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arXiv:0707.1036 · Physical Review A

Tunable quantum-fluctuation-controlled coherent spin dynamics

Jun Liang Song, Fei Zhou

Published Mar 27, 2008• 10 citations
arXivHTMLPDF

Abstract

Temporal evolution of a macroscopic condensate of ultracold atoms is usually driven by mean-field potentials, either due to scattering between atoms or due to coupling to external fields; and coherent quantum dynamics of this type have been observed in various cold atom experiments. In this paper, we report results of studies of a class of quantum spin dynamics which are purely driven by zero point quantum fluctuations of spin collective coordinates. Unlike the usual mean-field coherent dynamics, quantum-fluctuation-controlled spin dynamics (or QFCSD) studied here are very sensitive to variation of quantum fluctuations and the corresponding driving potentials induced by zero point motions can be tuned by four to five orders of magnitude using optical lattices. These dynamics have unique dependence on optical lattice potential depths and quadratic Zeeman fields. We also find that thermal fluctuations generally can further enhance the induced potentials although the enhancement in deep optical lattices is much less substantial than in traps or shallow lattices. QFCSD can be potentially used to calibrate quantum fluctuations and investigate correlated fluctuations and various universal scaling properties near quantum critical points.

DOI
10.1103/physreva.77.033628

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Temporal evolution of a macroscopic condensate of ultracold atoms is usually driven by mean-field potentials, either due to scattering between atoms or due to coupling to external fields; and coherent quantum dynamics of this type have been observed in various cold atom experiments. In this paper, we report results of studies of a class of quantum spin dynamics which are purely driven by zero point quantum fluctuations of spin collective coordinates. Unlike the usual mean-field coherent dynamics, quantum-fluctuation-controlled spin dynamics (or QFCSD) studied here are very sensitive to variation of quantum fluctuations and the corresponding driving potentials induced by zero point motions can be tuned by four to five orders of magnitude using optical lattices. These dynamics have unique dependence on optical lattice potential depths and quadratic Zeeman fields. We also find that thermal fluctuations generally can further enhance the induced potentials although the enhancement in deep optical lattices is much less substantial than in traps or shallow lattices. QFCSD can be potentially used to calibrate quantum fluctuations and investigate correlated fluctuations and various universal scaling properties near quantum critical points.
We have studied the quantum spin dynamics of small condensates of cold sodium atoms. For a condensate initially prepared in a mean-field ground state, we show that coherent spin dynamics is purely driven by quantum fluctuations of collective spin coordinates and can be tuned by quadratic Zeeman coupling and magnetization. This dynamics in small condensates can be probed in a high-finesse optical cavity where the temporal behaviors of the excitation spectra of a coupled condensate-photon system reveal the time evolution of populations of atoms at different hyperfine spin states.
In this thesis, we have investigated several fluctuation-driven phenomena in ultracold spinor Bose gases. In Bose-Einstein condensates of hyperfine spin-two (F=2) atoms, it is shown that zero-point quantum fluctuations completely lift the accidental continuous degeneracy in quantum spin nematic phases predicted by mean field analysis, and these fluctuations select out two distinct spin nematic states with higher symmetries. It is further shown that fluctuations can drive a novel type of coherent spin dynamics which is very sensitive to the variation of quantum fluctuations controlled by magnetic fields or potential depths in optical lattices. These results have indicated fundamental limitations of precision measurements based on mean field theories. In addition, fluctuation-driven coherent spin dynamics studied here is a promising tool to probe correlated fluctuations in many body systems. In another system -- a two-dimension superfluid of spin-one (F=1) Na²³ atoms -- we have investigated spin correlations associated with half quantum vortices. It is shown that when cold atoms become superfluid below a critical temperature a unique nonlocal topological order emerges simultaneously due to fluctuations in low dimensional systems. Our simulation have indicated that there exists a nonlocal softened pi-spin disclination structure associated with a half-quantum vortex although spin correlations are short ranged. We have also estimated fluctuation-dependent critical frequencies for half-quantum vortex nucleation in rotating optical traps. These results indicate that the strongly fluctuating ultracold spinor system is a promising candidate for studying topological orders that are the focus of many other fields.
Cold atoms in optical lattices offer an exciting new laboratory where quantum many-body phenomena can be realized in a highly controlled way. They can even serve as quantum simulators for notoriously difficult problems like high-temperature superconductivity. This review is focussed on the recent developments and new results in multi-component systems. Fermionic atoms with SU(N) symmetry have exotic superfluid and flavor-ordered ground states. We discuss symmetry breaking, collective modes, and detection issues, e.g. in Bragg scattering. On the other hand, bosonic multiflavor ensembles allow for engineering of spin Hamiltonians which are interesting from a quantum computation point of view. Finally, we address the role of disorder in optical lattices. Fermionic atoms experience Anderson localization at sufficiently strong disorder. Interactions among the atoms induce a competing tendency towards delocalization. We present a complete phase diagram obtained within dynamical mean-field theory and discuss experimental observability of the Mott and Anderson phases.
The understanding of quantum many-body physics is the key to develop new quantum technologies including novel quantum materials, high-precision sensors, and quantum computers. However, understanding the general quantum many-body physics is extremely difficult, particularly when such systems are driven far from an equilibrium state. Ultracold atoms, a clean, fully controllable, and coherent quantum many-body systems can provide useful insights into the fundamental properties of quantum matter. This thesis discusses experiments on studying nonequilibrium dynamics in driven ultracold bosonic atoms with fantastic static and dynamical controls of the inter-particle interactions through Feshbach resonances and external trapping potentials using optical lattices and digital micromirror device (DMD). With this versatile apparatus, we first study the critical dynamics across a quantum phase transition in shaken optical lattices. Across a ferromagnetic transition where the Z2\mathbb{Z}_2Z2​ inversion symmetry is broken, we are interested in how the system evolves toward the new ground states generally with a different symmetry. Utilizing the phase imprinting technique with DMD, we show that the macroscopic coherence is maintained across the phase transition, the system undergoes a coherent population transfer of particles toward lower energy states and quantum fluctuations determine the domain structure but do not destroy the macroscopic coherence. We then present the complex correlations rising from the matter-wave version of a high-harmonic generation with oscillating interaction. This high-harmonic generation of matterwave is a result of stimulated secondary collisions. The stimulated primary collisions, two condensate atoms collide absorbing one energy quantum from the oscillating field, give rise to the first observation of Bose fireworks. The scattered atoms from the primary collisions can further collide with each other or the ground-state atoms from the condensate and such secondary collisions promote atoms to higher momentum modes. Moreover, we show the density-wave dynamics prior to the jets emission within the condensate with oscillating interactions and explain the asymmetry in the jets emission pattern based on near-field interference. Besides, we further demonstrate the spatial and temporal phase coherence of the emitted jets using matter-wave interference and connect our matter-wave jets emission to the famous Unruh radiation in relativistic physics.
Quantum fluctuations are usually regarded as a background effect that perturbs classical order. In this work we propose that quantum fluctuations themselves can undergo a phase transition, a phenomenon we term the Quantum Fluctuation Phase Transition (QFPT). We develop a theoretical framework that treats the amplitude of quantum fluctuations as an order parameter, allowing a direct mapping between the fluctuation strength and the free‑energy landscape. Using a transverse‑field Ising model with tunable long‑range couplings, we derive a mean‑field free energy that exhibits a discontinuity in the fluctuation amplitude at a critical field strength. We further analyze the critical scaling, demonstrating that the QFPT belongs to a new universality class distinct from conventional quantum critical points. The theory predicts observable signatures in the low‑temperature heat capacity, dynamic structure factor, and entanglement entropy, and suggests that extreme‑cold atom or solid‑state systems with controllable interaction ranges could realize QFPTs. This novel mechanism for quantum phase change offers a route to discovering new quantum phases and could have implications for quantum technologies that rely on fluctuation‑driven properties.
We report on the observation of coherent, purely collisionally driven spin dynamics of neutral atoms in an optical lattice. For high lattice depths, atom pairs confined to the same lattice site show weakly damped Rabi-type oscillations between two-particle Zeeman states of equal magnetization, induced by spin-changing collisions. Moreover, measurement of the oscillation frequency allows for precise determination of the spin-changing collisional coupling strengths, which are directly related to fundamental scattering lengths describing interatomic collisions at ultracold temperatures.