Products> Wavelength-Tunable Sources

High Energy Optical Parametric Amplifier

TOPAS-PRIME-HE High Energy Optical Parametric Amplifier.
  • 189 nm – 20 μm tuning range
  • Up to 60 mJ pump pulse energy
  • Up to 50% conversion efficiency
  • Idler CEP slow drift stabilization option available
  • Fresh pump channel for improved sum‑frequency generation
Download datasheet
TOPAS-PRIME-HE High Energy Optical Parametric Amplifier.

TOPAS-PRIME-HE is a high-energy femtosecond optical parametric amplifier (OPA) based on TOPAS-PRIME, featuring an additional high-energy and low-dispersion amplification stage, which allows using pump pulse energies of up to 60 mJ while maintaining the shortest possible output pulse.

  • TOPAS-PRIME-HE accepts pump pulse energies of up to 15 mJ at 35 – 70 fs (up to 27 mJ at 100 – 200 fs).
  • TOPAS-PRIME-HE-PLUS supports higher pump pulse energies, up to 35 mJ at 35 – 70 fs (up to 60 mJ at 100 – 200 fs). The 60 mJ pump pulse energy is achievable with longer pulse durations, around 150 fs.

Both models include wavelength extension options:

  • TOPAS-PRIME-HE: Tunable from 189 nm to 20 μm.
  • TOPAS-PRIME-HE-PLUS: Tunable from 240 nm to 20 μm.

Ultrafast (20–70 fs)
Specifications notes

TOPAS-PRIME-HE and TOPAS-PRIME-HE-PLUS specifications are given for the following pump laser parameters:

  • Wavelength: 800 nm
  • Pulse energy: 6 mJ
  • Repetition rate: 1 kHz
  • Pulse duration: 30 – 40 fs
  • Beam profile: Gaussian

Note 1: Specifications depend on the pump wavelength and pulse duration. If these differ from the values listed above, contact  sales@lightcon.com.

Note 2: TOPAS-PRIME-HE output pulse energy scales linearly within the 3 – 20 mJ range, provided the device is installed and optimized for a specific pump energy. Re-optimization is required if the pump energy changes by more than 10% from the installation value.

Pump laser requirements
ModelTOPAS-PRIME‑HETOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUSTOPAS‑PRIME-HE‑PLUS
ModelTOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUS
Pump wavelength770 – 830 nm770 – 830 nm770 – 830 nm770 – 830 nm
Pump wavelength770 – 830 nm
Pump pulse duration (FWHM)20 – 35 fs35 – 70 fs20 – 35 fs35 – 70 fs
Pump pulse energy2 – 8 mJ2 – 15 mJ2 – 18 mJ2 – 35 mJ
Repetition rate< 25 kHz 1)< 25 kHz 1)< 25 kHz 1)< 25 kHz 1)
Repetition rate< 25 kHz 1)
Maximum pump power40 W 2)40 W 2)40 W 2)40 W 2)
Maximum pump power40 W 2)
Pump polarizationHorizontalHorizontalHorizontalHorizontal
Pump polarizationHorizontal
Spectral bandwidth< 1.2 × transform limit< 1.2 × transform limit< 1.2 × transform limit< 1.2 × transform limit
Spectral bandwidth< 1.2 × transform limit
Pulse-to-pulse energy stability< 1% RMS deviation 3)< 1% RMS deviation 3)< 1% RMS deviation 3)< 1% RMS deviation 3)
Pulse-to-pulse energy stability< 1% RMS deviation 3)
Pulse duration stability< 1% pulse-to-pulse 4)< 1% pulse-to-pulse 4)< 1% pulse-to-pulse 4)< 1% pulse-to-pulse 4)
Pulse duration stability< 1% pulse-to-pulse 4)
Pulse front tilt< 10% of pulse duration< 10% of pulse duration< 10% of pulse duration< 10% of pulse duration
Pulse front tilt< 10% of pulse duration
Pulse contrast< 1 : 20< 1 : 20< 1 : 20< 1 : 20
Pulse contrast< 1 : 20
Beam quality, M2< 1.3 5)< 1.3 5)< 1.3 5)< 1.3 5)
Beam quality, M2< 1.3 5)
Beam astigmatism< 0.15 6)< 0.15 6)< 0.15 6)< 0.15 6)
Beam astigmatism< 0.15 6)
Beam spatial profileGaussian – Super GaussianGaussian – Super GaussianGaussian – Super GaussianGaussian – Super Gaussian
Beam spatial profileGaussian – Super Gaussian
Intensity modulation< 15%, no hotspots 7)< 15%, no hotspots 7)< 15%, no hotspots 7)< 15%, no hotspots 7)
Intensity modulation< 15%, no hotspots 7)
Beam pointing stability< 10 μrad 8)< 10 μrad 8)< 10 μrad 8)< 10 μrad 8)
Beam pointing stability< 10 μrad 8)
Beam divergence< 1.2 × diffraction limit< 1.2 × diffraction limit< 1.2 × diffraction limit< 1.2 × diffraction limit
Beam divergence< 1.2 × diffraction limit
Beam height from optical table125 – 185 mm 125 – 185 mm 125 – 185 mm 125 – 185 mm 
Beam height from optical table125 – 185 mm 
Beam diameter, 1/e2< 19 mm 9) 10)< 19 mm 9) 10)< 19 mm 9) 10)< 19 mm 9) 10)
Beam diameter, 1/e2< 19 mm 9) 10)
ModelTOPAS-PRIME‑HETOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUSTOPAS‑PRIME-HE‑PLUS
ModelTOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUS
  1. The maximum repetition rate for DFG1 (NDFG1) option is 1 kHz.
  2. Contact sales@lightcon.com for higher pump power options.
  3. Normalized to average pulse energy. Expressed as normalized root mean squared deviation (NRMSD).
  4. Normalized to average pulse duration. Expressed as NRMSD.
  5. M2 specification valid for Gaussian beam.
  6. Normalized astigmatism – difference of the waist positions, divided by Rayleigh length.
  7. Normalized to Gaussian or Super-Gaussian fits. Expressed as NRMSD.
  8. Expressed as NRMSD, full angle.
  9. An optional external telescope can be ordered for a beam size of < 39 mm, 1/e2 (69 mm clear aperture mirrors).
  10. A limitation on the minimum beam diameter applies. The minimum beam diameter depends on pulse duration and energy. 
Output
ModelTOPAS-PRIME-HETOPAS-PRIME-HE-PLUS
Tuning range1160 – 1600 nm (Signal)
1600 – 2600 nm (Idler)		1160 – 1600 nm (Signal)
1600 – 2600 nm (Idler)
Tuning range1160 – 1600 nm (Signal)
1600 – 2600 nm (Idler)
Conversion efficiency at peak (Signal and Idler combined)> 30%> 30%
Conversion efficiency at peak (Signal and Idler combined)> 30%
Pulse duration(1 – 1.5) × pump pulse duration @ 1160 – 1550 nm
< 2 × pump pulse duration @ 1550 – 2600 nm		(1 – 1.5) × pump pulse duration @ 1160 – 1550 nm
< 2 × pump pulse duration @ 1550 – 2600 nm
Pulse duration(1 – 1.5) × pump pulse duration @ 1160 – 1550 nm
< 2 × pump pulse duration @ 1550 – 2600 nm
Time-bandwidth product< 1< 1
Time-bandwidth product< 1
PolarizationVertical (Signal)
Horizontal (Idler)		Vertical (Signal)
Horizontal (Idler)
PolarizationVertical (Signal)
Horizontal (Idler)
Pulse-to-pulse energy stability< 3% RMS deviation 1) @ 1160 – 1550 nm< 3% RMS deviation 1) @ 1160 – 1550 nm
Pulse-to-pulse energy stability< 3% RMS deviation 1) @ 1160 – 1550 nm
ModelTOPAS-PRIME-HETOPAS-PRIME-HE-PLUS
  1. Normalized to average pulse energy. Expressed as NRMSD.
VIS–UV–DUV extensions (189 – 1160 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
ControlManual change of wavelength separatorsManual change of wavelength separators
ControlManual change of wavelength separators
Maximum tuning range189 – 1160 nm240 – 1160 nm
HousingMonolithic housingMonolithic housing
HousingMonolithic housing
Number of output portsFour 1)Six 1)
Available withTOPAS-PRIME-HETOPAS‑PRIME-HE‑PLUS
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
  1. Output ports are wavelength-dependent.
VIS extensions (475 – 1160 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
SHI (800 – 1160 nm)
Tuning range800 – 1160 nm800 – 1160 nm
Tuning range800 – 1160 nm
Conversion efficiency at peak> 2% 1)> 2% 1)
Conversion efficiency at peak> 2% 1)
Pulse duration(1 – 1.5) × pump pulse duration(1 – 1.5) × pump pulse duration
Pulse duration(1 – 1.5) × pump pulse duration
PolarizationVerticalVertical
PolarizationVertical
SHS (580 – 800 nm)
SFI (533 – 600 nm)
SFS (475 – 533 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
  1. > 1.6% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  2. > 3.3% at peak with NIRUVIS‑DUV, due to additional pump pulse energy into the DUV option.
  3. > 2.5% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  4. > 3% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
UV extensions (240 – 480 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
FHI (400 – 480 nm)
Tuning range400 – 480 nm400 – 480 nm
Tuning range400 – 480 nm
Conversion efficiency at peak> 0.3% 1)> 0.3% 1)
Conversion efficiency at peak> 0.3% 1)
Pulse duration(1.2 – 2) × pump pulse duration(1.2 – 2) × pump pulse duration
Pulse duration(1.2 – 2) × pump pulse duration
PolarizationHorizontalHorizontal
PolarizationHorizontal
FHS (290 – 400 nm)
SH of SFI (266 – 295 nm)
SH of SFS (240 – 266 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
  1. > 0.2% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  2. > 0.4% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
DUV extensions (189 – 240 nm)
ExtensionNIRUVIS-HE-DUVNIRUVIS-HE-DUVNIRUVIS-HE-DUV
ExtensionNIRUVIS-HE-DUV
Pump + FHSPump + SH of SFIPump + SH of SFS
Tuning range215 – 240 nm200 – 215 nm189 – 200 nm
Conversion efficiency at peak> 0.2% 1)Not specifiedNot specified
Conversion efficiency at peak> 0.2% 1)Not specified
PolarizationVerticalVerticalVertical
PolarizationVertical
ExtensionNIRUVIS-HE-DUVNIRUVIS-HE-DUVNIRUVIS-HE-DUV
ExtensionNIRUVIS-HE-DUV
  1. Assuming 15% of the pump pulse energy is allocated to the DUV channel and another 15% to the fresh pump channel.
DFG extensions (2600 – 15000 nm)
ExtensionNDFG1W 1) 2)NDFG1KNDFG2 3)
Tuning range2.6 – 9 μm2.6 – 4.5 μm4 – 15 μm
Conversion efficiency at peak> 0.3%> 0.4%> 0.2%
Pulse duration< 3 × pump pulse duration< 3 × pump pulse durationNot specified
Pulse duration< 3 × pump pulse durationNot specified
PolarizationHorizontalHorizontalHorizontal
PolarizationHorizontal
ExtensionNDFG1W 1) 2)NDFG1KNDFG2 3)
  1. Maximum pump repetition rate is 1 kHz; crystal lifetime of 1000 – 2000 h.
  2. Not available with TOPAS‑HE-PRIME-PLUS.
  3. Extended lead time for TOPAS‑HE-PRIME-PLUS.
Fast (70–200 fs)
Specifications notes

TOPAS-PRIME-HE and TOPAS-PRIME-HE-PLUS specifications are given for the following pump laser parameters:

  • Wavelength: 800 nm
  • Pulse energy: 10 mJ
  • Repetition rate: 1 kHz
  • Pulse duration: 100 fs
  • Beam profile: Gaussian

Note 1: Specifications depend on the pump wavelength and pulse duration. If these differ from the values listed above, contact  sales@lightcon.com.

Note 2: TOPAS-PRIME-HE output pulse energy scales linearly within the 3 – 20 mJ range, provided the device is installed and optimized for a specific pump energy. Re-optimization is required if the pump energy changes by more than 10% from the installation value.

Pump laser requirements
ModelTOPAS-PRIME‑HETOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUSTOPAS‑PRIME-HE‑PLUS
ModelTOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUS
Pump wavelength770 – 830 nm770 – 830 nm770 – 830 nm770 – 830 nm
Pump wavelength770 – 830 nm
Pump pulse duration (FWHM)70 – 100 fs100 – 200 fs70 – 100 fs100 – 200 fs
Pump pulse energy2 – 20 mJ2 – 27 mJ2 – 47 mJ2 – 60 mJ
Repetition rate< 25 kHz 1)< 25 kHz 1)< 25 kHz 1)< 25 kHz 1)
Repetition rate< 25 kHz 1)
Maximum pump power40 W 2)40 W 2)40 W 2)40 W 2)
Maximum pump power40 W 2)
Pump polarizationHorizontalHorizontalHorizontalHorizontal
Pump polarizationHorizontal
Spectral bandwidth< 1.2 × transform limit< 1.2 × transform limit< 1.2 × transform limit< 1.2 × transform limit
Spectral bandwidth< 1.2 × transform limit
Pulse-to-pulse energy stability< 1% RMS deviation 3)< 1% RMS deviation 3)< 1% RMS deviation 3)< 1% RMS deviation 3)
Pulse-to-pulse energy stability< 1% RMS deviation 3)
Pulse duration stability< 1% pulse-to-pulse 4)< 1% pulse-to-pulse 4)< 1% pulse-to-pulse 4)< 1% pulse-to-pulse 4)
Pulse duration stability< 1% pulse-to-pulse 4)
Pulse front tilt< 10% of pulse duration< 10% of pulse duration< 10% of pulse duration< 10% of pulse duration
Pulse front tilt< 10% of pulse duration
Pulse contrast< 1 : 20< 1 : 20< 1 : 20< 1 : 20
Pulse contrast< 1 : 20
Beam quality, M2< 1.3 5)< 1.3 5)< 1.3 5)< 1.3 5)
Beam quality, M2< 1.3 5)
Beam astigmatism< 0.15 6)< 0.15 6)< 0.15 6)< 0.15 6)
Beam astigmatism< 0.15 6)
Beam spatial profileGaussian – Super GaussianGaussian – Super GaussianGaussian – Super GaussianGaussian – Super Gaussian
Beam spatial profileGaussian – Super Gaussian
Intensity modulation< 15%, no hotspots 7)< 15%, no hotspots 7)< 15%, no hotspots 7)< 15%, no hotspots 7)
Intensity modulation< 15%, no hotspots 7)
Beam pointing stability< 10 μrad 8)< 10 μrad 8)< 10 μrad 8)< 10 μrad 8)
Beam pointing stability< 10 μrad 8)
Beam divergence< 1.2 × diffraction limit< 1.2 × diffraction limit< 1.2 × diffraction limit< 1.2 × diffraction limit
Beam divergence< 1.2 × diffraction limit
Beam height from the optical table125 – 185 mm 125 – 185 mm 125 – 185 mm 125 – 185 mm 
Beam height from the optical table125 – 185 mm 
Beam diameter, 1/e2< 13.5 mm 9) 10)< 13.5 mm 9) 10)< 19 mm 9) 10)< 19 mm 9) 10)
Beam diameter, 1/e2< 13.5 mm 9) 10)< 19 mm 9) 10)
ModelTOPAS-PRIME‑HETOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUSTOPAS‑PRIME-HE‑PLUS
ModelTOPAS-PRIME‑HETOPAS‑PRIME-HE‑PLUS
  1. The maximum repetition rate for DFG1 (NDFG1) option is 1 kHz.
  2. Contact sales@lightcon.com for higher pump power options.
  3. Normalized to average pulse energy. Expressed as normalized root mean squared deviation (NRMSD).
  4. Normalized to average pulse duration. Expressed as NRMSD.
  5. M2 specification valid for Gaussian beam.
  6. Normalized astigmatism – difference of the waist positions, divided by Rayleigh length.
  7. Normalized to Gaussian or Super-Gaussian fits. Expressed as NRMSD.
  8. Expressed as NRMSD, full angle.
  9. An optional external telescope can be ordered for a beam size of < 39 mm, 1/e2 (69 mm clear aperture mirrors).
  10. A limitation on the minimum beam diameter applies. The minimum beam diameter depends on pulse duration and energy.  
Output
ModelTOPAS-PRIME-HETOPAS-PRIME-HE-PLUS
Tuning range (Signal and Idler combined)1160 – 2600 nm1160 – 2600 nm
Tuning range (Signal and Idler combined)1160 – 2600 nm
Conversion efficiency at peak (Signal and Idler combined)> 30%> 30%
Conversion efficiency at peak (Signal and Idler combined)> 30%
Pulse duration(0.7 – 1) × pump pulse(0.7 – 1) × pump pulse
Pulse duration(0.7 – 1) × pump pulse
Time-bandwidth product< 1< 1
Time-bandwidth product< 1
PolarizationVertical (Signal)
Horizontal (Idler)		Vertical (Signal)
Horizontal (Idler)
PolarizationVertical (Signal)
Horizontal (Idler)
Pulse-to-pulse energy stability< 2% RMS deviation 1) @ 1160 – 1550 nm< 2% RMS deviation 1) @ 1160 – 1550 nm
Pulse-to-pulse energy stability< 2% RMS deviation 1) @ 1160 – 1550 nm
ModelTOPAS-PRIME-HETOPAS-PRIME-HE-PLUS
  1. Normalized to average pulse energy. Expressed as NRMSD.
VIS–UV–DUV extensions (189 – 1160 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
ControlManual change of wavelength separatorsManual change of wavelength separators
ControlManual change of wavelength separators
Maximum tuning range189 – 1160 nm240 – 1160 nm
HousingMonolithic housingMonolithic housing
HousingMonolithic housing
Number of output portsFour 1)Six 1)
Available with TOPAS-PRIME-HETOPAS‑PRIME-HE‑PLUS
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
  1. Output ports are wavelength-dependent.
VIS extensions (475 – 1160 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
SHI (800 – 1160 nm)
Tuning range800 – 1160 nm800 – 1160 nm
Tuning range800 – 1160 nm
Conversion efficiency at peak> 5% 1)> 5% 1)
Conversion efficiency at peak> 5% 1)
Pulse duration(0.7 – 1)× pump pulse duration(0.7 – 1)× pump pulse duration
Pulse duration(0.7 – 1)× pump pulse duration
PolarizationVerticalVertical
PolarizationVertical
SHS (580 – 800 nm)
SFI (533 – 600 nm)
SFS (475 – 533 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
  1. > 4% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  2. > 11% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  3. > 6% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  4. > 8% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
UV extensions (240 – 480 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
FHI (400 – 480 nm)
Tuning range400 – 480 nm400 – 480 nm
Tuning range400 – 480 nm
Conversion efficiency at peak> 1% 1)> 1% 1)
Conversion efficiency at peak> 1% 1)
Pulse duration(0.7 – 1) × pump pulse duration(0.7 – 1) × pump pulse duration
Pulse duration(0.7 – 1) × pump pulse duration
PolarizationHorizontalHorizontal
PolarizationHorizontal
FHS (290 – 400 nm)
SH of SFI (266 – 295 nm)
SH of SFS (240 – 266 nm)
ExtensionNIRUVIS-HE-(DUV)NIRUVIS-GE
  1. > 1% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  2. > 2% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  3. > 0.4% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
  4. > 0.5% at peak when equipped with DUV, due to additional pump pulse energy into the DUV option.
DUV extensions (189 – 240 nm)
ExtensionNIRUVIS-HE-DUVNIRUVIS-HE-DUVNIRUVIS-HE-DUV
ExtensionNIRUVIS-HE-DUV
Pump + FHSPump + SH of SFIPump + SH of SFS
Tuning range215 – 240 nm200 – 215 nm189 – 200 nm
Conversion efficiency at peak> 0.5% 1)Not specifiedNot specified
Conversion efficiency at peak> 0.5% 1)Not specified
PolarizationVerticalVerticalVertical
PolarizationVertical
ExtensionNIRUVIS-HE-DUVNIRUVIS-HE-DUVNIRUVIS-HE-DUV
ExtensionNIRUVIS-HE-DUV
  1. Assuming 15% of the pump pulse energy is allocated to the DUV channel and another 15% to the fresh pump channel.
DFG extensions (2600 – 20000 nm)
ExtensionNDFG1W 1) 2)NDFG1KNDFG2 3)
Tuning range2.6 – 11 μm2.6 – 4.9 μm4 – 20 μm
Conversion efficiency at peak> 1.5%> 1.5%> 0.6%
Pulse duration< 2 × pump pulse duration< 2 × pump pulse durationNot specified
Pulse duration< 2 × pump pulse durationNot specified
PolarizationHorizontalHorizontalHorizontal
PolarizationHorizontal
ExtensionNDFG1W 1) 2)NDFG1KNDFG2 3)
  1. The maximum pump repetition rate is 1 kHz; the crystal lifetime of 1000 – 2000 h.
  2. Not available with TOPAS‑HE-PRIME-PLUS.
  3. Extended lead time for TOPAS‑HE-PRIME-PLUS.
Picosecond (1–4 ps)

Contact sales@lightcon.com for specifications.

Performance
TOPAS-PRIME-HE tuning curves.

TOPAS-PRIME-HE tuning curves.

Pump: 22 mJ, 45 fs, 805 nm.

CEP Stabilization of Idler

The Idler of TOPAS (1600 – 2600 nm) is passively carrier-envelope phase (CEP) locked due to the three-wave interaction process. However, a slow CEP drift may occur as a result of pump beam pointing fluctuations or changes in environmental conditions. This drift can be compensated by employing an f-2f interferometer combined with a feedback loop, which controls the temporal delay between seed and pump in the power amplification stage of TOPAS-PRIME and TOPAS-PRIME-HE.

CEP stability of Idler over 14 min

TOPAS-PRIME CEP stability of the Idler over 14 minutes without drift compensation.

CEP stability of Idler over 14 min

TOPAS-PRIME CEP stability of the Idler over 14 minutes with drift compensation using a slow loop.

Drawings
TOPAS-PRIME-HE High Energy Optical Parametric Amplifier.

TOPAS-PRIME-HE High Energy Optical Parametric Amplifier.

TOPAS-PRIME-HE High Energy Optical Parametric Amplifier (rear view)

TOPAS-PRIME-HE High Energy Optical Parametric Amplifier (rear view).

TOPAS-PRIME-HE drawing

TOPAS-PRIME-HE drawing.

Publications
Nonlinear optics PHAROS TOPAS-PRIME-HE ORPHEUS-TWINS
Unzipping hBN with ultrashort mid-infrared pulses
C. Y. Chen, S. L. Moore, R. Maiti, J. S. Ginsberg, M. M. Jadidi et al.
Science Advances • 2024
Nonlinear microscopy TOPAS-PRIME-HE
Phonon-enhanced nonlinearities in hexagonal boron nitride
J. S. Ginsberg, M. M. Jadidi, J. Zhang, C. Y. Chen, N. Tancogne‑Dejean et al.
Nature Communications • 2023
Nonlinear optics TOPAS-PRIME-HE
Energy scaling of carrier-envelope-phase-stable sub-two-cycle pulses at 1.76 µm from hollow-core-fiber compression to 1.9 mJ
K. S. Zinchenko, F. Ardana‑Lamas, V. U. Lanfaloni, Y. Pertot, T. T. Luu et al.
Optics Express • 2022
Photoemission spectroscopy TOPAS-PRIME-HE
Direct evidence for efficient ultrafast charge separation in epitaxial WS 2 /graphene heterostructures
S. Aeschlimann, A. Rossi, M. Chávez‑Cervantes, R. Krause, B. Arnoldi et al.
Science Advances • 2020
Nonlinear optics Laser pumping and seeding X-ray generation TOPAS-PRIME-HE
Femtosecond Optical Laser System with Spatiotemporal Stabilization for Pump-Probe Experiments at SACLA
T. Togashi, S. Owada, Y. Kubota, K. Sueda, T. Katayama et al.
Applied Sciences • 2020
X-ray generation TOPAS-PRIME-HE
Taking a snapshot of the triplet excited state of an OLED organometallic luminophore using X-rays
G. Smolentsev, C. J. Milne, A. Guda, K. Haldrup, J. Szlachetko et al.
Nature Communications • 2020
High harmonic generation TOPAS-PRIME-HE
High-harmonic generation from an epsilon-near-zero material
Y. Yang, J. Lu, A. Manjavacas, T. S. Luk, H. Liu et al.
Nature Physics • 2019
High harmonic generation TOPAS-PRIME-HE
Extreme–ultraviolet high–harmonic generation in liquids
T. T. Luu, Z. Yin, A. Jain, T. Gaumnitz, Y. Pertot et al.
Nature Communications • 2018
High harmonic generation TOPAS-PRIME-HE
Interferometry of dipole phase in high harmonics from solids
J. Lu, E. F. Cunningham, Y. S. You, D. A. Reis, and S. Ghimire
Nature Photonics • 2018
Pulse characterization Volume modification TIPA TOPAS-PRIME-HE
Crossing the threshold of ultrafast laser writing in bulk silicon
M. Chanal, V. Y. Fedorov, M. Chambonneau, R. Clady, S. Tzortzakis et al.
Nature Communications • 2017
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TOPAS Optical Parametric Amplifiers for Ti:Sapphire Lasers

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Femtosecond Laser Systems for Industry & Science

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飞秒激光器飞秒科研系统

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Overview
Ultrafast (20–70 fs)
Fast (70–200 fs)
Picosecond (1–4 ps)
Performance
Drawings
Publications
Downloads
Overview