Photoconductors – effect of optical illumination on device behavior with ohmic contacts For a photoconductor that has equal electron and hole mobilities and perfectly ohmic end contacts (no built-in photovoltaic action), what change is mainly produced when the intensity of optical illumination is increased?
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AA change in open-circuit voltage across the contacts
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BA change in short-circuit current at zero applied bias
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CA decrease in the material's resistance (increase in conductivity)
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DAn increase in the material's resistance (decrease in conductivity)
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EGeneration of a DC voltage even with no external bias (photovoltaic mode)
Answer
Correct Answer: A decrease in the material's resistance (increase in conductivity)
Explanation
Introduction / Context:Photoconductors are light-sensitive resistive devices. When photons are absorbed, additional electron–hole pairs are generated, which changes the carrier concentration and therefore the conductivity of the material. With ohmic contacts and no built-in junction, the device operates in photoconductive mode rather than photovoltaic mode.
Given Data / Assumptions:
- Contacts are perfectly ohmic, so there is no junction built-in field and no appreciable open-circuit voltage is produced by illumination.
- Electron and hole mobilities are equal, simplifying current contributions from both carriers.
- Illumination intensity increases, generating more excess carriers.
- Bias, if present, is small and used only to read out conductivity change.
Concept / Approach:
Conductivity sigma of a semiconductor is sigma = q * (n * mu_n + p * mu_p). If mu_n = mu_p and photo-generation increases carrier densities n and p by Delta n and Delta p, conductivity increases approximately in proportion to the excess carriers. In a photoconductor, the measurable effect is a reduction in resistance R = L / (sigma * A). There is generally no light-induced open-circuit voltage because ohmic contacts do not create a built-in electric field; instead, a bias is applied and the photocurrent is read as an increase over the dark current.
Step-by-Step Solution:
Start from sigma = q * (n * mu + p * mu) with mu_n = mu_p = mu.Under illumination: n → n + Delta n, p → p + Delta p.Thus sigma_light = q * mu * (n + p + Delta n + Delta p) > sigma_dark.Therefore R_light = L / (A * sigma_light) < R_dark, which means resistance decreases.Verification / Alternative check:
In practice, I–V curves of photoconductors under different light levels are straight lines with increasing slope as illumination increases, confirming lower resistance and no significant open-circuit photovoltage for purely ohmic contacts.
Why Other Options Are Wrong:
Option (a) and (e): open-circuit voltage generation is characteristic of photovoltaic junctions (p–n, Schottky), not purely ohmic contacts. Option (b): at zero bias an ohmic photoconductor does not sustain a notable short-circuit current. Option (d): illumination does not increase resistance; it decreases it.
Common Pitfalls:
Confusing photoconductive devices with photovoltaic cells, or assuming any illuminated semiconductor creates a DC voltage without a junction.
Final Answer:
A decrease in the material's resistance (increase in conductivity)