Quadratic pseudospectrum
FORCE_EVAL / PROPERTIES / QUADRATIC_PSEUDOSPECTRUM finds states approximately localized in both
position and energy from a converged GPW/GAPW calculation. It reports no topological index and
requires no additional library.
For Hermitian covariant AO observables \(A_j\), queries \(\lambda_j\), positive weights \(w_j\) and overlap \(S\), the generalized eigenproblem is
The lowest eigenpairs describe joint approximate states. The output includes \(\sqrt{q}\), separate energy/position residuals and expectation values. States satisfy \(c^\dagger S c=1\). Residuals concern projected finite-basis operators, not exact continuum variances.
&PROPERTIES
&QUADRATIC_PSEUDOSPECTRUM
FORMULATION FINITE
POSITION [bohr] 0 0 0
ENERGY [hartree] 0.0
KAPPA [hartree*bohr^-1] 0.01
NSTATES 2
&STATES
&END
&END
&END
Observables
FINITEuses analytic Cartesian moments. It requires matchingCELL/POISSON PERIODIC NONEwithout explicit k-points.PERIODICuses sine/cosine coordinates on the fullMP_GRIDtorus at the frozen SCF potential. Only periodic directions are localized. Nonperiodic mesh dimensions must be one.TRANSLATIONuses analytic translated-Gaussian overlaps for \(U(a)\psi(r)=\psi(r+a)\). Specify repeatedTRANSLATION_VECTORandWAVE_VECTORqueries and positiveTRANSLATION_SCALEinstead ofKAPPA. The target phase is \(\exp(i k\cdot a)\) without an additional \(2\pi\). This path includes the full continuum translation norm and reports leakage outside the AO span, rather than treating compressed AO translation matrices as unitary.
The periodic paths construct a complete analysis torus, independently of SCF symmetry reduction.
SOC T uses post-SCF GTH spin-orbit coupling after a restricted calculation with suitable
pseudopotentials.
Output and limits
SOLVER DENSE uses a metric-aware dense reference calculation. MAX_AO bounds the complete scalar
AO space, including periodic cells. EPS_METRIC rejects ill-conditioned overlap matrices, and
EPS_EIGEN bounds eigenpair residuals. NSTATES selects the number of states.
The STATES print section writes complex AO coefficients. Spin-up precedes spin-down for SOC, with
cell-major ordering inside each spin block on a torus. Individual vectors in a degenerate subspace
are gauge dependent. Compare subspaces, residuals and observables instead of individual
coefficients.
Choose energy, position and scales for the physical question and check basis and size dependence. Broader examples are available in TopologicalCP2K.