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  • It is known that the Heisenberg and Robertson-Schrodinger uncertainty relations can be replaced by sharper uncertainty relations in which the %22classical%22 (depending on the gradient of the phase of the wave function) and %22quantum%22 (depending on the gradient of the envelope of the wave function) parts of the variances <(Delta x)^2> and a<(Delta p)(2)> are separated. In this paper, three types of uncertainty relations for a different number of classical parts (2, 1 or 0) with different time behaviour of their left-hand and right-hand sides are discussed. For the Gaussian wave packet and two classical parts, the left-hand side of the corresponding relations increases for t -> infinity as t ^2 and is much larger than hbar^2/4. For one classical part, the left-hand side of the corresponding relation goes to the right-hand side equal to hbar^2/4. For no classical part, both the right-hand and left-hand sides of the corresponding relation go quickly to zero. Therefore, the well-known limitations following from the usual uncertainty relations can be overcome in the corresponding measurements.
  • It is known that the Heisenberg and Robertson-Schrodinger uncertainty relations can be replaced by sharper uncertainty relations in which the %22classical%22 (depending on the gradient of the phase of the wave function) and %22quantum%22 (depending on the gradient of the envelope of the wave function) parts of the variances <(Delta x)^2> and a<(Delta p)(2)> are separated. In this paper, three types of uncertainty relations for a different number of classical parts (2, 1 or 0) with different time behaviour of their left-hand and right-hand sides are discussed. For the Gaussian wave packet and two classical parts, the left-hand side of the corresponding relations increases for t -> infinity as t ^2 and is much larger than hbar^2/4. For one classical part, the left-hand side of the corresponding relation goes to the right-hand side equal to hbar^2/4. For no classical part, both the right-hand and left-hand sides of the corresponding relation go quickly to zero. Therefore, the well-known limitations following from the usual uncertainty relations can be overcome in the corresponding measurements. (en)
Title
  • Internal Structure of the Heisenberg and Robertson-Schrodinger Uncertainty Relations
  • Internal Structure of the Heisenberg and Robertson-Schrodinger Uncertainty Relations (en)
skos:prefLabel
  • Internal Structure of the Heisenberg and Robertson-Schrodinger Uncertainty Relations
  • Internal Structure of the Heisenberg and Robertson-Schrodinger Uncertainty Relations (en)
skos:notation
  • RIV/00216208:11320/13:10173454!RIV14-MSM-11320___
http://linked.open...avai/riv/aktivita
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  • 80799
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  • RIV/00216208:11320/13:10173454
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  • Three types of uncertainty relations; Uncertainty relations; Quantum mechanics (en)
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  • US - Spojené státy americké
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  • [8FC5E58BFC30]
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  • International Journal of Theoretical Physics
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  • 52
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  • Skála, Lubomír
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  • 000324099800004
issn
  • 0020-7748
number of pages
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  • 10.1007/s10773-013-1640-1
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  • 11320
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