Data from: Room-temperature spinor condensate in halide perovskite microcavity
Data files
Apr 28, 2026 version files 4.44 MB
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CsPbBr3_spinor_dataset_KY_8th_SA.xlsx
4.44 MB
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README.md
4.52 KB
Abstract
We have submitted our experimental and analysis dataset (CsPbBr3_spinor_dataset_KY_8th_SA.xlsx), which contains all numerical data used to generate the figures in the associated manuscript. Each sheet in the Excel file corresponds to a specific figure or supplementary figure.
No additional compressed archives are included. Some large datasets (Figs. S7–S9) are not included due to file size limitations and can be made available upon reasonable request.
Description
File: CsPbBr3_spinor_dataset_KY_8th_SA.xlsx
This Excel file contains multiple sheets corresponding to experimental measurements and theoretical analysis of spinor polariton condensation in CsPbBr₃ microcavities.
Each sheet is labeled according to the figure number in the manuscript.
General Data Structure
- Colormap data
- First column: in-plane wavevector (µm⁻¹) or pumping fluence
- First row: energy (eV) or fluence (J/cm²)
- Matrix values:
- Photoluminescence (PL) intensity (a.u.)
- Stokes parameters (dimensionless)
- Plot data
- Columns correspond to physical quantities such as:
- PL intensity (a.u.)
- Full width at half maximum (FWHM, eV)
- Energy (eV)
- Wavelength (nm)
- Stokes parameters
- Columns correspond to physical quantities such as:
Figures 1a–1d
Colormap data of unpolarized PL dispersion under different pumping fluences.
- First column: in-plane wavevector (µm⁻¹)
- First row: energy (eV)
- Values: PL intensity (a.u.)
Figures 1e–1g
Fluence-dependent measurements:
- PL intensity (a.u.)
- FWHM (eV)
- Peak energy (eV)
Two simultaneously observed spinor-condensed modes are included.
One of them was observable at the fluence above 9.21 µJ/cm², thus the data sets below 9.21 µJ/cm are missing ("null").
Figures 2a–2f
Colormap data of Stokes parameters:
- S1, S2, S3 (dimensionless)
- Below- and above-threshold regimes
Figures 3b–3e, 3g–3j
Fluence-dependent Stokes parameters for two samples with different detuning energies.
- First column: pumping fluence
- First row: energy (eV)
Figure 4a
Comparison of theoretical and experimental Stokes parameters:
- Theoretical:
- S, Sx/S, Sy/S, Sz/S
- Experimental:
- S0, S1, S2, S3
Figure 4b
Blueshift of the condensed polariton mode:
- P: polariton density (µm⁻²)
- exp: experimentally measured peak energy (eV)
Supplementary Data
Figs. S1a–S1b
Absorption spectra of CsPbBr₃ crystals prepared by different fabrication methods.
Fig. S2
Transmittance spectra of distributed Bragg reflectors (DBRs).
Fig. S4
Angle-resolved photoluminescence (ARPL) below threshold.
Figs. S5a–S5l
Polarization-resolved PL:
- Linear polarization: H, V, D, A
- Circular polarization: R, L
Measured at:
- Below threshold (~0.85 P_th)
- Above threshold (~1.35 P_th)
Figs. S6b–S6c
Interferometric measurements:
- Fringe visibility (spatial profile)
- Delay-time dependence
Figs. S7–S9
Full colormap datasets of S1–S3 (not included; available upon request)
Fig. S10
Degree of polarization calculated from Stokes parameters. The data include error bars in y axis.
Fig. S11
Simulation results of spinor condensation dynamics.
Parameters:
- ℏγ_d = 6 meV
- ℏγ_c = 23 meV
- ℏγ_R = 50 meV
Variable ranges:
- δg = 0.062–0.62 µeV·µm²
- Ω = 10–100 meV
Key Information Sources
All data were obtained from:
- Angle-resolved photoluminescence (ARPL) measurements
- Polarization-resolved spectroscopy
- Interferometric coherence measurements
- Numerical simulations based on a spin-dependent Gross–Pitaevskii model
Code/Software
Data analysis and simulations were performed using standard scientific computing tools.
- Python (NumPy, SciPy, Matplotlib)
- MATLAB (modeling and fitting)
- Origin / Igor Pro (data visualization)
Workflow
- Data acquisition (ARPL, polarization-resolved PL)
- Extraction of dispersion relations and peak parameters
- Calculation of Stokes parameters
- Numerical simulation using spinor Gross–Pitaevskii equations
- Figure generation
Notes
- No special missing-value codes are used
- All datasets are directly usable without preprocessing
- Large datasets not included can be requested from the authors
