Abstract
An analytical expression for the lower bound of the average number of hyperfine component particles in the ground state of spin-1 condensates (denoted as ) under a magnetic field has been derived. In the derivation the total magnetization is kept rigorously conserved. Numerical examples are given to show the applicability of the analytical expression. It was found that, in a broad domain of parameters specified in the paper, the lower bound is very close to the actual . Thereby, in this domain, $\overset{\_\_}{% ρ_{0}}$ can be directly evaluated simply by using the analytical expression.
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