Unpinning the skyrmion lattice in MnSi

By employing magnetization and small angle neutron scattering (SANS) measurements, we have investigated the behavior of the skyrmion lattice (SKL) and the helical order in MnSi0.992Ga0.008. Our results indicate that the order of the SKL is sensitive to the orientation of an applied magnetic field with respect to the crystal lattice and small variations in the sequence of temperature and applied magnetic field changes. The disorder caused by the substitution of the heavier element Ga for Si is sufficient to reduce the pinning of the SKL to the underlying crystalline lattice. This reduces the propensity for the SKL to be aligned with the crystal lattice. This tendency is most evident when the applied field is not well oriented with respect to the high symmetry axes of the crystal resulting in disorder in the long range SKL while maintaining sharp radial order. We have also investigated the effect of substituting heavier elements into MnSi on the reorientation process of the helical domains with field cycling in MnSi0.992Ga0.008 and Mn0.985Ir0.015Si. A comparison of the reorientation process in these materials with field reduction indicates that the substitution of heavier elements on either Mn or Si sites creates a higher energy barrier for the reorientation of the helical order and for the formation of domains.

[1]  N. Nagaosa,et al.  Theory of the magnetic skyrmion glass , 2017, 1712.09782.

[2]  J. Betts,et al.  Anisotropic magnetocrystalline coupling of the skyrmion lattice in MnSi , 2017, 1712.05479.

[3]  K. Harada,et al.  Formation process of skyrmion lattice domain boundaries: The role of grain boundaries , 2017, 1907.00774.

[4]  T. Lograsso,et al.  Reorientations, relaxations, metastabilities, and multidomains of skyrmion lattices , 2017, 1707.04921.

[5]  D. Young,et al.  Exploring the origins of the Dzyaloshinskii-Moriya interaction in MnSi , 2017, 1707.05673.

[6]  Xubing Lu,et al.  Helical and skyrmion lattice phases in three-dimensional chiral magnets: Effect of anisotropic interactions , 2017, Scientific Reports.

[7]  C. Back,et al.  Dynamical Defects in Rotating Magnetic Skyrmion Lattices. , 2017, Physical review letters.

[8]  Y. Tokura,et al.  Topological domain walls in helimagnets , 2017, Nature Physics.

[9]  C. Pfleiderer,et al.  Symmetry breaking, slow relaxation dynamics, and topological defects at the field-induced helix reorientation in MnSi , 2016, 1611.06835.

[10]  M. Saghayezhian,et al.  Effect of negative chemical pressure on the prototypical itinerant magnet MnSi , 2016, 1609.08181.

[11]  Y. Endoh,et al.  Extended skyrmion lattice scattering and long-time memory in the chiral magnet Fe 1 − x Co x Si , 2016, 1610.07063.

[12]  Jan Muller Magnetic Skyrmions on a Two-Lane Racetrack , 2016, 1606.07412.

[13]  C. Pfleiderer,et al.  History dependence of the magnetic properties of single-crystal Fe 1 − x Co x Si , 2016, 1604.08025.

[14]  H. Berger,et al.  Multidomain Skyrmion Lattice State in Cu2OSeO3. , 2016, Nano letters.

[15]  C. Pfleiderer,et al.  Generic Aspects of Skyrmion Lattices in Chiral Magnets , 2016, 1603.08730.

[16]  H. Choi,et al.  Density functional theory study of skyrmion pinning by atomic defects in MnSi , 2016, 1601.00933.

[17]  M. Cantoni,et al.  Filming the formation and fluctuation of skyrmion domains by cryo-Lorentz transmission electron microscopy , 2015, Proceedings of the National Academy of Sciences.

[18]  J. White,et al.  A new class of chiral materials hosting magnetic skyrmions beyond room temperature , 2015, Nature Communications.

[19]  Y. Tokura,et al.  Topological properties and dynamics of magnetic skyrmions. , 2013, Nature nanotechnology.

[20]  D. Chernyshov,et al.  Chiral properties of structure and magnetism in Mn(1-x)Fe(x)Ge compounds: when the left and the right are fighting, who wins? , 2013, Physical review letters.

[21]  You-Quan Li,et al.  A mechanism to pin skyrmions in chiral magnets , 2012, Journal of physics. Condensed matter : an Institute of Physics journal.

[22]  M. Baenitz,et al.  Complex chiral modulations in FeGe close to magnetic ordering. , 2011, Physical review letters.

[23]  Y. Tokura,et al.  Possible skyrmion-lattice ground state in the B20 chiral-lattice magnet MnGe as seen via small-angle neutron scattering , 2012 .

[24]  T. Nattermann Domain walls in helical magnets: Elasticity and pinning , 2012, 1210.1358.

[25]  C. Pfleiderer,et al.  Magnetic phase diagram of MnSi inferred from magnetization and ac susceptibility , 2012, 1206.5774.

[26]  Y. Tokura,et al.  Magnetic stripes and skyrmions with helicity reversals , 2012, Proceedings of the National Academy of Sciences.

[27]  H. Berger,et al.  Long-wavelength helimagnetic order and skyrmion lattice phase in Cu2OSeO3. , 2012, Physical review letters.

[28]  Y. Tokura,et al.  Skyrmion flow near room temperature in an ultralow current density , 2012, Nature Communications.

[29]  T. Nattermann,et al.  Vortex domain walls in helical magnets. , 2011, Physical review letters.

[30]  Y. Tokura,et al.  Near room-temperature formation of a skyrmion crystal in thin-films of the helimagnet FeGe. , 2011, Nature materials.

[31]  Robert Georgii,et al.  Skyrmion Lattice Domains in Fe1−xCoxSi , 2010 .

[32]  P. Böni,et al.  Skyrmion Lattice in a Chiral Magnet , 2009, Science.

[33]  M. Calvo Micromagnetic theory of domain formation in helimagnets , 2008 .

[34]  Y. Tokura,et al.  Real-Space Observation of Helical Spin Order , 2006, Science.

[35]  Y. Ishizawa,et al.  MnSi and MnSi2−x single crystals growth by Ga flux method and properties , 2001 .

[36]  J. S. Pedersen,et al.  Small-angle neutron-scattering studies of the magnetic phase diagram of MnSi , 1995 .

[37]  M. Plumer Wavevector and spin-flop transitions in cubic FeGe , 1990 .

[38]  Jonte Bernhard,et al.  Magnetic structures of cubic FeGe studied by small-angle neutron scattering , 1989 .

[39]  P. Bak,et al.  Theory of helical magnetic structures and phase transitions in MnSi and FeGe , 1980 .