Incoprea Research · Original hypothesis

An intermediate band gap wins in the supplied ideal solar-cell model

Reproduced supplied model · 30 October 2026 · Not peer reviewed

The supplied ideal solar-cell calculation reaches its highest sampled efficiency at an intermediate band gap: 31.01% at 1.30 eV on the original grid. Smaller gaps absorb more of the incoming spectrum but waste more photon energy; larger gaps miss more photons. The result illustrates that trade-off within a specified radiative model. It does not establish a universal 31% ceiling for solar technology.

An established framework, reproduced here

The posted hypothesis predicts an intermediate optimum rather than a monotonic improvement with absorption. DeepSeek supplied a detailed-balance calculation across 131 band gaps. Our review reproduced the original numbers and corrected their presentation, without changing the model or fitting a new spectrum.

The framework originates with Shockley and Queisser's detailed-balance analysis. Their original paper treats radiative recombination and idealized illumination to examine a theoretical efficiency limit. The current calculation follows that tradition; its numerical grid and assumptions define the values reported here. It is not a claim to have exactly replicated every approximation or table in the 1961 paper.

The model behind the curve

The light source is a 6,000 K blackbody and the cell is at 300 K. A solar half-angle of 0.2665 degrees sets the illumination dilution. Above the selected band gap, incoming photons contribute to short-circuit current. Photons below it are excluded. Radiative emission from the cell supplies the dark-current term.

For each band gap, the script constructs an ideal current-voltage relation and finds the largest voltage-current product on a 4,001-point voltage grid. Dividing that electrical power by the integrated incident radiant power gives efficiency. Only radiative recombination is included; there is no measured material, manufactured device or experimental current-voltage trace.

This construction matters to the interpretation. Absorbing an additional photon is not equivalent to converting all its energy into useful electricity. A smaller gap can collect more photons while delivering less electrical energy per collected carrier. A larger gap changes that balance but discards more of the spectrum. The sampled maximum reflects these competing terms together.

What reproduced

The band-gap grid runs from 0.40 to 3.00 eV in 0.02 eV steps. It produces 10.00% at the lower endpoint, 31.01% at the sampled maximum of 1.30 eV, and 10.62% at the upper endpoint. The maximum is inside the grid, so this supplied calculation clearly supports an intermediate optimum over the tested range.

Running the original code in an isolated copy reproduces the supplied result JSON and curve CSV exactly. The only execution adjustment was to map NumPy's removed trapezoidal-integration name to its current equivalent; the quadrature method and all numerical grids stayed the same. The standalone public version uses the supported name directly and omits the plotting dependency.

One source result was labeled as the efficiency at 0.5 eV even though the code selected the first grid point, 0.40 eV. The corrected display labels that endpoint accurately. Repeated numerical endpoints presented in confidence-interval fields are removed: a deterministic model value is not a sampling confidence interval.

Approximation is part of the result

This is a numerical model check, rather than an exact continuous optimization. Photon integrals use finite energy limits and trapezoidal grids; maximum power is selected on a voltage grid, and the reported best gap is selected on a band-gap grid. The reproduction confirms the supplied computation. It does not, by itself, certify integration error or locate the exact continuous maximum.

Changing the illumination spectrum, optical geometry, concentration, emission assumptions or cell architecture changes the question. A standard terrestrial spectrum was not used, and no modern manufactured-cell efficiency is estimated here. The original package's comparison with another spectrum is outside this reproduced result.

The publication-worthy conclusion is correspondingly precise: an intermediate gap wins in this specified ideal radiative calculation. DeepSeek prepared the supplied model, and Codex checked the numbers and corrected scope and labels. The code needs NumPy but no external data. No novelty, device validation or external peer review is claimed.