IP Library Granted Patent US 11,824,497
Granted Patent B2
US 11,824,497 · App. 18/052,751 · Granted Nov 21, 2023

Microwave photoconductance spectrometer and methods of using the same

Inventors: Bryon William Larson (Golden, CO); Obadiah G. Reid (Ft. Collins, CO)
Assignees: Alliance for Sustainable Energy, LLC; The Regents of the University of Colorado
H02S50/10G01R31/2656
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Quick Facts
Patent No.
US 11,824,497
App. No.
18/052,751
Granted
Nov 21, 2023
Kind
B2
Abstract

A steady-state microwave conductivity method whereby a light beam is modulated to form an amplitude modulated light having a modulation frequency ω 1 . The method further includes producing a microwave waveform, exposing a sample to the amplitude modulated light and a first portion of the microwave waveform to produce an amplitude modulation signal on the first portion of the microwave waveform, and mixing a second portion of the microwave waveform and the amplitude modulation signal to produce a first signal and a second signal.

Claims (59)

1. A steady-state microwave conductivity method comprising:

modulating a light beam to form a modulated light having a modulation frequency ω 1 ;

producing a microwave waveform;

exposing a sample to the modulated light and a first portion of the microwave waveform to produce an amplitude modulated waveform;

mixing a second portion of the microwave waveform and the amplitude modulated waveform to produce at least one of a first signal or a second signal; and

creating a frequency-filtered difference signal based on ω 1 , wherein:

the first signal is produced from constructive interference of the amplitude modulated waveform with the second portion of the microwave waveform,

the second signal is produced from destructive interference of the amplitude modulated waveform with the second portion of the microwave waveform,

the frequency-filtered difference signal is calculated from at least one of subtracting the first signal from the second signal or measuring a difference signal resulting from the destructive interference, and

the frequency-filtered difference signal represents a photoconductivity parameter of the sample.

2. The steady-state microwave conductivity method of claim 1 , further comprising producing the light beam using a light source comprising at least one of a xenon arc lamp, a supercontinuum laser, or a light emitting diode.

3. The steady-state microwave conductivity method of claim 2 , further comprising:

filtering the light beam produced by the light source to create a filtered light, wherein:

the light beam produced by the light source has a first bandwidth, and

the filtered light has a second bandwidth that is narrower than the first bandwidth.

4. The steady-state microwave conductivity method of claim 3 , further comprising chopping the filtered light to create the modulated light.

5. The steady-state microwave conductivity method of claim 1 , wherein the exposing comprises placing the sample in a microwave resonator.

6. The steady-state microwave conductivity method of claim 1 , wherein the exposing comprises:

impinging the microwave waveform onto the sample using a first antenna; and

receiving the amplitude modulated waveform using a second antenna, wherein:

the first antenna may be the same as the second antenna or the first antenna may be an antenna distinct from the first antenna.

7. The steady-state microwave conductivity method of claim 1 , further comprising:

splitting the modulated light into a first portion and a second portion;

directing the first portion of the modulated light to a reference photodiode; and

directing the second portion of the modulated light to the sample, wherein:

the first portion of the modulated light is between 5% and 15% of the modulated light, and

the reference photodiode produces a frequency reference signal proportional to ω 1 .

8. The steady-state microwave conductivity method of claim 1 , further comprising:

splitting the microwave waveform into the first portion of the microwave waveform and the second portion of the microwave waveform;

directing the first portion of the microwave waveform to the sample; and

directing the second portion of the microwave waveform to the mixing.

9. The steady-state microwave conductivity method of claim 8 , further comprising, after producing the microwave waveform and before the mixing, shifting the second portion of the microwave waveform between zero degrees and 180 degrees.

10. The steady-state microwave conductivity method of claim 1 , further comprising:

producing the microwave waveform using a microwave source; and

modulating the microwave waveform at the microwave source to a separate frequency ω 2 , wherein the photoconductivity parameter is determined by at least one of the difference of ω 1 and ω 2 or the sum of ω 1 and ω 2 .

11. The steady-state microwave conductivity method of claim 1 , further comprising calculating the photoconductivity parameter as a photoconductance ΔG.

12. The steady-state microwave conductivity method of claim 11 , wherein the calculating comprises:

Δ

G

=

-

1

K

Δ

P

P

,

where K is a sensitivity factor of a microwave resonator or an antenna,

ΔP is a first microwave power reflected from at least one of the sample, the microwave resonator, or the antenna, and

P is a second microwave power reflected from at least one of the sample, the microwave resonator, or the antenna.

13. The steady-state microwave conductivity method of claim 11 , wherein the calculating comprises plotting ΔG versus a wavelength of the modulated light.

14. The steady-state microwave conductivity method of claim 1 , wherein the microwave waveform has a frequency between about 1 GHz and about 100 GHz.

15. The steady-state microwave conductivity method of claim 1 , wherein the microwave waveform has a frequency between about 8.2 GHz and about 12.4 GHz.

16. The steady-state microwave conductivity method of claim 1 , further comprising, after producing the microwave waveform rotating a polarization axis of the first portion of the microwave waveform by 90 degrees.

17. The steady-state microwave conductivity method of claim 1 , further comprising, prior to the exposing and the mixing, splitting the microwave wave form into the first portion and the second portion, wherein after the splitting, neither the first portion or the second portion are amplified prior to the exposing and mixing.

18. The steady-state microwave conductivity method of claim 1 , wherein the sample comprises a thin film comprising at least one of a perovskite, an OPV, a CIGS, or CdTe.

Assignments (3)
CHANGE OF NAME Recorded Dec 16, 2025
From: ALLIANCE FOR SUSTAINABLE ENERGY, LLC
To: ALLIANCE FOR ENERGY INNOVATION, LLC
Reel/Frame 073993/0276 →
CONFIRMATORY LICENSE Recorded Jun 5, 2023
From: NATIONAL RENEWABLE ENERGY LABORATORY
To: UNITED STATES DEPARTMENT OF ENERGY
Reel/Frame 063853/0508 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Nov 4, 2022
From: LARSON, BRYON WILLIAM
To: ALLIANCE FOR SUSTAINABLE ENERGY, LLC
Reel/Frame 061660/0894 →
Continuity (3)
Continuation 17047721
Provisional Application 62664498 · Apr 30, 2018
Related Publication 20230070273A1 · Mar 9, 2023