The extent to which the atomic fluctuations/displacements of a system are
  correlated with one another can be assessed by examining the magnitude
  of all pairwise cross-correlation coefficients (see McCammon and Harvey,
  1986).  This function returns a matrix of all atom-wise cross-correlations
  whose elements, Cij, may be displayed in a graphical representation
  frequently termed a dynamical cross-correlation map, or DCCM.
  If Cij = 1 the fluctuations of atoms i and j are completely correlated
  (same period and same phase), if Cij = -1 the fluctuations of atoms i
  and j are completely anticorrelated (same period and opposite phase),
  and if Cij = 0 the fluctuations of i and j are not correlated.
  Typical characteristics of DCCMs include a line of strong
  cross-correlation along the diagonal, cross-correlations emanating
  from the diagonal, and off-diagonal cross-correlations. The high
  diagonal values occur where i = j, where Cij is always equal to
  1.00. Positive correlations emanating from the diagonal indicate
  correlations between contiguous residues, typically within a secondary
  structure element or other tightly packed unit of structure.
  Typical secondary structure patterns include a triangular pattern for
  helices and a plume for strands.  Off-diagonal positive and negative
  correlations may indicate potentially interesting correlations between
  domains of non-contiguous residues.
  cov2dccm function calculates the N-by-N cross-correlation matrix 
  directly from a 3N-by-3N variance-covariance matrix. 
  If method = "pearson", the conventional Pearson's inner-product 
  correlaiton calculation will be invoked, in which only the diagnol of 
  each residue-residue covariance sub-matrix is considered. 
  If method = "lmi", then the linear mutual information
  cross-correlation will be calculated. LMI considers both
  diagnol and off-diagnol entries in sub-matrices, and so even grabs the
  correlation of residues moving on orthognal directions. (See more details
  in lmi.)