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CHAPTER 3. BIFURCATION ANALYSIS 64<br />

GMRES was able to more efficiently solve the linear systems in the Householder<br />

continuation than in the bordering method.<br />

3.9 Results<br />

Once the simulator was connected with LOCA, the first thing we wanted to do was<br />

analyze the original grid Nx = 86, Nk = 72 that our project’s physicists and engi-<br />

neers had used in reporting results to the scientific community. These results [8],<br />

[40] reported hystersis in the current-voltage (I-V) curves and current oscillation for<br />

some values of applied bias. Figure 3.6 shows a forward sweep in bias from V =0to<br />

V =0.480, with increments of 0.08 taken in bias. As you can see, the I-V curve drops<br />

suddenly at 0.318 volts to a lower curve and continues on. In the reverse bias case,<br />

wherewestartatV =0.480 and reduce by 0.08 volts to V = 0, the I-V curve follows<br />

out this lower branch, but does not jump up at 0.318 volts. Instead, it continues along<br />

this lower curve, until it jumps back up to the upper curve at 0.256 volts. Figure 3.7<br />

shows the window of voltage that creates current oscillation within the device. We<br />

can see the oscillation onsets between 0.240 volts and 0.248 volts and turns off again<br />

between 0.256 volts and 0.264 volts.<br />

Using LOCA’s pseudo arc-length continuation algorithm and eigensolver, we were<br />

able to explain why these phenomena occur. Figure 3.8 shows the I-V curve generated<br />

by LOCA. LOCA has found two turning points: one at 0.256 volts and one at 0.318<br />

volts. The branch connecting the two is an unstable steady-state solution branch,

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