
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.
Quantum sensing uses quantum systems, such as photons, atoms, or spins, to measure physical quantities by analyzing how these systems interact with their environment or how their signals are detected. Unlike classical sensing approaches, it often operates in regimes where signals are extremely weak, requiring the detection and analysis of individual quantum events.
Different physical platforms can be used for quantum sensing, including atomic systems, solid-state defects such as nitrogen-vacancy (NV) centers, and photonic systems. In photonic quantum sensing, information is encoded in properties of light such as arrival time, phase, or photon statistics, and is extracted through precise time-resolved and correlation-based detection.
Quantum sensing encompasses a broad range of techniques and applications. While quantum metrology focuses on achieving ultimate measurement precision and quantum imaging extends these concepts to spatially resolved measurements, quantum sensing serves as the overarching framework for extracting physical information from quantum signals in practical scenarios.
Quantum sensing encompasses a range of applications where physical information is extracted from quantum systems and quantum light. Depending on how the signal interacts with the environment and how it is detected, different sensing modalities can be realized.
Fluorescence-based quantum sensing directly uses emitted photons as the sensing signal. Here, the information is encoded in the properties of the emitted light itself, such as its intensity, timing, or statistical distribution, which reflect interactions at the molecular or material level.
By analyzing photon arrival times and emission statistics, processes such as energy transfer, molecular interactions, and environmental changes can be studied. This approach is widely used in spectroscopy, material science, and life sciences, particularly in regimes where signals are weak and require single-photon sensitivity.
Spin-based quantum sensing uses well-defined quantum states—such as electronic or atomic spins—as the actual sensing element. External perturbations, including magnetic or electric fields, temperature, or pressure, directly modify the spin state. This information is then transferred to the optical domain via spin–photon coupling, enabling optical initialization and readout.
The detected photons do not carry the primary sensing information themselves but act as a readout channel of the underlying spin dynamics, typically accessed through time-resolved detection and synchronized control sequences.
Nitrogen-Vacancy (NV) Centers
NV centers in diamond are widely used for nanoscale sensing. Their spin state can be optically initialized and read out, while microwave excitation enables optically detected magnetic resonance (ODMR). External fields shift the spin resonance, and these changes are mapped onto variations in the emitted fluorescence, allowing highly sensitive and spatially resolved measurements.
Atomic Quantum Sensors
Atomic systems, such as vapor cells or cold atom ensembles, exploit coherent spin dynamics of atomic states to sense external fields and forces. Optical probing converts changes in the atomic spin state into measurable signals, often requiring precise timing and synchronization with control sequences.
Quantum LiDAR uses single photons or correlated photon pairs to measure distances and object properties with high sensitivity. By precisely measuring photon arrival times, distance information can be extracted even under extremely low-light conditions.
Correlation-based detection schemes further enhance performance by suppressing background noise. By analyzing coincidences between emitted and detected photons, uncorrelated ambient light can be rejected, enabling robust operation in challenging environments such as long-range sensing or high-background scenarios.
Quantum imaging extends quantum sensing to spatially resolved measurements, where both the position and timing of detected photons carry information. By exploiting correlations and quantum properties of light, imaging can be performed under low-light conditions or in regimes inaccessible to classical techniques.
Quantum Ghost Imaging (QGI)
Coincidence detection between a “bucket” detector, which collects light interacting with the object, and a spatially resolving reference detector enables image reconstruction. This correlation-based approach uses spatial correlations between photon pairs to reconstruct images, even though the imaging detector never directly observes the object.
Quantum Imaging with Undetected Photons (QIUP)
In QIUP, imaging is achieved using photons that are never directly detected. Within a nonlinear interferometer, photons interacting with the object transfer their spatial information to another beam via interference. This enables imaging in spectral ranges where detectors are inefficient or unavailable, such as mid-infrared, while detection is performed in a convenient, often visible wavelength range.
The distinction between different quantum sensing modalities is not always strict, as many approaches combine multiple physical principles and measurement techniques. For example, fluorescence sensing and spectroscopy both analyze emitted photons, while spin-based sensing often relies on spectroscopic methods such as ODMR. Similarly, correlation-based techniques and interferometric methods are frequently used across different sensing applications.
Quantum sensing enables the detection and analysis of signals in regimes where classical approaches reach their limits. By leveraging single-photon detection and quantum systems, it provides access to information that is often hidden by noise or extremely low signal levels.
A key advantage is the ability to operate in the few-photon regime, where time-resolved detection and correlation analysis allow reliable signal extraction even under challenging conditions such as high background or low light.
In addition, quantum sensing provides access to multiple dimensions of information, including temporal dynamics, photon statistics, and phase. This enables more efficient use of each detected photon, improving sensitivity and measurement fidelity across a wide range of applications.
PicoQuant Time Tagging and TCSPC electronics for quantum sensing.PicoQuant provides high-precision timing and photon-counting instrumentation for quantum sensing applications. Accurate time tagging enables the extraction of information from photon arrival times, correlations, and signal statistics, forming the basis for time-resolved, correlation-based, and interferometric sensing. Low timing jitter and flexible synchronization support reliable measurements even at low signal levels and in complex experimental environments.
Key advantages include:
These time-tagging and TCSPC electronics address diverse experimental requirements in quantum sensing and quantum metrology.

PicoHarp 330 is ideally suited for flexible quantum sensing and photon-counting experiments requiring high timing accuracy and versatile triggering. It delivers picosecond resolution, ultra-short dead time of 680 ps, and configurable multi-channel operation, enabling precise photon-correlation and time-resolved measurements across a wide range of quantum optics and material science applications.

PMA Hybrid Series detectors are ideally suited for high-sensitivity quantum sensing and time-resolved photon-counting experiments. They combine single-photon sensitivity with excellent timing performance, low noise, and negligible afterpulsing, enabling accurate correlation measurements and reliable detection of weak optical signals across the UV–NIR spectral range.

PicoQuant’s picosecond pulsed diode lasers support quantum sensing experiments across a wide range of applications, from spectroscopy and fluorescence sensing to interferometric and time-of-flight measurements. Short pulse widths and stable repetition rates enable precise temporal control and synchronization, forming the basis for time-resolved detection, correlation analysis, and phase-sensitive measurements in photon-counting experiments.
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