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Spin nematic fluctuations near a spin-density-wave phase

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Yamase,  H.
Department Quantum Many-Body Theory (Walter Metzner), Max Planck Institute for Solid State Research, Max Planck Society;

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Zeyher,  R.
Department Quantum Many-Body Theory (Walter Metzner), Max Planck Institute for Solid State Research, Max Planck Society;
Former Departments, Max Planck Institute for Solid State Research, Max Planck Society;

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Citation

Yamase, H., & Zeyher, R. (2015). Spin nematic fluctuations near a spin-density-wave phase. New Journal of Physics, 17: 073030.


Cite as: https://hdl.handle.net/21.11116/0000-000E-CB38-F
Abstract
We study an interacting electronic system exhibiting a spin nematic instability. Using a phenomenological form for the spin fluctuation spectrum near the spin-density-wave (SDW) phase, we compute the spin nematic susceptibility in energy and momentum space as a function of temperature and the magnetic correlation length.. The spin nematic instability occurs when. reaches a critical value xi(cr), i.e., its transition temperature T-SN is always higher than the SDW critical temperature T-SDW. In particular, xi(cr) decreases monotonically with increasing T-SN. Concomitantly, low-energy nematic fluctuations are present in a wider temperature region as T-SN becomes higher. Approaching the spin nematic instability, the nematic spectral function at zero momentum exhibits a central peak as a function of energy for a finite temperature and a soft mode at zero temperature. These properties originate from the general feature that the imaginary part of the spin-fluctuation bubble has a term linear in energy and its coefficient is proportional to the square of temperature. Furthermore we find that the nematic spectral function exhibits a diffusive peak around zero momentum and zero energy without clear dispersive features. A possible phase diagram for the spin nematic and SDW transitions is also discussed.