulation, and a sample modulation, said method comprising: passing a beam of analytic radiation through the interferometer and the sample to the detector; using a phase modulation signal to subject the beam to a modulation at a known phase modulation frequency prior to the beam encountering the detector; using a sample modulation signal to subject the sample to a modulation at a known sample modulation frequency prior to the beam encountering the detector; using a polarization modulation signal to subject the beam to a modulation at a polarization modulation frequency prior to the beam encountering the detector; for each of a plurality of retardation steps of the interferometer, capturing a series of discrete digital values corresponding to an analog signal output from the detector, the series of discrete values having a time dependence over a sampling interval, which time dependence includes a carrier component resulting from the polarization modulation signal, extracting a polarization modulation phase and polarization modulation frequency of the carrier component from the series of discrete digital values, and using the known phase modulation frequency, the known sample modulation frequency, and the polarization modulation frequency and polarization modulation phase extracted at that retardation step to demodulate the series of discrete digital values at that retardation step and provide a set of output values; assembling the respective sets of output values from the plurality of retardation steps to provide a set of interferograms; and computing a set of spectra based on the interferograms.

Claim 14

In a step-scanning Fourier transform spectrometer comprising an interferometer, a detector, and a digital processor, a method for measuring a spectral response of a sample to multiple modulations, including a phase modulation, a polarization modulation, and a sample modulation, said method comprising: passing a beam of analytic radiation through the interferometer and the sample to the detector; using a phase modulation signal to subject the beam to a modulation at a known phase modulation frequency prior to the beam encountering the detector; using a sample modulation signal to subject the sample to a modulation at a known sample modulation frequency prior to the beam encountering the detector; using a polarization modulation signal to subject the beam to a modulation at a polarization modulation frequency prior to the beam encountering the detector; for each of a plurality of retardation steps of the interferometer, capturing a series of discrete digital values corresponding to an analog signal output from the detector, the series of discrete values having a time dependence over a sampling interval, which time dependence includes a carrier component resulting from the polarization modulation signal, extracting a polarization modulation phase and polarization modulation frequency of the carrier component from the series of discrete digital values, and using the known phase modulation frequency, the known sample modulation frequency, and the polarization modulation frequency and polarization modulation phase extracted at that retardation step to demodulate the series of discrete digital values at that retardation step and provide a set of output values; assembling the respective sets of output values from the plurality of retardation steps to provide a set of interferograms; and computing a set of spectra based on the interferograms.

Claim 15

The method of claim 10, wherein the modulation signal is driving an element in the spectrometer optical train that modulates the polarization of the beam incident on the detector.

Claim 16

The method of claim 10, and further comprising adding a signal at the polarization modulation frequency to the analog signal output from the detector before capturing the series of discrete digital values.

Claim 17

The method of claim 10, and further comprising correcting at least one of the sets of output values for a baseline component.

Claim 18

The method of claim 13, wherein the baseline component is determined by demodulating a set of discrete digital values at frequencies above and below the sample modulation frequency.

Claim 19

The method of claim 10, and further comprising calibrating the spectrometer by using a reference sample to determine a phase modulation rotation angle and a sample modulation rotation angle for use in demodulating the discrete digital values.