3. Results
- A.
Fundamental Limitation: Spectral Mismatch
The efficiency of photovoltaic (PV) energy conversion is fundamentally limited by spectral mismatch between the solar spectrum and semiconductor band gaps. Sunlight contains ultraviolet, visible, and infrared photons with a wide range of energies, while a single semiconductor absorber can efficiently convert only a narrow portion of that range. Photons with energy below the band gap pass through the device without generating carriers, while photons with excess energy lose the difference as heat through thermalization [
1,
2]. Because these losses occur before electrical conversion, they cannot be addressed solely by improving electrical transport within the solar cell.
To address this limitation, researchers have focused on controlling how light reaches the solar cell rather than only modifying the semiconductor itself. These approaches are generally referred to as spectral management techniques, where the goal is to match photon energy to the absorption better before electrical generation occurs [
3]. By improving this optical matching, a larger portion of the solar spectrum can be used more effectively.
One of the most direct spectral management strategies is solar spectrum splitting. In this approach, incoming sunlight is divided into multiple wavelength bands, and each band is directed to a device optimized for that specific energy range [
4]. This allows high-energy photons to be used by wide band gap materials and lower-energy photons to be utilized by narrow band gap devices, reducing both transmission and thermalization losses.
Compared to multijunction solar cells, which achieve spectral matching internally through stacked layers, spectrum splitting separates the optical and electrical design. This enables independent operation of each photovoltaic channel, greater flexibility in material selection, and simpler system integration. However, it also introduces challenges related to optical alignment, component losses, and system-level integration, which are important considerations in practical implementations.
- B.
Multijunction Solar Cells: Internal Spectrum Matching
Multijunction solar cells aim to reduce spectral mismatch by incorporating multiple semiconductor layers with different band gaps within a single device [
5,
6]. Each junction is designed to absorb a specific portion of the solar spectrum, allowing more efficient use of incoming photons compared with single-junction cells. By distributing the spectrum across multiple absorbers, these devices can achieve significantly higher conversion efficiencies.
However, multijunction cells are typically connected electrically in series, which means the same current must pass through every layer. An illustration of this design is shown in
Figure 1. If one junction produces less current due to changes in the solar spectrum, temperature, or material properties, it limits the performance of the entire device [
5].
This constraint, known as current matching, is a major challenge in maintaining optimal performance under real-world operating conditions.
In addition to electrical constraints, multijunction devices require complex fabrication processes, including precise material growth, lattice matching, and layer alignment. These requirements increase cost and limit scalability, especially for experimental or modular systems. As a result, while multijunction cells demonstrate very high efficiency, their complexity motivates the exploration of alternative approaches that can achieve spectral matching outside the semiconductor structure.
- C.
Optical Spectrum Splitting
Instead of stacking semiconductors, optical spectrum splitting separates wavelengths before the energy conversion process occurs. In this approach, optical components such as thin-film interference filters and dichroic mirrors are used to selectively reflect and transmit specific wavelength bands [
4,
7]. Each portion of the spectrum is then directed to a photovoltaic device that is better matched to that energy range. Hybrid receiver systems have shown that routing selected wavelengths to dedicated absorbers can improve spectral utilization while also reducing thermal loading on the photovoltaic device [
8].
A key advantage of this approach is that each photovoltaic channel can operate independently. Unlike multijunction cells, where all layers are electrically linked, spectrum-splitting systems avoid current-matching constraints and allow each device to operate closer to its optimal performance point. This provides greater flexibility in system design and material selection
However, thin-film interference filters are sensitive to the angle of incoming light. The cutoff wavelength shifts with the angle of incidence, which can reduce spectral selectivity and overall system performance under non-ideal conditions [
9]. Because outdoor sunlight is often diffused and not perfectly aligned, this angular sensitivity becomes a significant practical limitation for real-world applications.
- D.
Geometric Splitting Approaches
Other optical methods separate wavelengths spatially rather than through reflection-based filtering. Dispersive and diffractive elements, such as prisms and gratings, use wavelength-dependent refraction or diffraction to route different portions of the spectrum to separate physical locations [
10,
11]. In these systems, shorter and longer wavelengths follow different paths, allowing each band to be directed toward a dedicated photovoltaic receiver. A diagram of this process is depicted in
Figure 2.
Waveguide-based designs extend this concept by transporting selected spectral components laterally to different receivers. This can enable more compact system layouts and integrated designs, but it also introduces additional losses due to imperfect coupling and propagation within the waveguide structure [
12].
While these approaches demonstrate that spatial spectral allocation is feasible, they require precise optical alignment to function effectively. Small changes in geometry, positioning, or incident light conditions can significantly alter how wavelengths are distributed across the receivers. This sensitivity reduces system repeatability and robustness, particularly in compact or student-built systems where maintaining precise alignment is more difficult.
- E.
Hybrid PV-Thermal Systems
Another strategy is to use portions of the solar spectrum as heat instead of converting all photons into electricity. Hybrid photovoltaic–thermal (PV-T) systems, diagram shown in
Figure 3, route part of the incoming radiation to photovoltaic cells while directing the remaining wavelengths to thermal absorbers [
13,
14]. This approach increases total energy utilization by capturing both electrical and thermal energy from the same system.
However, while PV-T systems improve overall energy efficiency, they do not directly increase electrical output. The thermal energy produced is considered lower-quality energy compared to electrical energy because it has lower energy and is less flexible for practical use. Converting heat back into electricity requires additional processes, such as thermodynamic cycles, which introduce further losses and increase system complexity.
In contrast, photovoltaic systems convert photon energy directly into electrical energy through the photovoltaic effect, allowing for immediate and efficient use in electrical systems. This direct conversion avoids intermediate steps and preserves more of the original energy quality. As a result, while PV-T systems are beneficial for combined heat and power applications, they are less effective when the primary goal is maximizing electrical generation.
Additionally, integrating both thermal and electrical components increases system design complexity, requiring careful thermal management, additional materials, and more complex system integration. These factors make PV-T systems less suitable for compact, modular, or student-built applications where simplicity and direct electrical output are priorities.
- F.
Luminescent Solar Concentrators
Luminescent solar concentrators (LSCs) improve angular tolerance by absorbing incoming photons within a luminescent material and re-emitting them at longer wavelengths in random directions [
15,
16]. The re-emitted light is then guided through the material by total internal reflection toward photovoltaic cells located at the edges. Because the absorption process does not depend strongly on the angle of incoming light, LSCs can operate effectively under diffuse illumination, making them attractive for real-world outdoor conditions where sunlight is not perfectly collimated. A diagram of this process is demonstrated in
Figure 4.
However, this process introduces several inherent losses. First, during re-emission, photons are shifted to lower energy (longer wavelength), a phenomenon known as the Stokes shift. This reduces the maximum achievable electrical output because some of the original photon energy is lost before conversion. Additionally, not all absorbed photons are successfully guided to the photovoltaic cells—some are lost through escape cone losses, reabsorption, or non-radiative recombination within the material.
As a result, while LSCs improve optical collection and angular tolerance, they reduce the overall energy quality of the photons reaching the solar cell. Unlike direct photovoltaic conversion, where photon energy is converted immediately into electrical energy, LSC systems rely on an intermediate optical process that introduces additional inefficiencies. This trade-off highlights a key challenge: improving light capture under diffuse conditions often comes at the cost of reduced electrical conversion efficiency.
- G.
Photonic Crystal Spectral Filtering
Photonic crystal structures control light through a periodic variation in refractive index, which creates wavelength-selective optical behavior [
17]. This periodic structure forms photonic band gaps, where certain wavelengths are allowed to propagate while others are reflected or suppressed. As a result, photonic crystals can selectively transmit or reflect specific portions of the solar spectrum without relying entirely on geometric beam separation or angle-dependent filtering [
18,
19].
Because this filtering is governed by optical modes within the structure rather than simple ray direction, photonic crystals can maintain wavelength selectivity even when the angle of incoming light changes. This makes them less sensitive to alignment compared to thin-film interference filters or dispersive optical elements, which often require precise orientation to function effectively.
For spectrum splitting applications, this behavior offers a significant advantage. Photonic crystal filters can separate wavelengths while preserving the light’s direction toward photovoltaic receivers, enabling direct electrical conversion without intermediate energy-loss processes. At the same time, their reduced sensitivity to incidence angle allows them to operate more reliably under diffuse or partially scattered sunlight conditions.
This combination of wavelength selectivity, angular tolerance, and direct photon-to-electricity conversion makes photonic crystal filtering particularly attractive for compact, modular systems. In contrast to many existing approaches, these structures offer a pathway toward simplified alignment, improved robustness, and practical implementation in student-built or small-scale experimental platforms.
- H.
Electrical Integration After Spectral Separation
After the spectrum is split, each photovoltaic channel receives a different portion of the solar spectrum and therefore produces different voltage and current outputs. This occurs because photon energy directly influences the electrical characteristics of each device, with higher-energy photons generally contributing to higher voltages and lower-energy photons contributing to different current levels.
If the channels are connected in series, mismatch losses can occur, similar to those seen in multijunction solar cells. In this configuration, the total current is limited by the lowest-performing channel, which reduces the overall system output [
5]. Alternatively, if the channels are connected in parallel without proper design, differences in voltage between channels can lead to imbalance, power loss, or even reverse current flow, further reducing efficiency.
To address these issues, the independent operation of each photovoltaic channel is often preferred. By allowing each channel to operate at its own maximum power point, the system can maximize energy extraction from each portion of the spectrum [
20,
21]. This typically requires additional power electronics, such as separate maximum power point tracking (MPPT) or DC–DC conversion for each channel.
Therefore, spectrum splitting is not only an optical design problem but also an electrical system integration challenge. Effective implementation requires coordination between optical filtering and electrical architecture to ensure that the benefits of spectral separation are not lost due to electrical mismatch or inefficient power management.