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Superstructures and magnetic order in heavily Cu-substituted ( Fe 1x Cux ) 1+y Te

Journal Article · · Physical Review. B
 [1];  [1];  [2];  [3];  [4];  [5];  [4];  [4];  [1];  [6];  [6];  [6];  [6];  [7];  [1];  [8];  [1];  [3];  [4];  [9]
  1. Zhejiang Univ., Hangzhou (China)
  2. Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States); National Institute for Materials Science (NIMS), Tsukuba (Japan). Research Center for Electronic and Optical Materials
  3. Beijing Normal University, Beijing (China)
  4. Univ. of California, Berkeley, CA (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)
  5. Yale Univ., New Haven, CT (United States); Univ. of California, Berkeley, CA (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)
  6. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
  7. National Inst. of Standards and Technology (NIST), Gaithersburg, MD (United States). Center for Neutron Research; Univ. of Maryland, College Park, MD (United States)
  8. Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)
  9. Zhejiang Univ., Hangzhou (China); Univ. of California, Berkeley, CA (United States); Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States)
Most iron-based superconductors exhibit stripe-type magnetism, characterized by the ordering vector Q = ($$\frac{1}{2},\frac{1}{2}$$). In contrast, Fe1+yTe, the parent compound of the Fe1+yTe1–xSex superconductors, exhibits double-stripe magnetic order associated with the ordering vector Q = ($$\frac{1}{2},0$$). Here, we use elastic neutron scattering to investigate heavily Cu-substituted (Fe1–xCux)1+yTe compounds and reveal that (1) for x ≳ 0.4, short-range magnetic order emerges around the stripe-type vector at Q = ($$\frac{1}{2}$$ ± δ, $$\frac{1}{2}$$ ± δ, $$\frac{1}{2}$$) with δ ≈ 0.05; (2) the short-range magnetic order is associated with a superstructure modulation at Q = ($$\frac{1}{3},\frac{1}{3},\frac{1}{2}$$), with the magnetic correlation length shorter than that for the superstructure; and (3) for x ≳ 0.55, we observe an additional intergrown phase with higher Cu content, characterized by a superstructure modulation vector Q = ($$\frac{1}{3},\frac{1}{3},0$$) and magnetic peaks at Q = ($$\frac{2}{3},\frac{1}{3},\frac{1}{2}$$)/($$\frac{1}{3},\frac{2}{3},\frac{1}{2}$$). The positions of superstructure peaks suggest that relative to the tetragonal unit cell of Fe1+yTe, heavy Cu substitution leads to Fe-Cu orderings that expand the unit cell by $$\sqrt{2}$$ × 3$$\sqrt{2}$$ times in the ab plane, corroborated by first-principles calculations that suggest the formation of spin chains and spin ladders. Finally, our findings show that stripe-type magnetism is common in magnetically diluted iron pnictides and chalcogenides, despite the varying associated atomic orderings
Research Organization:
Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States); Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
Sponsoring Organization:
Key Research and Development Program of Zhejiang Province; National Key Research and Development Program of China; National Natural Science Foundation of China (NSFC); Pioneer and Leading Goose Research and Development Program of Zhejiang; USDOE Office of Science (SC), Basic Energy Sciences (BES); USDOE Office of Science (SC), Basic Energy Sciences (BES). Materials Sciences & Engineering Division (MSE); USDOE Office of Science (SC), Basic Energy Sciences (BES). Scientific User Facilities (SUF)
Grant/Contract Number:
AC02-05CH11231; AC05-00OR22725
OSTI ID:
2426067
Alternate ID(s):
OSTI ID: 2453881
OSTI ID: 2474357
Journal Information:
Physical Review. B, Journal Name: Physical Review. B Journal Issue: 4 Vol. 109; ISSN 2469-9950
Publisher:
American Physical Society (APS)Copyright Statement
Country of Publication:
United States
Language:
English

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