
iScan – Mode and Frequency Control
- For laser mode monitoring and frequency control
- Fast and precise scanning of tunable lasers
- Scan linearization, stabilization to any wavelength
- Static and dynamic mode surveillance
- Patented interferometer design (US 6,178,002)
The iScan comprises a patented interferometer for fast and precise frequency control of tunable lasers. The laser frequency can be scanned in a precisely linear or step-wise manner. The laser can also be stabilized to any value within its tuning range, including “off-resonant” values where no atomic or molecular transition is available. Applications include laser cooling, interferometry, LIDAR seeding, and cw terahertz experiments.
Technical Information
Technical Information
| Concept | Quadrature signal generation in a low-finesse etalon. Stand-alone interferometer head + 19” control electronics. |
|---|---|
| Input wavelength range | 400 – 1100 nm (standard version) 1100 – 1700 nm (IR version) |
| Input coupling | SM/PM fiber |
| Input power | Min. 20 .. 100 µW, wavelength dependent |
| Interferometer free spectral range | 8 GHz typ., other FSRs on request |
| Scan linearity (absolute) | 100 MHz typ., higher linearity on request |
| Scan resolution (relative) | 1 MHz typ., higher resolution on request |
| Scan speed (typ.) | 50 GHz / s (DFB lasers) |
| Long-term stability | < 20 MHz @ 3 hrs, laboratory environment |
| Error signal bandwidth | Up to 1 MHz |
| Arbitrary wavelength locking | Possible, resolution typ. 1 MHz, no grid |
| External control | PC, USB 2.0 interface |
| Software | Visual Basic sample program included |
| Operating temperature | 15 – 30° C |
| Electronics | 19” control rack |
| Operating voltage | 100..120 V / 220..240 V AC, 50..60 Hz (auto detect) |
| Suitability | Diode / fiber / dye / solid state lasers |
Design of the optical interferometer within the iScan head. A wedge-shaped beam splitter in the head generates two low intensity probe beams (PBA and PBB), which enter the etalon under slightly different angles. The etalon produces a pair of interference signals with a relative phase of π/4 (90°). These signals are detected by two photodiodes (a and b) and combined into a quadrature signal, the phase of which is a linear function of the optical frequency. Two additional photodiodes (Ia and Ib) behind the etalon provide normalization values.
Quadrature signals and mode signatures. When the laser frequency is scanned, each of the photodiodes a and b detects an oscillating, near-sinusoidal signal. An XY-display on an oscilloscope screen yields a circle, where the momentary phase angle represents the laser frequency. The completed circumference of the circle corresponds to the range of the frequency scan. A full circle equals a frequency shift of one FSR of the interferometer. The radius additionally reveals information on the mode properties of the laser. A mode-hop free scan yields a smooth curve, whereas a mode-hop within the scan range is recognized by a sudden jump across the circle.
Options & Related Products
Options & Related Products
- IR version with InGaAs photodetectors
- Customized free spectral range of etalon
- Twin iScan: Two measurement heads with a single control unit
Related Products:
| PID 110 | LIR 110 | PDD 110 | FALC 110 | DigiLock 110 | LaseLock | Wavelength Meter | Iscan | |
|---|---|---|---|---|---|---|---|---|
| Description / type | Analog PID | Analog Lock-In Regulator | Pound-Drever- Hall Signal Generation | Fast Analog 2-Channel PID | Versatile Digital Locking Solution | Suited for third party lasers | Wavelength meter with PID option | Low finesse etalons as reference with Lock-Electronics |
| Side-of-fringe | • | • | • | • | Not applicable | |||
| Top-of-fringe | With PDD | • | • | With PDD | • | • | ||
| Locking bandwidth* | kHz .. MHz | kHz range | ≈ 45 MHz | ≈ 10 MHz | 1 MHz | < 100 Hz | kHz range | |
| Modulation frequency | 0.6 Hz .. 14 kHz | 20 MHz ** | 17 Hz .. 25 MHz | 33 Hz .. 1 MHz | Not applicable | |||
| Accuracy | Depends on reference (can be very good) | > 10 MHz | 1 MHz (relative) | |||||
| Signal analysis | • | |||||||
| Relock mechanisms | • | • | • | • | • | |||
| Computer control | • | • | • | |||||
| High voltage output | • | • | • | • | ||||
| High bandwidth output | • | • | ||||||
| Two channel version | • | |||||||
| SYS DC 110 module | • | • | • | • | • | |||
| Stand-alone | • | • | • | |||||
| Catalog page | 35 | 36 | 36 | 35 | 37 | 40 | 55 | 42 |
| low budget | high end & preferrable | |||||||
*Estimated bandwidth depends on gain and PID settings **5- 40 MHz versions available
- Tunable diode lasers: DL pro, DL 100 / pro design, DL DFB, DL 100
- High power lasers: TA pro, DLX
- Frequency-converted lasers: DL SHG pro, TA SHG pro, TA FHG pro
- Laser packages for cw terahertz generation
Technical Drawings
Applications
Applications
Water absorption spectrum, recorded with a tunable diode laser with iScan frequency control. Left: 37 GHz scan across two absorption lines. Right: Frequency stepping. After the linear scan, the frequency is tuned in four discrete steps to the first resonance, an “off-line” value, the second resonance and the start of the scan ramp, respectively.
Linear 1200 GHz frequency scan of a DL DFB laser with iScan frequency control.
The iScan lends itself to
- Frequency control of semiconductor lasers, fiber lasers, solid state lasers, dye lasers
- Optimization of laser tuning parameters
- Long-term aging control
- LIDAR seeding
- Phase-shifting interferomtery
- Precision spectroscopy in frequency-domain terahertz applications
Application Notes
Download
Download
toptica_ScPaper_Sci_Instr_2008.pdf



