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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
Zolix 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.

ðŸ’Ą 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 Ξm pixels)0.12 nm
Dispersion2.29 nm/mm
Wavelength AccuracyÂą0.2 nm
Wavelength RepeatabilityÂą0.025 nm
Step Size0.005 nm
Stray Light Rejection5 × 10âŧâĩ
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 Ξm 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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