
Understanding the Light–Matter Interaction in Attenuated Total Reflectance Experiments
Is sample thickness important for signal detection? The answer is yes, and in this interview segment, Thomas Mayerhofer of Leibniz Institute of Photonic Technology explains why.
Attenuated total reflectance (ATR) spectroscopy is often
In their study, the researchers demonstrated that the evanescent field disappears when the rarer medium is absorbing
By analyzing electric field distributions and spectral responses in both semi-infinite media and finite layers, the researchers demonstrated that ATR spectra can still be obtained below the critical angle, even in the absence of an evanescent field. They also identify additional phenomena, such as tunneling and frustrated total reflection, particularly in systems involving a vacuum layer over a weakly absorbing medium.1
In this video clip, Mayerhofer discusses the transition from transmission spectroscopy to ATR spectroscopy, highlighting the importance of sample thickness for signal detection. Mayerhofer explains that with ATR spectroscopy, the interaction at the sample–crystal interface is crucial, especially for absorbing samples. Unlike transmission spectroscopy, only the light reflected at the interface is detected, not the light absorbed by the sample. This new perspective emphasizes the significance of the interface in ATR spectroscopy.
This interview is the third part of a five-part interview with Mayerhofer. The first part of our conversation focused on defining what the evanescent field is and how it relates to ATR spectroscopy. The second part of our conversation with Mayerhofer focused on what led him to re-examine several spectroscopic methods, including ATR spectroscopy.
References
- Mayerhofer, T.; Popp, J. Understanding the Role of the Evanescent Field in Attenuated Total Reflection (ATR) Spectroscopy. Appl. Spectrosc. 2026, 80 (2), 125–132. DOI:
10.1177/00037028251358400 - Mayerhofer, T.; Popp, J. Complex-Valued Chemometrics for Composition Analysis. Spectroscopy 2025, 40 (6), 16–21. DOI:
10.56530/spectroscopy.wn4265d4




