efficient photonic applications such as near infrared spectra analysis, [1] telecommunications, [2] biomedical and chemical sensing. [3] Rapidly advancing plasmonics are of particular interest, along with their selective light-trapping with strongly localized photon energy, surface plasmons (SPs) have attracted attention due to their potential applications in medicine and chemistry, [4,5] as well as optical switching and near-field photonics. [6][7][8] However, many studies still rely on the Kretschmann-Raether excitation method, [9] requiring additional equipment to couple external light to surface modes at high angles of incidence (such as prisms), [10] or demand a metal/dielectric hybrid systems with delicately designed nanostructures to localize the photon energy in a deep-subwavelength region. [11] Unlike SPs, Tamm plasmons (TPs) can be directly observed with direct incidence without prism couplers and/or nanostructure. Also, the TPs structure can support surface waves dispersed within the light cone. [12] Optical TPs can form at the interfaces between distributed Bragg reflectors (DBRs) and with layers having optical thicknesses (t opt ) close to half the wavelength of light, similar to the electronic states that can occur in the energy bandgap of a crystal surface. [13,14] Because of their scalability and spectral tunability with a high quality (Q)-factor, and as sophisticated patterning is not required, TPs can be exploited in high-efficiency photonic applications; e.g., for photodetection, photocatalysis, biomedical diagnostics, and industrial process monitoring. [9,[15][16][17][18] Based on these theoretical advantages, the design and fabrication of real TP structures for practical applications have been studied. Recent approaches utilizing cavity-layer coupling, additional layers such as metasurfaces, [19] topological insulators, [20] and two-dimensional (2D) materials, including graphene and transition metal dichalcogenides, [21][22][23][24] have enhanced the available TP modes through adjustment of additional coupling. However, although these attempts successfully enhanced the resonator performance, they diminished the manufacturing advantages of the TP and planar structure. From the design point of view for satisfying both performance and manufacturing issues, DBR layers were stacked onto the metal reflector as a reversed structure from conventional TP structure. With reduced pairs of periodic layers (N) and by matching the impedance (Z) between As a powerful planar plasmonics, Tamm plasmon (TP) structures open up new possibilities for high-efficiency photonic applications demanding high quality (Q)-factor with scalability and spectral tunability. Despite the theoretical advantages of TP structures, TP configurations alternately stacked within limited materials and integer ranges result in thicker device sizes and still struggle to achieve ideal designs. Here, by introducing a computational model with varying design parameters, the configurations of highperformance TPs are presented within thin scal...