Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Physical Review A

Nonadiabatic spin transitions in an inhomogeneous magnetic field

R. D. Hight, R. T. Robiscoe, Walter R. Thorson

Published Mar 1, 1977• 25 citations
Publisher

Abstract

Model calculations are presented for nonadiabatic passage of an oriented spin through a reversing solenoidal magnetic field; these are useful for comparison with experiments described elsewhere. The model corresponds closely to the well-known Landau-Zener-Stueckelberg model of a two-state curve crossing in molecular collision theory; various modifications appropriate to the Majorana problem are considered. The resulting transition amplitudes are discussed for the $F=1$ hyperfine component of the $2^{2}S_{\frac{1}{2}}$ metastable state of atomic hydrogen as an example.

DOI
10.1103/physreva.15.1079

Related papers

Nonadiabatic transition in n=2 atomic hydrogen

R. D. Hight, R. T. Robiscoe

We present an experiment studying the nonadiabatic passage of the $F=1$ hyperfine component of the $2^{2}S_{\frac{1}{2}}$ metastable state of atomic hydrogen through a reversing solenoidal magnetic field. The nonadiabatic region is compared to the model field of Hight, Robiscoe, and Thorson. The measured transition amplitudes are fitted by the calculated amplitudes and the results are discussed.

Physical Review A•Feb 1, 1978•16 citations

Spin transitions in time-dependent magnetic fields

Frank Garisto, B. C. Sanctuary

Nonadiabatic transitions in state-selection experiments on beams of metastable hydrogen atoms ($2{S}_{\frac{1}{2}}$) display oscillations in the population of the $F=1$, $m=\ensuremath{-}1$ state R. D. Hight and R. T. Robiscoe, [Phys. Rev. A 17, 561 (1978)]. In this paper, theoretical calculations using exact and model solenoid fields averaged over a velocity distribution show that the population oscillations arise from the presence of at least two nonadiabatic regions in the solenoid. No oscillations occur theoretically if only a single nonadiabatic region exists, unless the unlikely assumption of a coherent hydrogen-atom beam is invoked.

Physical Review A•Mar 1, 1981•2 citations

The Majorana formula and the Landau–Zener–Stückelberg treatment of the avoided crossing problem

Francesco Di Giacomo, Evgeniĭ E. Nikitin

The Majorana formula for the probability of spin-flipping in a time-dependent magnetic field which almost vanishes at a certain moment is discussed in connection with the celebrated work by Landau, Zener, and Stuckelberg for nonadiabatic dynamics in the avoided crossing situation.

Physics-Uspekhi•May 31, 2005•45 citations

On Nonadiabatic Processes in Inhomogeneous Fields

Julian Schwinger

The problem of calculating nonadiabatic transition probabilities is considered. It is shown that the general G\"uttinger equations are incorrect and lead to erroneous results in any case other than that of the rotating magnetic field, which he considered. The corrected equations are applied in the calculation of the transition probabilities between the various magnetic states of a field precessing with constant angular velocity.

Physical Review•Apr 15, 1937•119 citations

Nonadiabatic coupling in cold collisions of spin-polarized metastable hydrogen atoms

Robert C. Forrey, A. Dalgarno, Yulian V. Vanne +2 more

Previous calculations of low-temperature cross sections for collisions between spin-polarized metastable hydrogen atoms are improved to include nonadiabatic radial and angular coupling at large interatomic separations. The electrostatic dipole-quadrupole interaction produces nonadiabatic radial coupling between $(2s,2p)$ and $(2p,2p)$ states, while the Coriolis interaction produces nonadiabatic angular coupling. Both of these long-range contributions are handled in a space-fixed atomic gauge that is particularly convenient for a spin-polarized system. The improved theoretical results are compared with an existing experiment.

Physical Review A•Nov 29, 2007•7 citations

Majorana’s approach to nonadiabatic transitions validates the adiabatic-impulse approximation

Polina O. Kofman, O. V. Ivakhnenko, Sergey N Shevchenko +1 more

The approach by Ettore Majorana for non-adiabatic transitions between two quasi-crossing levels is revisited and significantly extended. We rederive the transition probability, known as the Landau-Zener-Stückelberg-Majorana formula, and introduce Majorana's approach to modern readers. This result, typically referred as the Landau-Zener formula, was published by Majorana before Landau, Zener and Stückelberg. Moreover, we go well beyond previous results and we now obtain the full wave function, including its phase, which is important nowadays for quantum control and quantum information. The asymptotic wave function correctly describes the dynamics away from the avoided-level crossing, while it has limited accuracy in that region.

arXiv:2208.00481•Scientific Reports•Mar 28, 2023•29 citations
Model calculations are presented for nonadiabatic passage of an oriented spin through a reversing solenoidal magnetic field; these are useful for comparison with experiments described elsewhere. The model corresponds closely to the well-known Landau-Zener-Stueckelberg model of a two-state curve crossing in molecular collision theory; various modifications appropriate to the Majorana problem are considered. The resulting transition amplitudes are discussed for the F=1F=1F=1 hyperfine component of the 22S122^{2}S_{\frac{1}{2}}22S21​​ metastable state of atomic hydrogen as an example.
We present an experiment studying the nonadiabatic passage of the F=1F=1F=1 hyperfine component of the 22S122^{2}S_{\frac{1}{2}}22S21​​ metastable state of atomic hydrogen through a reversing solenoidal magnetic field. The nonadiabatic region is compared to the model field of Hight, Robiscoe, and Thorson. The measured transition amplitudes are fitted by the calculated amplitudes and the results are discussed.
Nonadiabatic transitions in state-selection experiments on beams of metastable hydrogen atoms (2S122{S}_{\frac{1}{2}}2S21​​) display oscillations in the population of the F=1F=1F=1, $m=\ensuremath{-}1$ state R. D. Hight and R. T. Robiscoe, [Phys. Rev. A 17, 561 (1978)]. In this paper, theoretical calculations using exact and model solenoid fields averaged over a velocity distribution show that the population oscillations arise from the presence of at least two nonadiabatic regions in the solenoid. No oscillations occur theoretically if only a single nonadiabatic region exists, unless the unlikely assumption of a coherent hydrogen-atom beam is invoked.
Previous calculations of low-temperature cross sections for collisions between spin-polarized metastable hydrogen atoms are improved to include nonadiabatic radial and angular coupling at large interatomic separations. The electrostatic dipole-quadrupole interaction produces nonadiabatic radial coupling between (2s,2p)(2s,2p)(2s,2p) and (2p,2p)(2p,2p)(2p,2p) states, while the Coriolis interaction produces nonadiabatic angular coupling. Both of these long-range contributions are handled in a space-fixed atomic gauge that is particularly convenient for a spin-polarized system. The improved theoretical results are compared with an existing experiment.
The approach by Ettore Majorana for non-adiabatic transitions between two quasi-crossing levels is revisited and significantly extended. We rederive the transition probability, known as the Landau-Zener-Stückelberg-Majorana formula, and introduce Majorana's approach to modern readers. This result, typically referred as the Landau-Zener formula, was published by Majorana before Landau, Zener and Stückelberg. Moreover, we go well beyond previous results and we now obtain the full wave function, including its phase, which is important nowadays for quantum control and quantum information. The asymptotic wave function correctly describes the dynamics away from the avoided-level crossing, while it has limited accuracy in that region.