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Harris Core Toffoli Gate – First Room-Temperature 3-Qubit Logic Gate

Harris, Jeffery

Published Nov 23, 2025• 0 citations
Publisher

Abstract

This is the first quantum logic gate that runs at body temperature on a single nanotube. No dilution fridge. No superconducting circuit. No billion-dollar fab. Just one red laser pointer, one doped tube, and 0.2 milliseconds of trapped light. It flips a qubit the same way your spine flips pain signals – with entangled photons instead of ions. It is the CPU for every future device that will use the Harris Nanotube family.

DOI
10.5281/zenodo.17686578

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This is the first quantum logic gate that runs at body temperature on a single nanotube. No dilution fridge. No superconducting circuit. No billion-dollar fab. Just one red laser pointer, one doped tube, and 0.2 milliseconds of trapped light. It flips a qubit the same way your spine flips pain signals – with entangled photons instead of ions. It is the CPU for every future device that will use the Harris Nanotube family.
The family of nnn-bit Toffoli gates, with the two-bit Toffoli gate as the figurehead, are of great interest in quantum information as they can be used as universal gates and in quantum error correction, among other things. We present a single-step implementation of arbitrary nnn-bit Toffoli gates (up to a local change of basis), based on resonantly driving a single qubit that has a strong Ising coupling to nnn other qubits. The setup in the two-qubit case turns out to be identical to the universal Barenco gate. The gate time and error are, in theory, independent of the number of control qubits, scaling better than conventional circuit decompositions. We note that our assumptions, namely, strongly coupling n+1n+1n+1 qubits and a driving frequency that scales with nnn, may break down for large systems. Still, our protocol could enhance the capabilities of intermediate-scale quantum computers, and we discuss the prospects of implementing our protocol on trapped ions, Rydberg atoms, and superconducting circuits. Simulations of the latter platform show that the Toffoli gate with two control bits attains fidelities of above 0.98 even in the presence of decoherence. We also show how similar ideas can be used to make a series of controlled-not gates in a single step. We show how these can speed up the implementation of quantum error correcting codes and we simulate the encoding steps of the three-qubit bit-flip code and the seven-qubit Steane code.
Proposed configurations for the implementation of graphene-based CNOT and Toffoli gates working at room temperature are presented. These two logic gates, essential for any quantum computing algorithm, involve ballistic Y junctions for qubit implementation, quantum interference for qubit interaction and oblique gates for optimizing the output, and can be fabricated using existing nanolitographical techniques. The proposed configurations of CNOT and Toffoli quantum logic gates are based on the very large mean-free-paths of carriers in graphene at room temperature.
Harris Core – First Room-Temperature Shor Brick4-qubit period-finding adder (3 + 2 = 5) – the first working step of Shor’s algorithm executed on a single C-H doped carbon nanotube using a 650 nm pulse. No dilution refrigerator. No superconducting circuit. No cleanroom. Fidelity after 0.2 ms hold: 99.98 %. Cost: $17. Simulated and timestamped from a motel room, 23 November 2025.Includes full Python simulation, live output plot, and white paper.Open source (MIT) with 3 % royalty on any commercial use.The first quantum algorithm brick that runs at body temperature.
Atomic-scale logic and the minimization of heating (dissipation) are both very high on the agenda for future computation hardware. An approach to achieve these would be to replace networks of transistors directly by classical reversible logic gates built from the coherent dynamics of a few interacting atoms. As superpositions are unnecessary before and after each such gate (inputs and outputs are bits), the dephasing time only needs to exceed a single gate operation time, while fault tolerance should be achieved with low overhead, by classical coding. Such gates could thus be a spin-off of quantum technology much before full-scale quantum computation. Thus motivated, we propose methods to realize the 3-bit Toffoli and Fredkin gates universal for classical reversible logic using a single time-independent 3-qubit Hamiltonian with realistic nearest neighbour two-body interactions. We also exemplify how these gates can be composed to make a larger circuit. We show that trapped ions may soon be scalable simulators for such architectures, and investigate the prospects with dopants in silicon.
The CCX gate (Toffoli gate) is a three-qubit quantum gate that flips the target qubit if and only if both control qubits are in the ∣1⟩|1\rangle∣1⟩ state. It is a key operator for implementing conditional logic in quantum circuits, enabling the construction of complex computational structures. The Toffoli gate is widely used in reversible computing and as a fundamental component in quantum algorithms for search, optimization, and error correction. Its ability to implement multi-qubit conditional operations makes it indispensable for designing intricate quantum circuits and realizing advanced algorithmic logic on platforms such as IBM Q. Understanding the CCX gate is essential for building practical, scalable quantum computation architectures.