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SciCode / 70.8 / Write a function to compute the 3×3 evolution operator as defined in…
Problem
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step background
Background
The evolution operator is . If we discard the global phase, we are left with .
Plain-text mathematical notation (without MathML)
Background The evolution operator is U₃(L)=e^(−iH₃L)= e^(−ih₀1L)e^(−ih_(k)λ^(k)L). If we discard the global phase, we are left with U₃(L)=e^(−ih_(k)λ^(k)L).
Original LaTeX notation
Background
The evolution operator is $\mathbb{U}_{3}(L)=e^{-i H_{3} L}=$ $e^{-i h_{0} \mathbb{1} L} e^{-i h_{k} \lambda^{k} L}$. If we discard the global phase, we are left with $\mathbb{U}_{3}(L)=e^{-i h_{k} \lambda^{k} L}$.step description prompt
Write a function to compute the evolution operator as defined in the previous prompt (). Then compute the oscillation probabilities of the three neutrino oscillation problem using the expression , where is one of electron neutrino (), muon neutrino () or tau neutrino (). Use
$\nu_{e}=\left(\begin{array}{lll}1 & 0 & 0\end{array}\right)^{\mathrm{T}}, \nu_{\mu}=\left(\begin{array}{lll}0 & 1 & 0\end{array}\right)^{\mathrm{T}}$, and $\nu_{\tau}=\left(\begin{array}{lll}0 & 0 & 1\end{array}\right)^{\mathrm{T}}$. Return the probabilities in a list in the following order : , , and .Plain-text mathematical notation (without MathML)
Write a function to compute the 3×3 evolution operator as defined in the previous prompt (). Then compute the oscillation probabilities of the three neutrino oscillation problem using the expression P_(ν_(α)→ν_(β))(L)=|ν_(β)^(†)U₃(L)ν_(α)|², where ν is one of electron neutrino (e), muon neutrino (μ) or tau neutrino (τ). Use $\nu_{e}=\left(\begin{array}{lll}1 & 0 & 0\end{array}\right)^{\mathrm{T}}, \nu_{\mu}=\left(\begin{array}{lll}0 & 1 & 0\end{array}\right)^{\mathrm{T}}$, and $\nu_{\tau}=\left(\begin{array}{lll}0 & 0 & 1\end{array}\right)^{\mathrm{T}}$. Return the probabilities in a list in the following order : e→e/μ/τ, μ→e/μ/τ, and τ→e/μ/τ.Original LaTeX notation
Write a function to compute the $3 \times 3$ evolution operator as defined in the previous prompt (). Then compute the oscillation probabilities of the three neutrino oscillation problem using the expression $P_{\nu_{\alpha} \rightarrow \nu_{\beta}}(L)=\left|\nu_{\beta}^{\dagger} U_{3}(L) \nu_{\alpha}\right|^{2}$, where $\nu$ is one of electron neutrino ($e$), muon neutrino ($\mu$) or tau neutrino ($\tau$). Use $\nu_{e}=\left(\begin{array}{lll}1 & 0 & 0\end{array}\right)^{\mathrm{T}}, \nu_{\mu}=\left(\begin{array}{lll}0 & 1 & 0\end{array}\right)^{\mathrm{T}}$, and $\nu_{\tau}=\left(\begin{array}{lll}0 & 0 & 1\end{array}\right)^{\mathrm{T}}$. Return the probabilities in a list in the following order : $e \to e/\mu/\tau$, $\mu \to e/\mu/\tau$, and $\tau \to e/\mu/\tau$.Discussion
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