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CritPt / Challenge_30_main / Let H_(b), H_(B), H_(f), H_(P) each be a finite-dimensional Hilbert space, with…

Problem

Answer published by the source. Consult the official source to check your work against its answer.

code template

Code

import sympy as sp
from sympy.physics.quantum import Ket, Bra, Dagger

phi = Ket('phi')
psi = Ket('psi')
phi_star = Ket('phi*')
psi_star = Ket('psi*')
d_P, d_B = sp.symbols('d_P d_B')
d = sp.symbols('d')

def answer(phi, psi, phi_star, psi_star, d_P, d_B, d):
    r"""
    Return the expression of \overline{\lvert \langle\phi|V^\dagger V|\psi\rangle \rvert^2} in Sympy format.

    Inputs
    ----------
    phi: sympy.Symbol, state vector |\phi\rangle_b
    psi: sympy.Symbol, state vector |\psi\rangle_b
    phi_star: sympy.Symbol, state vector |\phi^*\rangle_b
    psi_star: sympy.Symbol, state vector |\psi^*\rangle_b
    d_P: sympy.Symbol, $d_P := \dim H_P$
    d_B: sympy.Symbol, $d_B := \dim H_B$
    d: sympy.Symbol, $d = \dim(H_b \otimes H_f)$

    Outputs
    ----------
    expr: sympy.Expr, \overline{\lvert \langle\phi|V^\dagger V|\psi\rangle \rvert^2},
        where the overline indicates the average over $O$.
    """

    # ------------------ FILL IN YOUR RESULTS BELOW ------------------
    expr = ...  # a SymPy expression of inputs
    # ---------------------------------------------------------------

    return expr

problem description

# Problem setup: Let HbH_b, HBH_B, HfH_f, HPH_P each be a finite-dimensional Hilbert space, with dimHb>dimHB\dim H_b > \dim H_B and dim(HbHf)=dim(HBHP)\dim(H_b \otimes H_f) = \dim(H_B \otimes H_P). Define the linear map V:HbHBV: H_b \to H_B as follows, \begin{equation} V = \sqrt{\dim(H_P)} \langle 0|_P O |0\rangle_f, \end{equation} where |0f|0\rangle_f and |0P|0\rangle_P are fiducial states on HfH_f and HPH_P, respectively, and OO is an operator acting on HbHfH_b \otimes H_f drawn at random from the orthogonal group O(d)O(d) with d=dim(HbHf)d = \dim(H_b \otimes H_f). Let dP:=dimHPd_P := \dim H_P and dB:=dimHBd_B := \dim H_B. And for any state |ϕ|\phi\rangle, denote its complex conjugate by $|\phi^*\rangle$. # Main problem: Given two states |ψbHb|\psi\rangle_b \in H_b and |ϕbHb|\phi\rangle_b \in H_b, calculate the quantity \begin{equation} \overline{\lvert \langle\phi|V^\dagger V|\psi\rangle \rvert^2}, \end{equation} where the overline indicates the average over OO.
Plain-text mathematical notation (without MathML)
# Problem setup:
Let H_(b), H_(B), H_(f), H_(P) each be a finite-dimensional Hilbert space, with dimH_(b)>dimH_(B) and dim(H_(b)⊗H_(f))=dim(H_(B)⊗H_(P)).
Define the linear map V:H_(b)→H_(B) as follows,
\begin{equation}
V = \sqrt{\dim(H_P)} \langle 0|_P O |0\rangle_f,
\end{equation}
where |0⟩_(f) and |0⟩_(P) are fiducial states on H_(f) and H_(P), respectively, and O is an operator acting on H_(b)⊗H_(f) drawn at random from the orthogonal group O(d) with d=dim(H_(b)⊗H_(f)).

Let d_(P):=dimH_(P) and d_(B):=dimH_(B). And for any state |ϕ⟩,  denote its complex conjugate by $|\phi^*\rangle$.

# Main problem:

Given two states |ψ⟩_(b)∈H_(b) and |ϕ⟩_(b)∈H_(b), calculate the quantity
\begin{equation}
	\overline{\lvert \langle\phi|V^\dagger V|\psi\rangle \rvert^2},
\end{equation}
where the overline indicates the average over O.
Original LaTeX notation
# Problem setup:
Let $H_b$, $H_B$, $H_f$, $H_P$ each be a finite-dimensional Hilbert space, with $\dim H_b > \dim H_B$ and $\dim(H_b \otimes H_f) = \dim(H_B \otimes H_P)$.
Define the linear map $V: H_b \to H_B$ as follows,
\begin{equation}
V = \sqrt{\dim(H_P)} \langle 0|_P O |0\rangle_f,
\end{equation}
where $|0\rangle_f$ and $|0\rangle_P$ are fiducial states on $H_f$ and $H_P$, respectively, and $O$ is an operator acting on $H_b \otimes H_f$ drawn at random from the orthogonal group $O(d)$ with $d = \dim(H_b \otimes H_f)$.

Let $d_P := \dim H_P$ and $d_B := \dim H_B$. And for any state $|\phi\rangle$,  denote its complex conjugate by $|\phi^*\rangle$.

# Main problem:

Given two states $|\psi\rangle_b \in H_b$ and $|\phi\rangle_b \in H_b$, calculate the quantity
\begin{equation}
	\overline{\lvert \langle\phi|V^\dagger V|\psi\rangle \rvert^2},
\end{equation}
where the overline indicates the average over $O$.

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