Pauli quantum computing: $I$ as $|0\rangle$ and $X$ as $|1\rangle$
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arXiv
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| Formato: | Preprint |
| Publicado: |
2024
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| _version_ | 1866916507159625728 |
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| author | Shang, Zhong-Xia |
| author_facet | Shang, Zhong-Xia |
| contents | We propose a new quantum computing formalism named Pauli quantum computing. In this formalism, we use the Pauli basis $I$ and $X$ on the non-diagonal blocks of density matrices to encode information and treat them as the computational basis $|0\rangle$ and $|1\rangle$ in standard quantum computing. There are significant differences between Pauli quantum computing and standard quantum computing from the achievable operations to the meaning of measurements, resulting in novel features and comparative advantages for certain tasks. We will give three examples in particular. First, we show how to design Lindbladians to realize imaginary time evolutions and prepare stabilizer ground states in Pauli quantum computing. These stabilizer states can characterize the coherence in the steady subspace of Lindbladians. Second, for quantum amplitudes of the form $\langle +|^{\otimes n}U|0\rangle^{\otimes n}$ with $U$ composed of $\{H,S,T,\text{CNOT}\}$, as long as the number of Hadamard gates in the unitary circuit $U$ is sub-linear $\mathit{o}(n)$, the gate (time) complexity of estimating such amplitudes using Pauli quantum computing formalism can be exponentially reduced compared with the standard formalism ($\mathcal{O}(ε^{-1})$ to $\mathcal{O}(2^{-(n-\mathit{o}(n))/2}ε^{-1})$). Third, given access to a searching oracle under the Pauli encoding picture manifested as a quantum channel, which mimics the phase oracle in Grover's algorithm, the searching problem can be solved with $\mathcal{O}(n)$ scaling for the query complexity and $\mathcal{O}(\text{poly}(n))$ scaling for the time complexity. While so, how to construct such an oracle is highly non-trivial and unlikely efficient due to the hardness of the problem. |
| format | Preprint |
| id |
arxiv_https___arxiv_org_abs_2412_03109 |
| institution | arXiv |
| publishDate | 2024 |
| record_format | arxiv |
| spellingShingle | Pauli quantum computing: $I$ as $|0\rangle$ and $X$ as $|1\rangle$ Shang, Zhong-Xia Quantum Physics We propose a new quantum computing formalism named Pauli quantum computing. In this formalism, we use the Pauli basis $I$ and $X$ on the non-diagonal blocks of density matrices to encode information and treat them as the computational basis $|0\rangle$ and $|1\rangle$ in standard quantum computing. There are significant differences between Pauli quantum computing and standard quantum computing from the achievable operations to the meaning of measurements, resulting in novel features and comparative advantages for certain tasks. We will give three examples in particular. First, we show how to design Lindbladians to realize imaginary time evolutions and prepare stabilizer ground states in Pauli quantum computing. These stabilizer states can characterize the coherence in the steady subspace of Lindbladians. Second, for quantum amplitudes of the form $\langle +|^{\otimes n}U|0\rangle^{\otimes n}$ with $U$ composed of $\{H,S,T,\text{CNOT}\}$, as long as the number of Hadamard gates in the unitary circuit $U$ is sub-linear $\mathit{o}(n)$, the gate (time) complexity of estimating such amplitudes using Pauli quantum computing formalism can be exponentially reduced compared with the standard formalism ($\mathcal{O}(ε^{-1})$ to $\mathcal{O}(2^{-(n-\mathit{o}(n))/2}ε^{-1})$). Third, given access to a searching oracle under the Pauli encoding picture manifested as a quantum channel, which mimics the phase oracle in Grover's algorithm, the searching problem can be solved with $\mathcal{O}(n)$ scaling for the query complexity and $\mathcal{O}(\text{poly}(n))$ scaling for the time complexity. While so, how to construct such an oracle is highly non-trivial and unlikely efficient due to the hardness of the problem. |
| title | Pauli quantum computing: $I$ as $|0\rangle$ and $X$ as $|1\rangle$ |
| topic | Quantum Physics |
| url | https://arxiv.org/abs/2412.03109 |