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// -->
Latest News for: specific detectivity
Edit
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Loading...');
var query = jQuery('.radio_query').val();
jQuery.ajax({
data: { query: query },
url: '/api/upge/cheetah-photo-search/radio',
success: function(text) {
jQuery('.radio-search-results').html(jQuery(text));
updateHeight();
$('#RadioSearchTable').tablesorter();
$('#RadioSearchTable').trigger("update");
}
});
return false; // do not submit the form
});
$(".search-tools-btn").click(function () {
header = $(this);
content = $(".search-tools-content");
if(content.is(':visible')) {
content.hide('slow');
header.html('Tools ');
}else{
content.show('slow');
header.html('Hide ');
}
});
});
, where 
is the area of the photosensitive region of the detector and 
is the frequency bandwidth. It is commonly expressed in Jones units (
)in honor of 
(in units of 
or 
) and the 
(in units of 
or 
) as 
, it's common to see the specific detectivity expressed as 
.![D^* = \frac{q\lambda \eta}{hc} \left[\frac{4kT}{R_0 A}+2q^2 \eta \Phi_b\right]^{-1/2}](http://assets.wn.com/wiki/en/6/2e/525927cbe77472820bc35-6509f6.png)
is the wavelength of interest, h is Planck's constant, c is the speed of light, k is Boltzmann's constant, T is the temperature of the detector, 
is the zero-bias dynamic resistance area product (often measured experimentally, but also expressible in noise level assumptions), 
is the quantum efficiency of the device, and 
is the total flux of the source (often a blackbody) in photons/sec/cm².
Fox31 Denver
12 Jan 2025
Fox31 Denver
12 Jan 2025