Quantum revival explained

In quantum mechanics, the quantum revival^[1] is a periodic recurrence of the quantum wave functionfrom its original form during the time evolution either many times in space as the multiple scaled fractionsin the form of the initial wave function (fractional revival) or approximately or exactly to its original form from the beginning (full revival). The quantum wave function periodic in time exhibits therefore the full revival every period. The phenomenon of revivals is most readily observable for the wave functions being well localized wave packets at the beginning of the time evolution for example in the hydrogen atom. For Hydrogen, the fractional revivals show up as multiple angular Gaussian bumps around the circle drawn by the radial maximum of leading circular state component (that with the highest amplitude in the eigenstate expansion) of theoriginal localized state and the full revival as the original Gaussian.^[2] The full revivals are exact for the infinite quantum well, harmonic oscillator or the hydrogen atom, while for shorter times are approximate for the hydrogen atom and a lot of quantum systems.^[3]

The plot of collapses and revivals of quantum oscillations of the JCM atomic inversion.^[4]

Example - arbitrary truncated wave function of the quantum system with rational energies

Consider a quantum system with the energies

E _{i} and the eigenstates \psi _{i} H \psi _{i} = E _{i} \psi _{i}

and let the energies be the rational fractions of some constant

C E _{i=} C {M _{i} \over N _{i}} M _{i=1} , N ^{2} _{i = i} , C =-13 . 6 eV .

Then the truncated (till

N _{max} of states) solution of the time dependent Schrödinger equation is\Psi(t) = \sum ^{N _{max}} _{i =0} a _{i} e ^{- i {{E _{i}} \over \hbar} t} \psi _{i}

.

Let

L _{cm} be to lowest common multiple of all N _{i} and L _{cd} greatest common divisor of all M _{i} then for each N _{i} the {L _{cm} }/ N_i is an integer, for each M _{i} the {M _{i} }/ L_ is an integer, 2 \pi M _{i} {L _{cm} }/(N_i L_) is the full multiple of 2 \pi angle and\Psi(t) = \Psi(t + T)

after the full revival time time

T = { 2 \pi \hbar \over {L _{cd} C}} L _{cm} .

For the quantum system as small as Hydrogen and

N _{max} as small as 100 it may take quadrillions of years till it will fully revive. Especially once created by fields the Trojan wave packet in ahydrogen atom exists without any external fieldsstroboscopically and eternally repeating itself after sweeping almost the whole hypercube of quantum phases exactly every full revival time.

The striking consequence is that no finite-bit computer can propagate the numerical wave function accurately for the arbitrarily long time. If the processor number is n-bit long floating point number then the number can be stored by the computer only with the finite accuracy after the comma and the energy is (up to 8 digits after the comma) for example 2.34576893 = 234576893/100000000 and as the finite fraction itis exactly rational and the full revival occurs for any wave function of any quantum system after the time

t/ 2 \pi =100000000 which is its maximum exponent and so on that may not be true for all quantum systems or all stationary quantum systems undergo the full and exact revival numerically.

In the system with the rational energies i.e. where the quantum exact full revival exists its existence immediately proves the quantum Poincaré recurrence theorem and the time of the full quantum revival equals to the Poincaré recurrence time. While the rational numbers are dense in real numbers and the arbitrary function of the quantum number can be approximated arbitrarily exactly with Padé approximants with the coefficients of arbitrary decimal precision for the arbitrarily long time each quantum system therefore revives almost exactly. It also means that the Poincaré recurrence and the full revival is mathematically the same thing^[5] and it is commonly accepted that the recurrence is called the full revival if it occurs after the reasonable and physically measurable time that is possible to be detected by the realistic apparatus and this happens due to a very special energy spectrum having a large basic energy spacing gap of which the energies are arbitrary (not necessarily harmonic) multiples.

See also

• Poincaré recurrence theorem

Notes and References

1. J.H. Eberly . N.B. Narozhny . J.J. Sanchez-Mondragon . amp . 1980. Periodic spontaneous collapse and revival in a simple quantum model. Phys. Rev. Lett.. 44. 20. 1323–1326. 10.1103/PhysRevLett.44.1323 . 1980PhRvL..44.1323E.
2. Z. Dacic Gaeta . C. R. Stroud, Jr. . amp . 1990. Classical and quantum mechanical dynamics of quasiclassical state of a hydrogen atom. Phys. Rev. A. 42. 11. 6308–6313. 10.1103/PhysRevA.42.6308. 9903927 . 1990PhRvA..42.6308G.
3. Nonsmooth and level-resolved dynamics illustrated with a periodically driven tight binding model . 2014 . Zhang . Jiang-Min . Haque . Masudul . Scienceopen Research . 10.14293/S2199-1006.1.SOR-PHYS.A2CEM4.v1 . 1404.4280. 57487218 . free .
4. A. A. Karatsuba . E. A. Karatsuba . A resummation formula for collapse and revival in the Jaynes–Cummings model. 195304, 16. J. Phys. A: Math. Theor.. 42. 2009. 19 . 10.1088/1751-8113/42/19/195304. 2009JPhA...42s5304K . 120269208 .
5. P. . Bocchieri . A. . Loinger . Quantum Recurrence Theorem . . 107 . 2 . 337–338 . 1957 . 10.1103/PhysRev.107.337 . 1957PhRv..107..337B .