TY - JOUR
T1 - Photoinduced collective mode, inhomogeneity, and melting in a charge-order system
AU - Seo, Hitoshi
AU - Tanaka, Yasuhiro
AU - Ishihara, Sumio
N1 - Funding Information:
The authors would like to thank S. Iwai, A. Ono, and K. Yonemistu for valuable discussions. This work was supported by JSPS KAKENHI Grants No. 26400377, No. 15H02100, No. 16H02393, No. 17H02916, and No. 18H05208.
Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/12/26
Y1 - 2018/12/26
N2 - We theoretically investigate photoresponses of a correlated electron system upon stimuli of a pulsed laser light. Real-time dynamics of an interacting spinless fermion model on a one-dimensional chain, as a model of charge order (CO), are numerically simulated using the time-dependent Hartree-Fock method. In particular, we discuss the differences between two situations as the initial state: the homogeneous order and the presence of a domain wall, i.e., a kink structure embedded in the CO bulk. Coherent dynamics are seen in the former case: When the frequency of the pump light ωp is varied, along with single particle excitations across the CO gap (ΔCO), the resonantly-excited collective phase mode near ωp≃ΔCO/2 efficiently destabilizes CO. In clear contrast, in the latter case, when ωp is tuned at such in-gap frequencies and the intensity of light is sufficiently large, inhomogeneity spreads out from the kink to the bulk region through kink creations. Moreover, even stronger intensity induces the inhomogeneous melting of CO where the CO gap is destroyed.
AB - We theoretically investigate photoresponses of a correlated electron system upon stimuli of a pulsed laser light. Real-time dynamics of an interacting spinless fermion model on a one-dimensional chain, as a model of charge order (CO), are numerically simulated using the time-dependent Hartree-Fock method. In particular, we discuss the differences between two situations as the initial state: the homogeneous order and the presence of a domain wall, i.e., a kink structure embedded in the CO bulk. Coherent dynamics are seen in the former case: When the frequency of the pump light ωp is varied, along with single particle excitations across the CO gap (ΔCO), the resonantly-excited collective phase mode near ωp≃ΔCO/2 efficiently destabilizes CO. In clear contrast, in the latter case, when ωp is tuned at such in-gap frequencies and the intensity of light is sufficiently large, inhomogeneity spreads out from the kink to the bulk region through kink creations. Moreover, even stronger intensity induces the inhomogeneous melting of CO where the CO gap is destroyed.
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U2 - 10.1103/PhysRevB.98.235150
DO - 10.1103/PhysRevB.98.235150
M3 - Article
AN - SCOPUS:85059505434
SN - 2469-9950
VL - 98
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 23
M1 - 235150
ER -