Ziyu Ye’s research while affiliated with East China Normal University and other places

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Publications (7)


Polaritonic temporal logic gates
Two femtosecond laser pulses, denoted input A and input B, are incident at the same point on a ZnO microcavity to manipulate the underlying dynamics of the macroscopic quantum states. The leaking photons can be detected as the ‘output’ signal in the transmission direction. The full set of logical gate functions are realized in the localized EP ensemble. The polariton NOT gate is realized on the basis of tailored bosonic cascading relaxation of several polariton modes in a ZnO microcavity. The arrival of the control pulse can shut off an existing polariton Bose–Einstein condensate (BEC) by driving the polariton population to the neighbouring polariton branch. The AND and OR logical gates are created through stimulated amplification, which is driven by two pumping laser pulses. The behaviour of the time-resolved photoluminescence emission (illustrated by the coloured profile) meets the criteria of the full set of logical gates shown in the tables, depending on the specific injection levels and time delays between the two pumping pulses.
Polariton temporal NOT gate based on manipulating the bosonic cascading relaxation in exciton polaritons
The NOT gate is obtained by using two-pulse non-resonant injection, with the pump and control pulses fixed at ~1.2Fth and 0.1Fth, respectively. a, Photoluminescence emission spectra of EPs as a function of the time delay between the pump and the probe pulses. The insets show time-integrated dispersion of the photoluminescence distributions at time delays of 200 fs and 0 fs, which correspond to the ‘on’ and ‘off’ states for the output signal, respectively. E is the energy and k is the in-plane momentum. b, Integrated signal intensity for the U and the L polariton modes as a function of the time delay. The scattered data are obtained from experiments. The solid curves are calculation results obtained on the basis of rate equations involving the cascading process between the polariton modes³⁴. Data are presented as mean values with 95% CI (n = 3). The blue curve represents a NOT gate function close to zero time delay. A ~80 fs FWHM of the response time is obtained. c,d, Time-resolved spectra of the photoluminescence emission as a function of time for the ‘on’ (c) and ‘off’ (d) output states. The time delays are at 200 fs and 0 fs, respectively.
Localized exciton polaritons excited by multiple non-resonant injections
a–c, The integrated angle-resolved spectra for single-pulse injection below (a) and above (b) the condensation threshold, and for two successive pulse injections (c) at a delay of 5 ps. The fluence of each pulse is kept at about 0.6Fth. d, Spectra for two pulse injections as a function of the time delay. Condensation can be achieved within a delay of about 120 ps. e, Time-resolved photoluminescence intensity obtained for the indicated relative delays. The light blue dashed line represents the arrival of the first excitation pulse at zero time delay. The dashed lines of other colours indicate the arrival time of the second excitation laser pulses. f, The linewidth and buildup time of the resulting condensation signals for bi-injection at various delays. Error bars are estimated from the experimental instability (n = 3). g, Simulation results based on solving the open-dissipative GP equation. The light blue dashed line indicates the injection of the first laser pulse at zero time delay. The dark blue curve shows the dynamics of exciton density where the sudden enhancement at about 20 ps is induced by the second pulse injection (marked by the purple dashed line). The red curve represents the time-resolved EP population produced by stimulated amplification. ∣ψ∣² is the density of the lower polariton mode, which is presented by a magnification of 70 times for better comparison. nR represents the calculated density of the exciton reservior. h, Threshold behaviours as a function of the second injection fluence with delays of 10, 40 and 70 ps, respectively. The dark yellow curve represents a single-pulse injection scenario.
The dynamical amplification of the two-pulse non-resonant injection
The first injection pulse is fixed at ~1.5Fth above the condensation threshold. a, Time-resolved photoluminescence intensity obtained at various strengths for the second laser pulse. The dashed lines indicate the arrival times of the two injection laser pulses. b, The calculated dynamics of the exciton reservior (nR) and the polaritons (∣ψ∣²) for the experimental conditions in a. c, Fluence-dependent buildup time and bandwidth. Data are presented as mean values ± s.e.m. (n = 3). d,e, Energy shift (d) and signal gain (e) (defined as the ratio of the integrated signal in the grey region in a to that without a second pulse injection). Data are presented as mean values ± s.e.m. (n = 3).
All-optical temporal logic gates in localized exciton polaritons
  • Article
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August 2024

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298 Reads

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6 Citations

Nature Photonics

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Haoyuan Jia

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Exciton polaritons—quasi-particle excitations consisting of strongly coupled photons and excitons—present fascinating possibilities for photonic circuits, owing to their strong nonlinearity, ultrafast reaction times and their ability to form macroscopic quantum states at room temperature via non-equilibrium condensation. Past implementations of transistors and logic gates with exciton polaritons have been mostly realized using the spatial propagation of polariton fluids, which place high demands on the fabrication of the microcavities and typically require complex manipulations. In this work we have implemented the full set of logical gate functionalities (that is, temporal AND, OR and NOT gates) in localized exciton polaritons at room temperature, on the basis of precisely controlling the interplay between polariton condensate and exciton reservoir dynamics, using a two-pulse excitation scheme. The dynamics intrinsically covers the cascadability required by the logical operations, enabling efficient information processing without the need for spatial flow. The temporal polariton logic gates demonstrate advantages in ultrafast switching, universality and simplified compatibility with other dimensional controls, showing great potential for building polariton logic networks in strongly coupled light–matter systems.

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The steady-state angle-resolved PL spectra of non-zero momenta EP fluids, at the pump powers of (a) 0.52 μW, (b) 0.70 μW, (c) 0.82 μW, (d) 0.96 μW, (e) 1.20 μW and (f) 1.40 μW. The red dashed curves represent the fitted dispersion curves for the LP branches, corresponding to modes with N = 49, 48, 47, and 46. The four energy modes are named M1-M4 accordingly. Figure (f) is plotted in log scale to increase the visibility of signals at M4. Other figures are plotted in linear scale. (g) Schematic illustration of the generation mechanism of the non-zero momenta EP fluids in real space. The presence of a narrow potential barrier from the exciton reservoir leads to the generation of EP fluids across a wide range of angles.
(a)–(f) PL emission as a function of time and energy at different pump powers (as being indicated by the red values), (a) 0.52 μW, (b) 0.70 μW, (c) 0.82 μW, (d) 0.96 μW, (e) 1.20 μW, and (f) 1.40 μW. The red and white dashed lines guide the eyes to observe the time-dependent energy red shift, and the triangles indicate the inflection point for M1 and M2.
(a)–(d) The PL distributions as functions of time and energy for fluids M1, M2, M3 and M4, at P = 1.40 μW. The red dashed circle marks the high energy regions for M1. (e)–(h) The PL distributions as functions of time and emission angle for M1, M2, M3 and M4. The white dashed lines aid in distinguishing the angular decay channels, marked as C1–C5. (i)–(l) The angle-integrated signals of the C1–C5 channels obtained for energy channels M1, M2, M3 and M4, respectively.
Theoretical calculations of the PL distribution as a function of time and emission angle under (a) stronger and (b) weaker laser induced potentials. The values of the parameters used are as follows: m = 1.35 × 10⁻⁴ me, g = 0.05 ps⁻¹ μm², R = 2.40 ps⁻¹ μm², g R = 0.01 ps⁻¹ μm², γR = 0.01 ps⁻¹. P(r,t) is taken as a Gaussian in space with FWHM = 1 μm. And in (a), G = 0.18 μm², γc = 1.0 ps⁻¹; in (b), G = 0.11 μm², γc = 0.6 ps⁻¹.
Ultrafast dynamics of exciton-polariton fluids at non-zero momenta

In this study, we have explored the ultrafast formation and decay dynamics of exciton-polariton fluids at non-zero momenta, non-resonantly excited by a small-spot femtosecond pump pulse in a ZnO microcavity. Using the femtosecond angle-resolved spectroscopic imaging technique, multidimensional dynamics in both the energy and momentum degrees of freedom have been obtained. Two distinct regions with different decay rate in the energy dimension and various decay-channels in the momentum dimension can be well-resolved. Theoretical simulations based on the generalized Gross–Pitaevskii equation can reach a qualitative agreement with the experimental observations, demonstrating the significance of the initial potential barrier induced by the pump pulse during the decay process. The finding of our study can provide additional insights into the fundamental understanding of exciton-polariton condensates, enabling further advancements for controlling the fluids and practical applications.


Ultrafast intermode parametric scattering dynamics in room-temperature polariton condensates

February 2023

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105 Reads

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4 Citations

Parametric scattering dynamics are general and of crucial importance for cavity exciton polaritons. Here, parametric scattering process driven by exciton polariton condensates has been revealed in a 1D ZnO microcavity between the whispering-gallery mode and quasiwhispering-gallery mode. When the occupation of the produced polariton condensate is dense enough, polariton condensates formed on quasiwhispering-gallery mode can be scattered towards the ground state of the adjacent whispering-gallery modes at higher and lower energies. By using the femtosecond angle-resolved spectroscopic imaging technique, the ultrafast dynamics of this intermode polariton parametric scattering have been explicitly observed. The scattering towards a higher mode occurs faster than that to a lower-energy mode by less than a picosecond. The revealed dynamics can not only expand the present investigations on polariton parametric scattering, but also promote the potential applications in, e.g., quantum information processing.


FIG. 1. (a) The experimental scheme. (b) Schematic energymomentum dispersion for the ZnO microwire. Two photons from the 700 nm control pulse induce stimulated scattering from the polariton condensate formed at around k == ¼ 0 on the LP branch. The idler photon is at a long wavelength of 3.4 μm. (c) The integrated angle-resolved PL spectrum obtained at 350 nm at the pump fluence of about 7.0 × 10 −4 J=cm 2 . The pump fluence dependence of (d) the ground-state occupation, the emission linewidth, and (e) the energy at the maximum of the PL emission spectra. (f) The integrated angle-resolved PL spectrum obtained for excitation at 700 nm at the fluence of 3.4 × 10 −3 J=cm 2 .
FIG. 2. Control pulse delay dependence of polariton condensate population for fixed control power. The pump power is ∼6P th . The fluence of the control pulse is about 2.9 × 10 −3 J=cm 2 . (a) The time-resolved, momentum-integrated PL spectra. The integrated signal from all the LP branches to the time axis with (b) no control pulse, control pulse with delay at (c) 1.7, (d) 2.3, (e) 3.0, and (f) 4.5 ps. The duration and the arrival time of the control pulses are indicated by the gray areas.
FIG. 3. Control pulse power dependence of polariton condensate population for fixed control pulse delay at 2.4 ps. Color images shown are the time-resolved, momentum-integrated PL spectra. The pump power is ∼6P th for all cases with (a) no control pulse, control pulse fluence at (b) 2.3 × 10 −3 J=cm 2 , (c) 3.4 × 10 −3 J=cm 2 , (d) 5.7 × 10 −3 J=cm 2 . The blue curves represent the integrated signal from all the LP branches. The blue arrows indicate the times where the polariton is switched off. The black arrow in (c) indicates the 6 orders of magnitude (OOM) difference between the "on" and the "off" states.
FIG. 4. Numerical simulation of the optical switch using an open-dissipative Gross-Pitaevskii equation. (a) Comparison of the simulated and the experimentally measured polariton signal obtained from the data shown in Fig. 3(b). (b) The calculated dynamics for polariton condensation and the parametric scattering process for the various participating modes as labeled. (c) Effect on polariton revival as a function of control pulse intensity.
Optically Controlled Femtosecond Polariton Switch at Room Temperature

July 2022

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398 Reads

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41 Citations

Physical Review Letters

Exciton polaritons have shown great potential for applications such as low-threshold lasing, quantum simulation, and dissipation-free circuits. In this paper, we realize a room temperature ultrafast polaritonic switch where the Bose-Einstein condensate population can be depleted at the hundred femtosecond timescale with high extinction ratios. This is achieved by applying an ultrashort optical control pulse, inducing parametric scattering within the photon part of the polariton condensate via a four-wave mixing process. Using a femtosecond angle-resolved spectroscopic imaging technique, the erasure and revival of the polariton condensates can be visualized. The condensate depletion and revival are well modeled by an open-dissipative Gross-Pitaevskii equation including parametric scattering process. This pushes the speed frontier of all-optical controlled polaritonic switches at room temperature towards the THz regime.


Buildup dynamics of room-temperature polariton condensation

July 2022

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63 Reads

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4 Citations

By using the femtosecond angle-resolved spectroscopic imaging technique, the ultrafast buildup dynamics of room-temperature polariton condensation is explicitly visualized in a ZnO whispering gallery mode microcavity. The buildup time of polariton condensation with respect to the arrival of the femtosecond pump pulse decreases with the increasing pump power and reaches a lower limit of about 4 ps. Simulation results by numerically solving the open-dissipative Gross-Pitaevskii equation coupled to an incoherent reservoir are in quantitative agreement with the experimental observations, showing that the scattering from exciton reservoir to the lower polariton branches and the decay from these branches dominate the buildup process.


The ground-state occupancy vs pump power for polarization directions along 0, 30, 60 and 90 degree, respectively. Corresponding condensation threshold powers are found to be around 0.52 μW, 0.56 μW, 0.61 μW and 0.66 μW. Inserted figure: sketch of the ZnO WG microcavity and the coordinates. The pump pulses are along the x axis. 0/90 degree polarization is along the y/z-axis. The crystallographic axis (c-axis) is along the z-axis.
(a)–(c) Static-state k-space angle-resolved PL mappings for polariton condensates under excitation pulses along three different polarization directions. The dispersion curves (indicated by the white dashed curves) are obtained from fitting with the classical plane waves model. (d) The excitation polarization dependence of the condensation signal at a fixed pump power of 0.8 μW. The solid line is from a linear fitting.
(a)–(d) The PL emission of the polariton condensation as a function of energy and time. (e) The signal are projected onto the energy axis for various polarization directions. The solid curves are fit with Gaussian function. (f) The dynamics of polariton condensation for various polarization directions. The solid curves are the calculation results based on rate equations. For a better quality of the figure, only 10% of the measured data points are shown here.
The polarization dependence of polariton condensates dynamics at pump powers of (a) P = 0.80 μW (b) P = 0.95 μW (c) P = 1.10 μW. As P increasing, the time interval shrinks. For a better quality of the figure, only 10% of the measured data points are shown here.
Excitation-polarization-dependent dynamics of polariton condensates at room temperature

March 2022

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119 Reads

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5 Citations

Based on ZnO microcavities with high quality factors, where the gain medium exhibits confinement of wave packets due to the intrinsically formed whispering gallery microcavity, strong coupling between excitons and cavity photons can be obtained at room temperature resulting in hybrid quasiparticles, e.g. exciton polaritons. In this work, polariton condensation is induced under the non-resonant excitation by linearly polarized femtosecond pulses with different polarization directions. The dynamical angle-resolved k-space spectra of the photoluminescence emission of polariton condensates are measured with sub-picosecond resolution by the self-developed femtosecond angle-resolved spectroscopic imaging technique. Our results show that the ultrafast dynamics of polariton condensation is sensitive to the polarization direction of the excitation pulses which can be explained qualitatively by the combined effect of selective excitation of distinct exciton modes in the sample and the effective coupling strength of the excitation pulses in the ZnO microcavity for various polarization directions. This work strengthened the understanding of the underlying physics of the condensation process for cavity exciton polaritons at room temperature.room temperature.


Ultrafast Dynamics of Exciton-Polariton in Optically Tailored Potential Landscapes at Room Temperature

October 2021

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318 Reads

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9 Citations

In this work, by using femtosecond angle-resolved spectroscopic imaging technique, the ultrafast dynamics of confined exciton-polaritons in an optical induced potential well based on a ZnO whispering-gallery microcavity is explicitly visualized. The sub-picosecond transition between succeeding quantum harmonic oscillator states can be experimentally distinguished. The landscape of the potential well can be modified by the pump power, the spatial distance and the time delay of the two input laser pulses. Clarifying the underlying mechanism of the polariton harmonic oscillator is interesting for the applications of polariton-based optoelectronic devices and quantum information processing.

Citations (6)


... This research uncovers new physical phenomena, such as quantum entanglement and chiral quantum light fields [11], while also offering practical implications for the advancement of cuttingedge optoelectronic devices and quantum information technologies. Chiral exciton-polaritons, for instance, hold potential for realizing all-optical switches [12]- [14], optical logic gates [15], novel quantum light sources [16], [17], and optical isolators [18], furthering advancements in quantum computing and communication. ...

Reference:

A general model for designing the chirality of exciton-polaritons
All-optical temporal logic gates in localized exciton polaritons

Nature Photonics

... Indeed, nonlinearities of polaritons governed by polaritonic interactions have become one of the most studied topics in the field of polariton physics. A variety of nonlinear phenomena, such as inter-and intra-band parametric scattering, 2,[8][9][10][11] polariton blockade, [12][13][14] topological edge mode, [15][16][17] and evaporative cooling 18) have been reported in recent years. Understanding and controlling the nonlinearities of polaritons is critical for both fundamental polariton physics and their potential optoelectronic applications. ...

Ultrafast intermode parametric scattering dynamics in room-temperature polariton condensates
  • Citing Article
  • February 2023

... This is because EPs are formed through the strong coupling between photons and excitons, thereby possessing properties from both photon and matter 17 . The photon component endows EPs with an exceptionally small effective mass, allowing them to exhibit Bose-Einstein condensates (BEC)-like behaviors [18][19][20][21] , and form condensation without the need for the cryogenic conditions required in cold atomic systems [22][23][24][25][26][27][28] . The resulting superfluid effects create an effective platform for simulating quantum coherent systems [29][30][31] . ...

Optically Controlled Femtosecond Polariton Switch at Room Temperature

Physical Review Letters

... We show that the ultrafast switching dynamics can be well manipulated by the controlling pulse, supporting THz operational speed and high extinction ratio at room temperature. The dynamics of the subpicosecond switching of polariton condensates are characterized by a femtosecond angle-resolved spectroscopic imaging technique [31][32][33]. We explain the phenomenon by parametric scattering of the photonic part of the polariton condensate through a four-wave mixing process [34,35]. ...

Excitation-polarization-dependent dynamics of polariton condensates at room temperature

... Schematic illustrations of (a) exciton-polariton fringes from the interference between the surface reflection and the scattering from the MoSe 2 waveguide based on[53]. (b) Exciton-plasmon-polaritons (plexcitons) at a TMDC and Au interface based on[58]. Rabi oscillations and Rabi splitting resulting from the strong coupling between plasmons and excitons can be observed. ...

Ultrafast Dynamics of Exciton-Polariton in Optically Tailored Potential Landscapes at Room Temperature