A quantum battery refers to a quantum system capable of storing and extracting energy, and it offers potential advantages in charging speed compared with classical batteries. However, the relationship between charging advantages and the intrinsic quan...
A quantum battery refers to a quantum system capable of storing and extracting energy, and it offers potential advantages in charging speed compared with classical batteries. However, the relationship between charging advantages and the intrinsic quantum features of quantum batteries has remained unclear.
We investigate how charging advantages relate to their quantum characteristics—namely, quantum entanglement, quantum coherence, and quantum global operators. We first examine the necessary conditions for achieving such charging advantages. Although the advantage can grow at most linearly with system size, it has been unclear whether global operators, all interaction operators, or both are required. We demonstrate that generic interaction operators do not contribute to quantum charging, establishing that only global operators can enhance charging performance.
We show that quantum entanglement is necessary for achieving charging advantages, while certain forms of entanglement can in fact hinder charging. We decompose the charging power into contributions from quantum entanglement and from the quantum speed limit. This allows us to characterize the entanglement-dependent contribution: it is always equal to one in the absence of entanglement and can exceed one only when entanglement is present. However, this contribution does not scale proportionally with the amount of entanglement; in particular, it returns to unity when entanglement is maximal. This indicates that only highly specific structures of entanglement can lead to enhanced charging performance.
Finally, we define a distance space that characterizes quantum charging, thereby expressing the charging speed as a geometric physical quantity. The distance we introduce coincides with the Bures angle for pure states, while it is always larger for mixed states. We also show that this distance does not scale with the system size, from which we derive that the charging advantage increases linearly with the size of the quantum system.