Keep a band-gap interpretation conditional on transport assumptions
A supplied intrinsic-carrier transport family has log conductivity L(T)=A+p ln(T/300)−Theta/T, where Theta=Eg/(2kB). The logarithm is of conductivity relative to a declared reference unit. The exponent p describes a stipulated mobility or prefactor temperature dependence. A is unknown to the inverse analyst even though the teaching generator reveals A=0.
Learning outcome: Fit both two-parameter families with the same two records, keeping the mobility exponent independent. Freeze their third-temperature predictions and check positivity before logarithms. Change the assumed exponent and identify which inferred parameter shifts. Retain an independent-contact or temperature-calibration test.
Starting recap
Review finite sums, exponential and logarithmic functions, radial integration measures, first-order coupled equations and mass-energy units. Keep state counts, occupations, calibration records and unused tests distinct.
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For Theta=1000 K and p=1, L300=−10/3 and L400=ln(4/3)−2.5. Removing the known mobility term recovers 1000 K, while ignoring it gives about 1345.218487 K. With kB=8.617333262×10^−5 eV/K, the conditional gap is about 0.172346665 eV. The unused 500 K log response is ln(5/3)−2.
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Why is the fitted activation parameter not automatically a unique measured band gap?
Experiment
Fit both two-parameter families with the same two records, keeping the mobility exponent independent. Freeze their third-temperature predictions and check positivity before logarithms. Change the assumed exponent and identify which inferred parameter shifts. Retain an independent-contact or temperature-calibration test.
Compare activation and contact alternatives on an unused temperature
Worked teaching model · synthetic values · Original indications obey ln(sigma)=A+p ln(T/300)−Theta/T, with A=0 a revealed generator not a known inverse amplitude. Independently stipulated p is used to fit A, Theta from 300 and400 K. A different two-parameter contact-limited resistance R=C+D/T fits the same two records; 500 K is fresh. No unique band gap follows without mobility/contact/model calibration.
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Calibration records and a fresh temperature
Graph axes rescale independently; read units and values, not screen angles. 1: fitted stipulated-exponent activation model (solid).2: unused temperature record (open-circle marked location). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Calibration records and a fresh temperature
fitted stipulated-exponent activation model
| temperature (K) | log relative conductivity |
|---|---|
| 300 | -3.333333 |
| 303.3333 | -3.285653 |
| 306.6667 | -3.238891 |
| 310 | -3.193017 |
| 313.3333 | -3.148004 |
| 316.6667 | -3.103828 |
| 320 | -3.060461 |
| 323.3333 | -3.017882 |
| 326.6667 | -2.976067 |
| 330 | -2.934993 |
| 333.3333 | -2.894639 |
| 336.6667 | -2.854986 |
| 340 | -2.816013 |
| 343.3333 | -2.777702 |
| 346.6667 | -2.740034 |
| 350 | -2.702992 |
| 353.3333 | -2.666559 |
| 356.6667 | -2.630719 |
| 360 | -2.595456 |
| 363.3333 | -2.560755 |
| 366.6667 | -2.526602 |
| 370 | -2.492982 |
| 373.3333 | -2.459882 |
| 376.6667 | -2.427289 |
| 380 | -2.39519 |
| 383.3333 | -2.363573 |
| 386.6667 | -2.332426 |
| 390 | -2.301738 |
| 393.3333 | -2.271498 |
| 396.6667 | -2.241695 |
| 400 | -2.212318 |
| 403.3333 | -2.183358 |
| 406.6667 | -2.154805 |
| 410 | -2.12665 |
| 413.3333 | -2.098883 |
| 416.6667 | -2.071496 |
| 420 | -2.04448 |
| 423.3333 | -2.017827 |
| 426.6667 | -1.991529 |
| 430 | -1.965579 |
| 433.3333 | -1.939968 |
| 436.6667 | -1.914689 |
| 440 | -1.889735 |
| 443.3333 | -1.8651 |
| 446.6667 | -1.840776 |
| 450 | -1.816757 |
| 453.3333 | -1.793037 |
| 456.6667 | -1.76961 |
| 460 | -1.746469 |
| 463.3333 | -1.723609 |
| 466.6667 | -1.701024 |
| 470 | -1.678709 |
| 473.3333 | -1.656659 |
| 476.6667 | -1.634867 |
| 480 | -1.61333 |
| 483.3333 | -1.592041 |
| 486.6667 | -1.570998 |
| 490 | -1.550193 |
| 493.3333 | -1.529624 |
| 496.6667 | -1.509286 |
| 500 | -1.489174 |
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.
unused temperature record
| temperature (K) | log relative conductivity |
|---|---|
| 500 | -1.489174 |
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 |
|---|---|---|
| First log conductivity record at 300 K | -3.333333 | log relative response |
| Second log conductivity record at 400 K | -2.212318 | log relative response |
| Fitted activation parameter conditional on mobility exponent | 1000 | K |
| Frozen log conductivity at 500 K | -1.489174 | log relative response |
| Fresh log conductivity at 500 K | -1.489174 | log relative response |
| Alternative predicted resistance at 500 K | -2.199982 | relative resistance |
| Alternative positive resistance at fresh temperature | 0 | flag |
| Apparent activation if mobility power is ignored | 1345.218 | K |
| Conditional gap using kB8.617333262e−5 eV/K | 0.1723467 | eV |
The contact-family extrapolation predicts nonpositive resistance and is rejected at the fresh temperature.
Fit the two unknown coefficients only after independently stipulating p. Subtract p ln(T/300), then the slope versus1/T is−Theta. Ignoring p changes the apparent slope. The different two-parameter resistance family C+D/T fits the same two records and may fail positivity or the third reading. Theta=Eg/(2kB) is conditional on the supplied intrinsic-carrier law; mobility, contacts, doping and temperature calibration can invalidate it.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
The contact-family extrapolation predicts nonpositive resistance and is rejected at the fresh temperature.
Fit the two unknown coefficients only after independently stipulating p. Subtract p ln(T/300), then the slope versus1/T is−Theta. Ignoring p changes the apparent slope. The different two-parameter resistance family C+D/T fits the same two records and may fail positivity or the third reading. Theta=Eg/(2kB) is conditional on the supplied intrinsic-carrier law; mobility, contacts, doping and temperature calibration can invalidate it.
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