Single-line-extracted pure rotational Raman lidar to measure atmospheric temperature and aerosol profiles

Patent metadata

Field	Value
Publication number	US-10620318-B2
Application number	US-201715600780-A
Country	US
Kind code	B2
Filing date	May 21, 2017
Priority date	Jan 3, 2017
Publication date	Apr 14, 2020
Grant date	Apr 14, 2020

Abstract

A single-line-extracted pure rotational Raman lidar system, including: a transmitter unit configured to emit extremely narrow-band laser light that is guided into atmosphere zenithward; a receiver unit configured to collect backscattered signals from the atmosphere; and a data acquisition and control unit configured to deliver data and guarantee automatic operation of the lidar system orderly. The transmitter unit employs a powerful injection-seeded Nd: YAG laser to emit 532.23 nm laser beam with a pulse energy of approximately 800 mJ, a repetition rate of 30 Hz and linewidth of <0.006 cm −1 . The lidar system has an optical bandwidth of approximately 30 pm for the two Raman channels and an optical bandwidth of 0.3 nm for an elastic channel, as well as a field of view of approximately 0.4 mrad. The two Raman channels extract the N 2 anti-Stokes pure rotational Raman line signals with J=6 and 16, respectively.

First claim

The invention claimed is:

1. A single-line-extracted pure rotational Raman lidar system, comprising:
a transmitter unit, comprising an injection-seeded Nd: YAG laser to emit a laser beam that is guided into atmosphere zenithward;
a receiver unit, being configured to collect backscatter signals from molecules and aerosols in the atmosphere; the receiver unit comprising an elastic channel, a first Raman channel, and a second Raman channel; the first Raman channel comprising two first interference filters and a first Fabry-Perot interferometer; the second Raman channel comprising two second interference filters and a second Fabry-Perot interferometer; and the elastic channel comprising a third interference filter; and
a data acquisition and control unit, being configured to deliver data and guarantee automatic operation of the lidar system;

wherein:
the injection-seeded Nd: YAG laser is adapted to emit a 532.23 nm laser beam with a pulse energy of 800 mJ, a repetition rate of 30 Hz and linewidth of <0.006 cm −1 ;
the first Raman channel is disposed downstream the second Raman channel, and the second Raman channel is disposed downstream the elastic channel;
the first Fabry-Perot interferometer is disposed downstream the two first interference filters, and the second Fabry-Perot interferometer is disposed downstream the two second interference filters;
the third interference filter has a center wavelength of 532.23 nm, and has a bandwidth of 0.3 nm at the center wavelength of 532.23 nm;
each of the two second interference filters has a center wavelength of 531.00 nm, and has a bandwidth of 0.3 nm at the center wavelength of 531.00 nm;
each of the two first interference filters has a center wavelength of 528.77 nm, and has a bandwidth of 0.3 nm at the center wavelength of 528.77 nm;
each of the first and second Fabry-Perot interferometers has a bandwidth of 30 μm;
the elastic channel is adapted to extract an elastic signal of 532.23 nm;
the second Raman channel is adapted to extract a signal having a single anti-Stokes pure rotational Raman line from N 2 molecules with J=6, and the first Raman channel is adapted to extract a signal having a single anti-Stokes pure rotational Raman line from N 2 molecules with J=16; and each of the first and second Raman channels provides a suppression of >8 orders of magnitude to the elastic signal of 532.23 nm, as well as a suppression of >1.5 orders of magnitude to adjacent O 2 molecule lines; and
the receiver unit has a field of view of 0.4 mrad.

2. The system of claim 1 , wherein the transmitter unit comprises a seeder, an optical fiber, the injection-seeded Nd: YAG laser, a beam expander, and a first reflecting mirror; the seeder is adapted to generate an infrared 1064 nm fundamental laser light; the optical fiber is adapted to guide the 1064 nm light into the injection-seeded Nd: YAG laser; the beam expander is adapted to compress a beam divergence by a factor of 8 and reduce a radiant flux density of the laser beam from the injection-seeded Nd: YAG laser to yield an expanded laser beam; the first reflecting mirror is adapted to reflect the expanded laser beam into atmosphere zenithward with a reflectivity of >99.5%.

3. The system of claim 2 , wherein:
the receiver unit comprises a telescope, an iris, a second reflecting mirror, a collimator, a first beam splitter, the third interference filter, a third lens, a third detector, a second beam splitter, the two second interference filters, the second Fabry-Perot interferometer, a second lens, a second detector, the two first interference filters, the first Fabry-Perot interferometer, a first lens, and a first detector;
the telescope is adapted to transmit the backscatter signals through the iris to the second reflecting mirror, the second reflecting mirror is adapted to reflect the backscatter signals to the collimator; and the collimator is adapted to collimate the backscatter signals to yield a collimated light beam;
the iris is located on a focal plane of the telescope, and a diameter of the iris is 0.8 mm;
the first beam splitter is adapted to reflect the collimated light beam with a reflectivity of 10% onto the third interference filter, and transmit the collimated light beam with a transmittance of 90% onto the second beam splitter;
the third lens is adapted to focus a beam from the third interference filter, and the third detector is adapted to detect a beam from the third lens;
the second beam splitter is adapted to reflect and transmit an incoming collimated light beam with a reflectivity to transmittance (R-to-T) ratio of 1:1;
the two second interference filters and the second Fabry-Perot interferometer are adapted to extract the signal having the single anti-Stokes pure rotational Raman line from N 2 molecules with J=6 from a reflected light beam from the second beam splitter;
the two first interference filters and the first Fabry-Perot interferometer are adapted to extract the signal having the single anti-Stokes pure rotational Raman line from N 2 molecules with J=16 from a transmitted light beam from the second beam splitter;
the second lens is adapted to focus the signal having the single anti-Stokes pure rotational Raman line from N 2 molecules with J=6, and the second detector is adapted to detect the signal having the single anti-Stokes pure rotational Raman line from N 2 molecules with J=6; and
the first lens is adapted to focus the signal having the single anti-Stokes pure rotational Raman line from N 2 molecules with J=16, and the first detector is adapted to detect the signal having the single anti-Stokes pure rotational Raman line from N 2 molecules with J=16.

4. The system of claim 3 , wherein the data acquisition and control unit comprises a computer that stores acquired data and controls the operation of the lidar system.

5. The system of claim 4 , wherein:
the third interference filter has a peak transmission of >50% at the center wavelength of 532.23 nm, as well as a suppression of >3 orders of magnitude to signals out of a transmission band of the third interference filter;
the second interference filter has a peak transmission of >50% at the center wavelength of 531.00 nm, as well as a suppression of >3 orders of magnitude to signals including the elastic signal of 532.23 nm that are out of a transmission band of the second interference filter;
the first interference filter has a bandwidth of 0.3 nm and a peak transmission of >35% at the center wavelength of 528.77 nm, as well as a suppression of >3 orders of magnitude to signals including the elastic signal of 532.23 nm that are out of a transmission band of the first interference filter;
both the first and second Fabry-Perot interferometers have an aperture of 50 mm, an air spacing of 0.189 mm, a cavity surface reflectivity of 90%, a fineness of 23 and free a free spectral range of 0.75 nm;
a working temperature for each of the first and second Fabry-Perot interferometers is controlled with a temperature controlling precision of smaller than 0.1° C.;
a working angle for each of the first and second Fabry-Perot interferometers is controlled with a step value of <1.25×10 −3 degree;
the second Fabry-Perot interferometer has a peak transmission of 30% at the center wavelength of 531.00 nm and a suppression of >2 orders of magnitude to the elastic signal of 532.23 nm, as well as a suppression of >1.5 orders of magnitude to both a 531.18 nm signal corresponding to the O 2 molecule J=7 line and a 530.85 nm signal corresponding to the O 2 molecule J=9 line, while and the first Fabry-Perot interferometer has a peak transmission of 30% at the center wavelength of 528.77 nm, a suppression of >2 orders of magnitude to the elastic signal of 532.23 nm, as well as a suppression of >1.5 orders of magnitude to a 528.91 nm sign

Assignees

• Univ Wuhan

Inventors

• Yi Fan
• Weng miao
• Liu Fuchao
• Zhang Yunpeng
• Yu Changming
• He Yujin
• Tan Ying
• Yi Yang
• Pan Xiangliang

Classifications

• G01S7/484

  Transmitters · CPC title

• G01S7/4861

  Circuits for detection, sampling, integration or read-out · CPC title

• G01S17/95 Primary

  for meteorological use · CPC title

• Y02A90/19

  Cross-Sectional Technologies · mapped topic

• Y02A90/10

  Information and communication technologies [ICT] supporting adaptation to climate change, e.g. for weather forecasting or climate simulation · CPC title