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To fulfill the conditions for TIR in the fiber, the angle of incidence of light launched into the fiber must be less than a certain angle, which is defined as the acceptance angle, . Snell's law can be used to calculate this angle: where ncore is the refractive index of the fiber core, nclad is the refractive index of the fiber cladding, n is the refractive index of the outside medium, . The numerical aperture (NA) is a dimensionless quantity used by fiber manufacturers to specify the acceptance angle of an optical fiber and is defined as: In step- index fibers with a large core (multimode), the NA can be calculated directly using this equation. The NA can also be determined experimentally by tracing the far- field beam profile and measuring the angle between the center of the beam and the point at which the beam intensity is 5% of the maximum; however, calculating the NA directly provides the most accurate value. Number of Modes in an Optical Fiber. Each potential path that light propagates through in an optical fiber is known as a guided mode of the fiber. Depending on the physical dimensions of the core/cladding regions, refractive index, and wavelength, anything from one to thousands of modes can be supported within a single optical fiber. The two most commonly manufactured variants are single mode fiber (which supports a single guided mode) and multimode fiber (which supports a large number of guided modes). In a multimode fiber, lower- order modes tend to confine light spatially in the core of the fiber; higher- order modes, on the other hand, tend to confine light spatially near the core/cladding interface. Using a few simple calculations, it is possible to estimate the number of modes (single mode or multimode) supported by an optical fiber. The normalized optical frequency, also known as the V- number, is a dimensionless quantity that is proportional to the free space optical frequency but is normalized to guiding properties of an optical fiber. The V- number is defined as: where V is the normalized frequency (V- number), a is the fiber core radius, and . Multimode fibers have very large V- numbers; for example, a . To meet this condition, a single mode fiber has a much smaller core size and NA compared to a multimode fiber at the same wavelength. One example of this, SMF- 2. Ultra single mode fiber, has a nominal NA of 0. The sources of these losses are typically wavelength dependent and range from the material used in the fiber itself to bending of the fiber. Common sources of attenuation are detailed below: Absorption. Because light in a standard optical fiber is guided via a solid material, there are losses due to absorption as light propagates through the fiber. Standard fibers are manufactured using fused silica and are optimized for transmission from 1. At longer wavelengths (> 2. Fluoride glasses such as Zr. F4 and In. F3 are used in manufacturing Mid- IR optical fibers primarily because they exhibit lower loss at these wavelengths. Zr. F4 and In. F3 fibers have a multi- phonon edge of ~3. One example of an undesired impurity is water molecules that are trapped in the glass of the optical fiber, which will absorb light around 1. Since telecom signals and some lasers operate in that same region, any water molecules present in the fiber will attenuate the signal significantly. The concentration of ions in the fiber glass is often controlled by manufacturers to tune the transmission/attenuation properties of a fiber. For example, hydroxyl ions (OH- ) are naturally present in silica and absorb light in the NIR- IR spectrum. Therefore, fibers with low- OH content are preferred for transmission at telecom wavelengths. On the other hand, fibers with high- OH content typically exhibit increased transmission at UV wavelengths and thus may be preferred by users interested in applications such as fluorescence or UV- VIS spectroscopy. Scattering. For the majority of fiber optics applications, light scattering is a source of loss that occurs when light encounters a change in the refractive index of the medium. These changes can be extrinsic, caused by impurities, particulates, or bubbles; or intrinsic, caused by fluctuations in the glass density, composition, or phase state. Scattering is inversely related to the wavelength of light, so scattering loss becomes significant at shorter wavelengths such as the UV or blue regions of the spectrum. Using proper fiber cleaning, handling, and storage procedures may minimize the presence of impurities on tips of fibers that cause large scattering losses. Bending Loss. Losses that occur due to changes in the external and internal geometry of an optical fiber are known as bending loss. These are usually separated into two categories: macrobending loss and microbending loss. Macrobend loss is typically associated with the physical bending of an optical fiber; for example, rolling it in a tight coil. As shown in the image to the right, guided light is spatially distributed within the core and cladding regions of the fiber. When a fiber is bent at a radius, light near the outer radius of the bend cannot maintain the same spatial mode profile without exceeding the speed of light. Instead, the energy is lost to the surroundings as radiation. For a large bend radius, the losses associated with bending are small; however, at bend radii smaller than the recommended bend radius of a fiber, bend losses become very significant. For short periods of time, optical fibers can be operated at a small bend radius; however, for long- term storage, the bend radius should be larger than the recommended value. Use proper storage conditions (temperature and bend radius) to reduce the likelihood of permanently damaging the fiber; the FSR1 Fiber Storage Reel is designed to minimize high bend loss. Microbend loss arises from changes in the internal geometry of the fiber, particularly the core and cladding layers. These random variations (i. Unlike macrobend loss, which is controlled by the bend radius, microbend loss occurs due to permanent defects in the fiber that are created during fiber manufacturing. Cladding Modes. While most light in a multimode fiber is guided via TIR within the core of the fiber, higher- order modes that guide light within both the core and cladding layer, because of TIR at the cladding and coating/buffer interface, can also exist. This results in what is known as a cladding mode. An example of this can be seen in the beam profile measurement to the right, which shows cladding modes with a higher intensity in the cladding than in the core of the fiber. These modes can be non- propagating (i. TIR) or they can propagate over a significant length of fiber. Because cladding modes are typically higher- order, they are a source of loss in the presence of fiber bending and microbending defects. Cladding modes are also lost when connecting two fibers via connectors as they cannot be easily coupled between optical fibers. Cladding modes may be undesired for some applications (e. Over long fiber lengths, these modes will naturally attenuate. For short fiber lengths (< 1. Launch Conditions. Underfilled Launch Condition. For a large multimode fiber which accepts light over a wide NA, the condition of the light (e. NA) coupled into the fiber can have a significant effect on performance. 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An overfilled launch completely exposes the fiber core and some of the cladding to light, enabling the filling of lower- and higher- order modes equally (as seen in the images below) and increasing the likelihood of coupling into cladding modes of the fiber. This increased percentage of higher- order modes means that overfilled fibers are more sensitive to bending loss. The measured insertion loss for an overfilled launch tends to be higher than typical, but results in an overall higher output power compared to an underfilled fiber launch. There are advantages and disadvantages to underfilled or overfilled launch conditions, depending on the needs of the intended application. For measuring the baseline performance of a multimode fiber, Thorlabs recommends using a launch condition where the beam diameter is 7. Best Carton Box Design Downloads. 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