A pole of a scattering matrix arising from the numerator rather than a zero of the incoming Jost function can fail to correspond to a bound state. For , the pole at is associated with the incoming zero; the pole at comes from the numerator. The regular Eckart realization has . The distinction and this explicit example are discussed in dipot.ulb.ac.be/dspace/bitstream/2013/373712/4/2306.12216.pdf.
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