Inspire Femtosecond OPO

- Gap-free tuning across the UV, Visible and IR [345 – 2500 nm (4000 – 28985 cm-1)] with a single configuration and without any change of optics.
- Fully-automated computer-controlled tuning and self-calibration.
- Simultaneous UV, Visible and IR beams available through 3 separate output ports.
- Integrated Second Harmonic Generation Unit for doubling the un-depleted pump.
- Ultrashort Pulses (typ. 180 fs) at 80 MHz.

A fully-automated femtosecond optical parametric oscillator (OPO) that offers gap-free wavelength coverage across the UV, Visible and IR with no change of optics or crystals and just one single configuration. The InspireTM advanced control software ensures fast and reliable tuning while providing a selection of practical operating features.
The Inspire is a femtosecond OPO, pumped by a mode-locked Ti:Sapphire oscillator, which offers the broadest tunability in the UV, Visible and IR, across 345 – 2500 nm. Four separate output ports emitting the doubled pump [345 – 540 nm (18518 – 28985 cm-1)], signal [490 – 750 nm (13333 – 20408 cm-1)], depleted-pump [680 – 1080 nm (9259 – 14705 cm-1)], and idler [930 – 2500 nm (4000 – 10752 cm-1)] are available. Selection between the simultaneous signal and idler outputs (tunable across the range at a fixed pump wavelength), or the simultaneous doubled and depleted-pump outputs (tunable across the range while tuning the pump laser) is straightforward and can be achieved via the dedicated PC-user-interface. The depleted-pump output at a fixed wavelength is also simultaneously available with the signal and idler outputs.
The doubled and depleted-pump outputs are generated using the state-of-the-art second-harmonic generator incorporated inside the OPO. This doubles the frequency of the pump laser, providing broad wavelength coverage [345-540 nm (18518 – 28985 cm-1)], high conversion efficiency (up to 45 %), reduced pulse broadening (<180 fs) and excellent beam quality (Tem00).
Near-transform-limited pulses are offered thanks to the specially-designed dispersion compensation module which enables dynamic and independent control of the dispersion for every signal wavelength. The Inspire operates at room temperature, and as a result avoids the need for ovens, water-cooling units and pipes inside the OPO cavity. The Inspire is a USB compatible and compact system consisting on a single optics unit (954 x 360 x 230 mm), which does not require additional bulky external units such as chillers or MRU air re-circulators. A portable and ready installed computer is also available with this OPO.
The superior performance of the Inspire is strengthened by its unique automation features that offer high simplicity of use. Additional to fully-automated tuning, self-calibration is also available via the dedicated PC-user-interface and provides automatic alignment optimization of the OPO cavity. This increases the OPO operation repeatability without the need for manual alignment and enhances the overall usability of the system. The control software also incorporates useful information and a graphical display of the spectral profile of the emitted pulses, recorded with the integrated spectrometer.
The Inspire can be pumped by both the Mai Tai® HP and the Tsunami® Ti:sapphire oscillators from Spectra Physics, and delivers high power in the UV and Visible. This is an ideal tool for sophisticated scientific applications such as time-resolved microscopy and multiple wavelength pump-probe experiments, where short pulses, broad wavelength coverage and hands-free operation are required.
A selection of Inspire The Inspire is distributed exclusively via Spectra Physics worldwide.
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Inspire HF 100
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Inspire Auto 100
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Inspire HF 50
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Inspire Auto 50
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Tuning range
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Tuning range
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Tuning range
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Tuning range
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Signal wavelength: 490 – 750 nm
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Signal wavelength: 490 – 750 nm
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Signal wavelength: 490 – 750 nm
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Signal wavelength: 490 – 750 nm
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Idler wavelength: 990 – 2500 nm
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Idler wavelength: 990 – 2500 nm
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Idler wavelength: 990 – 2500 nm
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Idler wavelength: 990 – 2500 nm
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Pump wavelength: 690 – 1040 nm
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Pump wavelength: 690 – 1040 nm
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Pump wavelength: 690 – 1040 nm
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Pump wavelength: 690 – 1040 nm
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SHG wavelength: 345 – 520 nm
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SHG wavelength: 345 – 520 nm
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SHG wavelength: n/a
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SHG wavelength: n/a
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Average power
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Average power
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Average power
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Average power
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Signal average power: 350 mW
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Signal average power: 350 mW
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Signal average power: 350 mW
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Signal average power: 350 mW
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Idler average power: 170 mW
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Idler average power: 170 mW
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Idler average power: 170 mW
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Idler average power: 170 mW
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Pump average power: 1100 mW
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Pump average power: 1100 mW
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Pump average power: 1100 mW
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Pump average power: 1100 mW
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SHG average power: 1100 mW
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SHG average power: 1100 mW
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SHG average power: n/a
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SHG average power: n/a
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Pulse duration: Femtosecond
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Pulse duration: Femtosecond
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Pulse duration: Femtosecond
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Pulse duration: Femtosecond
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Integrated pump: No
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Integrated pump: No
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Integrated pump: No
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Integrated pump: No
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| Output Characteristics(2) | Inspire Auto 50 | Inspire Auto 100 | Inspire Hand Free 50 | Inspire Hand Free 100 |
| Average Power |
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| SHG @ 400 nm (25000 cm-1) | n/a | 1100 mW | n/a | 1100 mW |
| Signal @ 550 nm (18181 cm-1) | 350 mW | 350 mW | 350 mW | 350 mW |
| Depleted Fundamental @ 800 nm (12500 cm-1) | 1100 mW | 1100 mW | 1100 mW | 1100 mW |
| Idler (at peak) | 170 mW | 170 mW | 170 mW | 170 mW |
| Pulse Width | ||||
| SHG | n/a | <140 fs | n/a | <140 fs |
| Signal | 100–250 fs (adjustable) | 100–250 fs (adjustable) | 200 fs | 200 fs |
| Depleted Fundamental | <140 fs | <140 fs | <140 fs | <140 fs |
| Idler | 80–250 fs (adjustable) | 80–250 fs (adjustable) | 200 fs | 200 fs |
| Tuning Range | ||||
| SHG | n/a | 345–520 nm (19230 – 28985 cm-1) | n/a | 345–520 nm (19230 – 28985 cm-1) |
| Signal (Simultaneous with Idler) | 490 – 750 nm (13333 – 20408 cm-1) | 490 – 750 nm (13333 – 20408 cm-1) | 490 – 750 nm (13333 – 20408 cm-1) | 490 – 750 nm (13333 – 20408 cm-1) |
| Depleted Fundamental | 690 – 1040 nm (9615 – 14492 cm-1) | 690 – 1040 nm (9615 – 14492 cm-1) | 690 – 1040 nm (9615 – 14492 cm-1) | 690 – 1040 nm (9615 – 14492 cm-1) |
| Idler (Simultaneous with Signal) | 930 – 2500 nm (4000 – 10752 cm-1) | 930 – 2500 nm (4000 – 10752 cm-1) | 930 – 2500 nm (4000 – 10752 cm-1) | 930 – 2500 nm (4000 – 10752 cm-1) |
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| Repetition Rate | 80 MHz | 80 MHz | 80 MHz | 80 MHz |
| Noise | <1% rms | <1% rms | <1% rms | <1% rms |
| Wavelength Stability @ 555 nm | <0.5 nm | <0.5 nm | <0.5 nm | <0.5 nm |
| Polarization | Horizontal for Signal and Idler, Vertical for SHG | Horizontal for Signal and Idler, Vertical for SHG | Horizontal for Signal and Idler, Vertical for SHG | Horizontal for Signal and Idler, Vertical for SHG |
| Spectrometer for UV and Visible Range(3) | 350–900 nm (11111 – 28571 cm-1) (integrated into optics unit) | 350–900 nm (11111 – 28571 cm-1) (integrated into optics unit) | 350–900 nm (11111 – 28571 cm-1) (integrated into optics unit) | 350–900 nm (11111 – 28571 cm-1) (integrated into optics unit) |
| Dimensions (W x L x H)(4) | 14.2 x 37.6 x 9.1 in (36.0 x 95.4 x 23.2 cm) | 14.2 x 37.6 x 9.1 in (36.0 x 95.4 x 23.2 cm) | 14.2 x 37.6 x 9.1 in (36.0 x 95.4 x 23.2 cm) | 14.2 x 37.6 x 9.1 in (36.0 x 95.4 x 23.2 cm) |
Note:
(1) Specifications are subject to change without notice.
(2) Pumped by Mai Tai® HP Ti:sapphire oscillators, 2.8W, 100fs, 820nm. Output characteristics for alternative pump lasers, such as TsunamiTM are available upon request.
(3) IR spectral region available upon request.
(4) PC controllable. No control electronics unit required.
Inspire Typical Tuning Curve

Inspire Wavelenght Coverage

Advanced Photonics
- A tunable transition metal dichalcogenide entangled photon-pair source, Nature Comm. 2024.
- Fast optoelectronic charge state conversion of silicon vacancies in diamond, Science 2024.
- Enhanced Nonlinearity of Epsilon-Near-Zero Indium Tin Oxide Nanolayers with Tamm Plasmon-Polariton States, ArXiv 2023.
- Three-Photon Excitation of InGaN Quantum Dots, Physical Review Letters 2022.
- Consistent pattern printing of the gap structure in femtosecond laser DMD projection lithography, Optics Express 2022.
- Structure-dependent optical nonlinearity of indium tin oxide, Applied Physics Letters 2022.
- Subwavelength-scalelasingperovskitewith ultrahighPurcellenhancement, Matter 2021.
- Li@C60 thin films: characterization and nonlinear optical properties, RSC Advances 2021.
- Ultrafast Electron Cooling and Decay in Monolayer WS2 Revealed by Time- and Energy-Resolved Photoemission Electron Microscopy, NanoLetters 2020.
- Quantum electrodynamics at room temperature coupling a single vibrating molecule with a plasmonic nanocavity, Nature Comm. 2019.
- Chiral selection rules for multi-photon processes in two dimensional honeycomb materials, Optica 2019.
- Impact of environment on dynamics of exciton complexes in a WS2 monolayer, 2D Materials 2018.
- Pulsed Molecular Optomechanics in Plasmonic Nanocavities: From Nonlinear Vibrational Instabilities to Bond-Breaking, Physical Review X 2017.
- Background-Free 3D Nanometric Localization and Sub-nm Asymmetry Detection of Single Plasmonic Nanoparticles by Four-Wave Mixing Interferometry with Optical Vortices, Physical Review X 2017.
- Structural phase transition in monolayer MoTe2 driven by electrostatic doping, Nature 2017.
- Nonlinear optical selection rule based on valley-exciton locking in monolayer WS2, Nature 2015.
- Enhanced photoluminescence of Si nanocrystals-doped cellulose nanofibers by plasmonic light scattering, Applied Physics Letters 2015.
Laser Spectroscopy
- Impact of Cooperativity on the Spatial and Temporal Evolution of the Light-induced Spin-State Switching of the Fe(phen)2(SCN)2 Spin-Crossover Complex, ArXiv 2025.
- Picosecond transfer from short-term to long-term memory in analog antiferromagnetic memory device, ArXiv 2025.
- Quantitative measurement of graphitic sp2 on single nanodiamonds with sub-monolayer sensitivity using differential interference contrast and photo-thermal microscopy, Carbon 2024.
- Accelerated molecular vibrational decay and suppressed electronic nonlinearities in plasmonic cavities through coherent Raman scattering, Physical Review B 2024.
- A tunable transition metal dichalcogenide entangled photon-pair source, Nature Comm. 2024.
- Femtosecond laser-induced fluorescence spectroscopy for the rapid detection of pathogenic bacteria, Optical and Quantum Electronics 2024.
- Chirality conferral enables the observation of hyper-Raman optical activity, Nature Photonics 2024.
- Spatially inhomogeneous inverse Faraday effect provides tunable nonthermal excitation of exchange dominated spin waves, Nanophotonics 2024.
- Nonlinear dispersion relation and out-of-plane second harmonic generation in MoSSe and WSSe Janus monolayers, Advanced Optical Materials 2023.
- Giant optomechanical spring effect in plasmonic nano- and picocavities probed by surface-enhanced Raman scattering, Nature Comm. 2023.
- Near-field terahertz nonlinear optics with blue light, Light: Science & Applications 2023.
- Semitransparent Organic Photovoltaics Utilizing Intrinsic Charge Generation in Non-Fullerene Acceptors, Advanced Materials. 2023.
- Photocyclization reaction and related photodynamics in the photoproducts of a tetraphenylethylene derivative with bulky substituents: unexpected solvent viscosity effect, PCCP 2023.
- Interrogating the Behaviour of a Styryl Dye Interacting with a Mesoscopic 2D-MOF and Its Luminescent Vapochromic Sensing, International Journal of Molecular Sciences 2022.
- Anomalous deep-red luminescence of perylene black analogues with strong π-π interactions, Nature Comm. 2022.
- Three-Photon Excitation of InGaN Quantum Dots, Physical Review Letters 2022.
- Structure-dependent optical nonlinearity of indium tin oxide, Applied Physics Letters 2022.
- Photophysics of Defect-Passivated Quasi-2D (PEA)2PbBr4 Perovskite Using an Organic Small Molecule, ACS Energy Letters 2022.
- Ultraviolet/Visible Quasicylindrical Waves on Semimetal Cd3As2 Nanoplates, Advanced Photonics Materials 2022.
- Coherent dynamics of a single Mn-doped quantum dot revealed by four-wave mixing, ArXiv 2022.
- Subwavelength-scale lasing perovskite with ultrahigh Purcell enhancement, Matter 2021.
- Optical Activity in Third-Harmonic Rayleigh Scattering: A NewRoute for Measuring Chirality, Laser and Photonics Reviews 2021.
- Intrinsic efficiency limits in low-bandgap non-fullerene acceptor organic solar cells, Nature Materials. 2021.
- Two-Photon-Induced [2 + 2] Cycloaddition of Bis-thymines, ACS omega 2020.
- Ultrafast and Long-Range Exciton Migration through Anisotropic Coulombic Coupling in the Textured Films of Fused-Ring Electron Acceptors, J. Phys. Chem. Lett. 2020.
- Relaxation and transfer of photoexcited electrons at a coplanar few-layer 1T′/2H-MoTe2 heterojunction, Nature Communications Materials 2020.
- Ultrafast Electron Cooling and Decay in Monolayer WS2 Revealed by Time- and Energy-Resolved Photoemission Electron Microscopy, NanoLetters 2020.
- Enhancing the Charge Extraction and Stability of Perovskite Solar Cells Using Strontium Titanate (SrTiO3) Electron Transport Layer, ACS Applied Energy Materials 2019.
- Quantum electrodynamics at room temperature coupling a single vibrating molecule with a plasmonic nanocavity, Nature Comm. 2019.
- Giant peak of the Inverse Faraday effect in the band gap of magnetophotonic microcavity, Nature 2018.
- Heterodyne dual-polarization epi-detected CARS microscopy for chemical and topographic imaging of interfaces, APL Photonics 2018.
- Impact of environment on dynamics of exciton complexes in a WS2 monolayer, 2D Materials 2018.
- Pulsed Molecular Optomechanics in Plasmonic Nanocavities: From Nonlinear Vibrational Instabilities to Bond-Breaking, Physical Review X 2017.
- Ultrafast fluorescent decay induced by metal-mediated dipole–dipole interaction in two-dimensional molecular aggregates, PNAS 2017.
- Antireflective photonic structure for coherent nonlinear spectroscopy of single magnetic quantum dots, Crystal Growth & Design 2017.
- Conformational Coupling across the Plasma Membrane in Activation of the EGF Receptor, Cell 2016.
- Ultrafast pump-probe photo-induced force microscopy at nanoscale, Appl. Phys. Lett. 2015.
- Nonlinear optical selection rule based on valley-exciton locking in monolayer WS2, Nature 2015.
- Probing excitonic dark states in single-layer tungsten disulphide, Nature 2014.
Microscopy
- Erbium doping of lithium niobate on insulator using low-temperature ion exchange, Optical Materials Express 2024.
- Second harmonic generation in monolithic gallium phosphide metasurfaces, Nanophotonics 2024.
- Front-contact passivation through 2D/3D perovskite heterojunctions enables efficient bifacial perovskite/silicon tandem solar cells, Matter 2023.
- Spatially engineered nonlinearity in resonant metasurfaces, Optica Photonics Research 2023.
- Correlative light-electron microscopy using small gold nanoparticles as single probes, Light Sci. Appl. 2023.
- Revealing low-loss dielectric near-field modes of hexagonal boron nitride by photoemission electron microscopy, Nature Comm. 2023.
- Near-field terahertz nonlinear optics with blue light, Light: Science & Applications 2023.
- Simultaneous microscopic imaging of thickness and refractive index of thin layers by heterodyne interferometric reflectometry (HiRef), ArXiv 2021.
- Visible-wavelength two-photon excitation microscopy with multifocus scanning for volumetric live-cell imaging, Journal of Biomedical Optics 2020.
- Ultrafast Electron Cooling and Decay in Monolayer WS2 Revealed by Time- and Energy-Resolved Photoemission Electron Microscopy, NanoLetters 2020.
- Preserving the Emission Lifetime and Efficiency of a Monolayer Semiconductor upon Transfer, Advanced Optical Materials 2019.
- Background-Free 3D Nanometric Localization and Sub-nm Asymmetry Detection of Single Plasmonic Nanoparticles by Four-Wave Mixing Interferometry with Optical Vortices, Physical Review X 2017.
Quantum Technology
- A tunable transition metal dichalcogenide entangled photon-pair source, Nature Comm. 2024.
- Spatio-Spectral Quantum State Estimation of Photon Pairs from Optical Fiber Using Stimulated Emission, ArXiv 2024.
Optical Communication
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ZENITH Picosecond OPOAreas:
Advanced Photonics, Laser Spectroscopy, Microscopy
Tuning range
signal-wavelength: 1387 - 2020 nm
idler-wavelength: 2100 - 4000 nm
pump-wavelength: 1030 nm
shg-wavelength: n/a
Average power
signal-average-power: >4 W
idler-average-power: >2 W
pump-average-power: n/a
shg-average-power: n/a
pulse-duration: Picosecond
integrated-pump: Yes
View more -
ORIA IR Femtosecond OPOAreas:
Advanced Photonics, Laser Spectroscopy, Microscopy, Optical Communications, Quantum Technology
Tuning range
signal-wavelength: 1000 - 1580 nm.
idler-wavelength: 1696 - 4090 nm
pump-wavelength: 690 - 1040 nm
shg-wavelength: n/a
Average power
signal-average-power: >1 W
idler-average-power: >350 mW
pump-average-power: n/a
shg-average-power: n/a
pulse-duration: Femtosecond
integrated-pump: No
View more -
Titan CW Broadly Tunable LaserAreas:
Advanced Photonics, Laser Spectroscopy, Quantum Technology
Tuning range
signal-wavelength: 1435 - 2000 nm
idler-wavelength: 2270 - 4138 nm
pump-wavelength: n/a
shg-wavelength: n/a
Average power
signal-average-power: >2.5 W
idler-average-power: >4 W
pump-average-power: n/a
shg-average-power: n/a
pulse-duration: Continuos-Wave
integrated-pump: Yes
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