Monotonic binding conjecture for bosonic electron numbers

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Let Z>0Z>0 be a nuclear charge, let Nmax(Z)N_{\mathrm{max}}(Z) be the maximum number of bosonic electrons that a nucleus of charge ZZ can bind, and write ΨBose(Z,N)\Psi^{(Z,N)}_{\mathrm{Bose}} for a proper NN-body ground-state wave function of the Coulomb Hamiltonian.

Monotonic binding conjecture. A proper NN-body ground-state wave function ΨBose(Z,N)\Psi^{(Z,N)}_{\mathrm{Bose}} exists for every integer NN satisfying

1≤N≤Nmax(Z).1\leq N\leq N_{\mathrm{max}}(Z).

Equivalently, if the nucleus binds NN electrons, it also binds every smaller positive number of electrons. This is stated as an open problem in the cited literature and is known from Zhislin's theorem only in the range N<Z+2N<Z+2.

References

Primary source

Michael K. -H. Kiessling, “The Hartree limit of Born's ensemble for the ground state of a bosonic atom or ion”, arXiv:1204.2511 (2012).

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