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FANG ZHAO, FU-QUAN DOU, AND QING ZHAO PHYSICAL REVIEW RESEARCH 4, 013172 (2022) FIG. 6. The maximum energy and ergotropy of a QB. (a) and (c) are the QB’s energy with the spin numbers N = 5 and N = 6, respectively. (b) and (d) are the QB’s ergotropy with the spin numbers N = 5 and N = 6, respectively. dimerization suppresses the QB energy and ergotropy in the degenerate ground state regime. However, the dimerization spin pairs have a huge occupation with a larger energy and ergotropy in the fully nondegenerate ground state regime. That means the dimerization parameters are beneficial to the energy and ergotropy of a QB on the fully nondegenerate ground state regime. Now we define the parameter R to characterize the charge capacity for the QB’s energy and ergotropy. It is defined as follows: E Reb=E −E , . (11) (12) maxε G Repb = B Emax − EG (a) 0.984 0.982 0.980 0.978 0.976 -1.0 -0.5 0.0 0.5 1.0 0.9 0.8 0.7 0.6 -1.0 -0.5 0.0 0.5 1.0 <> <!!> <""> <##> <$$> qq FIG. 7. The occupations of each spin with spin numbers N = 5. (a) and (b) are the spin occupations for hopping strengths J = 0.3 and J = 2.5, respectively. 013172-6 (b) <> <!!> <""> <##> <$$> OiPDF Image | Charging performance of the Su-Schrieffer-Heeger quantum battery
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