Diode laser based high spectral resolution lidar

Patent metadata

Field	Value
Publication number	US-10794998-B2
Application number	US-201615090063-A
Country	US
Kind code	B2
Filing date	Apr 4, 2016
Priority date	Jun 29, 2015
Publication date	Oct 6, 2020
Grant date	Oct 6, 2020

Abstract

Lidar is an acronym for Light Detection And Ranging. The technology may be used to measure distance by illuminating a target with a laser beam and performing analysis on the reflected laser beam light. In the atmospheric sciences, Lidar may be used to study the optical depth of clouds, the impact of aerosols on clouds, and the interactions between aerosols and clouds on the climate. The present application proposes a lidar-based technology using a diode laser (101) beam sent through a tapered semiconductor optical amplifier (106) and an axicon pair expander (108) wherein the laser light may be transmitted through a telescope (110) at an object to be studied. Upon striking the object to be studied, the laser (101) is reflected and recovered by the telescope (110). The reflected laser is then sent through a heated rubidium vapor cell (115) and a total detection channel (116) for analysis.

First claim

The invention claimed is:

1. A device comprising:
a laser ( 101 ) emitting a laser beam;
a first splitter ( 102 ) which separates the laser beam and generates a first portion of the separated laser beam and a second portion of the separated laser beam;
an amplifier which receives the first portion of the separated laser ( 101 ) beam and generates an amplified separated beam;
prisms ( 108 ) which receive and expand the amplified separated laser beam and generates an expanded amplified separated laser beam;
a telescope ( 110 ) which transmits the expanded amplified separated laser beam and receives a return signal;
a second splitter ( 114 ) which splits the return signal into a first return signal portion and a second return signal portion; and
a heated rubidium cell ( 115 ) which receives the second return signal portion and generates a molecular return signal,
wherein the first return signal portion comprises a total detection signal.

2. The device of claim 1 further comprising:
a mirror with a hole ( 121 ) which reflects the return signal from the telescope;
a filter ( 113 ) to receive and filter the return signal; and
an etalon for receiving and filtering the return signal.

3. The device of claim 2 wherein the telescope ( 110 ) comprises an inner portion that transmits the expanded amplified separated laser beam and an outer portion that receives the return signal.

4. The device of claim 2 , wherein the telescope further comprises an outer portion to receive the return signal, the filter ( 113 ) comprises an interference filter, and the device further comprises:
a total detection channel which receives the total detection signal and generates a total detection signal count; and
a molecular channel detector ( 116 ) which receives the molecular return signal and generates a molecular return signal count.

5. The device of claim 1 wherein the amplifier comprises a tapered semiconductor optical amplifier.

6. The device of claim 1 further comprising:
a depolarization channel ( 116 ) configured to analyze the first return signal portion.

7. The device of claim 1 , wherein the laser ( 101 ) comprises a diode laser, the amplifier comprises an inline fiber isolator and a tapered semiconductor optical amplifier, the prisms ( 108 ) further comprise at least one pair of axicon prisms which form the expanded amplified separated laser beam into an annular shape, and the telescope ( 110 ) contains an inner portion through which the laser beam is transmitted.

8. The device of claim 1 wherein the laser ( 101 ) uses at least one of a distributed Bragg reflector (DBR), or a distributed feedback (DFB) laser.

9. The device of claim 1 wherein the laser ( 101 ) has a wavelength of approximately 780 nanometers.

10. The device of claim 1 wherein second portion of the separated laser beam is directed to at least one of a wavelength meter or a device for monitoring and controlling the wavelength of the laser.

11. A method of analysis comprising:
generating a laser beam using a laser;
splitting the laser beam into a first portion of the separated laser beam and a second portion of the separated laser beam using a first splitter;
generating high energy pulses from the first portion of the laser beam using an amplifier which receives the first portion of the separated laser beam and generates an amplified separated beam;
expanding the first portion of the laser beam using prisms which receive and expand the amplified separated laser beam and generates an expanded amplified separated laser beam;
transmitting the expanded amplified separated laser beam using a telescope;
receiving a return signal via the telescope;
splitting the return signal into a first return signal portion and a second return signal portion using a second splitter; and
generating a molecular return signal from the second return signal portion using a heated rubidium cell,
wherein the first return signal portion comprises a total detection signal.

12. The method of claim 11 wherein the laser is at least one of a distributed Bragg reflector (DBR), or a distributed feedback (DFB) laser.

13. The method of claim 11 wherein the amplifier is a tapered semiconductor optical amplifier.

14. The method of claim 11 wherein the prisms comprise an axicon pair.

15. The method of claim 11 wherein the transmitting the expanded amplified separated laser beam comprises using an inter portion of the telescope.

16. The method of claim 11 further comprising:
receiving return signal via an outer portion of a telescope.

17. The method of claim 16 further comprising:
filtering the return signal via an interference filter and a narrow band etalon.

Assignees

• Univ Corporation For Atmospheric Research
• Wisconsin Alumni Res Found

Inventors

• Spuler Scott
• Hayman Matthew
• Morley Bruce
• Eloranta Edwin W

Classifications

• G01S7/4812

  transmitted and received beams following a coaxial path · CPC title

• G01S7/499

  using polarisation effects · CPC title

• G01S7/484

  Transmitters · CPC title

• H01S5/50

  Amplifier structures not provided for in groups H01S5/02 - H01S5/30 · CPC title

• G01S7/4816

  of receivers alone · CPC title