Laser Pulse Characterization with Spectral Phase Interferometry for Direct Electric-field Reconstruction

Spider Family

Our Spider – Spectral Phase Interferometry for Direct Electric-field Reconstruction – family is designed for phase resolved ultrafast pulse measurements. FC (Few Cycle) Spider offers a precision tool for the complete characterization of ultrashort laser pulses with just a few electric field cycles — down to 5 fs pulse width. LX Spider is a highly compact instrument for the characterization of femtosecond laser pulses in the range of 16 … 200 fs. Spider IR is the best choice for pulses between 30 and 500 fs at 1 µm central wavelength.

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Rita - Working with Compact LX Spider

Spectral Phase Interferometry for Direct Electric-field Reconstruction

Spectral Phase Interferometry for Direct Electric-field Reconstruction (abrev.: SPIDER) is an ultrashort pulse measurement technique. Interference between two pulses allows the spectral phase at one frequency to be referenced to the spectral phase at a different frequency. In the following video, Rita is showing the concept of Spectral phase interferometry for direct electric-field reconstruction on a LX Spider.

Spectral Phase Interferometry for Direct Electric-field Reconstruction

0:19 Hello and welcome to a APE in Berlin in Germany. My name is Rita and over the next few minutes I’m going to show you how easy it is to set up your LX spider pulse measuring system. Like our autocorrelator, LX Spider lets you measure pulse durations with incredible accuracy but what makes it more remarkable is that it also measures the group delay distribution of the pulse of spectral components in a single shot manner. Because of this you can do so much more. You can online you the true shape of the pulse, measure the chirp behavior and access a wealth of additional information: all in real time.

1:00 First you have direct access to the pulse spectrum due to the built-in spectrometer. Second, the spectral phase of the pulse is directly measured. Third the spectral phase is instantly analyzed with regard to dispersive contributions. Next the temporal pulse shape is evaluated in real time by fast Fourier transformation, and finally single laser pulses can be measured at low laser repetition rates.

1:33 Nothing this powerful has ever been so compact and affordable and it’s easy to use. There are no buttons or dolls or even a controller unit. You control everything via one software program. Setup is simple too. But before we begin let me show you how a LX Spider works starting with the alignment.

1:59 Step one: Incoming beam passes through a series of optics to reach the splitting mirror. This splits the beam spatially into two separate beings. These beams are then tilted downward to pass through the non-linear crystal. In alignment mode, a steering mirror reflects both beams into the alignment window. After alignment is complete, LX Spider automatically moves the alignment mirror out of the way. This allows the two beams to strike the focusing mirror.  Then merge the entrance of the spectrometer for sensitive phase measurement.

2:36 For robust measurement of the pulse spectrum a diffuser can be turned into the initial beam  path. Its innovative design allows for a more compact size and full automation. Once you’ve aligned the incoming beam our software does all the work for you.

2:56 First open it by clicking the LX Spider icon in the upper right corner of your screen. You should see a green light next to motors initialized. Then click the alignment button to set LX Spider in alignment mode. Finally make sure the input aperture of LX Spider is fully open. You also need to ensure the beam is correctly pre-aligned. It should run at a constant height above the table – equal to the height of the input aperture. An additional alignment aperture can help you do this.

3:31 Now you can put LX Spider in the beam path. Turn it into place until a double spot appears in the alignment window. You’re looking for two half-moons of equal size and brightness one on each side of the crosshair. When that’s complete, clamp LX Spider to the table to ensure it doesn’t move out of place later on. As a final step optimize the two spots in the alignment window by aligning the near mirror. When you’re finished click the alignment button. This will switch LX Spider out of alignment mode. So it will deliver the two upconverted beams to the spectrometer.

4:09 Now we’re ready to obtain the full information on the pulse. To do this we need two data sets, and the first is the pulse spectrum in the right column. Check the measure spectrum box, then use the exposure slider on the left to increase or decrease detector sensitivity. If you prefer, you can also have LX Spider find the ideal level of sensitivity.  Just press the auto exposure button. When you’re ready press the safe spectrum button followed by confirm. Then uncheck the measure spectrum box. And the interferogram of the fundamental signal should be visible.

5:09 First make sure that auto exposure mode is switched off. To start set the spectral range to second harmonic. Then tune the crystal to the correct wavelength by checking the tune to center of gravity box as an alternative. You can manually enter the center wavelength and press the tune button. Be sure to reset the exposure time if needed. If you need to further optimize the signal you can adjust the focus mirror by using the hex key provided with your LX spider. Here’s how:

5:45 On the right side of LX spider are the two alignment screws for the focusing mirror. Use your hex key to adjust the horizontal and vertical tilt. The adjustment is complete when you’ve  reached the highest intensity and best modulation of the green signal curve.

6:03 The last step is to save the calibration. Again, our software makes it easy. Just activate auto exposure mode and set the spectral range to fundamental. Press the safe calibration button and when you’re asked to replace the spectrum choose “no”. Then return the spectral range to second harmonic.  LX Spider will immediately show you the pulse in the spectral domain.

6:28 The previously safe pulse spectrum will appear as a white curve and the current reconstruction of the spectral phase will appear as a blue curve. You can evaluate the chirp of the pulse from the curvature of the phase. If you’d like to see the actual temporal pulse shape click the time domain button. A second graph will open the display. The pulse shape at the Fourier limit in green and the actual pulse shape as a white curve.

6:56 The temporal phase is also shown on the right. Characteristic values of the pulses can be monitored such as the pulse duration and the time bandwidth product. And that’s it. Setup is Complete. You’re now ready to start taking real-time measurements.

This is from the transcript of Spectral Phase Interferometry for Direct Electric-field Reconstruction.

Software Features

Important software features for advanced pulse characterization are provided with all APE Spiders. If desired, a PC or notebook with pre-installed software will be delivered together with the instrument.

Spider IR & FC Spider Software Features

  • Spectral and temporal reconstruction based on Spectral Phase Interferometry for Direct Electric-field Reconstruction
  • Alternative interferogram demodulation methods: Fourier / Wavelet
  • E-field plot
  • Peak power calculation
  • Measurement of phase differences
  • Spectral phase derivation up to fourth order
  • Simulation of additional theoretical dispersion (GDD, TOD, FOD)
  • Spectrogram (X-FROG, SHG-FROG) and Wigner trace representation of the pulse

A comparison of Spectral Phase Interferometry for Direct Electric-field Reconstruction (Spider) with Frequency-resolved Optical Gating (FROG).

In comparison with other pulse characterization methods, Spider offers some differences. The following table gives some aspects that could be considered.


  • Relatively complex setup
  • Direct measurement in the spectral domain (amplitude and phase)
  • Intrinsically single shot
  • Insensitive to intensity noise
  • Fast and direct reconstruction mathematics
  • Unambiguous in the sign of the chirp and time
  • Different parameter ranges often require an optimized single-setup


  • Relatively simple optical setup
  • Direct sampling in the time domain possible
  • Highly variable for different parameter ranges (pulse duration, wavelength)
  • Iterative fitting algorithm may make data interpretation more complex
  • Measure spectrally broadband pulses in single shot mode often not possible

The Spider Family made by APE

Compact LX Spider

The Ti:Sa Expert | 16 - 300 fs

Compact LX Spider is the Ideal for the Wavelength Range of 750 – 900 nm. Therefore, it is the ideal candidate for Ti:Sa laser applications. Two interchangeable Optics Sets are available to cover pulse durations between 16 – 300 fs.

Spider IR

Central Wavelength 1 µm | 30 - 500 fs

Spider IR is best suited for the characterization of Lasers with 1 µm Central Wavelength. It covers relatively small bandwidths, that is longer pulses in the range of  about 30 to 500 fs.

FC Spider

< 5 fs Pulses | Wavelengths for VIS, NIR, IR

The precise characterization of very short pulses down to < 5 fs is available with the FC Spider, whereas FC stands for few cycles. FC Spider is available for different wavelength ranges: VIS, NIR, and IR.

Contact Us


Email & Phone Contacts

APE has distributors around the world to give you the best support. Choose a country to find your local sales contact:

APE Angewandte Physik & Elektronik GmbH
Plauener Strasse 163-165 | Haus N
13053 Berlin, Germany

Tel +49 30 98601130
Fax +49 30 986011333

Sales: sales@ape-berlin.de
Support: service@ape-berlin.de

Coherent Scientific pty. Ltd.
Hilton SA 5033, South Australia

Phone: +61 8 8150 5200
Email: sales@coherent.com.au

Pinnacle Scientific Cooperation
Hangzhou, Jianggan District
China 310020

Phone +86 571 88225151
Email: sales@psci.cn

PulsePower Technology Ltd.
Beijing, Haidan District
China 100090

Phone +86 10 62565117
Email: mlu@pulsepower.cn

199 00 Praha 9, Česko

phone +420 212 247 293
Email: info@optixs.cz

Gammadata Instrument AB
750 02 Uppsala

Tel: +46 18 56 68 35
Email: jenny.lindvall@gammadatainstrument.se

F 92170 Vanves, France

Tel: +33 1 419 061 80
Email: info@optoprim.com

Laser Sciences Services Pvt. Ltd.

Tel: +91 2778 1673
Email: sales@laserscience.in

Photonic Solutions PLC
Edinburgh, UK

Tel: +44 131 664 8122
Email: sales@photonicsolutions.co.uk

Ammo Engineering Ltd.
Petach Tikva 49517, Israel

Tel: +972 3 9239 666
Email: ammo1@ammo.co.il

Optoprim Srl.
20052 Monza, Italy

phone +39 (039) 834977
Email: info@optoprim.it

Phototechnica Corporation
Saitama 336-0017, Japan

Tel: +81 48 871 0067
Email: voc@phototechnica.co.jp

Seoul 137-862, Korea

Tel: +82 2 3461 1103
Email: sales@rayvis.co.kr

Mexico City 03100, Mexico

Tel: 52(55) 5575-0312/0269/9929
Email: sales@mexitek.com

Eurotek International
02-668 Warsaw, Poland

Tel: +48 2284 379 40

Innova Scientific S.L.
28290 Las Rozas de Madrid, Espana

Tel: +34 91 7105650
Email: rafael.pereira@innovasci.com

AceXon Technologies Pte. Ltd.
Singapore 658065

Tel: +65 (6565) 7300
Email: lawrence.chua@acexon.com

Innova Scientific S.L.
28290 Las Rozas de Madrid

Tel: +34 91 7105650
Email: rafael.pereira@innovasci.com

Dyneos AG
CH-8307 Effretikon

Tel: +41 52 355 12 40
Email: info@dyneos.ch

SuperbIN Company Ltd.
Taipei 11493
Taiwan, R.O.C.

Tel: +886 2 265 706 78
Email: info@superbin.com.tw

Photonic Solutions PLC

Tel: +44 131 664 8122
Email: sales@photonicsolutions.co.uk

APE Applied Physics & Electronics, Inc.
45401 Research Ave., Suite 141
Fremont, CA 94539, USA

Tel: +1(888) 690-3250
Email: sales@ape-america.com
Email: service@ape-america.com