Abstract:We study multipoint scatterers with zero-energy bound states in three dimensions. We present examples of such scatterers with multiple zero eigenvalue or with strong multipole localization of zero-energy bound states.
“…The more active the metal element, and the poorer its capacity to attract electrons, the bigger the nonmetal element's electronegativity; this was consistent with the fact that the XPS peak for FeCo-SA/DABCO changes to higher binding energy. [46][47][48] Previous research revealed that in transition metal monosulfides, the S 2p XPS peak appears as a quasi-single peak, but in disulfides, the existence of an equal intensity doublet is a distinct peak. According to Fig.…”
“…The more active the metal element, and the poorer its capacity to attract electrons, the bigger the nonmetal element's electronegativity; this was consistent with the fact that the XPS peak for FeCo-SA/DABCO changes to higher binding energy. [46][47][48] Previous research revealed that in transition metal monosulfides, the S 2p XPS peak appears as a quasi-single peak, but in disulfides, the existence of an equal intensity doublet is a distinct peak. According to Fig.…”
“…It is important that for the multipoint scatterers the scattering eigenfunctions and scattering amplitudes are calculated explicitly (see, for example, [2,15,16]). Let…”
Section: Preliminariesmentioning
confidence: 99%
“…. , n, the strength ε j of the point scatterer ε j δ(x − y j ) in (1.2) is encoded by a real parameter α j ; see, also, for example, [2,16].…”
Section: Preliminariesmentioning
confidence: 99%
“…These "renormalized" δ-functions for d = 2, 3 are known as Bethe-Peierls-Fermi-Zeldovich-Beresin-Faddeev-type point scatterers. Exact definitions for the multipoint scatterers in dimensions d = 2, 3 can be found in [2,15,16]. Historically, mathematical definitions of point scatterers in dimension d = 3 go back to [5,4].…”
Section: Introductionmentioning
confidence: 99%
“…. , n, the strength ε j of the point scatterer ε j δ(x − y j ) in (1.2) is encoded by α j , see, for example, [2,16]. If α j = ∞, then ǫ j = 0 (and the corresponding single point scatterer vanishes).…”
We study the transmission eigenvalues for the multipoint scatterers of the Bethe-Peierls-Fermi-Zeldovich-Beresin-Faddeev type in dimensions d = 2 and d = 3. We show that for these scatterers: 1) each positive energy E is a transmission eigenvalue (in the strong sense) of infinite multiplicity; 2) each complex E is an interior transmission eigenvalue of infinite multiplicity. The case of dimension d = 1 is also discussed.
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