Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

IEEE Photonics Technology Letters

Nonlinear Quasi-BIC With Non-Hermitian Polarization Phase Quantization in Sm 3+ :BiPO 4

Muhammad Asad Iqbal, Zeeshan Mujahid, Muhammad Qasim Khan, U. Javed, M. Usman, Faisal Munir, F. Nadeem, Fiza Latif, P. Li, Yanpeng Zhang

Published Jan 28, 2026• 0 citations
Publisher

Abstract

This study investigates quasi bound states in the continuum (qBICs) in profile and resonance signals arising from polarization phase quantization in Sm3+:BiPO4. Two types of profile qBICs (third-order non-resonance profile qBIC and fourth-order resonance profile qBIC), result from destructive and constructive quantization phase, respectively. In addition, two types of third-order resonance qBICs, namely two-dark/one-bright states (2D1B) and one-dark/two-bright states (1D2B), are observed at constructive and destructive channel phase, respectively. The third-order 2D1B states resonance qBIC together with two optical jump, comes from eigenvector amplitude splitting near the exceptional point (EP) due to quasi-constructive quantization phase. These findings suggest potential applications in the interference-based quantum memory devices.

DOI
10.1109/lpt.2026.3658487

Related papers

Non-Hermitian optical bistability with polarization quantization in Sm3+:BiPO4

Usman Javed, Qasim Khan, Faisal Munir +5 more

In this study, we investigate non-Hermitian optical bistability in Sm3+:BiPO4 under the influence of polarization quantization. Our work focuses on how polarization affects this bistability, especially near exceptional points (EPs) in a non-Hermitian system. We demonstrate two types of optical bistability jumps: two-step one optical bistability jump and three-step two optical bistability jumps resulting from constructive and destructive polarization quantization. One optical bistability jump, without and with a non-Hermitian self-dressing switch, is observed at destructive and constructive polarization quantization near EP region, respectively. Two optical bistability jumps via nested-cascade dressing at horizontal polarization quantization are stronger than three cascaded dressings at circular polarization quantization. In addition, two types of non-Hermitian optical bistability jumps fit the second-order eigenvector intensity splitting theoretical model. Our findings are significant in controlling optical switching in materials used for quantum technologies. Such results have potential applications in quantization phase transitions in non-Hermitian photonic systems and advanced optical devices.

Applied Physics Letters•Jan 12, 2026•5 citations

Non‐Hermitian Photon‐Phonon Quantization Evolution Controlled by QWP Polarization Phase in Sm 3+ : BiPO 4

Sehrish Aslam, Usman Javed, Fiza Latif +4 more

ABSTRACT Non‐Hermitian quantum dynamics provide powerful approaches for controlling gain and loss in open quantum systems. However, experimental methods for tuning non‐Hermitian quantization remain limited. In this work, we investigate the evolution of non‐Hermitian photon–phonon dressed‐state quantization in Sm 3+ : BiPO 4 controlled by the polarization‐dressing phase using a quarter‐wave plate (QWP). We observed three types of destructive and constructive switching behavior, governed by the initial phase and determined by the competition between photon‐dressing Rabi frequency and dephasing rate. By continuously tuning the polarization phase, destructive quantization appears when the dephasing rate is dominant, whereas constructive quantization is stabilized by the photon Rabi frequency. These regimes exhibit discrete optical jumps, Landau‐like step‐level macroscopic quantization, and exceptional‐point switching between correlated states. Lower excitation power further enhances polarization‐controlled dressing quantization because of the larger dephasing rate. These results establish polarization phase as an effective control parameter for non‐Hermitian quantum jumps and macroscopic quantization, opening new possibilities for optical switching and quantum memory applications.

Advanced Quantum Technologies•Aug 29, 2026•0 citations

Non-Hermitian high-order constructive-destructive polarization quantization centers in Sm3+: BiPO4

Muhammad Qasim Khan, Hamza javaid, Fiza Latif +4 more

Optics & Laser Technology•Mar 11, 2026•0 citations

Photon–phonon destructive–constructive polarization quantization in Sm3+:BiPO4

Iqbal Hussain, Faisal Nadeem, Qasim Khan +4 more

We report photon-phonon dressing quantization dependency on polarization. Destructive dressing polarization quantization is exhibited in fluorescence (FL) for narrowband signals, while constructive dominant dressing quantization is exhibited in fluorescence (FL) for broadband signals due to phase perturbation. Furthermore, constructive polarization quantization results due to coexistence of generation and dressing effects in strong and competitive Rabi frequency. Low power also contributes to more dressing polarization quantization, the same as in the FL region (large de-phase rate). Furthermore, linear and circular dressing quantization with polarization quantization shows inverse and direct relationships in the FL and spontaneous four-wave-mixing (SFWM) regions, respectively. Such investigations have potential in alignment of crystal field (CF) redistribution by polarization quantization at the input.

Optics Letters•Nov 13, 2024•8 citations

Quantum Pair Generation in Nonlinear Metasurfaces with Mixed and Pure Photon Polarizations

Jiho Noh, Tomás Santiago‐Cruz, Vitaliy Sultanov +4 more

Metasurfaces are highly effective at manipulating classical light in the linear regime; however, effectively controlling the polarization of nonclassical light generated from nonlinear resonant metasurfaces remains a challenge. Here, we present a solution by achieving polarization engineering of frequency-nondegenerate biphotons emitted via spontaneous parametric down-conversion in GaAs metasurfaces, utilizing quasi-bound states in the continuum (qBIC) resonances to enhance biphoton generation. Through comprehensive polarization tomography, we demonstrate that the emitted photons' polarization directly reflects the qBIC mode's far-field properties. Furthermore, we show that both the type of qBIC mode and the symmetry of the meta-atoms can be tailored to control each single-photon polarization state, and that the subsequent two-photon polarization states are nearly separable, offering potential applications in the heralded generation of single photons with adjustable polarization. This work provides a significant step toward utilizing metasurfaces to generate quantum light and engineer their polarization, a critical aspect for future quantum technologies.

arXiv:2409.04569•Nano Letters•Nov 21, 2024•21 citations

Cavity magnonics and bound states in the continuum with Bragg and anti-Bragg mirrors

B. -Y. Wu, K. -P. Li, G. Chen +7 more

A periodic resonant emitter array coupled to a one-dimensional waveguide can act as a mirror. A typical example is a Bragg mirror, where emitters are spaced by multiples of half wavelengths and collectively enhance light reflection. Two such mirrors form an effective cavity that hosts bound states in the continuum (BICs). However, generating and detecting the spatial profiles of such BICs has proven challenging. Here, we experimentally demonstrate BICs in cavity magnonics using two periodic ferrimagnetic-sphere arrays and a probe sphere in a dual-open-waveguide architecture. We realize both Bragg and anti-Bragg cavities, whose mirrors have different lattice constants. In the Bragg cavity, there are degenerate supermodes formed by mirror spheres. We show that a single dark supermode coherently couples to the probe magnon in the cavity region, forming two polaritons whose splitting scales with both the probe-sphere size and the number of mirror spheres. By contrast, the anti-Bragg cavity has bright and dark supermodes in a bandgap, substantially changing the magnon-cavity interaction. Moreover, by moving the probe sphere, we perform position-dependent detection of the cavity field, highlighting the role of BICs in these cavities. Our flexible experimental setup with a scanning probe opens possibilities to detect other exotic states created by light-matter interaction, to interface with superconducting circuits in hybrid quantum networks, and to study non-Hermitian physics with Bragg and anti-Bragg cavities.

quant-pharXiv:2609.34365•Sep 29, 2026
This study investigates quasi bound states in the continuum (qBICs) in profile and resonance signals arising from polarization phase quantization in Sm3+:BiPO4. Two types of profile qBICs (third-order non-resonance profile qBIC and fourth-order resonance profile qBIC), result from destructive and constructive quantization phase, respectively. In addition, two types of third-order resonance qBICs, namely two-dark/one-bright states (2D1B) and one-dark/two-bright states (1D2B), are observed at constructive and destructive channel phase, respectively. The third-order 2D1B states resonance qBIC together with two optical jump, comes from eigenvector amplitude splitting near the exceptional point (EP) due to quasi-constructive quantization phase. These findings suggest potential applications in the interference-based quantum memory devices.
In this study, we investigate non-Hermitian optical bistability in Sm3+:BiPO4 under the influence of polarization quantization. Our work focuses on how polarization affects this bistability, especially near exceptional points (EPs) in a non-Hermitian system. We demonstrate two types of optical bistability jumps: two-step one optical bistability jump and three-step two optical bistability jumps resulting from constructive and destructive polarization quantization. One optical bistability jump, without and with a non-Hermitian self-dressing switch, is observed at destructive and constructive polarization quantization near EP region, respectively. Two optical bistability jumps via nested-cascade dressing at horizontal polarization quantization are stronger than three cascaded dressings at circular polarization quantization. In addition, two types of non-Hermitian optical bistability jumps fit the second-order eigenvector intensity splitting theoretical model. Our findings are significant in controlling optical switching in materials used for quantum technologies. Such results have potential applications in quantization phase transitions in non-Hermitian photonic systems and advanced optical devices.
ABSTRACT Non‐Hermitian quantum dynamics provide powerful approaches for controlling gain and loss in open quantum systems. However, experimental methods for tuning non‐Hermitian quantization remain limited. In this work, we investigate the evolution of non‐Hermitian photon–phonon dressed‐state quantization in Sm 3+ : BiPO 4 controlled by the polarization‐dressing phase using a quarter‐wave plate (QWP). We observed three types of destructive and constructive switching behavior, governed by the initial phase and determined by the competition between photon‐dressing Rabi frequency and dephasing rate. By continuously tuning the polarization phase, destructive quantization appears when the dephasing rate is dominant, whereas constructive quantization is stabilized by the photon Rabi frequency. These regimes exhibit discrete optical jumps, Landau‐like step‐level macroscopic quantization, and exceptional‐point switching between correlated states. Lower excitation power further enhances polarization‐controlled dressing quantization because of the larger dephasing rate. These results establish polarization phase as an effective control parameter for non‐Hermitian quantum jumps and macroscopic quantization, opening new possibilities for optical switching and quantum memory applications.
We report photon-phonon dressing quantization dependency on polarization. Destructive dressing polarization quantization is exhibited in fluorescence (FL) for narrowband signals, while constructive dominant dressing quantization is exhibited in fluorescence (FL) for broadband signals due to phase perturbation. Furthermore, constructive polarization quantization results due to coexistence of generation and dressing effects in strong and competitive Rabi frequency. Low power also contributes to more dressing polarization quantization, the same as in the FL region (large de-phase rate). Furthermore, linear and circular dressing quantization with polarization quantization shows inverse and direct relationships in the FL and spontaneous four-wave-mixing (SFWM) regions, respectively. Such investigations have potential in alignment of crystal field (CF) redistribution by polarization quantization at the input.
Metasurfaces are highly effective at manipulating classical light in the linear regime; however, effectively controlling the polarization of nonclassical light generated from nonlinear resonant metasurfaces remains a challenge. Here, we present a solution by achieving polarization engineering of frequency-nondegenerate biphotons emitted via spontaneous parametric down-conversion in GaAs metasurfaces, utilizing quasi-bound states in the continuum (qBIC) resonances to enhance biphoton generation. Through comprehensive polarization tomography, we demonstrate that the emitted photons' polarization directly reflects the qBIC mode's far-field properties. Furthermore, we show that both the type of qBIC mode and the symmetry of the meta-atoms can be tailored to control each single-photon polarization state, and that the subsequent two-photon polarization states are nearly separable, offering potential applications in the heralded generation of single photons with adjustable polarization. This work provides a significant step toward utilizing metasurfaces to generate quantum light and engineer their polarization, a critical aspect for future quantum technologies.
A periodic resonant emitter array coupled to a one-dimensional waveguide can act as a mirror. A typical example is a Bragg mirror, where emitters are spaced by multiples of half wavelengths and collectively enhance light reflection. Two such mirrors form an effective cavity that hosts bound states in the continuum (BICs). However, generating and detecting the spatial profiles of such BICs has proven challenging. Here, we experimentally demonstrate BICs in cavity magnonics using two periodic ferrimagnetic-sphere arrays and a probe sphere in a dual-open-waveguide architecture. We realize both Bragg and anti-Bragg cavities, whose mirrors have different lattice constants. In the Bragg cavity, there are degenerate supermodes formed by mirror spheres. We show that a single dark supermode coherently couples to the probe magnon in the cavity region, forming two polaritons whose splitting scales with both the probe-sphere size and the number of mirror spheres. By contrast, the anti-Bragg cavity has bright and dark supermodes in a bandgap, substantially changing the magnon-cavity interaction. Moreover, by moving the probe sphere, we perform position-dependent detection of the cavity field, highlighting the role of BICs in these cavities. Our flexible experimental setup with a scanning probe opens possibilities to detect other exotic states created by light-matter interaction, to interface with superconducting circuits in hybrid quantum networks, and to study non-Hermitian physics with Bragg and anti-Bragg cavities.