Hiptmair–Xu preconditioner

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In mathematics, Hiptmair–Xu (HX) preconditioners[1] are preconditioners for solving and problems based on the auxiliary space preconditioning framework.[2] An important ingredient in the derivation of HX preconditioners in two and three dimensions is the so-called regular decomposition, which decomposes a Sobolev space function into a component of higher regularity and a scalar or vector potential. The key to the success of HX preconditioners is the discrete version of this decomposition, which is also known as HX decomposition. The discrete decomposition decomposes a discrete Sobolev space function into a discrete component of higher regularity, a discrete scale or vector potential, and a high-frequency component.

HX preconditioners have been used for accelerating a wide variety of solution techniques, thanks to their highly scalable parallel implementations, and are known as AMS[3] and ADS[4] precondition. HX preconditioner was identified by the U.S. Department of Energy as one of the top ten breakthroughs in computational science[5] in recent years. Researchers from Sandia, Los Alamos, and Lawrence Livermore National Labs use this algorithm for modeling fusion with magnetohydrodynamic equations.[6] Moreover, this approach will also be instrumental in developing optimal iterative methods in structural mechanics, electrodynamics, and modeling of complex flows.

HX preconditioner for edit

Consider the following   problem: Find   such that

  with  .

The corresponding matrix form is

 

The HX preconditioner for   problem is defined as

 

where  is a smoother (e.g., Jacobi smoother, Gauss–Seidel smoother),   is the canonical interpolation operator for   space,   is the matrix representation of discrete vector Laplacian defined on  ,  is the discrete gradient operator, and   is the matrix representation of the discrete scalar Laplacian defined on  . Based on auxiliary space preconditioning framework, one can show that

 

where   denotes the condition number of matrix  .

In practice, inverting   and   might be expensive, especially for large scale problems. Therefore, we can replace their inversion by spectrally equivalent approximations,   and  , respectively. And the HX preconditioner for   becomes  

HX Preconditioner for edit

Consider the following   problem: Find  

 with  .

The corresponding matrix form is

 

The HX preconditioner for   problem is defined as

 

where   is a smoother (e.g., Jacobi smoother, Gauss–Seidel smoother),  is the canonical interpolation operator for   space,   is the matrix representation of discrete vector Laplacian defined on  , and   is the discrete curl operator.

Based on the auxiliary space preconditioning framework, one can show that

 

For   in the definition of  , we can replace it by the HX preconditioner for   problem, e.g.,  , since they are spectrally equivalent. Moreover, inverting   might be expensive and we can replace it by a spectrally equivalent approximations  . These leads to the following practical HX preconditioner for  problem,

 

Derivation edit

The derivation of HX preconditioners is based on the discrete regular decompositions for  and  , for the completeness, let us briefly recall them.

Theorem:[Discrete regular decomposition for  ]

Let   be a simply connected bounded domain. For any function  , there exists a vector ,  ,  , such that  and 

Theorem:[Discrete regular decomposition for  ] Let   be a simply connected bounded domain. For any function  , there exists a vector   ,     such that   and  

Based on the above discrete regular decompositions, together with the auxiliary space preconditioning framework, we can derive the HX preconditioners for   and   problems as shown before.

References edit

  1. ^ Hiptmair, Ralf; Xu, Jinchao (2007-01-01). "{Nodal auxiliary space preconditioning in $backslash$bf H($backslash$bf curl) and $backslash$bf H($backslash$rm div)} spaces". SIAM J. Numer. Anal. ResearchGate: 2483. doi:10.1137/060660588. Retrieved 2020-07-06.
  2. ^ J.Xu, The auxiliary space method and optimal multigrid preconditioning techniques for unstructured grids. Computing. 1996;56(3):215–35.
  3. ^ T. V. Kolev, P. S. Vassilevski, Parallel auxiliary space AMG for H (curl) problems. Journal of Computational Mathematics. 2009 Sep 1:604–23.
  4. ^ T.V. Kolev, P.S. Vassilevski. Parallel auxiliary space AMG solver for H(div) problems. SIAM Journal on Scientific Computing. 2012;34(6):A3079–98.
  5. ^ Report of The Panel on Recent Significant Advancements in Computational Science, https://science.osti.gov/-/media/ascr/pdf/program-documents/docs/Breakthroughs_2008.pdf
  6. ^ E.G. Phillips, J. N. Shadid, E.C. Cyr, S.T. Miller, Enabling Scalable Multifluid Plasma Simulations Through Block Preconditioning. In: van Brummelen H., Corsini A., Perotto S., Rozza G. (eds) Numerical Methods for Flows. Lecture Notes in Computational Science and Engineering, vol 132. Springer, Cham 2020.