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PRODID:UW-Madison-Physics-Events
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UID:UW-Physics-Event-9478
DTSTART:20251106T160000Z
DURATION:PT1H0M0S
DTSTAMP:20260405T165750Z
LAST-MODIFIED:20251024T143602Z
LOCATION:5310 Chamberlin
SUMMARY:Searching for Experimental Signatures of Fractionalization\, R
 . G. Herb Condensed Matter Seminar\, Pietro Bonetti\, Harvard
DESCRIPTION:In this talk\, I will present some of my recent work which
  aims at understanding experimental observations in several strongly c
 orrelated platformsâ€”cuprates\, cold atomic simulators and organic co
 mpoundsâ€”in terms of exotic fractionalized states exhibiting topologi
 cal order.<br>\n<br>\nIn the cuprates\, the pseudogap phase shows mult
 iple signatures of reconstruction of the large Fermi surface into four
  small hole pockets. In the absence of spontaneous symmetry breaking\,
  this appears to contradict Luttingerâ€™s theorem\, which predicts tha
 t the volume enclosed by the Fermi surface remains constant. The resol
 ution of this apparent contradiction lies in assuming that the pseudog
 ap phase hosts fractionalized excitations with emergent gauge fields. 
 I will show that these excitations are crucial not only for preserving
  Luttingerâ€™s theorem but also for reproducing the Fermi surface topo
 logy observed in quantum oscillation measurements at low temperatures\
 , where charge density wave order develops and further reconstructs th
 e four hole pockets.<br>\n<br>\nIn the second part of the talk\, I wil
 l discuss a recent experiment realizing a Hubbard model on a Lieb latt
 ice in a cold atomic simulator [Lebrat et al.\, arXiv:2404.17555 (2024
 )]. At half-filling\, a flat band was observed for zero Hubbard U\, an
 d a ferrimagnetic state for nonzero U\, in agreement with theoretical 
 predictions. In the presence of strong interactions\, a new flat band 
 was reported to emerge at quarter filling without symmetry breaking. E
 mploying parton theories\, we consider quantum fluctuations of several
  magnetic ground states identified using Hartree-Fock theory. We find 
 a state with a flat band at the Fermi level coexisting with fractional
 ized bosonic spinon excitations carrying Z2â€‹ gauge charges. This sta
 te represents a striking realization of doping-induced fractionalizati
 on.<br>\n<br>\nIf time permits\, I will briefly review how ultrafast s
 pectroscopic experiments in the cuprates and in the organic compound Î
 º-(BEDT-TTF)2Cu2(CN)3â€‹ can be interpreted in terms of fractionalized
  excitations.
URL:https://www.physics.wisc.edu/events/?id=9478
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