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Optical Fiber Spectroscopy

Optical Fiber Spectroscopy

Optical fibers (or fiber optic cables) are cables which transmit light efficiently along an extremely thin glass (silica) or plastic fiber. Light travels down the cable due to total internal reflection. There is relatively low loss of signal over large distances at specific wavelengths. Optical fibers are often used in telecommunications or data communication. However, they can also be useful in spectroscopy as they can transfer light efficiently between modular spectroscopy elements with little attenuation.

Example of a fiber optic spectrometer setup
Example setup of a fiber optic spectrometer.

Using optical fibers can help you ensure that your sample is reached by the maximum amount of light from your light source. They are also useful for negating any alignment issues when setting up your spectrometer and can act as a waveguide for light emitted by your sample. In many cases, using optical fibers can also significantly improve your signal-to-noise ratio. This is especially true when used in conjunction with a modular spectrometer like the Ossila Optical Spectrometer. It's for this reason that these compact, modular spectrometers are sometimes referred to as fiber optic spectrometers.

What are Optical Fibers?


Optical fibers consist of a thin glass fiber core, surrounded by some protective cladding and a final protective coating. This thin core is usually made of silica glass with a diameter between 50 - 1000 µm, but it can sometimes be made of a polymer material, such as PMMA.

optical fiber design - core, cladding and coating
Components of an optical fiber: core, cladding and protective casing.

This glass fiber core is then surrounded by cladding which has a slightly higher refractive index than the core. This difference can be as subtle as a 1% difference; however, in refractive index it will determine the critical angle θC. This angle θC is the angle of incidence where the light will be refracted at 90° to the surface normal and is defined with the following equation:

Optical fiber refractive index equation

For optical fibers, the critical angle is determined at the boundary between the core (with a refractive index, n2) and the cladding (with a refractive index, n1). If the angle of incidence is larger than this critical angle compared to the normal, then the light will be totally internally reflected - and therefore transmitted down the cable.

Optical fiber critical angle diagram

Another important factor to consider when using optical fibers is the acceptance angle of the cable, α. This angle defines the "cone" of acceptance of the fiber. In other words, this is the maximum angle through which light can enter into the optical fiber and be totally internally reflected at the core-cladding boundary. If the entrance angle is greater than this acceptance angle, then θ < θC and the light will escape the fiber.

Acceptance angle equation

Optical Fiber Attenuation


Attenuation is a measure of how much light is lost during its transmission through an optical fiber. When light enters the fiber, it is transmitted down the cable by total internal reflection. At certain wavelengths, these fibers can guide this signal down the fiber with extremely low levels of attenuation (or loss of light signal). Attenuation in an optical fiber is defined using this equation:

Where Px is the power at a distance x, down the cable and P0 is the power in the fiber when x=0. In high quality optical fibers and at the right wavelength, this attenuation is over measured over very large distances (kilometers). Attenuation can be approximately related to transmission of light as shown in the table below.

Attenuation (dB) Transmission (%)
0.01 99.8
0.1 98
0.5 89
1 79
2 63
3 50
5 32
10 10
attenuation for the ossila optical fibers
Attenuation curve for the Ossila Optical Fibers over visible wavelengths

The graph above shows the attenuation curve for the Ossila Optical Fiber. You can see here that this fiber has decent optical transmission below 400 nm (T>80%) and very good optical transmission between 400 nm and 1100 nm (T>98%). This should help you waveguide light between modular spectroscopy components, increasing signal and reducing noise.

When to use Optical Fibers in Spectroscopy


P3HT:o-IDTBR absorbance - averaging number
PFO fluorescence measurements taken in air and through optical fibers

Using optical fibers can help you capture and waveguide emitted light efficiently. As you can see in the above graph, the signal intensity (and therefore signal-to-noise ratio) is greatly improved by using optical cables between modular components of the spectrometer. Fluorescence measurements are emitted in all directions equally and is therefore not a collimated emission. Optical fibers help direct these photons to the spectrometer, and you therefore achieve a better signal to noise ratio.

OPV with and without optical fibers
Absorbance measurements of P3HT:o-IDTBR films measuring through air and through optical cables.

However, when taking absorbance measurements of thick, dark films — for example with photovoltaic materials — transmission levels through the film will be quite low. For example, a measurement of 1.0 A.U. means that 10% of the light source is transmitted through the sample and measured. If there is any loss of signal through the optical fiber this will decrease the size of your absorbance signal significantly.

Optical fibers will transmit visible light less efficiently, so there may be a loss of signal when measuring absorbance through optical fibers, especially due to the increased distance travelled. Therefore, measuring absorbance through optical fibers will only decrease the signal-to-noise ratio and may lead to a noisier measurement. Therefore, when measuring transmission or absorbance on thick or dark films, we recommend measuring without optical cables. When taking measurements through air, be sure to place the components as close as possible towards one another or use appropriate optics to direct this transmitted light to the spectrometer.

Optical Spectrometer

Optical Spectrometer

Losses in Optical Fibers


There are several sources of loss in optical fibers, such as absorption of light within the cable, cable bending, connector losses, etc. You may notice attenuation through an optical fiber if there are intrinsic issues with the cable. Intrinsic faults fall into three categories: absorption, dispersion and scattering.

Absorption accounts for the light that is absorbed by the materials within the fiber. The largest causes of absorption in optical fibers are residual OH+ ions within the silica or from dopants which are used to alter the refractive index of the glass or cladding. Attenuation due to absorption will increase with increasing cable length.

Dispersion refers to the distortion a signal experiences as it travels through an optical fiber. For example, if you start with a laser light source of narrow band width, the broadening of this signal after transmission through the optical fiber is the dispersion of the signal. Scattering losses can also occur in an optical fiber occur because of defects or density fluctuations in the cable. Scattering losses are wavelength dependent. Therefore, at higher wavelengths there is less attenuation due to scattering.

Bending is the one of the most common issues that arises when using optical fibers. Micro bending relates to very small distortions in the walls of the cable or the cladding of an optical fiber. Macro bending however is when the arrangement of your optical components means that θ < θC and light escapes the fiber. Improper handling of the optical cable can result in bending issues.

Attenuation is lowest in silica optical fibers in the IR region. In fact, the minimum attenuation within silica optical fibers is at around 1550 nm. Therefore, IR signals are used for transmitting informational signals over longer distances. Using optical fibers can be very useful in setting up modular fiber optic spectrometer. However, bear in mind that there can be attenuation in the visible light region.

Contributing Authors


Written by

Dr. Mary O'Kane

Application Scientist

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