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Related Concept Videos

P-N junction01:11

P-N junction

1.4K
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
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When light of a particular wavelength strikes a metal surface, electrons are emitted. This is called the photoelectric effect. The minimum frequency of light that can cause such emission of electrons is called the threshold frequency, which is specific to the metal. Light with a frequency lower than the threshold frequency, even if it is of high intensity, cannot initiate the emission of electrons. However, when the frequency is higher than the threshold value, the number of electrons ejected...
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Related Experiment Video

Updated: Feb 24, 2026

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Negative illumination thermoradiative solar cell.

Tianjun Liao, Xin Zhang, Xiaohang Chen

    Optics Letters
    |August 16, 2017
    PubMed
    Summary
    This summary is machine-generated.

    This study presents the negative illumination thermoradiative solar cell (NITSC), optimizing its design for maximum efficiency. Key findings aid in the optimal operation and design of thermoradiative cells (TRCs).

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    Area of Science:

    • Thermoradiative photovoltaics
    • Solar energy conversion
    • Optical physics

    Background:

    • Thermoradiative solar cells (TRCs) offer a pathway for solar energy conversion.
    • Optimizing TRC performance requires careful consideration of radiative and reflective losses.
    • The negative illumination thermoradiative solar cell (NITSC) integrates a concentrator, absorber, and TRC.

    Purpose of the Study:

    • To analytically derive the power output and overall efficiency of the NITSC.
    • To determine the optimal operating conditions and bandgap for maximum NITSC efficiency.
    • To provide insights for the improved design and operation of TRCs.

    Main Methods:

    • Development of thermal equilibrium equations to determine TRC operating temperature.
    • Analytical derivation of NITSC power output and efficiency, considering environmental losses.
    • Optimization of TRC output voltage and concentrating factor for a given bandgap.

    Main Results:

    • The study analytically derives the power output and efficiency of the NITSC.
    • Optimal bandgap values and operating conditions for maximum efficiency were determined.
    • Calculations incorporated radiation and reflection losses from the absorber and TRC.

    Conclusions:

    • The derived analytical model provides a framework for understanding NITSC performance.
    • Optimized bandgap and operating conditions are crucial for maximizing NITSC efficiency.
    • This research facilitates the optimal design and operation of thermoradiative solar cells.