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Abstract book - phy

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P-3 45<br />

NMR study of incommensurate helical<br />

magnetic order in the spin-chain<br />

cuprates LiCu 2 O 2 and NaCu 2 O 2<br />

A.A. Gippius 1 , N. Buettgen 2 , W. Kraetschmer 2 , M. Baenitz 3 ,<br />

L.E. Svistov 4 , A.S. Moskvin 5 , A.A. Bush 6<br />

1 Moscow State University, 119991 Moscow, Russia<br />

2 University of Augsburg, D-86135 Augsburg, Germany<br />

3 MPI for Chemical Physics of Solids 01187 Dresden Germany<br />

4 Institute for Physical Problems, 119334 Moscow, Russia<br />

5 Ural State University, 620083 Ekaterinburg, Russia<br />

6 Moscow Institute of Radiotechnics, 117464 Moscow, Russia<br />

A 7 Li NMR study of a LiCu 2 O 2 single crystal without twinning was performed<br />

in the temperature range around the transition into the magnetically<br />

ordered state. The transition into the incommensurate (IC) low-temperature<br />

helical phase occurs in two successive stages at temperatures T c1 = 24.7 K<br />

and T c2 = 22.8 K. The 7 Li NMR line shape evolution was studied in detail<br />

in the temperature range 22 K – 25 K in an external field around 7.7 T applied<br />

along the main crystallographic axes. The observed 7 Li NMR spectra<br />

in the intermediate temperature range differ considerably from those obtained<br />

in the low-temperature phase (T < T c2 ). This yields a clear signature<br />

of the different character of the IC magnetic structures of Cu 2+ spins in<br />

the intermediate and low-temperature phases, respectively. The 7 Li NMR<br />

results are compared with the 23 Na NMR spectra obtained in a NaCu 2 O 2<br />

single crystal [1] and are discussed in terms of both helical and collinear IC<br />

magnetic structures of Cu 2+ spins.<br />

[1] A.A. Gippius et al., Physical Review B 77 (2008) 180403R

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