In this work, we study multimodal interference filters with a graphite oxide coating. The use of the multimodal interference filter shows a distinctive peak in the signal spectrum, and when using the exfoliated graphite coated multimodal interference filter the signal shows different spectral changes, such as the full width at half maximum of the curve, the maximum power, and the central wavelength, which indicates that graphite oxide absorbs part of the energy. In addition, microscope observations when a He-Ne laser is passed through the filter confirmed graphite oxide is adhered to the filter.

In this work, we study multimodal interference filters with a graphite oxide coating. The use of the multimodal interference filter shows a distinctive peak in the signal spectrum, and when using the exfoliated graphite coated multimodal interference filter the signal shows different spectral changes, such as the full width at half maximum of the curve, the maximum power, and the central wavelength, which indicates that graphite oxide absorbs part of the energy. In addition, microscope observations when a He-Ne laser is passed through the filter confirmed graphite oxide is adhered to the filter.

In this work, we study multimodal interference filters with a graphite oxide coating. Use of the multimodal interference filter shows a distinctive peak in the signal spectrum, and when using the exfoliated graphite coated multimodal interference filter, the signal shows different spectral changes, such as the full width at half maximum of the curve, the maximum power, and central wavelength, which indicates that graphite oxide absorbs part of the energy. In addition, microscope observations when a He–Ne laser is passed through the filter confirm that graphite oxide is adhered to the filter.