Table of Contents
- Introduction
- Overview of Ultracold Atomic Interactions
- Scattering Length and Low-Energy Collisions
- Magnetic Tuning of Interactions
- Feshbach Resonance: Basic Principle
- Open and Closed Channels
- Resonance Width and Strength
- Effective Scattering Length Formula
- Experimental Realization of Feshbach Resonances
- Species with Accessible Feshbach Resonances
- Applications in Bose Gases
- Control of Collapse and Explosion in BECs
- Feshbach Molecules and Binding Energies
- Applications in Fermi Gases
- BEC–BCS Crossover Physics
- Efimov States and Universal Few-Body Physics
- Optical and Radio-Frequency Feshbach Resonances
- Multichannel Quantum Defect Theory (MQDT)
- Limitations and Technical Challenges
- Conclusion
1. Introduction
Feshbach resonances provide a powerful method for tuning atomic interactions in ultracold gases. By varying an external magnetic field, researchers can precisely control the scattering length, enabling exploration of quantum many-body physics from weak to strong coupling regimes.
2. Overview of Ultracold Atomic Interactions
At ultralow temperatures, atomic interactions are dominated by s-wave scattering. The interaction potential can be characterized by a single parameter: the scattering length \( a \).
3. Scattering Length and Low-Energy Collisions
The s-wave scattering length \( a \) governs the low-energy behavior of the scattering amplitude:
\[
f(k) pprox -rac{a}{1 + ika}
\]
Positive \( a \): repulsive; negative \( a \): attractive; \( a = 0 \): non-interacting limit.
4. Magnetic Tuning of Interactions
A magnetic field shifts the energy of internal atomic states via the Zeeman effect. Near a resonance, the energy of a bound molecular state (closed channel) aligns with a scattering state (open channel), modifying \( a \).
5. Feshbach Resonance: Basic Principle
A Feshbach resonance occurs when the bound state of a closed channel becomes degenerate with the collisional energy of the open channel. This causes a resonant enhancement in the scattering amplitude.
6. Open and Closed Channels
- Open channel: free atom pair in an entrance channel
- Closed channel: bound molecular state in a different hyperfine configuration
Coupling between channels modifies scattering properties near resonance.
7. Resonance Width and Strength
Resonances are characterized as:
- Broad: strong coupling, large range of tunability
- Narrow: weak coupling, sensitive to field stability
The resonance strength impacts thermalization and loss rates.
8. Effective Scattering Length Formula
The scattering length near a magnetic Feshbach resonance is given by:
\[
a(B) = a_{ ext{bg}} \left( 1 – rac{\Delta}{B – B_0}
ight)
\]
where \( a_{ ext{bg}} \) is the background scattering length, \( B_0 \) is the resonance position, and \( \Delta \) is the width.
9. Experimental Realization of Feshbach Resonances
Feshbach resonances were first observed in \(^{85} ext{Rb}\) and \(^{23} ext{Na}\) using magnetic field sweeps. They are now routinely used in experiments on bosons and fermions alike.
10. Species with Accessible Feshbach Resonances
- Bosons: \(^{85} ext{Rb}\), \(^{133} ext{Cs}\), \(^{39} ext{K}\)
- Fermions: \(^{6} ext{Li}\), \(^{40} ext{K}\)
These species feature rich and well-characterized resonance spectra.
11. Applications in Bose Gases
- Tuning interaction strength to observe collapse (attractive \( a < 0 \)) and stable condensates (repulsive \( a > 0 \))
- Engineering solitons, droplets, and quantum turbulence
12. Control of Collapse and Explosion in BECs
Adjusting \( a \) can induce:
- BEC collapse at large negative \( a \)
- Controlled “Bosenova” explosions
- Stabilization via three-body loss or dipolar interactions
13. Feshbach Molecules and Binding Energies
On the attractive side of a resonance, weakly bound diatomic molecules form. These molecules serve as precursors to deeper bound states or BECs of molecules.
14. Applications in Fermi Gases
Feshbach tuning enables crossover from:
- Weakly bound Cooper pairs (BCS side, \( a < 0 \))
- Tightly bound bosonic molecules (BEC side, \( a > 0 \))
- Unitary regime (\( |a| o \infty \)): strongly interacting quantum fluid
15. BEC–BCS Crossover Physics
Ultracold fermions across a Feshbach resonance allow exploration of superfluidity, pairing gaps, vortex lattices, and pseudogap behavior in the crossover regime.
16. Efimov States and Universal Few-Body Physics
Near a Feshbach resonance, three-body systems support Efimov states—universal trimers whose energy levels follow a geometric scaling:
\[
E_n \propto e^{-2\pi n/s_0}
\]
These have been observed in three-body loss spectra.
17. Optical and Radio-Frequency Feshbach Resonances
Optical Feshbach resonances use laser-induced coupling to modify scattering length. RF fields can also induce transitions between channels, offering time-dependent interaction control.
18. Multichannel Quantum Defect Theory (MQDT)
MQDT provides a framework for modeling multi-channel scattering, allowing predictive understanding of resonance positions, widths, and universal properties.
19. Limitations and Technical Challenges
- Magnetic field noise and resolution
- Three-body loss near resonance
- Heating and stability of BEC/DFG
- Need for species-dependent calibration
20. Conclusion
Feshbach resonances have revolutionized the study of ultracold matter by enabling tunable interactions. From quantum phase transitions to universal few-body physics, they provide a key to exploring and engineering new quantum states.
