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- From: Kormos Márton <kormos.marton AT ttk.bme.hu>
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- Subject: [Fizinfo] BME ElmFiz szeminárium, okt. 9. Werner Miklós
- Date: Wed, 7 Oct 2026 20:59:40 +0000
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MEGHÍVÓ
BME Elméleti Fizika Szeminárium,
okt. 9. péntek 10:15,
1111 Budapest, Budafoki út 8., BME F III. magasföldszint 01.,
Elméleti Fizika Tanszék szemináriumi szoba
Werner Miklós (Wigner Fizikai Kutatóközpont)
Block entropy area based non-local fermionic mode optimization with gradient
disentanglers
In this talk, I will discuss the use of tensor network approaches for systems
of interacting fermions. Combining optimization by unitary rotations within
the single-particle active space with the density matrix renormalization
group (DMRG) yields an efficient low-rank ground-state algorithm. The first
efficient implementations relied on local (nearest-neighbor) mode
optimizations based on Rényi entropies, together with heuristic[1,2] or
systematic[3,4] reorderings of the modes. For fermionic lattice models, it
has also been shown that, despite the increased complexity of the
Hamiltonian, the computational cost can be reduced by three to four orders of
magnitude when optimized modes are used[2]. However, reorderings become
destructive as the optimum is approached[3,4], since they are themselves
single-particle unitaries (permutations) that change the cost function,
namely the block-entropy area. This can lead to undamped oscillations that
prevent convergence.
Recently, we introduced a systematic non-local mode optimization algorithm
based on the gradient of the block-entropy area[5]. From this gradient, we
construct a long-range, non-interacting effective disentangler Hamiltonian.
We then minimize the cost function by simulating the time-dependent
Schrödinger equation driven by this Hamiltonian, using the time-dependent
variational principle with projector splitting. Combining DMRG with this
gradient-based entanglement minimization results in a superior low-rank
iterative ground-state algorithm that requires no reorderings and is
therefore free from the spurious oscillations of earlier approaches. We
demonstrate the method on two-dimensional lattice models of interacting
fermions and on the Fe$_4$S$_4$ cluster, and show its robustness and
advantages over earlier protocols based on nearest-neighbor mode rotations
and reorderings.
[1] C. Krumnow, L. Veis, Ö. Legeza, and J. Eisert, Phys. Rev. Lett. 117,
210402 (2016).
[2] A. Menczer, K. Kapás, MAW, Ö. Legeza, Phys. Rev. B 109, 195148 (2024).
[3] G. Friesecke, MAW, K. Kapás, A. Menczer, Ö. Legeza, arXiv:2406.03449
(2024).
[4] MAW, A. Menczer, Ö. Legeza (arXiv:2501.18263), published in Advances
Quantum Chemistry 94, Hungarian Quantum Chemistry: Part B - Contemporary
Research (2026).
[5] MAW, G. Friesecke, A. Menczer, K. Kapás, Ö. Legeza, arXiv:2609.11811
(2026)
Minden érdeklődőt szeretettel várunk.
A további program megtekinthető itt: https://physics.ttk.bme.hu/theoryseminars
Kormos Márton
szemináriumi koordinátor
- [Fizinfo] BME ElmFiz szeminárium, okt. 9. Werner Miklós, Kormos Márton, 10/07/2026
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