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Landauer Entropy and Timekeeping: Exploring Information-Theoretic Limits via Planck Time with Experimental Tests on IBM Quantum Hardware

AYDIN HUSEYIN

Published Dec 24, 2025• 0 citations
Publisher

Abstract

We explore timekeeping through the lens of Landauer's principle of bit erasure, where each erasure event produces exactly ln(2) bits of entropy. We reformulate the entropy-time connection as dt = dS/k, where k = R ln(2) is the entropy production rate determined by the erasure rate R. We introduce a dimensionless coupling constant alpha = k t_P, where t_P is the Planck time. At the Planck frequency limit, this yields alpha = ln(2) approximately 0.693. We note a numerical coincidence with loop quantum gravity: the Immirzi parameter, recently derived from Landauer's principle, is gamma = ln(2)/(pi sqrt(3)). Both expressions contain ln(2), though whether this indicates a fundamental connection remains an open question. We present new experimental results from IBM Quantum hardware (ibm_torino), testing a proxy for our temperature-independence prediction. Using the reset gate as a Landauer erasure operation, we measure reset fidelity across different initial states parametrized by angle theta. We find a coefficient of variation CV = 0.31%, indicating that reset performance is largely independent of initial state. Additionally, Ramsey interferometry experiments show that Landauer erasure destroys quantum coherence (visibility drops from 98.5% to 4.7%), consistent with irreversible entropy production. Two-qubit experiments demonstrate entropy transfer from system to reservoir. While these results are consistent with our framework, we emphasize that they do not constitute direct verification of the temperature-independence prediction, which requires controlled temperature variation in trapped-ion or similar systems.

DOI
10.5281/zenodo.18049904

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We explore timekeeping through the lens of Landauer's principle of bit erasure, where each erasure event produces exactly ln(2) bits of entropy. We reformulate the entropy-time connection as dt = dS/k, where k = R ln(2) is the entropy production rate determined by the erasure rate R. We introduce a dimensionless coupling constant alpha = k t_P, where t_P is the Planck time. At the Planck frequency limit, this yields alpha = ln(2) approximately 0.693. We note a numerical coincidence with loop quantum gravity: the Immirzi parameter, recently derived from Landauer's principle, is gamma = ln(2)/(pi sqrt(3)). Both expressions contain ln(2), though whether this indicates a fundamental connection remains an open question. We present new experimental results from IBM Quantum hardware (ibm_torino), testing a proxy for our temperature-independence prediction. Using the reset gate as a Landauer erasure operation, we measure reset fidelity across different initial states parametrized by angle theta. We find a coefficient of variation CV = 0.31%, indicating that reset performance is largely independent of initial state. Additionally, Ramsey interferometry experiments show that Landauer erasure destroys quantum coherence (visibility drops from 98.5% to 4.7%), consistent with irreversible entropy production. Two-qubit experiments demonstrate entropy transfer from system to reservoir. While these results are consistent with our framework, we emphasize that they do not constitute direct verification of the temperature-independence prediction, which requires controlled temperature variation in trapped-ion or similar systems.
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We investigate how nonequilibrium quantum initial states can reduce the finite-time thermodynamic cost of Landauer erasure. Considering a general finite-dimensional quantum memory coupled to a thermal reservoir via a Davies generator, we show that the dissipated heat at a fixed operational erasure fidelity is largely controlled by the overlap of the initial state with the slowest Liouvillian relaxation mode. We derive a modified finite-time Landauer bound in which the excess dissipation above the quasistatic limit scales quadratically with this slow mode projection, and we prove a sufficient Mpemba Landauer condition under which a hotter state can erase faster and dissipate less heat than a colder preparation, without violating Landauer's principle. A minimal qutrit model illustrates these quantum Mpemba speedups and reveals broad parameter regimes where coherence and Hamiltonian-induced modes conspire to suppress finite-time entropy production. We further identify practical control knobs, including temperature tuning, coherence engineering, and Hamiltonian shaping of Liouvillian spectra, which enable Mpemba-enhanced erasure to be directly tested on platforms such as superconducting circuits, trapped ions, semiconductor quantum dots, and solid-state spins.
One of the outstanding challenges to information processing is the eloquent suppression of energy consumption in the execution of logic operations. The Landauer principle sets an energy constraint in deletion of a classical bit of information. Although some attempts have been made to experimentally approach the fundamental limit restricted by this principle, exploring the Landauer principle in a purely quantum mechanical fashion is still an open question. Employing a trapped ultracold ion, we experimentally demonstrate a quantum version of the Landauer principle, i.e., an equality associated with the energy cost of information erasure in conjunction with the entropy change of the associated quantized environment. Our experimental investigation substantiates an intimate link between information thermodynamics and quantum candidate systems for information processing.
Quantum information reset is an intrinsically irreversible process constrained by the second law of thermodynamics. In contemporary superconducting processors, dissipation during qubit reset is frequently dominated not only by quantum limits but by a classical energy floor on the order of 10^{-21} J. In contrast, the entropic bound T \Delta S at dilution refrigerator temperatures (\sim 15 mK) corresponds to a lower energy scale of approximately 10^{-23} J, establishing entropy production as the organizing physical principle that limits both the efficiency and the speed of reset operations. We introduce an entropy-limited efficiency estimator, \eta_S = 1 - (T \Delta S / W_{\rm diss}), which quantifies the thermodynamic distance from the entropic (Landauer) limit. By construction, \eta_S = 0 corresponds to the saturation of the entropy production limit, while \eta_S \to 1 indicates dissipation dominated by non-entropic (classical) contributions. Maximizing \eta_S is equivalent to a constrained variational problem in which dissipated work is minimized subject to the second law of thermodynamics. For typical superconducting qubits (\omega_q/2\pi \sim 5 GHz, T_1 \sim 50–100 \mus, T \sim 15 mK), the entropic bound T \Delta S \sim 10^{-23} J lies two orders of magnitude below the experimentally observed classical dissipation floor W_{\rm floor} \sim 10^{-21} J. Figures 1 and 2 were generated using the provided scripts_generate_figures.py script, using parameters: \omega_q/2\pi = 5 GHz, T_1 = 80 \mus, and T = 15 mK.
We derive a thermodynamic quantum speed limit for irreversible processes: (kB ∆Σ)·τ ≥ ■/(2T), where ∆Σ is the entropy produced in units of kB , τ is the process duration, T is the temperature, and ■ is thereduced Planck constant. We call this the Parker Relation. It is derived by two routes for thermalLindblad channels in the weak-coupling limit (γ/ω ■ 1): (1) the Deffner–Lutz quantum speed limit foropen systems applied to the amplitude damping channel, with a Hilbert–Schmidt norm bound on theLindblad generator rigorous to leading order in γ/ω; and (2) the open-system Margolus–Levitin bound,where the effective driving energy T × kB × ∆Σ follows from the free energy budget of a Markovianthermal channel with no external work. We establish explicitly when the relation is novel versus when itreduces to existing bounds. For thermal relaxation (∆Σ = ■ω/kB T) the Parker bound reproduces thestandard Mandelstam–Tamm result τ ≥ 1/(2ω) — a consistency check. For Landauer logical erasure (∆Σ= ln 2) the bound is independent of existing quantum speed limits. The classical bridge is established viathe incoherent limit of the quantum amplitude damping channel, which reduces exactly to the classicaltwo-state master equation governing bistable erasure devices. ■ appears in the classical bound becauseevery thermal bath has a quantum mechanical substrate; the classical Fisher–Rao speed limit combinedwith the quantum-limited attempt frequency ν0~ kBT/■ gives τmin ~ ■/(2kB T) to within a numericalprefactor of order unity (see Appendix A). The primary novel prediction is the minimum time forirreversible bit erasure at 300 K: τ min = ■/(2kB T ln 2) = 18.4 femtoseconds — a quantum-derivedfoundational floor that real CMOS devices exceed by 8 orders of magnitude. For a 5 GHz transmon at20 mK the bound gives τ min ≈ 16 ns — 60 000× below current best T2 values, a consistency check not anovel prediction. Four open questions are identified: tightening the generator norm bound numericallyvia QuTiP; completing the Route 2 formal connection to del Campo–Funo; extending beyond thermalLindblad channels; and completing the classical bridge via Nicholson et al. or Dechant. The relation isconjectured to hold generally for all irreversible processes at temperature T.
Landauer's Principle states that the work cost of erasure of one bit of information has a fundamental lower bound of kT ln(2). Here we prove a quantitative Landauer's principle for arbitrary processes, providing a general lower bound on their work cost. This bound is given by the minimum amount of (information theoretical) entropy that has to be dumped into the environment, as measured by the conditional max-entropy. The bound is tight up to a logarithmic term in the failure probability. Our result shows that the minimum amount of work required to carry out a given process depends on how much correlation we wish to retain between the input and the output systems, and that this dependence disappears only if we average the cost over many independent copies of the input state. Our proof is valid in a general framework that specifies the set of possible physical operations compatible with the second law of thermodynamics. We employ the technical toolbox of matrix majorization, which we extend and generalize to a new kind of majorization, called lambda-majorization. This allows us to formulate the problem as a semidefinite program and provide an optimal solution.