Abstract:We construct a metamaterial from radio-frequency harmonic oscillators, and find two topologically distinct phases resulting from dissipation engineered into the system. These phases are distinguished by a quantized value of bulk energy transport. The impulse response of our circuit is measured and used to reconstruct the band structure and winding number of circuit eigenfunctions around a dark mode. Our results demonstrate that dissipative topological transport can occur in a wider class of physical systems th… Show more
“…Previous studies have focused on nonlinearityinduced local self-interactions in the fundamental harmonic, which can give rise to solitons with anomalous * blzhang@ntu.edu.sg † yidong@ntu.edu.sg plateau-like decay profiles in nonlinear SSH chains [8,21], or chiral solitons in two-dimensional lattices [22][23][24][25][26][27]. It has also been suggested that topological edge states in nonlinear lattices could be used for robust traveling-wave parametric amplification [28], optical isolation [29], and other applications [30][31][32][33].…”
Nonlinear transmission lines (NLTLs) are nonlinear electronic circuits used for parametric amplification and pulse generation, and it is known that left-handed NLTLs support enhanced harmonic generation while suppressing shock wave formation. We show experimentally that in a left-handed NLTL analogue of the Su-Schrieffer-Heeger (SSH) lattice, harmonic generation is greatly increased by the presence of a topological edge state. Previous studies of nonlinear SSH circuits focused on solitonic behaviours at the fundamental harmonic. Here, we show that a topological edge mode at the first harmonic can produce strong propagating higher-harmonic signals, acting as a nonlocal cross-phase nonlinearity. We find maximum third-harmonic signal intensities five times that of a comparable conventional left-handed NLTL, and a 250-fold intensity contrast between topologically nontrivial and trivial configurations. This work advances the fundamental understanding of nonlinear topological states, and may have applications for compact electronic frequency generators.
“…Previous studies have focused on nonlinearityinduced local self-interactions in the fundamental harmonic, which can give rise to solitons with anomalous * blzhang@ntu.edu.sg † yidong@ntu.edu.sg plateau-like decay profiles in nonlinear SSH chains [8,21], or chiral solitons in two-dimensional lattices [22][23][24][25][26][27]. It has also been suggested that topological edge states in nonlinear lattices could be used for robust traveling-wave parametric amplification [28], optical isolation [29], and other applications [30][31][32][33].…”
Nonlinear transmission lines (NLTLs) are nonlinear electronic circuits used for parametric amplification and pulse generation, and it is known that left-handed NLTLs support enhanced harmonic generation while suppressing shock wave formation. We show experimentally that in a left-handed NLTL analogue of the Su-Schrieffer-Heeger (SSH) lattice, harmonic generation is greatly increased by the presence of a topological edge state. Previous studies of nonlinear SSH circuits focused on solitonic behaviours at the fundamental harmonic. Here, we show that a topological edge mode at the first harmonic can produce strong propagating higher-harmonic signals, acting as a nonlocal cross-phase nonlinearity. We find maximum third-harmonic signal intensities five times that of a comparable conventional left-handed NLTL, and a 250-fold intensity contrast between topologically nontrivial and trivial configurations. This work advances the fundamental understanding of nonlinear topological states, and may have applications for compact electronic frequency generators.
“…Electronic circuits have recently emerged as a convenient and accessible platform for studying the combination of non-linearity with band topology 13,85,[119][120][121][122][123][124][125][126][127] . Key advantages include the ease with which such circuits can be designed and fabricated using circuit simulators, printed circuit boards (PCBs), and other commodity technologies; the fact that they can be characterized using inexpensive laboratory equipment such as function generators and oscilloscopes; the availability of strongly nonlinear circuit elements; and the exciting prospect of using circuit wiring to implement complex geometries (like Möbius strips 119 ) that are practically impossible to realize on other platforms.…”
Section: Nonlinear Circuitsmentioning
confidence: 99%
“…119 was designed to have multiple identical sublattices whose interconnections replicate the effects of the complex inter-site couplings associated with a magnetic vector potential 120 ; this ensured that the states of the target quantum Hall system, including the crucial topological edge states, are a multiply-degenerate subset of the states of the T-symmetric circuit. A variety of T-symmetric topological phases have also been realized with LC circuits without using this sublattice trick, including linear 1D and 2D Su-Schrieffer-Heeger models 122,125 , topological crystalline insulators 124 , higher-order topological insulators 123,126 , and intrinsically non-Hermitian topological lattices 121 .…”
Section: Nonlinear Circuitsmentioning
confidence: 99%
“…In typical circuit experiments, the normal modes are studied using weakly-coupled probes such as pickup coils 119,124 , or direct connections to an oscilloscope or network analyzer 121,125 . Lee et al have also developed a rigorous frequency-domain formalism for analyzing circuits with explicit current sources and sinks 122 .…”
Rapidly growing demands for fast information processing have launched a race for creating compact and highly efficient optical devices that can reliably transmit signals without losses. Recently discovered topological phases of light provide a novel ground for photonic devices robust against scattering losses and disorder. Combining these topological photonic structures with nonlinear effects will unlock advanced functionalities such as nonreciprocity and active tunability. Here we introduce the emerging field of nonlinear topological photonics and highlight recent developments in bridging the physics of topological phases with nonlinear optics. This includes a design of novel photonic platforms which combine topological phases of light with appreciable nonlinear response, self-interaction effects leading to edge solitons in topological photonic lattices, nonlinear topological circuits, active photonic structures exhibiting lasing from topologically-protected modes, and harmonic generation from edge states in topological arrays and metasurfaces. We also chart future research directions discussing device applications such as mode stabilization in lasers, parametric amplifiers protected against feedback, and ultrafast optical switches employing topological waveguides.
“…Non-Hermitian quantum mechanics has been attracting much attention in many fields of physics in the past decades. Many experimental studies have realized various physical systems with non-Hermitian effects [1][2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18][19] . Among these experimental studies, appearance of exceptional points and rings where some energy eigenvalues become degenerate and the corresponding eigenstates coalesce 20,21 , and intriguing phenomena have been observed [22][23][24][25][26][27][28][29][30][31][32][33] .…”
To describe eigenstates in non-Hermitian crystalline systems, the non-Bloch band theory has recently been established, and the generalized Brillouin zone (GBZ) has unique features which are absent in Hermitian systems. In this Letter, we show that in one-dimensional non-Hermitian systems with both sublattice symmetry and time-reversal symmetry, a topological semimetal phase with exceptional points is stable. This stems from the unique features of the GBZ. We can relate the motion of the exceptional points with the change of the value of a topological invariant characterizing a topological insulator phase. It is also shown that the energy bands are divided into three region, depending on the symmetry of the eigenstates.
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