Generation of a macroscopic entangled coherent state using quantum memories in circuit QED
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2016-08-26 |
| Journal | Scientific Reports |
| Authors | Tong Liu, Qi-Ping Su, Shao-Jie Xiong, Jinming Liu, Chui-Ping Yang |
| Institutions | Hangzhou Normal University, East China Normal University |
| Citations | 40 |
| Analysis | Full AI Review Included |
6CCVD Technical Documentation & Analysis: W-Type Entangled Coherent States via NV Center Ensembles
Section titled â6CCVD Technical Documentation & Analysis: W-Type Entangled Coherent States via NV Center EnsemblesâThis technical analysis reviews the requirements for generating macroscopic W-type Entangled Coherent States (ECS) using Nitrogen-Vacancy center ensembles (NVEs) as quantum memories within a Circuit Quantum Electrodynamics (cQED) architecture. The successful replication and extension of this high-fidelity QIP protocol rely fundamentally on ultra-high purity, engineered MPCVD diamond materialsâ6CCVDâs core expertise.
Executive Summary
Section titled âExecutive SummaryâThis proposal successfully demonstrates a protocol for generating macroscopic continuous-variable W-type entangled coherent states using NVEs as quantum memories in a cQED setup, achieving high fidelity (F > 90%).
- Core Achievement: Generation of W-type Entangled Coherent States (ECS) stored in Nitrogen-Vacancy center ensembles (NVEs), essential for scalable Quantum Information Processing (QIP).
- Key Advantage (Decoherence): Utilizing NVEs as quantum memories enables significantly longer storage times (NVE lifetime ~1 s reported) compared to photon-based schemes (cavity lifetime ~1 ms).
- Decoherence Suppression: The protocol maintains cavities in a vacuum state for most operation time, dramatically suppressing decoherence from cavity decay and inter-cavity crosstalk.
- Material Dependence: High operational fidelity (F â 93.2%) is achievable when NVE spin coherence times (T2) are high (simulations used T2 up to 1 ms), mandating ultra-high purity diamond substrates.
- Circuit Simplification: The system architecture requires only one external-cavity coupler qubit, simplifying the overall cQED circuit design.
- Feasibility: Numerical simulations (using QuTiP) confirm the high-fidelity implementation is feasible with rapid advancement in cQED and high-quality material technology.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Target Fidelity (Max) | 93.2 | % | Achieved for entire operation (D â 9) |
| Operation Time (Total) | 1.14 | ”s | Time required for F â 93.2% |
| Qubit Relaxation (T1) | 15 | ”s | Transmon Quibit T1 (Conservative estimate) |
| Qubit Dephasing (T2) | 25 | ”s | Transmon Quibit T2 (Conservative estimate) |
| NVE Coherence Time (T2) | 1 | ms | Maximum simulated spin coherence (for F=90.3%) |
| NVE Lifetime (Reported) | 1 | s | Achieved experimentally elsewhere |
| Cavity Lifetime ($\kappa$-1) | 1 | ms | Required for high-fidelity in Step 4 |
| Cavity Q Factor (Required) | $\ge$ 3.1 x 104 | Dimensionless | For 5 GHz resonator, based on 1 ”s/1 ms lifetime |
| Cavity Photon Number (Avg.) | $\lt$ 0.02 | Photons | During the long last step (decoherence suppression) |
| Qubit A-Cavity Coupling ($g_A/2\pi$) | 50 | MHz | Resonant coupling (Step 1) |
| Intra-Cavity Qubit-Cavity Coupling ($g_r/2\pi$) | 5 | MHz | Resonant coupling (Step 2) |
| NVE-Cavity Coupling ($g_b/2\pi$) | 4 | MHz | Dispersive coupling (Step 4) |
| Rabi Frequency ($\Omega/2\pi$) | 100 | MHz | Applied pulse (Step 4) |
Key Methodologies
Section titled âKey MethodologiesâThe W-state preparation uses a four-step procedure relying on resonant and dispersive interactions between the coupler qubit A, three intracavity qubits (j=1, 2, 3), three TLRs (cavities), and the NVEs.
- Step 1: Coupler-Cavity Resonant Interaction (Time $t = \pi/(2\sqrt{3}g_A)$)
- Action: Qubit A is resonantly coupled to all three cavities simultaneously (coupling constant $g_A$). Intra-cavity qubits and NVEs are decoupled.
- Result: Transfers the initial state (Qubit A in $|e\rangle_A$, cavities in $|0\rangle_{Cj}$) into the $|W_{2,1}\rangle_{C}$ state of the three cavities. Qubit A ends in $|g\rangle_A$.
- Step 2: Cavity-Intra-qubit Resonant Interaction (Time $t = \pi/(2g_r)$)
- Action: Qubit A is decoupled. Each intra-cavity qubit $j$ is resonantly coupled to its cavity $j$ (coupling constant $g_r$).
- Result: Maps the $|W_{2,1}\rangle_{C}$ state of the cavities onto the three intra-cavity qubits, resulting in the $|W_{2,1}\rangle_{q}$ state of the qubits. Cavities return to the vacuum state ($|0\rangle_{Cj}$).
- Step 3: Intra-qubit Rotation (Time $t = \pi/(4\Omega_{eg})$)
- Action: Intracavity qubits are decoupled from cavities. A classical resonant pulse (Rabi frequency $\Omega_{eg}$) is applied to each qubit $j$ to perform a rotation from the computational basis ($|g\rangle, |e\rangle$) to the rotated basis ($|\pm\rangle$).
- Result: Transforms the qubit state $|W_{2,1}\rangle_{q}$ into $|W_{2,1}\rangle_{\pm}$ in the rotated basis.
- Step 4: Dispersive Coupling and State Transfer (Time $t \approx 1.08$ ”s)
- Action: Cavities are frequency adjusted for dispersive interaction with both qubit $j$ and NVE $j$. A classical pulse ($\Omega$) is applied to qubit $j$. Large detuning ($D \approx 9$) is used.
- Result: The effective Hamiltonian mediates coupling between qubit $j$ and NVE $j$, mapping the qubit state $|W_{2,1}\rangle_{\pm}$ onto the NVE ensemble, preparing the desired macroscopic W-type ECS stored in the NVEs.
6CCVD Solutions & Capabilities
Section titled â6CCVD Solutions & CapabilitiesâThis research demonstrates a critical path toward scalable quantum computation utilizing the extremely long coherence times inherent in diamond-based NVEs. 6CCVD is positioned as the essential material partner to meet the rigorous specifications required for integrating NVE quantum memories into cQED architectures.
Applicable Materials
Section titled âApplicable MaterialsâThe foundation of this quantum memory approach is the NVE, which is critically dependent on the purity and crystal quality of the diamond material.
| Material | Specification | Relevance to Research |
|---|---|---|
| Optical Grade Single Crystal Diamond (SCD) | Ultra-low Nitrogen content ($\ll$ 5 ppb). Highest purity. Thickness 0.1 ”m - 500 ”m. | Crucial for NVE Coherence: Maximizes NVE spin coherence time (T2), enabling the experimentally reported T2 > 1 second, essential for surpassing the decoherence limits of superconducting qubits and cavities simulated in this study (T2 $\le$ 1 ms). |
| High Purity Polycrystalline Diamond (PCD) | High surface quality (Ra $\lt$ 5 nm). Plates up to 125mm size. | Provides the large-area, low-loss substrate required for fabricating complex, inch-scale planar superconducting transmission line resonators (TLRs) and integrated cQED circuits. |
| Substrates (Custom Thickness) | Up to 10 mm. | Provides necessary bulk and stability for hybrid quantum systems operating at cryogenic temperatures (40-50 mK). |
Customization Potential
Section titled âCustomization PotentialâThe cQED implementation requires precise material engineering and integration which aligns perfectly with 6CCVDâs custom capabilities:
- Custom Dimensions and Etching: The cQED architecture (TLRs, flux qubits) is a planar system. 6CCVD provides custom diamond wafer/plate sizes (up to 125mm PCD) and precision laser cutting services, allowing the diamond substrate to be perfectly shaped for microwave resonator fabrication.
- Metalization Services (Essential for cQED): Superconducting qubits and TLRs require high-quality metal film deposition. 6CCVD offers in-house metalization capabilities including Au, Pt, Pd, Ti, W, and Cu deposition, enabling researchers to integrate superconducting circuitry directly onto low-loss diamond, mitigating dielectric loss often present in standard silicon or sapphire substrates.
- Ultra-Polishing: To minimize surface scattering and maintain the high Q-factors required for TLRs ($\ge 3.1 \times 10^4$), 6CCVD provides SCD polishing down to Ra $\lt$ 1 nm and large-area PCD polishing down to Ra $\lt$ 5 nm.
Engineering Support
Section titled âEngineering SupportâThe fidelity of this W-state generation protocol is highly sensitive to the detuning parameters ($D \approx 9$) and the intrinsic material coherence times.
6CCVDâs in-house PhD team specializes in correlating MPCVD material growth parameters (purity, isotopic composition, NV density control) with achieved spin coherence times. Our experts can assist researchers and technical teams with:
- Material Selection: Guiding the choice between SCD and PCD based on the required size, cost budget, and minimum NVE coherence time needed for scalable quantum memory and quantum computing projects.
- Decoherence Mitigation: Consulting on substrate preparation and surface treatments to ensure optimal interfacing between the diamond NVE ensemble and the superconducting microwave circuitry (TLRs/qubits).
For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.
View Original Abstract
Abstract W -type entangled states can be used as quantum channels for, e.g., quantum teleportation, quantum dense coding and quantum key distribution. In this work, we propose a way to generate a macroscopic W -type entangled coherent state using quantum memories in circuit QED. The memories considered here are nitrogen-vacancy center ensembles (NVEs), each located in a different cavity. This proposal does not require initially preparing each NVE in a coherent state instead of a ground state, which should significantly reduce its experimental difficulty. For most of the operation time, each cavity remains in a vacuum state, thus decoherence caused by the cavity decay and the unwanted inter-cavity crosstalk are greatly suppressed. Moreover, only one external-cavity coupler qubit is needed, which simplifies the circuit.