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https://github.com/vale981/notes_io_loop
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small fixes in the io writeup
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1 changed files with 9 additions and 10 deletions
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@ -17,8 +17,8 @@ headinclude=true,footinclude=false,BCOR=0mm]{scrartcl}
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\newcommand{\inputf}[0]{\ensuremath{\mathrm{in}}}
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\newcommand{\inputf}[0]{\ensuremath{\mathrm{in}}}
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\newcommand{\outputf}[0]{\ensuremath{\mathrm{out}}}
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\newcommand{\outputf}[0]{\ensuremath{\mathrm{out}}}
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\usetikzlibrary{math}
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\usetikzlibrary{math}
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\usetikzlibrary{external}
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% \usetikzlibrary{external}
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\tikzexternalize[prefix=tikz/]
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% \tikzexternalize[prefix=tikz/]
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\usepackage{pgfplots}
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\usepackage{pgfplots}
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\begin{document}
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\begin{document}
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@ -97,7 +97,7 @@ Transforming the \(h_{m}\) according to
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where
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where
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\begin{equation}
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\begin{equation}
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\label{eq:35}
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\label{eq:35}
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O_{nγ}(t)\equiv O_{nγ}\eu^{\iu ε_{n}t}
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O^\ast_{nγ}(t)\equiv O^\ast_{nγ}\eu^{-\iu ε_{n}t}
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\end{equation}
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\end{equation}
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leaves us with a very simple Hamiltonian.
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leaves us with a very simple Hamiltonian.
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@ -465,9 +465,9 @@ first diagonalize \(V^{0}_{mn} + δ_{mn}\pqty{ε_{m}-i η_{m}}\)
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to obtain \(O_{mγ}(t)\) and find
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to obtain \(O_{mγ}(t)\) and find
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\begin{equation}
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\begin{equation}
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\label{eq:32}
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\label{eq:32}
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\dot{d}_{γ} = ∑_{m}O^{\ast}_{mγ}\dot{\tilde{c}}_{m} =
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\dot{d}_{γ} = ∑_{m}\pqty{O^{-1}(t)}_{γm}\dot{\tilde{c}}_{m} =
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-\iu\bqty{\pqty{ω_{γ} - \iu \tilde{η}_{γ}}d_{γ} +
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-\iu\bqty{\pqty{ω_{γ} - \iu \tilde{η}_{γ}}d_{γ} +
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∑_{σ=\pm}∑_{m}O^{\ast}_{mγ}(t)\frac{g_{m,σ}^\ast }{\sqrt{ω_{m}^{0}}} \eu^{\iu ω_{m}^{0}t}
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∑_{σ=\pm}∑_{m}\pqty{O^{-1}(t)}_{γm}\frac{g_{m,σ}^\ast }{\sqrt{ω_{m}^{0}}} \eu^{\iu ω_{m}^{0}t}
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b_{\inputf,σ}^{m}(t)}.
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b_{\inputf,σ}^{m}(t)}.
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\end{equation}
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\end{equation}
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@ -487,10 +487,10 @@ constant. With these considerations in mind we can simplify
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and
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and
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\begin{gather}
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\begin{gather}
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\label{eq:34}
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\label{eq:34}
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\dot{d}_{γ} = ∑_{m}O^{\ast}_{mγ}\dot{\tilde{c}}_{m} =
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\dot{d}_{γ} =
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-\iu\bqty{\pqty{ω_{γ}-\iu \tilde{η}_{γ}}d_{γ} + \sqrt{κ} ∑_{σ=\pm}
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-\iu\bqty{\pqty{ω_{γ}-\iu \tilde{η}_{γ}}d_{γ} + \sqrt{κ} ∑_{σ=\pm}
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U^{\pm}_{γ}(t) \frac{b_{\inputf}(t)}{\sqrt{ω_{0}}}}\\
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U^{\pm}_{γ}(t) \frac{b_{\inputf}(t)}{\sqrt{ω_{0}}}}\\
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U^{σ}_{γ}(t) = ∑_{m,β} δ_{\sgn({β}),σ}U^\ast_{βm}O^\ast_{mγ}(t) \eu^{\iu ω_{m}^{0}t}= ∑_{m,β} δ_{\sgn({β}),σ}U^\ast_{βm}O^\ast_{mγ} \eu^{\iu (ω_{m}^{0}-ε_{m})t}.
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U^{σ}_{γ}(t) = ∑_{m,β} δ_{\sgn({β}),σ}U^\ast_{βm}\pqty{O^{-1}(t)}_{γm} \eu^{\iu ω_{m}^{0}t}= ∑_{m,β} δ_{\sgn({β}),σ}U^\ast_{βm}\pqty{O^{-1}}_{γm}\eu^{\iu (ω_{m}^{0}-ε_{m})t}.
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\end{gather}
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\end{gather}
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These simplifications still capture the essence of the physics, as
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These simplifications still capture the essence of the physics, as
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@ -729,7 +729,7 @@ To maximize the residual rotating terms, the minimum of the
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Δ_{\max}\equiv \max_{δ}Δ_{\min}(δ) = \max_{δ}\min\Bqty{2δ, \abs{Ω_{B}-δ}, \abs{Ω_{B}-3δ},
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Δ_{\max}\equiv \max_{δ}Δ_{\min}(δ) = \max_{δ}\min\Bqty{2δ, \abs{Ω_{B}-δ}, \abs{Ω_{B}-3δ},
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\abs{2Ω_{B}-3δ}, \abs{Ω_{B}-2δ}}.
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\abs{2Ω_{B}-3δ}, \abs{Ω_{B}-2δ}}.
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\end{equation}
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\end{equation}
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We find that \(Δ_{\max}=Ω_{B}/4\) for
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We find that \(Δ_{\max}=2Ω_{B}/5\) for
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\begin{equation}
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\begin{equation}
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\label{eq:63}
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\label{eq:63}
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δ_{\mathrm{opt}}=Ω_{B}/5,
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δ_{\mathrm{opt}}=Ω_{B}/5,
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@ -748,7 +748,6 @@ as can be ascertained from \cref{fig:delta_choice}.
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xtick = {0}, ytick = \empty,
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xtick = {0}, ytick = \empty,
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clip = false,
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clip = false,
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xtick={},ytick={},
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xtick={},ytick={},
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tick num = 10,
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minor tick num=5,
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minor tick num=5,
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grid=both,
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grid=both,
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grid style={line width=.1pt, draw=gray!10},
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grid style={line width=.1pt, draw=gray!10},
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@ -760,7 +759,7 @@ as can be ascertained from \cref{fig:delta_choice}.
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y label style={at={(axis description cs:-0.06,.5)},rotate=90,anchor=south},
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y label style={at={(axis description cs:-0.06,.5)},rotate=90,anchor=south},
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]
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]
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\addplot[domain = 0:1, restrict y to domain = 0:1, samples =
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\addplot[domain = 0:1, restrict y to domain = 0:1, samples =
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1000, color = cerulean]{min(2*x, 1-x, abs(1-3*x), abs(2-3*x),
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1000]{min(2*x, 1-x, abs(1-3*x), abs(2-3*x),
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abs(1-2*x))};
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abs(1-2*x))};
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\addplot[color = black, mark = *, only marks, mark size = 3pt]
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\addplot[color = black, mark = *, only marks, mark size = 3pt]
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coordinates {(.2, .4)};
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coordinates {(.2, .4)};
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