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Quantum simulation & computing

FermiQP

At MPQ we are building the FermiQP demonstrator, a quantum processor in which fermionic lithium-6 atoms are to work both as an analogue quantum simulator and as a digital quantum computer.

Computer rendering of an atomic physics apparatus on optical tables. On the left, a vacuum system with two red pump housings and windowed chambers, its lower part mounted on rails; in the centre, a square frame with copper-coloured magnetic field coils around the vacuum chamber, with laser beams drawn in orange; on the right, a tall cylindrical tower of optics mounts on a raised breadboard.
Computer rendering of the FermiQP apparatus. Image: Quantum Munich

How can controlled motion and collisions turn a fermionic quantum simulator into a programmable processor?

The platform

FermiQP is a joint project funded by the German Federal Ministry of Research, Technology and Space (BMFTR). Its processor is designed to run in two modes. In the analogue mode, ultracold fermionic ⁶Li atoms in an optical lattice simulate the Fermi-Hubbard model and a quantum gas microscope reads them out site by site. In the digital mode, controlled collisions in an optical superlattice act as global two-qubit gates, combined with laser-driven control of individual spins. Our group builds the demonstrator, with partners in Tübingen, Munich, Jülich, Berlin, Jena and industry.

Three-dimensional illustration: red and blue atoms sit in the wells of a corrugated optical-lattice potential above a microscope objective labelled FERMISCOPE. A focused violet beam from above addresses one atom, marked by a ring; on the left a dashed outline marks an empty site next to a doubly occupied one. Grey arrows show the lattice-beam directions.Enlarge (opens the full-size figure)
Schematic of the FermiQP quantum gas microscope. Atoms in two internal states (blue and red) occupy a two-dimensional optical lattice; a focused beam (violet) addresses a single atom, and the objective below images every site. On the left, an atom has tunnelled into a neighbouring site, leaving a hole beside a doubly occupied site. Illustrative, not to scale. Illustration: I. Bloch

One machine, two modes

Conventional quantum computers use qubits, which do not obey fermionic statistics. To simulate electrons, the exchange statistics of fermions must first be translated into qubit operations, and this adds computational cost. FermiQP is designed to compute with fermionic atoms directly. At its start in 2021 the project targeted about 1,000 to 10,000 atoms in the analogue mode and about 200 fully connected qubits in the digital mode. Digital gate sequences then prepare the initial state of an analogue simulation and set its readout basis.

Square fluorescence image in an inverted colour scale: individual atoms appear as dark blue dots on a pale background. They fill a roughly round cloud more than a hundred lattice sites across; in the dense centre the dots line up along the rows of a square lattice, and towards the edges the atoms become sparse.Enlarge (opens the full-size figure)
Fluorescence image of single lithium atoms in an optical lattice on the FermiQP apparatus. Each dark dot is one atom. Image: Quantum Munich

Collisional gates with fermionic atoms

We tested the basic gate operation on our existing lithium quantum gas microscope. An optical superlattice of 532 nm and 1,064 nm light splits each lattice site into a double well, most of them holding one spin-up and one spin-down atom. Lowering the barrier between the wells lets the atoms tunnel and interact, which drives spin exchange and pair tunnelling. Stopping halfway gives an entangling √SWAP gate. Spin- and charge-resolved fluorescence imaging records the outcome in every double well.

The √SWAP gate reaches an average fidelity of 99.75(6) % across 64 lattice sites, and the coherence time of the entangled Bell states is estimated to exceed 10 s. We also demonstrated a proof-of-principle composite pair-exchange gate, a basic operation for simulations of quantum chemistry. The lithium microscope, built for analogue Fermi-Hubbard simulations, can therefore also run digital gates, the combination FermiQP is designed for.

Two-panel schematic. Left: applications of fermionic quantum computing, namely the Fermi-Hubbard model with a circuit of digital, analogue and digital blocks followed by measurements, lattice gauge theories with a three-quark sketch and a phase diagram of hadrons and quark-gluon plasma, and quantum chemistry with a molecule and a pair-exchange gate PX(Θ) in a double well. Right: block structure of the two-atom Hamiltonian in a double well and four double-well sketches. Tunnelling t connects states with one atom in each well to states with both atoms in one well, which lie higher by the interaction energy U, and an effective coupling J swaps the two spins or moves the pair between the wells.Enlarge (opens the full-size figure)
Concept of a fermionic quantum processor (left) and the double-well physics behind its collisional gates (right): tunnelling t and on-site interaction U give an effective coupling J for spin exchange and pair tunnelling. Bojović et al., Nature 652, 602 (2026), Fig. 1 · CC BY 4.0

Algorithms for fermionic hardware

With theory colleagues we design protocols that use the native operations of the hardware. One theory study shows how complex-valued Loschmidt echoes of the Fermi-Hubbard model could be measured, using short pulse sequences on an initial state of 2 × 2 plaquettes followed by a global quench. These give access to spectral quantities such as the local density of states.

A second proposal (PRX Quantum, accepted) treats superlattice tunnelling and site-resolved energy shifts as beam splitters and phase shifters. Following the Clements scheme of linear optics, any single-particle unitary, such as a discrete Fourier transform or an arbitrary coherent rearrangement of atoms, can be built this way. In a preprint we propose how a two-dimensional optical lattice with a projected pattern of repulsive potentials could realise the three-band Emery model in regimes relevant to cuprates and infinite-layer nickelates.

Research directions

Next steps are local addressing of individual atoms, larger systems and longer gate circuits. With these tools we want to prepare and probe strongly correlated fermionic states, for example to study high-temperature superconductivity, and to run fermionic algorithms for quantum chemistry and materials research.

Selected results & publications

High-fidelity collisional quantum gates with fermionic atomsNature 652, 602–608 (2026) · Journal ArticlePhase-Sensitive Measurements on a Fermi-Hubbard Quantum ProcessorQuantum 10, 2103 (2026) · Journal ArticleRealizing the Emery Model in Optical Lattices for Quantum Simulation of Cuprates and NickelatesarXiv:2603.11037 (2026) · Preprint

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Discuss student projects, doctoral research or postdoctoral opportunities with the scientific contact; project scope and availability are agreed individually.

Methods and topics: Coherent atom control, Optical superlattices, Quantum algorithms.

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Group photo of the FermiQP team: ten researchers standing in front of the glass entrance of a building.

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