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pre-rewrite: some small typo fixes
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@ -883,7 +883,7 @@ For \(n>m\) we have
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Δ_{+,-}&=2δ\\
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\label{eq:57}Δ_{n>0,-} &= n Ω_{B} + δ\\
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\label{eq:58}Δ_{n>0,+} &= n Ω_{B} - δ\\
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\label{eq:59}Δ_{n>0,m>0} &= (n-m) Ω_{B} - δ.
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\label{eq:59}Δ_{n>0,m>0} &= (n-m) Ω_{B}.
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\end{align}
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To couple exactly one other mode with \(n>0\) to the \(+\) mode, the
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RWA requires that \(\abs{Δ_{n,+}}\neq \abs{Δ_{kl}}\) for \(k\neq n\), \(l\neq +\).
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@ -1009,7 +1009,7 @@ With this, we have for \(m=\pm,-N,-N+1,\ldots,-1,1,2,\ldots,N\)
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\begin{equation}
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\label{eq:94}
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\begin{aligned}
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ω^{0}_{m\neq \pm} &= ω_{n}^{B} & ω^{0}_{\pm} &= \pm δ \cos(ψ)\\
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ω^{0}_{m\neq \pm} &= ω_{n}^{B} & ω^{0}_{\pm} &= ω_{s} \pm δ \cos(ψ)\\
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η^{0}_{m\neq\pm} &= η_{B} = η_S+2δΔ & η^{0}_{\pm} &= η_{S} + δΔ =
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\frac{η_{S}+ η_{B}}{2}.
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\end{aligned}
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