2016
DOI: 10.1103/physrevb.94.224403
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Intertwined nematic orders in a frustrated ferromagnet

Abstract: We investigate the quantum phases of the frustrated spin-$\frac{1}{2}$ $J_1$-$J_2$-$J_3$ Heisenberg model on the square lattice with ferromagnetic $J_1$ and antiferromagnetic $J_2$ and $J_3$ interactions. Using the pseudo-fermion functional renormalization group technique, we find an intermediate paramagnetic phase located between classically ordered ferromagnetic, stripy antiferromagnetic, and incommensurate spiral phases. We observe that quantum fluctuations lead to significant shifts of the spiral pitch ang… Show more

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Cited by 48 publications
(42 citation statements)
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“…Finally, as we lower J 2 /J 1 further, the ferromagnetic J 1 coupling becomes dominant enough to drive the system into a ferromagnetic ordered state which onsets at J 2 /J 1 = −0.153 (5). On comparison with the classical transition boundary at J 2 /J 1 ≈ −0.171, we see that the antiferromagnetic CS order intrudes into a portion of the phase diagram occupied by the ferromagnetic order at the classical level, as expected from general considerations [93,166]. For the J 1 = −1-only model [marked by a black disk in Fig.…”
Section: B Quantum Phase Diagramsupporting
confidence: 68%
“…Finally, as we lower J 2 /J 1 further, the ferromagnetic J 1 coupling becomes dominant enough to drive the system into a ferromagnetic ordered state which onsets at J 2 /J 1 = −0.153 (5). On comparison with the classical transition boundary at J 2 /J 1 ≈ −0.171, we see that the antiferromagnetic CS order intrudes into a portion of the phase diagram occupied by the ferromagnetic order at the classical level, as expected from general considerations [93,166]. For the J 1 = −1-only model [marked by a black disk in Fig.…”
Section: B Quantum Phase Diagramsupporting
confidence: 68%
“…Our finding of extended domains characterized by an absence of long-range dipolar magnetic order in the S = 1/2 model lays the avenue for future numerical investigations aiming to identify the nature of the nonmagnetic phase which could potentially be host to a plethora of exotic nonmagnetic phases such as quantum spin liquids, valence-bond-crystals, and latticenematics or feature quadrupolar ordered phases, i.e., spinnematic orders [107]. Indeed, in the S = 1/2 J 1 -J 2 -J 3 square lattice Heisenberg model, these orders were found to be stabilized [22]. The question of the microscopic identification of the nature of the nonmagnetic phase can be addressed within the PFFRG framework itself by combining it with a self-consistent Fock-like mean-field scheme to calculate lowenergy effective theories for emergent spinon excitations in S = 1/2 systems as has been recently achieved on the square and kagome lattices [108].…”
Section: Discussionmentioning
confidence: 99%
“…Thus, in contrast to the square lattice S = 1/2 J 1 -J 2 Heisenberg model [22,[35][36][37], there is an absence of an intermediate quantum paramagnetic phase, a manifestation of the weakening of quantum fluctuations in 3D. Note however, that for the square lattice model with FM J 1 , the very existence of quantum paramagnetic phase is not very clear yet [22,38,39]. On the BCC lattice, the role of a further neighbor frustrating AF J 3 coupling in Eq.…”
Section: Introductionmentioning
confidence: 95%
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“…Consequently, radical reactions have attracted growing research interest over the last few decades and have been employed in synthesis of many bioactive natural products. [1,2] Radicals are expected to be highly reactive and unstable, hence the control of enantioselectivity in radical transformations has proven to be of great importance but a challenging task. The early efforts were primarily focused on exploiting interactions between chiral Lewis acid and radical acceptors or donors.…”
Section: Introductionmentioning
confidence: 99%