
Complete confocal fluorescence microscope that empowers researchers to advance quantitative functional imaging from individual molecules to cells and tissues.

Modular, customizable, time-resolved confocal microscope with single-molecule sensitivity for life and materials science.

Compact FLIM and FCS upgrade kit that adds advanced functional imaging and correlation analysis to existing laser scanning microscopes.

Designed for flexible, sensitive, and precise steady-state and time-resolved spectroscopy across the UV to NIR range and time scales from picoseconds to milliseconds.

Modular lifetime spectrometer designed for flexible fluorescence and photoluminescence measurements in both materials and life science research.

Add spectral and time-resolved photoluminescence to your setup through flexible microscope–spectrometer coupling options.

Get the most out of superconducting nanowire detectors in large-scale quantum communication and computing experiments requiring precise multichannel timing.

Boost your time-resolved experiments with a flexible, high-precision time tagging and TCSPC unit for materials science and quantum sensing.

Scale your photonic quantum computing and detector characterization setups while maintaining performance, flexibility, and high data throughput.

Compact 3-color picosecond laser delivering flexible ns to ms excitation with cost-effective multicolor performance and straightforward operation.

Smart picosecond laser diode heads covering UV-A to NIR, providing the right combination of power, pulse width, and diode type for any time-resolved technique.

VisUV provides clean short pulses and stable timing across key UV and visible wavelengths, including deep UV lines as well as 488 nm and 532 nm.

Enhance your single-photon counting experiments with wide dynamic range and excellent timing precision in the UV and visible even at the highest count rates.

Capture even the weakest signals over large areas with maximum dynamic range and enhanced low-light sensitivity in a compact detector design.

Unlock spatially resolved single-photon detection with a 23-pixel SPAD array, combining low dark counts and precise time tagging for advanced experiments.

Advanced FLIM analysis software for fast, accurate interpretation of lifetime imaging data.

Intuitive, free software solution for real-time, high-precision photon data acquisition, visualization, and initial data analysis.

Advanced software for time-resolved fluorescence acquisition and analysis.

An imaging technique that uses fluorescence lifetimes to generate image contrast.

Investigating how proteins dynamically explore multiple conformational states that control biological function.

Investigating how biomolecules separate into dynamic liquid phases to organize cellular space and regulate biological function.

A time-resolved technique that measures photoluminescence lifetimes to reveal excited-state dynamics in materials.

Studying exciton dynamics, charge carrier processes, and structural properties through optical and time-resolved characterization methods.

Investigating charge-carrier lifetimes and recombination dynamics to enable precise optical characterization of material quality and device performance.

A quantum optical signature revealed by time-resolved photon correlation analysis to identify single-photon emission in materials and nanostructures.

The transmission of information using individual photons, using quantum effects to ensure absolute security.

Quantifying photons per detection event enables direct access to photon-number statistics, providing insight into quantum and statistical properties of light.

An optical technique that analyzes light emission under electrical excitation to reveal electronic properties of electroluminescent materials.

Monitoring environmental signals and trace compounds to understand dynamic changes in natural and engineered environments.

A photon timing technique that measures single-photon arrival times to resolve ultrafast dynamics in fluorescence, materials research, and quantum optics.
Coincidence correlation measurement is a time-resolved photon counting method used to identify correlated photon detection events across two or more detectors. It quantifies whether photons arrive simultaneously or within a defined temporal window, providing direct access to photon correlation statistics. The method is widely used in quantum optics to study the statistical properties of light and in materials science to characterize photon emission from solid-state systems.
In coincidence correlation experiments, photons emitted from a light source are detected by multiple single-photon detectors. The detection times are recorded with picosecond resolution, typically using time-correlated single photon counting (TCSPC). Coincidence events are identified by comparing timestamps and counting photon pairs that occur within a defined coincidence window. Repeating this process over many events yields statistically meaningful correlation data that describe the temporal photon correlation function.
Antibunching
Coincidence correlation between two detectors in a Hanbury-Brown and Twiss (HBT) configuration identifies single-photon emission by measuring the absence of simultaneous detections at zero delay. This suppression of “double-clicks” in g²(0) measurements confirms a sub-Poissonian light source, which is essential for ensuring that, e.g., only one qubit is processed at a time.
Hong–Ou–Mandel (HOM) Interferometry
Suppression of coincidence events between two separate input modes measures the spatial and temporal indistinguishability of photons. This quantum interference effect, visualized as the “HOM dip”, verifies the perfect wave-packet overlap required for high-fidelity gates in photonic quantum computing.
Coincidence counting between spatially separated detection channels characterizes correlated photon pairs generated via spontaneous parametric down-conversion and supports evaluation of source performance.
Coincidence measurements of entangled photon pairs verify the non-classical correlations and Bell-state projections necessary for high-fidelity quantum teleportation. By correlating detection events across remote nodes, these systems facilitate long-distance state transfer and enable secure quantum key distribution (QKD) by detecting eavesdroppers through the violation of Bell inequalities.
Linear Optical Quantum Computing (LOQC)
In photonic computers, photons do not naturally interact with one another. Coincidence correlation is used to “herald” (confirm) the success of quantum logic gates. For example, in a CNOT gate, the simultaneous detection of photons at specific output ports, monitored by coincidence units, indicates that a specific quantum operation has been successfully performed on the qubits.
Boson Sampling
In this non-universal scheme, multiple indistinguishable photons are injected into a massive, multi-port interferometer. The “computation” consists of the photons interfering with each other across all possible paths. Coincidence counting at the output modes samples the complex probability distribution of these photons. Because calculating this distribution is #P-hard for classical computers, measuring these multi-photon coincidences provides a direct route to demonstrating quantum advantage.
Measurement-Based Quantum Computing (MBQC)
Coincidence correlation is used to “herald” the successful creation of large, entangled cluster states from individual photon sources. By performing coincidence-based fusion measurements, which is the core mechanic of Fusion-Based Quantum Computing (FBQC), small resource states are stitched together into a massive, entangled lattice. These correlated detections confirm the entanglement links required to perform computation via sequential single-qubit measurements.
Quantum LiDAR
Correlation-based detection using entangled signal and idler photons increases robustness against background noise and active jamming. By performing coincidence counting between the returned signal and a local reference, the system filters out uncorrelated ambient light, significantly improving the signal-to-noise ratio and ranging precision in low-light environments.
Quantum Ghost Imaging (QGI)
Coincidence detection between a “bucket” detector (collecting scattered light) and a spatially resolving “reference” detector enables image reconstruction of objects that never interacted with the imaging sensor. This correlation-based technique utilizes the spatial entanglement of photon pairs to achieve high-resolution imaging with superior resilience to atmospheric turbulence.
Quantum Imaging with Undetected Photons (QIUP)
Coincidence correlation within a nonlinear interferometer allows the properties of an object to be imaged using a photon that was never actually detected. By interfering the “idler” photons that interacted with the object with a second set of “signal” photons, the spatial information is transferred to the detectable signal beam, enabling imaging in challenging spectral ranges (like Mid-IR) using standard visible-light cameras.
UniHarp software interface showing real-time second-order correlation g²(τ) analysis with a pronounced antibunching dip at zero delay.Coincidence correlation data are typically represented as coincidence time traces, histograms or correlation functions, such as second-order correlation g²(τ). These analyses reveal temporal correlations between photon detection events and enable the identification of antibunching, bunching, or uncorrelated events. Quantitative parameters include coincidence rates, coincidence-to-accidental ratios (CAR), and normalized correlation functions. Timing resolution, bin width, and integration time directly influence the statistical accuracy and interpretability of the results.
PicoQuant software supports flexible coincidence correlation analysis via UniHarp and snAPI as well as quantitative evaluation of g²(τ) data for antibunching studies via QuCoa.
Coincidence correlation reveals the statistical nature of light beyond simple intensity measurements by resolving detections in both the time and space domains. It is the fundamental tool for verifying single-photon purity and photon indistinguishability, providing the “heralding” signal required to confirm successful entanglement and logic operations.
In quantum optics, it enables the high-fidelity state transfer and secure protocols used in computing and networking. In materials and life sciences, it serves as a critical diagnostic for evaluating solid-state emitters and resolving single-molecule dynamics within complex environments. By isolating specific quantum events from background noise, coincidence correlation acts as the primary bridge between raw detection and actionable quantum information.
Instrumentation suited for coincidence correlation measurements, including PMA Hybrid Series, PDM Series and HydraHarp 500.Reliable coincidence correlation measurements require fast single-photon detectors with low timing jitter and minimal dead time, such as avalanche photodiodes (SPADs), hybrid photomultipliers (HPDs) or superconducting nanowires (SNSPDs). High-resolution timing electronics, typically time tagging & TCSPC modules, are essential to accurately record photon arrival times and identify coincidence events. Stable pulsed or continuous-wave excitation sources, synchronized detection channels, and high data throughput are critical to ensure accurate correlation statistics, especially in multi-detector or high-count-rate experiments.
Explore PicoQuant’s compatible components designed for coincidence correlation measurements.

Picosecond pulsed diode lasers provide controlled near-infrared excitation for time-resolved measurements. Stable repetition rates and short pulse durations enable precise characterization of photon propagation in scattering tissue.

Single-photon sensitive detectors record weak transmitted or fluorescent signals with high timing precision. Low timing jitter and high sensitivity are essential for accurate extraction of absorption and scattering properties.

Time-Correlated Single Photon Counting (TCSPC) and time tagging electronics measure photon arrival times with picosecond resolution across multiple channels. This enables precise reconstruction of temporal point spread functions for quantitative tissue imaging.

Antibunching is a quantum phenomenon in which photons emitted by a single quantum emitter are separated by a minimum time interval, preventing simultaneous detection. It is experimentally verified through coincidence correlation measurements of the second-order correlation function g²(τ), where a suppressed coincidence rate at zero delay indicates single-photon emission.
Poster on high-spatial photoluminescence studies of nanostructures and quantum emitters using time-resolved confocal microscopy and spectroscopy.
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