[go: up one dir, main page]
More Web Proxy on the site http://driver.im/
You seem to have javascript disabled. Please note that many of the page functionalities won't work as expected without javascript enabled.
 
 
Sign in to use this feature.

Years

Between: -

Subjects

remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline
remove_circle_outline

Journals

Article Types

Countries / Regions

Search Results (219)

Search Parameters:
Keywords = terahertz (THz) technology

Order results
Result details
Results per page
Select all
Export citation of selected articles as:
12 pages, 4233 KiB  
Article
Theoretical Investigation of Terahertz Spoof Surface-Plasmon-Polariton Devices Based on Ring Resonators
by Can Liu, Shenghao Gu, Mingming Sun, Ya Liu, Ying Zhang and Jiaguang Han
Photonics 2025, 12(1), 70; https://doi.org/10.3390/photonics12010070 - 15 Jan 2025
Viewed by 328
Abstract
Terahertz is one of the most promising technologies for high-speed communication and large-scale data transmission. As a classical optical component, ring resonators are extensively utilized in the design of band-pass and frequency-selective devices across various wavebands, owing to their unique characteristics, including optical [...] Read more.
Terahertz is one of the most promising technologies for high-speed communication and large-scale data transmission. As a classical optical component, ring resonators are extensively utilized in the design of band-pass and frequency-selective devices across various wavebands, owing to their unique characteristics, including optical comb generation, compactness, and low manufacturing cost. While substantial progress has been made in the study of ring resonators, their application in terahertz surface wave systems remains less than fully optimized. This paper presents several spoof surface plasmon polariton-based devices, which were realized using ring resonators at terahertz frequencies. The influence of both the radius of the ring resonator and the width of the waveguide coupling gap on the coupling coefficient are investigated. The band-stop filters based on the cascaded ring resonator exhibit a 0.005 THz broader frequency bandwidth compared to the single-ring resonator filter and achieve a minimum stopband attenuation of 28 dB. The add–drop multiplexers based on the asymmetric ring resonator enable selective surface wave outputs at different ports by rotating the ring resonator. The devices designed in this study offer valuable insights for the development of on-chip terahertz components. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Schematic of the device based on the RR, with geometrical parameters shown in the inset. (<b>b</b>) Dispersion relation of the spoof SPP modes for different periods <span class="html-italic">p</span>. (<b>c</b>) The normalized transmission spectra of an RR as a function of ring radius and gap width. Three sets of RR parameters: ring radius <span class="html-italic">R</span> = 700 μm and the gap width <span class="html-italic">g</span> = 40 μm, <span class="html-italic">R</span>−66 = 634 μm and <span class="html-italic">g</span> = 40 μm, and <span class="html-italic">R</span> = 700 μm and <span class="html-italic">g</span> + 30 = 70 μm. The black line is the fitting line. (<b>d</b>) The normalized simulated electric component |<span class="html-italic">E</span><sub>z</sub>| distribution at 0.529 THz. (<b>e</b>) The normalized transmittance of ports and minimum attenuation in stopband (red wire).</p>
Full article ">Figure 2
<p>(<b>a</b>) Coupling between a curved waveguide and a straight waveguide. (<b>b</b>) Setting the RR’s radius at <span class="html-italic">R</span>’ = 930 μm. The transmittances of curved waveguide are affected by changes in <span class="html-italic">g</span>, at 0.522 THz and 0.5315 THz.</p>
Full article ">Figure 3
<p>(<b>a</b>) Schematic of the band-stop filter with cascaded RRs. (<b>b</b>) Transmittance for a single RR with R = 634 μm and cascaded RRs with R<sub>1</sub> = 700 μm and R<sub>2</sub> = 634 μm, respectively. (<b>c</b>) The normalized port transmittance and stopband attenuation corresponding to frequencies. (<b>d</b>) The normalized simulated electric component |<span class="html-italic">E</span><sub>z</sub>| distribution at different frequencies.</p>
Full article ">Figure 4
<p>(<b>a</b>) Schematic diagram of the add–drop multiplexer. (<b>b</b>) The normalized transmittance of the pass port and the drop port.</p>
Full article ">Figure 5
<p>(<b>a</b>) Schematic diagram of add–drop multiplexer, with an asymmetric RR. (<b>b</b>) Comparison of the transmittance of <span class="html-italic">output1</span> and <span class="html-italic">output2</span> for ADM with different <span class="html-italic">θ</span> (<b>c</b>,<b>d</b>). The normalized simulated electric component |<span class="html-italic">E</span>z| distribution at 0.5315 THz for ADM with different <span class="html-italic">θ</span> of 0° and 180°, respectively.</p>
Full article ">Figure 6
<p>(<b>a</b>) Conceptual diagram and parameters of the add type coupled device. (<b>b</b>) The output loss of the port in the operating state of the device before and after rotation, respectively. (<b>c</b>,<b>d</b>) Normalized Ez electric field simulation before and after rotation, respectively, where z = 150 um.</p>
Full article ">
16 pages, 2064 KiB  
Systematic Review
The Application of Terahertz Technology in Corneas and Corneal Diseases: A Systematic Review
by Bing Jie Chow, Chang Liu, Mingyi Yu, Isabelle Xin Yu Lee, Jodhbir S. Mehta, Qing Yang Steve Wu, Regina Wong Kay Ting, Ke Lin and Yu-Chi Liu
Bioengineering 2025, 12(1), 45; https://doi.org/10.3390/bioengineering12010045 - 8 Jan 2025
Viewed by 555
Abstract
Terahertz (THz) waves reside in the electromagnetic spectrum between the microwave and infrared bands. In recent decades, THz technology has demonstrated its potential for biomedical applications. With the highly unique characteristics of THz waves, such as the high sensitivity to water and optimal [...] Read more.
Terahertz (THz) waves reside in the electromagnetic spectrum between the microwave and infrared bands. In recent decades, THz technology has demonstrated its potential for biomedical applications. With the highly unique characteristics of THz waves, such as the high sensitivity to water and optimal spatial resolution coupled with the characteristics of the human cornea, such as its high water content, THz technology has been explored as a potential modality to assess corneas and corneal diseases. This systematic review provides an overview of the characteristics of THz waves, the safety profile of THz technology in the field of ophthalmology, and its clinical applications, including the objective evaluation of the corneal hydration, tear film, dry eye disease, corneal endothelium, corneal elasticity, and scarring. The paper also presents our viewpoint on the present challenges and future directions of THz technology prior to its broader integration into clinical practice. Full article
(This article belongs to the Special Issue Bioengineering and the Eye—2nd Edition)
Show Figures

Figure 1

Figure 1
<p>Illustration of Terahertz Radiation in the electromagnetic spectrum. The figure was created with <a href="http://Biorender.com" target="_blank">Biorender.com</a>.</p>
Full article ">Figure 2
<p>Flow diagram of the literature selection process for the present article.</p>
Full article ">Figure 3
<p>The schematic diagram of the THz system used in cornea application.</p>
Full article ">Figure 4
<p>The changes in THz total intensity with time in two patients with DED (unpublished data from the authors).</p>
Full article ">Figure 5
<p>Illustration of THz spectroscopy and imaging of corneal scars in rabbits. (<b>A</b>) Slit lamp photos of a laser-induced scar (arrows). (<b>B</b>) THz 2 2D B-scan reconstructed images delineated the scar and demonstrated the scar density (unpublished data from the authors).</p>
Full article ">Figure 6
<p>Illustration of the potential clinical applications of THz technology in assessing corneal diseases. The figure was created with <a href="http://BioRender.com" target="_blank">BioRender.com</a>.</p>
Full article ">
57 pages, 2877 KiB  
Review
A Comprehensive Exploration of 6G Wireless Communication Technologies
by Md Nurul Absar Siddiky, Muhammad Enayetur Rahman, Md Shahriar Uzzal and H. M. Dipu Kabir
Computers 2025, 14(1), 15; https://doi.org/10.3390/computers14010015 - 3 Jan 2025
Viewed by 543
Abstract
As the telecommunications landscape braces for the post-5G era, this paper embarks on delineating the foundational pillars and pioneering visions that define the trajectory toward 6G wireless communication systems. Recognizing the insatiable demand for higher data rates, enhanced connectivity, and broader network coverage, [...] Read more.
As the telecommunications landscape braces for the post-5G era, this paper embarks on delineating the foundational pillars and pioneering visions that define the trajectory toward 6G wireless communication systems. Recognizing the insatiable demand for higher data rates, enhanced connectivity, and broader network coverage, we unravel the evolution from the existing 5G infrastructure to the nascent 6G framework, setting the stage for transformative advancements anticipated in the 2030s. Our discourse navigates through the intricate architecture of 6G, highlighting the paradigm shifts toward superconvergence, non-IP-based networking protocols, and information-centric networks, all underpinned by a robust 360-degree cybersecurity and privacy-by-engineering design. Delving into the core of 6G, we articulate a systematic exploration of the key technologies earmarked to revolutionize wireless communication including terahertz (THz) waves, optical wireless technology, and dynamic spectrum management while elucidating the intricate trade-offs necessitated by the integration of such innovations. This paper not only lays out a comprehensive 6G vision accentuated by high security, affordability, and intelligence but also charts the course for addressing the pivotal challenges of spectrum efficiency, energy consumption, and the seamless integration of emerging technologies. In this study, our goal is to enrich the existing discussions and research efforts by providing comprehensive insights into the development of 6G technology, ultimately supporting the creation of a thoroughly connected future world that meets evolving demands. Full article
Show Figures

Figure 1

Figure 1
<p>Communication networks evolution: 1G to a speculative 6G is observed through the lens of user experience.</p>
Full article ">Figure 2
<p>An overview of 6G architecture: a transition from 5G (adapted from [<a href="#B10-computers-14-00015" class="html-bibr">10</a>]). It streamlines computing, storage, and networking, introduces sliced local breakout for low-latency inter-operator connectivity, adds an AI-plane alongside U-Plane and C-Plane, and disaggregates 3GPP entities (PCF, AMF, and UPF) into cloud-based lambda functions.</p>
Full article ">Figure 3
<p>Comparative analysis of 5G versus 6G communications in terms of quality. Adopted from [<a href="#B1-computers-14-00015" class="html-bibr">1</a>], it is intended as a conceptual, high-level, qualitative illustration of the relative improvements anticipated with 6G as compared to 5G across multiple dimensions rather than actual numeral quantities.</p>
Full article ">Figure 4
<p>The 6G key performance indicators. Adopted from [<a href="#B24-computers-14-00015" class="html-bibr">24</a>].</p>
Full article ">Figure 5
<p>The overall features of 6G networks. The features are improved relative to 5G.</p>
Full article ">Figure 6
<p>Potential 6G application scenarios. Adopted from [<a href="#B24-computers-14-00015" class="html-bibr">24</a>].</p>
Full article ">Figure 7
<p>Categories of potential 6G application scenarios. Adopted from [<a href="#B42-computers-14-00015" class="html-bibr">42</a>].</p>
Full article ">Figure 8
<p>Depiction of a standard base station (BS) design for millimeter-wave and sub-6 GHz frequencies featuring radio/fiber technology. To prevent confusion, only a single antenna element is displayed. This illustration is adapted from [<a href="#B270-computers-14-00015" class="html-bibr">270</a>]. The abbreviations are power amplifier (PA), low-noise amplifier (LNA), intermediate frequency (IF), and microcontroller unit (MCU).</p>
Full article ">
12 pages, 3602 KiB  
Communication
Multi-Degree-of-Freedom Stretchable Metasurface Terahertz Sensor for Trace Cinnamoylglycine Detection
by Huanyu Li, Wenyao Yu, Mengya Pan, Shuo Liu, Wanxin Nie, Yifei Zhang and Yanpeng Shi
Biosensors 2024, 14(12), 602; https://doi.org/10.3390/bios14120602 - 9 Dec 2024
Viewed by 697
Abstract
Terahertz (THz) spectroscopy, an advanced label-free sensing method, offers significant potential for biomolecular detection and quantitative analysis in biological samples. Although broadband fingerprint enhancement compensates for limitations in detection capability and sensitivity, the complex optical path design in operation restricts its broader adoption. [...] Read more.
Terahertz (THz) spectroscopy, an advanced label-free sensing method, offers significant potential for biomolecular detection and quantitative analysis in biological samples. Although broadband fingerprint enhancement compensates for limitations in detection capability and sensitivity, the complex optical path design in operation restricts its broader adoption. This paper proposes a multi-degree-of-freedom stretchable metasurface that supports magnetic dipole resonance to enhance the broadband THz fingerprint detection of trace analytes. The metasurface substrate and unit cell structures are constructed using polydimethylsiloxane. By adjusting the sensor’s geometric dimensions or varying the incident angle within a narrow range, the practical optical path is significantly simplified. Simultaneously, the resonance frequency of the transmission curve is tuned, achieving high sensitivity for effectively detecting cinnamoylglycine. The results demonstrate that the metasurface achieves a high-quality factor of 770.6 and an excellent figure of merit of 777.2, significantly enhancing the THz sensing capability. Consequently, the detection sensitivity for cinnamoylglycine can reach 24.6 µg·cm−2. This study offers critical foundations for applying THz technology to biomedical fields, particularly detecting urinary biomarkers for diseases like gestational diabetes. Full article
(This article belongs to the Special Issue Flexible and Stretchable Electronics as Biosensors)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Structural view of an all-dielectric metasurface, showing the periodic arrangement of pure PDMS cubic clusters. (<b>b</b>) Unit cell of the periodic structure. (<b>c</b>) Schematic of the structure of the holder with the y-axis fixed and moving along the x-axis. (<b>d</b>) THz-TDS system based on a photoconductive antenna.</p>
Full article ">Figure 2
<p>(<b>a</b>) Metasurface transmission spectra at stretch factor S = 100% and S = 107%. (<b>b</b>) Electric and magnetic field distributions measured at the surface of the PDMS substrate at stretch factor S = 100%.</p>
Full article ">Figure 3
<p>(<b>a</b>) Effect of varying periodicity in the x-direction P<sub>x</sub> on the transmission curve. (<b>b</b>) Effect of varying periodicity in the y-direction P<sub>y</sub> on the transmission curve. (<b>c</b>) Impact of varying cube size w on the transmission curve. (<b>d</b>) Influence of varying substrate thickness t on the transmission curve. (<b>e</b>) Effect of varying inter-cube cluster distance L on the transmission curve. (<b>f</b>) Effect of varying cube cluster height h on the transmission curve.</p>
Full article ">Figure 4
<p>(<b>a</b>) Schematic diagram of the metasurface structure with the attached analyte as the stretching factor S varying from 100% to 130%. (<b>b</b>) Two-dimensional contour plot of the transmittance as a function of the stretching factor and frequency. (<b>c</b>) Normalized transmission spectra without analyte (stretching factor ranging from 100% to 130%).</p>
Full article ">Figure 5
<p>(<b>a</b>) Refractive index and complex refractive index of cinnamoylglycine in the THz band. (<b>b</b>) Stretch factor dependent transmission spectra of 0.6 µm thick cinnamoylglycine on a metasurface. (<b>c</b>) The electric field distribution measured at the substrate surface in the x–y plane at 0.487 THz for specific stretching factors S, corresponding to the transmission spectra shown in (<b>b</b>), respectively.</p>
Full article ">Figure 6
<p>(<b>a</b>) Normalized transmission spectra of 0.6 µm thick cinnamoylglycine with stretch factors ranging from 100% to 130%, the S values increasing by 1% between each curve. The corresponding envelopes have been plotted with red lines. (<b>b</b>) Transmission envelope curves for different thicknesses of analytes.</p>
Full article ">Figure 7
<p>(<b>a</b>) Schematic diagram of angle multiplexing in the x–z plane of the metasurface. (<b>b</b>) Normalized transmission spectra without any analyte, with angles of incidence ranging from 0° to 15°, the values increasing by 0.5° between each curve. (<b>c</b>) Integrated transmission spectrum of a 0.6 µm thick cinnamoylglycine film with incidence angles ranging from 0° to 15°, the values increasing by 0.5° between each curve. The corresponding envelope has been plotted with a red line.</p>
Full article ">
10 pages, 2457 KiB  
Article
Angle-Controlled Nanospectrum Switching from Lorentzian to Fano Lineshapes
by Fu Tang, Qinyang Zhong, Xiaoqiuyan Zhang, Yuxuan Zhuang, Tianyu Zhang, Xingxing Xu and Min Hu
Nanomaterials 2024, 14(23), 1932; https://doi.org/10.3390/nano14231932 - 30 Nov 2024
Viewed by 560
Abstract
The tunability of spectral lineshapes, ranging from Lorentzian to Fano profiles, is essential for advancing nanoscale photonic technologies. Conventional far-field techniques are insufficient for studying nanoscale phenomena, particularly within the terahertz (THz) range. In this work, we use a U-shaped resonant ring on [...] Read more.
The tunability of spectral lineshapes, ranging from Lorentzian to Fano profiles, is essential for advancing nanoscale photonic technologies. Conventional far-field techniques are insufficient for studying nanoscale phenomena, particularly within the terahertz (THz) range. In this work, we use a U-shaped resonant ring on a waveguide substrate to achieve precise modulation of Lorentzian, Fano, and antiresonance profiles. THz scattering scanning near-field optical microscopy (s-SNOM) reveals the underlying physical mechanism of these transitions, driven by time-domain phase shifts between the background excitation from the waveguide and the resonance of the U-shaped ring. Our approach reveals a pronounced asymmetry in the near-field response, which remains undetectable in far-field systems. The ability to control spectral lineshapes at the nanoscale presents promising applications in characterizing composite nanoresonators and developing nanoscale phase sensors. Full article
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Schematic diagram of the THz s-SNOM system. (<b>b</b>) Optical image and (<b>c</b>) second-order near-field white-light image of the U-shaped ring.</p>
Full article ">Figure 2
<p>(<b>a</b>) Experimental real of the near-field spectra from 0° to 90°. (<b>b</b>) Experimental and Fano formula fitted imaginary near-field spectra from 0° to 90°. (<b>c</b>) Simulated imaginary part of the spectrum as the U-shaped ring rotates from 0° to 90°. (<b>d</b>) Fano parameters <span class="html-italic">q</span> of experimental and simulated imaginary parts of the spectrum.</p>
Full article ">Figure 3
<p>(<b>a</b>) Near-field time-domain signal from 0° to 90°, (<b>b</b>,<b>c</b>) The enlarged view of the highlighted region of (<b>a</b>).</p>
Full article ">Figure 4
<p>(<b>a</b>,<b>b</b>) Near-field spectra with the tip positioned in the left arm of the U-shaped ring, showing the real (<b>a</b>) and imaginary (<b>b</b>) parts from 0° to 180°. (<b>c</b>,<b>d</b>) Near-field spectra with the tip positioned in the right arm of the U-shaped ring, showing the real (<b>c</b>) and imaginary (<b>d</b>) parts from 0° to 180°.</p>
Full article ">Figure 5
<p>Simulated real (<b>a</b>) and imaginary parts (<b>b</b>) of the spectrum for waveguide substrate thicknesses <span class="html-italic">Z</span> from 8 to 28 µm. Simulated real (<b>c</b>) and imaginary parts (<b>d</b>) of the spectrum for <span class="html-italic">L</span> from 20 to 45 µm.</p>
Full article ">
19 pages, 16285 KiB  
Article
Sub-Terahertz Imaging-Based Real-Time Non-Destructive Inspection System for Estimating Water Activity and Foreign Matter Depth in Seaweed
by Dong-Hoon Kwak, Ho-Won Yun, Jong-Hun Lee, Young-Duk Kim and Doo-Hyun Choi
Sensors 2024, 24(23), 7599; https://doi.org/10.3390/s24237599 - 28 Nov 2024
Viewed by 549
Abstract
As the importance of hygiene and safety management in food manufacturing has been increasingly emphasized, research on non-destructive and non-contact inspection technologies has become more active. This study proposes a real-time and non-destructive food inspection system with sub-terahertz waves which penetrates non-conducting materials [...] Read more.
As the importance of hygiene and safety management in food manufacturing has been increasingly emphasized, research on non-destructive and non-contact inspection technologies has become more active. This study proposes a real-time and non-destructive food inspection system with sub-terahertz waves which penetrates non-conducting materials by using a frequency of 0.1 THz. The proposed system detects not only the presence of foreign matter, but also the degree of depth to which it is mixed in foods. In addition, the system estimates water activity levels, which serves as the basis for assessing the freshness of seaweed by analyzing the transmittance of signals within the sub-terahertz image. The system employs YOLOv8n, which is one of the newest lightweight object detection models. This lightweight model utilizes the feature pyramid network (FPN) to effectively detect objects of various sizes while maintaining a fast processing speed and high performance. In particular, to validate the performance in real manufacturing facilities, we implemented a hardware platform, which accurately inspects seaweed products while cooperating with a conveyor device moving at a speed of 45 cm/s. For the validation of the estimation performance against various water activities and the degree of depth of foreign matter, we gathered and annotated a total of 9659 sub-terahertz images and optimized the learning model. The final results show that the precision rate is 0.91, recall rate is 0.95, F1-score is 0.93, and mAP is 0.97, respectively. Overall, the proposed system demonstrates an excellent performance in the detection of foreign matter and in freshness estimation, and can be applied in several applications regarding food safety. Full article
(This article belongs to the Special Issue Innovative Sensors and Embedded Sensor Systems for Food Analysis)
Show Figures

Figure 1

Figure 1
<p>Detailed configuration of the entire system.</p>
Full article ">Figure 2
<p>Sub-terahertz seaweed image from different belts: (<b>a</b>) transparent belt and (<b>b</b>) opaque belt.</p>
Full article ">Figure 3
<p>A tot of dried seaweed.</p>
Full article ">Figure 4
<p>Comparison of signal intensity.</p>
Full article ">Figure 5
<p>Post-compensated sub-terahertz images: (<b>a</b>) seaweed and (<b>b</b>) seaweed with foreign matter.</p>
Full article ">Figure 6
<p>Depth range of each class: (<b>a</b>) TB (<b>b</b>), TMB, and (<b>c</b>) thickness of seaweed.</p>
Full article ">Figure 7
<p>Proportion of acquired data: (<b>a</b>) TB Type and (<b>b</b>) TMB Type.</p>
Full article ">Figure 8
<p>Example of sub-terahertz image annotation.</p>
Full article ">Figure 9
<p>Proportions of the divided dataset.</p>
Full article ">Figure 10
<p>Architecture of YOLOv8.</p>
Full article ">Figure 11
<p>PR curve, each class’s AP and mAP: (<b>a</b>) TB model and (<b>b</b>) TMB model.</p>
Full article ">Figure 12
<p>Inspection platform operation example: (<b>a</b>) safe product and (<b>b</b>) defective product.</p>
Full article ">Figure 13
<p>Platform operation scene.</p>
Full article ">
11 pages, 3441 KiB  
Article
THz Polarimetric Imaging of Carbon Fiber-Reinforced Composites Using the Portable Handled Spectral Reflection (PHASR) Scanner
by Kuangyi Xu, Zachery B. Harris, Paul Vahey and M. Hassan Arbab
Sensors 2024, 24(23), 7467; https://doi.org/10.3390/s24237467 - 22 Nov 2024
Viewed by 564
Abstract
Recent advancements in novel fiber-coupled and portable terahertz (THz) spectroscopic imaging technology have accelerated applications in nondestructive testing (NDT). Although the polarization information of THz waves can play a critical role in material characterization, there are few demonstrations of polarization-resolved THz imaging as [...] Read more.
Recent advancements in novel fiber-coupled and portable terahertz (THz) spectroscopic imaging technology have accelerated applications in nondestructive testing (NDT). Although the polarization information of THz waves can play a critical role in material characterization, there are few demonstrations of polarization-resolved THz imaging as an NDT modality due to the deficiency of such polarimetric imaging devices. In this paper, we have inspected industrial carbon fiber composites using a portable and handheld imaging scanner in which the THz polarizations of two orthogonal channels are simultaneously captured by two photoconductive antennas. We observed significant polarimetric differences between the two-channel images of the same sample and the resulting THz Stokes vectors, which are attributed to the anisotropic conductivity of carbon fiber composites. Using both polarimetric channels, we can visualize the superficial and underlying interfaces of the first laminate. These results pave the way for the future applications of THz polarimetry to the assessment of coatings or surface quality on carbon fiber-reinforced substrates. Full article
(This article belongs to the Special Issue Millimeter Wave and Terahertz Source, Sensing and Imaging)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) Front surface of the first test panel from Boeing Company. (<b>b</b>) Microscopic image (10×) of the bare substrate, appearing as unidirectional CFRP.</p>
Full article ">Figure 2
<p>(<b>a</b>) Back surface of the second test panel from Boeing Company. (<b>b</b>) Microscopic image (2.5×) of the back surface, appearing as interwoven (plain-weaved) CFRP.</p>
Full article ">Figure 3
<p>(<b>a</b>) The THz signals reflected from unidirectional CFRP at the sample orientations of 0° and 90°, corresponding to the TM and TE modes of polarization, respectively. The dashed box shows the difference in the propagation of the TE and TM modes in a single CFRP ply. (<b>b</b>,<b>c</b>) are the spectra of reflectivity and impulse responses retrieved from signals in (<b>a</b>). (<b>d</b>) The impulse responses are measured at different locations of interwoven CFRP, where the fiber orientations are different.</p>
Full article ">Figure 4
<p>Cross-section images (B-scan) of (<b>a</b>) the unidirectional CFRP and the interwoven CFRP in the (<b>b</b>) X and (<b>c</b>) Y channels. The colors are on the same scale and have been extended to [−1, 1].</p>
Full article ">Figure 5
<p>(<b>a</b>) Photo of the interwoven CFRP, top view. (<b>b</b>,<b>c</b>) are the C-scanned THz images of the X channel, at the optical depths of z = 0 and z = 0.52 mm, respectively. (<b>d</b>,<b>e</b>) are the correlated images of the Y channel, at the optical depths of z = 0 and z = 0.60 mm, respectively.</p>
Full article ">Figure 6
<p>The spatial variation in the Stokes parameters <span class="html-italic">I</span>, <span class="html-italic">Q</span>, <span class="html-italic">U</span>, and <span class="html-italic">V</span> for the interwoven CFRP at different frequencies. <span class="html-italic">I</span> is in arbitrary units while the other Stokes parameters are normalized by <span class="html-italic">I</span>.</p>
Full article ">Figure 7
<p>(<b>a</b>) Two ROIs (blue and red) are selected in the C-scan images of interwoven CFRP. (<b>b</b>) The mean value and standard deviation of the reflectivity in the two ROIs. (<b>c</b>–<b>f</b>) The distribution of pixels in the 2D plane of |R<sub>x</sub>| and |R<sub>y</sub>|, indicating the separation of orthogonal fibers in the 0.4–0.6 THz range.</p>
Full article ">
19 pages, 7130 KiB  
Review
Recent Trend of Rate-Splitting Multiple Access-Assisted Integrated Sensing and Communication Systems
by Sukbin Jang, Nahyun Kim, Gayeong Kim and Byungju Lee
Electronics 2024, 13(23), 4579; https://doi.org/10.3390/electronics13234579 - 21 Nov 2024
Viewed by 1011
Abstract
In the next-generation communication systems, multiple access (MA) will play a crucial role in achieving high throughput to support future-oriented services. Recently, rate-splitting multiple access (RSMA) has received much attention from both academia and industry due to its ability to flexibly mitigate inter-user [...] Read more.
In the next-generation communication systems, multiple access (MA) will play a crucial role in achieving high throughput to support future-oriented services. Recently, rate-splitting multiple access (RSMA) has received much attention from both academia and industry due to its ability to flexibly mitigate inter-user interference in a broad range of interference regimes. Further, with the growing emphasis on spectrum resource utilization, integrated sensing and communication (ISAC) technology, which improves spectrum efficiency by merging communication and radar signals, is expected to be one of the key candidate technologies for the sixth-generation (6G) wireless networks. In this paper, we first investigate the evolution of existing MA techniques and basic principles of RSMA-assisted ISAC systems. Moreover, to make the future RSMA-assisted ISAC systems, we highlight prime technologies of 6G such as non-terrestrial networks (NTN), reconfigurable intelligent surfaces (RIS), millimeter wave (mmWave) and terahertz (THz) technologies, and vehicular-to-everything (V2X), along with the main technical challenges and potential benefits to pave the way for RSMA-assisted ISAC systems. Full article
(This article belongs to the Special Issue Multi-Scale Communications and Signal Processing)
Show Figures

Figure 1

Figure 1
<p>Evolution of mobile communication from 1G to 6G.</p>
Full article ">Figure 2
<p>Resource allocation for various MA technologies.</p>
Full article ">Figure 3
<p>RSMA tranceiver architecture.</p>
Full article ">Figure 4
<p>RSMA-assisted ISAC systems.</p>
Full article ">Figure 5
<p>RSMA-assisted LEO-ISAC systems.</p>
Full article ">Figure 6
<p>RSMA-assisted RIS-ISAC systems.</p>
Full article ">Figure 7
<p>RSMA-assisted ISAC systems with hybrid beamforming.</p>
Full article ">
14 pages, 5927 KiB  
Article
Terahertz Spectroscopy in Assessing Temperature-Shock Effects on Citrus
by Junbo Wang, Ziyi Zang, Xiaomei Li, Dongyun Tang, Qi Xiao, Mingkun Zhang and Shihan Yan
Sensors 2024, 24(22), 7315; https://doi.org/10.3390/s24227315 - 15 Nov 2024
Viewed by 562
Abstract
Rapid assessment of physiological status is a precondition for addressing biological stress in trees so that they may recover. Environmental stress can cause water deficit in plants, while terahertz (THz) spectroscopy is sensitive to changes in aqueous solutions within organisms. This has given [...] Read more.
Rapid assessment of physiological status is a precondition for addressing biological stress in trees so that they may recover. Environmental stress can cause water deficit in plants, while terahertz (THz) spectroscopy is sensitive to changes in aqueous solutions within organisms. This has given the THz sensor a competitive edge for evaluating plant phenotypes, especially under similar environmental stress, if there are existing differences in the corresponding THz information. In this study, we utilized THz technology in association with traditional weighing methods to explore physiological changes in citrus leaves under different temperature, duration, and stress treatment conditions. It was found that the higher the temperature and the longer the exposure duration, the more severe the reduction in the relative absorption coefficient. There was a positive correlation between the trends and the increase in the ion permeability of cells. In addition, based on the effective medium theory, THz spectral information can be transformed into information on free water and bound water in the leaves. Under different treatment conditions, water content shows different trends and degrees of change on the time scale, and accuracy was verified by traditional weighing methods. These findings revealed that characteristics of THz information can serve as a simple and clear indicator for judging a plant’s physiological status. Full article
Show Figures

Figure 1

Figure 1
<p>Schematic diagram of the experimental process.</p>
Full article ">Figure 2
<p>THz-TDS system (<b>a</b>), THz spectral measurement in working mode (<b>b</b>), and sample holder with leaf sample (<b>c</b>).</p>
Full article ">Figure 3
<p>Relative absorption coefficient of leaves after high−temperature stress at 30 °C (<b>a</b>), 35 °C (<b>b</b>), 40 °C (<b>c</b>) for 1, 2, 4, 6 and 16 h, and (<b>d</b>) linear fitting curves. The original reference zero is shown as red dashed line.</p>
Full article ">Figure 4
<p>Volume fraction of water, free water, and bound water and the ratio of bound water and free water in leaves after high-temperature stress at 30 °C, 35 °C, and 40 °C for 1, 2, 4, 6, and 16 h based on THz spectroscopy.</p>
Full article ">Figure 5
<p>Correlation analysis of relative electrolyte leakage rate and relative absorption coefficient.</p>
Full article ">Figure 6
<p>Correlation analysis of leaf WC (<b>a</b>), FWC (<b>b</b>), BWC (<b>c</b>), and BWC/FWC (<b>d</b>) content measured using THz spectroscopy and gravimetric methods.</p>
Full article ">Figure 7
<p>Linear fitting curves of relative absorption coefficients of leaves under five consecutive intermittent high−temperature cycles.</p>
Full article ">Figure 8
<p>Relative change in volume fraction of water, free water, bound water, and the ratio of bound water and free water in leaves under 5 consecutive intermittent high−temperature cycles at 30 °C, 35 °C, and 40 °C using THz spectroscopy.</p>
Full article ">
29 pages, 8732 KiB  
Review
Microfabrication Technologies for Interaction Circuits of THz Vacuum Electronic Devices
by Xinghui Li and Jinjun Feng
Micromachines 2024, 15(11), 1357; https://doi.org/10.3390/mi15111357 - 8 Nov 2024
Viewed by 1913
Abstract
Advances in manufacturing technology are allowing for the realization of interaction circuit with microstructures. The capability to produce small circuit structures is allowing new opportunities for vacuum electronic devices producing terahertz (THz) frequency radiation, which is impractical with traditional machining technology. This publication [...] Read more.
Advances in manufacturing technology are allowing for the realization of interaction circuit with microstructures. The capability to produce small circuit structures is allowing new opportunities for vacuum electronic devices producing terahertz (THz) frequency radiation, which is impractical with traditional machining technology. This publication reviews recent progress on advanced microfabrication technologies applicable to interaction circuits of THz vacuum electronic devices, including LIGA/UV-LIGA (Ultraviolet Lithographic, Galvonoformung and Abformung), deep reactive ion etching (DRIE), micro/nano computer numerical control (CNC) milling, three-dimension (3D) printing, etc., and describes the current State-of-the-Art of their applications. Full article
(This article belongs to the Special Issue Recent Advances in Terahertz Devices and Applications)
Show Figures

Figure 1

Figure 1
<p>Conceptual illustration of a THz vacuum electron amplifier (oscillator).</p>
Full article ">Figure 2
<p>Diagrammatic illustration of a folded waveguide.</p>
Full article ">Figure 3
<p>Process flow diagram of LIGA.</p>
Full article ">Figure 4
<p>Scanning electron microscope images of (<b>a</b>) two-step LIGA-fabricated FWG and (<b>b</b>) post-LIGA machined FWG [<a href="#B49-micromachines-15-01357" class="html-bibr">49</a>].</p>
Full article ">Figure 5
<p>Trial 300 GHz FWG fabricated with X-ray LIGA [<a href="#B50-micromachines-15-01357" class="html-bibr">50</a>].</p>
Full article ">Figure 6
<p>SEM photo of 850 GHz FWG circuit; scale bar, 100 μm; scale bar in insert, 10 μm [<a href="#B51-micromachines-15-01357" class="html-bibr">51</a>].</p>
Full article ">Figure 7
<p>220 GHz FWG fabricated by UV-LIGA with electron channel fabricated by EDM.</p>
Full article ">Figure 8
<p>W-band FWG fabricated by two-step UV-LIGA process.</p>
Full article ">Figure 9
<p>Embedded polymer monofilament concept. (<b>a</b>) The monofilament is set, (<b>b</b>) photoresist is applied, (<b>c</b>) UV-exposure and developing, (<b>d</b>) electroforming metal, (<b>e</b>) removal of the monofilament and photoresist [<a href="#B73-micromachines-15-01357" class="html-bibr">73</a>].</p>
Full article ">Figure 10
<p>Schematic of Bosch method: Sidewall passivation using C<sub>4</sub>F<sub>8</sub> and silicon isotropic etching using SF<sub>6</sub>.</p>
Full article ">Figure 11
<p>Process flow diagram of DRIE for interaction circuit fabrication.</p>
Full article ">Figure 12
<p>(<b>a</b>) Cross-sectional SEM image of a multi-level interaction circuit; scale bar, 1 mm; (<b>b</b>) SEM image of etched bottom layer; scale bar, 5 μm [<a href="#B115-micromachines-15-01357" class="html-bibr">115</a>].</p>
Full article ">Figure 13
<p>340 GHz FWG with modified circular bends fabricated by micro/nano CNC milling.</p>
Full article ">Figure 14
<p>SEM images of helical slow-wave circuits for (<b>a</b>,<b>b</b>) the 95 GHz TWT and (<b>c</b>,<b>d</b>) the 650 GHz BWO [<a href="#B164-micromachines-15-01357" class="html-bibr">164</a>].</p>
Full article ">Figure 15
<p>Schematic of planar microstrip meander line slow-wave structure.</p>
Full article ">
13 pages, 1510 KiB  
Article
A Three-Dimensional Time-Varying Channel Model for THz UAV-Based Dual-Mobility Channels
by Kai Zhang, Fenglei Zhang, Yongjun Li, Xiang Wang, Zhaohui Yang, Yuanhao Liu, Changming Zhang and Xin Li
Entropy 2024, 26(11), 924; https://doi.org/10.3390/e26110924 - 30 Oct 2024
Viewed by 642
Abstract
Unmanned aerial vehicle (UAV) as an aerial base station or relay device is a promising technology to rapidly provide wireless connectivity to ground device. Given UAV’s agility and mobility, ground user’s mobility, a key question is how to analyze and value the performance [...] Read more.
Unmanned aerial vehicle (UAV) as an aerial base station or relay device is a promising technology to rapidly provide wireless connectivity to ground device. Given UAV’s agility and mobility, ground user’s mobility, a key question is how to analyze and value the performance of UAV-based wireless channel in the terahertz (THz) band. In this paper, a three-dimensional (3D) time-varying channel model is proposed for UAV-based dual-mobility wireless channels based on geometric channel model theory in THz band. In this proposed channel model, the small-scale fading (e.g., scattering fading and reflection fading) on rough surfaces of communication environment and the atmospheric molecule absorption attenuations are considered in THz band. Moreover, the statistical properties of the proposed channel model, including path loss, time autocorrelation function (T-ACF) and Doppler power spectrum density (DPSD), have been derived and the impact of several important UAV-related and vehicle-related parameters have been investigated and compared to millimeter wave (mm-wave) band. Furthermore, the correctness of the proposed channel model has been verified via simulation, and some useful observations are provided for the system design of THz UAV-based dual-mobility wireless communication systems. Full article
Show Figures

Figure 1

Figure 1
<p>Real UAV-based dual-mobility wireless communications scenario in the THz band.</p>
Full article ">Figure 2
<p>Different propagation paths between UAV and vehicle in time-varying UAV-based wireless communication system in the THz band: (<b>a</b>) LoS propagation path survival; (<b>b</b>) LoS propagation path death and NLoS propagation path birth.</p>
Full article ">Figure 3
<p>The T-ACF with different moving speeds of Tx and Rx for the NLoS path (including reflection and scattering paths).</p>
Full article ">Figure 4
<p>The T-ACF with different vertical distance of Tx and Rx for the NLoS path (including reflection and scattering paths).</p>
Full article ">Figure 5
<p>The T-ACF with different power ratio of reflection and scattering propagations for the NLoS path (including reflection and scattering paths).</p>
Full article ">Figure 6
<p>The T-ACF with different Ricican <span class="html-italic">K</span>-factor.</p>
Full article ">Figure 7
<p>Path loss of the MPCs (including LoS, reflection, and scattering paths) with different carrier frequencies.</p>
Full article ">Figure 8
<p>The DPSD with different moving times and different paths.</p>
Full article ">
21 pages, 7437 KiB  
Review
A Review of Thermal Detectors of THz Radiation Operated at Room Temperature
by Zbigniew Bielecki, Janusz Mikolajczyk and Jacek Wojtas
Sensors 2024, 24(21), 6784; https://doi.org/10.3390/s24216784 - 22 Oct 2024
Viewed by 3306
Abstract
This article concerns optical detection issues in the terahertz (THz) range. This is a kind of guide to various types of uncooled thermal detectors in the most often applications. Particular attention is paid to the principle of their operation, technology, and practical features. [...] Read more.
This article concerns optical detection issues in the terahertz (THz) range. This is a kind of guide to various types of uncooled thermal detectors in the most often applications. Particular attention is paid to the principle of their operation, technology, and practical features. In addition, some detection methods were also characterized by comparing their performances. The article ends with a performance summary of the selected THz thermal detectors. Full article
(This article belongs to the Special Issue Research Development in Terahertz and Infrared Sensing Technology)
Show Figures

Figure 1

Figure 1
<p>The electromagnetic spectrum [<a href="#B1-sensors-24-06784" class="html-bibr">1</a>].</p>
Full article ">Figure 2
<p>Scheme of explored and future THz applications [<a href="#B2-sensors-24-06784" class="html-bibr">2</a>].</p>
Full article ">Figure 3
<p>Classification of THz detectors (adopted after [<a href="#B5-sensors-24-06784" class="html-bibr">5</a>]), where CMOS is a complementary metal–oxide–semiconductor.</p>
Full article ">Figure 4
<p>(<b>a</b>) Thermal detector: scheme of operation [<a href="#B8-sensors-24-06784" class="html-bibr">8</a>]; (<b>b</b>) the main steps of the detection procedure.</p>
Full article ">Figure 5
<p>Thermal detectors used for THz detection.</p>
Full article ">Figure 6
<p>A simplified schematic of the direct detection method.</p>
Full article ">Figure 7
<p>(<b>a</b>) The schematic principle of Golay cell [<a href="#B19-sensors-24-06784" class="html-bibr">19</a>]; (<b>b</b>) photo of Golay detector [<a href="#B20-sensors-24-06784" class="html-bibr">20</a>].</p>
Full article ">Figure 8
<p>Cross-section of the Golay detector structure [<a href="#B22-sensors-24-06784" class="html-bibr">22</a>].</p>
Full article ">Figure 9
<p>(<b>a</b>) Diagram of the thermopile; (<b>b</b>) cross-section of the thermopile with a single/dual structure [<a href="#B7-sensors-24-06784" class="html-bibr">7</a>,<a href="#B23-sensors-24-06784" class="html-bibr">23</a>].</p>
Full article ">Figure 10
<p>(<b>a</b>) Structure view of the CMOS–MEMS thermopile [<a href="#B27-sensors-24-06784" class="html-bibr">27</a>]; (<b>b</b>) an image of the Si nanomembrane thermal detectors [<a href="#B28-sensors-24-06784" class="html-bibr">28</a>].</p>
Full article ">Figure 11
<p>(<b>a</b>) Conceptual diagram of BBR-based PTE passive liquid monitoring with the device; device responses during liquid flowing (<b>b</b>) in different temperatures and (<b>c</b>) in different viscosities (adopted after [<a href="#B29-sensors-24-06784" class="html-bibr">29</a>]).</p>
Full article ">Figure 12
<p>(<b>a</b>) Fundamental structure of a bolometer; (<b>b</b>) temperature dependence of resistance of three bolometer material types [<a href="#B30-sensors-24-06784" class="html-bibr">30</a>].</p>
Full article ">Figure 13
<p>Bolometric THz detector with metallic absorber where AR is the antireflective coating, <span class="html-italic">s</span>—substrate, <span class="html-italic">b</span>—bolometer (<span class="html-italic">h</span>—vacuum gap, <span class="html-italic">d</span>—dielectric membrane, <span class="html-italic">a</span>—metallic THz absorber), <span class="html-italic">g</span>—vacuum gap, <span class="html-italic">r</span>—reflector, <span class="html-italic">w</span>—window [<a href="#B33-sensors-24-06784" class="html-bibr">33</a>].</p>
Full article ">Figure 14
<p>Structure of single pixel in THz focal plane array (FPA) [<a href="#B35-sensors-24-06784" class="html-bibr">35</a>].</p>
Full article ">Figure 15
<p>(<b>a</b>) A schematic view of the antenna-coupled Ti-microbolometer; (<b>b</b>) a flat-top view of the central part of THz antenna; (<b>c</b>) the side 3D view [<a href="#B38-sensors-24-06784" class="html-bibr">38</a>].</p>
Full article ">Figure 16
<p>(<b>a</b>) A schematic view of a double-clamped MEMS beam resonator as a sensitive thermistor [<a href="#B39-sensors-24-06784" class="html-bibr">39</a>]; (<b>b</b>) an ultrasensitive micromechanical resonator bolometer using a Si<sub>3</sub>N<sub>4</sub> trampoline [<a href="#B41-sensors-24-06784" class="html-bibr">41</a>].</p>
Full article ">Figure 17
<p>(<b>a</b>) Scheme of a pyroelectric detector; (<b>b</b>) QMC Instruments Ltd. (Cardiff, UK) room-temperature pyroelectric THz detector [<a href="#B44-sensors-24-06784" class="html-bibr">44</a>].</p>
Full article ">Figure 18
<p>(<b>a</b>) Scheme of the pyroelectric detector with an integrated resonant absorber; (<b>b</b>) the absorptivity of the absorber [<a href="#B50-sensors-24-06784" class="html-bibr">50</a>].</p>
Full article ">Figure 19
<p>The sensitivity of the Lasertechnik pyroelectric detectors normalized to the sensitivity at 1 THz (adopted after [<a href="#B55-sensors-24-06784" class="html-bibr">55</a>]).</p>
Full article ">Figure 20
<p>Examples of measured transmission spectra for some standard filters. BP means filter model, and the number means the central frequency (adopted after [<a href="#B55-sensors-24-06784" class="html-bibr">55</a>]).</p>
Full article ">Figure 21
<p>Parameters comparison of commercially available detection heads (red circles—sensitivity, blue squares—maximum power).</p>
Full article ">Figure 22
<p>Spectral operation range of some THz thermal detectors. Refs. [<a href="#B35-sensors-24-06784" class="html-bibr">35</a>,<a href="#B38-sensors-24-06784" class="html-bibr">38</a>,<a href="#B50-sensors-24-06784" class="html-bibr">50</a>,<a href="#B67-sensors-24-06784" class="html-bibr">67</a>,<a href="#B76-sensors-24-06784" class="html-bibr">76</a>,<a href="#B77-sensors-24-06784" class="html-bibr">77</a>,<a href="#B78-sensors-24-06784" class="html-bibr">78</a>] are cited in the figure.</p>
Full article ">
16 pages, 3710 KiB  
Article
Experimental Analysis of Terahertz Wave Scattering Characteristics of Simulated Lunar Regolith Surface
by Suyun Wang and Kazuma Hiramatsu
Remote Sens. 2024, 16(20), 3819; https://doi.org/10.3390/rs16203819 - 14 Oct 2024
Cited by 1 | Viewed by 862
Abstract
This study investigates terahertz (THz) wave scattering from a simulated lunar regolith surface, with a focus on the Brewster feature, backscattering, and bistatic scattering within the 325 to 500 GHz range. We employed a generalized power-law spectrum to characterize surface roughness and fabricated [...] Read more.
This study investigates terahertz (THz) wave scattering from a simulated lunar regolith surface, with a focus on the Brewster feature, backscattering, and bistatic scattering within the 325 to 500 GHz range. We employed a generalized power-law spectrum to characterize surface roughness and fabricated Gaussian correlated surfaces from Durable Resin V2 using 3D printing technology. The complex dielectric permittivity of these materials was determined through THz time-domain spectroscopy (THz-TDS). Our experimental setup comprised a vector network analyzer (VNA) equipped with dual waveguide frequency extenders for the WR-2.2 band, transmitter and receiver modules, polarizing components, and a scattering chamber. We systematically analyzed the effects of root-mean-square (RMS) height, correlation length, dielectric constant, frequency, polarization, and observation angle on THz scattering. The findings highlight the significant impact of surface roughness on the Brewster angle shift, backscattering, and bistatic scattering. These insights are crucial for refining theoretical models and developing algorithms to retrieve physical parameters for lunar and other celestial explorations. Full article
(This article belongs to the Special Issue Future of Lunar Exploration)
Show Figures

Figure 1

Figure 1
<p>The geometry of wave scattering from rough surface.</p>
Full article ">Figure 2
<p>The rough surface samples are designed with specified RMS heights and correlation lengths.</p>
Full article ">Figure 3
<p>The measured dielectric constant of the material by THz-TDS.</p>
Full article ">Figure 4
<p>The roughness validation of one selected rough surface with an RMS height of 0.8<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and a correlation length of 2<math display="inline"><semantics> <mi>λ</mi> </semantics></math>.</p>
Full article ">Figure 5
<p>The experiment configuration.</p>
Full article ">Figure 6
<p>The polarizer consists of three reflectors.</p>
Full article ">Figure 7
<p>The comparison between the simulated and experimental HH and VV reflections from a flat surface with a dielectric constant of <math display="inline"><semantics> <mrow> <mn>2.597</mn> <mo>+</mo> <mi>j</mi> <mn>0.165</mn> </mrow> </semantics></math>.</p>
Full article ">Figure 8
<p>The frequency effect on THz scattering from rough surface.</p>
Full article ">Figure 9
<p>The correlation length effect on THz scattering from rough surface. (<b>a</b>) <math display="inline"><semantics> <mi>σ</mi> </semantics></math> = 0.8<math display="inline"><semantics> <mi>λ</mi> </semantics></math> (<b>b</b>) <math display="inline"><semantics> <mi>σ</mi> </semantics></math> = 0.1<math display="inline"><semantics> <mi>λ</mi> </semantics></math>.</p>
Full article ">Figure 10
<p>The RMS height effect on THz scattering from rough surface. (<b>a</b>) <span class="html-italic">l</span> = 2<math display="inline"><semantics> <mi>λ</mi> </semantics></math> (<b>b</b>) <span class="html-italic">l</span> = 0.4<math display="inline"><semantics> <mi>λ</mi> </semantics></math>.</p>
Full article ">Figure 11
<p>Comparison of bistatic scattering from flat and rough surfaces with RMS heights of 0.5<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and 0.8<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and a fixed correlation length of 2<math display="inline"><semantics> <mi>λ</mi> </semantics></math> at incident angles of 30°, 45°, and 60° for both HH and VV polarizations.</p>
Full article ">Figure 12
<p>Comparison of bistatic scattering from flat and rough surfaces with RMS heights of 0.1<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and 0.08<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and a fixed correlation length of 0.4<math display="inline"><semantics> <mi>λ</mi> </semantics></math> at incident angles of 30°, 45°, and 60° for both HH and VV polarizations.</p>
Full article ">Figure 13
<p>Comparison of bistatic scattering from the flat surface and rough surface with different correlation lengths of 2<math display="inline"><semantics> <mi>λ</mi> </semantics></math>, 4<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and 6<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and a fixed RMS height of 0.8<math display="inline"><semantics> <mi>λ</mi> </semantics></math> at the incident angle of 30°, 45° and 60° for HH and VV polarizations.</p>
Full article ">Figure 14
<p>Comparison of bistatic scattering from rough surfaces with correlation lengths of 1.5<math display="inline"><semantics> <mi>λ</mi> </semantics></math>, 1<math display="inline"><semantics> <mi>λ</mi> </semantics></math>, and 0.4<math display="inline"><semantics> <mi>λ</mi> </semantics></math> and a fixed RMS height of 0.1<math display="inline"><semantics> <mi>λ</mi> </semantics></math> at incident angles of 30°, 45°, and 60° for both HH and VV polarizations.</p>
Full article ">Figure 15
<p>Comparison of three different incident angles 30°, 45°, and 60° for HH and VV polarizations from a Gaussian correlated surface of <span class="html-italic">l</span> = 1.0 <math display="inline"><semantics> <mi>λ</mi> </semantics></math>, <math display="inline"><semantics> <mi>σ</mi> </semantics></math> = 0.1 <math display="inline"><semantics> <mi>λ</mi> </semantics></math>. ((<b>left</b>): VV polarization, (<b>right</b>): HH polarization).</p>
Full article ">Figure 16
<p>Comparison of three different incident angles 30°, 45°, and 60° for HH and VV polarizations from a Gaussian correlated surface of <span class="html-italic">l</span> = 2.0 <math display="inline"><semantics> <mi>λ</mi> </semantics></math>, <math display="inline"><semantics> <mi>σ</mi> </semantics></math> = 0.5 <math display="inline"><semantics> <mi>λ</mi> </semantics></math>. ((<b>left</b>): VV polarization, (<b>right</b>): HH polarization).</p>
Full article ">
10 pages, 3134 KiB  
Communication
All-Dielectric Metasurface-Based Terahertz Molecular Fingerprint Sensor for Trace Cinnamoylglycine Detection
by Qiyuan Xu, Mingjun Sun, Weijin Wang and Yanpeng Shi
Biosensors 2024, 14(9), 440; https://doi.org/10.3390/bios14090440 - 13 Sep 2024
Cited by 1 | Viewed by 1314
Abstract
Terahertz (THZ) spectroscopy has emerged as a superior label-free sensing technology in the detection, identification, and quantification of biomolecules in various biological samples. However, the limitations in identification and discrimination sensitivity of current methods impede the wider adoption of this technology. In this [...] Read more.
Terahertz (THZ) spectroscopy has emerged as a superior label-free sensing technology in the detection, identification, and quantification of biomolecules in various biological samples. However, the limitations in identification and discrimination sensitivity of current methods impede the wider adoption of this technology. In this article, a meticulously designed metasurface is proposed for molecular fingerprint enhancement, consisting of a periodic array of lithium tantalate triangular prism tetramers arranged in a square quartz lattice. The physical mechanism is explained by the finite-difference time-domain (FDTD) method. The metasurface achieves a high quality factor (Q-factor) of 231 and demonstrates excellent THz sensing capabilities with a figure of merit (FoM) of 609. By varying the incident angle of the THz wave, the molecular fingerprint signal is strengthened, enabling the highly sensitive detection of trace amounts of analyte. Consequently, cinnamoylglycine can be detected with a sensitivity limit as low as 1.23 μg·cm2. This study offers critical insights into the advanced application of THz waves in biomedicine, particularly for the detection of urinary biomarkers in various diseases, including gestational diabetes mellitus (GDM). Full article
(This article belongs to the Special Issue Photonics for Bioapplications: Sensors and Technology)
Show Figures

Figure 1

Figure 1
<p>(<b>a</b>) The structural diagram of the all-dielectric metasurface, illustrating the periodic arrangement of the high-index triangular prism tetramer based on the quartz substrate; (<b>b</b>) a unit cell of the periodic structure with a y-polarized source incident downwards in the z direction; (<b>c</b>) the main view of the unit cell (y–z plane) and corresponding parameters.</p>
Full article ">Figure 2
<p>(<b>a</b>) Transmission spectra for x-polarized and y-polarized incident waves at 0°; (<b>b</b>) transmission spectra for x-polarized and y-polarized incident waves at 37°; (<b>c</b>) the electric and magnetic field distribution measured at the surface of the quartz substrate at vertical incidence. The left and right figures correspond to the x-polarized and y-polarized incident wave, respectively.</p>
Full article ">Figure 3
<p>(<b>a</b>) Transmission spectra at different incident angles without any analyte; (<b>b</b>) the experimentally measured refractive index (n) and extinction coefficient (k) of cinnamoylglycine across the relevant frequency range; (<b>c</b>) transmission spectra at different incident angles with a <math display="inline"><semantics> <mrow> <mn>1</mn> <mo> </mo> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math> thick layer of analyte; (<b>d</b>) the electric field distribution measured at the substrate surface in the x–y plane at 0.487 THz for specific incident angles, corresponding to the transmission spectra shown in (<b>c</b>), respectively.</p>
Full article ">Figure 4
<p>(<b>a</b>) Comprehensive transmission spectra without any analyte, with the incident angle ranging from 13° to 70°. Specifically, the rightmost line represents the transmission curve for an angle of 13°, while the leftmost line corresponds to 70°; (<b>b</b>) comprehensive transmission spectra with <math display="inline"><semantics> <mrow> <mn>1</mn> <mo> </mo> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="normal">m</mi> </mrow> </semantics></math> thick cinnamoylglycine, with the incident angle ranging from 13° to 62°. The corresponding envelope curve has been plotted by red line in the figure.</p>
Full article ">Figure 5
<p>(<b>a</b>) Transmission envelope curves for analytes of varying thicknesses; (<b>b</b>) the relationship between the thickness of the analyte and the transmission at <math display="inline"><semantics> <mrow> <mn>0.487</mn> <mo> </mo> <mi mathvariant="normal">T</mi> <mi mathvariant="normal">H</mi> <mi mathvariant="normal">z</mi> </mrow> </semantics></math>.</p>
Full article ">
12 pages, 2932 KiB  
Article
Temperature Dependence of the Sensitivity of PVDF Pyroelectric Sensors to THz Radiation: Towards Cryogenic Applications
by Artem N. Sinelnikov, Anatoly R. Melnikov, Yaroslav V. Getmanov, Darya A. Kolomeec, Evgeny V. Kalneus, Matvey V. Fedin and Sergey L. Veber
Sensors 2024, 24(17), 5808; https://doi.org/10.3390/s24175808 - 6 Sep 2024
Viewed by 1121
Abstract
The application of terahertz (THz) science in industrial technology and scientific research requires efficient THz detectors. Such detectors should be able to operate under various external conditions and conform to existing geometric constraints in the required application. Pyroelectric THz detectors are among the [...] Read more.
The application of terahertz (THz) science in industrial technology and scientific research requires efficient THz detectors. Such detectors should be able to operate under various external conditions and conform to existing geometric constraints in the required application. Pyroelectric THz detectors are among the best candidates. This is due to their versatility, outstanding performance, ease of fabrication, and robustness. In this paper, we propose a compact pyroelectric detector based on a bioriented poled polyvinylidene difluoride film coated with sputtered metal electrodes for in situ absorption measurement at cryogenic temperature. The detector design was optimized for the registration system of the electron paramagnetic resonance (EPR) endstation of the Novosibirsk Free Electron Laser facility. Measurements of the detector response to pulsed THz radiation at different temperatures and electrode materials showed that the response varies with both the temperature and the type of electrode material used. The maximum signal level corresponds to the temperature range of 10–40 K, in which the pyroelectric coefficient of the PVDF film also has a maximum value. Among the three coatings studied, namely indium tin oxide (ITO), Au, and Cu/Ni, the latter has the highest increase in sensitivity at low temperature. The possibility of using the detectors for in situ absorption measurement was exemplified using two typical molecular spin systems, which exhibited a transparency of 20–30% at 76.9 cm−1 and 5 K. Such measurements, carried out directly in the cryostat with the main recording system and sample fully configured, allow precise control of the THz radiation parameters at the EPR endstation. Full article
(This article belongs to the Special Issue Research Development in Terahertz and Infrared Sensing Technology)
Show Figures

Figure 1

Figure 1
<p>General scheme of the optical system of the EPR endstation, the detection system, and the location of the PVDF detector inside the helium cryostat.</p>
Full article ">Figure 2
<p>(<b>a</b>) The structure of the brass parallelepiped with the plane mirror and two functional axial holes for the THz waveguide and sample holder. The pyroelectric detector is fixed to the parallelepiped with four screws. (<b>b</b>) The general design of the sensing unit of the pyroelectric detector and its connection to the detection system.</p>
Full article ">Figure 3
<p>Examples of the response of the pyroelectric detectors measured by two different approaches, namely by a transimpedance amplifier measuring a constant current, blue solid line, QS-IF5 pyrodetector, and by registering the voltage on the sides of the sensing film and further amplifying by the high-impedance amplifier with a gain of 100, red solid line, ITO pyrodetector.</p>
Full article ">Figure 4
<p>Temperature dependence of the response of the pyroelectric detectors with different sputtered electrodes. Symbols show: “○”—ITO; “☆”—Cu/Ni; “x”—Au. The response is normalized to room temperature. Solid lines are guides for the eye.</p>
Full article ">Figure 5
<p>Linearity of the detector responses measured at 5 K. Symbols show: “○”—ITO; “☆”—Cu/Ni; “x”—Au; the dashed line is a guide for the eye; 1 arb. u. of power and intensity depends on the detector used and is in the range of 1–3 W and 100–300 mV, respectively.</p>
Full article ">
Back to TopTop