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1: 18.1 Notation
or the dilated Chebyshev polynomials of the first and second kinds:
C n ( x ) = 2 T n ( 1 2 x ) ,
S n ( x ) = U n ( 1 2 x ) .
2: 1.18 Linear Second Order Differential Operators and Eigenfunction Expansions
This dilatation transformation, which does require analyticity of q ( x ) in (1.18.28), or an analytic approximation thereto, leaves the poles, corresponding to the discrete spectrum, invariant, as they are, as is the branch point, actual singularities of ( z T ) 1 f , f . …
3: Bibliography S
  • B. Simon (1973) Resonances in n -body quantum systems with dilatation analytic potentials and the foundations of time-dependent perturbation theory. Ann. of Math. (2) 97, pp. 247–274.