Quantum Dynamics of the Hubbard-Holstein Model in Equilibrium and Nonequilibrium: Application to Pump-Probe Phenomena

被引:63
|
作者
De Filippis, G. [1 ,2 ]
Cataudella, V. [1 ,2 ]
Nowadnick, E. A. [3 ,4 ]
Devereaux, T. P. [3 ,5 ]
Mishchenko, A. S. [6 ,7 ]
Nagaosa, N. [6 ,8 ]
机构
[1] Univ Naples Federico II, SPIN CNR, I-80126 Naples, Italy
[2] Univ Naples Federico II, Dipartimento Sci Fis, I-80126 Naples, Italy
[3] Stanford Inst Mat & Energy Sci, SLAC Natl Accelerator Lab, Menlo Pk, CA 94025 USA
[4] Stanford Univ, Dept Phys, Stanford, CA 94305 USA
[5] Stanford Univ, Geballe Lab Adv Mat, Stanford, CA 94305 USA
[6] RIKEN Adv Sci Inst ASI, Cross Correlated Mat Res Grp, Wako, Saitama 3510198, Japan
[7] RRC Kurchatov Inst, Moscow 123182, Russia
[8] Univ Tokyo, Dept Appl Phys, Bunkyo Ku, Tokyo 113, Japan
基金
日本学术振兴会; 日本科学技术振兴机构;
关键词
OPTICAL-ABSORPTION; ELECTRON; PHASE; CONDUCTIVITY; EXCITATIONS; SYSTEMS; LATTICE; HOLE;
D O I
10.1103/PhysRevLett.109.176402
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The spectral response and physical features of the 2D Hubbard-Holstein model are calculated both in equilibrium at zero and low chemical dopings, and after an ultrashort powerful light pulse, in undoped systems. At equilibrium and at strong charge-lattice couplings, the optical conductivity reveals a three-peak structure in agreement with experimental observations. After an ultrashort pulse and at nonzero electron-phonon interaction, phonon and spin subsystems oscillate with the phonon period T-ph approximate to 80 fs. The decay time of the phonon oscillations is about 150-200 fs, similar to the relaxation time of the charge system. We propose a criterion for observing these oscillations in high T-c compounds: the time span of the pump light pulse tau(pump) has to be shorter than the phonon oscillation period T-ph.
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页数:5
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