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The morphology, chemical, and vibrational characteristics of the nanostructures were investigated. The dependency of the photocurrent of Au decorated ZnO NRsA on wavelength was evaluated by photogain response. Due to the induced surface plasmon excitation, selective response to green laser was observed. An analytical dispersion formalism was constructed to fit the experimental absorption spectrum of both ZnO NRsA and Au-decorated ZnO NRsA, over a wide spectrum range in order to evaluate the bandgap energy, subband tailing, dielectric constant and carrier effective mass and density, and nonlinear optical parameters. The proposed model exploits the Forouhi–Bloomer (FB) parameterization and Gaussian oscillator dispersion for the complex dielectric function of Au-decorated ZnO NRsA. Both the sharp variation in the optical absorption around the band edge and absorption behavior beyond the bandgap energy are covered well. It is surprising that the surface plasmon resonance (SPR) is included without introducing a new formalism. The photogain study on ZnO NRsA-Au 40 nm heterostructure shows that the obtained ESPR from the dispersion model is in complete agreement with the selective green response of the heterostructure. Furthermore, the new model was satisfactorily tested on the optical absorption spectra of CuO thin films.",{"EN":195,"VI":196},"Surface Plasmon Resonance and Absorption Features Beyond the Bandedge in ZnO Nanorods Array – Au Heterostructures: Prediction and More Accurate Representation","Cộng hưởng plasmon bề mặt và các đặc trưng hấp thụ ngoài mép dải trong dị cấu trúc mảng thanh nano ZnO – Au: Dự đoán và biểu diễn chính xác hơn",{"VOID":198},"Forouhi AR, Bloomer I (2019) New dispersion equations for insulators and semiconductors valid throughout radio-waves to extreme ultraviolet spectral range. J. Phys. Commun. 3:035022\nLi Z, Lin SH, Qiu GM, Wang JY, Yu YP (2018) A method for determining band parameters from the optical absorption edge of amorphous semiconductor Application to a-Si:H. J Appl Phys 124:025702\nFranta D, Cermak M, Vohanka J, Ohlidal I (2017) Dispersion models describing interband electronic transitions combining Tauc’s law and Lorentz model. Thin Solid Films 631:12–22\nLikhachev DV, Malkova N, Poslavsky L (2015) Modified Tauc-Lorentz dispersion model leading to a more accurate representation of absorption features below the bandgap. Thin Solid Films 589:844–851\nKumar A, Kumar A, Srivastava SK (in press) Silicon nitride-BP-based surface plasmon resonance highly sensitive biosensor for virus SARS-CoV-2 detection. Plasmonics. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-021-01589-1\nSagar P, Srivastava M, Prakashb R, Srivastava SK (2020) The fabrication of an MoS2 QD–Au NP modified screen-printed electrode for the improved electrochemical detection of cefixime. Anal Methods 12:3014–3024\nCampi D, Coriasso C (1988) Prediction of optical properties of amorphous tetrahedrally bonded materials. J Appl Phys 64(8):4128–4134\nJellison GE, Modine FA (1996) Parameterization of the optical functions of amorphous materials in the interband region. Appl Phys Lett 69(3):371–373\nCody GD (1984) Semiconductors and semimetals. Vol. 21\nRodriguez- De Marcos LV, Larruquert JI (2016) Analytic optical-constant model derived from Tauc-Lorentz and Urbach tail. Opt Express 24(25):28561\nFoldyna M, Postava K, Bouchala J, Pitora J, Yamaguchi T (2003) Model dielectric function of amorphous materials including Urbach tail. Proc SPIE 5445:301–305\nFerlauto AS, Koh J, Rovira PI, Wronski CR, Collins RW, Ganguly G (2000) Modeling the dielectric functions of silicon-based films in the amorphous, nanocrystalline and microcrystalline regimes. J Non-Cryst Solids 266–269:269–273\nFranta D, Ohlídal I, Nečas D, Vižd’a F, Caha O, Hasoň M, Pokorný P (2011) Optical characterization of HfO2 thin films. Thin Solid Films 519:6085–6091\nFerlauto AS, Ferreira GM, Pearce JM, Wronski CR, Collins RW, Deng X, Ganguly G (2004) Analytical model for the optical functions of amorphous semiconductors and its applications for thin film solar cells. Thin Solid Films 455–456:388–392\nMei JJ, Chen H, Shen WZ, Dekkers HFW (2006) Optical properties and local bonding configurations of hydrogenated amorphous silicon nitride thin films. J Appl Phys 100:073516\nShahi N, Rahmati A (2019) Ag Incorporated ZnO Nanorods Array\u002FZnSe Heterostructure. ECS J Solid State Sci Technol 8(10):Q200–Q206\nRahmati A, Farokhipour A (2019) Rectifying behaviour and photocatalytic activity in ZnO nanorods array\u002F Ag \u002F CuSe heterostructure. J Cluster Sci 30:521–529\nGhaemi-moghadam M, Hassanzadeh A, Rahmati A (2021) Charge transfer plasmon coupled surface photosensing in ZnO nanorods–Au array hetero-nanostructures. Opt Lasers Eng 137:106384\nFox M(2010) Optical properties of solids, Second Edition. Oxford University Press, page 39\nFujiwara H, Kondo M (2005) Effects of carrier concentration on the dielectric function of ZnO: Ga and In2O3: Sn studied by spectroscopic ellipsometry: analysis of free-carrier and band-edge absorption. Phys Rev B 71:075109\nKumar A, Kumar A, Kushwaha AS, Dubey SK, Srivastava SK (2022) A comparative study of different types of sandwiched structures of SPR biosensor for sensitive detection of ssDNA. Photonics Nanostruct Fundam Appl 48:100984\nDe Sousa Meneses D, Malki M, Echegut P (2006) Structure and lattice dynamics of binary lead silicate glasses investigated by infrared spectroscopy. J Non-Cryst Solids 352:769–776\nAkaltun Y, Yıldırım MA, Ateş A, Yıldırım M (2012) Zinc concentration effect on structural, optical and electrical properties of Cd1−x ZnxSe thin films. Mater Ress Bull 47:3390–3396\nMezrag F, Mohamed WK, Bouarissa N (2010) The effect of zinc concentration upon optical and dielectric properties of Cd1−xZnxSe. Physica B 405:2272–2276\nHerve P, Vandamme LKJ (1994) General relation between refractive index and energy gap in semiconductors. Infrared Phys Technol 35:609–615\nDimitrov V, Sakka S (1996) Linear and nonlinear optical properties of simple oxides. II. J Appl Phys 79(3):1741–1745\nHannachi L, Bouarissa N (2009) Band parameters for cadmium and zinc chalcogenide compounds. Physica B 404:3650–3654\nTiwari P, Jaiswal J, Chandra R (2019) Optical and electrical properties of highly ordered α-, γ- and α + γ-MnS films deposited by reactive sputtering technique. J Appl Phys 126:213108\nHassanieh AS, Aly KA, Akl AA (2016) Study of optical properties of thermally evaporated ZnSe thin films annealed at different pulsed laser power. J Alloy Compd 685:733–742\nGupta V, Bhattacharya P, Yuzuk YI, Sreenivas K, Katiyar RS (2006) Optical phonon modes in ZnO nanorods on Si prepared by pulsed laser deposition. J Cryst Growth 287:39–43\nAlim K, Fonoberov VA, Shamsa M, Balandin AA (2005) Micro-Raman investigation of optical phonons in ZnO quantum dots. J Appl Phys 97:124313\nSagar P, Gupta GK, Srivastava M, Srivastavab A, Srivastava SK (2021) Tagetes erecta as an organic precursor: synthesis of highly fluorescent CQDs for the micromolar tracing of ferric ions in human blood serum. RSC Adv 11:19924–19934\nMurakami H, Takarada T, Tonouchi M (2020) Low temperature GaAs based plasmonics photoconductive terahertz detector with au nanoislands. Photonics Res 8:1448–1456\nRahmati A, Rahmani B, Farokhipour A (2018) Hetero plasmonic 2D and 3D ZnO\u002FAg nanostructures: electrical and photocatalytic applications. J Mater Sci Mater Electron 29:6350–6360\nBaxter JB, Schmuttenmaer CA (2006) Conductiviy of ZnO nanowire, nanoparticles, and thin films using time-resolved terahertz spectroscopy. Journal Phys Chem B 110:25229–25239\nAkaltun Y (2015) Effect of thickness on the structural and optical properties of CuO thin films grown by successive ionic layer adsorption and reaction. 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Iran",[],{"id":252,"sortIndex":176,"affiliation":253,"properties":259},"952986b6-b72e-4c9f-b05c-6be511de36a0",{"id":252,"createTime":19,"updateTime":19,"relativeEntities":254,"slug":19,"properties":255,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":258,"statistic":19},[],{"title":256},{"VI":257},"Nanostructured Materials Laboratory, Vali-E-Asr University of Rafsanjan, Rafsanjan, Iran",[],{},{"title":261},{"VI":262},"Ali 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generation efficiency of surface plasmon polaritons at metallic nanoslit is theoretically analyzed, and a novel plasmonic lens with two semiannular nanoslits is proposed in this paper. Based on the analysis results, the focusing performance of the proposal is optimized with a maximum field intensity enhancement factor of 7.69 and the full width at half maximum is 132 nm (~0.2λ\n                i), far beyond theoretical diffraction limit. Meanwhile, some other classical plasmonic lenses are also optimized through improving generation efficiency of surface plasmon polaritons at nanoslit and the focusing performances are consequently greatly enhanced.",{"EN":338,"VI":339},"Optimization on Plasmonic Lenses Based on Generation Efficiency of Surface Plasmon Polaritons at Metallic Nanoslit","Tối ưu hóa thấu kính plasmonic dựa trên hiệu suất tạo polariton plasmon bề mặt tại khe hẹp nano kim loại",{"VOID":341},"Shin YB, Kim HM, Jung Y, Chung BH (2010) A new palm-sized surface plasmon resonance (SPR) biosensor based on modulation of a light source by a rotating mirror. Sensors Actuators B Chem 150(1):1–6\nLuo XG, Ishihara T (2004) Surface plasmon resonant interference nanolithography technique. Appl Phys Lett 84(23):4780–4782\nLi YX, Liu F, Ye Y, et al. (2014) Two-surface-plasmon-polariton-absorption based lithography using 400 nm femtosecond laser. Appl Phys Lett 104(8):081115\nShi LP, Chong TC, Yao HB, Tan PK, Miao XS (2002) Super-resolution near-field optical disk with an additional localized surface plasmon coupling layer. Appl Phys Lett 91(12):10209–10211\nGuo YH, Yan LS, Pan W, Luo B (2015) Achromatic polarization manipulation by dispersion management of anisotropic meta-mirror with dual-metasurface. Opt Express 23(21):27566–27575\nGuo YH, Wang YQ, Pu MB, Zhao ZY, et al. (2015) Dispersion management of anisotropic metamirror for super-octave bandwidth polarization conversion. Sci Report 5:8483\nVerhagen E, Polman A, Kuipers LK (2008) Nanofocusing in laterally tapered plasmonic waveguides. Opt Express 16(1):45–57\nArtamonov M, Seideman T (2010) Molecular focusing and alignment with plasmon fields. Nano Lett 10(12):4908–4912\nLiu ZW, Steele JM, Srituravanich W, Pikus Y, et al. (2005) Focusing surface plasmons with a plasmonic lens. Nano Lett 5(9):1726–1729\nLi YX, Liu F, Xiao L, Cui KY, et al. (2013) Two-surface-plasmon-polariton-absorption based on nanolithography. Appl Phys Lett 102(6):063113\nCao L, Li W, Wang Y, Tian X, et al. (2014) Manipulating surface plasmon polaritons using F-shaped nanoslits array. IEEE Photon Technol Lett 26(12):1247–1250\nChen W, Abeysinghe DC, Nelson RL, Zhan Q (2009) Plasmonic lens made of multiple concentric metallic rings under radially polarized illumination. Nano Lett 9(12):4320–4325\nYang S, Chen W, Nelson RL, Zhan Q (2009) Miniature circular polarization analyzer with spiral plasmonic lens. Opt Lett 34(20):3047–3049\nLi J, Yang C, Zhao H, Lin F, Zhu X (2014) Plasmonic focusing in spiral nanostructures under linearly polarized illumination. Opt Express 22(14):16686–16693\nGjonaj B, David A, Blau Y, Spektor G, et al. (2014) Sub-100 nm focusing of short wavelength plasmons in homogeneous 2D space. Nano Lett 14(10):5598–5602\nLi J, Yang C, Li JM, Li Z, et al. (2014) Plasmonic focusing in nanostructures. Plasmonics 9(4):879–886\nFang Z, Peng Q, Song W, Hao F, et al. (2011) Plasmonic focusing in symmetry broken nanocorrals. Nano Lett 11(2):893–897\nLiu J, Gao Y, Ran L, Guo K, et al. (2015) Focusing surface plasmon and constructing central symmetry of focal field with linearly polarized light. Appl Phys Lett 106(1):013116\nLopez-Tejeira F, Rodrigo SG, Martin-Moreno L, Garcia-Vidal FJ, et al. (2007) Efficient unidirectional nanoslit couplers for surface plasmons. Nat Phys 3(5):324–328\nKoev ST, Agrawal A, Lezec HJ, Aksyuk VA (2012) An efficient large-area grating coupler for surface plasmon polaritons. Plasmonics 7(2):269–277\nJavaid M, Iqbal T (2016) Plasmonic bandgap in 1D metallic nanostructured devices. Plasmonics 11(1):167–173\nGuo YH, Yan LS, Pan W, Luo B (2016) Generation and manipulation of orbital angular momentum by all-dielectric metasurfaces. Plasmonics 11(1):337–344\nSun WJ, He Q, Sun SL, Zhou L (2016) High-efficiency surface plasmon meta-couplers: concept and microwave-regime realizations. Light Sci Appl 5:e16003\nWu CJ, Cheng YZ, Wang WY, He B, et al. (2015) Ultra-thin and polarization-independent phase gradient metasurface for high-efficiency spoof surface-plasmon-polariton coupling. Appl Phys Express 8(12):122001\nZakharian AR, Moloney JV, Mansuripur M (2007) Surface plasmon polaritons on metallic surfaces. Opt Express 15(1):183–197\nVassallo C (1991) Optical waveguide concepts. Elsevier Amsterdam, New York\nSnyder AW, Love JD (1983) Optical waveguide theory. Chapman and Hall, Springer, New York\nLalanne P, Hugonin JP, Rodier JC (2005) Theory of surface plasmon generation at nanoslit. Phys Rev Lett 95(26):263902",{"VOID":343},"10.1007\u002Fs11468-016-0296-0","2025-01-27T05:15:57.424+00:00",[206],"https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-016-0296-0",[348,363,376,389,403,417],{"id":349,"sortIndex":20,"researcher":19,"roles":350,"affiliations":351,"properties":360,"displayName":362,"givenName":19,"familyName":19},"8c0daf81-acdb-4c82-8bc4-a5356dbfdb13",[212],[352],{"id":353,"sortIndex":20,"affiliation":354,"properties":19},"652431db-9175-4789-90ac-a9a9ae46d823",{"id":353,"createTime":19,"updateTime":19,"relativeEntities":355,"slug":19,"properties":356,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":359,"statistic":19},[],{"title":357},{"VI":358},"Center for Information Photonics & Communications, School of Information Science & Technology, Southwest Jiaotong University, Chengdu, China",[],{"title":361},{"VI":362},"Xiantao 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properties of the terahertz resonant surface plasmons wave on the carbon nanotube film and dielectric interface have been investigated. As a first step towards engineering terahertz SPPs-like surface modes, we present a computer experiment to demonstrate that the carbon nanotube film surface can also be employed to concentrate and guide the terahertz SPPs wave. The carbon nanotube film is modeled in an experimentally realizable geometry. It is shown that a unique electromagnetic surface mode in terahertz region can be supported along the carbon nanotube film\u002Fdielectric interface when the free-space broadband terahertz pulse is incident on the carbon nanotube film with subwavelength gratings. Comparing with noble metals, plasmonic nano-structure materials based on carbon nanotube film offer a potentially more versatile approach to engineering tightly confined surface modes in the THz regime.",{"EN":506,"VI":507},"Surface Plasmon Resonant THz Wave Transmission on Carbon Nanotube Film","Truyền sóng THz cộng hưởng plasmon bề mặt trên màng ống nano carbon",{"VOID":509},"Williams CR, Andrews SR, Maier SA, Fernandez-Dominguez AI, Martin-Moreno L, Garcia-Vidal FJ (2008) Highly confined guiding of THz surface plasmon polaritons on structured metal surfaces. Nat Photon 2:175–179\nStefan A (2007) Plasmonics: fundamentals and applications. Springer, Berlin\nOzbay E (2006) Plasmonics: merging photonics and electronics at nanoscale dimensions. Science 311:189–193\nBaumberg JJ, Kelf TA, Sugawara Y, Cintra S, Abdelsalam ME, Bartlett PN, Russell AE (2005) Angle-resolved surface-enhanced Raman scattering on metallic nanostructure plasmonic crystals. Nano Lett 5:2262–2267\nTomasz JA, Piotr W, Tomasz S (2011) Performance of scanning near-field optical microscope probes with single groove and various metal coatings. Plasmonics 6:11–18\nLi ZB, Zhou WY, Yan WG, Tian JG (2011) Near-field enhancement through a single subwavelength aperture with gaps inside. Plasmonic 6:149–154\nLiu ZW, Wei QH, Zhang X (2005) Surface plasmon interference nanolithography. Nano Lett 5:957–961\nSrituravanich W, Fang N, Sun C, Luo Q, Zhang XP (2004) Plasmonic nanolithography. Nano Lett 4:1085–1088\nTsai WH, Tsao YC, Lin HY, Sheu BC (2005) Cross-point analysis for a multimode fiber sensor based on surface plasmon resonance. Opt Lett 30:2209–2211\nFu YQ, Zhou XL (2010) Plasmonic lenses: a review. Plasmonics 5:287–310\nAzad AK, Zhao YG, Zhang WL, He MX (2006) Effect of dielectric properties of metals on THz transmission in subwavelength hole arrays. Opt Lett 31:2637–2639\nHuang CP, Zhu YY (2007) Plasmonics: manipulating light at the subwavelength scale. Active and Passive Electronic Components ID30946\nSaxler J, Gomez Rivas J, Janke C, Pellemans HPM, HaringBolivar P, Kurz H (2004) Time-domain measurements of surface plasmon polaritons in the THz frequency range. Phys Rev B 69:155427\nO’Hara J, Averitt R, Taylor A (2005) Prism coupling to THz surface plasmon polaritons. Opt Express 13:6117–6126\nColeman S, Grischkowsky D (2003) A THz transverse electromagnetic mode two-dimensional interconnect layer incorporating quasi-optics. Appl Phys Lett 83:3656–3658\nJeon TI, Son JH, An KH, Lee YH, Lee YS (2005) THz absorption and dispersion of fluorine-doped single-walled CNT. J Appl Phys 98:034316\nJeon TI, Kim KJ, Kang C, Oh SJ, Son JH, An KH, Bae DJ, Lee YH (2002) THz conductivity of anisotropic singe walled carbon nanotube films. Appl Phys Lett 80:3403–3404\nUgawa A, Rinzler AG, Tanner DB (1999) Far-infrared gaps in single-wall carbon nanotubes. Phys Rev B 60:R11305\nOrdal MA, Long LL, Bell RJ, Bell SE, Bell RR, Alexander RW, Ward CA (1983) Optical properties of the metals Al, Co, Cu, Au, Fe, Pb, Ni, Pd, Pt, Ag, Ti, and W in the infrared and far infrared. Appl Opt 22:1099–1120\nDong XQ, Grischkowsky D, Zhang WL (2004) THz transmission properties of thin, subwavelength metallic hole arrays. Opt Lett 29:896–898\nwww.srpcb.com\u002Fbbs\u002Fdownload.php?no=52&name=metcladcompchart\nBarnes WL, Dereux A, Ebbesen TW (2003) Surface plasmon subwavelength optics. Nat Photon 424:824–830\nRaether H (1988) Surface plasmons on smooth and rough surfaces and on grating. Springer, Berlin",{"VOID":511},"10.1007\u002Fs11468-011-9322-4","2025-01-25T15:05:23.384+00:00",[206],"https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-011-9322-4",[516,540,553,568,581,594],{"id":517,"sortIndex":20,"researcher":19,"roles":518,"affiliations":519,"properties":537,"displayName":539,"givenName":19,"familyName":19},"dd7556a9-966f-4a24-954c-d22396d25444",[212],[520,528],{"id":521,"sortIndex":20,"affiliation":522,"properties":19},"ef6ff577-67fa-4c46-9bab-9fce82790ada",{"id":521,"createTime":19,"updateTime":19,"relativeEntities":523,"slug":19,"properties":524,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":527,"statistic":19},[],{"title":525},{"VI":526},"Department of Electronic Science and Technology, Harbin University of Science and Technology, Harbin, China",[],{"id":529,"sortIndex":176,"affiliation":530,"properties":536},"7ff5f87e-d0c6-43df-9451-9a2ad14d69e0",{"id":529,"createTime":19,"updateTime":19,"relativeEntities":531,"slug":19,"properties":532,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":535,"statistic":19},[],{"title":533},{"VI":534},"Key Laboratory of Engineering Dielectrics and Its Application, Ministry of Education, Harbin University of Science and Technology, Harbin, China",[],{},{"title":538},{"VI":539},"Yue 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strong light-matter interactions opens opportunities for wide applications including quantum information processing, enhancing optical processes, and ultrasensitive sensing, especially for explorations of novel photonic devices. Here, we have theoretically demonstrated the practicability of tuning the strong coupling between the propagating surface plasmon and molecular exciton modes towards the deep ultraviolet (DUV) region for the first time. Moreover, the Rabi splitting strength and wavelength of strong coupling as well as corresponding electromagnetic-field characteristics have been systematically manipulated by adjustment of exciton resonance frequency based on the Lorentzian model. These findings not only extend the working wavelength of strong coupling to DUV region, but also provide an attractive avenue to facilitate the rational design of strong-coupling configurations covering the solar spectrum.",{"EN":682},"Efficient Manipulation of Strong Coupling Towards the Deep Ultraviolet Region",{"VOID":684},"[\"16010227238115921246\"]",{"VOID":686},"Zhang SP, Bao K, Halas NJ, Xu HX, Nordlander P (2011) Substrate-induced Fano resonances of a plasmonic nanocube: a route to increased-sensitivity localized surface plasmon resonance sensors revealed. Nano Lett 11:1657–1663. https:\u002F\u002Fdoi.org\u002F10.1021\u002Fnl200135r\nWang Y, Yu J, Mao YF, Chen J, Wang S et al (2020) Stable, high-performance sodium-based plasmonic devices in the near infrared. Nature 581:401–405. https:\u002F\u002Fdoi.org\u002F10.1038\u002Fs41586-020-2306-9\nMoskovits M (1985) Surface-enhanced spectroscopy. Rev Mod Phys 57:783. https:\u002F\u002Fdoi.org\u002F10.1103\u002FRevModPhys.57.783\nLi JF, Huang YF, Ding Y, Yang ZL, Li SB et al (2010) Shell-isolated nanoparticle-enhanced Raman spectroscopy. Nature 464:392. https:\u002F\u002Fdoi.org\u002F10.1038\u002Fnature08907\nLi Z, Pan Y, You QZ, Zhang LS, Zhang D et al (2020) Graphene-coupled nanowire hybrid plasmonic gap mode–driven catalytic reaction revealed by surface-enhanced Raman scattering. Nanophotonics 9:4519–4527. https:\u002F\u002Fdoi.org\u002F10.1515\u002Fnanoph-2020-0319\nZeng ZC, Meng LY, Li MH, Huang TX, Zhong JH, Wang X, Yang ZL, Ren B (2015) Electrochemical tip-enhanced Raman spectroscopy. J Am Chem Soc 37:11928–11931. https:\u002F\u002Fdoi.org\u002F10.1021\u002Fjacs.5b08143\nZheng J, Yang WM, Wang JY, Zhu JF, Qian LH et al (2019) An ultranarrow SPR linewidth in the UV region for plasmonic sensing. Nanoscale 11:4061–4066. https:\u002F\u002Fdoi.org\u002F10.1039\u002Fc8nr09703h\nQing YM, Ren YZ, Lei DY, Ma HF, Cui TJ (2022) Strong coupling in two-dimensional materials-based nanostructures: a review. J Opt 24:024009. https:\u002F\u002Fdoi.org\u002F10.1088\u002F2040-8986\u002Fac47b3\nGarcia-Vidal FJ, Ciuti C, Ebbesen TW (2021) Manipulating matter by strong coupling to vacuum fields. Science 373:178. https:\u002F\u002Fdoi.org\u002F10.1126\u002Fscience.abd0336\nShen SH, Meng LY, Zhang YJ, Han J, Ma ZH et al (2015) Plasmon-enhanced second-harmonic generation nanorulers with ultrahigh sensitivities. Nano Lett 15:6716–6721. https:\u002F\u002Fdoi.org\u002F10.1021\u002Facs.nanolett.5b02569\nTorma P, Barnes WL (2015) Strong coupling between surface plasmon polaritons and emitters: a review. Rep Prog Phys 78:013901. https:\u002F\u002Fdoi.org\u002F10.1088\u002F0034-4885\u002F78\u002F1\u002F013901\nSun J, Hu H, Pan D, Zhang S, Xu H (2020) Selectively depopulating valley-polarized excitons in monolayer MoS2 by local chirality in single plasmonic nanocavity. Nano Lett 20:4953–4959. https:\u002F\u002Fdoi.org\u002F10.1021\u002Facs.nanolett.0c01019\nNiu Y, Xu H, Wei H (2022) Unified scattering and photoluminescence spectra for strong plasmon-exciton coupling. Phys Rev Lett 128:167402. https:\u002F\u002Fdoi.org\u002F10.1103\u002FPhysRevLett.128.167402\nChen S, Meng L, Hu J, Yang Z (2014) Fano interference between higher localized and propagating surface plasmon modes in nanovoid arrays. Plasmonics 10:71–76. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-014-9779-z\nKikawada M, Ono A, Inami W, Kawata Y (2014) Enhanced multicolor fluorescence in bioimaging using deep-ultraviolet surface plasmon resonance. 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Opt Lett 39:4994–4997. https:\u002F\u002Fdoi.org\u002F10.1364\u002FOL.39.004994\nYadav RK, Bourgeois MR, Cherqui C, Juarez XG, Wang W et al (2020) Room temperature weak-to-strong coupling and the emergence of collective emission from quantum dots coupled to plasmonic arrays. ACS Nano 14:7347–7357. https:\u002F\u002Fdoi.org\u002F10.1021\u002Facsnano.0c02785\nHuang H, Deng F, Xiang J, Li S, Lan S (2021) Plasmon-exciton coupling in dielectric-metal hybrid nanocavities with an embedded two-dimensional material. Appl Surf Sci 542:148660. https:\u002F\u002Fdoi.org\u002F10.1016\u002Fj.apsusc.2020.148660\nQin J, Chen YH, Zhang Z, Zhang Y, Blaikie RJ et al (2020) Revealing strong plasmon-exciton coupling between nanogap resonators and two-dimensional semiconductors at ambient conditions. 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Nanoscale 9:13947–13955. https:\u002F\u002Fdoi.org\u002F10.1039\u002Fc7nr03909c\nLiu W, Lee B, Naylor CH, Ee HS, Park J et al (2016) Strong exciton-plasmon coupling in MoS2 Coupled with plasmonic lattice. Nano Lett 16:1262–1269. https:\u002F\u002Fdoi.org\u002F10.1021\u002Facs.nanolett.5b04588\nWang J, Yang W, Sun G, He Y, Ren P et al (2022) Boosting anapole-exciton strong coupling in all-dielectric heterostructures. Photonics Res. https:\u002F\u002Fdoi.org\u002F10.1364\u002Fprj.453099\nAgarwal GS (1984) Vacuum-field Rabi splittings in microwave absorption by Rydberg atoms in a cavity. Phys Rev Lett 53:1732–1734. https:\u002F\u002Fdoi.org\u002F10.1103\u002FPhysRevLett.53.1732\nZhang H, Abhiraman B, Zhang Q, Miao J, Jo K et al (2020) Hybrid exciton-plasmon-polaritons in van der Waals semiconductor gratings. 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Adv Opt Mater 7:1900857. https:\u002F\u002Fdoi.org\u002F10.1002\u002Fadom.201900857\nZhang Y, Esteban RB, Boto RA, Urbieta M, Arrieta XB et al (2021) Addressing molecular optomechanical effects in nanocavity-enhanced Raman scattering beyond the single plasmonic mode. Nanoscale 13:1938–1954. https:\u002F\u002Fdoi.org\u002F10.1039\u002Fd0nr06649d",{"VOID":688},"10.1007\u002Fs11468-023-01808-x","2024-05-16T02:24:16.369+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-023-01808-x",[692,716,736,756,776,796,811],{"id":693,"sortIndex":20,"researcher":19,"roles":694,"affiliations":695,"properties":713,"displayName":715,"givenName":19,"familyName":19},"abfa4e7c-4cce-483a-bfbf-ac16c2169797",[212],[696,704],{"id":697,"sortIndex":20,"affiliation":698,"properties":19},"b0ca472e-4cc7-4ef2-9d64-00c02932f022",{"id":697,"createTime":19,"updateTime":19,"relativeEntities":699,"slug":19,"properties":700,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":703,"statistic":19},[],{"title":701},{"VI":702},"Xinjiang Key Laboratory of Solid State Physics and Devices, Xinjiang University, Urumqi, People’s Republic of 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The strong transverse magnetic field intensity is also plotted for the biomedical sensor to analyze the penetration depth. The designed surface plasmon resonance sensor’s optimal penetration depth into the sensing medium is 137 nm. 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Appl Surf Sci 475:342–347. https:\u002F\u002Fdoi.org\u002F10.1016\u002Fj.apsusc.2018.12.283","https:\u002F\u002Fdoi.org\u002F10.1016\u002Fj.apsusc.2018.12.283",{"mag":1388,"openalex":1389,"doi":1390},"2907016417","W2907016417","10.1016\u002Fj.apsusc.2018.12.283",{"id":19,"text":1392,"url":1393,"identifiers":1394},"Singh S (2022) Sensitivity enhancement of SPR biosensor employing heterostructure blue phosphorus \u002FMoS2 and silicon layer. Emerging Materials Research 11(2):239–250. https:\u002F\u002Fdoi.org\u002F10.1680\u002Fjemmr.22.00009","http:\u002F\u002Fdx.doi.org\u002F10.1680\u002Fjemmr.22.00009",{"doi":1395},"10.1680\u002Fjemmr.22.00009",{"id":1397,"text":1398,"url":1399,"identifiers":1400},"6a7e105f-ab9b-411b-8783-9ab7ef02c6a3","Yu Y, Hu X, Wang S, Qiao H, Liu Z, Song K, Shen X (2022) High mass loading Ni4Co1-OH@ CuO core-shell nanowire arrays obtained by electrochemical reconstruction for alkaline energy storage. Nano Res 15(1):685–693. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs12274-021-3547-0","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs12274-021-3547-0",{"doi":1401},"10.1007\u002Fs12274-021-3547-0",{"id":1403,"createTime":1404,"updateTime":1405,"relativeEntities":1406,"slug":1407,"properties":1408,"entityType":201,"verifyStatus":202,"verifyTime":1419,"verifyNote":204,"languages":19,"translateLanguages":19,"viewCount":20,"primaryUrl":1420,"fullTextUrl":19,"authors":1421,"publicationType":263,"publisherRelationship":1540,"citationCount":122,"citationInfo":1600,"publishDate":1603,"publishYear":1601,"citationAnalyzeStatus":1604,"lastCitationAnalyze":1605,"indexDatabases":1606,"openAccess":19,"references":19,"isForceReanalyzing":327},"9739006f-64f8-4bd3-8098-78b74cb5472f","2024-01-04T02:33:07.769+00:00","2026-07-28T08:59:05.008+00:00",[],"Temperature-Regulated-Surface-Plasmon-Resonance-Imaging-System-for-Bioaffinity-Sensing",{"abstract":1409,"title":1411,"gsPaper":1413,"references":1415,"doi":1417},{"EN":1410},"We describe a temperature-regulated surface plasmon resonance (SPR) imaging biosensor in this article. The sample temperature can be regulated for specific requirements of the bioaffinity sensing, and stabilized to suppress the measurement noise caused by temperature fluctuations. The water thermo optic coefficient is measured to test the temperature regulation performance. The protein interaction is monitored to demonstrate the feasibility of this system for real-time biomolecular interaction analysis. This temperature-regulated SPR imaging biosensor can be readily implemented by adding the common water path and peristaltic pump to the conventional SPR imaging system, which may provide an economical and convenient scheme to improve the analysis accuracy and quality of bioaffinity sensing using SPR sensing platform.",{"EN":1412},"Temperature-Regulated Surface Plasmon Resonance Imaging System for Bioaffinity Sensing",{"VOID":1414},"[\"6669714754418032763\"]",{"VOID":1416},"Homola J, Yee SS, Gauglitz G (1999) Surface plasmon resonance sensors: review. Sensor Actuat B-Chem 54:3–15\nKarlsson R (2004) SPR for molecular interaction analysis: a review of emerging application areas. J Mol Recognit 17:151–61\nHomola J (2008) Surface plasmon resonance sensors for detection of chemical and biological species. Chem Rev 108:462–93\nWong CL, Olivo M (2014) Surface plasmon resonance imaging sensors: a review. Plasmonics 9:809–24\nSmith EA, Thomas WD, Kiessling LL, Corn RM (2003) Surface plasmon resonance imaging studies of protein-carbohydrate interactions. J Am Chem Soc 125:6140–8\nGifford LK, Sendroiu IE, Corn RM, Luptak A (2010) Attomole detection of mesophilic DNA polymerase products by nanoparticle-enhanced surface plasmon resonance imaging on glassified gold surfaces. J Am Chem Soc 132:9265–7\nChong XY, Liu L, Liu ZY, Ma SH, Guo J, Ji YH, He YH (2013) Detect the hybridization of single-stranded DNA by parallel scan spectral surface plasmon resonance imaging. Plasmonics 8:1185–91\nLin H, Wang LP, Dong JX, Xu XY, Liu L, Zhang L, Huang Q, Zhang XH, Liu QQ (2015) Study on trace sample of chronic skin ulcer with a symmetrical optical waveguide-based surface plasmon resonance biosensor. Plasmonics in press. doi: 10.1007\u002Fs11468-015-9983-5\nHomola J (2003) Present and future of surface plasmon resonance biosensors. Anal Bioanal Chem 377:528–39\nO'Brien MJ, Perez-Luna VH, Brueck SRJ, Lopez GP (2001) A surface plasmon resonance array biosensor based on spectroscopic imaging. Biosens Bioelectron 16:97–108\nShi H, Liu ZY, Wang XX, Guo J, Liu L, Luo L, Guo JH, Ma H, Sun SQ, He YH (2013) A symmetrical optical waveguide based surface plasmon resonance biosensing system. Sensor Actuat B-Chem 185:91–6\nHomola J, Lu HB, Nenninger GG, Dostalek J, Yee SS (2001) A novel multichannel surface plasmon resonance biosensor. Sensor Actuat B-Chem 76:403–10\nDostalek J, Vaisocherova H, Homola J (2005) Multichannel surface plasmon resonance biosensor with wavelength division multiplexing. Sensor Actuat B-Chem 108:758–64\nDyankov G, Zekriti M, Bousmina (2012) Dual-mode surface-plasmon sensor based on bimetallic film. Appl Opt 51:2451–6\nZhang PF, Liu L, He YH, Ji YH, Ma H (2015) Self-referenced plasmon waveguide resonance sensor using different waveguide modes. J Sens 2015:945908\nZhang PF, Liu L, He YH, Shen ZY, Guo J, Ji YH, Ma H (2014) Non-scan and real-time multichannel angular surface plasmon resonance imaging method. Appl Opt 53:6037–42\nLiu L, Ma SH, Ji YH, Chong XY, Liu ZY, He YH, Guo JH (2011) A two-dimensional polarization interferometry based parallel scan angular surface plasmon resonance biosensor. Rev Sci Instrum 82:023019\nMao HB, Yang TL, Cremer PS (2002) A microfluidic device with a linear temperature gradient for parallel and combinatorial measurements. 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Appl Phys Lett 70:1852–4\nMa H, Hao X, Ma J, Yang Y, Huang S, Chen F, Wang Q, Zhang D (2002) Bias voltage dependence of properties for ZnO: Al films deposited on flexible substrate. Surf Coat Technol 161:58–61\nLiu L, Guo J, He YH, Zhang PF, Zhang YL, Guo JH (2015) Study on the despeckle methods in angular surface plasmon resonance imaging sensors. Plasmonics 10:729–37\nMaier JS, Walker SA, Fantini S, Franceschini MA, Gratton E (1994) Possible correlation between blood glucose concentration and the reduced scattering coefficient of tissues in the near infrared. Opt Lett 19:2062–4\nZhou YF, Zhang PF, He YH, Xu ZH, Liu L, Ji YH, Ma H (2014) Plasmon waveguide resonance sensor using an Au-MgF2 structure. Appl Opt 53:6344–50\nPiliarik M, Homola J (2009) Surface plasmon resonance (SPR) sensors: approaching their limits? Opt Express 17:16505–17\nSpringer T, Bockova M, Homola J (2013) Label-free biosensing in complex media: a referencing approach. Anal Chem 85:5637–40",{"VOID":1418},"10.1007\u002Fs11468-015-0108-y","2024-05-09T01:58:16.498+00:00","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-015-0108-y",[1422,1447,1464,1485,1500,1520],{"id":1423,"sortIndex":20,"researcher":19,"roles":1424,"affiliations":1425,"properties":1442,"displayName":1444,"givenName":19,"familyName":19},"0efd05f9-4bea-439b-9119-76e4cdc4c849",[212],[1426,1434],{"id":1427,"sortIndex":20,"affiliation":1428,"properties":19},"3640ba4e-ea09-4019-a3ed-7905130f5504",{"id":1427,"createTime":19,"updateTime":19,"relativeEntities":1429,"slug":19,"properties":1430,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1433,"statistic":19},[],{"title":1431},{"VI":1432},"Shenzhen Key Laboratory for Minimal Invasive Medical Technologies, Institute of optical imaging and sensing, Graduate School at Shenzhen, Tsinghua University, Shenzhen, China",[],{"id":1435,"sortIndex":176,"affiliation":1436,"properties":19},"3a0d9711-4048-4fb1-8f04-654c07d12e66",{"id":1435,"createTime":19,"updateTime":19,"relativeEntities":1437,"slug":19,"properties":1438,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1441,"statistic":19},[],{"title":1439},{"VI":1440},"Department of Physics, Tsinghua University, Beijing, China",[],{"title":1443,"gsAuthor":1445},{"VI":1444},"Pengfei 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nanostructures have sharp tips and edges, and the gap between each trunk and branch is narrow. The structure is ideal for generating high-density plasmonic “hot spots” to achieve a high-intensity local electromagnetic (EM) field, which is beneficial for improving the substrate Raman activity. In this paper, an electrochemical method is used to prepare a silver fractal nanostructure substrate. A single layer of graphene is transferred to the surface of the silver fractal structure substrate by a wet chemical transfer method to prepare a graphene\u002Fmetal (G\u002Fsilver fractal) nanostructure composite substrate. Experimental observations show that G\u002Fsilver fractal nanostructures exhibit higher Raman activity than that of pure silver fractal nanostructures. Numerical simulation calculation also verifies the accuracy of the experiment. In addition, the diversity of substrate detection is analyzed, and the experimental results show that the substrate can detect Rh6G and CV probe molecules simultaneously, which provides an experimental basis for investigating multichannel Raman spectroscopy sensing substrates. 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W (1998) Interfaces and thin films as seen by bound electromagnetic waves. 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Nature (London) 424:824–830",{"doi":1303},{"id":1299,"text":2341,"url":1301,"identifiers":2342},"Hutter E, Fendler JH (2004) Exploitation of localized surface plasmon resonance. Adv Mater 16:1685–1706",{"doi":1303},{"id":1299,"text":2344,"url":1301,"identifiers":2345},"Lerman GM, Yanai A, Ben-Yosef N, Levy U (2010) Demonstration of an elliptical plasmonic lens illuminated with radially-like polarized field. Opt Express 18(10):10871–10877",{"doi":1303},{"id":1299,"text":2347,"url":1301,"identifiers":2348},"Baron CA, Elezzabi AY (2009) Active plasmonic devices via electron spin. Opt Express 17(9):71171–77129",{"doi":1303},{"id":1299,"text":2350,"url":1301,"identifiers":2351},"Liu ZW, Steele JM, Srituravanich W, Pikus Y, Sun C, Zhang X (2005) Focusing surface plasmons with a plasmonic lens. Nano Lett 5(9):1726–1729",{"doi":1303},{"id":1299,"text":2353,"url":1301,"identifiers":2354},"Lerman G, Yanai A, Levy U (2009) Demonstration of nanofocusing by the use of plasmonic lens illuminated with radially polarized Light. Nano Lett 9:2139–2143",{"doi":1303},{"id":1299,"text":2356,"url":1301,"identifiers":2357},"Zhan Q (2006) Evanescent Bessel beam generation via surface plasmon resonance excitation by a radially polarized beam. Opt Lett 31:1726–1728",{"doi":1303},{"id":1299,"text":2359,"url":1301,"identifiers":2360},"Gorodetski Y, Niv A, Kleiner V, Hasman E (2008) Observation of the spin-based plasmonic effect in nanoscale structures. Phys Rev Lett 101:043903",{"doi":1303},{"id":1299,"text":2362,"url":1301,"identifiers":2363},"Yang S, Chen W, Nelson RL, Zhan Q (2009) Miniature circular polarization analyzer with spiral plasmonic lens. Opt Lett 34:3047–3049",{"doi":1303},{"id":1299,"text":2365,"url":1301,"identifiers":2366},"Chen W, Abeysinghe DC, Nelson RL, Zhan Q (2010) Experimental confirmation of miniature spiral plasmonic lens as a circular polarization analyzer. Nano Lett 10(6):2075–2079",{"doi":1303},{"id":1299,"text":2368,"url":1301,"identifiers":2369},"Miao J, Wang Y, Guo C, Tian Y, Guo S, Liu Q, Zhou Z (2011) Plasmonic lens with multiple-turn spiral nano-structures. Plasmonics 6:235–239",{"doi":1303},{"id":1299,"text":2371,"url":1301,"identifiers":2372},"Wang T, Wang X, Kuang C, Hao X, Liu X (2010) Experimental verification of the far-field subwavelength focusing with multiple concentric nanorings. Appl Phys Lett 97:231105",{"doi":1303},{"id":19,"text":2374,"url":19,"identifiers":2375},"Fu Y, Zhou X (2010) Topical review: plasmonic lenses. Plasmonics 5(3):287–310",{},{"id":1299,"text":2377,"url":1301,"identifiers":2378},"Wang J, Zhou W (2010) Experimental investigation of focusing of gold planar plasmonic lenses. Plasmonics 5:325–329",{"doi":1303},{"id":19,"text":2380,"url":2381,"identifiers":2382},"FDTD Solutions. Lumerical Solutions Inc, http:\u002F\u002Fwww.lumerical.com.","http:\u002F\u002Fwww.lumerical.com",{},{"id":1299,"text":2384,"url":1301,"identifiers":2385},"Palik ED (1985) Handbook of optical constants of solids. Academic, New York",{"doi":1303},{"id":1299,"text":2387,"url":1301,"identifiers":2388},"Nikitin A, Lopez-Tejeira F, Martin-Moreno L (2007) Scattering of surface plasmon polaritons by one-dimensional inhomogeneities. Phys Rev B 75(3):35129",{"doi":1303},{"id":2390,"createTime":2391,"updateTime":2392,"relativeEntities":2393,"slug":2394,"properties":2395,"entityType":201,"verifyStatus":202,"verifyTime":2408,"verifyNote":204,"languages":19,"translateLanguages":19,"viewCount":20,"primaryUrl":2409,"fullTextUrl":19,"authors":2410,"publicationType":263,"publisherRelationship":2635,"citationCount":20,"citationInfo":2690,"publishDate":2693,"publishYear":2691,"citationAnalyzeStatus":1604,"lastCitationAnalyze":2694,"indexDatabases":2695,"openAccess":19,"references":19,"isForceReanalyzing":327},"ad1e4e29-0e16-4461-8121-38ebccec1d72","2024-04-06T19:33:23.224+00:00","2026-07-26T02:04:56.017+00:00",[],"Eco-Friendly-Fabrication-of-Silver-Nanoparticles-for-Sustainable-Water-Purification-and-Antibacterial-Synergy",{"abstract":2396,"title":2398,"gsPaper":2400,"keywords":2402,"references":2404,"doi":2406},{"EN":2397},"Silver nanoparticles (AgNPs) were synthesized using the aqueous extract of Terminalia chebula (T-Chebula) fruits. Characterization through X-ray diffraction (XRD) and scanning electron microscopy (SEM) revealed AgNPs with a crystalline size ranging from 21 to 24 nm. The biosynthesized AgNPs exhibited a morphology unique to T-Chebula-AgNPs (TC-AgNPs), with an average size of 50 nm and a band gap energy of 2.8 eV. Evaluation of antimicrobial properties against Escherichia coli (E. coli) showcased the potential antibacterial activity of AgNPs compared to the standard gentamicin antibiotic. Notably, increasing concentrations of TC-AgNPs correlated with larger zones of inhibition, highlighting their efficacy. In contrast, the T-Chebula extract alone showed no bactericidal activity. Furthermore, under visible light irradiation, TC-AgNPs exhibited significant catalytic potential in degrading water-soluble industrial methylene (MB) dyes, achieving 92% dye degradation rate compared to the previous studies. The stability and recyclability of TC-AgNPs were notably robust across three iterations. Biogenically synthesized TC-AgNPs demonstrate exceptional potential in degrading organic pollutants and deactivating microorganisms. These findings underscore their promising applications in microbial control and the photodegradation of organic pollutants, highlighting their role in sustainable environmental remediation efforts.",{"EN":2399},"Eco-Friendly Fabrication of Silver Nanoparticles for Sustainable Water Purification and Antibacterial Synergy",{"VOID":2401},"[\"7755675044795686056\"]",{"EN":2403},"",{"VOID":2405},"Ahmad J et al (2016) Differential cytotoxicity of copper ferrite nanoparticles in different human cells. J Appl Toxicol 36(10):1284–1293\nHe HM et al (2022) Metal-organic framework supported Au nanoparticles with organosilicone coating for high-efficiency electrocatalytic N2 reduction to NH3. 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