 Hands-On Exercises

# Exercise 7: Use of Deflation Subspaces

The term deflation refers to the use of the knowledge of one or more eigenpairs to find other eigenpairs. For instance, most eigensolvers try to approximate a number of eigenpairs and, as soon as one of them has converged, they deflate it for better approximating the other ones. Another case is when one eigenpair is known a priori and one wants to use this knowledge to compute other eigenpairs. SLEPc supports this by means of deflation subspaces.

This example illustrates the use of deflation subspaces to compute the smallest nonzero eigenvalue of the Laplacian of a graph corresponding to a 2-D regular mesh. The problem is a standard symmetric eigenproblem Ax=λx, where A = L(G) is the Laplacian of graph G, defined as follows: Aii = degree of node i, Aij = -1 if edge (i,j) exists in G, zero otherwise. This matrix is symmetric positive semidefinite and singular, and [1 1 ... 1]T is the eigenvector associated with the zero eigenvalue. In graph theory, one is usually interested in computing the eigenvector associated with the next eigenvalue (the so-called Fiedler vector).

## Compiling

Copy the file ex11.c [plain text] to your directory and add these lines to the makefile

```ex11: ex11.o
\${RM} ex11.o
```

Note: In the above text, the blank space in the 2nd and 3rd lines represents a tab.

Build the executable with the command

```\$ make ex11
```

## Source Code Details

This example computes the smallest eigenvalue by setting `EPS_SMALLEST_REAL` in EPSSetWhichEigenpairs. An alternative would be to use a shift-and-invert spectral transformation with a zero target to compute the eigenvalues closest to the origin, or to use harmonic extraction with a zero target.

By specifying a deflation subspace (the one associated to the eigenvector [1 1 ... 1]T) with the function EPSSetDeflationSpace, the convergence to the zero eigenvalue is avoided. Thus, the program should compute the smallest nonzero eigenvalues.

## Running the Program

Run the program simply with

```\$ ./ex11
```

For the case of using an inexact spectral transformation, the command line would be:

```\$ ./ex11 -eps_target 0.0 -eps_target_real -st_type sinvert
-st_ksp_rtol 1e-10 -st_ksp_type gmres -st_pc_type jacobi
```

Note that a shift-and-invert spectral transformation should always be used in combination with `EPS_TARGET_MAGNITUDE` or `EPS_TARGET_REAL`.

And for the case of harmonic extraction:

```\$ ./ex11 -eps_target 0.0 -eps_target_real -eps_harmonic
```
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