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  • Sturm-Schrodinger equations H psi = E W psi with H not equal H-dagger and W not equal W-dagger not equal I are considered, with a weak point of the theory lying in the purely numerical matrix-inversion form of the double-series definition of the necessary metric operator circle minus in the physical Hilbert space of states [M Znojil, J. Phys. A: Math. Theor. 41, 215304 (2008)]. This shortcoming is removed here via an amended, single-series definition of circle minus.
  • Sturm-Schrodinger equations H psi = E W psi with H not equal H-dagger and W not equal W-dagger not equal I are considered, with a weak point of the theory lying in the purely numerical matrix-inversion form of the double-series definition of the necessary metric operator circle minus in the physical Hilbert space of states [M Znojil, J. Phys. A: Math. Theor. 41, 215304 (2008)]. This shortcoming is removed here via an amended, single-series definition of circle minus. (en)
Title
  • Sturm-Schrodinger equations: Formula for metric
  • Sturm-Schrodinger equations: Formula for metric (en)
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  • Sturm-Schrodinger equations: Formula for metric
  • Sturm-Schrodinger equations: Formula for metric (en)
skos:notation
  • RIV/61389005:_____/09:00329630!RIV10-MSM-61389005
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  • P(GA202/07/1307), P(LC06002), Z(AV0Z10480505)
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  • 2
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  • 344579
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  • RIV/61389005:_____/09:00329630
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  • Crypto-Hermiticity; Sturm-Schrodinger bound-state problem; Oscillators (en)
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  • IN - Indická republika
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  • [96ABF0710F26]
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  • Pramana: journal of physics
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  • 73
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  • Znojil, Miloslav
  • Geyer, H. B.
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  • 000269548500009
http://linked.open...n/vavai/riv/zamer
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  • 0304-4289
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