In part I of this work we defined a Titchmarsh-Weyl-coefficient M(X) for singular I( hermitian systems of arbitrary deficiency index. This construction proceeded by the method of von Nmmann for selfadjoint extensions of symmetric operators. In this part we show how a Titchmarsh-Wuyl coefficient f i ( X ) defined by a limit of Titchmarsh-Weyl coefficiente on compact intervals is Iuliited to our M(X). Examplea are given in the intermediate deficiency index case which show that IWI. all limits of Titchmarsh -Weyl coefficients on compact intervals give rise to a singular selfadjoint Iiwblern. I . IntroductionIn [7] the Titchmarsh -Weyl coefficient was defined for separated selfadjoint boundnry conditons for a singular Shermitian system. This was accomplished by a con-~t.ruction using the von Neumann theory of selfadjoint extensions of symmetric opernl.ors. For the details concerning the assumptions and the notations we refer to [7], wj)ecially to Theorem 4.7.The traditional method of defining the Titchmarsh -Weyl coefficient is to define it for a regular problem on a compact subinterval [a,c] of [a,b) and then investigate the Jliriit for c -t b. In the minimal deficiency index case, that means 76 = 0 (for the tldinition of q, see (3.1) in [7]) the method is quite satisfactory, since the limit for v --+ b is unique and independent of the boundary condition imposed on the regular lriidpoint c. This method can also be made satisfactory for the maximal deficiency Itidex case, that is n = m. For details we refer to [4, 51 as well as to [2].

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MACI in the PF joint with concurrent correction of PF maltracking if required leads to similar clinical and radiological outcomes compared with MACI on the femoral condyles.

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