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Scientific Research GradeAstigmatism-Free

HiperS-320iAberration-Free Imaging Spectrometer

By implementing a full focal plane aberration correction optical design, the HiperS-320i eliminates off-axis astigmatism across the entire sensor surface. This delivers superior multi-channel measurement capabilities, increased spectral resolution, and reliable, peak-accurate intensity measurements across large-format CCD and sCMOS detectors.

✓ 320mm Focal Length
✓ On-axis Triple Turret
✓ Up to 20% Resolution Boost
✓ Flat Field corrected plane
HiperS-320i aberration-free imaging spectrometer

Key Technologies

Advanced Optomechanical Design

Engineered for high-end research applications including LIBS, Confocal Raman, Multi-track Fluorescence, and Transient Absorption Spectroscopy.

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Multi-Port Configuration

Supports up to two automated entrance ports and two exit ports. Fully motorized optical path switching provides maximum experimental flexibility.

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On-Axis Grating Turret

Grating rotation on the optical axis increases the active area of the diffraction gratings. Optimizes illumination efficiency and provides a 15% increase in grating utility.

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Resolution Intensifier

A built-in optical intensifier module increases standard spectrometer resolution by up to 20%, concentrating photons into narrower, sharper peaks.

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Intelligent Auto-Focus

Automatic focusing mirror adjusts positioning dynamically during grating rotation to maintain perfect focus and high spectral/spatial resolution.

Interactive Laboratory Demo

Performance Verification Plots

Explore the optical behavior of the HiperS-320i compared to standard Czerny-Turner layouts. Toggle the controls to visualize real performance characteristics.

Interactive Peak Profile
FWHM: 0.096 nm (-20%)Wavelength (nm)Normalized Intensity435.5435.7435.83436.0436.20.00.40.81.2Intensifier Active (+20% Res)

Spectral Resolution Enhancement Module

Standard spectrographs encounter aberrations away from the center of the detector plane. The HiperS-320i incorporates a built-in Resolution Intensifier Module.

When engaged, this optical array optimizes the wave curvature. This reduces the spectral line Full Width at Half Maximum (FWHM) by approximately 20%.

Example: At 435.83 nm, the FWHM narrows from 0.120 nm down to 0.096 nm. This allows you to resolve closely spaced emission bands that would otherwise merge.

💡 Scientific Impact

By eliminating astigmatism, photons are not spread vertically across multiple pixel rows but are instead concentrated onto a minimal pixel footprint. This dramatically improves the Signal-to-Noise Ratio (SNR) and absolute limit of detection for weak fluorescence or Raman signals.

Specifications

Instrument Parameters

HiperS-320i Core Specs

Focal Length320 mm
Aperture Ratiof/4.4
Scan Range (with 1200 g/mm)0 – 1430 nm
Resolution (PMT)0.06 nm
Resolution (CCD, 15 μm pixels)0.12 nm
Dispersion2.29 nm/mm
Wavelength Accuracy±0.2 nm
Wavelength Repeatability±0.025 nm
Step Size0.005 nm
Stray Light Rejection5 × 10⁻⁵
Focal Plane Size29 mm (w) × 14 mm (h)
Optical Axis Height156.3 – 171.3 mm (adjustable)
Grating Dimensions68 mm × 68 mm
Grating MountOn-Axis Triple Turret
Slit Configuration0.01 – 3.00 mm continuous manual slit (motorized optional). Height options: 2, 4, 14 mm.
Physical Dimensions591 × 460 × 260 mm (L × W × H)
Weight30 kg (excluding options)
Communication InterfaceUSB 2.0 / RS-232

Performance by Grating Selection

System performance (resolution, dispersion, spectral coverage) shifts depending on the groove density of the installed diffraction grating. The HiperS-320i turret fits up to 3 gratings.

GratingDisp. (nm/mm)Scan (nm)Res (PMT)Res (CCD)One-Shot (nm)
2400 g/mm0.910 – 7150.03 nm0.048 nm26.4 @30mm
1800 g/mm1.390 – 9530.04 nm0.073 nm40.3 @30mm
1200 g/mm2.290 – 14300.06 nm0.12 nm66.4 @30mm
600 g/mm4.870 – 28600.12 nm0.256 nm141.2 @30mm
300 g/mm9.970 – 42900.24 nm0.523 nm289.1 @30mm
150 g/mm20.130 – 114400.48 nm1.06 nm583.8 @30mm

Note 1: Slit resolution measured at central wavelength of 435.83 nm, with a 10 μm slit width.

Note 2: CCD one-shot spectral range is computed for a typical 30 mm width CCD detector.

Note 3: Dispersion varies inversely with central wavelength settings.

Configurations

Typical Selection & Port Codes

Configure your HiperS-320i layout matching your detector and light source geometry.

ModelOptomechanical Port Configuration
HiperS-3204iSide entrance slit, double CCD exit ports
HiperS-3205iSide entrance slit, front exit slit
HiperS-3206iSide entrance slit, front CCD exit port
HiperS-3207iSide entrance slit, double exit slits
HiperS-3208iSide entrance slit, front CCD exit port and side exit slit
HiperS-3224iDouble entrance slits, double CCD exit ports
HiperS-3227iDouble entrance slits, double exit slits
HiperS-3228iDouble entrance slits, front CCD exit port and side exit slit
HiperS-3247iSide entrance slit, double exit slits with UV coating
HiperS-3248iSide entrance slit, front CCD exit port and side exit slit with UV coating
Gratings, motorized slits, filter wheels, shutters, and coupling optical adapters are configured individually.

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