Research Highlights:
O(N) Krylov-subspace method for large-scale systems 
   
   
   
   
      Figure: Underlying idea of the  O(N) Krylov subspace method.
   
   
   
 
The computational cost of conventional density functional theories (DFT) calculations scales as the third power 
of the number of atoms, which means that the computational time becomes a thousand times longer than 
that for an original system when you try to calculate a ten times larger system. This presents an apparent 
difficulty to researchers who deal with realistic large-scale problems. On another front, it is known that 
chemical properties of functional groups in molecules are mostly determined by local atomic arrangement. 
The chemical intuition may enable us to develop an efficient method which determines the local electronic 
structure by making use of mainly short-range information. Along this line, we have developed an efficient 
and robust O(N) method by unifying two ideas of the divide-conquer and Krylov subspace methods, shown in
the upper figure, whose computational cost scales only linearly as a function of the number of atoms [1]. 
   
   
   
   
      Figure: Difference charge density for a (10,0) finite sized zigzag
 
          carbon nanotube on aluminum surface calculated by the O(N) method.
   
   
   
 
The O(N) computational cost is guaranteed by the idea of the divide-conquer method, and the reduction of 
dimension by the Krylov subspace method provides a small computational prefactor. The practical algorithm 
is cast to solving a series of embedded cluster problems defined in Krylov subspaces. 
The O(N) method is expected to be a promising approach for realization of large-scale ab initio 
calculations for a wide variety of materials, since it is applicable to not only insulators 
but also metals in a single framework. The bottom figure shows difference charge density caused by 
the interaction between Al (001) and a (10,0) zigzag carbon nanotube, calculated by the O(N) method.
We have been applying the O(N) method to various interface problems such as electrode-electrolyte 
and metal-insulator. 
  - 
      "O(N) Krylov-subspace method for large-scale ab initio electronic structure calculations",
      T. Ozaki, Phys. Rev. B 74, 245101 (2006).