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All optical excitation of spin polarization in d-wave altermagnets

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arxiv 2408.05187 v3 pith:Y65ROICC submitted 2024-08-09 cond-mat.mtrl-sci cond-mat.mes-hall

All optical excitation of spin polarization in d-wave altermagnets

classification cond-mat.mtrl-sci cond-mat.mes-hall
keywords spinopticalpolarizationaltermagneticd-waveelectronicfilmslinearly
verification ladder T0 review T1 audit T2 compute T3 formal T4 reserved
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The recently discovered altermagnets exhibit collinear magnetic order with zero net magnetization but with unconventional spin-polarized d/g/i-wave band structures, expanding the known paradigms of ferromagnets and antiferromagnets. In addition to novel current-driven electronic transport effects, the unconventional time-reversal symmetry breaking in these systems also makes it possible to obtain a spin response to \emph{linearly polarized} fields in the optical frequency domain. We show through ab-initio calculations of the prototypical d-wave altermagnet RuO$_2$, with a symmetry combining twofold spin rotation with fourfold lattice rotation, $[C_2\|C_{4z}]$, that there is an optical analogue of a spin splitter effect, as the coupling to a linearly polarized exciting laser field makes the d-wave character of the altermagnet directly visible. By magneto-optical measurements on RuO$_2$ films of different thicknesses ranging from $2$ to $8\,$nanometers, we demonstrate the predicted connection of the linear polarization of an ultrashort pump pulse to the sign and magnitude of the optically excited electronic spin polarization in the ultrathin RuO$_2$ films. The possibility of exciting and controlling an electronic spin polarization by linearly polarized optical pulses in a compensated system is a unique consequence of the altermagnetic material properties. Our experimental results therefore establish an optical pump-probe based protocol for detection of altermagnetic characteristics in ultrathin RuO$_2$ films, but our all-optical approach should apply more generally to materials in this altermagnetic symmetry class.

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Cited by 9 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

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    cond-mat.mtrl-sci 2026-06 unverdicted novelty 7.0

    Bichromatic Floquet driving activates giant perpendicular Edelstein polarizations in 2D altermagnets by breaking rotational symmetry.

  2. RKKY interaction in altermagnets with adiabatic electron-phonon coupling

    cond-mat.mtrl-sci 2026-04 unverdicted novelty 7.0

    Static lattice distortions from adiabatic electron-phonon coupling act as a tuning knob that alters the magnitude, anisotropy, phase, and chirality of noncollinear RKKY couplings in Rashba d-wave altermagnets.

  3. High-Harmonic Spin and Charge Pumping in Altermagnets

    cond-mat.mes-hall 2026-02 unverdicted novelty 7.0

    Altermagnets intrinsically generate hundreds of high harmonics in spin and charge pumping under magnetic dynamics, with amplitudes exceeding light-driven schemes and without needing extra spin-orbit coupling.

  4. Magneto-optical Kerr effect in pump-probe setups

    cond-mat.mtrl-sci 2025-12 unverdicted novelty 7.0

    A DPOA-based formalism computes time-resolved Kerr rotation from the time-evolved single-particle density matrix in pumped systems, demonstrated on a two-band model and germanium.

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    cond-mat.str-el 2025-10 unverdicted novelty 7.0

    Cavity driving induces coherent magnetization and polariton signatures in d-wave altermagnets via selective sublattice coupling in a mean-field Lindblad model.

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    cond-mat.mtrl-sci 2025-10 unverdicted novelty 7.0

    Slow phonons suppress the spin Edelstein effect in strained Rashba d-wave altermagnets through energy renormalization that collapses the Fermi surface, producing tunable anisotropic depolarization.

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    cond-mat.mtrl-sci 2025-08 unverdicted novelty 7.0

    Interlayer sliding in M2A2B and M2AA'B bilayer altermagnets induces ferrovalley polarization and antiferromagnetic half-metallicity, with Mo2O2O showing 0.31 eV valley splitting and V2SSeO as a candidate half-metal.

  8. Chiral Altermagnetic Magnetoelectrics

    cond-mat.mtrl-sci 2025-08 unverdicted novelty 7.0

    Introduces chiral altermagnetic magnetoelectrics in nonpolar chiral systems and identifies K[Co(HCOO)3] as a platform with Néel-vector and chirality-controlled switchable polarization.

  9. Strain Engineering of Altermagnetic Symmetry in Epitaxial RuO$_2$ Films

    cond-mat.mtrl-sci 2025-10 unverdicted novelty 6.0

    Compressive strain along [001] stabilizes altermagnetism in RuO2 films on (100) and (110) TiO2 substrates, tunable by film thickness, with (100) orientation yielding ideal altermagnetic order and (110) showing uncompe...