2021
DOI: 10.1103/physrevb.103.104429
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Diffraction by multipoles in a 5d2 rhenium double perovskite

Abstract: This is a copy of the published version, or version of record, available on the publisher's website. This version does not track changes, errata, or withdrawals on the publisher's site.

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Cited by 7 publications
(3 citation statements)
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“…Having thus placed bounds on the range of possible ordered moments in Ba 2 YReO 6 , we return to the implications on the possible underlying multipolar order. From a recent atomic theory [39], the dipole magnetic moment is μ o = (2/3) sin(2χ ) μ B where χ is the mixing angle for nonmagnetic and magnetic components of the ground state.…”
Section: Multipoles and Multipolar Ordermentioning
confidence: 99%
“…Having thus placed bounds on the range of possible ordered moments in Ba 2 YReO 6 , we return to the implications on the possible underlying multipolar order. From a recent atomic theory [39], the dipole magnetic moment is μ o = (2/3) sin(2χ ) μ B where χ is the mixing angle for nonmagnetic and magnetic components of the ground state.…”
Section: Multipoles and Multipolar Ordermentioning
confidence: 99%
“…In this paper, we focus on d 2 Mott insulators, where [20,21,27,28] have argued for a local J = 2 spin mo-ment, which can lead to various exotic orders including quadrupolar phases. We have recently reexamined this issue [29,30] and shown that virtual excitations into the high energy e g orbitals split the five-fold degeneracy of the J = 2 moment as 2(E g )⊕3(T 2g ), resulting in a ground state non-Kramers E g doublet carrying quadrupolar and octupolar moments.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast to magnetic orderings, the breaking of time-reversal (T ) symmetry is not necessary, and hence, qualitatively distinct low-energy excitations and physical phenomena are expected. The electronic nematic states have been discussed in various contexts, such as the Pomeranchuk instability [4][5][6], spin nematic state [7][8][9][10][11][12][13][14], and charge/orbital nematic state [15][16][17][18][19][20][21], which have been observed in d-electron materials like Ba 2 MgReO 6 [22][23][24] and f -electron materials, such as CeB 6 [25][26][27][28], PrPb 3 [29][30][31], PrT 2 X 20 (T = Ir, Rh, X = Zn; T = V, X = Al) [32][33][34][35][36], and CeCoSi [37][38][39][40][41][42][43]. Recently, further exotic states coexisting spin and nematic orders have been suggested, such as the CP 2 skyrmion [44][45][46][47] and other multiple-Q states [48]…”
Section: Introductionmentioning
confidence: 99%