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Alpha CRS

High-speed coherent Raman imaging

The Stuttgart Instruments Alpha CRS is a complete coherent Raman imaging light source: a tunable pump and a synchronized Stokes beam from one box. It is optimized for the fast image acquisition in stimulated Raman scattering (SRS) and coherent anti-Stokes Raman scattering (CARS) microscopy.

  • 10 MHz and 1 ps for maximum coherent Raman signal
  • Full Raman window coverage from 400 – 4500 cm⁻¹ Stokes shift with optional simultaneous dual-Stokes acquisition
  • Shot-noise-limited RIN below −168 dBc/Hz
Alpha CRS laser system

Alpha CRS specifications

Values below are representative for the standard configuration. Ask us for a configuration-specific datasheet.

Alpha CRS 1 psAlpha CRS 2 ps
Stokes wavelength1030 nm
Stokes 2 wavelength (optional)1020 – 1035 nm
Pump wavelength700 – 980 nm
Stokes shift400 – 4500 cm⁻¹
Pulse duration1 ps2 ps
Linewidth< 25 cm⁻¹< 12 cm⁻¹
Time–bandwidth product< 0.6
Repetition rate10 MHz
Stokes modulationDC – 5 MHz
RIN< −168 dBc/Hz at 50 kHz – 5 MHz
Beam pointing< 30 µrad
Power stability< 0.5 %
Spectral stability< 0.01 %
Output power 1000 mW at 1030 nm
300 mW at 1020 – 1035 nm (2nd Stokes, optional)
500 mW at 1030 nm (100 fs, optional)
90 mW at 700 nm
300 mW at 800 nm
200 mW at 950 nm

Optimized for fastest image acquisition

−168 dBc/Hz
Ultra-low relative intensity noise
10 MHz
Speed-optimized repetition rate
20 cm⁻¹
SNR-optimized linewidth

Short 1 ps pulses concentrate more peak power into the stimulated Raman process at the same average power, enhancing the measured signal. Lower repetition rate further enhances the signal as it permits higher pulse energies on the sample before thermal damage sets in. The ultra-low RIN ensures that demodulation or boxcar acquisition exploit their full potential at any frequency above 50 kHz with simple single-channel detection.

Measured relative intensity noise of Alpha CRS pump and Stokes versus frequency
Measured relative intensity noise of the Stokes (1030 nm) and pump (790 nm) outputs, shot-noise limited above 50 kHz at 20 mW.
  • Flexible Full Raman frequency range, 400 – 4500 cm⁻¹
  • Robust Low spectral drift, < 0.05 cm⁻¹/h
  • Simple Single-channel, shot-noise-limited detection

Options

Dual Stokes output

A second, independently set Stokes wavelength for simultaneous multi-band acquisition.

Beam combining and delay compensation

Pump and Stokes are combined and delay-matched at the output, microscopy ready.

100 fs bypass for broadband CARS

An optional 100 fs bypass path adds broadband CARS capability alongside the standard narrowband SRS configuration.

Stimulated Raman histology

100 Mpx
SRH image of brain tissue
≈ 512 ns
Pixel dwell time
2 min
Total measurement time*
Stimulated Raman histology overview of brain tissue, roughly 1 millimeter field of view
100 Mpx SRH image of brain tissue recorded at approximately 512 ns pixel dwell time.
Stimulated Raman histology detail, roughly 100 micrometer field of view

*Including mechanical repositioning. Image recorded by the group of Dr. Sandro Heuke (CNRS, Marseille).

“The 11 MHz ps-OPO from Stuttgart Instruments delivers outstanding stability, fast and broad tunability, significantly speeding up our coherent Raman measurements.”

Dr. Sandro Heuke CNRS, Marseille

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