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Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the …
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Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the single-soliton comb highly challenging. Furthermore, limited wavelength tunability and low-power of on-chip lasers make controlled excitation of different soliton comb states in an integrated platform, where both the pump laser and microresonator are on the same chip, difficult. Here we address all these issues and demonstrate efficient excitation of soliton combs, and reversible switching between a two-soliton crystal and single-soliton state using polarization control of a fixed wavelength pump. We directly pump a silica microsphere with ~35 mW power from a continuous-wave laser at a fixed wavelength and tune its polarization to generate Brillouin laser-pumped soliton combs and achieve deterministic switching from a two-soliton crystal to a single-soliton comb and back to two-soliton crystal. While switching from a higher-order soliton crystal to single-soliton state has been demonstrated earlier, to the best of our knowledge, deterministic switching from a single-soliton to a higher-order soliton crystal has not been observed. The observed comb lines for the three- and two-soliton crystals are only 4 and 6 dB lower, respectively, than the Brillouin Stokes signal, resulting in an enhancement factor of up to ~2000 compared to similar works, where the comb lines are 20-40 dB lower than the center comb line. The obtained comb was immune to variations in polarization and could be re-excited and reproduced at the same wavelength just by controlling the polarization. Demonstration of a Brillouin laser-pumped microcomb soliton through the polarization control of a low-power laser at a fixed frequency paves the way for an efficient fully integrated microcomb soliton using on-chip lasers, microresonators and electro-optic polarization controllers for applications ranging from on-chip optical atomic clocks to quantum computing.
Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the …
Lire le résumé scientifique complet
Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the single-soliton comb highly challenging. Furthermore, limited wavelength tunability and low-power of on-chip lasers make controlled excitation of different soliton comb states in an integrated platform, where both the pump laser and microresonator are on the same chip, difficult. Here we address all these issues and demonstrate efficient excitation of soliton combs, and reversible switching between a two-soliton crystal and single-soliton state using polarization control of a fixed wavelength pump. We directly pump a silica microsphere with ~35 mW power from a continuous-wave laser at a fixed wavelength and tune its polarization to generate Brillouin laser-pumped soliton combs and achieve deterministic switching from a two-soliton crystal to a single-soliton comb and back to two-soliton crystal. While switching from a higher-order soliton crystal to single-soliton state has been demonstrated earlier, to the best of our knowledge, deterministic switching from a single-soliton to a higher-order soliton crystal has not been observed. The observed comb lines for the three- and two-soliton crystals are only 4 and 6 dB lower, respectively, than the Brillouin Stokes signal, resulting in an enhancement factor of up to ~2000 compared to similar works, where the comb lines are 20-40 dB lower than the center comb line. The obtained comb was immune to variations in polarization and could be re-excited and reproduced at the same wavelength just by controlling the polarization. Demonstration of a Brillouin laser-pumped microcomb soliton through the polarization control of a low-power laser at a fixed frequency paves the way for an efficient fully integrated microcomb soliton using on-chip lasers, microresonators and electro-optic polarization controllers for applications ranging from on-chip optical atomic clocks to quantum computing.
Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the …
Lire le résumé scientifique complet
Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the single-soliton comb highly challenging. Furthermore, limited wavelength tunability and low-power of on-chip lasers make controlled excitation of different soliton comb states in an integrated platform, where both the pump laser and microresonator are on the same chip, difficult. Here we address all these issues and demonstrate efficient excitation of soliton combs, and reversible switching between a two-soliton crystal and single-soliton state using polarization control of a fixed wavelength pump. We directly pump a silica microsphere with ~35 mW power from a continuous-wave laser at a fixed wavelength and tune its polarization to generate Brillouin laser-pumped soliton combs and achieve deterministic switching from a two-soliton crystal to a single-soliton comb and back to two-soliton crystal. While switching from a higher-order soliton crystal to single-soliton state has been demonstrated earlier, to the best of our knowledge, deterministic switching from a single-soliton to a higher-order soliton crystal has not been observed. The observed comb lines for the three- and two-soliton crystals are only 4 and 6 dB lower, respectively, than the Brillouin Stokes signal, resulting in an enhancement factor of up to ~2000 compared to similar works, where the comb lines are 20-40 dB lower than the center comb line. The obtained comb was immune to variations in polarization and could be re-excited and reproduced at the same wavelength just by controlling the polarization. Demonstration of a Brillouin laser-pumped microcomb soliton through the polarization control of a low-power laser at a fixed frequency paves the way for an efficient fully integrated microcomb soliton using on-chip lasers, microresonators and electro-optic polarization controllers for applications ranging from on-chip optical atomic clocks to quantum computing.
Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the …
Lire le résumé scientifique complet
Excitation of microcomb solitons requires optimization of a number of pump laser parameters such as wavelength scan speed, pump detuning from the cavity resonance, and optical power, making their efficient excitation, and reversible switching between a N-soliton crystal and the single-soliton comb highly challenging. Furthermore, limited wavelength tunability and low-power of on-chip lasers make controlled excitation of different soliton comb states in an integrated platform, where both the pump laser and microresonator are on the same chip, difficult. Here we address all these issues and demonstrate efficient excitation of soliton combs, and reversible switching between a two-soliton crystal and single-soliton state using polarization control of a fixed wavelength pump. We directly pump a silica microsphere with ~35 mW power from a continuous-wave laser at a fixed wavelength and tune its polarization to generate Brillouin laser-pumped soliton combs and achieve deterministic switching from a two-soliton crystal to a single-soliton comb and back to two-soliton crystal. While switching from a higher-order soliton crystal to single-soliton state has been demonstrated earlier, to the best of our knowledge, deterministic switching from a single-soliton to a higher-order soliton crystal has not been observed. The observed comb lines for the three- and two-soliton crystals are only 4 and 6 dB lower, respectively, than the Brillouin Stokes signal, resulting in an enhancement factor of up to ~2000 compared to similar works, where the comb lines are 20-40 dB lower than the center comb line. The obtained comb was immune to variations in polarization and could be re-excited and reproduced at the same wavelength just by controlling the polarization. Demonstration of a Brillouin laser-pumped microcomb soliton through the polarization control of a low-power laser at a fixed frequency paves the way for an efficient fully integrated microcomb soliton using on-chip lasers, microresonators and electro-optic polarization controllers for applications ranging from on-chip optical atomic clocks to quantum computing.
Abstract The Wronskians solutions to the sine-Gordon (sG) equation that can provide interaction of different kinds of solutions are revisited. A novel expression N-soliton solution with a nonzero background is presented which is used to construct the soliton and breather …
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Abstract The Wronskians solutions to the sine-Gordon (sG) equation that can provide interaction of different kinds of solutions are revisited. A novel expression N-soliton solution with a nonzero background is presented which is used to construct the soliton and breather solutions. Due to the existences of abundant structures of the solitons and breathers, it is possible to search for the coherent structures, or bounded states of solitons and breathers. By introducing the velocity resonant conditions, the sG equation is proved to possess the bounded state for breathers-soliton, or breather-soliton molecules (BSMs) and the bounded state for breathers, or breather molecules (BMs) by different parameters selections. In addition, an approximately bounded state for solitons is demonstrated. The interesting thing is the interactions among the BSMs, BMs and solitons, breathers may be nonelastic by the particular meaning the sizes of the BSMs and BMs change.
Abstract We propose a novel platform for quantum metrology based on qubit states of two Bose-Einstein condensate solitons, optically manipulated, trapped in a double-well potential, and coupled through nonlinear Josephson effect. We describe steady-state solutions in different scenarios and perform …
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Abstract We propose a novel platform for quantum metrology based on qubit states of two Bose-Einstein condensate solitons, optically manipulated, trapped in a double-well potential, and coupled through nonlinear Josephson effect. We describe steady-state solutions in different scenarios and perform a phase space analysis in the terms of population imbalance - phase difference variables to demonstrate macroscopic quantum self-trapping regimes. Schrödinger-cat states, maximally path-entangled (N00N) states, and macroscopic soliton qubits are predicted and exploited to distinguish the obtained macroscopic states in the framework of binary (non-orthogonal) state discrimination problem. For arbitrary phase estimation in the framework of linear quantum metrology approach, these macroscopic soliton states are revealed to have a scaling up to the Heisenberg limit (HL). The examples illustrate the HL estimation of angular frequency between the ground and first excited macroscopic states of the condensate, which opens new perspectives for current frequency standard technologies.