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This tutorial visualizes the push-pull of electrons and holes at a PN junction and how applied voltage changes the depletion region and energy bands. You see the physical picture (carriers and lattice) and the band diagram in one view.
Mathematical foundation1. PN junction In N-type silicon, majority carriers are electrons (blue dots). In P-type, majority carriers are holes (red circles). At the junction, electrons diffuse into the P side and recombine with holes, leaving a depletion region with few free carriers and a built-in potential Vbi (about 0.7 V for Si). 2. Bias and depletion width Forward bias (V > 0) reduces the barrier: the depletion region shrinks, carriers cross and recombine, and current flows. Reverse bias (V < 0) increases the barrier: the depletion region widens, carriers are pulled away from the junction, and only a tiny saturation current flows. 3. Energy bands The conduction band Ec and valence band Ev bend near the junction. The offset between P and N sides is q Vbi. With forward bias the "hill" flattens; with reverse bias it becomes a steep cliff. 4. Diode equation The current is I = Is (eqV/(n k T) − 1). Forward: I grows exponentially with V. Reverse: I ≈ −Is. The I–V graph in the separate canvas below shows this curve and the operating point as you move the voltage slider.
1.60 V
0.40 Hz
Forward: carriers cross and recombine. Reverse: depletion widens, little current.
I–V curve
Input (V) and output (I) vs time
UsageFollow these steps to explore the diode mechanism:
Tips: Set voltage to 0 to see zero bias (moderate depletion, small barrier). Then move to +1 V or +2 V to see strong forward behavior (recombination, flat bands). Then move to −2 V or −3 V to see reverse (wide depletion, steep bands, almost no current). Parameters
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