We use cookies to distinguish you from other users and to provide you with a better experience on our websites. Close this message to accept cookies or find out how to manage your cookie settings.
To save content items to your account,
please confirm that you agree to abide by our usage policies.
If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account.
Find out more about saving content to .
To save content items to your Kindle, first ensure [email protected]
is added to your Approved Personal Document E-mail List under your Personal Document Settings
on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part
of your Kindle email address below.
Find out more about saving to your Kindle.
Note you can select to save to either the @free.kindle.com or @kindle.com variations.
‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi.
‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.
The photon signal-to-noise ratio (SNR) is defined in terms of statistical quantities, and the Poisson and Gaussian probability distribution functions are defined and described. Those distributions are applied to lidar measurements, and the effect of background light on lidar SNR is quantified. The signal-limited and background-limited SNR regimes are defined. The lidar equation is then introduced as a model of the range-dependent lidar signal, and the background model is a constant additional term. All the variables in both models are introduced and defined. They include the number of photons in each laser pulse, the optical efficiencies of the transmitter and receiver, the geometrical function, the receiver solid angle, the range bin length, the volume backscatter coefficient, the extinction coefficient, the spectral radiance of the background, the receiver field of view, the receiver optical bandpass, and the sampling interval of the data system. Finally, a lidar system known as the Eye safe Atmospheric Research Lidar (EARL) is introduced because it is used as an example throughout the rest of the book.
In Chapter 5, having introduced the physics behind light scattering, we present the lidar equation. This sets the stage for consideration and simulation of various types of lidar. These include the following broadband lidars: Rayleigh–Mie, polarization, vibrational Raman and fluorescence, and differential absorption. They also include high–spectral resolution (narrowband) lidars: Lidar ratio and aerosol properties, temperature profiling by integration Rayleigh+Raman, temperature profiling with rotational Raman and Cabannes scattering, Rayleigh–Mie wind profiling, and mesopause–region resonance fluorescence wind+temperature profiling.
Recommend this
Email your librarian or administrator to recommend adding this to your organisation's collection.