Audit a supplied bandgap detector without claiming a real device
In a semiconductor, electronic states form bands rather than only isolated-atom lines. A valence-to-conduction transition leaves both an electron and an unoccupied valence state called a hole. A band gap is an energy separation, not a physical empty layer between two pieces of material. Doping changes available levels and carrier populations; it does not mean every photon is collected or that a material has one universal efficiency independent of wavelength and temperature.
Learning outcome: Compare equal, below and above-gap photons, then hold photon energy fixed while changing gap. Retain photon rate, current and selected energy shares separately. Explain why no full electrical output efficiency follows.
Starting recap
Separate per-event energy, expectation rate and measurement indication. Check particle identities, conservation, threshold branches and calibration roles before making a source or detector claim.
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At gap 1.5 eV and photons2 eV, collected current is0.6×1/2=0.3 nA. The selected branch receives0.6 nW; pair-creation energy rate is0.45 nW and excess thermalization0.15 nW. Their sum is0.6 nW, not the total incident1 nW.
Open the experimentPredict
In this supplied model, one collected electron-hole pair contributes to external current with charge magnitude:
Experiment
Compare equal, below and above-gap photons, then hold photon energy fixed while changing gap. Retain photon rate, current and selected energy shares separately. Explain why no full electrical output efficiency follows.
Audit a supplied photon-to-carrier energy budget
Worked teaching model · synthetic values · Supplied ideal threshold detector at incident power 1 nW, external collected-pair yield 0.6 only strictly above the gap. Exact equality is an energetic threshold with no finite-yield prediction. Pair creation energy and excess thermalization are tracked for the collected branch only; no complete device efficiency or actual material performance claim.
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An energy gap is not a complete spectral response
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: sampled supplied response; no interpolation across the ideal threshold (open markers). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for An energy gap is not a complete spectral response
sampled supplied response; no interpolation across the ideal threshold
| photon energy (eV) | collected current under stipulated yield (nA) |
|---|---|
| 1 | 0 |
| 1.025 | 0 |
| 1.05 | 0 |
| 1.075 | 0 |
| 1.1 | 0 |
| 1.125 | 0 |
| 1.15 | 0 |
| 1.175 | 0 |
| 1.2 | 0 |
| 1.225 | 0 |
| 1.25 | 0 |
| 1.275 | 0 |
| 1.3 | 0 |
| 1.325 | 0 |
| 1.35 | 0 |
| 1.375 | 0 |
| 1.4 | 0 |
| 1.425 | 0 |
| 1.45 | 0 |
| 1.475 | 0 |
| 1.5 | 0 |
| 1.525 | 0.393443 |
| 1.55 | 0.387097 |
| 1.575 | 0.380952 |
| 1.6 | 0.375 |
| 1.625 | 0.369231 |
| 1.65 | 0.363636 |
| 1.675 | 0.358209 |
| 1.7 | 0.352941 |
| 1.725 | 0.347826 |
| 1.75 | 0.342857 |
| 1.775 | 0.338028 |
| 1.8 | 0.333333 |
| 1.825 | 0.328767 |
| 1.85 | 0.324324 |
| 1.875 | 0.32 |
| 1.9 | 0.315789 |
| 1.925 | 0.311688 |
| 1.95 | 0.307692 |
| 1.975 | 0.303797 |
| 2 | 0.3 |
| 2.025 | 0.296296 |
| 2.05 | 0.292683 |
| 2.075 | 0.289157 |
| 2.1 | 0.285714 |
| 2.125 | 0.282353 |
| 2.15 | 0.27907 |
| 2.175 | 0.275862 |
| 2.2 | 0.272727 |
| 2.225 | 0.269663 |
| 2.25 | 0.266667 |
| 2.275 | 0.263736 |
| 2.3 | 0.26087 |
| 2.325 | 0.258065 |
| 2.35 | 0.255319 |
| 2.375 | 0.252632 |
| 2.4 | 0.25 |
| 2.425 | 0.247423 |
| 2.45 | 0.244898 |
| 2.475 | 0.242424 |
| 2.5 | 0.24 |
| 2.525 | 0.237624 |
| 2.55 | 0.235294 |
| 2.575 | 0.23301 |
| 2.6 | 0.230769 |
| 2.625 | 0.228571 |
| 2.65 | 0.226415 |
| 2.675 | 0.224299 |
| 2.7 | 0.222222 |
| 2.725 | 0.220183 |
| 2.75 | 0.218182 |
| 2.775 | 0.216216 |
| 2.8 | 0.214286 |
| 2.825 | 0.212389 |
| 2.85 | 0.210526 |
| 2.875 | 0.208696 |
| 2.9 | 0.206897 |
| 2.925 | 0.205128 |
| 2.95 | 0.20339 |
| 2.975 | 0.201681 |
| 3 | 0.2 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Energetic threshold wavelength | 826.667 | nm |
| Incident photon rate | 3120750000 | s⁻¹ |
| Strictly above ideal gap | 1 | flag |
| Exact threshold, no finite-yield prediction | 0 | flag |
| Collected pair rate under supplied yield | 1872450000 | s⁻¹ |
| Collected current magnitude | 0.3 | nA |
| Pair-creation energy rate for collected branch | 0.45 | nW |
| Excess-energy thermalization rate for collected branch | 0.15 | nW |
| Selected-branch absorbed power | 0.6 | nW |
| Selected energy ledger residual | 0 | nW |
Enough photon energy is necessary for a band transition; actual absorption and collection need further material evidence.
A valence-to-conduction transition leaves an electron and a hole, not two independent charge quanta delivered through the same external circuit. With the stipulated external yield, current is e times the collected pair rate. For that selected branch, gap energy plus excess thermalization equals absorbed photon energy; uncollected photons and later recombination are outside this partial ledger. Doping changes carrier populations and available levels; the abrupt ideal threshold does not model an actual material, indirect-gap phonons, temperature, dark current or device conversion efficiency.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Enough photon energy is necessary for a band transition; actual absorption and collection need further material evidence.
A valence-to-conduction transition leaves an electron and a hole, not two independent charge quanta delivered through the same external circuit. With the stipulated external yield, current is e times the collected pair rate. For that selected branch, gap energy plus excess thermalization equals absorbed photon energy; uncollected photons and later recombination are outside this partial ledger. Doping changes carrier populations and available levels; the abrupt ideal threshold does not model an actual material, indirect-gap phonons, temperature, dark current or device conversion efficiency.
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