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[Paper Review] Entanglement-magic separation in hybrid quantum circuits

Gerald E. Fux, Emanuele Tirrito|arXiv (Cornell University)|Dec 4, 2023
Quantum Computing Algorithms and Architecture4 citations
TL;DR

This paper demonstrates a measurement-induced phase transition in magic—quantified by stabilizer entropy—in a hybrid quantum circuit with controlled T-gate injection and projective measurements. Unlike entanglement, which exhibits a volume-to-area law transition at a different measurement rate, magic shows an independent phase transition, revealing that non-Clifford resources can be protected from measurement-induced suppression, highlighting a new layer in the resource theory of quantum advantage beyond entanglement.

ABSTRACT

Magic describes the distance of a quantum state to its closest stabilizer state. It is -- like entanglement -- a necessary resource for a potential quantum advantage over classical computing. We study magic, quantified by stabilizer entropy, in a hybrid quantum circuit with projective measurements and a controlled injection of non-Clifford resources. We discover a phase transition between a (sub)-extensive and area law scaling of magic controlled by the rate of measurements. The same circuit also exhibits a phase transition in entanglement that appears, however, at a different critical measurement rate. This mechanism shows how, from the viewpoint of a potential quantum advantage, hybrid circuits can host multiple distinct transitions where not only entanglement, but also other non-linear properties of the density matrix come into play.

Motivation & Objective

  • To investigate whether magic, like entanglement, undergoes measurement-induced phase transitions in hybrid quantum circuits.
  • To determine if the critical measurement rate for magic transitions differs from that of entanglement transitions.
  • To explore the role of non-Clifford resources (via T-gates) in stabilizing magic against measurement-induced suppression.
  • To establish a phase diagram for magic scaling in relation to measurement rate and T-gate density.
  • To clarify the implications of separate magic and entanglement transitions for quantum advantage and quantum error correction.

Proposed method

  • The study employs a one-dimensional hybrid quantum circuit with random Clifford gates, projective measurements, and controlled injection of T-gates at a tunable density.
  • Magic is quantified using stabilizer entropy, a measure of non-stabilizer resource content.
  • The system is simulated via Monte Carlo sampling over many stochastic trajectories to compute steady-state magic and entanglement entropy.
  • The T-gate density is scaled as $ \eta/N^\beta $, allowing analysis of the thermodynamic limit for varying $ \beta $, including $ \beta = 1 $ and $ \beta < 1 $.
  • For analytical tractability, a separable model with single-site Clifford gates is introduced, enabling exact derivation of magic scaling as $ \bar{\mathcal{M}}_{\mathrm{ss}} \propto N^{1-\beta} $.
  • Phase transitions are identified by analyzing scaling behavior: (sub)extensive vs. area law, with critical rates determined numerically and analytically.
Figure 1: Phase transitions in entanglement (a) compared to the possible phase transitions in entanglement and magic (b) in one–dimensional quantum circuits. Quantum circuits in phase I may lead to an advantage over classical computing, while circuits in phases II and III are amenable to simulation
Figure 1: Phase transitions in entanglement (a) compared to the possible phase transitions in entanglement and magic (b) in one–dimensional quantum circuits. Quantum circuits in phase I may lead to an advantage over classical computing, while circuits in phases II and III are amenable to simulation

Experimental results

Research questions

  • RQ1Does magic in hybrid quantum circuits exhibit a measurement-induced phase transition distinct from entanglement transitions?
  • RQ2At what measurement rate does magic transition from (sub)extensive to area-law scaling, and how does this compare to the entanglement transition rate?
  • RQ3How does the density of T-gates, scaled as $ \eta/N^\beta $, affect the scaling of magic in the thermodynamic limit?
  • RQ4Can the stabilizer formalism or tensor network methods simulate circuits where magic remains (sub)extensive despite high measurement rates?
  • RQ5What is the role of entangling two-qubit Clifford gates in protecting magic from measurement-induced suppression?

Key findings

  • The paper identifies a distinct measurement-induced phase transition in magic, with a critical measurement rate $ p_c^{\text{magic}} $ that differs from the entanglement transition rate $ p_c^{\text{ent}} $, demonstrating that magic and entanglement are governed by different mechanisms.
  • In the regime of low measurement rates, both entanglement and magic scale (sub)extensively, indicating a phase where both resources are robust.
  • For intermediate measurement rates, entanglement transitions to an area law while magic remains (sub)extensive, defining a phase where quantum advantage may still be accessible despite reduced entanglement.
  • For high measurement rates, both entanglement and magic transition to area law scaling, placing the system in a classically simulable regime.
  • Analytical results for a separable model confirm that magic scales as $ \bar{\mathcal{M}}_{\mathrm{ss}} \propto N^{1-\beta} $ for $ \beta < 1 $, remains constant at $ \beta = 1 $, and vanishes for $ \beta > 1 $, indicating a critical dependence on T-gate density scaling.
  • The presence of two-qubit Clifford gates in the full circuit enhances magic protection, suggesting that entanglement can shield non-Clifford resources from measurement-induced degradation.
Figure 2: Hybrid quantum circuit with a brickwork structure of random 2–site Clifford gates interspersed with measurements in the computational bases and T–gates for $N=8$ qubits and 4 time steps. The measurements and T–gates appear randomly with probability $p$ and $q(N)=\eta/N^{\beta}$ , respectiv
Figure 2: Hybrid quantum circuit with a brickwork structure of random 2–site Clifford gates interspersed with measurements in the computational bases and T–gates for $N=8$ qubits and 4 time steps. The measurements and T–gates appear randomly with probability $p$ and $q(N)=\eta/N^{\beta}$ , respectiv

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This review was created by AI and reviewed by human editors.