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Characterization of HgCdTe MWIR Back-Illuminated II-VI-07 ... - Voxtel

Characterization of HgCdTe MWIR Back-Illuminated II-VI-07 ... - Voxtel

Characterization of HgCdTe MWIR Back-Illuminated II-VI-07 ... - Voxtel

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1E-7<br />

10000<br />

Relative Response<br />

1E-8<br />

1E-9<br />

1E-10<br />

V = -5 V<br />

V = 0<br />

Gain, avg = 10.8<br />

163-A1, El 56<br />

λ CO =4.24 µm at 80 K<br />

T=79 K<br />

With filter 1000<br />

FWHM:<br />

210.97 µm at 0 V<br />

214.73 µm at -5 V<br />

∆=3.76 µm<br />

100<br />

10<br />

Ratio<br />

1E-11<br />

1<br />

-250 -200 -150 -100 -50 0 50 100 150 200 250<br />

Distance (µm)<br />

Fig. 9. Spot scan pr<strong>of</strong>iles for a 250×250 µm² unit cell in a 4×4 e-APD array at 79 K, for V=0 and V=-5.0 V.<br />

The ratio <strong>of</strong> the -5.0 V data to the V=0 data is defined as the gain, and is plotted on the right-hand axis. The<br />

gain is spatially uniform in the interior <strong>of</strong> the diode, with an average value <strong>of</strong> 10.8 at -5.0 V. There is<br />

evidence <strong>of</strong> gain enhancement seen at the edges <strong>of</strong> the junction.<br />

5<br />

4<br />

3<br />

163A1, El 80<br />

λ CO =4.06 µm at 160 K<br />

250x250 µm²<br />

T = 196 K<br />

V = -0.1 V to -9.0 V<br />

<strong>Voxtel</strong> data<br />

k=0<br />

k=0.025<br />

El 80<br />

F(M)<br />

2<br />

1<br />

F(M) normailzed to 1 at V=-0.1 V<br />

0<br />

0 20 40 60 80 100 120 140 160<br />

Gain<br />

Fig. 10. Data for the excess noise multiplication factor F(M) plotted versus gain, at T=196 K, taken at <strong>Voxtel</strong><br />

Inc. The two solid curves are plots <strong>of</strong> the standard McIntyre equation for F(M).<br />

-27-

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