arXiv subjects

C E Campbell

Publications and source records attributed to C E Campbell.

3 recordsLinked to original sources

arXiv2015

Frustrated Heisenberg antiferromagnet on the honeycomb lattice with spin quantum number $s \geq 1$

The ground-state (GS) phase diagram of the frustrated spin-$s$ $J_{1}$--$J_{2}$--$J_{3}$ Heisenberg antiferromagnet on the honeycomb lattice is studied using the coupled cluster method, for spin quantum numbers $s=1,\,\frac{3}{2},\,2\,,\frac{5}{2}$. We study the case $J_{3}=J_{2}=κJ_{1}$, in the range $0 \leq κ\leq 1$, which includes the point of maximum classical ($s \to \infty$) frustration, viz., the classical critical point at $κ_{\rm cl}=\frac{1}{2}$, separating the Néel phase for $κ< κ_{\rm cl}$ and the collinear striped AFM phase for $κ> κ_{\rm cl}$. Results are presented for the GS energy, magnetic order parameter and plaquette valence-bond crystal (PVBC) susceptibility. For all spins $s \geq \frac{3}{2}$ we find a quantum phase diagram very similar to the classical one, with a direct first-order transition between the two collinear AFM states at a value $κ_{c}(s)$ which is slightly greater than $κ_{\rm cl}$ [e.g., $κ_{c}(\frac{3}{2}) \approx 0.53(1)$] and which approaches it monotonically as $s \to \infty$. By contrast, for the case $s=1$ the transition is split into two such that the stable GS phases are ones with Néel AFM order for $κ< κ_{c_{1}} = 0.485(5)$ and with striped AFM order for $κ> κ_{c_{2}} = 0.528(5)$, just as in the case $s=\frac{1}{2}$ (for which $κ_{c_{1}} \approx 0.47$ and $κ_{c_{2}} \approx 0.60$). For both the $s=\frac{1}{2}$ and $s=1$ models the transition at $κ_{c_{2}}$ appears to be of first-order type, while that at $κ_{c_{1}}$ appears to be continuous. However, whereas in the $s=\frac{1}{2}$ case the intermediate phase appears to have PVBC order over the entire range $κ_{c_{1}} < κ< κ_{c_{2}}$, in the $s=1$ case PVBC ordering either exists only over a very small part of the region or, more likely, is absent everywhere.

cond-mat.str-el↗

arXiv2013

A frustrated spin-1 $J_{1}$--$J_{2}$ Heisenberg antiferromagnet: An anisotropic planar pyrochlore model

The zero-temperature ground-state (GS) properties and phase diagram of a frustrated spin-1 $J_{1}$--$J_{2}$ Heisenberg model on the checkerboard square lattice are studied, using the coupled cluster method. We consider the case where the nearest-neighbour exchange bonds have strength $J_{1}>0$ and the next-nearest-neighbour exchange bonds present (viz., in the checkerboard pattern of the planar pyrochlore) have strength $J_{2} \equiv κJ_{1}>0$. We find significant differences from both the spin-1/2 and classical versions of the model. We find that the spin-1 model has a first phase transition at $κ_{c_{1}} \approx 1.00 \pm 0.01$ (as does the classical model at $κ_{\rm cl}=1$) between two antiferromagnetic phases, viz., a quasiclassical Néel phase (for $κ< κ_{c_{1}}$) and one of the infinitely degenerate family of quasiclassical phases (for $κ> κ_{c_{1}}$) that exists in the classical model for $κ> κ_{\rm cl}$, which is now chosen by the {\it order by disorder} mechanism as (probably) the "doubled Néel" (or Néel$^{\ast}$) state. By contrast, none of this family survives quantum fluctuations to form a stable GS phase in the spin-1/2 case. We also find evidence for a second quantum critical point at $κ_{c_{2}} \approx 2.0 \pm 0.5$ in the spin-1 model, such that for $κ> κ_{c_{2}}$ the quasiclassical (Néel$^{\ast}$) ordering melts and a nonclassical phase appears, which, on the basis of preliminary evidence, appears unlikely to have crossed-dimer valence-bond crystalline (CDVBC) ordering, as in the spin-1/2 case. Unlike in the spin-1/2 case, where the Néel and CDVBC phases are separated by a phase with plaquette valence-bond crystalline (PVBC) ordering, we find very preliminary evidence for such a PVBC state in the spin-1 model for all $κ> κ_{c_{2}}$.

cond-mat.str-el↗

arXiv2008

Effect of anisotropy on the ground-state magnetic ordering of the spin-one quantum $J_{1}^{XXZ}$--$J_{2}^{XXZ}$ model on the square lattice

We study the zero-temperature phase diagram of the $J_{1}^{XXZ}$--$J_{2}^{XXZ}$ Heisenberg model for spin-1 particles on an infinite square lattice interacting via nearest-neighbour ($J_1 \equiv 1$) and next-nearest-neighbour ($J_2 > 0$) bonds. Both bonds have the same $XXZ$-type anisotropy in spin space. The effects on the quasiclassical Néel-ordered and collinear stripe-ordered states of varying the anisotropy parameter $Δ$ is investigated using the coupled cluster method carried out to high orders. By contrast with the spin-1/2 case studied previously, we predict no intermediate disordered phase between the Néel and collinear stripe phases, for any value of the frustration $J_2/J_1$, for either the $z$-aligned ($Δ> 1$) or $xy$-planar-aligned ($0 \leq Δ< 1$) states. The quantum phase transition is determined to be first-order for all values of $J_2/J_1$ and $Δ$. The position of the phase boundary $J_{2}^{c}(Δ)$ is determined accurately. It is observed to deviate most from its classical position $J_2^c = {1/2}$ (for all values of $Δ> 0$) at the Heisenberg isotropic point ($Δ= 1$), where $J_{2}^{c}(1) = 0.55 \pm 0.01$. By contrast, at the XY isotropic point ($Δ= 0$), we find $J_{2}^{c}(0) = 0.50 \pm 0.01$. In the Ising limit ($Δ\to \infty$) $J_2^c \to 0.5$ as expected.

cond-mat.str-el↗