(2.52) |

In the linear response regime of the Landauer theory the heat current is proportional to the temperature difference by:

(2.53) |

This can alternatively be written as:

(2.54) |

where the phononic window function is given by [57]:

(2.55) |

As , one can express the lattice contribution to the thermal conductance as [58]:

To extract the ballistic phonon transmission in Eq. 2.56, similar to the electronic quantities (Eqs. 2.39-2.42), the phononic density of modes is calculated using the phononic bandstructures, where denotes the energy of a phonon with frequency . In our calculations for phonon density of states , we broadened the delta function by . This helps to numerically smoothen the DOS function, without affecting the thermal conductance calculations.

The FCM can also be effectively coupled to NEGF for the investigation of coherent phonon transport in low dimensional systems. The NEGF method has been traditionally employed for electronic transport studies, but has been extended to phonon studies as well [54]. Here, the phononic device Green's function is obtained by

where is device dynamic matrix and is the phonon energy [59]. Note that this is a Green's function of a classical wave equation, which is second order in time. Therefore, the square of the energy appears in Eq. 2.57. This is in contrast to the Schrodinger equation for quantum treatment of electrons which is first order in time, such that the eigen energy appears linearly in that case.

Finally, similar to the electron transport, the transmission probability of phonons through the rough channel can then be calculated using:

(2.58) |

Here, the phononic broadening and contact self-energy matrices are obtained in a similar way as the electronic ones (Eq. 2.51) with the substitutions and .