# US 11,029,261 B2 · Methods and apparatus for direct multiplication Fourier transform millimeter wave spectroscopy

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- Number: US 11,029,261 B2
- Document ID: US11029261B2
- Status: Granted
- Kind: B2
- Application number: 16/807,270
- Filed: 2020-03-03
- Published: 2020-07-02
- Granted: 2021-06-08
- Earliest claimed: 2016-01-07
- Assignees: BrightSpec, Inc.
- Applicants: BrightSpec, Inc.
- Inventors: Justin L. Neill; Brent Harris; Brooks Hart Pate
- Web page: https://patentgrep.com/patent/US11029261B2

## CPC

- G01N 22/00: Investigating or analysing materials by the use of microwaves or radio waves, i.e. electromagnetic waves with a wavelength of one millimetre or more (G01N3/00 - G01N17/00, G01N24/00 take precedence)
- G01J 3/42: Absorption spectrometry; Double beam spectrometry; Flicker spectrometry; Reflection spectrometry (beam switching arrangements G01J3/08)
- G01J 3/44: Raman spectrometry; Scattering spectrometry {; Fluorescence spectrometry}
- G01J 3/453: by correlation of the amplitudes
- G01N 21/636: {using an arrangement of pump beam and probe beam; using the measurement of optical non-linear properties; (non-linear optics per se G02F1/35)}
- G01N 21/3581: using far infrared light; using Terahertz radiation
- G01N 2021/3595: {using FTIR}
- G01N: INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES (measuring or testing apparatus or processes other than immunoassay, involving enzymes or microorganisms C12M, C12Q)
- G01J: MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY (light sources F21, H01J, H01K, H05B; investigating properties of materials by optical means G01N)

## Abstract

Methods and apparatuses for direct multiplication Fourier transform millimeter wave spectroscopy are disclosed herein. A sample method includes generating at least one pulse of microwave electromagnetic energy. The sample method also includes frequency-multiplying the pulse(s) to generate at least one frequency-multiplied pulse and filtering at least one spurious harmonic of the frequency-multiplied pulse to generate at least one filtered pulse. The spurious harmonic is generated by frequency-multiplying the pulse. The method also includes exciting a sample using the filtered pulse. The method further includes detecting an emission from the sample. The emission is elicited at least in part by the filtered pulse.

## Claims

### Claim 1

An apparatus, comprising:
a signal generator configured to generate at least one pulse of microwave electromagnetic energy in response to a trigger signal;
a frequency multiplier circuit coupled to the signal generator, the frequency multiplier circuit configured to frequency-multiply the at least one pulse to generate at least one frequency-multiplied pulse, the frequency multiplier circuit further configured to excite a sample using the at least one frequency-multiplied pulse; and
an emission detector configured to detect an emission from the sample, the emission elicited at least in part by the at least one frequency-multiplied pulse.

### Claim 2 (depends on 1)

The apparatus of claim 1, wherein the signal generator is further configured to generate the at least one pulse as at least one chirped pulse within a frequency range from about 1 GHz to about 3 GHz.

### Claim 3 (depends on 1)

The apparatus of claim 1, wherein the emission detector is further configured to detect the emission in response to the trigger signal.

### Claim 4 (depends on 1)

The apparatus of claim 1, wherein the at least one pulse comprises a first pulse,
wherein the signal generator is further configured to generate a second pulse of microwave electromagnetic energy, the second pulse in phase with the first pulse,
wherein the frequency multiplier circuit is further configured to frequency-multiply the second pulse generate a second frequency-multiplied pulse, and
wherein the emission detector is further configured to mix the second frequency-multiplied pulse and the emission to generate a downconverted emission signal within the bandwidth of an analog-to-digital converter (ADC).

### Claim 5 (depends on 1)

The apparatus of claim 1, wherein the emission detector is further configured to detect the emission via heterodyne detection.

### Claim 6 (depends on 1)

The apparatus of claim 1, wherein the signal generator comprises an internally derived timebase configured to generate the trigger signal.

### Claim 7 (depends on 1)

The apparatus of claim 1, wherein the emission detector is configured to detect the emission in response to the trigger signal.

### Claim 8 (depends on 1)

The apparatus of claim 1, wherein the signal generator is configured to receive the trigger signal from a variable frequency source external to the signal generator.

### Claim 9

A method comprising:
generating, with a free-running signal generator, a first microwave pulse and a second microwave pulse in response to a first trigger signal;
frequency-multiplying the first microwave pulse to form a first millimeter-wave signal, the first millimeter-wave signal including a first millimeter-wave pulse and a first spurious emission;
filtering the first spurious emission from the first millimeter-wave signal to yield the first millimeter-wave pulse;
frequency-multiplying the second microwave pulse to form a second millimeter-wave signal, the second millimeter-wave signal including a second millimeter-wave pulse and a second spurious emission;
filtering the second spurious emission from the first millimeter-wave signal to yield the first millimeter-wave pulse;
exciting a sample with the first millimeter-wave pulse to produce a first sample emission;
mixing the first sample emission with the second millimeter-wave pulse to produce a first downconverted sample emission;
detecting the first downconverted sample emission to produce a first electronic signal;
generating, with the free-running signal generator, a third microwave pulse and a fourth microwave pulse in response to a second trigger signal, the third microwave pulse and the fourth microwave pulse being phase-coherent with the first microwave pulse and the second microwave pulse;
frequency-multiplying the third microwave pulse to form a third millimeter-wave signal, the third millimeter-wave signal including a third millimeter-wave pulse and a third spurious emission;
filtering the third spurious emission from the third millimeter-wave signal to yield the third millimeter-wave pulse;
frequency-multiplying the fourth microwave pulse to form a fourth millimeter-wave signal, the fourth millimeter-wave signal including a fourth millimeter-wave pulse and a fourth spurious emission;
filtering the fourth spurious emission from the fourth millimeter-wave signal to yield the fourth millimeter-wave pulse;
exciting the sample with the third millimeter-wave pulse to produce a second sample emission, the second sample emission being phase-coherent with the first sample emission;
mixing the second sample emission with the fourth millimeter-wave pulse to produce a second downconverted sample emission;
detecting the second downconverted sample emission to produce a second electronic signal; and
averaging the first electronic signal and the second electronic signal.

### Claim 10 (depends on 9)

The method of claim 9, wherein the frequency of first millimeter-wave pulse is offset from the frequency of the second millimeter-wave pulse by from about 720 MHz to about 1440 MHz.
