1. Introduction
Bragg reflectors are optical elements that exploit graded structures capable of reflecting particular light wavelengths. Such patterns mainly depend on periodically stacked layers of materials having different refractive indices, which cause constructive interference that results in the reflection of specific portions of light. Lately, the field of optics has seen an upsurge in the use of Bragg reflectors for telecommunications, lasers, and optical filters, where controlling the light wavelength is the priority [1]. However, one of the main limitations of the classical Bragg reflection mirrors is that they are usually developed for a single wavelength and therefore lack the flexibility in dynamic optical systems. A continuously tunable Bragg reflector, adjustable throughout the entire reflective wavelength in real time, would have obvious benefits. By allowing the tuning of the working wavelength, this can improve the process in various fields, like adaptive optics, tunable lasers, and wavelength-specific filtering.
This paper examines the concept of noise and its implications for engineering projects, as well as methods for reducing it. This entails a brief discussion of the basic principles of engineering involved in this process, involving choices of materials, structural design, and tuning processes.
Developing a continuously tunable Bragg reflector for visible light holds significant promise in advancing optical technologies. The ability to dynamically adjust reflected wavelengths opens new pathways for adaptable and high-performance optical systems across disciplines. Potential impacts include enhanced precision in medical imaging and diagnostics, real-time wavelength selection in telecommunications, and improved adaptability in environmental sensing and monitoring. This research also contributes to the broader understanding of tunable photonic structures, laying the groundwork for future innovations in multifunctional optical devices that integrate sensing, modulation, and filtering capabilities.
2. The Engineering Challenge
In the field of optical technology, certain limitations exist in current designs, such as the rigidity of traditional Bragg reflectors. This section discusses these constraints and the growing importance of tunability in adapting Bragg reflectors for modern applications.
2.1. Limitations of Classical Bragg Reflectors
Classical Bragg grating mirrors are based on a uniform periodic structure, where coexisting media of different refractive indices create constructive interference to reflect some specific wavelengths of light [2]. These designs work very effectively for those applications where light reflection of coarse wavelength is required to be exact in the required position. However, these systems are relatively rigid, and therefore, in this case, they are required to adapt dynamically. Traditional Bragg reflectors' fixed arrangement deprives flexibility in optical systems. With no possibility to deploy their full potential, these reflectors can change their properties from time to time, and then they are only used for a specific requirement. The necessity of being able to cover a wide range of wavelengths, on the one hand, requires either a large number of reflectors or very complicated mechanical devices, which add to system complexity and costs.
2.2. The Significance of Adjustable Solutions for Naturally Occurring Visible Light
Visible light is the range where most optical technologies operate and have their relevance, and, therefore, it plays a vital role in achieving tunability within this frequency range [3]. Tunable Bragg reflectors will serve as a universal tool for tailoring light to specific needs and conditions. For instance, in adaptive optics, a tunable reflector could enhance imaging systems by impeding the wavefront distortion within the imaging systems. Besides, tunable reflectors might serve as a high-nuance technique used in medical diagnostics where a fine calibration of light reflection is important, for instance, optical coherence tomography [4]. Expanding this tunability could also lead to advancements in environmental monitoring and material sensing, where adjustable wavelengths enhance the detection of varied spectral signatures.
3. Alternative Approaches
Given the limitations discussed above, researchers have also explored other alternative solutions to achieve tunability in Bragg reflectors, though these approaches may also carry certain constraints.
3.1. Advanced Static Solutions
One of the technological developments is the invention of tunable Bragg reflectors, which have been designed with the goal of becoming a better version of traditional fixed designs. Another common approach involves thermal tuning of such materials, in which their refractive index can be changed with their temperature. Another approach utilizes liquid crystal or other electroactive media which can be switched with an electric field to obtain an opto-electrical tuning. The method is not only faster than the heat methods, but also is used in optical filtering systems [5]. additionally, mechanical tuning involves deforming the system to enlarge the gap between the layers, thus controlling the reflected wavelength.
3.2. Differences and Limitations
Every technique in its toolkit has its set of problems. Taking thermal tuning as an example, this method is slow, thus unsuitable for applications that require rapid adjustments. Electro-optic tuning is faster staining, but is limited by the number of materials available and their predisposition to external disturbances (like temperature and humidity) [6]. On the one hand, mechanical tuning achieves bigger range tuning (mainly shaped by deformation or mechanical stress), but its dynamics (frequency shifts) deteriorate the performance over time, especially in the same size of deformation or flexibility environments.
Additionally, each of these tuning methods faces limitations in terms of scalability. Furthermore, while each approach can provide some level of tunability, they often lack the precision needed for applications in sensitive optical technologies, such as high-resolution imaging and spectroscopy, where exact wavelength control is paramount.
4. Design of a Continuously Tunable Bragg Reflector
4.1. Material Selection
For the purpose of a stable tunable Bragg reflector, which is continuously variable, it has to undergo particularly precise material selection, especially optical and mechanical features. Titanium dioxide (TiO₂) is selected as the high-refractive index material on the basis of its good transparency and the roughly 2.5 refractive index in the visible range. Thanks to its great stability and power of building good films of light interference, it is an excellent host material for optical applications. The refractive index of silicon oxide (SiO₂) is ~1.45 that is a suitable material for a low refractive index to pair with Titanium dioxide ivory to create the contrast that is required to build the desired structure [7]. They are chosen for their long-lasting physical properties as well as their non-induced optical aberrations.
This type of tunability is made possible by adding the liquid crystal 5CB. 5CB is nematic, which means that it can react with an electric field, thus leading to changes in its refractive index and creating a dynamic modulation of the reflection wavelength. Its plottant is called polydimethylsiloxane (PDMS), picked for both its flexibility and transparency. PDMS acts as a flexible substrate that allows mechanical tuning by stretching or compressing the bandgap around the Bragg layers.
4.2. Structural Design
The structure is formed by TiO2/SiO2 pairs, with the layer thickness adjusted according to the designed wavelength. An example of this would be a TiO2 layer of about 50 nm thick in resonance with 500 nm light and a SiO2 layer of about 86 nm thick, considering their refractive indices. Consequently, this design is determined through the Bragg condition, given as
\( λ=2ndcosθ \) (1)
where n is the refractive index, d represents the layer thickness, and λ is the reflected light [8]. Such a multilayer structure of a mirror is characterized by a series of 10 to 20 alternating pairs.
In the procedure, the liquid crystal layer is put on top of the dielectric layers to add control by tuning up the refractive index. The PDMS substrate supports mainly this type of design, thus providing mechanical strain of the entire setup that brings about modulation of the layer spacing, which, in turn, gives rise to a shift of the reflection wavelength. All in all, this mixture of materials gives a precise, though flexible, reflector.
4.3. Tuning Mechanisms
The reflector's tunability relies on two mechanisms: the electric field tuning and the mechanical strain.
Electric field tuning takes place in the liquid crystal layer. When an external electric field is applied, the liquid crystals will reorient, affecting the refractive index. The phase of this optical path length modulates the wavelength of the reflected light. This provides the most suitable means of reflection while ensuring no physical structure alteration is used [9].
The mechanical stress tuning results from of the PDMS substrate. By applying defined mechanical stress to the sample, the reflected wavelength can be adjusted by the periodicity of the TiO2 and SiO2 layers. Such a method provides a wide tunable range of these metals, making it applicable across various optical techniques.
The two tuning mechanisms separately allow for continuous active control of the reflected wavelength. Hence, the proposed design can be considered as a potential advanced optical system where the dynamic adaptability of different wavelengths and the correct operation mode of the system are crucial.
5. Applications
5.1. Flexibly and broadly tunable optical devices
Continuously tunable Bragg reflectors exhibit a variety of dynamic optical systems involving wavelength control crucial for accurate color reflection. Another one is the tunable optical filters, which serve as an instrument that can limit the passage of certain light wavelengths while others go through. By adjusting the reflector’s periodicity or refractive index via electric fields or mechanical strain, these filters can be dynamically tuned across a wide spectral range, making them ideal for applications in optical communication systems [10]. Furthermore, this kind of operation is also used in the case of tunable lasers. For example, the design of a laser with a selective resonator that uses a Bragg reflector as a feedback element to tune the output wavelength. By creating a laser with such flexibility, we can then tune it with ease anywhere within a broad range [11]. Such a degree of modulation can be applied to spectroscopy, telecommunication, and even medical diagnostics.
Meanwhile, these reflectors vary in structure and can be implemented in the development of reconfigurable optical devices like beam-splitting systems, where the light’s path and spectrum can be controlled and modified at will. The devices play essential roles in the vision of current optoelectronic circuits because of the high-quality control over light that offers good performance in information processing, computing, and sensors. The material deformation property used in the reflectors, for example, the PDMS substrate, provides a multi-dimensional flexibility that gives flexibility in the construction of bendable or flexible photonic systems.
5.2. Analysis and Imaging
Bragg reflectors with continuously tunable wavelengths are considered particularly beneficial in the sensing and imaging fields, owing to the possibility of instantaneously changing the wavelengths of the reflected waves [12]. For instance, in spectral imaging (where the use of different color bands, with respective reflection signatures, enables the system to switch between them), tunable reflectors offer new capabilities by changing the bands on demand. These devices assist in identifying particular bombardments employing unique absorption or emission spectra. The flexibility of the reflector made by mingling Bragg reflectors allows adjusting the parameters in real time to measure a wide range of compounds, thus improving both accuracy and flexibility of the sensing system.
Such optical reflectors with tunable properties are of great use in developing advanced optical sensors, which detect the changes of the refractive index of biological samples as these changes could mean the presence of certain biomolecules or pathogens [13]. Through the ability to shift the frequency of the reflected light, these tools operate through, or within, a number of wavelength ranges, allowing them to deliver several additional details related to the examined sample. Nonetheless, in optical coherence tomography (OCT), also a non-invasive imaging technology, tunable Bragg reflectors can solve the problem of lower resolution and imaging depth of tissues by permitting the selection of light of various wavelengths in a way that more precise structural imaging can be obtained.
Taking into consideration the wide range of available materials, such as liquid crystals and PDMS, the tunable Bragg reflectors are being explored as suitable components for wearable and small implantable biosensing devices in applications like biosensors and environmental monitorization [14]. Their adaptability ensures high precision wavelength control, making these kinds of sensors suitable for a variety of imaging and sensing applications.
Overall, the use of continuously tunable Bragg reflectors in modern optical technologies involves a wide range of areas, ranging from telecommunications to biomedical imaging, thus signifying this reflective component as a cornerstone of the next generation of optical systems.
6. Discussion
The current continuously tunable Bragg reflector design reveals advantageous factors, which exhibit essential features that should be taken into consideration when developing optical systems. The two-level tuning strategy, combining electronic and mechanical actuation, realizes a large variety of tuning throughout the entire range and maintains a quick response. Notwithstanding such improvement, problems still exist in the control of thickness and other parameters during the manufacturing process. When the thickness of TiO₂ and SiO₂ layers doesn't match the target, it results in poor mirror's quality, necessitating the development of advanced manufacturing techniques. Along with this, the continuity of the electric field across the liquid crystal layer areas is necessary for tunability expansion, which turns out to be tough at the larger scales. Last but not least, the quality of PDMS substrate materials should also be considered, as they can be drastically influenced by material fatigue over time.
Such a process may result in tunable wavelengths that could be beyond the visible range, creating substantial opportunities for their applications in imaging, sterilization, and ultraviolet technologies [15]. Such operative unity, moreover, can improve the effectiveness of fewer complex models in the scope of incorporation into large-scale, multiple-function optical systems requiring constant sensing, modulation, and filtering at the same time.
7. Conclusion
The tunable nature of the Bragg reflector, envisioned by the arrangement of alternating TiO₂ and SiO₂ layers, leads to a PDMS substrate that exhibits suitable mechanical properties and allows both electric and mechanical adjustment of the wavelength, resulting in real-time tuning. This kind of setup outperforms a fixed Bragg mirror in terms of wavelength modulation, which can be adjusted constantly. The specific method suggests the outlook for the innovative designs of dynamic optical systems and superior metric sensing and imaging devices. The ongoing importance of the material-related discoveries will bring into the phase of tunable Bragg reflectors as being one of the key factors in functionalizing next-generation optical devices.
However, challenges remain, particularly concerning long-term durability under repeated stress, maintaining precise wavelength control, and further optimizing material properties for improved environmental resilience. Future research should focus on enhancing the mechanical robustness of flexible substrates like PDMS to minimize material fatigue and on exploring advanced materials or composites that can broaden the tuning range and increase reflectivity. Additionally, integrating multifunctional capabilities such as adaptive response to environmental changes would significantly expand the applicability of tunable Bragg reflectors across diverse fields, from wearable sensors to adaptive optics in space exploration. These advancements could pave the way for even more sophisticated applications.
References
[1]. Jaehoon Kim, Hyung-Jun Song. Strategies for efficient and stable colored perovskite module with Bragg reflector and luminescent down-shifting layer. Cell Reports Physical Science, Volume 5, Issue 7, 2024, 102070, ISSN 2666-3864, https://doi.org/10.1016/j.xcrp.2024.102070.
[2]. M. Portnoi, T. J. Macdonald, et al, All-Silicone-Based Distributed Bragg Reflectors for Efficient Flexible Luminescent Solar Concentrators. Nano Energy, vol.70, 104507, 2020. doi: 10.1016/j.nanoen.2020.104507.
[3]. Z. Tahir, M. U. Rashid, S. Kim, et al. Highly reflective distributed Bragg reflectors for planar microcavities: From modelling to experimentation. Journal of the Korean Physical Society, vol. 82, no. 2, pp. 147-156, 2023. doi: 10.1007/s40042-023-00165-7.
[4]. Rocío Ortiz, Marina Richet, Noella Lemaitre, Eva Gutiérrez. Tunable distributed Bragg reflector developed by magnetron sputtering to improve the power conversion efficiency of transparent IR cells for solar energy harvesting applications. Organic Electronics, Volume 135, 2024, 107106, ISSN 1566-1199, https://doi.org/10.1016/j.orgel.2024.107106.
[5]. Yingjian Liu, Kai Jiang, et al. High responsivity evanescently coupled waveguide photodiode using spot-size converter and distributed Bragg reflector at 1.55 μm wavelength, Infrared Physics & Technology, Volume 130, 2023, 104619, ISSN 1350-4495, https://doi.org/10.1016/j.infrared.2023.104619.
[6]. Kaipeng Qin, Xin-Hua Deng, et al. Tunable multiband THz perfect absorber due to the strong coupling of distributed Bragg reflector cavity mode and Tamm plasma polaritons modes based on MoS2 and graphene, Optics Communications, Volume 550, 2024, 129947, ISSN 0030-4018, https://doi.org/10.1016/j.optcom.2023.129947.
[7]. Saravanan Sigamani, R.S. Dubey, S. Kalainathan. Optimization of distributed Bragg’s reflectors in thin film solar cells, Materials Today: Proceedings, Volume 89, Part 2, 2023, Pages 8-13, ISSN 2214-7853, https://doi.org/10.1016/j.matpr.2023.05.540.
[8]. Morgan Bergthold, Daniel Wasserman, Aaron J. Muhowski. Plasmon-enhanced distributed Bragg reflectors, Infrared Physics & Technology, Volume 125, 2022, 104236, ISSN 1350-4495, https://doi.org/10.1016/j.infrared.2022.104236.
[9]. Ranjith B. Gowda, H.N. Gayathri, Preeta Sharan, K. Saara. Theoretical investigation of Bragg Reflector optical sensor for the measurement of cryogenic temperature, Materials Today: Proceedings, Volume 58, Part 1, 2022, Pages 451-455, ISSN 2214-7853, https://doi.org/10.1016/j.matpr.2022.02.482.
[10]. M. Anaya, A. Rubino, M. E. Calvo, and H. Míguez. Solution processed high refractive index contrast distributed Bragg reflectors. Journal of Materials Chemistry C, vol. 5, no. 16, pp. 3913-3921, 2017. doi: 10.1039/c6tc00663a.
[11]. Hansol Kim, Mine Kaya, Shima Hajimirza. Broadband solar distributed Bragg reflector design using numerical optimization. Solar Energy, Volume 221, 2021, Pages 384-392, ISSN 0038-092X, https://doi.org/10.1016/j.solener.2021.04.045.
[12]. Lisha C. Lohithakshan, Vishnu Geetha, Pradeesh Kannan. Single polymer-variable index for the design and fabrication of variable stop band distributed Bragg reflectors. Optical Materials, Volume 110, 2020, 110509, ISSN 0925-3467, https://doi.org/10.1016/j.optmat.2020.110509.
[13]. Chia-Jung Wu, Yi-Yun Chen, et al. Anisotropic properties of pipe-GaN distributed Bragg reflectors, Nanoscale Advances. Volume 2, Issue 4, 2020, Pages 1726-1732, ISSN 2516-0230, https://doi.org/10.1039/c9na00743a.
[14]. R.S. Dubey, V. Ganesan. Fabrication and characterization of TiO2/SiO2 based Bragg reflectors for light trapping applications. Results in Physics, Volume 7, 2017, Pages 2271-2276, ISSN 2211-3797, https://doi.org/10.1016/j.rinp.2017.06.041.
[15]. Sang Hoon Oh, Tae Ho Lee, Kyung-Rock Son, Tae Geun Kim. Fabrication of HfO2/TiO2–based conductive distributed Bragg reflectors: Its application to GaN-based near-ultraviolet micro-light-emitting diodes. Journal of Alloys and Compounds, Volume 773, 2019, Pages 490-495, ISSN 0925-8388, https://doi.org/10.1016/j.jallcom.2018.09.287.
Cite this article
Lin,Y. (2025). Design and Applications of a Continuously Tunable Bragg Reflector for the Visible Spectrum. Applied and Computational Engineering,128,183-188.
Data availability
The datasets used and/or analyzed during the current study will be available from the authors upon reasonable request.
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References
[1]. Jaehoon Kim, Hyung-Jun Song. Strategies for efficient and stable colored perovskite module with Bragg reflector and luminescent down-shifting layer. Cell Reports Physical Science, Volume 5, Issue 7, 2024, 102070, ISSN 2666-3864, https://doi.org/10.1016/j.xcrp.2024.102070.
[2]. M. Portnoi, T. J. Macdonald, et al, All-Silicone-Based Distributed Bragg Reflectors for Efficient Flexible Luminescent Solar Concentrators. Nano Energy, vol.70, 104507, 2020. doi: 10.1016/j.nanoen.2020.104507.
[3]. Z. Tahir, M. U. Rashid, S. Kim, et al. Highly reflective distributed Bragg reflectors for planar microcavities: From modelling to experimentation. Journal of the Korean Physical Society, vol. 82, no. 2, pp. 147-156, 2023. doi: 10.1007/s40042-023-00165-7.
[4]. Rocío Ortiz, Marina Richet, Noella Lemaitre, Eva Gutiérrez. Tunable distributed Bragg reflector developed by magnetron sputtering to improve the power conversion efficiency of transparent IR cells for solar energy harvesting applications. Organic Electronics, Volume 135, 2024, 107106, ISSN 1566-1199, https://doi.org/10.1016/j.orgel.2024.107106.
[5]. Yingjian Liu, Kai Jiang, et al. High responsivity evanescently coupled waveguide photodiode using spot-size converter and distributed Bragg reflector at 1.55 μm wavelength, Infrared Physics & Technology, Volume 130, 2023, 104619, ISSN 1350-4495, https://doi.org/10.1016/j.infrared.2023.104619.
[6]. Kaipeng Qin, Xin-Hua Deng, et al. Tunable multiband THz perfect absorber due to the strong coupling of distributed Bragg reflector cavity mode and Tamm plasma polaritons modes based on MoS2 and graphene, Optics Communications, Volume 550, 2024, 129947, ISSN 0030-4018, https://doi.org/10.1016/j.optcom.2023.129947.
[7]. Saravanan Sigamani, R.S. Dubey, S. Kalainathan. Optimization of distributed Bragg’s reflectors in thin film solar cells, Materials Today: Proceedings, Volume 89, Part 2, 2023, Pages 8-13, ISSN 2214-7853, https://doi.org/10.1016/j.matpr.2023.05.540.
[8]. Morgan Bergthold, Daniel Wasserman, Aaron J. Muhowski. Plasmon-enhanced distributed Bragg reflectors, Infrared Physics & Technology, Volume 125, 2022, 104236, ISSN 1350-4495, https://doi.org/10.1016/j.infrared.2022.104236.
[9]. Ranjith B. Gowda, H.N. Gayathri, Preeta Sharan, K. Saara. Theoretical investigation of Bragg Reflector optical sensor for the measurement of cryogenic temperature, Materials Today: Proceedings, Volume 58, Part 1, 2022, Pages 451-455, ISSN 2214-7853, https://doi.org/10.1016/j.matpr.2022.02.482.
[10]. M. Anaya, A. Rubino, M. E. Calvo, and H. Míguez. Solution processed high refractive index contrast distributed Bragg reflectors. Journal of Materials Chemistry C, vol. 5, no. 16, pp. 3913-3921, 2017. doi: 10.1039/c6tc00663a.
[11]. Hansol Kim, Mine Kaya, Shima Hajimirza. Broadband solar distributed Bragg reflector design using numerical optimization. Solar Energy, Volume 221, 2021, Pages 384-392, ISSN 0038-092X, https://doi.org/10.1016/j.solener.2021.04.045.
[12]. Lisha C. Lohithakshan, Vishnu Geetha, Pradeesh Kannan. Single polymer-variable index for the design and fabrication of variable stop band distributed Bragg reflectors. Optical Materials, Volume 110, 2020, 110509, ISSN 0925-3467, https://doi.org/10.1016/j.optmat.2020.110509.
[13]. Chia-Jung Wu, Yi-Yun Chen, et al. Anisotropic properties of pipe-GaN distributed Bragg reflectors, Nanoscale Advances. Volume 2, Issue 4, 2020, Pages 1726-1732, ISSN 2516-0230, https://doi.org/10.1039/c9na00743a.
[14]. R.S. Dubey, V. Ganesan. Fabrication and characterization of TiO2/SiO2 based Bragg reflectors for light trapping applications. Results in Physics, Volume 7, 2017, Pages 2271-2276, ISSN 2211-3797, https://doi.org/10.1016/j.rinp.2017.06.041.
[15]. Sang Hoon Oh, Tae Ho Lee, Kyung-Rock Son, Tae Geun Kim. Fabrication of HfO2/TiO2–based conductive distributed Bragg reflectors: Its application to GaN-based near-ultraviolet micro-light-emitting diodes. Journal of Alloys and Compounds, Volume 773, 2019, Pages 490-495, ISSN 0925-8388, https://doi.org/10.1016/j.jallcom.2018.09.287.