We analyze the dispersion of collective modes in a superconductor with $d\text{−}\mathrm{wave}$ symmetry of the order parameter in the presence of long-range Coulomb interaction. We use diagrammatic technique and quasiclassical theory in the Keldysh-Nambu formalism to compute longitudinal and transverse pair susceptibilities and extract from them the dispersion of the longitudinal and transverse collective mode. We show that at $T=0$ the dispersion of the transverse (plasma) mode is the same as in an $s$-wave superconductor, but at a finite $T$ it is softer and has a much larger decay rate due to the partial screening of the Coulomb potential by nodal quasiparticles. We show that the dispersion of the longitudinal mode depends on the direction of momentum with respect to the positions of the nodes of the $d\text{−}\mathrm{wave}$ gap, while the decay rate of this mode does not depend on momentum. We discuss experimental implications of our results.

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• Plasmons
• Quasiparticles & collective excitations
• Superconductivity