Method and apparatus for reducing fringe interference in laser spectroscopy

Claim 3

The method according to claim 1 further comprising the step of determining the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal; wherein the predetermined peak-to-peak amplitude of the triangular waveform is selected to generate a frequency swing of the laser beam substantially equal to (n+1/2) times the free spectral range frequency of the interference fringe when the difference between the free spectral range of the interference fringe and the absorption induced signal linewidth is about one order of magnitude or less; and wherein n is a positive integer.

Claim 4

The method according to claim 2 wherein the step of demodulating the signal received at the optical detector comprises the step of demodulating the signal at an odd harmonic of the second predetermined frequency of the triangular waveform.

Claim 5

The method according to claim 1 further comprising the step of determining the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal; and wherein the predetermined peak-to-peak amplitude of the triangular waveform is selected to generate a predetermined frequency swing of the laser beam substantially equal to a positive integer times the free spectral range frequency of the interference fringe when the difference between the free spectral range of the interference fringe and the absorption induced signal linewidth is about one order of magnitude or less.

Claim 6

The method according to claim 4 wherein the step of demodulating the signal received at the optical detector comprises the step of demodulating the signal at an even harmonic of the second predetermined frequency of the triangular waveform.

Claim 7

The method according to claim 1 wherein the predetermined peak-to-peak amplitude of the triangular waveform is selected to produce a frequency swing of the laser beam to maximize the absorption induced signal.

Claim 8

The method according to claim 6 further comprising the step of determining the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal; and wherein the step of demodulating the signal received by the optical detector comprises the step of demodulating the signal at the second harmonic or a higher harmonic of the second predetermined frequency of the triangular waveform when the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal is in the range of about one order of magnitude to two orders of magnitude.

Claim 11

The method according to claim 8 further comprising the step of determining the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal; wherein the predetermined peak-to-peak amplitude of the triangular waveform is selected to generate a frequency swing of the laser beam substantially equal to (n+1/2) times the free spectral range frequency of the interference fringe when the difference between the free spectral range of the interference fringe and the absorption induced signal linewidth is about one order of magnitude or less; and wherein n is a positive integer.

Claim 12

The method according to claim 9 wherein the step of demodulating the signal received at the optical detector comprises the step of demodulating the signal at an odd harmonic of the second predetermined frequency of the triangular waveform.

Claim 13

The method according to claim 8 further comprising the step of determining the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal; and wherein the predetermined peak-to-peak amplitude of the triangular waveform is selected to generate a predetermined frequency swing of the laser beam substantially equal to a positive integer times the free spectral range frequency of the interference fringe when the difference between the free spectral range of the interference fringe and the absorption induced signal linewidth is about one order of magnitude or less.

Claim 14

The method according to claim 11 wherein the step of demodulating the signal received at the optical detector comprises the step of demodulating the signal at an even harmonic of the second predetermined frequency of the triangular waveform.

Claim 15

The method according to claim 8 wherein the predetermined peak-to-peak amplitude of the triangular waveform is selected to produce a frequency swing of the laser beam to maximize the absorption induced signal.

Claim 16

The method according to claim 13 further comprising the step of determining the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal; and wherein the step of demodulating the signal received by the optical detector comprises the step of demodulating the signal at the second harmonic or a higher harmonic of the second predetermined frequency of the triangular waveform when the difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal is in the range of about one order of magnitude to two orders of magnitude.

Claim 17

A laser spectrometer for detecting and absorption induced signal from a sample, said spectrometer comprising: a frequency tunable laser for generating a laser beam; an optical detector positioned in the optical path of the laser beam; a cell for containing a sample, said cell positioned in the optical path of the laser beam between said frequency tunable laser and said optical detector; a modulator coupled to said frequency tunable laser for modulating same at a first predetermined frequency and having the undesired effect of generating a periodic fringe near an absorption induced signal; a triangular waveform generator cooperating with said modulator for further modulating said frequency tunable laser with a triangular waveform having a predetermined peak-to-peak amplitude and a second predetermined frequency different from said first predetermined frequency, said predetermined peak-to-peak amplitude of said triangular waveform producing a frequency swing of said laser beam so as to generate from the periodic interference fringe a signal having reduced components near the absorption induced signal of the sample; and a demodulator coupled to said optical detector for obtaining the absorption induced signal, said demodulator including a lock-in amplifier tuned to a predetermined harmonic of said second predetermined frequency of said triangular waveform.

Claim 18

A laser spectrometer for detecting and absorption induced signal from a sample, said spectrometer comprising: a frequency tunable laser for generating a laser beam; an optical detector positioned in the optical path of the laser beam; a cell for containing a sample, said cell positioned in the optical path of the laser beam between said frequency tunable laser and said optical detector; a modulator coupled to said frequency tunable laser for modulating same at a first predetermined frequency and having the undesired effect of generating a periodic fringe near an absorption induced signal; a triangular waveform generator cooperating with said modulator for further modulating said frequency tunable laser with a triangular waveform having a predetermined peak-to-peak amplitude and a second predetermined frequency different from said first predetermined frequency, said predetermined peak-to-peak amplitude of said triangular waveform producing a frequency swing of said laser beam so as to generate from the periodic interference fringe a signal having reduced components near the absorption induced signal of the sample; and a demodulator coupled to said optical detector for obtaining the absorption induced signal, said demodulator including a lock-in amplifier tuned to a predetermined harmonic of said second predetermined frequency of said triangular waveform.

Claim 19

The laser spectrometer according to claim 15 wherein said triangular waveform generator includes means for generating a predetermined peak-to-peak amplitude of said triangular waveform so as to produce a frequency swing of the laser beam substantially equal to (n+1/2) times the free spectral range frequency of the periodic interference fringe; wherein n is a positive integer; and wherein said lock-in amplifier is tuned to an odd harmonic of the second predetermined frequency of said triangular waveform.

Claim 20

The laser spectrometer according to claim 15 wherein said triangular waveform generator includes means for generating a predetermined peak-to-peak amplitude of said triangular waveform so as to produce a frequency swing of said laser beam substantially equal to a positive integer times the free spectral range frequency of the periodic interference fringe; and wherein said demodulator includes a lock-in amplifier tuned to an even harmonic of the second predetermined frequency of said triangular waveform.

Claim 21

The laser spectrometer according to claim 15 wherein said triangular waveform generator includes means for generating a predetermined peak-to-peak amplitude of said triangular waveform so as to maximize the absorption induced signal.

Claim 22

The laser spectrometer according to claim 18 wherein said lock-in amplifier is tuned to the second harmonic or a higher harmonic of the second predetermined frequency of the triangular waveform when a difference between the free spectral range of the interference fringe and the spectral linewidth of the absorption induced signal is in the range of about one order of magnitude to two orders of magnitude.

Claim 23

The laser spectrometer according to claim 15 further comprising a controller cooperating with said modulator for slowly sweeping the first predetermined frequency of said laser beam over a range to obtain a spectrum including the absorption induced signal.