Introduce the fixed endpoint values . The Lagrangian is
Thus , , and
This is a symmetric tridiagonal matrix, reflecting that only nearest-neighbour masses are coupled.
Expand the tridiagonal determinant along its first row. The diagonal entry contributes . In the off-diagonal cofactor, expansion along its first column supplies the other factor , and the cofactor sign makes the net contribution . Therefore
The initial values are and . Writing the same formula at forces , the empty determinant convention. This is the tridiagonal determinant recurrence.
Substitute into the recurrence. Since , its roots are nonzero and satisfy
For distinct roots, the general recurrence solution is . The initial values require and , giving
At a repeated root, and , this quotient must be replaced by its limit:
It also follows by solving the repeated-root recurrence as . This exceptional case is necessary to avoid introducing a false root in the next part; it is included in the fixed-end spring-chain determinant and its repeated-root limit.
For distinct nonzero recurrence roots, the determinant formula gives
The ratio one is excluded: at that repeated root, part (iii) gives . Thus the naive extra root corresponding to equal recurrence roots is spurious.
To count the physical solutions without ambiguity from exchanging and , write and with . Then
Its distinct zeros occur at , . They give exactly distinct positive normal frequencies, or equivalently distinct roots in :
If signed is counted, the characteristic equation has roots . The sine quotient is the Chebyshev polynomial of the second kind representation of the fixed-end spring-chain determinant and its repeated-root limit.

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