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Waves","description":{"id":"4673c7c3-4eae-5172-9bb7-197684c099a7","childMarkdownRemark":{"id":"b9a30b7e-8242-50b8-991b-c88ed4c3b155","html":"M. Dragoman, M. Aldrigo, A. Dinescu, D. Vasilache, S. Iordanescu, and D. Dragoman. “Nanomaterials and Devices for Harvesting Ambient Electromagnetic Waves”. Nanomaterials 13, no. 3: 595, 2023
"}},"body":{"id":"adb86358-10a0-5b7e-bae8-2d37382b2946","childMarkdownRemark":{"id":"c5141c46-e494-5c70-b1d9-cc1dcabe89f5","html":"Authors: M. Dragoman, M. Aldrigo, A. Dinescu, D. Vasilache, S. Iordanescu, and D. Dragoman.
\nTitle: Nanomaterials and Devices for Harvesting Ambient Electromagnetic Waves
\nAbstract: In this review, we consider energy harvesting from ambient electromagnetic (EM) waves, since this method, together with energy harvesting from heat, are the most promising approaches for renewable energy production after photovoltaic DC power production via solar cells. Furthermore, solar cells are not referred to here, since there are already a large number of reviews dedicated to these devices, which are widespread in daily life. Although solar cells have been commercialized for some time, the research for more efficient harvesting solutions is growing every year, supported by the discovery of new materials, such as perovskites; among the reviews on the latter type of solar cells, see [1]. At the end of 2020, solar cells provided about 1 TW of electrical energy around the globe [2].\nThe radiofrequency (RF) energy harvesting (RF-EH) challenge originates from the unprecedented development of wireless high-frequency communications, such as 5G and 6G networks, able to generate an ambient EM energy available at any time and in a large band, spreading from the microwave spectrum up to sub-terahertz frequencies. This EM energy can be used on demand by equipment such as smartphones, tablets, laptops, and receivers at various frequencies, but a large part of it is not used and, hence, is lost. Harvesting the fraction of EM energy that is unexploited allows the self-powering of low-consumption electronic devices, e.g., those connected within Internet of things (IoT) architectures. The power supply mechanism associated with RF-EH techniques is based on a rectenna, i.e., an antenna loaded with an (un)biased diode [3,4,5]. Figure 1 shows the schematic of a generic rectenna, in which the antenna provides the RF input to a rectifying diode, whose DC output voltage VDC is the voltage drop on the load capacitor. A DC block capacitance and a RF choke inductance are (ideally) necessary at the input and output, respectively, of the diode to let only the DC component of the received RF signal pass. Furthermore, the diode should work in the unbiased state; however, in some circumstances (e.g., when the power at the input of the diode is too low to allow the device working in forward conduction), a small DC bias voltage could be necessary to force the rectifier to operate in its nonlinear region (this bias could be provided by EH sources other than the RF ones). Depending on the requested DC power, these rectennas can be arranged in arrays with various configurations involving one or more diodes. Many new materials are involved in the gathering of this ambient EM energy, such as two-dimensional (2D) materials (e.g., graphene and MoS2) [6,7], oxides [8], and nanoscale ferroelectrics (e.g., HfO2-based ferroelectrics) [9].
\nPublished in: Nanomaterials 13, no. 3: 595
\nDate/Place: \t2023
\nDOI: https://doi.org/10.3390/nano13030595
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"}},"email":null,"phone":null,"facebook":null,"twitter":null,"github":null,"image":null},"publishDate":"May 21st, 2022","tags":null},"site":{"siteMetadata":{"title":"Nano-eh","description":"This is my description that will be used in the meta tags and important for search results","base_font":"nunito-sans","site_url":"https://www.nano-eh.eu/","footer":{"content":"Project Coordinator: Dr Mircea MODREANU, Tyndall National Institute (TNI), University College Cork | PROPRIETARY RIGHTS STATEMENT: THIS DOCUMENT CONTAINS INFORMATION, WHICH IS PROPRIETARY TO THE NANO-EH CONSORTIUM. NEITHER THIS DOCUMENT NOR THE INFORMATION CONTAINED HEREIN SHALL BE USED, DUPLICATED OR COMMUNICATED BY ANY MEANS TO ANY THIRD PARTY, IN WHOLE OR IN PARTS, EXCEPT WITH THE PRIOR WRITTEN CONSENT OF THE NANO-EH CONSORTIUM. THIS RESTRICTION LEGEND SHALL NOT BE ALTERED OR OBLITERATED FROM THIS DOCUMENT. DISCLAIMER: FUNDED BY THE EUROPEAN UNION. VIEWS AND OPINIONS EXPRESSED ARE HOWEVER THOSE OF THE AUTHOR(S) ONLY AND DO NOT NECESSARILY REFLECT THOSE OF THE EUROPEAN UNION OR EUROPEAN COMMISSION. NEITHER THE EUROPEAN UNION NOR THE GRANTING AUTHORITY CAN BE HELD RESPONSIBLE FOR THEM.","has_nav":true,"nav_links":[{"label":"Terms of Service","style":"link","url":"/terms-of-service"},{"label":"Privacy Policy","style":"link","url":"/privacy-policy"}],"sections":[{"content":"Nano EH","form_fields":null,"form_id":null,"hide_labels":null,"image":"images/logo.svg","image_alt":"Footer logo","image_url":"/","nav_links":null,"submit_label":null,"title":null,"type":"footer_text"},{"content":null,"form_fields":null,"form_id":null,"hide_labels":null,"image":null,"image_alt":null,"image_url":null,"nav_links":[{"label":"About Us","style":"link","url":"/about"},{"label":"Blog","style":"link","url":"/blog"},{"label":"Sign Up","style":"link","url":"/signup"},{"label":"Contact","style":"link","url":"/contact"}],"submit_label":null,"title":"Company","type":"footer_nav"},{"content":null,"form_fields":null,"form_id":null,"hide_labels":null,"image":null,"image_alt":null,"image_url":null,"nav_links":[{"label":"Twitter","style":"link","url":"https://twitter.com/"},{"label":"LinkedIn","style":"link","url":"https://www.linkedin.com/"},{"label":"GitHub","style":"link","url":"https://github.com/"}],"submit_label":null,"title":"Community","type":"footer_nav"},{"content":"Stay up to date with our latest developments.","form_fields":[{"default_value":"Enter email address","input_type":"email","is_required":true,"label":"Email","name":"email"}],"form_id":"contactForm","hide_labels":true,"image":null,"image_alt":null,"image_url":null,"nav_links":null,"submit_label":"Subscribe","title":"Subscribe","type":"footer_form"}]},"header":{"has_nav":true,"logo_img":"images/logo.svg","logo_img_alt":"Logo","nav_links":[{"label":"Home","style":"link","url":"/"},{"label":"Features","style":"link","url":"/features"},{"label":"Pricing","style":"link","url":"/pricing"},{"label":"News","style":"link","url":"/news"},{"label":"Sign Up","style":"primary","url":"/signup"}]},"palette":"blue"}}},"pageContext":{"slug":"nanomaterials-and-devices-for-harvesting-ambient-electromagnetic-waves","prev":{"title":"Electrochemical deposition of polyaniline for supercapacitor applications","shortName":"Electrochemical deposition of polyaniline for supercapacitor applications","slug":"electrochemical-deposition-of-polyaniline-for-supercapacitor-applications","description":{"id":"211a8e3c-e54d-5d2c-a2e0-0149f0b38078","childMarkdownRemark":{"id":"18b425d0-2325-5d79-9608-9685a89f5b48","html":"M. Gheorghe, M. Modreanu, C. Cobianu, S. Gheorghe, P. Svasta. “Nanomaterials and Devices for Harvesting Ambient Electromagnetic Waves”. 2022 IEEE 9th Electronics System-Integration Technology Conference (ESTC), 13-16 Sept. 2022, Sibiu
"}},"body":{"id":"008e3489-9557-5a3f-bf8c-8f5e0ab40b9f","childMarkdownRemark":{"id":"9412fd83-272a-55c9-badc-213933acef8e","html":"Authors: M. Gheorghe, M. Modreanu, C. Cobianu, S. Gheorghe, P. Svasta
\nTitle: Electrochemical deposition of polyaniline for supercapacitor applications
\nPublished in: 2022 IEEE 9th Electronics System-Integration Technology Conference (ESTC)
\nDate/Place: \t13-16 Sept. 2022, Sibiu
\nDOI: 10.1109/ESTC55720.2022.9939387
"}},"author":{"name":"Admin","title":"Admin","company":"Nano-EH","shortBio":{"id":"f54a09fc-3ed1-5644-adea-83b5fe2c8f8a","childMarkdownRemark":{"id":"83f8d273-3b5d-54bc-b2d5-4d3d91953f6b","html":"Admin
"}},"email":null,"phone":null,"facebook":null,"twitter":null,"github":null},"publishDate":"May 21st, 2022","tags":null},"next":{"title":"Ultrathin tin sulfide field-effect transistors with subthreshold slope below 60 mV/decade","shortName":"Ultrathin tin sulfide field-effect transistors with subthreshold slope below 60 mV/decade","slug":"ultrathin-tin-sulfide-field-effect-transistors-with-subthreshold-slope-below","description":{"id":"364c2b4b-4e02-5afa-8270-7b5d33afb453","childMarkdownRemark":{"id":"31891c40-3f56-5abe-bba4-22760b163f5b","html":"M. Dragoman, A. Dinescu, A. Avram, D. Dragoman, S. Vulpe, M. Aldrigo, T. Braniste, V. Suman, E. Rusu, and I. Tiginyanu. “Ultrathin tin sulfide field-effect transistors with subthreshold slope below 60 mV/decade”. Nanotechnology 33 405207, 2022
"}},"body":{"id":"467cd955-7bc7-5ccf-b610-d72e74e22cea","childMarkdownRemark":{"id":"1521fd45-33eb-54a7-8c93-a2f19b7a061f","html":"Authors: M. Dragoman, A. Dinescu, A. Avram, D. Dragoman, S. Vulpe, M. Aldrigo, T. Braniste, V. Suman, E. Rusu, and I. Tiginyanu
\nTitle: Ultrathin tin sulfide field-effect transistors with subthreshold slope below 60 mV/decade
\nAbstract: In this paper, we present for the first time a field-effect-transistor (FET) having a 10 nm thick tin sulfide (SnS) channel fabricated at the wafer scale with high reproducibility. SnS-based FETs are in on-state for increasing positive back-gate voltages up to 6 V, whereas the off-state is attained for negative back-gate voltages not exceeding −6 V, the on/off ratio being in the range 102–103 depending on FET dimensions. The SnS FETs show a subthreshold slope (SS) below 60 mV/decade thanks to the in-plane ferroelectricity of SnS and attaining a minimum value SS = 21 mV/decade. Moreover, the low SS values can be explained by the existence of a negative value of the capacitance of the SnS thin film up to 10 GHz (for any DC bias voltage between 1 and 5 V), with the minimum value being −12.87 pF at 0.1 GHz.
\nPublished in: Nanotechnology 33 405207
\nDate/Place: \t2022
\nDOI: 10.1088/1361-6528/ac7cf8
"}},"author":{"name":"Admin","title":"Admin","company":"Nano-EH","shortBio":{"id":"f54a09fc-3ed1-5644-adea-83b5fe2c8f8a","childMarkdownRemark":{"id":"83f8d273-3b5d-54bc-b2d5-4d3d91953f6b","html":"Admin
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