2020
DOI: 10.1126/sciadv.abc1160
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Coexistence of a new type of bound state in the continuum and a lasing threshold mode induced by PT symmetry

Abstract: Some photonic systems support bound states in the continuum (BICs) that have infinite lifetimes, although their frequencies and momenta are matched to vacuum modes. Using a prototypical system that can be treated analytically, we show that each of these BICs always splits into a pair of new type BIC and lasing threshold mode when a parity-time (PT)–symmetric perturbation is introduced. The radiation loss at the lasing threshold is exactly balanced by the net gain of the particles. These PT symmetry-induced BIC… Show more

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Cited by 63 publications
(35 citation statements)
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“…The wavelength-dependent complex refractive index of Si is extracted from experimental data 49 , and the constant refractive index of 1.45 is assigned to SiO 2 . Note that we choose the dimer design as it belongs to a symmetric geometry of C 2v group and possesses more structural parameters to be tuned than C 4v configurations [50][51][52][53][54][55][56][57][58][59] . Benefiting from the additional degree of freedom, it is possible to manipulate the excitation of dual BIC resonances by adjusting the structural geometry and rotating the fundamental pump polarization.…”
Section: Polarization-controlled Dual Bound States In the Continuummentioning
confidence: 99%
“…The wavelength-dependent complex refractive index of Si is extracted from experimental data 49 , and the constant refractive index of 1.45 is assigned to SiO 2 . Note that we choose the dimer design as it belongs to a symmetric geometry of C 2v group and possesses more structural parameters to be tuned than C 4v configurations [50][51][52][53][54][55][56][57][58][59] . Benefiting from the additional degree of freedom, it is possible to manipulate the excitation of dual BIC resonances by adjusting the structural geometry and rotating the fundamental pump polarization.…”
Section: Polarization-controlled Dual Bound States In the Continuummentioning
confidence: 99%
“…A PT -symmetric Hamiltonian satisfies [ Ĥ, P T ] = 0, with the joint parity-time operator ( P T ). PT -symmetric non-Hermitian Hamiltonians feature unconventional properties in numerous systems ranging from classical [4][5][6][7][8][9][10][11][12][13][14][15] to quantum systems [16][17][18][19][20][21][22][23][24][25][26]. When the Hamiltonian parameters cross the exceptional point (EP), PT symmetry is broken, leading to a symmetry-breaking transition.…”
Section: Introductionmentioning
confidence: 99%
“…In the last two decades, BICs have been observed in many photonic structures such as photonic crystals, metasurfaces, [2][3][4], chains of coupled resonators [5][6][7][8], waveguides [9][10][11][12][13] and even single subwavelength resonators supporting quasi-BIC in a form of supercavity modes [14][15][16]. A divergent radiative quality (Q) factor, strong spatial localization, and drastic enhancement of the incident field make BICs very prospective for many applications including lasers [17][18][19][20][21][22][23][24][25], optical filters [26][27][28], biological and chemical sensors [29][30][31][32][33], and non-linear photonics [34][35][36][37][38][39][40][41][42][43].…”
Section: Introductionmentioning
confidence: 99%