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PicoQuant Time-resovled Confocal Fluorescence Microscope – MT200 STED

Time-resolved Confocal Fluorescence Microscope with Super-Resolution Capability

Picoquant Time-resolved Confocal Fluorescence Microscope – MicroTime 200 STED

  • 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 4 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, analysis and visualisation 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.
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**

For STED

  • 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
Microscope
  • 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)
Objectives
  • 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)
Scanning
  • 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
Detectors
  • 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 four channels
Software
  • 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.

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 theMicroTime 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

 

STED 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.

Mount for phase plate

 

Choice of excitation wavelengths

The 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 driverPDL 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.

 

Laser Combining Unit (LCU) of the MicroTime 200 STED

Detection subsystem with single photon sensitivity

In 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 four 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.

Detection unit of the MicroTime 200 STED

Gated STED with picosecond resolution

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.

HydraHarp 400 - Mutichannel TCSPC Module (small configuration)

 

Intuitive data acquisition and analysis

SymPhoTime 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.

SymPhoTime 64 STED

 

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.