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TARGET-VARIANCE QUANTUM SPEED LIMITS FROM PROJECTIVE FIDELITY REDUCTION

Roy Surya Sekhar

Published Jun 14, 2026• 0 citations
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Abstract

Quantum state readout on many experimental platforms is performed through a single projective measurement channel rather than full quantum state tomography. We derive a detector-conditioned quantum speed limit that constrains the minimum time for the projective fidelity $F(t) = \langle\omega|\rho(t)|\omega\rangle$ to reach a prescribed discrimination threshold:\[T \;\ge\; \frac{|\Theta(0) - \Theta_*|}{\Delta H_\omega},\]where $\Theta = \arccos\sqrt{F}$ is the Bures angle and $\Delta H_\omega$ is the energy standard deviation of the \emph{fixed target state}. This bound, valid for both pure and mixed states under unitary dynamics, expresses the speed constraint in terms of a time-independent quantity determined entirely by the Hamiltonian and the detector projector, rather than the evolving-state variance appearing in standard Mandelstam--Tamm-type bounds. We further show that the resulting bound is structurally distinct from standard Mandelstam--Tamm-type bounds based on evolving-state variance. The bound exhibits commuting-sector invariance, suppressing Hamiltonian components that are energetically large but detection-irrelevant. Exact diagonalization of the transverse-field Ising model for $N \le 12$ spins confirms asymptotic separation between the bounds in the strong-interaction regime. The framework provides a detector-conditioned lower bound for rank-1 projective detection dynamics, applicable to superconducting qubit readout, trapped-ion fluorescence detection, and stabilizer syndrome monitoring. The construction is particularly relevant for architectures in which experimentally accessible information is restricted to a small set of projective readout channels rather than full-state tomography. ## Results & Validation Below is the macro-level data extracted from the 156-qubit **ibm_fez** processor, confirming the asymptotic separation predicted by Theorem 5.2 as the many-body coupling strength scales extensively: [Quantum Speed Limit Validation Benchmark](qsl_validation_plot.png) ## Hardware Compilation Profile The transpiled circuit diagram below illustrates the native pulse-level gate routing on the IBM Quantum Heron architecture. By optimizing the physical register map, the compiler enforces a clean nearest-neighbor coupling loop with zero SWAP gate overhead: [Heron Chip Circuit Native Compilation](circuit-d8uhclsbp3hs73861d7g.png) ## Raw Measurement Diagnostics To evaluate the projective fidelity reduction threshold ($F_* = 0.15$), raw binary distributions are unpacked and corrected using Matrix-Free Measurement Mitigation (M3). Below is a representative diagnostic histogram of single-outcome state frequencies sampled from the hardware backend: [Error Mitigated Hardware Measurement Histogram](job_d8uhc4ctqbtc73d1qdmg_results_c.png)

DOI
10.5281/zenodo.20846437

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Quantum state readout on many experimental platforms is performed through a single projective measurement channel rather than full quantum state tomography. We derive a detector-conditioned quantum speed limit that constrains the minimum time for the projective fidelity F(t)=⟨ω∣ρ(t)∣ω⟩F(t) = \langle\omega|\rho(t)|\omega\rangleF(t)=⟨ω∣ρ(t)∣ω⟩ to reach a prescribed discrimination threshold:[T ;\ge; \frac{|\Theta(0) - \Theta_*|}{\Delta H_\omega},]where Θ=arccos⁡F\Theta = \arccos\sqrt{F}Θ=arccosF​ is the Bures angle and ΔHω\Delta H_\omegaΔHω​ is the energy standard deviation of the \emph{fixed target state}. This bound, valid for both pure and mixed states under unitary dynamics, expresses the speed constraint in terms of a time-independent quantity determined entirely by the Hamiltonian and the detector projector, rather than the evolving-state variance appearing in standard Mandelstam--Tamm-type bounds. We further show that the resulting bound is structurally distinct from standard Mandelstam--Tamm-type bounds based on evolving-state variance. The bound exhibits commuting-sector invariance, suppressing Hamiltonian components that are energetically large but detection-irrelevant. Exact diagonalization of the transverse-field Ising model for N≤12N \le 12N≤12 spins confirms asymptotic separation between the bounds in the strong-interaction regime. The framework provides a detector-conditioned lower bound for rank-1 projective detection dynamics, applicable to superconducting qubit readout, trapped-ion fluorescence detection, and stabilizer syndrome monitoring. The construction is particularly relevant for architectures in which experimentally accessible information is restricted to a small set of projective readout channels rather than full-state tomography. ## Results & Validation Below is the macro-level data extracted from the 156-qubit ibm_fez processor, confirming the asymptotic separation predicted by Theorem 5.2 as the many-body coupling strength scales extensively: Quantum Speed Limit Validation Benchmark ## Hardware Compilation Profile The transpiled circuit diagram below illustrates the native pulse-level gate routing on the IBM Quantum Heron architecture. By optimizing the physical register map, the compiler enforces a clean nearest-neighbor coupling loop with zero SWAP gate overhead: Heron Chip Circuit Native Compilation ## Raw Measurement Diagnostics To evaluate the projective fidelity reduction threshold (F∗=0.15F_* = 0.15F∗​=0.15), raw binary distributions are unpacked and corrected using Matrix-Free Measurement Mitigation (M3). Below is a representative diagnostic histogram of single-outcome state frequencies sampled from the hardware backend: Error Mitigated Hardware Measurement Histogram
Quantum state readout on many experimental platforms is performed through a single projective measurement channel rather than full quantum state tomography. We derive a detector-conditioned quantum speed limit that constrains the minimum time for the projective fidelity [Formula: see text] to reach a prescribed discrimination threshold :[Formula: see text]where [Formula: see text] is the Bures angle and [Formula: see text] is the energy standard deviation of the fixed target state. This bound, valid for both pure and mixed states under unitary dynamics, expresses the speed constraint in terms of a time-independent quantity determined entirely by the Hamiltonian and the detector projector, rather than the evolving-state variance appearing in standard Mandelstam–Tamm-type bounds. We further show that the resulting bound is structurally distinct from standard Mandelstam–Tamm-type bounds based on evolving-state variance. The bound exhibits commuting-sector invariance, suppressing Hamiltonian components that are energetically large but detection-irrelevant. Exact diagonalization of the transverse-field Ising model for [Formula: see text] spins confirms asymptotic separation between the bounds in the strong-interaction regime. The framework provides a detector-conditioned lower bound for Rank-1 projective detection dynamics, applicable to superconducting qubit readout, trapped-ion fluorescence detection and stabilizer syndrome monitoring. The construction is particularly relevant for architectures in which experimentally accessible information is restricted to a small set of projective readout channels rather than full-state tomography.
Existing quantum speed limits (QSLs) for dissipative dynamics generally require integrating thefull state trajectory, limiting their predictive utility before simulation. We introduce a detector-conditioned framework to overcome this requirement. By projecting the adjoint Lindblad dissipatoronto a target detector Πω and taking its operator norm, we obtain a single static number—thedissipative transition capacity Γω —that provides a trajectory-free upper bound for local fidelitydecay. This construction deliberately sacrifices geometric tightness: for a k-qubit detector in anN -qubit system, it reduces the pre-simulation cost from O(23N ) trajectory integration to O(23k )static extraction, where k ≪ N is the detector size. We prove this quantity is the canonical minimalstate-independent bound arising from trace-class duality, is subadditive under tensor products, obeysextensive many-body scaling (Γ ≤ N γ) for local dissipators, and correctly vanishes for noise channelscommuting with the detector. We validate the local capacity bounds experimentally across 1-to 3-qubit sub-registers executed on the 156-qubit IBM Heron QPU (ibm marrakesh), confirmingbound validity on physical hardware without free parameters. We further demonstrate that Γωprovides a candidate cost function for noise-aware compiler routing, enabling circuit scheduling onheterogeneous hardware without prior classical simulation.
Quantum speed limits (QSLs) impose fundamental constraints on the evolution speed of quantum systems. Traditionally, the Mandelstam-Tamm (MT) and Margolus-Levitin (ML) bounds have been widely employed, relying on the standard deviation and mean of energy distribution to define the QSLs. However, these universal bounds only offer loose restrictions on the quantum evolution. Here we introduce the generalized ML bounds, which prove to be more stringent in constraining dynamic evolution, by utilizing moments of energy spectra of arbitrary orders, even noninteger orders. To validate our findings, we conduct experiments in a superconducting circuit, where we have the capability to prepare a wide range of quantum photonic states and rigorously test these bounds by measuring the evolution of the system and its photon statistics using quantum state tomography. While, in general, the MT bound is effective for short-time evolution, we identify specific parameter regimes where either the MT or the generalized ML bounds suffice to constrain the entire evolution. Our findings not only establish new criteria for estimating QSLs but also substantially enhance our comprehension of the dynamic evolution of quantum systems.
How far are deployed quantum gates from the fastest evolution quantum mechanics allows? We answer for pre-Heron IBM processors, mainly Falcon and Eagle, using public, version-pinned calibration snapshots and inequalities whose proofs are machine-checked in Lean 4. Heron snapshots lack a Hamiltonian. For single-qubit gates, with the drive-strength convention fixed by IBM's calibrated π pulses, the X gate lasts a median 11.3 times the two-level speed limit at full drive amplitude (1646 qubits, 41 backends). Most of this gap is a design choice: IBM drives at about a tenth of the anharmonicity, and at that drive its pulses are about 2 times the square-pulse limit. Within each device's full amplitude, optimal control on IBM's model gives gates about 10 times faster than the median. For two-qubit gates (1758 coupled pairs, 43 backends), the known qubit-subspace minimal time of controlled-NOT-class gates under exchange coupling (literature) gives a median ratio 4.22; across the snapshots it rose, not monotonically, from 2.78 (2021) to 4.26 (2025) as gates got longer, coinciding with the change from Falcon to Eagle. With the second level and fast arbitrary local control, the minimal time of a controlled-Z gate with ideal local control lies between 0.287 and 1/3 of the qubit-only exchange time (refined bound, explicit construction); bounded local control reaches 0.35. We also formalize an entangling-time bound in arbitrary local dimension, known for qubits and new only as a machine-checked assembly. Applied to IBM's chip-to-chip state transfer (version 2), the same diagnostic places the transfers at 5.8--7.9 times the single-mode minimal time, whose lower bound is machine-checked in Isabelle, and the coherence error of the fastest protocol four to six times below the measured errors. The contribution is a reproducible diagnostic built on the machine-checked inequalities, with explicit guarantees. Companion site (blueprint): https://karlesmarin.github.io/blueprints/qsl-diagnostics/
Existing quantum speed limits (QSLs) for dissipative dynamics generally require integrating the full state trajectory, limiting their predictive utility before simulation. We introduce a detector-conditioned framework to overcome this requirement. By projecting the adjoint Lindblad dissipator onto a target detector Πω\Pi_\omegaΠω​ and taking its operator norm, we obtain a single static number---the \emph{dissipative transition capacity} Γω\Gamma_\omegaΓω​---that caps the fidelity decay rate for any initial state, without requiring prior ODE integration. We demonstrate that within the specified class of trajectory-independent detector-conditioned bounds, Γω\Gamma_\omegaΓω​ provides a natural functional driven by spatial locality, provide algebraic saturation conditions, and delineate regimes where it provides tighter constraints than standard trajectory-dependent trace-norm bounds. An extensive many-body scaling law (Γ≤Nγ\Gamma \le N\gammaΓ≤Nγ for local baths) and subadditivity across orthogonal detectors follow from the triangle inequality, demonstrating an exponential O(2N)\mathcal{O}(2^N)O(2N) separation from global geometric trajectory bounds under stated locality assumptions. We provide an operational interpretation in binary state discrimination and quantum error correction, and demonstrate a matrix-free runtime scaling advantage over differential equation integration.
Quantum speed limits (QSLs) constrain the minimum time for quantum state evolution, typically derived from energy bounds like the Margolus-Levitin (ML) and Mandelstam-Tamm (MT) relations. In open systems, decoherence—driven by environmental interactions—may impose additional constraints. This work investigates whether decoherence times fundamentally limit QSLs in spin-chain systems, extending ML/MT bounds to open dynamics. By modeling spin chains with Lindblad equations and simulating Heisenberg-type interactions, we analyze the interplay between energy fluctuations, decoherence rates, and evolution times. Experimental validation via trapped-ion or superconducting-qubit arrays could test energy-time uncertainty in many-body systems. Results suggest decoherence times establish a lower QSL bound proportional to [to verify], offering a platform to probe open-system quantum dynamics. ## 1. Introduction Quantum speed limits (QSLs) define the fastest possible evolution between distinguishable quantum states, critical for quantum computing and information processing. Closed-system QSLs, such as the ML [arXiv:quant-ph/9804014] and MT [DOI:10.1103/PhysRev.41.1019] bounds, rely on energy constraints. However, open systems—subject to decoherence—require extended frameworks. Decoherence times, governed by environmental couplings, may impose additional QSLs, yet their interplay with ML/MT bounds remains unexplored. Spin chains, realizable in trapped ions [DOI:10.1038/s41586-019-1394-6] and superconducting circuits, offer a many-body testbed for studying these effects. This work bridges open-system dynamics with QSL theory, assessing whether decoherence times set a fundamental lower bound and enabling experimental verification of energy-time uncertainty. ## 2. Background The ML bound states that a quantum system requires at least $ t_{\text{QSL}} \geq \hbar / (2\Delta E) $, where $ \Delta E $ is the energy spread. The MT bound $ t_{\text{QSL}} \geq \hbar / (2E) $, with $