Returns the diffusion distance matrix when the spectrum (more precisely, the eigendecomposition) of the Laplacian is provided as input (useful to speed up batch calculations).

For instance, the random walk normalised Laplacian \(I - D^{-1}A\), which generates the classical continuous-time random walk over a network, can be easily and obtained from the spectral decomposition of the symmetric normalised Laplacian \(\mathcal{L} = D^{-\frac{1}{2}} L D^{-\frac{1}{2}} = D^{-\frac{1}{2}} (D - A) D^{-\frac{1}{2}}\). More specifically, \(\bar{L} = I - D^{-1} A = D^{-\frac{1}{2}} \mathcal{L} D^{\frac{1}{2}}\) and, since \(\mathcal{L}\) is symmetric it can be decomposed into \(\mathcal{L} = \sum_{l = 1}^N \lambda_l u_l u_l^T\), hence $$\bar{L} = \sum_{l = 1}^N \lambda_l u^R_l u^L_l$$ where \(u^L_l = u_l^T D^{\frac{1}{2}}\) and \(u^R_l = u_l D^{-\frac{1}{2}}\).

get_ddm_from_eigendec(tau, Q, Q_inv, lambdas, verbose = FALSE)

Arguments

tau

diffusion time (scalar)

Q

eigenvector matrix

Q_inv

inverse of the eigenvector matrix

lambdas

eigenvalues (vector)

verbose

whether warnings have to be printed or not

Value

The diffusion distance matrix \(D_t\), a square numeric matrix of the Euclidean distances between the rows of the stochastic matrix \(P(t) = e^{-\tau L}\), where \(-L\) is the Laplacian generating a continuous-time random walk (Markov chain) over the network. The matrix exponential is here computed using the given eigendecomposition of the Laplacian matrix \(e^{-\tau L} = Q e^{-\tau \Lambda} Q^{-1}\).

References

Bertagnolli, G., & De Domenico, M. (2021). Diffusion geometry of multiplex and interdependent systems. Physical Review E, 103(4), 042301. doi: 10.1103/PhysRevE.103.042301 arXiv: 2006.13032

See also