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Fluorescence Microscopes

MicroTime 200 STED

Time-resolved Confocal Fluorescence Microscope with Super-resolution Capability

  • Complete confocal STED system based on a inverted microscope body
  • Optical resolution below 50 nm
  • Excitation at 640 nm and optionally with additional lasers at 595 nm and 660 nm
  • Up to 6 truly parallel detection channels using SPADs or Hybrid-PMTs
  • Supports gated STED (gSTED) and gSTED-FCS
  • Piezo scanning for 2D- and 3D-(lifetime) imaging and accurate point positioning
  • Advanced easy-to-use data acquisition and analysis software SymPhoTime 64
  • Upgrade options for simultaneous AFM/FLIM/STED measurements
  • Supports all other methods available for the MicroTime 200, i.e., FLIM, FCS, FCCS, FLCS, FRET, etc.

Nomination Innovationspreis Berlin Brandenburg 2014PicoQuant was nominated for the innovation award “Innovationspreis Berlin Brandenburg” in 2014 for the development of the MicroTime 200 STED.


Confocal image of 20nm Crimson beads STED image of 20nm Crimson beads

In the recent years, super-resolution microscopy has gained more and more attention. It has now evolved beyond the stage of development and permits to investigate biological systems that were formerly obscured by the diffraction limit of light. One of the most popular techniques for super-resolution imaging is Stimulated Emission Depletion (STED) microscopy. STED is usually performed with confocal microscopes and is therefore ideally suited to be added to the MicroTime 200. The integration of STED into the system has been driven towards highest robustness and ease-of-use. The system permits to perform STED microscopy without lengthy alignment preparations while still having the choice to modify the system and use the full capability of the open microscopy platform MicroTime 200.

Less than 50 nm optical resolution

Mount for phase plateSTED microscopy uses the principle of stimulated emission based depletion. After exciting fluorophores in the laser focus, a second, donut-shaped focus of a laser with longer wavelength is used to actively de-excite the molecules in the periphery via stimulated emission. In the MicroTime 200 STED, the donut is created using a so-called EASYDOnut phase plate. It is inserted into the beam path and changes the STED laser focus to a donut-shape, while leaving the excitation laser unaffected. This simple implementation makes spatial alignment of the two laser beams, which emerge from the same optical fiber, unnecessary and yields a spatial resolution of less than 50 nm. Due to the time-resolved data acquisition principle of the MicroTime 200 STED, it is additionally possible to apply time-gates to all measured data. This gated STED (or gSTED) approach leads to an enhanced resolution in images and a reduced observation volume for FCS.

Choice of excitation wavelengths

Laser Combining Unit (LCU) of the MicroTime 200 STEDThe excitation system of the MicroTime 200 STED is build around a dedicated laser combining unit that integrates the excitation lasers for STED, and the STED laser itself. The standard excitation wavelength is 640 nm, which can optionally be combined with additional lasers at 595 nm and 660 nm for dual species STED imaging. Due to the high power of the invisible STED laser at 765 nm, special care was taken to ensure the user's safety when operating the instrument. A second laser combining unit with additional pulsed diode lasers can also be attached to the system for non-STED applications such as FLIM, FRET or FCS.

The laser power and repetition rate can be flexibly adjusted by the multichannel laser driver PDL 828 “Sepia II”, which even allows to address several lasers in parallel enabling advanced techniques like Pulsed Interleaved Excitation (PIE). The time delay between the excitation pulse and the STED pulse is adjustable for highest flexibility and best STED resolution.

The supercontinuum laser Solea can also be offered as an option (currently not available in the USA).

Detection subsystem with single photon sensitivity

Detection unit of the MicroTime 200 STEDIn the MicroTime 200 STED, scanning is facilitated through a piezo table optionally combined with a high precision PiFoc element for 3D imaging. The choice of piezo scanning ensures a high repositioning accuracy and stability, which is essential for high quality STED images. The system can be configured for up to six individual detection channels. For the deep-red emission of the STED dyes depleted at 765 nm, SPADs are typically used, since they feature a high detection efficiency of up to 70% in this spectral range.

Gated STED with picosecond resolution

HydraHarp 400 - Mutichannel TCSPC Module (small configuration)Data acquisition is performed using time-correlated single photon counting (TCSPC) using PicoQuant's unique time-tagged time-resolved (TTTR) data acquisition mode with picosecond resolution. The acquired TTTR data can not only be used for regular STED imaging, but also to perform gated STED (gSTED) measurements. The advantage of TTTR data acquisition mode is that it allows to perform vastly different measurement procedures besided STED, such as FLIM, FCS, or even coincidence correlation (“antibunching”), based on just one fundamental data format. The TTTR format ist supported by all available TCSPC electronics from PicoQuant.

Intuitive data acquisition and analysis

SymPhoTime 64 STEDSymPhoTime 64, the MicroTime 200 STED system software, features dedicated STED data acquisition and analysis protocols. For example, preset time-gating is integrated in the measurement preview, and flexible time gates for higher STED resolution can be set during data analysis. The unique fluorescence pattern matching approach can be used to separate multiple species from data recorded with the same STED laser wavelength.

FLIM, FRET, FCS, and more

The MicroTime 200 STED can not only be used to perform STED and STED-FCS, but also supports all other measurement and analysis procedures available for the MicroTime 200. This includes FLIM, FCS, FCCS, FLCS, FRET, PIE-FRET, or intensity time-traces, to name just a few.

Optical resolution
  • below 50 nm (STED)
  • below 300 nm (confocal)
Excitation system
  • Picosecond diode lasers (375 nm – 900 nm) with repetition rates up to 80 MHz inside a compact Laser Combining Unit
  • Single or multichannel laser driver
  • Optional: excitation down to 266 nm*
  • Optional: external laser (e.g., Titanium:Sapphire laser)
  • Optional: Supercontinuum laser Solea**


  • 640 nm (excitation), 765 nm (STED laser)
  • Dual species STED with 640 nm and 595 nm excitation
  • Dual species STED with 640 nm and 660 nm excitation
  • Inverted microscope IX 73 or IX 83 from Olympus
  • Specially designed right side port for confocal microscope
  • Left side port and back port still accessible (for e.g., widefield imaging or TIRF)
  • Transmission illumination unit included
  • Special manual sample positioning stage with 25 mm range
  • Standard sample holder for 20 mm x 20 mm cover slips
  • Optional: epifluorescence illumination
  • Optional: cryostat for low temperature measurements
  • Optional: combination with Atomic Force Microscope (AFM)
  • Air objectives with 20x and 40x magnification (standard)
  • Various high-end objectives available (oil/water immersion, air spaced, IR/UV-enhanced, TIRF, or long working distance objectives)
  • Computer controlled
  • 2-dimensional piezo objective scanning with 80 μm x 80 μm scan range at nominal 1 nm positioning accuracy
  • PIFOC for 3-dimensional imaging, 80 μm range at nominal 1 nm positioning accuracy
  • Optional: sample scanning
  • Optional: large area scanning table with cm scan range
Main optical unit
  •  Confocal detection set-up in a compact housing with up to four parallel detection channels
  • Specialized high-end major dichroics with enhanced stability
  • All optical elements easily accessible, adjustable, and exchangeable
  • CCD camera for beam diagnostics and photodiode for relative power measurements
  • Variable beam-splitting units and exit ports to connect external devices
  • Single Photon Avalanche Diodes
  • Hybrid-Photomultiplier Tubes
Data acquisition
  • Based on the method of Time-Correlated Single Photon Counting (TCSPC) in the unique Time-Tagged Time Resolved (TTTR) measurement mode
  • Simultaneous data acquisition of up to six channels
  • SymPhoTime 64

Not all options can be combined with each other.
* deep-UV not yet in combination with STED
** currently not available in the USA (coming soon)

All Information given here is reliable to our best knowledge. However, no responsibility is assumed for possible inaccuracies or omissions. Specifications and external appearances are subject to change without notice.

Combination with AFMs

MicroTime 200 - Combination with AFMThe combination of atomic force microscopy (AFM) with single-molecule-sensitive confocal fluorescence microscopy enables a fascinating investigation into the structure, dynamics and interactions of single molecules or their assemblies. AFM reveals the structure of macromolecular complexes with nanometer resolution, while fluorescence can facilitate the identification of their constituent parts. In addition, nanophotonic effects, such as fluorescence quenching or enhancement due to the AFM tip, can be used to increase the optical resolution beyond the diffraction limit. For the first time, this development grants access to the effects of precise physical impact on biomaterials like cells and its effects simultaneously measured by fluorescence parameters. The combination of the MicroTime 200 STED with an AFM has currently been realized for three different AFMs:

Solea supercontinuum laser

Solea - Supercontinuum LaserThe wavelength tunability and the variable repetition rates of the supercontinuum laser Solea, combined with the short pulse widths offers high flexibility for fluorescence lifetime measurements over a broad spectral and temporal range with only a single laser.*
The Solea can also be combined with up to four other pulsed diode lasers ranging from 375 to 900 nm using the Laser Combining Unit (LCU). In that way, Pulsed Interleaved Excitation (PIE) schemes using the Solea and another pulsed diode laser become possible, making the Solea the most flexible solution available for PIE using the MicroTime 200. Control of the necessary pulse patterns is possible using the laser driver PDL 828 "Sepia II", which is integrated in the system software SymPhoTime 64.

* currently not available in the USA (coming soon)

Spectrograph add-on

Adding a spectrograph (SR-163 from Andor) along with a single molecule sensitive CCD camera to the MicroTime 200 STED opens up new prospects in the investigations of single molecules. The spectrograph is attached via a multimode fibre to an exit port of the main optical unit of the MicroTime 200 STED. Inside the main optical unit, a suitable optical element is used to direct a defined part of the emitted light towards the exit port. An easy exchange of the optical element (100% mirror, 50/50 beamsplitter, ...) allows for the customization of the experimental conditions. Depending on the context of the experiment, a defined part of the fluorescence is utilized to acquire the spectral information. Intensity fluctuations, fluorescence decay properties and spectral data of a single molecule can be obtained simultaneously. Both, the observation of spectral changes as a function of time, and the comparison of spectra from different molecules are possible with this combination.

Tunable bandpass filter

Tunable pandpass for the MicroTime 200The tunable bandpass filters offer wavelength tunability over a wide range of wavelengths by manually adjusting the angle of incidence. Different filters cover the wavelength from 440 nm to 700 nm with a fixed spectral bandpass around 17 nm.

Simultaneous Measurement of Topological and Fluorescence Parameters

FLIM-STED and AFM height map collected from same sample areaIn this example, both fluorescence and topological information of dye-labeled beads were recorded simultaneously from the same sample area. Fluorescence parameters like emission intensity and lifetime shown in the top figure were obtained with STED super-resolution (<50 nm) on a MicroTime 200 STED. A JPK NanoWizard 3 atomic force microscope (AFM) was interfaced to the time-resolved fluorescence microscope, which allowed recording a height map from the same sample are (as shown in the lower picture).

The easy-to-use combination of fluorescence lifetime imaging (FLIM) with topological information from AFM offers exciting avenues for investigating the structure-fluorescence interactions in e.g., biomaterials.


  • Sample: 20 nm beads labeled with dye
  • Excitation: 640 nm
  • STED laser: 765 nm
  • PDL 828 “Sepia II” with SOM 828-D oscillator module
  • JPK NanoWizard 3 AFM

Multicolor Nanorulers for Super-resolution Microscopy

Confocal image of multicolor GATTAquant nanorulersSTED image of multicolor GATTAquant nanorulers

Nanorulers labeled with two different dyes are available to evaluate the resolution of diffraction-limit-breaking microscopes. This example shows GATTAquant STED 140RYR nanorulers, labeled with two red (ends) and a yellow dye (middle part). The distance between a red and yellow marker is 70 nm, while two red dyes on the same nanoruler are separated by a distance of 140 nm.


  • Excitation: 595 and 640 nm
  • Depletion: 765 nm
  • PDL 828 "Sepia II" with SOM 828-D oscillator module

The samples were kindly provided by GATTAquant GmbH


PIE-STED Fluorescence Correlation Spectroscopy

FCS with PIE-STED excitation

Fluorescence Correlation Spectroscopy (FCS) is a well established method for studying the diffusion behavior of molecules in solution or membranes. Under confocal conditions, the minimal size of the FCS observation volume is restricted by the diffraction limit. However, this limit can be circumvented by employing Stimulated Emission Depletion (STED) and the observation volume can be shrunk in a gradual manner by increasing the STED laser intensity.

At low STED laser powers, a small increase in intensity leads to a rapid shrinking of the lateral observation area diameter. Going from 0 to 50 mW reduces the spot diameter from 250 to less than 100 nm, depending on the fluorophore used. At high STED powers, however, increases in intensity will result in slower shrinking until a diameter below 50 nm can be reached.

Shrinking the detection volume helps in overcoming averaging issues in long transit paths and also enables determining the type of hindered diffusion behavior of fluorophores in lipid membranes. Furthermore, using a fully Pulsed Interleaved Excitation (PIE) illumination scheme for excitation and STED lasers allows collecting FCS data under both confocal and STED conditions quasi-simultaneously. PIE-STED-FCS allows for a straightforward check whether the STED laser has an influence on the investigated diffusion dynamics.


  • Excitation: 640 nm
  • Depletion: 765 nm
  • PDL 828 "Sepia II" with SOM 828-D oscillator module

Reference: Koenig, M. et al., Proceedings of SPIE, Vol.9712, 97120T (2016)

Cytoskeleton – microtubules

Confocal image of tubulin structures in a HeLa cell labeled with Abberior STAR635pSTED image of tubulin structures in a HeLa cell labeled with Abberior STAR635p

The example shows tubulin structures in a HeLa cell labeled with Abberior STAR635p. Super-resolution permits the clearer distinction of the filamentous structures in the STED image.


  • Excitation: 640 nm
  • Depletion: 765 nm

FLIM-STED pattern matching for dual species separation

Confocal image - U2OS cell labeled for tubulin with Abberior STAR 635p (green) and giantin with Atto647N STED image - U2OS cell labeled for tubulin with Abberior STAR 635p (green) and giantin with Atto647N

Two fluorescent species can be distinguished by pulsed interleaved excititation (PIE) with two different diode lasers at 640 and 660 nm. Fluorescence is detected in two spectral bands. Fluorescence pattern matching was used to identify the contributions of each fluorophore. The example shows part of a U2OS cell labeled for tubulin with Abberior STAR 635p (green) and giantin with Atto647N (red) utilizing a single STED laser wavelength.


  • Excitation 640 and 660 nm
  • Depletion: 765 nm
  • PDL 828 "Sepia II" with SOM 828-D oscillator module

Sample courtesy of Markus Sauer, University of Würzburg, Germany


Crimson beads

Confocal image of crimson beads with 20 nm diameterSTED image of crimson beads with 20 nm diameter

The example shows a comparison between confocal and STED images of Crimson beads (20 nm diameter). Fluorescent beads are often used to evaluate the resolution of a microscope. The FWHM in the confocal image is 260 nm, and in the STED image it is 38 nm. The resolution enhancement is clearly visible.


  • Excitation: 640 nm
  • Depletion: 765 nm

Evaluating resolution with DNA origami

DNA origamiDNA origami

Specifically labeled DNA origami is now commonly used to evaluate the resolution of diffraction-limit-breaking microscopes. Here, origami with two rows of 11 dye molecules with a distance of 71 nm was used. Image size: 4 µm x 4µm


  • Excitation: 640 nm
  • Depletion: 765 nm

The samples were provided by GATTAquant GmbH and the Tinnefeld lab, TU Braunschweig, Germany


Latest 10 publications referencing MicroTime 200, SymPhoTime

The following list is an extract of 10 recent publications from our bibliography that either bear reference or are releated to this product in some way. Do you miss your publication? If yes, we will be happy to include it in our bibliography. Please send an e-mail to info@picoquant.com containing the appropriate citation. Thank you very much in advance for your kind co-operation.