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Page 2 of 19          Lee et al. Microstructures 2023;3:2023021  https://dx.doi.org/10.20517/microstructures.2023.08

               materials will experience the quantum confinement effect. This phenomenon relates to the exciton and
               electronic energy level, which is continuous in bulk but becomes discrete in nanocrystals as the electron
               movement is confined to a specific energy level. An exciton is a bound state between an electron hole in
               valence band (VB) and an electron through Coulomb interaction. When a photon interacts with a
               semiconductor material and the energy of the photon exceeds or equals the bandgap (Eg), an electron in the
               VB is excited to the conduction band (CB), resulting in the formation of a positively charged hole referred
               to as an electron hole. As the excited electron and electron hole are confined within a limited space, more
               energy is required to excite them, which results in size-dependent band gaps and light emission. When a
               material is confined in one dimension, it forms a quantum well structure. Similarly, two-dimensional
               confinement results in a quantum wire, while three-dimensional confinement leads to a quantum dot,
                                                                      [1-8]
               which is a material that is confined in all three dimensions . This energy state results in unique
               characteristics, including long fluorescence lifetime, narrow and symmetrical photoluminescence emission,
               wide  absorption,  and  high  photoluminescence  quantum  yield  (PLQY).  Furthermore,  the
               photoluminescence emission band gap can be tuned by varying the size of QDs. Traditionally, combinations
               of 0D core-shell structure materials and group 12-16 elements have been investigated as promising
               quantum dot materials, such as ZnSe, ZnO, InP, InAs, and CdSe [9-11] . Recently, organic-inorganic metal
               halide perovskites have been noticed as promising QD materials due to the recent successful development
               of photovoltaic (PV) cells, LEDs, and sensors based on perovskite QDs [12-17] . However, in light of increasing
               concerns about the potential toxicity of some materials, there is growing interest in developing alternatives
               that are more biocompatible and environmentally friendly. For instance, carbon quantum dots (CQDs) and
               graphene quantum dots (GQDs) are emerging as promising candidates [18-20] . Graphene Quantum Dots
               (GQDs) exhibit remarkable size-dependent luminescence properties that are attributed to their quantum
               confinement and edge effects. These properties make GQDs highly attractive for optoelectronic and
               photodetector applications, including LEDs and electroluminescent devices. However, GQDs often suffer
               from reduced fluorescence, which hampers their ability to function as optoelectronic devices due to phase
               separation and agglomeration in organic or inorganic solvents. Furthermore, the non-stoichiometric nature
               of GQDs makes it particularly challenging to achieve precise control over their chemical structure, size,
               shape, and structural defects, which are directly related to their optoelectronic properties. Therefore, there
               have been numerous attempts to incorporate GQDs into matrices such as polymer films or mesoporous
               solids in order to control the size of the nanoparticles and stabilise them. However, since many of the
               current fabrication methods are complicated and difficult to control, there is a need to investigate more
               reproducible and simpler methods to fully utilise the great fluorescence properties of GQDs [21-25] .


               Despite the promising potential of quantum dots (QDs) in various applications and the significant progress
               achieved in material sciences, several challenges continue to hinder their widespread implementation. These
               challenges include issues such as agglomeration, precise size control, and operational stability, which
               demand further research and development to mitigate effectively. Generally, QDs show a strong tendency to
               aggregate into larger particles due to their high surface energy, which leads to the loss of their unique
               characteristics. Several recent studies have tried to mitigate the limitations of QDs through solvent
               engineering, surface passivation using semiconducting film, encapsulation with polymers, or embedment of
               QDs within porous nanomaterials [26-29] . However, most of these strategies require complex fabrication
               processes, and it remains difficult to control the outcomes, which may reduce the efficacy of these methods.


               Traditional nanomaterials with microporosity, such as mesoporous silica, zeolites, and porous carbon, have
               been investigated for various applications, including drug delivery, biosensing, separation, and catalysts [30,31] .
               Despite their great advantages, i.e., high surface area, tunable porosity, and biocompatibility, they tend to
               have limited chemical tunability. This limitation inspired scientists to develop microporous functional
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