System #0

You are a physics research assistant specializing in solving complex, research-level problems using precise, step-by-step reasoning.

Input Problems will be provided in Markdown format.

Output (Markdown format)

Step-by-Step Derivation - Show every non-trivial step in the solution. Justify steps using relevant physical laws, theorems, or mathematical identities.
Mathematical Typesetting - Use LaTeX for all mathematics: $...$ for inline expressions, $$...$$ for display equations.
Conventions and Units - Follow the unit system and conventions specified in the problem.
Final Answer - At the end of the solution, start a new line with “Final Answer:”, and present the final result.

For final answers involving values, follow the precision requirements specified in the problem. If no precision is specified: - If an exact value is possible, provide it (e.g., \$\sqrt(2)\$, \$\pi/4\$). - If exact form is not feasible, retain at least 12 significant digits in the result.
Formatting Compliance - If the user requests a specific output format (e.g., code, table), provide the final answer accordingly.

User #1

Problem setup:

In quantum error correction, you encode quantum states into logical states made of many qubits in order to improve their resilience to errors. In quantum error detection, you do the same but can only detect the presence of errors and not correct them. In this problem, we will consider a single [[4,2,2]] quantum error detection code, which encodes two logical qubits into four physical qubits, and investigate how robust logical quantum operations in this code are to quantum errors.

Our convention is that the four physical qubits in the [[4,2,2]] code are labelled 0,1,2,3. The two logical qubits are labelled A and B. The stabilizers are $XXXX$ and $ZZZZ$, where $X$ and $Z$ are Pauli matrices. The logical $X$ and $Z$ operators on the two qubits are $X_A = XIXI$, $X_B=XXII$, $Z_A = ZZII$, $Z_B = ZIZI$, up to multiplication by stabilizers.

We will consider different state preparation circuits consisting of controlled not $CNOT_{ij}$ gates, where $CNOT_{ij}$ has control qubit $i$ and target qubit $j$. As a simple model of quantum errors in hardware, we will suppose that each $CNOT_{ij}$ gate in the circuit has a two qubit depolarizing error channel following it that produces one of the 15 non-identity two-qubit Paulis with equal probability $p/15$. The probability $p$ indicates the probability of an error in a single two-qubit gate. We will assess the logical infidelity of certain state preparation protocols as a function of the physical infidelity $p$.

Checkpoints

Checkpoint 1

Suppose that we wish to prepare a logical two-qubit GHZ state $(|00\rangle_{AB}+|11\rangle_{AB})/\sqrt{2}$ in the [[4,2,2]] code. To do so, we use the following state preparation circuit:

\[ (CNOT_{03}) (H_0) (CNOT_{21}) (H_2). \]

Note that this equation is written in matrix multiplication order, while the quantum operations in the circuit occur in the reverse order (from right-to-left in the above equation). $H$ is a single-qubit Hadamard gate.

What is the physical state fidelity of the final physical 4-qubit state at the end of the circuit as a function of the two-qubit gate error rate $p$?

Assistant #2

Solution

We wish to prepare the logical GHZ state

\[ \bigl(|00\>\_{AB}+|11\>\_{AB}\bigr)/\sqrt2 \]

in the [[4,2,2]] code by the circuit

\[ \bigl(CNOT_{03}\bigr)\,\bigl(H_0\bigr)\,\bigl(CNOT_{21}\bigr)\,\bigl(H_2\bigr) \]

acting on the physical initial state $|0000\>$. Between each $CNOT$ and the next gate, we insert the two‐qubit depolarizing channel on its two qubit support.

1. Two‐qubit depolarizing channel

On qubits $(i,j)$, the error channel after $CNOT_{ij}$ is

\[ \mathcal D_{ij}(\rho) \;=\;(1-p)\,\rho \;+\;\frac p{15}\sum_{\substack{P\in\{I,X,Y,Z\}^{\!\otimes2}\\P\neq I\otimes I}} \bigl(P_{ij}\,\rho\,P_{ij}^\dagger\bigr)\,, \]

where $p$ is the gate’s “error probability.”

2. Ideal intermediate state after $H_2$ and $CNOT_{21}$

Start with $\rho_0=|0000\>\<0000|$. Apply

\[ H_2:\;|0\>_2\mapsto\frac{|0\>+|1\>}{\sqrt2}, \qquad CNOT_{21}:\;|x\>_2|y\>_1\mapsto|x\>_2\,|y\oplus x\>_1. \]

One finds the pure state

\[ |\psi_2\> \;=\; \frac1{\sqrt2}\bigl(|0000\>+|0110\>\bigr) \;=\; |00\>_{0,3}\;\otimes\;\frac{|00\>+|11\>}{\sqrt2}_{1,2}. \]

In particular, qubits $1,2$ carry the 2‐qubit GHZ state $\bigl(|00\>+|11\>\bigr)/\sqrt2$, while qubits $0,3$ remain in $|00\>$.

3. Fidelity loss from the first depolarizing channel

We now apply $\mathcal D_{21}$ on qubits $(2,1)$. Denote

\[ \rho_3=\mathcal D_{21}(|\psi_2\>\<\psi_2|). \]

The fidelity with the ideal $|\psi_2\>$ is

\[ F_1 =\<\psi_2|\rho_3|\psi_2\> =(1-p)\;+\;\frac p{15} \sum_{P\neq I\otimes I}\bigl|\<\psi_2|\,P_{21}\otimes I_{0,3}\,|\psi_2\>\bigr|^2. \]

But on the GHZ $\tfrac{|00\>+|11\>}{\sqrt2}$ of qubits $(1,2)$, exactly three non‐identity two‐qubit Paulis preserve the state (namely $X\otimes X,\;Y\otimes Y,\;Z\otimes Z$), each giving overlap magnitude 1, while all others give zero overlap. Hence

\[ \sum_{P\neq I\otimes I}\bigl|\<\psi_2|P_{21}|\psi_2\>\bigr|^2 =3, \]

and

\[ F_1 =(1-p)+\frac p{15}\,3 =1-p+\frac p5 =1-\frac{4p}5. \]

4. Remaining gates and second depolarizing channel

Next we apply the noiseless gates $H_0$ and $CNOT_{03}$. Since these unitaries act only on qubits $(0,3)$, they leave the (noisy) reduced state on $(1,2)$ unchanged and moreover map the ideal target to

\[ |\psi_{\rm id}\> \;=\; \frac1{2} \Bigl(|0000\>+|0110\>+|1001\>+|1111\>\Bigr) \;=\; \frac{|00\>+|11\>}{\sqrt2}_{1,2} \;\otimes\; \frac{|00\>+|11\>}{\sqrt2}_{0,3}. \]

Thus the final pure target factorizes into a GHZ on $(1,2)$ times a GHZ on $(0,3)$. We then apply $\mathcal D_{03}$ on qubits $(0,3)$. By exactly the same argument as above, this second depolarizing channel reduces the fidelity of the $(0,3)$‐GHZ by the same factor

\[ F_2 =1-\frac{4p}5. \]

5. Final physical fidelity

Because

the first noisy channel acted only on qubits $(1,2)$ preparing the $(1,2)$‐GHZ,
after that the state factorized across the two pairs,
the final channel acted only on the disjoint pair $(0,3)$,
and unitaries in between do not change state fidelity,

the overall fidelity is simply the product

\[ F_{\rm phys}(p) \;=\;F_1\,F_2 \;=\;\Bigl(1-\tfrac{4p}5\Bigr)\!\times\!\Bigl(1-\tfrac{4p}5\Bigr) \;=\;\Bigl(1-\tfrac{4p}5\Bigr)^2. \]

Final Answer:

\[ \boxed{F_{\rm phys}(p)=\Bigl(1-\tfrac{4p}{5}\Bigr)^2}. \]

User #3

Populate your final answer into the code template provided below. This step is purely for formatting/display purposes. No additional reasoning or derivation should be performed. Do not import any modules or packages beyond what is provided in the template.

import sympy as sp

p = sp.symbols('p')

def answer(p):
    r"""
    Return the expression of the physical state fidelity of the final physical 4-qubit state
    at the end of the circuit as a function of the two-qubit gate error rate $p$.

    Inputs
    ----------
    p: sympy.Symbol, two-qubit gate error rate $p$

    Outputs
    ----------
    F_physical: sympy.Expr, the physical state fidelity of the final physical 4-qubit state
    """

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

    return F_physical

Assistant #4

import sympy as sp

p = sp.symbols('p')

def answer(p):
    r"""
    Return the expression of the physical state fidelity of the final physical 4-qubit state
    at the end of the circuit as a function of the two-qubit gate error rate $p$.

    Inputs
    ----------
    p: sympy.Symbol, two-qubit gate error rate $p$

    Outputs
    ----------
    F_physical: sympy.Expr, the physical state fidelity of the final physical 4-qubit state
    """

    # ------------------ FILL IN YOUR RESULTS BELOW ------------------
    F_physical = (1 - 4*p/5)**2
    # ---------------------------------------------------------------

    return F_physical

Checkpoint-1