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Theory and Modern Applications

Table 3 \(a=0\), the four eigenvalues with \(l=2\) and h

From: An efficient finite element method and error analysis for eigenvalue problem of Schrödinger equation with an inverse square potential on spherical domain

h

\(\lambda _{2h}^{1}\)

\(\lambda _{2h}^{2}\)

\(\lambda _{2h}^{3}\)

\(\lambda _{2h}^{4}\)

1/64

33.221527912004

82.779965293070

152.120849702143

241.466504738343

1/128

33.218478774072

82.734418406613

151.921374315241

240.893774149263

1/256

33.217716151749

82.723028162111

151.871499583334

240.750621394948

1/512

33.217525475045

82.720180381294

151.859030542575

240.714835156415

1/1024

33.217477804567

82.719468422366

151.855913260174

240.705888719943