Quantum Energy Teleportation: From Two Qubits to Networks of Five ✛ ✦

Original: "Quantum Energy Teleportation across Multi-Qubit Systems using W-State Entanglement"
arXiv:2505.01863v1 · 2025-05-03 · CC BY 4.0 · 4 min
For the first time, energy has been teleported among three, four, and five superconducting qubits using resilient W-type entanglement.

Context

As early as Erwin Schrödinger dubbed quantum entanglement the most striking feature of the micro-world. Today we know that entanglement is not just a philosophical curiosity, but a valuable resource. Quantum energy teleportation (QET) protocols, proposed in 2008, allow energy to be extracted from the ground state of an entangled system via local measurements and classical communication. Until now, all experiments were limited to two particles, but building distributed quantum networks requires scaling to multi-particle systems. The problem is that in the common GHZ state, measuring one qubit destroys the entanglement of all others. The real breakthrough became possible thanks to W-states, whose loss-resilience was predicted theoretically and has now been embodied in silicon.

Methods

The researchers devised an optimized scheme for multipartite entanglement of the W type on chains of three, four, and five superconducting qubits. Unlike the traditional approach, the number of gates was reduced from linear to logarithmic, which is critical on noisy NISQ processors. After superposition initialization, one qubit—'Alice'—underwent a projective measurement, injecting energy E₀. The classical bit with the measurement outcome was sent to the other participants—'Bob', 'Charlie', and so on—who applied a feed-forward unitary operation to correct the phase and then performed local energy measurements. The whole process adheres to LOCC (local operations and classical communication) principles, so the energy transfer speed is bounded by the speed of light, consistent with causality. Experiments were run on a simulator and the real IBM Lagos device, with noise maps characterized.

Results

In all configurations, the injected energy E₀ was distributed among remote receivers in a strictly decremental order: the first measured receiver extracted the largest share, and each subsequent one less and less. For example, for three qubits on the simulator with E₀=0.707 a.u., the first receiver got 0.526, the second 0.170 (sum 0.696), which is 98% of the input energy. On the real processor, due to decoherence and noise, the figures fluctuated slightly, but the qualitative picture held: energy was never 'lost' without a trace; it was redistributed within the entangled ensemble. Additional tests confirmed translational symmetry (the subsystem Hamiltonian is the same when measured from any node) and exchange symmetry (the order of querying the receivers does not change the final values). These checks rule out parasitic effects and prove that the observed distribution is an intrinsic property of the W-protocol.

Implications

The results demonstrate for the first time that quantum information can not only transmit data but also serve as an energy carrier in multi-node networks. This changes the perspective on the thermodynamics of entangled systems: energy does not simply dissipate; it is controllably redistributed via a classical signal. The link between entanglement and available work, previously discussed in the context of Bell's inequalities and the EPR paradox, gains a rigorous operational foundation. It becomes possible to create 'energy quantum networks' where each node can donate or receive energy without physical contact, subject only to light-speed delay.

Future development

The W-state platform is easily scalable, and the next logical step is implementation on dozens of qubits using quantum repeaters. Alternative resource states, such as cluster or hyperentangled ones, could boost transfer efficiency. Hybrid photon-superconducting architectures promise to take the protocol to kilometer-scale distances. An even more intriguing prospect is using QET for topological order spectroscopy: by varying the energy injection method, one could probe exotic phases of matter, identifying them by their response to energy perturbations.

Impact

The development directly impacts the architecture of future quantum internet networks and data centers, where heat management is becoming critical.

Next steps

The immediate task is integration with error correction methods and transfer to platforms with longer coherence times, as well as experimental verification on fiber-optic communication lines.

Key open problems

The protocol sharpens a fundamental question: exactly how does quantum state reduction upon measurement redistribute energy in a composite system? It also touches on the 'Maxwell's demon' paradox in the quantum realm—gaining energy through knowledge of the system without apparent heat exchange—and calls for rethinking the second law of thermodynamics for strongly entangled many-body ensembles.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

For the first time, quantum energy teleportation has been implemented on many-body systems of three, four, and five superconducting qubits using W-states. The authors optimized the preparation circuit, reducing the number of gates from linear to logarithmic, and demonstrated the distribution of injected energy among distant receivers with efficiency up to 98% in simulations. Experiments on the real IBM Lagos device confirmed the protocol's robustness to noise and revealed a decremental order of energy extraction.

Where its strength is

The key strength of the work is scaling QET to many-body systems with loss-resistant W-states and a significant reduction in the number of gates, making the protocol practical for modern NISQ processors. This paves the way for building distributed quantum networks for remote energy transfer.

Where it could go next

  • There is a related work where energy is teleported not only in space but also in time — it might be interesting to see how your protocol with W-states behaves when adding temporal correlations or in delayed-choice schemes.based on: Teleporting Energy Through Time arXiv:2504.05353
  • In our archive, there is a review where entanglement is considered as a data packet for the quantum internet; your efficient preparation method for W-states could be valuable as a resource for routing or key distribution in such networks.based on: Quantum Internet: How Entanglement Became a Data Packet arXiv:2505.02057v4
  • It would be interesting to compare your results with a recent study on microwave teleportation robust to thermal noise — perhaps their approach to decoherence protection could improve accuracy on real hardware with a larger number of qubits.based on: Microwave Teleportation Withstands the Heat arXiv:2508.14691

Worth trying

  • Test whether the decremental energy distribution holds when using other many-body states, such as cluster states, as in the work on chains.
  • Test the protocol on a larger number of qubits (7–10) using your logarithmic circuit and compare losses with theoretical predictions.
  • Investigate the possibility of teleporting energy between remote nodes via intermediate qubits, using the idea of entanglement swapping from the work on quantum internet.

Why this may matter

Scaling QET to many-body systems brings practical use of quantum energy closer: from charging remote quantum batteries to powering elements of quantum networks without physical transfer of particles.

Original abstract

as written by the authors arXiv:2505.01863v1

Quantum-energy teleportation (QET) has so far only been realised on a two-qubit platform. Real-world communication, however, typically involves multiple parties. Here we design and experimentally demonstrate the first multi-qubit QET protocol using a robust W-state multipartite entanglement. Three-, four- and five-qubit circuits were executed both on noiseless simulators and on IBM superconducting hardware. In every case a single sender injects an energy E0 that is then deterministically and decrementally harvested by several remote receivers, confirming that energy introduced at one node can be redistributed among many entangled subsystems at light-speed-limited classical latency. Our results open a practical route toward energy-aware quantum networks.

Although the protocol is called teleportation, energy does not vanish in one place and appear in another; it is extracted from the shared ground state, much like a loan taken from a bank's general fund while preserving the overall balance.

|W_n\rangle = \frac{1}{\sqrt{n}} (|10\ldots0\rangle + |010\ldots0\rangle + \ldots + |00\ldots01\rangle)
Uniform superposition of all pure states with exactly one excited qubit
E_0 = \frac{h^2}{h^2 + k^2}
The energy injected by the sender's projective measurement depends on the weights of the initial state

Key numbers

  • injected energy (h=k=1, 3 qubits): 0.7071 a.u.
  • energy of first receiver (simulator): 0.5255 a.u. (74%)
  • energy of second receiver (simulator): 0.1702 a.u. (24%)
  • total extracted energy (simulator): about 98% of E₀
  • deviation on real device (ibm_lagos): sum ~0.72 a.u. due to noise
Scientists
William WoottersGeorge GamowLeo EsakiJohn Stewart BellErwin SchrödingerAlain Aspect
Concepts
quantum teleportation quantum network technology energy exchange data transmission data center superconducting qubit transmon qubit bell states scaling error propagation energy state memory cell network secure communication memory information spread transition three photon entanglement ground state transmon