OSE1

Superluminescent Diode, 14-Pin Butterfly, Broadband, CW, Center wavelength option 770-1700 nm, FWHM 10-100nm, Up to 50 mW

Key Features:

  • Great power/spectral coverage
  • Low coherence length
  • Low spectral ripple
  • Many center wavelength (CW) options from 770-1700 nm
  • Bandwidth FWHM: 10-100 nm
  • Low Deg. of Polarization option
  • Compact, 14-Pin BF package
  • FC/APC (optional FC/PC, SMA)
  • SM or PM fiber options
  • Telcordia GR-486 certification and RoHS compliance
  • RIN: -140dB/Hz – 125dB/Hz

There are many different configurations, choices for center wavelength, and other options. Get help selecting the right configuration for you!

Need Quantities? Have a question? Looking for a quote?

The SLED Series

The SLED Series represents a family of high-performance Superluminescent Diode (SLED) light sources, designed to deliver exceptional broadband spectral coverage and low temporal coherence. Leveraging advanced semiconductor technology, the SLED Series combines the high power and brightness of laser diodes with the broad spectral output of conventional LEDs. Available in compact, industry-standard packages such as 14-pin butterfly, these sources feature integrated thermoelectric coolers (TEC), monitor photodiodes, and isolators to ensure stable, high-quality performance.

With center wavelengths ranging from 770nm to 1680nm and bandwidths from 10nm to 460nm, the SLED Series offers customizable spectral stitching and power options (up to 130mW free space), making it ideal for a wide range of applications. The series meets Telcordia GR-468 and RoHS/Reach standards, ensuring reliability and compliance, and offers specialty devices featuring distributed feedback (DFB), tunable external cavity lasers, semiconductor optical amplifiers, and amplified spontaneous emission (ASE) sources.

OSE1 – Optical Spectral Engine SLED – Overview

DAYY Photonics Corporation superluminescent light-emitting diode (SLED or SLD) is a superluminescence-based edge-emitting semiconductor light source that combines the high power and brightness of a laser diode with the low coherence of conventional lightemitting diodes.

Our light source product family comes in a wide range of center wavelengths and spectral bandwidth ranging from 770nm-1700nm. The light source is packaged in a 14pin industry standard butterfly package meeting Telcordia GR-468, RoHS/Reach standards.

Our Light Source covers all the bands needed for broadband and high- power requirements, our SLED-based light sources will cover all the main bands used in telecom applications, and communications and test applications. Our product family is ideal for broadband applications, and passive component testing, as well as fiber- optic sensing, spectroscopy and more.

OSE1 Low DOP Option:

Low-Degree of Polarization (DOP): with the ISB1 controller, we can provide under 5% DOP across spectrum – this minimizes polarization sensitivity of fiber sensors and reduces the effects of polarization dependent loss.

Customization, Packaging & Assembly Capabilities

High-Resolution Retinal Imaging Made Simpler:

830 nm SLED for Ophthalmology OCT

Retinal OCT systems in ophthalmology demand stable broadband light for sharp axial resolution without swept-source complexity. The DAYY ASM002408 830 nm Single-SLED delivers >5 mW SM fiber-coupled power, >35 nm FWHM bandwidth (810–850 nm coverage), integrated TEC stabilization, monitor photodiode, and zero polarization dependence. This yields cleaner interferograms, higher-contrast images, and drop-in OEM integration in a compact 14-pin butterfly package with FC/APC output.

Inquire about the ASM002408 for OCT:

OSE1 – Optical Spectral Engine Benefits:

  • Extensive Wavelength Range:
    • Maximize application flexibility – options from 770 to 1700nm & bandwidths of 10 to 100nm, covering telecom, sensing & imaging needs.
  • High Power and Brightness:
    • Ensure reliable performance, combined with low coherence, ideal for precision optical testing and broadband applications.
  • Industry-Standard 14-Pin Butterfly Packaging
    • Simplify integration with FC/APC connectors (FC/PC or SMA optional) and SM/PM fiber options.
  • Low Spectral Ripple & Low RIN:
    • Enhance system stability, including low relative intensity noise (-140dB/Hz to -125dB/Hz), reducing noise in sensitive measurements.
  • Direct Modulation up to 600 MHz:
    • Enable advanced modulation in specific models, supporting dynamic telecom and test applications.
  • Telcordia GR-468 and RoHS Compliance:
    • Meets rigorous standards, ensuring durability and environmental safety for industrial and biomedical use.
  • Low DOP Options:
    • Minimize polarization challenges via the ISB1 driver module, optimizing performance in fiber-optic sensing and component testing.

OSE1 – Optical Spectral Engine Applications:

  • Optical Component Testing
  • Telecom Test Equipment
  • Medical Optical Coherence Tomography
  • Industrial Optical Coherence Tomography

  • Industrial and Biomedical Imaging Systems
  • Optical Sensing
  • Test and Measurement
  • Research and Development

If you have any questions or need more information, please contact us:

Back to all DAYY Photonics products

How can we help you?

Talk to one of our experienced product managers today!

Contact us

CW Lasers FAQs

How do I align my optical system?

How do I align my optical system?

Laser alignment can be a challenging task, but aligning a laser beam doesn’t have to be as complicated as it might seem with the right optical alignment tools and proper laser alignment techniques. Multiple optical alignment techniques have been developed over the years, utilized by technicians and engineers to simplify the alignment process. With the development of these universal laser beam alignment methods, along with some laser alignment tips and tricks, you don’t need to be a laser expert to perform your alignments with relative ease, ensuring your laser beam path is right where you want it to be and your beam is on target every time. Read our article, titled “Laser Alignment: HeNe Lasers, Methods, and Helpful Tips” to get the knowledge and advice you need for proper optical beam path alignment utilizing HeNe Lasers. Get more information from our Lasers 101, Blogs, Whitepapers, FAQs, and Press Release pages in our Knowledge Center!

Should I choose multimode or single-mode for Raman spectroscopy?
Should I choose multimode or single-mode for Raman spectroscopy?

On the surface, this seems like a simple question since Raman is a nonlinear optical effect and therefore the tighter the beam can be focused the higher the conversion efficiency.  Seemingly a single-mode laser would be preferable, but in practice there are other factors that can complicate the situation. The first question you should ask yourself when considering which type of laser to choose is whether you are doing microscopy or bulk sampling.  If the answer to that question is microscopy, then you immediately should go with a single mode laser.  Since the goal of any microscopy system is to produce the highest resolution image possible, the number one consideration should be how tightly can the laser beam be focused down. However, there are several other considerations when choosing between multimode and single-mode. Learn which is best for you in this article: “Multimode vs Single-Mode Lasers for Raman Spectroscopy.” Get more information from our Lasers 101, Blogs, Whitepapers, FAQs, and Press Release pages in our Knowledge Center!

What is a CW Laser?
What is a CW Laser?

A CW or continuous-wave laser is any laser with a continuous flow of pump energy. It emits a constant stream of radiation, as opposed to a q-switched or mode-locked pulsed laser with a pulsed output beam. A laser is typically defined as having a pulse width greater than 250 ms. The first CW laser was a helium-neon (HeNe) gas laser, developed in 1960, which you can read more about in this blog “HeNe Lasers: Bright Past, Brighter Future.” If you want to read more about the types of CW Lasers we offer, check out the Overview of CW Lasers section on our Lasers 101 Page!

What is the best laser for optical surface flatness testing?
What is the best laser for optical surface flatness testing?

It is essential that the laser exhibit a high level of spectral stability, ensuring that any changes in the interference pattern are caused by features in the sample and not originating from the laser beam. In addition to spectral stability, high beam pointing stability ensures consistent measurements by mitigating any beam position drift concerning the position of the sample. Lasers with longer coherence lengths, and subsequently narrower linewidths, play an important role in determining the resolution of the measurement, as well as consideration of the wavelength used. Exhibiting both single longitudinal mode and single spatial mode has excellent benefits. Get more information from our Lasers 101, Blogs, Whitepapers, FAQs, and Press Release pages in our Knowledge Center!

What type of laser is best for Doppler LIDAR?

What type of laser is best for Doppler LIDAR?

Various LIDAR signal methods for measuring velocity have one critical requirement in common, the need for precise control over laser frequency. While a wide variety of single-frequency lasers have been used in Doppler LIDAR research, the industry as a whole has adopted single-frequency fiber lasers as the ideal light source. Fiber lasers have several advantages over traditional DPSS lasers, all of which derive from the geometry of the fiber optic itself, namely the innate ability to have an extremely long single-mode optical cavity. This geometry allows for the production of either extremely high-power, single-mode lasers producing unprecedented brightness, or extremely narrow band lasers, with near perfect single-frequency output. If you want to learn more about Doppler LIDAR, the critical considerations involved, and ideal laser sources, check out this whitepaper: “Single-Frequency Fiber Lasers for Doppler LIDAR.” Get more information from our Lasers 101, Blogs, Whitepapers, FAQs, and Press Release pages in our Knowledge Center!

What’s the difference between single transverse mode & single longitudinal mode?

What’s the difference between single transverse mode & single longitudinal mode?

Within the laser community, one of the most overused and often miscommunicated terms is the phrase “single mode.”  This is because a laser beam when traveling through air takes up a three-dimensional volume in space similar to that of a cylinder; and just as with a cylinder, a laser beam can be divided into independent coordinates each with their own mode structure.  For a cylinder we would call these the length and the cross-section, but as shown in the figure below for a laser beam, we define these as the transverse electromagnetic (TEM) plane and the longitudinal axis.   Both sets of modes are fundamental to the laser beam’s properties, since the TEM modes determine the spatial distribution of the laser beams intensity, and the longitudinal modes determine the spectral properties of the laser.  As a result, when a laser is described as being “single-mode” first you need to make sure that you truly understand which mode is being referred to.  Meaning that you must know if the laser is single transverse mode, single longitudinal mode, or both. Get all the information you need in this article: “What is Single Longitudinal Mode?” Get more information from our Lasers 101, Blogs, Whitepapers, FAQs, and Press Release pages in our Knowledge Center!