
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.
HydraHarp 500 combines best timing precision with configurable level triggers and constant fraction discriminators (CFD) in an upgradable multichannel architecture. A base resolution of 1 ps, timing jitter of 2.5 ps, and an ultrashort dead time below 680 ps ensure reliable event detection even at the highest count rates. The integrated White Rabbit interface enables ps precise remote synchronization of multiple devices, while the external FPGA interface allows real-time, custom data processing.
HydraHarp 500 is designed for the most advanced experiments in quantum optics and quantum photonics that demand both maximum timing accuracy and high data throughput, including multi-photon coincidence and correlation measurements such as g(2) antibunching, Hong–Ou–Mandel (HOM) interferometry, photon-number resolving (PNR) detection as well as quantum key distribution (QKD) and photonic quantum computing.
| HydraHarp 500 S | HydraHarp 500 M | |
| Number of detector channels (in addition to sync input) | 4 (Base model) | 5-8 (Base model + channel upgrades) | 4 (Base model) | 5-16 (Base model + channel upgrades) |
| Input voltage operating range (pulse peak into 50 Ohms) | - 1200 mV to 1200 mV | - 1200 mV to 1200 mV |
| Input voltage max. range (damage level) | -2500 mV to 2500 mV | -2500 mV to 2500 mV |
| Trigger method | Edge trigger: falling or rising edge (software adjustable) | CFD: falling edge | Level trigger |
| HydraHarp 500 S | HydraHarp 500 M | |
| Minimum time bin width | 1 ps | 1 ps |
| Timing precision* | 3.5 ps RMS typ. | 3.5 ps RMS typ. |
| Timing precision / √2* | 2.5 ps RMS typ. | 2.5 ps RMS typ. |
| Dead time | < 680 ps (edge trigger), < 6.8 ns (CFD) | < 680 ps (edge trigger), < 6.8 ns (CFD) |
| Differential non-linearity | < 5 % peak, < 1 % RMS (over full measurement range) | < 5 % peak, < 1 % RMS (over full measurement range) |
| Maximum sync rate (periodic pulse train) | 1200 MHz (edge trigger), 140 MHz (CFD) | 1200 MHz (edge trigger), 140 MHz (CFD) |
| HydraHarp 500 S | HydraHarp 500 M | |
| Count depth | 32 bit (4 294 967 296 counts) | 32 bit (4 294 967 296 counts) |
| Maximum number of time bins | 131072 | 131072 |
| HydraHarp 500 S | HydraHarp 500 M | |
| Peak count rate per input channel | 1.25 Gcps for burst durations up to 2048 events | 1.25 Gcps for burst durations up to 2048 events |
| Sustained count rate per input channel** | 80 Mcps | 80 Mcps |
| Total sustained count rate, sum over all input channels** | 85 Mcps | 85 Mcps |
| HydraHarp 500 S | HydraHarp 500 M | |
| Period | Programmable, 0.1 µs - 1.678 s (0.596 Hz - 10 MHz) | Programmable, 0.1 µs - 1.678 s (0.596 Hz - 10 MHz) |
| HydraHarp 500 S | HydraHarp 500 M | |
| Number | 4 | 4 |
| HydraHarp 500 S | HydraHarp 500 M | |
| Ref. IN | 10 MHz 200 … 1500 mV p.p. 50 Ohm; AC coupled | 10 MHz 200 … 1500 mV p.p. 50 Ohm; AC coupled |
| Ref. OUT | Default: 10 MHz White Rabbit mode: 31.25 MHz 250 mV p.p 50 Ohm; AC coupled | Default: 10 MHz White Rabbit mode: 31.25 MHz 250 mV p.p 50 Ohm; AC coupled |
| PPS IN | 1 s, LVTTL | 1 s, LVTTL |
| White Rabbit interface | Connector for SFP module | Connector for SFP module |
* In order to determine the timing precision it is necessary to repeatedly measure a time difference and to calculate the standard deviation (RMS error) of these measurements. This is done by splitting an electrical signal from a pulse generator and feeding the two signals each to a separate input channel. The differences of the measured pulse arrival times are calculated along with the corresponding standard deviation. This latter value is the RMS jitter which we use to specify the timing precision. However, calculating such a time difference requires two time measurements. Therefore, following from error propagation laws, the single channel RMS error is obtained by dividing the previously calculated standard deviation by √(2). We also specify this single channel RMS error here for comparison with other products.
** Sustained throughput depends on configuration and performance of host PC.
Provides detailed specifications of this high-resolution TCSPC and time-tagging module designed for fast, precise photon counting
HydraHarp 500 offers versatile software and control options to ensure seamless integration into any experimental workflow. From an intuitive graphical user interface to high-performance Python APIs and fully programmable libraries, the system adapts easily to both rapid measurements and advanced, custom-built applications.

HydraHarp 500 is fully compatible with UniHarp, PicoQuant’s modern and intuitive graphical user interface for TCSPC and time tagging. UniHarp provides seamless access to advanced measurement modes such as time trace, histogram, raw data, unfold, and correlation analysis including FCS and g², enabling efficient data acquisition and real-time experiment monitoring.

For users who require programmatic control, HydraHarp 500 supports snAPI, a high-performance Python interface built on a robust C++ core. snAPI enables fast device configuration, real-time data access, and direct handling of unfolded data or PTU files, allowing researchers to implement custom algorithms and automated analysis pipelines.

For maximum flexibility, the HydraHarp 500 offers a comprehensive programming library supporting C, C#, LabVIEW, Matlab, and Python. This enables full integration into custom experimental environments and synchronized measurement systems. Provided demo code and well-documented functions ensure a fast and straightforward start for advanced users.
HydraHarp 500 combines advanced time-tagging capabilities with flexible trigger configurations to support a wide range of time-resolved photon experiments.

PicoQuant‘s revolutionary TTTR mode records every detected photon as an individual time-tag event without early data reduction, preserving the full timing information of the experiment. This enables advanced analyses such as photon burst detection, detailed fluorescence dynamics, FCS, g2 correlation and high speed FLIM with unlimited image size. TTTR is also widely used in single molecule spectroscopy, time interval analysis and quantum optics. A dedicated blog article will provide a deeper introduction to TTTR, its modes and its application range.

In order to support the widest possible variety of single photon detectors, the PicoHarp 330 provides different input circuitry. For optimal timing with e.g. Single-Photon Avanlanche Diodes (SPADs) the inputs can be configured as level triggers while for best performance with Hybrid Photodetectors (HPD), Photomultiplier Tubes (PMTs), Micro Channel Plates (MCPs) or Superconducting Nanowire Single-Photon Detectors (SNSPDs) at high count rates they can be configured as Constant Fraction Discriminators (CFD). This way the overall system IRF may be tuned to become narrower. The same could not be achieved with a simple level trigger (comparator). Particularly with PMTs and MCPs, constant fraction discrimination is very important as their pulse amplitudes vary significantly.

Conti-Mode is PicoQuant’s hardware-based continuous histogramming workflow for high-speed, uninterrupted acquisition of time-resolved data. Instead of capturing a single histogram at a time, the instrument generates consecutive, gapless histogram blocks automatically, each combining precise timing metadata with full histogram content and channel sums. This makes Conti-Mode ideal for real-time monitoring, long measurement series, process control, and applications such as fluorescence lifetime flow cytometry where continuous streaming and instant evaluation of histogram data are essential.”
Poster on high-precision time tagging for scalable photonic quantum experiments using SNSPD arrays and multichannel TCSPC systems.
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