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Journal articles on the topic 'Frustrated Total Internal Reflection (FTIR)'

Author: Grafiati

Published: 7 July 2024

Last updated: 31 July 2025

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1

Filgueira-Rama, Carolina, Alejandro Doval, Yago Arosa, and Raúl de la Fuente. "Beneath and beyond frustrated total reflection: A practical demonstration." American Journal of Physics 93, no. 2 (2025): 157–63. https://doi.org/10.1119/5.0207113.

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Frustrated total internal reflection (FTIR) is analyzed from a novel perspective. Unlike similar works, the angle of incidence is used here as the experimental variable instead of the film thickness through which light tunnels. This method makes it possible to visualize not only the phenomenon of FTIR but also the resonance processes that occur for angles of incidence below the critical angle. An affordable straightforward experiment appropriate for undergraduates is presented. The experiment involves measuring the reflection and transmission of light through a pair of prisms separated by an a

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2

Martinez, J. C. "Confronting the Hartman effect with data from frustrated total internal reflection (FTIR)." Laser Physics 16, no. 7 (2006): 1123–27. http://dx.doi.org/10.1134/s1054660x06070176.

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3

Hial, Qahtan Ghatih. "Frustrated total internal reflection of newton rings multiple beam interference." Iraqi Journal of Physics (IJP) 15, no. 35 (2018): 29–39. http://dx.doi.org/10.30723/ijp.v15i35.51.

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Frustrated Total Internal Reflection FTIR phenomenon is manifested employing Newton‟s rings setup generated via a coherent light beam of a laser diode ( . All concentric bright and dark rings, except the central bright spot, were noticed to recede (disappear) when the incident angle exceeded the critical angle of 41o.It was also shown that the current setup has proven its applicability for other tests and can give convenient results that conform with theory. Neither the concept nor the design is beyond what can be realized in an undergraduate laboratory. However, technical improvements in moun

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4

Kolhe, Neel, and Sreyashi Shetty. "A novel cantenna based demonstration of frustrated total internal reflection as an analog for quantum tunnelling." Physics Education 58, no. 2 (2023): 025011. http://dx.doi.org/10.1088/1361-6552/acad59.

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Abstract We use a ‘Cantenna’ (portmanteau of ‘Can’ and ‘Antenna’), which is a unidirectional homemade waveguide, coupled to a standard readily available, 2.4 GHz Wi-Fi router as a source of microwaves to demonstrate Frustrated Total Internal reflection (FTIR) using paraffin-wax prisms. This largely inexpensive experiment provides an opportunity to demonstrate a process closely analogous to quantum tunnelling in an undergraduate physics lab. FTIR is often demonstrated with glass prisms and lasers, which may not allow for an intuitive understanding of evanescent waves and tunnelling. Wi-Fi signa

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5

Голубцова, Ю. В. "ОЦЕНКА КАЧЕСТВА И ПОДЛИННОСТИ ПЛОДОВО-ЯГОДНОГО СЫРЬЯ МЕТОДОМ ИК-ФУРЬЕ СПЕКТРОСКОПИИ НАРУШЕННОГО ПОЛНОГО ВНУТРЕННЕГО ОТРАЖЕНИЯ". ТЕХНИКА И ТЕХНОЛОГИЯ ПИЩЕВЫХ ПРОИЗВОДСТВ 2, № 45 (2017): 126–32. http://dx.doi.org/10.21179/2074-9414-2017-2-126-132.

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6

Lin, Jhe-Syuan, and Wen-Shing Sun. "A Hidden Fingerprint Device on an Opaque Display Panel." Applied Sciences 10, no. 6 (2020): 2188. http://dx.doi.org/10.3390/app10062188.

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In recent years, fingerprint recognition has become more and more widely used in mobile phones. A fingerprint recognition device hidden under an opaque display panel designed based on a waveguide and frustrated total internal reflection (FTIR) is proposed and demonstrated herein. In order to meet the demand for a high screen ratio for mobile phone displays, we use a symmetrical zoom-in and zoom-out coupler design. With this comprehensive coupler and waveguide design, not only can fingerprint recognition be achieved using an opaque display panel, but it also meets the appearance requirements fo

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7

Bacher, Emmanuel, Sergio Cartiel, Jorge Garcia-Pueyo, et al. "OptoSkin: Novel LIDAR Touch Sensors for Detection of Touch and Pressure Within Wave Guides." IEEE Sensors Journal 24, no. 20 (2024): 33268–80. https://doi.org/10.1109/JSEN.2024.3443615.

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Light detection and ranging (LIDAR) sensors, employing direct time-of-flight (dToF) measurements, are crucial for precise surface localization and are increasingly integrated into compact chip designs. These sensors have extensive use in proximity sensing in various applications. This article presents the innovative use of LIDAR sensors for ranging within waveguides to accurately detect touch and pressure. In our OptoSkin sensors, light propagates via total internal reflection (TIR) within the waveguide. Then, it is reflected back to the sensor as a result of waveguide deformation and/or scatt

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8

Shin, Manjae, Seungbong Lee, Seungbin Baek, Sunghoon Lee, and Sungmin Kim. "A Quantitative Analysis Study on the Effects of Moisture and Light Source on FTIR Fingerprint Image Quality." Sensors 25, no. 4 (2025): 1276. https://doi.org/10.3390/s25041276.

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The frustrated total internal reflection (FTIR) optical fingerprint scanning method is widely used due to its cost-effectiveness. However, fingerprint image quality is highly dependent on fingertip surface conditions, with moisture generally considered a degrading factor. Interestingly, a prior study reported that excessive moisture may improve image quality, though their findings were based on qualitative observations, necessitating further quantitative analysis. Additionally, since the FTIR method relies on optical principles, image quality is also influenced by the wavelength of the light s

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9

Жуков, Н. Д., А. Г. Роках та М. И. Шишкин. "Свойства наночастиц сульфида свинца в мультизеренной структуре". Физика и техника полупроводников 52, № 6 (2018): 608. http://dx.doi.org/10.21883/ftp.2018.06.45924.8686.

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AbstractThe structural and electrical properties of PbS nanoparticles (40–70 nm), produced by a chemical reaction of sodium hydroxide with lead nitrate and electrophoretically deposited onto a conductive substrate, are investigated. The composition and structure of the nanoparticles are identified by X-ray analysis as pure PbS phase with a face-centered cubic lattice. Several minima, related to plasma-resonance absorption at 10–17 μm, are observed in the frustrated total internal reflection (FTIR) spectra. The layer morphology and the nanoparticle shape and sizes are determined by scanning ele

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10

Aulika, Ilze, Andrejs Ogurcovs, Meldra Kemere, et al. "Influence of Material Optical Properties in Direct ToF LiDAR Optical Tactile Sensing: Comprehensive Evaluation." Materials 18, no. 14 (2025): 3287. https://doi.org/10.3390/ma18143287.

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Optical tactile sensing is gaining traction as a foundational technology in collaborative and human-interactive robotics, where reliable touch and pressure feedback are critical. Traditional systems based on total internal reflection (TIR) and frustrated TIR (FTIR) often require complex infrared setups and lack adaptability to curved or flexible surfaces. To overcome these limitations, we developed OptoSkin—a novel tactile platform leveraging direct time-of-flight (ToF) LiDAR principles for robust contact and pressure detection. In this extended study, we systematically evaluate how key optica

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11

Brodie, Graham, and Grigory Torgovnikov. "Microwave Soil Heating with Evanescent Fields from Slow-Wave Comb and Ceramic Applicators." Energies 15, no. 3 (2022): 1068. http://dx.doi.org/10.3390/en15031068.

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Microwave soil heating deactivates weed seeds; however, in many modern agricultural settings, weed seeds are mostly found in the top 1–2 cm of the soil profile. Until recently, microwave soil heating has been achieved using various antennas, which project the microwave energy deeply into the soil. The aim of this research was to develop new microwave applicators that provide shallow heating (less than 50 mm). This paper presents two applicator designs, one based on a comb slow-wave structure and the other on the frustrated total internal reflection (FTIR) principle, which utilise evanescent mi

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12

Becchetti, Matteo, Roberto Marsili, Ferdinando Cannella, and Alberto Garinei. "A new system for the measurement of gripping force based on scattering." ACTA IMEKO 6, no. 4 (2017): 100. http://dx.doi.org/10.21014/acta_imeko.v6i4.481.

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<p style="margin: 0cm 0cm 0pt;"><span lang="EN-US"><span style="font-family: Calibri; font-size: small;">The measurement of contact pressure of human fingers is very important to understand human perceptual mechanisms, that is the main goal of most of the neuroscientific studies. It may also lead to a correct development of tactile devices and haptic systems, as they are intended to convey controllable and effective stimuli.</span></span></p><span style="font-family: 'Garamond','serif'; font-size: 10pt; mso-bidi-font-size: 12.0pt; mso-fareast-font-family:

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13

Borković, Katarina, and Andreana Ćurić. "“Tap, Tap Water”. Quantum Tunneling Demonstration." Natural Science and Advanced Technology Education 31, no. 4 (2022): 359–70. http://dx.doi.org/10.53656/nat2022-4.04.

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Quantum tunneling is a phenomenon in which an atom or a subatomic particle appears on the other side of a potential barrier that should be impenetrable to the particle, given the difference between the kinetic energy of the particle and the potential energy of the barrier, the former being significantly lesser. However, if the barrier shrinks enough the particle will be able to tunnel right through it. This is among the most well-known quantum physics phenomena. Historically, physicists struggled to grasp the wavelike and particle-like duality of light and subatomic particles. The aforemention

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14

Hernandez, Alyssa M., Jessica A. Sandoval, Michelle C. Yuen, and Robert J. Wood. "Stickiness in shear: stiffness, shape, and sealing in bioinspired suction cups affect shear performance on diverse surfaces." Bioinspiration & Biomimetics 19, no. 3 (2024): 036008. http://dx.doi.org/10.1088/1748-3190/ad2c21.

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Abstract Aquatic organisms utilizing attachment often contend with unpredictable environments that can dislodge them from substrates. To counter these forces, many organisms (e.g. fish, cephalopods) have evolved suction-based organs for adhesion. Morphology is diverse, with some disc shapes deviating from a circle to more ovate designs. Inspired by the diversity of multiple aquatic species, we investigated how bioinspired cups with different disc shapes performed in shear loading conditions. These experiments highlighted pertinent physical characteristics found in biological discs (regions of

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15

Zhu, Yu, Chuanjun Yao, Jinbang Chen, and Rihong Zhu. "Frustrated total internal reflection evanescent switching." Optics & Laser Technology 31, no. 8 (1999): 539–42. http://dx.doi.org/10.1016/s0030-3992(99)00102-4.

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16

Balcou, Ph, L. Dutriaux, F. Bretenaker, and A. Le Floch. "Frustrated total internal reflection of laser eigenstates." Journal of the Optical Society of America B 13, no. 7 (1996): 1559. http://dx.doi.org/10.1364/josab.13.001559.

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17

Longhi, Stefano. "Resonant tunneling in frustrated total internal reflection." Optics Letters 30, no. 20 (2005): 2781. http://dx.doi.org/10.1364/ol.30.002781.

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18

Mamedov, R. K. "Combined element for multiple frustrated total internal reflection." Journal of Optical Technology 67, no. 9 (2000): 837. http://dx.doi.org/10.1364/jot.67.000837.

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19

MacFarlane, D. L., M. P. Christensen, K. Liu, et al. "Four-Port Nanophotonic Frustrated Total Internal Reflection Coupler." IEEE Photonics Technology Letters 24, no. 1 (2012): 58–60. http://dx.doi.org/10.1109/lpt.2011.2172204.

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20

Carey, John J., Justyna Zawadzka, Dino A. Jaroszynski, and Klaas Wynne. "Noncausal Time Response in Frustrated Total Internal Reflection?" Physical Review Letters 84, no. 7 (2000): 1431–34. http://dx.doi.org/10.1103/physrevlett.84.1431.

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21

Zhu, S., A. W. Yu, D. Hawley, and R. Roy. "Frustrated total internal reflection: A demonstration and review." American Journal of Physics 54, no. 7 (1986): 601–7. http://dx.doi.org/10.1119/1.14514.

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22

Vörös, Zoltán, and Rainer Johnsen. "A simple demonstration of frustrated total internal reflection." American Journal of Physics 76, no. 8 (2008): 746–49. http://dx.doi.org/10.1119/1.2904473.

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23

Goddard, Nicholas J., Kirat Singh, Richard J. Holmes, and Behnam Bastani. "Resonant grating sensors using frustrated total-internal reflection." Sensors and Actuators B: Chemical 51, no. 1-3 (1998): 131–36. http://dx.doi.org/10.1016/s0925-4005(98)00180-4.

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24

Grattan, K., A. Palmer, and D. Saini. "Frustrated-total-internal-reflection fiber-optic pressure sensor." Journal of Lightwave Technology 3, no. 5 (1985): 1130–34. http://dx.doi.org/10.1109/jlt.1985.1074290.

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25

Cluzel, Benoit, and Frédérique De Fornel. "Frustrated total internal reflection: the Newton experiment revisited." Photoniques, no. 116 (2022): 32–37. http://dx.doi.org/10.1051/photon/202211632.

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Three centuries ago, Isaac Newton reported the experimental observation of the tunnelling of a light ray between two prisms separated by a small gap once one of them was shinned in total internal reflection. This article describes a modern revisit of this seminal Newton’s experiment, generally known as the Frustrated Total Internal Reflection. This experiment was created in the framework of a series of lectures about near-field optics and nanophotonics for Master students. During a 4h lab work session, the students are running the experiment to evidence and quantify the evanescent wave on top

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26

Hirano, John, and David Garmire. "Force Transducer Through Total Internal Reflection and Frustrated Total Internal Reflection for a Three-Axis Anemometer." IEEE Sensors Journal 15, no. 7 (2015): 3827–34. http://dx.doi.org/10.1109/jsen.2014.2385751.

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27

Suhr, Wilfried. "Gaining insight into antibubbles via frustrated total internal reflection." European Journal of Physics 33, no. 2 (2012): 443–54. http://dx.doi.org/10.1088/0143-0807/33/2/443.

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28

Huntoon, Nathan R., Marc P. Christensen, Duncan L. MacFarlane, Gary A. Evans, and C. S. Yeh. "Integrated photonic coupler based on frustrated total internal reflection." Applied Optics 47, no. 30 (2008): 5682. http://dx.doi.org/10.1364/ao.47.005682.

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29

Zanella, F. P., D. V. Magalhães, M. M. Oliveira, R. F. Bianchi, L. Misoguti, and C. R. Mendonça. "Frustrated total internal reflection: A simple application and demonstration." American Journal of Physics 71, no. 5 (2003): 494–96. http://dx.doi.org/10.1119/1.1523075.

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30

Hashemi, Mir Amid, and Charles M. Heron. "Analysis of particle contact using frustrated total internal reflection." Meccanica 54, no. 4-5 (2019): 653–65. http://dx.doi.org/10.1007/s11012-019-00966-9.

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31

Petrov, Nikolai I. "Frustrated-total-internal-reflection-based thin-film color separator." Optics Letters 32, no. 18 (2007): 2744. http://dx.doi.org/10.1364/ol.32.002744.

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32

Balcou, Ph, and L. Dutriaux. "Dual Optical Tunneling Times in Frustrated Total Internal Reflection." Physical Review Letters 78, no. 5 (1997): 851–54. http://dx.doi.org/10.1103/physrevlett.78.851.

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33

Pavlov, I. N. "Comparison of sensitivity of the refractometric methods of frustrated total internal reflection and surface plasmon resonance." Izmeritel`naya Tekhnika, no. 2 (2020): 44–49. http://dx.doi.org/10.32446/0369-1025it.2020-2-44-49.

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Two optical methods, namely surface plasmon resonance imaging and frustrated total internal reflection, are described in the paper in terms of comparing their sensitivity to change of refractive index of a thin boundary layer of an investigated medium. It is shown that, despite the fact that the theoretically calculated sensitivity is higher for the frustrated total internal reflection method, and the fact that usually in practice the surface plasmon resonance method, on the contrary, is considered more sensitive, under the same experimental conditions both methods show a similar result.

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34

Brinkevich, S. D., D. I. Brinkevich, V. S. Prosolovich, S. B. Lastovskii, and A. N. Pyatlitski. "Frustrated Total Internal Reflection Spectra of Diazoquinone–Novolac Photoresist Films." Journal of Applied Spectroscopy 87, no. 6 (2021): 1072–78. http://dx.doi.org/10.1007/s10812-021-01111-9.

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35

Pavlov, I. N., and B. S. Rinkevichyus. "Near-wall liquid flows visualization on frustrated total internal reflection." Optical Memory and Neural Networks 18, no. 4 (2009): 322–27. http://dx.doi.org/10.3103/s1060992x09040110.

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36

Volchek, B. Z., S. V. Kononova, E. N. Vlasova, R. K. Mamedov, and K. A. Mikhalev. "Study of microporous membranes using frustrated total internal reflection spectroscopy." Journal of Optical Technology 70, no. 1 (2003): 22. http://dx.doi.org/10.1364/jot.70.000022.

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37

Ghatak, Ajoy, and Swagata Banerjee. "Temporal delay of a pulse undergoing frustrated total internal reflection." Applied Optics 28, no. 11 (1989): 1960. http://dx.doi.org/10.1364/ao.28.001960.

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38

Kiven, Stacy B., Jianxun Lei, Varun Sagi, et al. "Calpain-1 Contributes to Pain and Organ Damage in Sickle Cell Disease." Blood 134, Supplement_1 (2019): 76. http://dx.doi.org/10.1182/blood-2019-127761.

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Sickle cell disease (SCD) is complex with disabling and life-threatening consequences including pain and organ damage. We hypothesized that calpain-1, a calcium-dependent protease may contribute to both organ damage and pain in SCD because deletion of calpain-1 in HbSS Townes mice ameliorated hyperalgesia (Nwankwo et al., Haematologica 2016), and BDA-410, a selective calpain-1 inhibitor, significantly improved age-associated organ damage in a mouse model of aging (Nabeshima et al., Sci Reports 2014). We performed a randomized double-blind placebo-controlled trial in homozygous female HbSS BERK

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39

Perel'man, Mark E. "Theory of frustrated total internal reflection: Superluminal singularities of optical waveguides." Physics Letters A 373, no. 6 (2009): 648–52. http://dx.doi.org/10.1016/j.physleta.2008.12.021.

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40

Smith, Nathan D., and James S. Sharp. "Accessible biometrics: A frustrated total internal reflection approach to imaging fingerprints." Science & Justice 57, no. 3 (2017): 193–98. http://dx.doi.org/10.1016/j.scijus.2017.03.003.

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41

Li, Chun-Fang, and Qi Wang. "Duration of tunneling photons in a frustrated-total-internal-reflection structure." Journal of the Optical Society of America B 18, no. 8 (2001): 1174. http://dx.doi.org/10.1364/josab.18.001174.

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42

Beddows, David C. S., Ben C. Griffiths, Ota Samek, and Helmut H. Telle. "Application of frustrated total internal reflection devices to analytical laser spectroscopy." Applied Optics 42, no. 30 (2003): 6006. http://dx.doi.org/10.1364/ao.42.006006.

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43

Chen, Xi, Xiao-Jing Lu, Pei-Liang Zhao, and Qi-Biao Zhu. "Energy flux and Goos–Hänchen shift in frustrated total internal reflection." Optics Letters 37, no. 9 (2012): 1526. http://dx.doi.org/10.1364/ol.37.001526.

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44

Zanoni, Andrea, Pierre Garbo, Pierangelo Masarati, and Giuseppe Quaranta. "Frustrated Total Internal Reflection Measurement System for Pilot Inceptor Grip Pressure." Sensors 23, no. 14 (2023): 6308. http://dx.doi.org/10.3390/s23146308.

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Sensing the interaction between the pilot and the control inceptors can provide important information about the pilot’s activity during flight, potentially enabling the objective measurement of the pilot workload, the application of preventive actions against loss of situational awareness, and the identification of the insurgence of adverse couplings with the vehicle dynamics. This work presents an innovative pressure-sensing device developed to be seamlessly integrated into the grips of conventional aircraft control inceptors. The sensor, based on frustrated total internal reflection of light

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45

Goldina, N. D. "Calculation of the reflection coefficient of metal-dielectric structures in frustrated total internal reflection." Optoelectronics, Instrumentation and Data Processing 45, no. 6 (2009): 571–75. http://dx.doi.org/10.3103/s8756699009060120.

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46

Fedchenko, Dmitry P., Petr N. Kim, and Ivan V. Timofeev. "Photonic Topological Insulator Based on Frustrated Total Internal Reflection in Array of Coupled Prism Resonators." Symmetry 14, no. 12 (2022): 2673. http://dx.doi.org/10.3390/sym14122673.

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Total internal reflection occurs at the interface between two media with different refractive indices during propagation of light rays from a medium with a higher refractive index to a medium with a lower refractive index. If the thickness of the second medium is comparable to a specific light wavelength, then total internal reflection is violated partially or completely. Based on the frustrated total internal reflection, herein we discuss a two-dimensional photonic topological insulator in an array consisting of triangular, quadrangular, or hexagonal transparent prism resonators with a narrow

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47

Ryu, Meguya, Soon Hock Ng, Vijayakumar Anand, et al. "Attenuated Total Reflection at THz Wavelengths: Prospective Use of Total Internal Reflection and Polariscopy." Applied Sciences 11, no. 16 (2021): 7632. http://dx.doi.org/10.3390/app11167632.

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Capabilities of the attenuated total reflection (ATR) at THz wavelengths for increased sub-surface depth characterisation of (bio-)materials are presented. The penetration depth of a THz evanescent wave in biological samples is dependent on the wavelength and temperature and can reach 0.1–0.5 mm depth, due to the strong refractive index change ∼0.4 of the ice-water transition; this is quite significant and important when studying biological samples. Technical challenges are discussed when using ATR for uneven, heterogeneous, high refractive index samples with the possibility of frustrated tota

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48

Zhukova, E. V., V. M. Zolotarev, N. B. Margaryants, and L. P. Shishatskaya. "Using frustrated total internal reflection spectroscopy to study color centers in crystals." Journal of Optical Technology 66, no. 1 (1999): 46. http://dx.doi.org/10.1364/jot.66.000046.

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49

Mamedov, R. K. "Methods and technology of frustrated-total-internal-reflection spectroscopy using thermoplastic glasses." Journal of Optical Technology 71, no. 10 (2004): 685. http://dx.doi.org/10.1364/jot.71.000685.

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50

Goldina, N. D. "Frustrated total internal reflection from thin-layer structures with a metal film." Optics and Spectroscopy 106, no. 5 (2009): 748–52. http://dx.doi.org/10.1134/s0030400x0905021x.

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