Megascopic Quantum Phenomena
361
Quantum mechanical original symmetry
Quantum field symmetry breaking
µ = -1
µ = 0
µ = 1
a
2 a
Fig. 1 Megascopic quantum jumps between the quantum mechanical and quantum field states of
the Universe, leading to the megascopic tunnelling of superconducting carriers. nuclei with electronic core, ◯ valence electrons in symmetric quantum mechanical and asymmetric quantum field
positions, μ einselection (environment-induced superselection) factor,
a original lattice constant
before the symmetry breaking
superconductivity microscopically. First, immeasurable megascopic quantum jumps
imply non-measurability of the density and the velocity of superconducting carriers.
Second, the “teleportation” of superconducting carriers, a new kind of non-local
quantum phenomenon, guarantees the bare electronic mass in the London moment
measurements. Third, only the holistic incorporation of the environment by way of
megascopic einselection is capable of responding to the asymmetry in the form of
an external magnetic field. Henceforth there is also no contradiction to the second
form of van Fraassen’s argument, and the Meissner effect can thus be explained.
Returning to the field solutions of Fig. 1, depicting distorted nuclear positions
with the adequate electronic redistribution one realizes that the electrons form some
kind of “chemical bonds” occupied by two electrons with opposite spins. As it was
explained in the previous section, megascopic quantum jumps do not occur in time,
but time is created by them. Denoting the quantum time scale as τ , the time t = nτ will
be understood as the interval of n megascopic events, i.e. n transitions from the field
state to the complementary mechanical state and back. After two megascopic events,
considering only a one-dimensional chain, the valence orbitals occupied by the two
electrons will be relocated to new positions, which are in the following relation to
the original positions
χ i↑ (r)χ i↓ (r)
2τ
=
χ i↑ (r − 2μa)χ i↓ (r − 2μa)
0
exp(iθ (r)); μ ∈ {−1, 0, 1}
(14.11)
Here the phase θ appears at the macroscopic level, reflecting the “teleportation” of
superconducting carriers, i.e. the valence orbitals occupied by two electrons. In our
361
Quantum mechanical original symmetry
Quantum field symmetry breaking
µ = -1
µ = 0
µ = 1
a
2 a
Fig. 1 Megascopic quantum jumps between the quantum mechanical and quantum field states of
the Universe, leading to the megascopic tunnelling of superconducting carriers. nuclei with electronic core, ◯ valence electrons in symmetric quantum mechanical and asymmetric quantum field
positions, μ einselection (environment-induced superselection) factor,
a original lattice constant
before the symmetry breaking
superconductivity microscopically. First, immeasurable megascopic quantum jumps
imply non-measurability of the density and the velocity of superconducting carriers.
Second, the “teleportation” of superconducting carriers, a new kind of non-local
quantum phenomenon, guarantees the bare electronic mass in the London moment
measurements. Third, only the holistic incorporation of the environment by way of
megascopic einselection is capable of responding to the asymmetry in the form of
an external magnetic field. Henceforth there is also no contradiction to the second
form of van Fraassen’s argument, and the Meissner effect can thus be explained.
Returning to the field solutions of Fig. 1, depicting distorted nuclear positions
with the adequate electronic redistribution one realizes that the electrons form some
kind of “chemical bonds” occupied by two electrons with opposite spins. As it was
explained in the previous section, megascopic quantum jumps do not occur in time,
but time is created by them. Denoting the quantum time scale as τ , the time t = nτ will
be understood as the interval of n megascopic events, i.e. n transitions from the field
state to the complementary mechanical state and back. After two megascopic events,
considering only a one-dimensional chain, the valence orbitals occupied by the two
electrons will be relocated to new positions, which are in the following relation to
the original positions
χ i↑ (r)χ i↓ (r)
2τ
=
χ i↑ (r − 2μa)χ i↓ (r − 2μa)
0
exp(iθ (r)); μ ∈ {−1, 0, 1}
(14.11)
Here the phase θ appears at the macroscopic level, reflecting the “teleportation” of
superconducting carriers, i.e. the valence orbitals occupied by two electrons. In our