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principles and applications of microearthquake networks

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34 2. Instrumentation Systems<br />

1 0 7 ~ I I I 1 I I I I I I I I\ I 1 I I<br />

i<br />

I I l l I I I / I I I l l I I I I<br />

0.01 0.1 1 10 100<br />

FREQUENCY (Hz)<br />

Fig. 13. Smoothed amplitude response <strong>of</strong> the seismic system used in the USGS Central<br />

California Microearthquake Network as determined by Bakun <strong>and</strong> Dratler ( 1976) using a<br />

Fourier transform technique.<br />

vidual components as well) could be adequately approximated by<br />

where w is the frequency in radians per second, al are the poles <strong>of</strong> the<br />

function F(w), Cj are real constants associated with each pole, 1 is the<br />

power <strong>of</strong> the low-frequency roll-<strong>of</strong>f, n - 1 is the power <strong>of</strong> the highfrequency<br />

roll-<strong>of</strong>f in the amplitude response, <strong>and</strong> Aj are amplitude factors<br />

representing the sensitivity or gain <strong>of</strong> individual components within the<br />

system.<br />

Because the physical system represented by F( w) is real <strong>and</strong> causal, all<br />

the poles lie in the upper half <strong>of</strong> the complex plane. They are located<br />

either on the imaginary axis or <strong>of</strong>f the axis as matched pairs (i,e,, mirror<br />

images through the imaginary axis). Those that lie on the imaginary axis<br />

are single poles <strong>and</strong> have the form -aj/( w - aj), or the form w/( w - af),<br />

where aj = iwo, <strong>and</strong> wo is the frequency in radians per second. Those poles<br />

that occur as matched pairs are double poles <strong>and</strong> have the form aJaL/( w -<br />

cq)(w - ak) or w2/(o - q )(w- ak), where

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