Bright-soliton frequency comb generation in a thin-film silicon nitride (SiN) microresonator at optical telecommunication wavelengths is numerically demonstrated using our recently developed approach for dispersionengineering by virtue of coupling-dispersion between two coupled microresonators. By coupling two identical resonators through an asymmetric Mach-Zehnder structure, sinusoidal splitting of the resonance frequencies can be achieved. This enables the engineering of the dispersion of the resulting modes of the coupled structure. Using this approach, anomalous dispersion of the resonant modes can be achieved at the pumping wavelength (which is selected to be the optical telecommunication wavelength, i.e., 1.55 µm) to enable Kerr-comb generation. In addition, by utilizing soliton-induced Cherenkov radiation in the coupled-resonator structure, we can increase the bandwidth of the resulting Kerr-comb signal.Bright-soliton frequency comb generation at the optical telecommunication wavelength is of great interest due to its application in enhancing the coherent telecommunication capacity through parallel transmission of data streams through the well-defined, low-noise comb lines, 1 in which, each comb line is used as a carrier in the wavelength-division-multiplexing (WDM) technique.Dissipative Kerr soliton (DKS) features coherent, low-noise comb lines, which can be used as oscillators in the WDM method. The combs associated with DKS inside a microresonator are generated through nonlinear interaction of photons through Kerr nonlinearity of the host material when seeded by the continuous-wave (CW) optical pumping. Thus, by using a coherent low-noise CW source for pumping, simultaneous well-defined, coherent, and low-noise frequency combs can be generated through DKS formation inside a microresonator. The nonlinear interaction is initiated by the modulation instability (MI), followed by cascaded four-wave mixing (FWM) to generate photons at other frequencies. Whispering-gallery-mode (WGM) resonators are widely used for efficient Kerr-comb generation, 2 especially in CMOS-compatible platform. However, generation of 1 arXiv:1806.11225v1 [physics.optics] 28 Jun 2018 wideband Kerr-comb signals requires precise control of the microresonator dispersion. 3 Anomalous dispersion of the resonant modes is a pre-requisite for wideband Kerr-comb generation. In addition, low-loss platforms with large nonlinear coefficients are essential for efficient low-power Kerr-comb generation. These requirements enforce limitations on the choice of material platform and device architecture (e.g., geometrical parameters of the microresonators). 3Among available CMOS-compatible materials, SiN is the preferred platform for Kerr-comb generation due to its wideband transparency window from visible to infrared wavelengths. In addition, the low material loss of SiN enables high quality-factor (Q) microresonators. 3, 4 Kerrcomb generation at optical telecommunication wavelengths is demonstrated in high-Q microresonators formed in thick SiN platform...