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This means that even the charger has a finite initial energy, particles in the battery cannot be excited, which leads to zero energy transfer and the battery remains uncharged

2nd excitation In the case of 2nd excitationn= 2, becauseϕ 2(x) is the even function, it is easy to verify that I2 = Z ϕ∗ 0(x)φ∗ 1(x)ϕ2(x)φ0(x)dx= 0

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Enhancing ultracold atomic batteries using tunable interactions

quant-ph · 2026-05-19 · unverdicted · novelty 5.0

Tuning charger frequency to resonance in a 1D bosonic quantum battery achieves perfect energy transfer, with many-body effects and attractive interactions enhancing charging power and efficiency over single-particle cases.

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  • Enhancing ultracold atomic batteries using tunable interactions quant-ph · 2026-05-19 · unverdicted · none · ref 4

    Tuning charger frequency to resonance in a 1D bosonic quantum battery achieves perfect energy transfer, with many-body effects and attractive interactions enhancing charging power and efficiency over single-particle cases.