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Temporal Goos-Hänchen Shift in Synthetic Discrete-Time Heterolattices.
Qin, Chengzhi; Wang, Shulin; Wang, Bing; Hu, Xinyuan; Liu, Chenyu; Li, Yinglan; Zhao, Lange; Ye, Han; Longhi, Stefano; Lu, Peixiang.
Affiliation
  • Qin C; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Wang S; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Wang B; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Hu X; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Liu C; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Li Y; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Zhao L; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Ye H; Wuhan National Laboratory for Optoelectronics and School of Physics, <a href="https://ror.org/00p991c53">Huazhong University of Science and Technology</a>, Wuhan 430074, China.
  • Longhi S; Dipartimento di Fisica, <a href="https://ror.org/01nffqt88">Politecnico di Milano</a>, Piazza Leonardo da Vinci 32, I-20133 Milano, Italy.
  • Lu P; <a href="https://ror.org/00pfxsh56">IFISC (UIB-CSIC)</a>, Instituto de Fisica Interdisciplinar y Sistemas Complejos, E-07122 Palma de Mallorca, Spain.
Phys Rev Lett ; 133(8): 083802, 2024 Aug 23.
Article in En | MEDLINE | ID: mdl-39241724
ABSTRACT
Experimental demonstration of tunable temporal Goos-Hänchen shift (GHS) in synthetic discrete-time heterolattices with scalar and vector gauge potentials is reported. By using Heaviside-function modulation in two fiber loops, we create a sharp gauge-potential interface and observe temporal GHS for total internal reflection (TIR), which manifests as a time delay rather than a spatial shift. The TIR occurs as the incident mode falls into the band gap of transmitted region with band shifting by scalar and vector potential. We find that both scalar and vector potential codetermine GHS by controlling the decay (imaginary part) and oscillation (real part) of a penetrated evanescent wave, in stark contrast to traditional spatial GHS only determined by the decay factor. We also observe diverging characteristics of GHS at band-gap edges where evanescent-to-propagating wave transition occurs. GHS for frustrated total internal reflection (FTIR) by a finite-width evanescent barrier is also demonstrated, which shows saturation properties to the single-interface TIR case under infinite-width limit. Finally, we develop an accumulation measurement method using multiple TIRs to improve the precision for measuring even tinier GHS. The study initiates precise measurement of temporal GHS for discrete-time reflections, which may feature potential applications in precise time-delay control and measurement.

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2024 Document type: Article Affiliation country: China Country of publication: Estados Unidos

Full text: 1 Collection: 01-internacional Database: MEDLINE Language: En Journal: Phys Rev Lett Year: 2024 Document type: Article Affiliation country: China Country of publication: Estados Unidos