| Allicdata Part #: | 9B16000087-ND |
| Manufacturer Part#: |
9B16000087 |
| Price: | $ 0.14 |
| Product Category: | Crystals, Oscillators, Resonators |
| Manufacturer: | TXC Corporation |
| Short Description: | CRYSTAL 16MHZ 30PF TH |
| More Detail: | 16MHz ±30ppm Crystal 30pF HC-49/US |
| DataSheet: | 9B16000087 Datasheet/PDF |
| Quantity: | 1000 |
| 1000 +: | $ 0.12600 |
| Series: | 9B |
| Packaging: | Bulk |
| Part Status: | Active |
| Type: | MHz Crystal |
| Frequency: | 16MHz |
| Frequency Stability: | ±50ppm |
| Frequency Tolerance: | ±30ppm |
| Load Capacitance: | 30pF |
| Operating Mode: | -- |
| Operating Temperature: | -10°C ~ 70°C |
| Ratings: | -- |
| Mounting Type: | Through Hole |
| Package / Case: | HC-49/US |
| Size / Dimension: | 0.453" L x 0.197" W (11.50mm x 5.00mm) |
| Height - Seated (Max): | 0.145" (3.68mm) |
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Crystals
Crystals are natural or man-made substances that are characterized by an internal lattice structure. This lattice structure is formed by equally spaced atoms or molecules that are held in place via an orderly arrangement of chemical bonds. A crystal is constructed in such a way that its components are strategically arranged in a periodic fashion, resulting in a highly ordered and organized solid substance.
The number 9B16000087 refers to a crystal known as a tunable optical parametric oscillator (TOPO) crystal. These crystals are designed to convert high-power pulsed lasers into two or more lower-power beams of light. The output beams can then be shaped and tailored to produce a wide range of properties, such as wavelength, polarization, or beam direction, depending on the type of crystal. TOPO crystals are popularly used in laser materials processing, fiber optics, and optical communications.
The working principle of a TOPO crystal is quite simple. It consists of two main parts: a gain medium, and a heat-sink. The gain medium is a material with a target refractive index, which is placed inside the cavity of the TOPO crystal. At the top of the crystal, a laser beam is applied, which is then focused onto the gain medium. Upon focusing, the light waves interact with the material inside the gain medium and are amplified – a process known as Stimulated Emission. As the light waves travel down the cavity, they are steered by Bragg gratings etched into the walls consisting of minute structures. This creates an anisotropic refraction of the light, which allows for the beams to be tailored into a specific shape or achieve a desired wavelength.
Furthermore, the heat-sink, placed at the bottom of the TOPO crystal, acts as a cooling system. It absorbs the heat released during the Stimulated Emission process, thereby ensuring the stability of the gain medium and preventing intense thermal distortion. In addition, the heat-sink also acts as a reflector and bounces the amplified light back and forth between the walls of the TOPO crystal. This ensures that a single light signal is amplified and sent out for further tailoring.
Therefore, 9B16000087 is an example of a TOPO crystal, which is widely used in applications such as laser materials processing, fiber optics, and optical communications. These crystals are highly efficient due to their capabilities to convert high-power pulsed lasers into lower-power beams of light, which can then be tailored to a desired wavelength, polarization, or beam direction.
The specific data is subject to PDF, and the above content is for reference
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9B16000087 Datasheet/PDF