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12 April 2007 Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere Jonathan Friedman Arecibo Observatory Seminar 12 April 2007

Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

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Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere. Jonathan Friedman Arecibo Observatory Seminar 12 April 2007. Outline. Atmospheric Structure Lidar Technique Light Scattering From photons to state parameters Transmitter - PowerPoint PPT Presentation

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Page 1: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Lidar Measurements of Atmospheric State Parameters in the

Mesosphere and Lower ThermosphereJonathan Friedman

Arecibo Observatory Seminar

12 April 2007

Page 2: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Outline• Atmospheric Structure• Lidar Technique

– Light Scattering– From photons to state parameters– Transmitter– Receiver (broadband/narrowband)

• Results– Ion-neutral interactions … sporadic layers

– Mesospheric chemistry– MLT temperature measurements & solar influence

Page 3: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Atmospheric Structure

Page 4: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Light Scattering

Page 5: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

N(z) = ηTA2( )PLτhc λ

⎝ ⎜

⎠ ⎟σ eff n z( )Δz( )

A R

4πz 2

⎛ ⎝ ⎜

⎞ ⎠ ⎟+ NBRτ( )

Total Receiver Efficiency No. of

transmitted photons

# of photons scattered from the atmosphere

Probability that a scattered photon will be collected by the telescope

Total Background photons

Lidar Equation

Page 6: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

BlockingDetector

RayleighScatter Resonance

Scatter

30 second average in 150 m bins

Example of lidar data

Page 7: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Rayleigh Temperatures in the upper stratosphere and

mesosphere

AssumptionsThe atmosphere is an ideal gasIn hydrostatic equilibrium

Assuming a starting temperature, T(z1), integrate downward

Page 8: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

– Resonance Technique : Laser is tuned to the resonance wavelength of the atoms to be studied.

– There is no signal if the laser is not on resonance with the target atoms. This allows us to map out the Doppler structure of the mesospheric metal atoms, both in terms of width (temperature) and shift (wind).

– We know with fairly high accuracy, << 10 MHz in 400 THz, where in the spectrum the excitation laser is. 10 MHz is roughly equivalent to 7 m/s wind error and 1 K temperature error.

Resonance Technique

Page 9: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Transmitter & Receiver

Page 10: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Daytime Receiver

Typical filter 1/2 width~ 1 nm.

1 pm 10 pm 100 pm 1 nm

100%

75%

25%

50%

0%

Faraday Filter 1/2 width 1–10 pm

Page 11: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Some Results1. Summary of some past results

• Sporadic layers• Metal layer seasonal structures• Metal layer and meteors• Temperatures, inversion layers, and Gravity

Wave events2. Recent scientific results on the seasonal

thermal structure of the mesopause over Arecibo and its place in the global picture.

Page 12: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Sporadic layer event during the 1998 Coquí II sounding

rocket campaign

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Page 13: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Tepley et al., 2003

Page 14: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

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Metal Layer Topside

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Page 15: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Temperatures and gravity waves

Page 16: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Seasonal Climatology and how the mesopause above Arecibo fits into the

global picture

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Page 17: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

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78°N, SpitsbergenHöffner, 2006

Latitude Comparison

35°N, Albuquerque, NM (Starfire)Chu et al., 2005

18°N, Arecibo, PRFriedman and Chu, 2007

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21°N, Maui, HIFriedman and Chu, 2006

Page 18: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Radiative vs. Dynamic Heating/Cooling

• Radiative balance & upper mesosphere temperatures:

- Coldest place on earth winter polar mesopause- Warmest mesopause summer pole- Tropical mesopause nearly isothermal

• In fact:- Coldest place on earth summer polar mesopause

Under constant sunlight!- Warmest mesopause equinox- Tropical mesopause structured and dynamic

• Does not explain the summer cold tropical lower thermosphere

Page 19: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

12-tidal oscillationsa work in progress

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12 April 2007

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January Analysis

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Page 21: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

12-h tide at 95 km

Dusk

Dawn

Midnight

Page 22: Lidar Measurements of Atmospheric State Parameters in the Mesosphere and Lower Thermosphere

12 April 2007

Summary• Lidar allows us to make remote measurements of the “ignorosphere” with high time and range resolution.

• Takes advantage of a high-intensity coherent source and an inefficient but reliable tracer to probe atmospheric state parameters.

• Allows us to study a variety of phenomena in the middle atmosphere.