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Quantum crossover: How to distinguish single-particle and pair currents

Quantum crossover: How to distinguish single-particle and pair currents
The vertical axis is the temperature divided by the Fermi temperature, and the horizontal axis is the attractive interaction strength. The red solid curve shows the superfluid critical temperature. The blue dashed line shows characteristic temperatures between normal and pseudogap phases. The green dotted line shows the characteristic temperatures between pseudogap and bound dimer phases. (b) Schematics for the tunneling transport process in the normal phase, the pseudogap phase, and the bound dimer phases. The Fano factor, the ratio between the current noise and the current, helps us distinguish pair-current and single-particle current. Credit: Tajima et. al. 2023

If you cool down low-density atomic gas to ultralow temperatures (−273°C), you get a new state of matter called the Bose-Einstein Condensate (BEC). A BEC has strongly coupled two-atom molecules behaving like a collective wave following quantum mechanics. If you reduce the pairing strength between them—for example, by increasing the magnetic field—the atoms form Cooper pairs according to Bardeen-Cooper-Schrieffer (BCS) theory (which won a Nobel Prize).

The process is called BCS-BEC crossover. And the theory forms the basis of superfluids and superconductors, materials that do not display viscosity or . Hiroyuki Tajima and his team from the University of Tokyo proposed a new method to distinguish current carriers in the BCS-BEC crossover. The key is in the fluctuations of current.

Electronic devices display images thanks to electrons moving in a conductor—aka single-particle current. Your device may heat up due to the resistance caused by collisions of electrons in the conductor that dissipate electric energy as heat. But superconductors show zero resistance to current flow, saving lots of energy. This is possible because of paired electrons, which would have otherwise repelled each other due to their negative charge. In other words, the current in superconductors is mainly due to the pair-tunneling transport involving moving paired-current carriers rather than a single-particle current carrier.

Tajima and his team investigated the quantum transport phenomena using an ultracold Fermi . It is an artificial quantum matter mimicking an electron or fermion system with adjustable interaction strength. "To understand non-trivial transport, we need to distinguish whether single-particle tunneling or pair tunneling is dominant in strongly interacting gas," said Tajima. "The identification of single-particle tunneling and pair tunneling is vital for understanding quantum transport not only in cold atomic systems but also in ."

Because the researchers could control the interactions between particles, the atomic gas allowed them to systematically study quantum many-body physics. The gas shows a normal when the interaction strength between atoms is weak. In this phase, it behaves like a relatively good conductor such as a metal showing electrical resistance. So, one can expect a single-particle current (electron tunneling transport) under a chemical potential bias (voltage).

If you increase the interaction strength, the gas crosses over to the bound dimer phase via an in-between pseudogap phase. The pseudogap phase is where the BCS-BEC crossover happens at low temperatures. At a for a given interaction strength, the atomic gas becomes superfluid with no viscosity. Below the phase transition temperature, Cooper pairs form and lead to pair current. In the pseudogap phase, non-superfluid Cooper pairs form due to attractive interactions, which leads to anomalous current in this region. But in the bound dimer phase, pair current is predominant. Tajima's team found a way to distinguish the current carriers in each phase by measuring an observable macroscopic property.

The team showed that the fluctuations of currents, quantified as the Fano factor, can distinguish single-particle- and pair-currents in a tunneling transport of strongly interacting Fermi gases. The Fano factor value is 1 for single-particle current and 2 for pair current. In the future, their approach can be applied to other unconventional superconductors and different many-body phenomena realized in cold atoms.

Quantum crossover: How to distinguish single-particle and pair currents
Fano factor (the ratio between the current noise and the current) in ultracold Fermi gases with controllable attractive interaction strength. Credit: Tajima et. al. 2023

"Our results show that it is possible to identify the microscopic carriers from the macroscopic observables (i.e., current and noise) even in strongly correlated quantum matter," added Tajima.

"This collaboration happened completely through online discussions, which surprisingly enabled us to exchange interdisciplinary knowledge, resulting in this research."

The study is published in the journal PNAS Nexus.

More information: Hiroyuki Tajima et al, Nonequilibrium noise as a probe of pair-tunneling transport in the BCS–BEC crossover, PNAS Nexus (2023). DOI: 10.1093/pnasnexus/pgad045

Journal information: PNAS Nexus

Citation: Quantum crossover: How to distinguish single-particle and pair currents (2023, March 7) retrieved 21 February 2024 from
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