## 1 Introduction  
Over the past few years, interest in creating materials allowing for the control the flow of electromagnetic waves (e.g., light) in exceptional ways has increased dramatically. Novel engineering tools have opened wide avenues to construct artificial materials possessing properties that are not possible in the case of the naturally existing materials. These new designs are possible due to the wide variety of inclusions. Moreover, the novel response appears to be because of their specific interactions with electromagnetic fields. These designs can be scaled down and constructed thanks to nanotechnology. Hyperbolic metamaterials represent a multi-functional platform providing a fertile ground for the realization of waveguiding, imaging, sensing, quantum, and thermal engineering outside the scope of conventional devices. These novel composites utilize the notion of tuning the fundamental dispersion relation of surface plasmon polaritons aiming to generate exceptional electromagnetic modes with a wide spectrum of applications. The hyperbolic metamaterial can be considered from the perspective of polaritonic crystal. The unique positioning of nanomaterials bridging atoms and bulk solids, along with their interesting features and potential applications [1] has provided a fertile ground for the growing scientific interest in them. The capability to create such nanoscale-sized materials advances many fields of modern science and technology. Transparent conductive oxides (TCOs) are of particular interest within the scientific community. These might be utilized as the optional materials for plasmonic applications [2] in the near-infrared region. It should be mentioned that TCOs such as indium tin oxide (ITO) show a wide spectrum of engineerable features [3]. The former is possible via doping and electric bias. The modelling and fulfillment of ultra-compact electro-absorption modulators [4; 5; 6; 7; 8], including the application of novel multimode modulator architectures, [9] has profited from the chance of actively switching between two different regimes. The unique properties of SP-based nanostructures and their applications in waveguides, sources, near-field optics, nonlinear optics, surface enhanced Raman spectroscopy (SERS), data storage, solar cells (or photovoltaic devices), chemical sensors, biosensors, etc. [10; 11], have stimulated a tremendous interest in their properties. Hyperbolic materials belong to a class of uniaxial materials. These are characterized by two different values for permittivity, i.e., parallel and perpendicular to the optical axis [12]. The exceptional wave is characterized by an electric field with components along the optical axis and perpendicular to it. Hyperbolic materials possess a remarkable property. They support propagating waves possessing arbitrary large wave vectors at a finite frequency [13; 14; 15]. Consequently, the corresponding local density of states is exceptionally large. In doing so, hyperbolic substances open wide avenues for many applications such as superresolution, enhanced spontaneous emission, and large energy density [16]. Based on the frequency range, one may divide sound waves into the types that follow: low frequency, intermediate frequency, and high frequency. Noise has a strong penetrating power and dissipates slowly during propagation. In doing so, it is a challenging task to engineer the sound waves. Hence, it is of particular importance to focus on the investigation of sound waves and vibration control. The investigations of surface waves and plasmonics represent an additional inherent part of nanophotonics. The former provide a fertile ground aiming to lower the length scales and dimensionality of a wide range of electromagnetic phenomena. Not remarkably, nonreciprocity and unidirectional propagation of surface plasmon-polaritons (SPPs) have stimulated a tremendous interest. Magneto-optical nonreciprocity in the transverse Voigt geometry is mostly dealt with in these studies, comprising topological quantum-Hall-effect states.