4.8 Article

Non-reciprocal phase transitions

期刊

NATURE
卷 592, 期 7854, 页码 -

出版社

NATURE PORTFOLIO
DOI: 10.1038/s41586-021-03375-9

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资金

  1. MRSEC [DMR-2011854]
  2. Simons Foundation
  3. Complex Dynamics and Systems Program of the Army Research Office [W911NF-19-1-0268]
  4. University of Chicago Materials Research Science and Engineering Center - National Science Foundation [DMR-2011854]
  5. NSF [PHY-1748958]
  6. [17J01238]

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The article discusses the impact of non-reciprocity on the collective behavior of multi-body systems in out-of-equilibrium states, indicating that non-reciprocity leads to the emergence of time-dependent phases controlled by exceptional points. The article describes the non-reciprocal generalizations of three archetypal classes of self-organization out of equilibrium, including synchronization, flocking, and pattern formation.
Out of equilibrium, a lack of reciprocity is the rule rather than the exception. Non-reciprocity occurs, for instance, in active matter(1-6), non-equilibrium systems(7-9), networks of neurons(10,11), social groups with conformist and contrarian members(12), directional interface growth phenomena(13-15) and metamaterials(16-20). Although wave propagation in non-reciprocal media has recently been closely studied(1,16-20), less is known about the consequences of non-reciprocity on the collective behaviour of many-body systems. Here we show that non-reciprocity leads to time-dependent phases in which spontaneously broken continuous symmetries are dynamically restored. We illustrate this mechanism with simple robotic demonstrations. The resulting phase transitions are controlled by spectral singularities called exceptional points(21). We describe the emergence of these phases using insights from bifurcation theory(22,23) and non-Hermitian quantum mechanics(24,25). Our approach captures non-reciprocal generalizations of three archetypal classes of self-organization out of equilibrium: synchronization, flocking and pattern formation. Collective phenomena in these systems range from active time-(quasi) crystals to exceptional-point-enforced pattern formation and hysteresis. Our work lays the foundation for a general theory of critical phenomena in systems whose dynamics is not governed by an optimization principle.

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