Quantum computers can simulate electrons in materials with unparalleled precision. This will lead to room-temperature superconductors — if we succeed.
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🧊 What Is Superconductivity?
Superconductivity is a quantum state of matter where a material carries electric current with zero resistance. Its discovery was made in 1911 by the Dutch physicist Heike Kamerlingh Onnes, who observed that the electrical resistance of mercury drops suddenly to zero when cooled to 4.15 K (−269 °C). This temperature — the “critical temperature” Tc — required liquid helium, an extremely expensive cooling medium.
The theoretical explanation came 46 years later. In 1957, John Bardeen, Leon Cooper, and Robert Schrieffer published BCS theory, which explains how electrons form pairs — called “Cooper pairs” — through interaction with crystal lattice vibrations (phonons). These pairs move collectively without scattering, eliminating resistance. BCS theory explains “conventional” superconductors perfectly, but fails for the newer high-temperature superconductors.
Superconductivity isn't merely low resistance — it's zero resistance. A current in a superconductor theoretically circulates forever without losing energy.
— Principle of superconductivity🔥 The Quest for Room Temperature
The great upheaval came in 1986, at the IBM research laboratory near Zurich. Physicists Georg Bednorz and K. Alex Müller discovered superconductivity in lanthanum-barium copper oxide (LBCO) at a temperature of 35 K — much higher than thought possible. They won the Nobel Prize in Physics in 1987. In less than a year, replacing lanthanum with yttrium (YBCO) raised the temperature to 92 K — above 77 K, the boiling point of liquid nitrogen, a cheap coolant.
This marked the birth of high-temperature superconductors (High-Tc). The main family consists of ceramic copper oxide materials — cuprate superconductors — featuring alternating CuO₂ layers and metal oxide layers. The record at atmospheric pressure belongs to the mercury-barium-calcium-copper system (HgBa₂Ca₂Cu₃O₈), with Tc around 133 K (−140 °C).
• 1911: Mercury (Hg) — 4.15 K
• 1986: LBCO (Bednorz & Müller, IBM) — 35 K
• 1987: YBCO — 92 K (above liquid nitrogen boiling point)
• 2001: MgB₂ — 39 K (highest “conventional” BCS superconductor)
• 2015: H₃S at 150 GPa (Drozdov et al.) — 203 K (−70 °C)
• 2019: LaH₁₀ at 170 GPa — 250 K (−23 °C)
• 2023: Nickelate La₃Ni₂O₇ — 80 K at high pressure (promising new family)
• Atmospheric pressure record: HgBaCaCuO — ~138 K
Progress didn't stop at cuprates. In 2006, iron-pnictide superconductors appeared as a second major family, with critical temperatures up to 56 K. Under extremely high pressure (~150-170 GPa), superhydrides — hydrogen-rich compounds — showed impressive results. In 2019, lanthanum decahydride (LaH₁₀) reached 250 K (−23 °C), just below room temperature, but at 170 GPa — about 1.7 million times atmospheric pressure.
❓ Why We Still Don't Understand High-Temperature Superconductors
Here lies one of the biggest open questions in modern physics. BCS theory explains conventional superconductors, but cuprates do not follow the same mechanism. The electrons form pairs, but the “glue” holding them together isn't phonons — or at least not phonons alone. Spin-fluctuation theory proposes that spin waves replace phonons as the pairing mechanism.
The difficulty lies in strong electron correlations. In cuprates, electrons interact so intensely with each other that Fermi liquid theory fails — the basic theory describing metals. Philip W. Anderson proposed Resonating Valence Bond (RVB) theory in 1987, but to this day there is no complete theoretical explanation. This is recognized as “one of the major unsolved problems of theoretical condensed matter physics.”
This inability is not technical — it is fundamental. Classical computational models cannot faithfully simulate the strong quantum correlations in many-body systems. The state space grows exponentially, and no supercomputer can keep up.
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💻 Quantum Simulation: The New Tool
This is where quantum simulation enters. Quantum computers can, theoretically, reproduce the behavior of strongly correlated electronic systems using a number of qubits proportional to the number of particles — instead of the exponential number of bits that a classical computer requires. This was precisely Richard Feynman's idea in 1982: "Nature isn't classical, dammit, and if you want to make a simulation of nature, you'd better make it quantum mechanical."
In practice, quantum material simulation follows two approaches. Analog simulation uses controllable quantum systems — such as trapped ions, ultracold atoms, or superconducting circuits — to mimic a material's Hamiltonian. Digital simulation uses quantum gates and algorithms, like VQE (Variational Quantum Eigensolver), to compute energy eigenvalues.
In 2018, Yuan Cao's team at MIT discovered superconductivity in bilayer graphene twisted at a “magic angle” of approximately 1.1 degrees. This discovery (twistronics) created a new field, as superconductivity appears in an extremely simple system — just two sheets of carbon — something that could help understand pairing mechanisms.
🚀 What Quantum Computers Give Us
Today, quantum material simulation is at an early but very promising stage. Quantum computers can:
• Simulate pairing mechanisms: If we understand exactly how Cooper pairs form in cuprates, we can design materials with even higher Tc.
• Map phase diagrams: Cuprates exhibit complex phenomena — antiferromagnetism, pseudogap, d-wave pairing symmetry — that interact with each other. Full understanding of the phase diagram requires simulation of many-body quantum systems.
• Explore new material families: Nickelates, discovered as superconductors in 2019, and superhydrides represent terra incognita. The search for candidate materials with high Tc at atmospheric pressure can be dramatically accelerated through quantum simulation.
The challenge remains enormous. Today's quantum systems (NISQ era) have limited qubits and significant noise. To realistically simulate a cuprate, hundreds or thousands of logical error-free qubits are needed — something years or even decades away. But progress in both hardware (noise reduction, error correction) and algorithms (error mitigation, hardware-efficient ansatz) gives cause for optimism.
Room-temperature superconductivity — the “Holy Grail” of condensed matter physics — won't be discovered by accident. It will be designed. And the design tools will be quantum computers.
— The promise of quantum simulationIf a superconductor at room temperature and atmospheric pressure becomes reality, the applications will transform the world: lossless electrical power transmission, maglev trains without expensive cryogenic systems, even more powerful MRI magnets, and countless technological innovations. Quantum material simulation doesn't just promise scientific understanding — it promises practical transformation.
