Confocal Raman Microscope
Handheld Confocal Raman Skin Analyzer
Spinning Disk Confocal Microscope
Laser Point Scanning Confocal Microscope
Research Line Scan Confocal Microscope
Industry Line Scan Confocal Microscope
More
Auto-Fluorescence Microscope
Compact Multi-channel fluorescence microscope Module
Four-channel Single-mode /Multi-mode laser(405-640 nm)
Silicon photomultiplier(SIPM)(300-950nm)
Photomultiplier Tube (Module)(160-900nm)
Motorized Filter Wheels
MMF laser speckle reducers & beam homogenizers
TCSPC System for SPAD (APD) Testing Solution
Fiber Spectrometers (200nm to 2.5um)
Raman Spectrometer 532/785/1064nm
X-Ray/XUV/VUV Spectrometers (1-300nm)
FT Infrared Spectrometer(900-16000nm)
Hyperspectral Camera (220nm-12.5μm)
Multi-Spectral Camera (400-1000nm)
Single Photon Detector (SPD)(200-1700nm)
Photomultiplier Tubes (PMT)(160-900nm)
Photodiode Detector (PD) (5-1700nm)
Pyroelectric Infrared Detectors (2-12um)
Single-Photon Avalanche Diode Array
UV-VIS Beam Profiler(190-1100nm)
VIS-NIR Beam Profiler(350-1750nm)
Mid-infrared Beam Profiler(2-16μm)
Compact Beam Profiler(190-1100nm)
Terahertz Beam Profiler
Scanning Slit Beam Profiler
Photodiode Power Sensors 250-2500nm
Power Meter Console
Integrating Spheres (10mm-100mm)
Power Meter Adaptor & Accessories
Thermoelectric laser power meter(0.19-25 μm)
Photoelectric power meter(200-1100nm)
VUV/UV Spectrograph
Standard Single Grating Monochromator
Hi-Res Single Grating Monochromator
Double Grating Scanning Monochromator
Triple Grating Scanning Monochromator
Hi-Res Triple Grating Monochromator
Micro laser Doppler vibrometer DC~2.5MHz
Laser Doppler Vibrometer 0.1Hz to 5Mhz
LIV Test Systems for Laser Diode / LED
White Light Interferometer
Optical Test Measurement System
RF Test Measurement System
Point confocal displacement sensor
Linear confocal displacement sensor
CW Pigtail Laser Diode (400-1920nm)
CW Laser Diode Module (375-785nm)
CW Single Channel Lasers (365-1570 nm)
CW Multi-Channel Lasers (375-808nm)
CW Narrow Linewidth Diode Laser
External Cavity Tunable Diode Laser (399-1260 nm)
Nanosecond Pulse Fiber Laser(1064-2μm)
Picosecond Pulse Fiber Laser (266nm-2μm)
Femtosecond Pulse Fiber Laser (515-1570nm)
CW & QCW Fiber Laser System (405nm-2μm)
CW Narrow Linewidth Laser(780nm-2μm)
C-Band Tunable Laser (1529 -1567nm)
L-Band Tunable Laser (1554 -1607nm)
Supercontinuum Fiber Lasers 375-2400nm
2 μm CW Wide Tunable Laser (1900-2000 nm)
Femtosecond OPA (650 - 2600nm)
Short-pulse OPA (650 - 2600nm)
Erbium Doped Fiber Amplifier
Ytterbium Doped Fiber Amplifier
Thulium-Doped Fiber Amplifier
Semiconductor Optical Amplifier
Fiber Raman Amplifier
EUV Light Sources(58-130nm)
VUV Light Sources(115-400nm)
ASE Light Sources (830-2000nm)
Microscopy Imaging LED Sources 360-780nm
Collimated LED Sources (265-1450nm)
Fiber-Coupled LED Sources (265-940 nm)
Standardized Repetition Locking Optical Combs
Fully Locked Optical Frequency Combs
Asynchronous Optical Sampling Light Source
Optical Frequency Comb Accessories
Maskless Lithography UV Laser Writer
Light Field Sythesizer
Hollow-Core Fiber Compressor
High Powered Hollow-Core Fiber Compressor
Ultra-High Contrast 3rd-Order Autocorrelator
Coherent Ultrabroadband XUV Light Source
Terahertz Quantum Cascade Lasers(1-4.5Thz)
MIR QCL Turn-Key System (3-13μm)
MIR Packaged QCL(4-9.7μm)
MIR QCL Chips(4-12μm, Package Customizable)
Compact Multi-channel fluorescence microscope imaging module
Fluorescence Upright / Inverted Microscope
Biological Upright / Inverted Microscope
Phase Contrast Microscope
Dark Field Microscope
Polarizing Microscope
Metallographic Upright / Inverted Microscope
Smart 3D Stereo Microscope
USB Digital Microscope With Platform
Built-in Digital Microscope
Plan Apochromatic Objective
Industrial Plan Objective
Biology Plan Objective
Physiology/Life Sciences Objectives
Microscope CCD Camera (VIS-NIR)
Microscope CMOS Camera (UV-NIR)
UV & NIR Enhanced CMOS Camera
Hyperspectral Camera for Microscope
Multispectral Camera For Microscope
Microscope Light & Lamp
Soft X-Ray BSI sCMOS Camera (80-1000eV)
High-Speed sCMOS Camera
High Sensitivity sCMOS Camera
38M Pixel large Format sCMOS Camera
Compact BSI/FSI sCMOS Camera
Intensified CMOS Camera (200-1100nm)
Full Frame CCD Camera for UV VIS NIR
Full Frame CCD Camera for VUV EUV X-ray
Full Frame In-vacuum CCD Cameras
Large Format In-vacuum CCD Cameras
HDMI Color CMOS Camera (Monitor)
High Speed Line Scan Camera
Large Format Camera
High Speed Large Format Camera
Frame Grabber
Infrared Pyrometers (-40-3000C)
Linear Array Infrared Thermal Imager
Matrix Array Infrared Thermal Imager
Blackbody Calibration Sources -15 to 1500°C
SWIR Camera(400-1700nm) InGaAs CMOS
SWIR Camera(900-2200nm) InGaAs CMOS
Mid-Wave Infrared Camera (MWIR)
Long-Wave Infrared Camera (LWIR)
Solar Blind UV Imaging Module 240-280nm
UV-VIS Online Monitoring Module
UV-VIS Dual Channel Camera
UV-VIS-IR Triple Spectral Fusion Camera
Ultraviolet Camera for Drone
Free Space Acousto-Optic Modulators (AOM)
Fiber Coupled Acousto-Optic Modulators
Free Space Acousto-Optic Tunable Filter
Fiber-coupled Acousto-optic Tunable Filter
Acousto-Optic Q-switch (AOQ)
Acousto-Optic Frequency Shift (AOFS)
Electro-optical Amplitude Modulator
Electro-optic Phase Modulator
Time-Correlated Single Photon Counting (TCSPC)
Ultra-fast Pulse Generator for TCSPC
Phase Spatial Light Modulator
Transmission Amplitude SLM
Reflection Amplitude SLM
Digital Micromirror Device (DMD)
Pulsed Voltage
Pulsed Current
General Purpose Pulse Generators
Medium and High Voltage Pulse Generators
High Speed Impulse Generator
Very High Speed Pulse Generators
Function Generators
Pulse Amplifiers
Single-channel Lock-in Amplifier
Dual-channel Lock-in Amplifier
Narrowband Tunable Filter
Broadband Tunable Filter
Bandpass Tunable Filter
TPX / HDPE Terahertz Plano Convex Lens
Off-Axis Parabolic Mirrors
Terahertz Hollow Retro Reflector
Terahertz Metallic Mirrors
ZnTe / GaSe Terahertz Crystals
Terahertz Beam Expander Reflection
Waveplates
Optical Isolator
Optical Polarizers
Beamsplitter Plate
Beamsplitter Cube
Dichroic Beamsplitters
Ultrathin Beamsplitter Plate
Bandpass Filters Fluorescence Microscope
Filters for Raman Spectroscopy
Narrow Filters for Laser
Filters for FISH
Filters for TIRF Microscope
Filters for FRET Microscope
Laser Crystals
Nonlinear Optical Crystals
Birefringent Crystals
Optical Crystals
Electro-optical Crystals
Micro-Channel Plate (MCP)
Micro-Channel Plate Assembly (MCP)
Fiber Optic Plates (FOP)
Micro Pore Optics
X-Ray Collimators
Hybrid Fiber Components
Electrically Adjustable Optical Delay Line
Manually Adjustable Optic Delay Line
Optical Circulator
FA Lens
Zoom Lens
Telecentric Lens Series
Optical Heating & Cryo Stage
Electrical Probe Temperature Stage
Adjustable Electrical Probe Station
In-situ Tensile Heating & Cryo Stage
SEM/XRD Heating & Cryo Stage
Live-Cell Incubator Stages
Single Axis Motorized Piezo Stage
XY Motorized Piezo Stages
Multi Axis Motorized Piezo Stages
Vacuum Non-magnetic Piezo Stage
Nano Electric Actuator
XY Stepper Motor Stages
XYZ 3 Axis Stepper Motor Stages
XY Microscope Piezo Stages
XY Microscope Linear Motor Stages
Motorized Filter Wheels Mount
FWR Motorized Filter Wheels
Manual Filter Wheels
Manual Filter Wheels Mount
13mm Linear Stages
25mm Linear Stages
Rotation and Tilt Stages
Rack and Pinion Stages
Vertical Axis Stages
2-Axis Stages
Solid Vibration Isolation Optical Table
Pneumatic Optical table
Pneumatic Optical Table With Pendulum Rod
Desktop Pneumatic Optical Table
Honeycomb Optical Breadboard
Lens Mounts
Mirror Mounts
Filter Mounts
Simtrum's Multimodal Microscopy Platform is a highly integrated, flexible, and modular fluorescence dynamics testing system designed for comprehensive characterization of all classes of luminescent materials. It supports conventional fluorescence, phosphorescence, and afterglow imaging.
Built on an open, modular optical architecture with high-precision mechanical interfaces, the platform enables seamless integration of:Multi-source excitation (lasers and LEDs),Multi-path illumination (upright, side, inverted),Synchronized acquisition of image, spectral, and lifetime data.
By swapping functional modules, users can switch between excitation modes in seconds—enabling rapid adaptation to diverse sample types including thin films, solutions, cells, tissues, microfluidic chips, and single nanoparticles. This platform supports the full research workflow: material discovery → mechanism elucidation → device validation.
Features
Supports independent or synchronized operation of laser and LED sources across 350–1550 nm. Specifically optimized for Photon Avalanche (PA) materials requiring stringent excitation conditions. Includes a high-stability 1064 nm laser (power stability ≤ ±0.5% RMS) with precise power density control (0.1–500 kW/cm²) for PA threshold crossing and nonlinear response measurements.
Switches between upright, side, and inverted excitation geometries in <2 minutes—without moving the sample or realigning optics. Compatible with slides, cuvettes, Petri dishes, microfluidic chips, and single particles. Ideal for both static characterization and dynamic process monitoring.
Integrates digital imaging, spectral resolution (200–1700 nm), and time-resolved detection (<30 ps time resolution). Simultaneously captures fluorescence intensity, emission peak position, and lifetime dynamics. Achieves <50 nm spatial resolution in single-particle PA super-resolution imaging and supports lifetime measurements from 100 ps to 10 s.
Uses standardized cage-based optics and quick-connect interfaces with auto-alignment. The companion software supports automatic background subtraction, multi-peak fitting, multi-exponential lifetime decay modeling, Stokes shift calculation, and one-click generation of standardized PDF/Excel reports—enhancing research efficiency and data reproducibility.
Applications
Highly Integrated Multimodal Fluorescence Dynamics Testing System – Excitation Light Source Subsystem
Dual-Laser Co-Excitation Module
It provides highly stable continuous-wave or pulsed laser output (power stability ≤ ±0.5% RMS), with wavelength coverage spanning 350–1550 nm, precisely matching the absorption transitions of luminescent centers such as Tm³⁺ and Er³⁺ (e.g., 1064 nm excitation for the ³H₆ → ³H₅ transition).
An integrated motorized polarization control unit enables rapid switching among linear, circular, and elliptical polarization states, fulfilling the requirements for polarization-dependent studies on anisotropic materials.
The dual-channel independent design supports either single-beam or synchronized dual-beam excitation (temporal synchronization accuracy < 1 ns), making it suitable for investigating complex photophysical processes such as upconversion cascades, cross-relaxation, and photon avalanche, thereby offering a quantifiable and reproducible excitation platform for cutting-edge luminescence mechanism research.
LED Beam Modulation Module
It employs a high-brightness single-band or multi-band composite LED light source, delivering incoherent excitation across a broad spectral range (365–940 nm) or narrow bands (full width at half maximum, FWHM: 15–40 nm), with low thermal impact, minimal phototoxicity, and high stability (power fluctuation ≤ ±1.0% RMS).
This makes it particularly well-suited for long-term dynamic observation of light-sensitive systems such as live cells, organic fluorescent dyes, and TADF (thermally activated delayed fluorescence) materials. Integrated with an motorized wavelength selection module, the system can switch to the desired excitation band in under 50 ms, effectively suppressing stray light interference.
Its uniform illumination mode significantly reduces the risk of photobleaching and enhances data reproducibility in broadband-response measurements, making it an ideal excitation solution for high-throughput screening, educational experiments, and combined laser-LED research applications.
Highly Integrated Multimodal Fluorescence Dynamics Testing System – Sample Excitation Configuration
Highly Integrated Multimodal Fluorescence Dynamics Testing System – Signal Acquisition Capability
Digital Imaging Module
Equipped with a scientific-grade sCMOS, EMCCD, or high-quantum-efficiency CCD camera (quantum efficiency > 82%, read noise ≤ 1.0 e⁻), the system delivers high sensitivity, low noise, and high frame rates, enabling clear capture of weak luminescence or transient dynamic signals.
It supports advanced imaging functions such as time-lapse acquisition, region-of-interest (ROI) imaging, and high dynamic range (HDR) imaging. A motorized, adjustable emission filter module positioned at the front end effectively suppresses background stray light, significantly enhancing image contrast and signal-to-noise ratio.
Whether for single-particle photoacoustic (PA) imaging (< 50 nm), cellular fluorescence distribution mapping, or large-area luminescence imaging, the system delivers professional-grade visualization results.
Spectral Resolution Acquisition ModuleCovering a broad spectral range from 200 to 1700 nm, the module achieves a spectral resolution of better than 0.1 nm in the visible region, enabling precise resolution of fine spectral features such as multi-peak structures, Stokes shifts, and energy-level splitting.
It employs a high-transmission focusing optical path combined with low-loss fiber coupling technology to ensure efficient signal delivery to the spectral analysis unit.
The accompanying intelligent software automatically performs background subtraction, peak identification, multi-peak fitting, intensity normalization, and component deconvolution, and can generate professional reports—complete with spectral curves and key parameters—with a single click. This fully supports applications ranging from basic characterization to in-depth mechanistic studies.
Time-resolved detection module
Based on Time-Correlated Single Photon Counting (TCSPC) technology, the system achieves a time resolution better than 50 ps, enabling precise measurement of dynamic processes across the full timescale—from nanosecond fluorescence decays to second-scale afterglow emissions.
It supports simultaneous acquisition of multidimensional parameters such as rise time, decay lifetime, and delayed luminescence intensity, offering comprehensive insights into excited-state energy relaxation, charge transfer, or triplet-state evolution mechanisms.
Equipped with highly sensitive detectors—including avalanche photodiodes (APDs), single-photon counting modules (SPCMs), or high-speed photomultiplier tubes (PMTs)—the system delivers high signal-to-noise ratio lifetime curves even under extremely low-concentration or weak-emission conditions. It serves as an essential tool for dynamic studies of advanced luminescent materials such as TADF emitters, phosphors, upconversion systems, and quantum dots.
Highly Integrated Multimodal Fluorescence Dynamics Testing System – System Integration and Control
Multimodal Configuration Module
As the core control unit of the system, it integrates three spatial excitation pathways—upright, side-illumination, and inverted—and supports two types of light sources: laser and LED.
It enables rapid switching among five operational modes: single/dual-laser upright, single/dual-laser side-illumination, LED upright, LED side-illumination, and laser inverted. Through built-in electronically controlled optical-path deflection components—including dichroic mirrors, reflectors, and optical switches—the system dynamically reconfigures both excitation light delivery and emission signal collection.
Users can switch between modes in seconds without any manual optical alignment, significantly enhancing experimental efficiency, data consistency, and operational convenience.
Multimodal and multipattern
Multimodal Operation Modes
The Multimodal Switching Hub integrates three spatial excitation geometries (upright, side, inverted) and two light sources (laser/LED), supporting five operational modes:
Mode switching takes <2 seconds via software or motorized sliders—no manual realignment needed. Factory-calibrated to sub-micron precision; optical loss <3%, pointing stability ≤ ±2 µm.
This “plug-and-play” design dramatically improves experimental efficiency and data reproducibility across diverse samples—from solid films and PA nanocrystals to dynamic solutions—and from static imaging to ultrafast time-resolved studies.
Dual-laser co-excitation modulation module
Spectral resolution / time-resolved detection module
Digital imaging module
Multi-functional sample stage (with side excitation)
Inverted sample excitation module
LED beam modulation module
Multi-module microscope optical path diagram
Front view of a multi-module microscope
Photon Avalanche (PA) Materials
Enables full-parameter characterization of ultra-nonlinear emitters (e.g., NaLuF₄:Tm³⁺ nanocrystals), including:
Single-particle NaLuF₄:Tm photon avalanche (PA) imaging with spatial resolution < 5
The nonlinear exponent of NaLuF₄:Tm reaches 281, significantly outperforming the NaYF₄ host matrix.
The 176 nm nanodisks exhibit an average optical nonlinearity exceeding 500,with highly reproducible performance.
Super-Resolution Optical Imaging
Leverages extreme nonlinearity of PA materials to achieve <50 nm resolution using a single continuous-wave laser—eliminating the need for complex STED or RESOLFT setups. Ideal for low-phototoxicity, long-term live-cell imaging.
Super-resolution reconstruction (<50 nm) using a single laser beam based on the PA effect
Diffraction-limited image (~300 nm), in stark contrast to the super-resolution result.
Ten-thousand-particle Monte Carlo simulations validate the universality of PA-based super-resolution.
Fluorescent Material Optimization & Screening
Combines spectral and lifetime data to rapidly evaluate:
Raman peak blueshift >10 cm⁻¹, indicating an increase in phonon energy.
HAADF-STEM and EDS mapping confirm uniform elemental doping.
XRD Rietveld refinement reveals lattice contraction (Δa ≈ −0.5%) due to Lu³⁺ substitution.
Fluorescent Probe Development
Validates targeting, sensitivity, and biocompatibility of smart probes for pH, ions, ROS, etc.—especially NIR-II PA probes for dynamic monitoring.
Multicolor PA probes for live-cell NIR-II super-resolution imaging.
Broad-spectrum upconversion emission covers the 450–1700 nm biological window.
Surface ligand engineering significantly influences the PA emission intensity and stability.
Photophysical Dynamics Studies
Precisely resolves transient behaviors: fluorescence lifetime, rise/decay times, delayed emission. Reveals microscopic mechanisms like excited-state relaxation, cross-relaxation (CR), and energy migration—providing quantitative inputs for multi-level systems (e.g., Tm³⁺/Er³⁺).
Key rate parameter table: GSA/ESA/CR enabling quantitative modeling.
The ³F₄ metastable level has a lifetime of 95 μs, supporting efficient avalanche cycling.
Host engineering modulates the Tm³⁺ energy level lifetimes to optimize PA dynamics.
Nanomaterial Spectral Analysis
Performs single-particle analysis of:
Multipeak emission spectra resolve the luminescence behavior in blue, red, and NIR channels.
XANES confirms Tm is in the +3 oxidation state, with no valence defects.
XPS reveals enhanced local crystal field, leading to improved luminescence efficiency.
Interdisciplinary Research & Industrial Testing
Applications span:
Comprehensive overview of PA materials applications in anti-counterfeiting, displays, sensing, and beyond.
Multichannel PA imaging enables multiplexed biological detection.
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Light Analysis
Microscope
Light Sources
Imaging
Optics