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other provinces and regions in Vietnam and other country.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Address\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Headquarters of Can Tho Journal of Medicine and Pharmacy, located Scientific Research and International Cooperation Office: 179 Nguyen Van Cu Street, An Khanh Ward, Ninh Kieu District, Can Tho City, Vietnam.\u003C\u002Fspan>\u003C\u002Fp>","\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Ngày 16\u002F7\u002F2015, Tạp chí Y Dược học Cần Thơ được cấp chỉ số quốc tế: ISSN 2354-1210.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Từ tháng 4\u002F2016, Tạp chí đã được Hội đồng Giáo sư ngành Y đưa vào danh sách các tạp chí khoa học Y học được tính điểm công trình 0-0,5 điểm cho một bài báo đăng.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Năm 2020 Tạp chí Y Dược học Cần Thơ đã được phê duyệt vào danh mục của các Hội đồng Giáo sư ngành Dược học được tính điểm công trình 0-0,5 điểm cho một bài báo đăng.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tạp chí Y Dược học Cần Thơ ra 12 số\u002Fnăm, 180-200 trang\u002Fsố.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Từ tháng 12\u002F2022 Tạp chí Y Dược học Cần Thơ là thành viên của hệ thống Crossref và từ tháng 01\u002F2023 tạp chí thực hiện bình duyệt online kín 2 chiều nhằm tăng tính minh bạch, tin cậy của các công trình nghiên cứu khoa học và đảm bảo tốt nhất chất lượng khoa học của bài viết.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tôn chỉ, mục đích và phạm vi của tạp chí\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tôn chỉ và mục đích hoạt động của tạp chí: xuất bản nhằm mục đích phổ biến kết quả từ các đề tài nghiên cứu khoa học; giao lưu trao đổi khoa học, chia sẻ kinh nghiệm, học tập, đồng thời cập nhật thông tin khoa học mới trong các lĩnh vực y, sinh, dược học trong và ngoài nước.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Phạm vi của tạp chí: Tạp chí xuất bản được chia thành 3 chuyên mục: (i) Bài báo nghiên cứu khoa học là kết quả công trình nghiên cứu khoa học có giá trị đã được triển khai nghiên cứu, (ii) Bài tổng quan y, sinh, dược học: phục vụ mục tiêu đào tạo liên tục trong lĩnh vực y, sinh, dược học; nhằm hệ thống hóa những kiến thức kinh điển và hiện đại; (iii) Thông tin cập nhật kiến thức mới về y, sinh, dược học trong nước và trên thế giới.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Chính sách truy cập mở\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tạp chí Y Dược học Cần Thơ áp dụng chính sách truy cập mở đối với các bài báo đã xuất bản đến với độc giả, nhằm mở rộng cơ hội tiếp cận các kết quả nghiên cứu chất lượng cao và tăng cường trao đổi kiến thức. Tạp chí đăng tải trực tuyến (miễn phí) toàn văn các bài báo được công bố trên website của Tạp chí (https:\u002F\u002Ftapchi.ctump.edu.vn).\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Đạo đức xuất bản\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tạp chí Y Dược học Cần Thơ cam kết tuân thủ đạo đức xuất bản phù hợp với các hướng dẫn và tiêu chuẩn của the Committee on Publication Ethics (COPE), tuân thủ các nguyên tắc của COPE’s Core Practices, Best Practices Guidelines for Journal Editors và Guidelines on Good Publication Practices.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Bản thảo bài báo chỉ được chấp nhận khi được tác giả chịu trách nhiệm chính cam kết các nội dung sau: Các nội dung của bản thảo chưa được đăng tải toàn bộ hoặc một phần ở các tạp chí khác; Tất cả các tác giả đều có đóng góp một cách đáng kể vào quá trình nghiên cứu hoặc chuẩn bị bản thảo và cùng chịu trách nhiệm về các nội dung của bản thảo; Tuân thủ các biện pháp đảm bảo đạo đức nghiên cứu (ví dụ thỏa thuận đồng ý tham gia nghiên cứu).\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Cam kết bảo mật\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tạp chí cam kết thực hiện và tuân thủ các quy định của luật và các văn bản hướng dẫn liên quan đến bảo mật thông tin cá nhân trên không gian mạng. Các thông tin mà người dùng (tác giả, độc giả, biên tập viên, người phản biện) nhập vào các biểu mẫu trên Hệ thống Quản lý xuất bản trực tuyến của tạp chí chỉ được sử dụng vào các mục đích đã được tuyên bố rõ ràng và sẽ không được cung cấp cho bất kỳ bên thứ ba nào khác, hay dùng vào bất kỳ mục đích nào khác.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Phí gửi bài\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Lệ phí gửi đăng bài: 1.000.000đ\u002Fbài báo\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Lệ phí gửi đăng nhanh: 1.500.000đ\u002Fbài báo\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Đối với tác giả là cán bộ viên chức thuộc Trường Đại học Y Dược Cần Thơ thì được hỗ trợ 50% lệ phí gửi đăng bài.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Đối với sinh viên thực hiện đề tài nghiên cứu khoa học cấp trường được hỗ trợ 100% lệ phí đăng bài ( Tác giả gửi đính kèm “ Quyết định về việc giao tổ chức thực hiện đề tài nghiên cứu khoa học cấp Trường của sinh viên”).\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Hình thức nộp lệ phí:\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">1. Tiền mặt:\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Nộp trực tiếp tại Phòng Tài chính - Kế toán, Trường Đại học Y Dược Cần Thơ, số 179 Nguyễn Văn Cừ, P. An Khánh, Q. Ninh Kiều, thành phố Cần Thơ.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">2. Chuyển khoản:\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tên Tài khoản: Trường ĐHYD Cần Thơ, Số TK: 0111000115668, tại ngân hàng Vietcombank chi nhánh Cần Thơ.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Thời gian: Áp dụng từ ngày 01\u002F02\u002F2023.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">* Phí gửi bài không được hoàn trả khi bài viết bị từ chối hoặc tác giả xin rút bài viết.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Quy trình phản biện bài báo\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tạp chí Y Dược học Cần Thơ thực hiện quy trình phản biện kín hai chiều nghiêm ngặt. Danh tính của những người phản biện không được tiết lộ cho các tác giả và ngược lại. Quy trình thẩm định bài báo đăng gồm các bước sau:\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tiếp nhận bản thảo\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Tác giả liên hệ gửi bản thảo đến Tạp chí qua hệ thống trực tuyến tại website: https:\u002F\u002Ftapchi.ctump.edu.vn. Hướng dẫn về cách đăng ký, gửi bài và chuẩn bị bản thảo được cung cấp trên website của Tạp chí.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Sàng lọc sơ bộ\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Sau khi Tòa soạn nhận được bài báo của tác giả, Ban Thư ký sẽ tiến hành kiểm tra sơ bộ bài báo (các yêu cầu về nội dung và hình thức). Những bài báo không đúng quy cách hoặc có nội dung không phù hợp hoặc vi phạm bản quyền sẽ bị từ chối (Ban Thư ký thông báo phản hồi đến tác giả trong vòng 1 tuần). Những bài báo đủ điều kiện, được Ban Thư ký tòa soạn chuyển đến Ban Biên tập có cùng chuyên môn với nội dung bài báo để đề xuất người phản biện. Thời gian kể từ khi Ban Biên tập nhận bài báo đến khi đề xuất người phản biện bài báo chậm nhất là 5 ngày.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Vòng phản biện\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">1. Ban Thư ký gửi bài và yêu cầu phản biện đến 02 phản biện độc lập.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">2. Các phản biện gởi nhận xét cho Ban Thư ký. Thời gian từ khi gửi bài cho phản biện đến khi nhận ý kiến của phản biện tối đa là 20 ngày.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Xử ký kết quả phản biện\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">1. Nếu ý kiến đồng ý cho đăng và không cần chỉnh sửa, Ban Thư ký tiếp tục đăng bài theo qui trình.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">2. Nếu ý kiến đồng ý đăng và cần chỉnh sửa, Ban Thư ký sẽ thông tin đến tác giả chỉnh sửa theo yêu cầu của người phản biện. Thời gian chỉnh sửa và gửi lại kéo dài không quá 2 tuần, từ khi tác giả bài báo nhận được thông tin (Quá trình này có thể lặp lại tối đa 2 lần\u002F1 bài báo). Khi có sự thống nhất, đồng ý của người phản biện; bài báo được tiếp tục đăng theo qui trình.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">3. Những bài báo có chất lượng không đạt yêu cầu, cả 2 phản biện không đồng ý cho đăng sẽ bị Tòa soạn từ chối đăng.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">Xuất bản\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">1. Ban Thư ký tổng hợp các bản thảo đã được tác giả hoàn thiện sau thẩm định trình Ban Biên tập xem xét, Tổng Biên tập phê duyệt, quyết định bài đăng theo các tiêu chí: sự phù hợp nội dung với tôn chỉ và mục đích, thể loại bài viết (ưu tiên các bài có bài có nghiên cứu chuyên sâu, hàm lượng khoa học cao), đóng góp mới bài báo, bài báo được ưu tiên đăng trong số gần nhất của Tạp chí theo thứ tự: tính thời sự, chất lượng bài báo và thời gian gửi bài.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">2. Ban Biên tập và Ban Thư ký biên tập bản thảo, chế bản, đọc rà soát lỗi. Thời gian hoàn thành từ 10-15 ngày.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">3. Ban Thư ký có trách nhiệm thông báo cho tác giả bài báo (bằng e-mail) về tình hình phê duyệt bài báo, thời gian, số kỳ, tập xuất bản bài báo theo qui định.\u003C\u002Fspan>\u003C\u002Fp>\u003Cp>\u003Cbr>\u003C\u002Fp>\u003Cp>\u003Cspan style=\"color: rgb(0, 0, 0);\">4. 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Core\u002Fshell nanoparticles were synthesized by means of laser ablation in ethanol without using a catalyst. The structural and optical properties of Au@LiNbO3 core\u002Fshell nanoparticles as a function of laser fluence are investigated. To fabricate the photodetector, a thin film of Au@LiNbO3 was deposited on a single crystal silicon substrate. X-ray diffraction (XRD) results show that the synthesized nanocomposite is crystalline with a rhombohedral structure and the presence of peaks related to a gold cubic structure, indicating the formation of a core\u002Fshell nanocomposite. Transmission electron microscopy (TEM) investigations confirm the formation of core\u002Fshell spherical nanoparticles, whose size depends on the laser fluence. The optical properties reveal that the optical energy gap of LiNbO3 was 4.08 eV, while the energy gap of the Au@LiNbO3 core\u002Fshell prepared at 1.3, 1.6, 2, and 2.2 J\u002Fcm2 was 3.6, 3.49, 3.4, and 3.8 eV, respectively. The optoelectronic properties of the Au@LiNbO3\u002FSi photodetector fabricated without a buffer layer and an antireflection coating as a function of laser fluence are investigated. The optoelectronic properties show that the maximum responsivity was 0.43 A\u002FW at 400 nm for the Au@LiNbO3\u002FSi photodetector fabricated at 2 J\u002Fcm2. The variation of laser fluence affects the structural, optical, and electrical properties of Au@LiNbO3 core\u002Fshell. The best core\u002Fshell characteristics and photodetector were obtained at a laser energy of 2 J\u002Fcm2. The energy band diagram confirmed that the presence of Au significantly improved the photoresponse of the photodetector.\n",{"EN":1012},"Nanosecond Laser Ablation of Au@LiNbO3 Core–Shell Nanoparticles in Ethanol: Properties and Application in Optoelectronic Devices",{"VOID":1014},"Rüter CE, Brüske D, Suntsov S, Kip D (2020) Investigation of ytterbium incorporation in lithium niobate for active waveguide devices. Appl Sci 10:2189\nHuang J, Zhang D, Qi Z, Zhang B, Wang H (2021) Hybrid Ag–LiNbO3 nanocomposite thin films with tailorable optical properties. Nanoscale Adv 3:1121–1126\nMeriche F et al (2010) Fabrication and investigation of 1D and 2D structures in LiNbO3 thin films by pulsed laser ablation. Opt Mater (Amst) 32:1427–1434\nFakhri MA, AbdulRazzaq MJ, Alwahib AA, Muttlak WH (2020) Theoretical study of a pure LinbO3\u002FQuartz waveguide coated gold nanorods using supercontinuum laser source. Opt Mater 109:110363\nJeong IK, Park S (2011) Correlated thermal motion in ferroelectric LiNbO3 studied using neutron total scattering and a rietveld analysis. J Korean Phys Soc 59:2756–2759\nTaleb SM, Fakhri MA, Adnanm SA (2020) Optical Investigations of Nanophotonic LiNbO3 Films Deposited by Pulsed Laser Deposition Method, Defect and Diffusion. Forum 398:16–22\nMeriche F et al (2007) Micro structuring of LiNbO3 by using nanosecond pulsed laser ablation. 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Ferroelectrics 92:181–187\nTumuluri A, Raju KCJ (2014) Luminescence of LiNbO3 polycrystalline ceramics: effect of Sc2O3 and Lu2O3 doping. Ceram Int 40:3371–3377\nShih WC, Wang TL, Sun XY, Wu MS (2008) Growth of c-axis-oriented LiNbO3 films on ZnO\u002FSiO2\u002FSi substrate by pulsed laser deposition for surface acoustic wave applications. Jpn J Appl Phys 47:4056–4405\nFakhri MA, Hashim U, Salim ET, Salim ZT (2016) Preparation and charactrization of photonic LiNbO3generated from mixing of new raw materials using spry pyrolysis method. J Mater Sci: Mater Electron 27(12):13105–13112\nLi W et al (2019) Fabrication and characteristics of heavily Fe-doped LiNbO3\u002FSi heterojunction. Materials (Basel) 12:1–7\nZhang J, Li Li, Xiao Z, Liu Di, Wang S, Zhang J, Hao Y, Zhang W (2016) Hollow sphere TiO2–ZrO2 prepared by self-assembly with polystyrene colloidal template for both photocatalytic degradation and H2 evolution from water splitting. ACS Sustain Chem Eng 4:2037–2046\nZhang M, Ngo TH, Rabiah NI, Otanicar TP, Phelan PE, Swaminathan R, Dai LL (2014) Core–shell and asymmetric polystyrene–gold composite particles via one-step pickering emulsion polymerization. Langmuir 30(201):75–82\nWang DP, Zeng HC (2009) Multifunctional roles of TiO2 nanoparticles for architecture of complex core−shells and hollow spheres of SiO2−TiO2−polyaniline system. Chem Mater 21:4811–4823\nMei Y, Lu Y, Polzer F, Ballauff M, Drechsler M (2007) Catalytic activity of palladium nanoparticles encapsulated in spherical polyelectrolyte brushes and core−shell microgels. Chem Mater 19:1062–1069\nSalim ZT, Hashim U, Arshad MM, Fakhri MA, Salim ET (2017) Zinc oxide flakes-corolla lobes like nano combined structure for SAW applications. Mater Res Bull 86:215–219\nRichter J et al (2014) Core-shell potassium niobate nanowires for enhanced nonlinear optical effects. Nanoscale 6:5200–5207\nNichols WT, Sasaki T, Koshizaki N (2006) Laser ablation of a platinum target in water. I. Ablation Mechanisms. J Appl Phys 100:114911\nFakhri MA, Salim ET, Hashim U, Abdulwahhab AW, Salim ZT (2017) Annealing temperature effect on structural and morphological properties of nano photonic LiNbO3. J Mater Sci: Mater Electron 28(22):16728–16735\nIsmail RA, Mousa AM, Amin MH (2018) Synthesis of hybrid Au@PbI2 core-shell nanoparticles by pulsed laser ablation in ethanol. Mater Res Express 29:1–16\nKhalil I, Chou CM, Tsai KL, Hsu S, Yehye WA, Hsiao VKS (2019) Gold nanofilm-coated porous silicon as surface-enhanced Raman Scattering substrate. Appl Sci 9:1–12\nFakhri MA, Wahid MH, Badr BA, Kadhim SM, Salim ET, Hashim U, Salim ZT (2007) Enhancement of Lithium Niobate nanophotonic structures via spin-coating technique for optical waveguides application. Eur Phys J 162(7):01004\nSon JW, Orlov SS, Phillips B, Hesselink L (2006) Pulsed laser deposition of single phase LiNbO3 thin film waveguides. J Electroceramics 17:591–595\nFakhri MA, Wahid MH, Kadhim SM, Badr BA, Salim ET, Hashim U, Salim ZT (2017) The structure and optical properties of lithium niobate grown on quartz for photonics application. Eur Phys J Conf 162:01005\nSun D, Zhang G, Huang J, Wang H, Li Q (2014) Plant-mediated fabrication and surface enhanced raman property of flower-like Au@Pd nanoparticles. Materials (Basel) 7:1360–1369\nAdnan SA, Tawfiq ZH, Fakhri MA (2020) Gold Nanoparticles in Liquid Based on Photonic Crystal Fiber PCF for Sensors Application Defect Diffus Forum 398:23–28\nChen Y, Yeh C (2002) Laser ablation method : Use of surfactants to form the dispersed Ag nanoparticles. Colloids Surf A: Physicochem Eng Asp 197:133–139\nAli HS, Fakhri MA (2020) An overview of Au & photonic crystal fiber of sensors. 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RSC Adv 2:1913–1916\nFakhri MA, Salim ET, Wahid MH, Hashim U, Salim ZT (2018) Optical investigations and optical constant of nano lithium niobate deposited by spray pyrolysis technique with injection of Li2CO3 and Nb2O5 as raw materials. J Mater Sci: Mater Electron 29(11):9200–9208\nSantulli AC, Zhou H, Berweger S, Raschke MB, Sutter E, Wong SS (2010) Synthesis of single-crystalline one-dimensional LiNbO3 nanowires. CrystEngComm 12:2675–2678\nFakhri MA, Salim ET, Abdulwahhab AW, Hashim U, Salim ZT (2018) Optical properties of micro and nano LiNbO3thin film prepared by spin coating. Opt Laser Technol 103:226–232\nShandilya S, Sharma A, Tomar M, Gupta V (2012) Optical properties of the c-axis oriented LiNbO3 thin film. Thin Solid Films 520:2142–2146\nFakhri MA, Salim ET, Wahid MHA, Abdulwahhab AW, Salim ZT, Hashim U (2019) Heat treatment assisted-spin coating for LiNbO3 films preparation: Their physical properties. 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Sens Actuator A Phys 317:112373\nMousa AM, Ismail RA, Amin MH (2019) Hybrid p-Au@PbI2\u002Fn-Si heterojunction photodetector prepared by pulsed laser ablation in liquid. Optik - Int J for Light Electron Opt 183:933–941\nLi W, Cui J, Zheng D, Wang W, Wang S, Song S, Liu H, Kong Y, Xu J (2019) Fabrication and characteristics of heavily Fe-doped LiNbO3\u002FSi heterojunction. Materials 12:2659",{"VOID":1016},"10.1007\u002Fs11468-022-01780-y","PUBLICATION","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-022-01780-y",[1020,1036,1049],{"id":1021,"sortIndex":20,"researcher":19,"roles":1022,"affiliations":1024,"properties":1033,"displayName":1035,"givenName":19,"familyName":19},"e33a521a-8c2f-4bcc-9355-c2542419c68a",[1023],"AUTHOR",[1025],{"id":1026,"sortIndex":20,"affiliation":1027,"properties":19},"3ae37554-fea2-4aba-8eee-4f9a42c0f9d1",{"id":1026,"createTime":19,"updateTime":19,"relativeEntities":1028,"slug":19,"properties":1029,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1032,"statistic":19},[],{"title":1030},{"VI":1031},"Applied Science Department, University of Technology-Iraq, Baghdad, Iraq",[],{"title":1034},{"VI":1035},"Raid A. Ismail",{"id":1037,"sortIndex":176,"researcher":19,"roles":1038,"affiliations":1039,"properties":1046,"displayName":1048,"givenName":19,"familyName":19},"41da67e2-5a84-4fd6-ade5-d4a266925e71",[1023],[1040],{"id":1026,"sortIndex":20,"affiliation":1041,"properties":19},{"id":1026,"createTime":19,"updateTime":19,"relativeEntities":1042,"slug":19,"properties":1043,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1045,"statistic":19},[],{"title":1044},{"VI":1031},[],{"title":1047},{"VI":1048},"Evan T. Salim",{"id":1050,"sortIndex":293,"researcher":19,"roles":1051,"affiliations":1052,"properties":1068,"displayName":1070,"givenName":19,"familyName":19},"2494524d-b17c-45a3-abc9-d48a6b20a2f6",[1023],[1053,1059],{"id":1026,"sortIndex":20,"affiliation":1054,"properties":19},{"id":1026,"createTime":19,"updateTime":19,"relativeEntities":1055,"slug":19,"properties":1056,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1058,"statistic":19},[],{"title":1057},{"VI":1031},[],{"id":1060,"sortIndex":176,"affiliation":1061,"properties":1067},"c47eabf3-fac4-41bd-af06-79dcaf678d48",{"id":1060,"createTime":19,"updateTime":19,"relativeEntities":1062,"slug":19,"properties":1063,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1066,"statistic":19},[],{"title":1064},{"VI":1065},"Laser and Optoelectronic Department, University of Technology-Iraq, Baghdad, Iraq",[],{},{"title":1069},{"VI":1070},"Marwa S. Alwazny","ARTICLE",{"url":1018,"publisher":1073,"properties":1127},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":1074,"slug":10,"properties":1075,"entityType":17,"verifyStatus":18,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":20,"subjectFields":1079,"manageAffiliations":1096,"indexDatabases":1107,"url":102,"thumbnailPath":19,"statistic":1122,"gsStatistic":19,"type":180,"analyzePriority":19},[],{"issn":1076,"title":1077,"eissn":1078},{"VOID":13},{"EN":10},{"VOID":16},[1080,1084,1088,1092],{"id":23,"createTime":19,"updateTime":19,"relativeEntities":1081,"label":1082,"description":1083,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":26},{},{"id":29,"createTime":19,"updateTime":19,"relativeEntities":1085,"label":1086,"description":1087,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":32},{},{"id":35,"createTime":19,"updateTime":19,"relativeEntities":1089,"label":1090,"description":1091,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":38},{},{"id":41,"createTime":19,"updateTime":19,"relativeEntities":1093,"label":1094,"description":1095,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":44},{},[1097,1102],{"id":48,"createTime":19,"updateTime":19,"relativeEntities":1098,"slug":19,"properties":1099,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1101,"statistic":19},[],{"title":1100},{"EN":52},[],{"id":55,"createTime":19,"updateTime":19,"relativeEntities":1103,"slug":19,"properties":1104,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1106,"statistic":19},[],{"title":1105},{"EN":59},[61],[1108,1115],{"id":64,"indexDatabase":1109,"url":75,"indexYears":76,"academicFieldIds":1114,"indexDatabaseRanking":82},{"id":66,"createTime":19,"updateTime":19,"relativeEntities":1110,"label":1111,"description":1112,"key":72,"publicationTags":1113,"standard":19},[],{"EN":69,"VI":69},{"EN":69,"VI":71},[74],[78,79,80,81],{"id":84,"indexDatabase":1116,"url":97,"indexYears":19,"academicFieldIds":1121,"indexDatabaseRanking":19},{"id":86,"createTime":19,"updateTime":19,"relativeEntities":1117,"label":1118,"description":1119,"key":93,"publicationTags":1120,"standard":19},[],{"EN":89,"VI":89},{"EN":91,"VI":92},[95,96],[99,100,101],{"impactFactor":20,"impactFactorByYear":1123,"i10Index":116,"i10IndexLast5Year":117,"totalPublication":118,"totalPublicationByYear":1124,"totalCitation":138,"totalCitationByYear":1125,"totalCitationPerPublication":158,"totalCitationPerPublicationByYear":1126,"hindexLast5Year":179,"hindex":179},{"2012":105,"2013":106,"2014":106,"2015":107,"2016":108,"2017":109,"2018":110,"2019":111,"2020":112,"2021":113,"2022":114,"2023":115},{"2006":120,"2007":121,"2008":122,"2009":117,"2010":123,"2011":124,"2012":125,"2013":126,"2014":127,"2015":128,"2016":129,"2017":130,"2018":131,"2019":132,"2020":133,"2021":134,"2022":135,"2023":136,"2024":137},{"2006":140,"2007":141,"2008":142,"2009":143,"2010":144,"2011":145,"2012":146,"2013":147,"2014":148,"2015":149,"2016":150,"2017":151,"2018":152,"2019":153,"2020":154,"2021":155,"2022":135,"2023":156,"2024":157},{"2006":160,"2007":161,"2008":162,"2009":163,"2010":164,"2011":165,"2012":166,"2013":167,"2014":168,"2015":169,"2016":170,"2017":171,"2018":172,"2019":173,"2020":174,"2021":175,"2022":176,"2023":177,"2024":178},{"pages":1128,"volume":1130},{"VOID":1129},"561-576",{"VOID":1131},"18","2023-01-19",2023,[95,82],false,{"id":1137,"createTime":1138,"updateTime":1139,"relativeEntities":1140,"slug":1141,"properties":1142,"entityType":1017,"verifyStatus":203,"verifyTime":1139,"verifyNote":1153,"languages":19,"translateLanguages":19,"viewCount":20,"primaryUrl":1154,"fullTextUrl":19,"authors":1155,"publicationType":1071,"publisherRelationship":1197,"citationCount":19,"citationInfo":19,"publishDate":1252,"publishYear":1253,"citationAnalyzeStatus":18,"lastCitationAnalyze":19,"indexDatabases":1254,"openAccess":19,"references":19,"isForceReanalyzing":1135},"002fd343-efa4-4f6e-863a-fef233d2573f","2024-04-07T00:06:01.357+00:00","2024-12-10T12:06:31.213+00:00",[],"Polarization-Controlling-of-Multi-Resonant-Graphene-Based-Microstrip-Antenna",{"abstract":1143,"title":1145,"keywords":1147,"references":1149,"doi":1151},{"EN":1144},"In this paper, a graphene-based patch antenna is proposed. The antenna structure is designed so that each of the various antenna sections affected by chemical potential changes can provide a certain radiation behavior for the antenna far-field. The main purpose of the design is to control the polarization of the antenna only by changing its graphene layer Fermi energy level, so that its physical structure remains fixed. In this way, it is possible to achieve a wideband antenna with a favorable matching in the frequency range of 0.82 to 1.07 THz. It is possible to control its polarization in three states: the right- and left-hand circular polarization with an axial ratio less than 3 dB for a frequency range of 0.975 to 1.025 THz, and linear polarization in frequency range of 0.82 to 1.07 THz. The important point is that the physical structure of the antenna by adding circular layered patches at its edges provided us with the possibility of achieving a circular polarization, and with the creation of multi resonance behavior in the input impedance, provided the possibility of increasing bandwidth, significantly.",{"EN":1146},"Polarization Controlling of Multi Resonant Graphene-Based Microstrip Antenna",{"EN":1148},"",{"VOID":1150},"Khani S, Danaie M, Rezaei P (2019) Design of a single-mode plasmonic bandpass filter using a hexagonal resonator coupled to graded-stub waveguides. Plasmonics 14(1):53–62\nKim WK, Oh J, Yoon HS, Kim SJ, Park JY, Jung J, Jun SC (2019) Impedance variation on lattice misoriented few-layer graphene via layer decoupling. IEEE Trans Nanotechnol 18:55–61\nSrivastava T, Jha R (2018) Black phosphorus: a new platform for gaseous sensing based on surface plasmon resonance. IEEE Photonics Technol Lett 30(4):319–322\nCastellanos-Gomez A (2015) Black phosphorus: narrow gap, wide applications. J Phys Chem Lett 6(21):4280–4291\nJafari Chashmi M, Rezaei P, Kiani N (2019) Reconfigurable graphene-based v-shaped dipole antenna: from quasi-isotropic to directional radiation pattern. Opt –Int J Light Electron Opt 184:421–427\nRamazannia Tuloti SH, Rezaei P, Tavakkol Hamedani F (2019) Unit-cell with flexible transmission phase slope for ultra wideband transmitarray antennas. IET Microw Antennas Propag DOI. https:\u002F\u002Fdoi.org\u002F10.1049\u002Fiet-map.2018.5288\nJafari Chashmi M, Ghobadi H, Oliaei M (2015) Design and fabrication of aperture coupled microstrip increased bandwidth antenna. App Compute Electromagn Soc J 30(10):1109–1114\nRamazannia Tuloti SH, Rezaei P, Tavakkol Hamedani F (2018) High-efficient wideband transmitarray antenna. IEEE Antennas Wireless Propag Lett 17(5):817–820\nFakharian MM, Rezaei P, Orouji AA (2016) Polarization and radiation pattern reconfigurability of a planar monopole-fed loop antenna for GPS application. Radioengineering J 25(4):680–686\nMousavi Z, Rezaei P, Rafii V (2017) Single layer CPSSA array with change polarization diversity in broadband application. Int J RF Microw Comp-Aided Eng 27(4):1–8\nFakharian MM, Rezaei P, Orouji AA (2015) Reconfigurable multilane extended U-slot antenna with switchable polarization for wireless applications. IEEE Antennas Propag Mag 57(2):194–202\nWang G, Zhu J, Wei D, Jiang F, Huang Y (2019) Enhanced air microcavity of channel SPP waveguide HAL by graphene material. Plasmonics 14(2):313–320\nDehghan M, Moravvej-Farshi MK, Ghaffari-Miab M, Darvish G (2019) Ultra-compact spatial terahertz switch based on graphing plasmonic-coupled waveguide. Plasmonics Available Online:1–11. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-019-00921-0\nLiu Q, Liu M, Zhan S, Wu L, Xie S, Chen Z, Zhang Y (2018) Tunable Fano resonance based mode interference in waveguide-cavity-graphene hybrid structure. Plasmonics Available Online 14:1005–1011. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-018-0887-z\nZheng P, Yang H, Fan M, Hu G, Zhang R, Yun B, Cui Y (2018) A hybrid plasmonic modulator based on graphene on channel plasmonic polariton waveguide. Plasmonics 13(6):2029–2035\nZhu J, Xu Z, Xu W, Fu D, Wei D (2018) Surface plasmon polariton waveguide by bottom and top of graphene. Plasmonics 13(5):1513–1522\nJaiswal RK, Pundit N, Pathak NP (2019) Center frequency and bandwidth reconfigurable spoof surface plasmonic metamaterial band-pass filter. Plasmonics Available Online:1–8. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-019-00948-3\nTavousi A, Mansouri-Birjandi MA, Janfaza M (2019) Graphene nanoribbon assisted refractometer based biosensor for mid-infrared label-free analysis. Plasmonics Available Online 14:1207–1217. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-019-00909-w\nHuang Z, Dai Y, Su G, Yan Z, Zhan P, Liu F, Wang Z (2018) Dynamically tunable electromagnetically induced transparency in graphene and split-ring hybrid metamaterial. Plasmonics 13(2):451–457\nWei B, Jian S (2018) A nanoscale Fano resonator by graphene-gold dipolar interference. Plasmonics 13(6):1889–1895\nMoazami A, Hashemi M, Cheraghi Shirazi N (2019) High efficiency tunable graphene-based plasmonic filter in the THz frequency range. Plasmonics 14(2):359–363\nJiang L-H, Wang F, Liang R, Wei Z, Meng H, Dong H, Cen H (2018) Tunable terahertz filters based on graphene plasmonic all-dielectric metasurfaces. Plasmonics 13(2):525–530\nFeng Y, Liu Y, Wang X, Dong D, Shi Y, Tang L (2018) Tunable multichannel plasmonic filter based on a single graphene sheet on a Fibonacci quasiperiodic structure. Plasmonics 13(2):653–659\nDeng Q, Shao H, He W, Cheng K, Hu J, Sun B, Wang X, Liu G, Wang J (2018) Adjustable plasmonic multi-channel demultiplexer with graphene sheets and ring resonators. Plasmonics Available Online 14:993–998. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-018-0885-1\nKiani N, Afsahi M (2019) Design and fabrication of a compact SIW diplexer in C-band. Iranian J Electr Electron Eng (IJEEE) 15(2):189–194\nGhasemi M, Choudhury PK, Baqir MA (2019) On the double nano-coned graphite metasurface-based multilane CIC absorber. Plasmonics Available Online 14:1189–1195. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-019-00907-y\nXiong H, Tang M-C, Li M, Li D, Jiang Y-N (2018) Equivalent circuit method analysis of graphene-metamaterial (GM) absorber. Plasmonics 13(3):857–862\nZhao Z, Li G, Yu F, Yang H, Chen X, Lu W (2018) Sub-wavelength grating enhanced ultra-narrow graphene perfect absorber. Plasmonics 13(6):2267–2272\nRashiditabar R, Nozhat N, Zare MS (2018) Tunable plasmonic absorber based on TiN-nanosphere liquid crystal hybrid in visible and near-infrared regions. Plasmonics 13(6):1853–1859\nDeng Y-W, Peng L, Liao X, Jiang X (2018) An ultra-broadband terahertz absorber based on coplanar graphene and gold hybridized metasurface. Plasmonics Available Online 14:1057–1061. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs11468-018-0893-1\nSun L-P, Zhai X, Lin Q, Liu G-D, Wang L-L (2018) Tunable nearly perfect absorber based on graphene metamaterials at the mid-infrared region. Plasmonics 13(3):1043–1048\nLuan J, Fan M, Zheng P, Yang H, Hu G, Yun B, Cui Y (2019) Design and optimization of a graphene modulator based on hybrid plasmonic waveguide with double low-index slots. 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Plasmonics 10(6):1663–1673\nZhu B, Ren G, Gao Y, Wu B, Lian Y, Jian S (2017) Creation of graphene plasmons vortex via cross shape nanoantennas under linearly polarized incidence. Plasmonics 12(3):863–868\nAditya RANS, Thampy AS (2019) Behavioral and modal analysis of graphene-based polygonal optical antenna for enhanced bio-molecular detection. Plasmonics 14(2):293–302\nLiu H, Sun S, Wu L, Bai P (2014) Optical near-field enhancement with graphene bowtie antennas. Plasmonics 9(4):845–850\nDash S, Patnaik A (2018) Performance of graphene plasmonic antenna in comparison with their counterparts for low-terahertz applications. Plasmonics 13(6):2353–2360\nEkşioğlu Y, Cetin AE, Durmaz H (2018) Multi-band plasmonic platform utilizing UT-shaped graphene antenna arrays. Plasmonics 13(3):1081–1088\nComputer Simulation Technology (CST), CST Microwave Studio Ver. 2015. www.cst.com.\nHanson GW (2008) Dyadic Green’s functions and guided surface waves for a surface conductivity model of graphene. J. 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J Phy Condens Matter 19(2):026222\nThampy AS, Darak MS, Dhamodharan SK (2015) Analysis of graphene based optically transparent patch antenna for terahertz communications. Physica E 66:67–73\nWibbeler J, Pfeifer G, Hietschold M (1998) Parasitic charging of dielectric surfaces in capacitive microelectromechanical systems (MEMS). Sens Actuators A Phys 71(1–2):74–80\nGómez-Díaz JS, Esquius-Morote M, Perruisseau-Carrier J (2013) Plane wave excitation-detection of non-resonant plasmons along finite-width graphene strips. 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study the refractive-index sensing properties of plasmonic nanotubes with a dielectric core and ultrathin metal shell. The few nanometer thin metal shell is described by both the usual Drude model and the nonlocal hydrodynamic model to investigate the effects of nonlocality. We derive an analytical expression for the extinction cross section and show how sensing of the refractive index of the surrounding medium and the figure of merit are affected by the shape and size of the nanotubes. Comparison with other localized surface plasmon resonance sensors reveals that the nanotube exhibits superior sensitivity and comparable figure of merit.",{"EN":1263},"Refractive-Index Sensing with Ultrathin Plasmonic Nanotubes",{"VOID":1265},"Anker JN, Hall WP, Lyandres O, Shah NC, Zhao J, van Duyne RP (2008) Nat Mater 7:442\nProdan E, Radloff C, Halas NJ, Nordlander P (2003) Science 302:419\nBrongersma ML (2003) Nat Mater 2:296\nRaschke G, Brogl S, Susha AS, Rogach AL, Klar TA, Feldmann J, Fieres B, Petkov N, Bein T, Nichtl A, Kürzinger K (2004) Nano Lett 4:1853\nNehl CL, Grady NK, Goodrich GP, Tam F, Halas NJ, Hafner JH (2004) Nano Lett 4:2355\nTam F, Moran C, Halas NJ (2004) J Phys Chem B 108:17290\nBardhan R, Lal S, Joshi A, Halas NJ (2011) Acc Chem Res 44:936\nProdan E, Nordlander P (2004) J Chem Phys 120:5444\nDavid C, García de Abajo FJ (2011) J Phys Chem C 115:19470\nToscano G, Raza S, Jauho A-P, Mortensen NA, Wubs M (2012) Opt Express 20:4176\nBoardman AD, Paranjape BV (1977) J Phys F: Met Phys 7:1935\nDasgupta BB, Fuchs R (1981) Phys Rev B 24:554\nRuppin R (1973) Phys Rev Lett 31:1434\nRaza S, Toscano G, Jauho A-P, Wubs M, Mortensen NA (2011) Phys Rev B 84:121412(R)\nJones WE, Kliewer KL, Fuchs R (1969) Phys Rev 178:1201\nMcPhillips J, Murphy A, Jonsson MP, Hendren WR, Atkinson R, Höök F, Zayats AV, Pollard RJ (2010) ACS Nano 4:2210\nLim MA, Kim DH, Park CO, Lee YW, Han SW, Li Z, Williams RS, Park I (2012) ACS Nano 6:598\nSchröter U, Dereux A (2001) Phys Rev B 64:125420\nZhu J, Li KF (2011) Eur Phys J B 80:83\nRakić AD, Djurišić AB, Elazar JM, Majewski ML (1998) Appl Opt 37:5271\nFuchs R, Claro F (1987) Phys Rev B 35:3722\nMayer KM, Hafner JH (2011) Chem Rev 111:3828\nMahmoud MA, El-Sayed MA (2010) J Am Chem Soc 132:12704\nJeppesen C, Xiao S, Mortensen NA, Kristensen A (2010) Opt Express 18:25075\nRuppin R (2001) Opt Commun 190:205\nZuloaga J, Prodan E, Nordlander P (2009) Nano Lett 9:887\nÖztürk ZF, Xiao S, Yan M, Wubs M, Jauho A-P, Mortensen NA (2011) J Nanophotonics 5:051602\nvan de Hulst H (1957) Light scattering by small particles. 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nonlinear optical properties of single gold nanorods (GNRs) with a large diameter of ∼200 nm and a long length of ∼800 nm were investigated by using a focused femtosecond (fs) laser light with tunable wavelength. While the linear and nonlinear optical properties of small-sized GNRs have been extensively studied, the nonlinear optical properties of large-sized GNRs and the effects of high-order surface plasmon resonances remain unexplored. Second harmonic generation (SHG) or\u002Fand two-photon-induced luminescence (TPL) were observed in the nonlinear response spectra, and their dependences on excitation wavelength and polarization were examined. The scattering and absorption spectra of the small- and large-sized GNRs were compared by using the discrete dipole approximation method. It was found that the extinction of large-sized GNRs is dominated by scattering rather than absorption, which is dominant in small-sized GNRs. In addition, it was revealed that the excitation wavelength-dependent SHG of a GNR is governed by the linear scattering of the GNR and the maximum SHG is achieved at the valley of the scattering spectrum. In comparison, the excitation wavelength dependence of TPL is determined by the absorption spectrum of the GNR. The polarization-dependent SHG of a GNR exhibits a strong dependence on the dimension of the GNR, and it may appear as bipolar distributions parallel or perpendicular to the long axis of the GNR or multipole distributions.",{"EN":1421},"Nonlinear Optical Properties of Large-Sized Gold Nanorods",{"VOID":1423},"Raether H (1988) Surface plasmons on smooth and rough surfaces and on gratings. Springer, Berlin\nPrasad PN (2004) Nanophotonics. John Wiley & Sons, New York\nBrongersma ML, Kik PG (2007) Surface plasmon nanophotonics. Springer, Netherlands\nNie S, Emory SR (1997) Probing single molecules and single nanoparticles by surface-enhanced Raman scattering. Science 275:1102–1106\nQian X, Peng X, Ansari DO, Yin-Goen Q, Chen GZ, Shin DM, Yang L, Young AN, Wang MD, Nie S (2008) In vivo tumor targeting and spectroscopic detection with surface-enhanced Raman nanoparticle tags. Nat Biotechnol 26:83–90\nHuang X, El-Sayed IH, Qian W, El-Sayed MA (2007) Cancer cells assemble and align gold nanorods conjugated to antibodies to produce highly enhanced, sharp, and polarized surface raman spectra: a potential cancer diagnostic marker. Nano Lett 7:1591–1597\nLink S, El-Sayed MA (1999) Spectral properties and relaxation dynamics of surface plasmon electronic oscillations in gold and silver nanodots and nanorods. J Phys Chem B 103:8410–8426\nCanfield BK, Husu H, Laukkanen J, Bai B, Kuittinen M, Turunen J, Kauranen M (2007) Local field asymmetry drives second-harmonic generation in noncentrosymmetric nanodimers. Nano Lett 7:1251–1255\nLink S, Mohamed MB, El-Sayed MA (1999) Simulation of the optical absorption spectra of gold nanorods as a function of their aspect ratio and the effect of the medium dielectric constant. J Phys Chem B 103:3073–3077\nMing T, Zhao L, Yang Z, Chen H, Sun L, Wang J, Yan C (2009) Strong polarization dependence of plasmon-enhanced fluorescence on single gold nanorods. Nano Lett 9:3896–3903\nKelly KL, Coronado E, Zhao LL, Schatz GC (2003) The optical properties of metal nanoparticles: the influence of size, shape, and dielectric environment. J Phys Chem B 107:668–677\nChon JWM, Bullen C, Zijlstra P, Gu M (2007) Spectral encoding on gold nanorods doped in a silica sol–gel matrix and its application to high-density optical data storage. Adv Funct Mater 17:875–880\nZijlstra P, Chon JWM, Gu M (2009) Five-dimensional optical recording mediated by surface plasmons in gold nanorods. Nature 459:410–413\nLi X, Lan TH, Tien CH, Gu M (2012) Three-dimensional orientation-unlimited polarization encryption by a single optically configured vectorial beam. Nat Commun 3:998\nZijlstra P, Paulo PMR, Orrit M (2012) Optical detection of single non-absorbing molecules using the surface plasmon resonance of a gold nanorod. Nat Nanotechnol 7:379–382\nShao L, Fang C, Chen H, Man YC, Wang J, Lin HQ (2012) Distinct plasmonic manifestation on gold nanorods induced by the spatial perturbation of small gold nanospheres. Nano Lett 12:1424–1430\nChen L, Li GY, Liu GC, Dai QF, Lan S, Tie SL, Deng HD (2013) Sensing the moving direction, position, size, and material type of nanoparticles with the two-photon-induced luminescence of a single gold nanorod. J Phys Chem C 117:20146–201453\nSönnichsen C, Alivisatos AP (2005) Gold nanorods as novel nonbleaching plasmon-based orientation sensors for polarized single-particle microscopy. Nano Lett 5:301–304\nSau TK, Murphy CJ (2004) Seeded high yield synthesis of short Au nanorods in aqueous solution. Langmuir 20:6414–6420\nNikoobakht B, El-Sayed MA (2003) Preparation and growth mechanism of gold nanorods (NRs) using seed-mediated growth method. Chem Mater 15:1957–1962\nGrzelczak M, Pérez-Juste J, Mulvaney P, Liz-Marzán LM (2008) Shape control in gold nanoparticle synthesis. Chem Soc Rev 37:1783–1791\nKhanal BP, Zubarev ER (2007) Rings of nanorods. Angew Chem Ed 46:2195–2198\nVan der Zande BMI, Koper GJM, Lekkerkerker HNW (1999) Alignment of rod-shaped gold particles by electric fields. J Phys Chem B 103:5754–5760\nKhatua S, Chang W, Swanglap P, Olson J, Link S (2011) Active modulation of nanorod plasmons. Nano Lett 11:3797–3802\nPelton M, Liu M, Kim HY, Smith G, Guyot-Sionnest P, Scherer NF (2006) Optical trapping and alignment of single gold nanorods by using plasmon resonances. Opt Lett 31:2075–2077\nZins I, Schubert O, Sönnichsen C, Oddershede LB (2008) Quantitative optical trapping of single gold nanorods. Nano Lett 8:2998–3003\nMohamed MB, Volkov V, Link S, El-Sayed MA (2000) The ‘lightning’ gold nanorods: fluorescence enhancement of over a million compared to the gold metal. Chem Phys Lett 317:517–523\nEustis S, El-Sayed MA (2005) Aspect ratio dependence of the enhanced fluorescence intensity of gold nanorods: experimental and simulation study. J Phys Chem B 109:16350–16356\nWang H, Huff TB, Zweifel DA, He W, Low PS, Wei A, Cheng J (2005) In vitro and in vivo two-photon luminescence imaging of single gold nanorods. Proc Natl Acad Sci U S A 102:15752–15756\nHubert C, Billot L, Adam PM, Bachelot R, Royer P, Grand J, Gindre D, Dorkenoo KD, Ford A (2007) Role of surface plasmon in second harmonic generation from gold nanorods. Appl Phys Lett 90:181105–181107\nButet J, Duboisset J, Bachelier G, Russier-Antoine I, Benichou E, Jonin C, Brevet P (2010) Optical second harmonic generation of single metallic nanoparticles embedded in a homogeneous medium. Nano Lett 10:1717–1721\nLink S, Burda C, Mohamed MB, Nikoobakht B, El-Sayed MA (2000) Femtosecond transient absorption dynamics of colloidal gold nanorods: shape independence of the electron-phonon relaxation time. Phys Rev B 61:6066–6090\nDeng HD, Li GC, Dai QF, Ouyang M, Lan S, Trofimov VA, Lysak TM (2013) Size dependent competition between second harmonic generation and two-photon luminescence observed in gold nanoparticles. Nanotechnology 24:075201\nPayne EK, Shuford KL, Park S, Schatz GC, Mirkin CA (2006) Multipole plasmon resonances in gold nanorods. J Phys Chem B 110:2150–2154\nOkamoto H, Imura K (2009) Near-field optical imaging of enhanced electric fields and plasmon waves in metal nanostructures. Prog Surf Sci 84:199–229\nYurkin MA, Maltsev VP, Hoekstra AG (2007) The discrete dipole approximation: an overview and recent developments. J Quant Spectrosc Radiat Transf 106:558–589\nDraine BT, Flatau PJ (2009) User guide to the giscrete dipole approximation code, DDSCAT 7.0. http:\u002F\u002Farxiv.org\u002Fabs\u002F0809.0337\nThe information on the refractive indices of materials are available on website http:\u002F\u002Frefractiveindex.info\u002F\nJain PK, Lee KS, El-Sayed IH, El-Sayed MA (2006) Calculated absorption and scattering properties of gold nanoparticles of different size, shape, and composition: applications in biological imaging and biomedicine. J Phys Chem B 110:7238–7248\nDadap JI, Shan J, Heinz TF (2004) Theory of optical second-harmonic generation from a sphere of centrosymmetric material: small-particle limit. J Opt Soc Am B 21:1328–1347\nDadap JI, Shan J, Eisenthal KB, Heinz TF (1999) Second-harmonic rayleigh scattering from a sphere of centrosymmetric material. Phys Rev Lett 83:4045–4048\nBachelier G, Butet J, Russier-Antoine I, Jonin C, Benichou E, Brevet PF (2010) Origin of optical second-harmonic generation in spherical gold nanoparticles: local surface and nonlocal bulk contributions. Phys Rev B 82:235403\nBachelier G, Russier-Antoine I, Benichou E, Jonin C, Brevet P (2008) Multipolar second-harmonic generation in noble metal nanoparticles. 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novel surface plasmon resonance (SPR) sensor with transition metal dichalcogenides (TMDCs) and polyaniline (PANI)\u002Fchitosan composite for detection of heavy metal ions in an aquatic environment is proposed and analyzed. A novel Goos-Hänchen (GH) shift sensing scheme based on TMDCs and PANI\u002Fchitosan structure is proposed. The theory shows that the GH shift can be significantly enhanced in the SPR structure silver (Ag), TMDCs, and PANI\u002Fchitosan heterostructures. The refractive index of Cu2+ ion is 1.3516, and the maximum GH shift of the hybrid structure of Ag-MoSe2-PANI\u002Fchitosan is−2067 λ at resonance angle 69.19° with MoSe2 4 layers and PANI\u002Fchitosan 123 nm. When different Cu2+ ion concentrations are added into the sample layer, the refractive index of the sample and GH shift of the SPR sensor will change. The maximum sensitivity of 2.425 × 106 λ\u002FRIU is obtained by Ag-WSe2-PANI\u002Fchitosan structure, which is 463.42 times higher than the traditional SPR Ag film and 112.84 times higher than Ag-PANI\u002Fchitosan structure. Therefore, the configuration with GH shift provides a new development direction for the detection of heavy metal ions in an aquatic environment.",{"EN":1598},"Enhanced Goos-Hänchen Shift of SPR Sensor with TMDCs and Doped PANI\u002FChitosan Composites for Heavy Metal Ions Detection in Aquatic Environment",{"VOID":1600},"Kamran M, Malik Z, Parveen A, Huang L, Riaz M, Bashir S et al (2020) Ameliorative effects of biochar on rapeseed (Brassica napus L.) growth and heavy metal immobilization in soil irrigated with untreated wastewater. J Plant Growth Regul 39:266–281\nTurkyilmaz A, Cetin M, Sevik H, Isinkaralar K, Saleh EAA (2020) Variation of heavy metal accumulation in certain landscaping plants due to traffic density. Environ Dev Sustain 22:2385–2398\nJung K, Lee SY, Choi J, Lee YJ (2019) A facile one-pot hydrothermal synthesis of hydroxyapatite\u002Fbiochar nanocomposites: Adsorption behavior and mechanisms for the removal of copper(II) from aqueous media. 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Opt Express 27:17638–17647",{"VOID":1602},"10.1007\u002Fs11468-023-01837-6","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-023-01837-6",[1605,1620,1635,1648,1661],{"id":1606,"sortIndex":20,"researcher":19,"roles":1607,"affiliations":1608,"properties":1617,"displayName":1619,"givenName":19,"familyName":19},"863de717-4830-4117-b14a-85d569bf9b13",[1023],[1609],{"id":1610,"sortIndex":20,"affiliation":1611,"properties":19},"d83d0bc1-7adb-4c27-9a6b-896c36a337c1",{"id":1610,"createTime":19,"updateTime":19,"relativeEntities":1612,"slug":19,"properties":1613,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1616,"statistic":19},[],{"title":1614},{"VI":1615},"College of Mechanical and Electrical Engineering, Inner Mongolia Agricultural University, Hohhot, China",[],{"title":1618},{"VI":1619},"Min 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work reports the efficient excitation of surface plasmons polaritons (SPPs) by optimizing the geometrical parameters of \n                \n                  \n                \n                $$Mo{S}_{2}$$\n                \n              -Au to increase the efficiency of plasmonic-based photovoltaic cells. This technique is quite useful for near-field and far-field analysis which is direly needed to understand the associate phenomenon. The impact of Au nano-grating on light absorption by using the plasmonic effect of noble metals has been investigated. We proposed a simple geometry for enhancing the coupling efficiency between the multilayering of \n                \n                  \n                \n                $$Mo{S}_{2}$$\n                \n               and Au noble metal thin film by varying the slit widths (270–480) nm and material thickness (40–50) nm, while the periodicity was kept constant (720 nm) for unit cell. The efficient SPP excitation occurs at slit widths, near half, and few more than half of periodicity (360–420) nm. Resonance wavelength at different slit widths has also been observed. Efficient SPP excitation tends to increase the electric field around the slit, hence increasing the substrate ability to absorb light. For material thickness 40 nm and 50 nm, it has been observed that changing y-component of electric field \n                \n                  \n                \n                $$({E}_{y})$$\n                \n               in solar cell is effective in achieving greater absorption. The geometry has been simulated by using COMSOL Multiphysics RF module. This study will have significant impact for enhancing the coupling efficiency of the incident light into SPPs which have potential application to enhance the efficiency of the plasmonic-based solar cell.\n",{"EN":1745},"Improved Efficiency of MoS2-Au Multilayer Plasmonic-Based Solar Cells: Far- and Near-Field Analysis",{"VOID":1747},"Ali A, El-Mellouhi F, Mitra A, Aïssa BJN (2022) Research progress of plasmonic nanostructure-enhanced photovoltaic solar cells. 12(5):788\nWilson GM et al (2020) The 2020 photovoltaic technologies roadmap. 53(49):493001\nVeith-Wolf BA, Schäfer S, Brendel R, Schmidt JJSEM, Cells S (2018) Reassessment of intrinsic lifetime limit in n-type crystalline silicon and implication on maximum solar cell efficiency. 186:194–199\nMandal P, Sharma SJR (2016) Progress in plasmonic solar cell efficiency improvement: a status review. 65:537–552\nIqbal T et al (2019) An optimal Au grating structure for light absorption in amorphous silicon thin film solar cell. 14(1):147–154\nWang S et al. (2019) Limits to strong coupling of excitons in multilayer WS2 with collective plasmonic resonances. 6(2):286–293\nButun S, Tongay S, Aydin KJNI (2015) Enhanced light emission from large-area monolayer MoS2 using plasmonic nanodisc arrays. 15(4):2700–2704\nLu Y et al (2018) Magnetic polariton enhanced broadband absorption and photoresponse of monolayer MoS2 based on normal and anomalous metallic gratings. 51(29):295104\nIqbal T, Afsheen SCAP (2016) Coupling efficiency of surface plasmon polaritons for 1D plasmonic gratings: role of under-and over-milling. 11(5):1247–1256\nGhosh G, Palik ED (1997) Handbook of optical constants of solids, five-volume set: handbook of thermo-optic coefficients of optical materials with applications. Elsevier Sci\nOumekloul Z, Zeng S, Achaoui Y, Mir A, Akjouj AJP (2021) Multi-layer MoS2-based plasmonic gold nanowires at near-perfect absorption for energy harvesting. 16(5):1613–1621\nIqbal TJCAP (2015) Propagation length of surface plasmon polaritons excited by a 1D plasmonic grating. 15(11):1445–1452\nVempati S, Iqbal T, Afsheen SJJoAP (2015) Non-universal behavior of leaky surface waves in a one dimensional asymmetric plasmonic grating. 118(4):043103\nNagaraju S, Gudino LJ, Kadam BV, Ookalkar R, Udeshi S (2016) RSSI based indoor localization with interference avoidance for Wireless Sensor Networks using anchor node with sector antennas,” in 2016 International Conference on Wireless Communications, Signal Processing and Networking (WiSPNET). 2233–2237:IEEE\nJavaid M, Iqbal TJP (2016) Plasmonic bandgap in 1D metallic nanostructured devices. 11(1):167–173\nKoev ST, Agrawal A, Lezec HJ, Aksyuk VAJP (2012) An efficient large-area grating coupler for surface plasmon polaritons. 7:269–277\nIqbal T, Afsheen SJCAP (2016) Extraordinary optical transmission: role of the slit width in 1D metallic grating on higher refractive index substrate. 16(4):453–458\nIqbal T, Afsheen SJP (2017) One dimensional plasmonic grating: high sensitive biosensor. 12(1):19–25\nBillaudeau C, Collin S, Pardo F, Bardou N, Pelouard JLJOe (2009) Tailoring radiative and non-radiative losses of thin nanostructured plasmonic waveguides. 17(5):3490–3499\nIqbal T et al (2019) An optimal Au grating structure for light absorption in amorphous silicon thin film solar cell. 14:147–154\nIqbal TJP (2017) Coupling efficiency of surface plasmon polaritons: far-and near-field analyses. 12:215–221\nIqbal M et al (2022) Plasmonic-based solar cell: geometrical optimization of 1D-nanostructured grating for enhanced efficiency. 1–30\nJabeen M, Haxha SJIJoQE (2018) Increased optical absorption and light–matter interaction in silicon thin-film solar cell nanostructure using graphene and 2-D Au\u002FAg nanograting. 54(6):1–12\nRomanato F, Ongarello T, Zacco G, Garoli D, Zilio P, Massari MJAo (2011) Extraordinary optical transmission in one-dimensional gold gratings: near-and far-field analysis. 50(22):4529–4534\nDarweesh AA, Bauman SJ, Debu DT, Herzog JBJN (2018) The role of Rayleigh-Wood anomalies and surface plasmons in optical enhancement for nano-gratings. 8(10):809",{"VOID":1749},"10.1007\u002Fs11468-023-01853-6","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-023-01853-6",[1752,1767,1780,1793,1808,1823,1838],{"id":1753,"sortIndex":20,"researcher":19,"roles":1754,"affiliations":1755,"properties":1764,"displayName":1766,"givenName":19,"familyName":19},"0a14756a-153e-4dab-b775-54705b4c3f15",[1023],[1756],{"id":1757,"sortIndex":20,"affiliation":1758,"properties":19},"d67a5b8c-6fa5-40e0-806d-a01700d49e65",{"id":1757,"createTime":19,"updateTime":19,"relativeEntities":1759,"slug":19,"properties":1760,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1763,"statistic":19},[],{"title":1761},{"EN":1762},"Department of Physics, Faculty of Science, University of Gujrat, Hafiz Hayat Campus, Gujrat, Pakistan",[],{"title":1765},{"VI":1766},"Tahir 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self-referencing plasmonic platform is proposed and analyzed. By introducing a thin gold layer below a periodic two-dimensional nano-grating, the structure supports multiple modes including localized surface plasmon resonance (LSPR), surface plasmon resonance (SPR), and Fabry-Perot resonances. These modes get coupled to each other creating multiple Fano resonances. A coupled mode between the LSPR and SPR responses is spatially separated from the sensor surface and is not sensitive to refractive index changes in the surrounding materials or surface attachments. This mode can be used for self-referencing the measurements. In contrast, the LSPR dominant mode shifts in wavelength when the refractive index of the surrounding medium is changed. The proposed structure is easy to fabricate using conventional lithography and electron beam deposition methods. A bulk sensitivity of 429 nm\u002FRIU is achieved. The sensor also has the ability to detect nanometer thick surface attachments on the top of the grating.",{"EN":1922},"Self-Referencing Plasmonic Array Sensors",{"VOID":1924},"Feng J, Siu VS, Roelke A, Mehta V, Rhieu SY, Palmore GTR, Pacifici D (2012) Nanoscale plasmonic interferometers for multispectral, high-throughput biochemical sensing. Nano Lett 12(2):602–609\nMasson J-F (2017) Surface plasmon resonance clinical biosensors for medical diagnostics. ACS Sensors 2(1):16–30\nWei H, Abtahi SMH, Vikesland PJ (2015) Plasmonic colorimetric and SERS sensors for environmental analysis. Environ Sci: Nano 2(2):120–135\nTseng S-Y, Li S-Y, Yi S-Y, Sun AY, Gao D-Y, Wan D (2017) Food quality monitor: paper-based plasmonic sensors prepared through reversal nanoimprinting for rapid detection of biogenic amine odorants. ACS Appl Mater Interfaces 9(20):17306–17316\nWang C, Yu C (2013) Detection of chemical pollutants in water using gold nanoparticles as sensors: a review. Rev Anal Chem 32(1):1–14\nGolightly RS, Doering WE, Natan MJ (2009) Surface-enhanced Raman spectroscopy and homeland security: a perfect match? ACS Publications,\nValsecchi C, Brolo AG (2013) Periodic metallic nanostructures as plasmonic chemical sensors. Langmuir 29(19):5638–5649\nAlleyne CJ, Kirk AG, McPhedran RC, Nicorovici N-AP, Maystre D (2007) Enhanced SPR sensitivity using periodic metallic structures. Opt Express 15(13):8163–8169\nLuk'yanchuk B, Zheludev NI, Maier SA, Halas NJ, Nordlander P, Giessen H, Chong CT (2010) The Fano resonance in plasmonic nanostructures and metamaterials. Nat Mater 9(9):707–715\nWang Y, Sun C, Li H, Gong Q, Chen J (2017) Self-reference plasmonic sensors based on double Fano resonances. Nanoscale 9(31):11085–11092\nWu L, Chu H, Koh W, Li E (2010) Highly sensitive graphene biosensors based on surface plasmon resonance. Opt Express 18(14):14395–14400\nJakab A, Rosman C, Khalavka Y, Becker J, Trügler A, Hohenester U, Sönnichsen C (2011) Highly sensitive plasmonic silver nanorods. ACS Nano 5(9):6880–6885\nWu PC, Sun G, Chen WT, Yang K-Y, Huang Y-W, Chen Y-H, Huang HL, Hsu W-L, Chiang HP, Tsai DP (2014) Vertical split-ring resonator based nanoplasmonic sensor. Appl Phys Lett 105(3):033105\nSonnefraud Y, Verellen N, Sobhani H, Vandenbosch GA, Moshchalkov VV, Van Dorpe P, Nordlander P, Maier SA (2010) Experimental realization of subradiant, superradiant, and Fano resonances in ring\u002Fdisk plasmonic nanocavities. ACS Nano 4(3):1664–1670\nCetin AE, Altug H (2012) Fano resonant ring\u002Fdisk plasmonic nanocavities on conducting substrates for advanced biosensing. ACS Nano 6(11):9989–9995\nKing NS, Liu L, Yang X, Cerjan B, Everitt HO, Nordlander P, Halas NJ (2015) Fano resonant aluminum nanoclusters for plasmonic colorimetric sensing. ACS Nano 9(11):10628–10636\nZhang Z, Zhou B, Huang Y, Liao Z, Li Z, Li S, Wang S, Wen W (2014) Gold crescent nanodisk array for nanoantenna-enhanced sensing in subwavelength areas. Appl Opt 53(31):7236–7240\nLiu N, Weiss T, Mesch M, Langguth L, Eigenthaler U, Hirscher M, Sonnichsen C, Giessen H (2009) Planar metamaterial analogue of electromagnetically induced transparency for plasmonic sensing. Nano Lett 10(4):1103–1107\nYanik AA, Cetin AE, Huang M, Artar A, Mousavi SH, Khanikaev A, Connor JH, Shvets G, Altug H (2011) Seeing protein monolayers with naked eye through plasmonic Fano resonances. Proc Natl Acad Sci 108(29):11784–11789\nSherry LJ, Chang S-H, Schatz GC, Van Duyne RP, Wiley BJ, Xia Y (2005) Localized surface plasmon resonance spectroscopy of single silver nanocubes. Nano Lett 5(10):2034–2038\nKhorasaninejad M, Raeis-Zadeh SM, Amarloo H, Abedzadeh N, Safavi-Naeini S, Saini SS (2013) Colorimetric sensors using nano-patch surface plasmon resonators. Nanotechnology 24(35):355501\nGartia MR, Hsiao A, Pokhriyal A, Seo S, Kulsharova G, Cunningham BT, Bond TC, Liu GL (2013) Colorimetric plasmon resonance imaging using nano lycurgus cup arrays. Adv Optic Mater 1(1):68–76\nMa R-M, Ota S, Li Y, Yang S, Zhang X (2014) Explosives detection in a lasing plasmon nanocavity. Nat Nanotechnol 9(8):600–604\nRose A, Zhu Z, Madigan CF, Swager TM, Bulović V (2005) Sensitivity gains in chemosensing by lasing action in organic polymers. Nature 434(7035):876–879\nHueber DM (2000) Self referencing photosensor. Google Patents,\nLee S-M, Saini SS, Jeong M-Y (2010) Simultaneous measurement of refractive index, temperature, and strain using etched-core fiber Bragg grating sensors. IEEE Photon Technol Lett 22(19):1431–1433\nMontero D, Vázquez C, Möllers I, Arrúe J, Jäger D (2009) A self-referencing intensity based polymer optical fiber sensor for liquid detection. Sensors 9(8):6446–6455\nChan LL, Cunningham BT, Li PY, Puff D (2007) Self-referenced assay method for photonic crystal biosensors: application to small molecule analytes. Sensors Actuators B Chem 120(2):392–398\nZu-Yin Z, Li-Na W, Hai-Feng H, Kang-Wen L, Xun-Peng M, Guo-Feng S (2013) A high figure of merit localized surface plasmon sensor based on a gold nanograting on the top of a gold planar film. Chinese Physics B 22(10):104213\nChen J, Sun C, Gong Q (2014) Fano resonances in a single defect nanocavity coupled with a plasmonic waveguide. Opt Lett 39(1):52–55\nSrivastava SK, Abdulhalim I (2015) Self-referenced sensor utilizing extra-ordinary optical transmission from metal nanoslits array. Opt Lett 40(10):2425–2428\nAbutoama M, Abdulhalim I (2015) Self-referenced biosensor based on thin dielectric grating combined with thin metal film. 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Anal Lett 36(1):1–19\nKawata H, Carter JM, Yen A, Smith HI (1989) Optical projection lithography using lenses with numerical apertures greater than unity. Microelectron Eng 9(1–4):31–36\nWu B, Kumar A (2007) Extreme ultraviolet lithography: a review. J Vacuum Sci Technol B 25(6):1743–1761\nVieu C, Carcenac F, Pepin A, Chen Y, Mejias M, Lebib A, Manin-Ferlazzo L, Couraud L, Launois H (2000) Electron beam lithography: resolution limits and applications. Appl Surf Sci 164(1–4):111–117\nMoharam M, Gaylord T (1981) Rigorous coupled-wave analysis of planar-grating diffraction. JOSA 71(7):811–818\nSynopsys’s Rsoft. Available online: https:\u002F\u002Fwww.synopsys.com\nYakubovsky DI, Arsenin AV, Stebunov YV, Fedyanin DY, Volkov VS (2017) Optical constants and structural properties of thin gold films. Opt Express 25(21):25574–25587\nEriksson T, Granqvist C (1986) Infrared optical properties of silicon oxynitride films: experimental data and theoretical interpretation. 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Nanomaterials 7(9):238\nCubukcu E, Zhang S, Park Y-S, Bartal G, Zhang X (2009) Split ring resonator sensors for infrared detection of single molecular monolayers. Appl Phys Lett 95(4):043113\nSepúlveda B, Calle A, Lechuga LM, Armelles G (2006) Highly sensitive detection of biomolecules with the magneto-optic surface-plasmon-resonance sensor. Opt Lett 31(8):1085–1087\nElhadj S, Singh G, Saraf RF (2004) Optical properties of an immobilized DNA monolayer from 255 to 700 nm. Langmuir 20(13):5539–5543",{"VOID":1926},"10.1007\u002Fs11468-020-01155-1","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-020-01155-1",[1929,1944],{"id":1930,"sortIndex":20,"researcher":19,"roles":1931,"affiliations":1932,"properties":1941,"displayName":1943,"givenName":19,"familyName":19},"7084c664-691e-4443-b005-dd0499d5f9de",[1023],[1933],{"id":1934,"sortIndex":20,"affiliation":1935,"properties":19},"172132e4-d038-45a7-81ec-ff1d2ee58b3f",{"id":1934,"createTime":19,"updateTime":19,"relativeEntities":1936,"slug":19,"properties":1937,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1940,"statistic":19},[],{"title":1938},{"VI":1939},"Department of Electrical and Computer Engineering, University of Waterloo, Waterloo, Canada",[],{"title":1942},{"VI":1943},"Reza Kohandani",{"id":1945,"sortIndex":176,"researcher":19,"roles":1946,"affiliations":1947,"properties":1954,"displayName":1956,"givenName":19,"familyName":19},"0696d599-a591-452d-bbc8-9e143cff0d86",[1023],[1948],{"id":1934,"sortIndex":20,"affiliation":1949,"properties":19},{"id":1934,"createTime":19,"updateTime":19,"relativeEntities":1950,"slug":19,"properties":1951,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1953,"statistic":19},[],{"title":1952},{"VI":1939},[],{"title":1955},{"VI":1956},"Simarjeet S. Saini",{"url":1927,"publisher":1958,"properties":2012},{"id":6,"createTime":7,"updateTime":8,"relativeEntities":1959,"slug":10,"properties":1960,"entityType":17,"verifyStatus":18,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":20,"subjectFields":1964,"manageAffiliations":1981,"indexDatabases":1992,"url":102,"thumbnailPath":19,"statistic":2007,"gsStatistic":19,"type":180,"analyzePriority":19},[],{"issn":1961,"title":1962,"eissn":1963},{"VOID":13},{"EN":10},{"VOID":16},[1965,1969,1973,1977],{"id":23,"createTime":19,"updateTime":19,"relativeEntities":1966,"label":1967,"description":1968,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":26},{},{"id":29,"createTime":19,"updateTime":19,"relativeEntities":1970,"label":1971,"description":1972,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":32},{},{"id":35,"createTime":19,"updateTime":19,"relativeEntities":1974,"label":1975,"description":1976,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":38},{},{"id":41,"createTime":19,"updateTime":19,"relativeEntities":1978,"label":1979,"description":1980,"parentId":19,"standard":19,"scholarHubFieldId":19},[],{"EN":44},{},[1982,1987],{"id":48,"createTime":19,"updateTime":19,"relativeEntities":1983,"slug":19,"properties":1984,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1986,"statistic":19},[],{"title":1985},{"EN":52},[],{"id":55,"createTime":19,"updateTime":19,"relativeEntities":1988,"slug":19,"properties":1989,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":1991,"statistic":19},[],{"title":1990},{"EN":59},[61],[1993,2000],{"id":64,"indexDatabase":1994,"url":75,"indexYears":76,"academicFieldIds":1999,"indexDatabaseRanking":82},{"id":66,"createTime":19,"updateTime":19,"relativeEntities":1995,"label":1996,"description":1997,"key":72,"publicationTags":1998,"standard":19},[],{"EN":69,"VI":69},{"EN":69,"VI":71},[74],[78,79,80,81],{"id":84,"indexDatabase":2001,"url":97,"indexYears":19,"academicFieldIds":2006,"indexDatabaseRanking":19},{"id":86,"createTime":19,"updateTime":19,"relativeEntities":2002,"label":2003,"description":2004,"key":93,"publicationTags":2005,"standard":19},[],{"EN":89,"VI":89},{"EN":91,"VI":92},[95,96],[99,100,101],{"impactFactor":20,"impactFactorByYear":2008,"i10Index":116,"i10IndexLast5Year":117,"totalPublication":118,"totalPublicationByYear":2009,"totalCitation":138,"totalCitationByYear":2010,"totalCitationPerPublication":158,"totalCitationPerPublicationByYear":2011,"hindexLast5Year":179,"hindex":179},{"2012":105,"2013":106,"2014":106,"2015":107,"2016":108,"2017":109,"2018":110,"2019":111,"2020":112,"2021":113,"2022":114,"2023":115},{"2006":120,"2007":121,"2008":122,"2009":117,"2010":123,"2011":124,"2012":125,"2013":126,"2014":127,"2015":128,"2016":129,"2017":130,"2018":131,"2019":132,"2020":133,"2021":134,"2022":135,"2023":136,"2024":137},{"2006":140,"2007":141,"2008":142,"2009":143,"2010":144,"2011":145,"2012":146,"2013":147,"2014":148,"2015":149,"2016":150,"2017":151,"2018":152,"2019":153,"2020":154,"2021":155,"2022":135,"2023":156,"2024":157},{"2006":160,"2007":161,"2008":162,"2009":163,"2010":164,"2011":165,"2012":166,"2013":167,"2014":168,"2015":169,"2016":170,"2017":171,"2018":172,"2019":173,"2020":174,"2021":175,"2022":176,"2023":177,"2024":178},{"pages":2013,"volume":2015},{"VOID":2014},"1359-1368",{"VOID":2016},"15","2020-04-06",2020,[95,82],{"id":2021,"createTime":2022,"updateTime":2023,"relativeEntities":2024,"slug":2025,"properties":2026,"entityType":1017,"verifyStatus":203,"verifyTime":2023,"verifyNote":1153,"languages":19,"translateLanguages":19,"viewCount":20,"primaryUrl":2035,"fullTextUrl":19,"authors":2036,"publicationType":1071,"publisherRelationship":2104,"citationCount":19,"citationInfo":19,"publishDate":2164,"publishYear":2018,"citationAnalyzeStatus":18,"lastCitationAnalyze":19,"indexDatabases":2165,"openAccess":19,"references":19,"isForceReanalyzing":1135},"011c2caf-4dcf-4005-b171-96751b7ee5ac","2024-02-13T06:25:57.523+00:00","2025-02-20T14:21:35.387+00:00",[],"Analytical-and-Numerical-Models-of-a-Highly-Sensitive-MDM-Plasmonic-Nano-structure-in-Near-infrared-Range",{"abstract":2027,"title":2029,"references":2031,"doi":2033},{"EN":2028},"Plasmon-induced transparency (PIT) is a spotlight technique for environmental monitoring. In this regard, a highly sensitive and tunable multilayer sensor including Ag–SiO2–Ag is presented in near-infrared range for both transverse mode (TE) and transverse mode (TM) modes at different incident waves. Actually, the proposed multilayer plasmonic sensor is presented to study the optical and sensing properties at near-infrared frequencies based on 3D finite-difference time-domain (FDTD). Sensitivity and tunability of all optical sensors are important parameters in their design, which are calculated based on propagation properties including absorption and reflection spectra, numerically and analytically. Results of absorption and reflection show that the proposed sensor has max sensitivity of 693.8 nm\u002FRIU by Δn = 0.05 changing of middle refractive index and figure of merit (FoM) equal to 9.8. Also, the proposed nano-scale sensor can operate as a light propagation controlling with slow and fast light and multispectral sensor. By using silver metal in the sensor structure, the fast and slow light coefficient is obtained at 220 and 70, respectively. In addition, by increasing the incident angle of light, multiabsorption peaks are created which can be used as multiwindow sensor and PIT. The analytical results are in good agreement with the obtained results of coupled mode theory (CMT) method.",{"EN":2030},"Analytical and Numerical Models of a Highly Sensitive MDM Plasmonic Nano-structure in Near-infrared Range",{"VOID":2032},"Na L, Mesch M, Weiss T, Hentschel M, Giessen H (2010) Infrared perfect absorber and its application as plasmonic sensor. Nano Lett 10(7):2342–2348\nKoray A, Ferry VE, Briggs RM, Atwater HA (2011) Broadband polarization-independent resonant light absorption using ultrathin plasmonic super absorbers. Nat Commun 2:517\nMingbo P, Ma X, Li X, Guo Y, Luo X (2017) Merging plasmonics and metamaterials by two-dimensional subwavelength structures. J Mater Chem C 5(18):4361–4378\nShinpei O, Kimata M (2018) Metal-insulator-metal-based plasmonic metamaterial absorbers at visible and infrared wavelengths: a review. Materials 11(3):458\nSabah C, Dincer F, Karaaslan M, Unal E, Akgol O, Demirel E (2014) Perfect metamaterial absorber with polarization and incident angle independencies based on ring and cross-wire resonators for shielding and a sensor application. Opt Commun 322:137–142\nJakir HM, Faruque MRI, Islam MT (2018) Perfect metamaterial absorber with high fractional bandwidth for solar energy harvesting. PLoS One 13(11):e0207314\nZafar R, Nawaz S, Singh G, d’Alessandro A, Salim M (2018) Plasmonics-based refractive index sensor for detection of hemoglobin concentration. IEEE Sensors J 18(11):4372–4377\nWenhui L, Wen K, Lin J, Guo Z, Hu Q, Fang Y (2018) Plasmonic filter and sensor based on a subwavelength end-coupled hexagonal resonator. Appl Opt 57(22):6369–6374\nMeng L, Zhao D, Li Q, Qiu M (2013) Polarization-sensitive perfect absorbers at near-infrared wavelengths. Opt Express 21(101):A111–A122\nLi S, Gao J, Cao X, Li W, Zhang Z, Zhang D (2014) Wideband, thin, and polarization-insensitive perfect absorber based the double octagonal rings metamaterials and lumped resistances. J Appl Phys 116(4):043710\nOgawa S, Takagawa Y, Kimata M (2018) Broadband polarization-selective uncooled infrared sensors using tapered plasmonic micrograting absorbers. Sensors Actuators A Phys 269:563–568\nLe LN, Thang NM, Thuy LM, Tung NT (2017) Hybrid semiconductor–dielectric metamaterial modulation for switchable bi-directional THz absorbers. Opt Commun 383:244–249\nWu J, Guo J, Wang X, Jiang L, Dai X, Xiang Y, Wen S (2018) Dual-band infrared near-perfect absorption by Fabry-Perot resonances and surface phonons. Plasmonics 13(3):803–809\nDayal G, Ramakrishna SA (2013) Design of multi-band metamaterial perfect absorbers with stacked metal–dielectric disks. J Opt 15(5):055106\nChoudhury SD, Badugu R, Nowaczyk K, Ray K, Lakowicz JR (2012) Tuning fluorescence direction with plasmonic metal–dielectric–metal substrates. J Phys Chem Lett 4(1):227–232\nLu X, Wan R, Zhang T (2015) Metal-dielectric-metal based narrow band absorber for sensing applications. Opt Express 23(23):29842–29847\nZhu J, Ma Z, Sun W, Ding F, He Q, Zhou L, Ma Y (2014) Ultra-broadband terahertz metamaterial absorber. Appl Phys Lett 105(2):021102\nAlipour A, Farmani A, Mir A (2018) High sensitivity and tunable nanoscale sensor based on plasmon-induced transparency in plasmonic metasurface. IEEE Sensors J 18(17):7047–7054\nAlipour AH, Mir A (2018) Design and simulation of a high-selective plasmon-induced reflectance in coupled dielectric-metal-dielectric nano-structure for senor devices and slow light propagation. Plasmonics 1–11\nThanh TN, Tanaka T (2018) Characterizations of an infrared polarization-insensitive metamaterial perfect absorber and its potential in sensing applications. Photon Nanostruct-Fundam Appl 28:100–105\nC. Cen, , H. Lin, C. Liang, J. Huang, X. Chen, Z. Yi, Y. Tang, T. Duan, X. Xu, S. Xiao, Y. Yi Tunable plasmonic resonance absorption characteristics in periodic H-shaped graphene arrays. Superlattice Microst (2018), 120, 427, 435\nMeng L, Zhao D, Ruan Z, Li Q, Yang Y, Qiu M (2014) Optimized grating as an ultra-narrow band absorber or plasmonic sensor. Opt Lett 39(5):1137–1140\nAouani H, Rahmani M, Sipova H, Torres V, Hegnerová K, Beruete M, Homola J, Hong M, Navarro-Cía M, Maier SA (2013) Plasmonic nanoantennas for multispectral surface-enhanced spectroscopies. J Phys Chem C 117(36):18620–18626\nPelzman C, Cho S-Y (2018) Multispectral and polarimetric photodetection using a plasmonic metasurface. J Appl Phys 123(4):043107\nAkhavan A, Abdolhosseini S, Ghafoorifard H, Habibiyan H (2018) Narrow band total absorber at near-infrared wavelengths using monolayer graphene and sub-wavelength grating based on critical coupling. J Lightwave Technol 36(23):5593–5599\nAsgari S, Granpayeh N, Kashani ZG (2019) Plasmonic mid-infrared wavelength selector and linear logic gates based on graphene cylindrical resonator. IEEE Trans Nanotechnol 18:42–50\nVafapour Z (2018) Slowing down light using terahertz semiconductor metamaterial for dual-band thermally tunable modulator applications. Appl Opt 57(4):722–729",{"VOID":2034},"10.1007\u002Fs11468-020-01294-5","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-020-01294-5",[2037,2052,2065,2078,2091],{"id":2038,"sortIndex":20,"researcher":19,"roles":2039,"affiliations":2040,"properties":2049,"displayName":2051,"givenName":19,"familyName":19},"ebb08381-83c9-4033-b272-aeaf921c10b1",[1023],[2041],{"id":2042,"sortIndex":20,"affiliation":2043,"properties":19},"9309040d-02df-4198-a253-638f263a585e",{"id":2042,"createTime":19,"updateTime":19,"relativeEntities":2044,"slug":19,"properties":2045,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":2048,"statistic":19},[],{"title":2046},{"VI":2047},"School of Electrical and Computer Engineering, Lorestan University, Khorramabad, Iran",[],{"title":2050},{"VI":2051},"A. Jeddi Golfazani",{"id":2053,"sortIndex":176,"researcher":19,"roles":2054,"affiliations":2055,"properties":2062,"displayName":2064,"givenName":19,"familyName":19},"3237b420-4fa1-41ca-af3c-69e171839b91",[1023],[2056],{"id":2042,"sortIndex":20,"affiliation":2057,"properties":19},{"id":2042,"createTime":19,"updateTime":19,"relativeEntities":2058,"slug":19,"properties":2059,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":2061,"statistic":19},[],{"title":2060},{"VI":2047},[],{"title":2063},{"VI":2064},"A. 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reduced Rayleigh equation for the scattering of a surface plasmon polariton incident non-normally on a one-dimensional ridge or groove on an otherwise planar metal surface is solved by a purely numerical approach. The solution is used to calculate the transmission, reflection, and out-of-plane scattering coefficients of the surface plasmon polariton. The angular dependence of the out-of-plane scattering is found to have a conical nature.",{"EN":2176},"Scattering of an Obliquely Incident Surface Plasmon Polariton from Sub-Micron Metal Grooves and Ridges",{"VOID":2178},"Sánchez-Gil JA (1998) Surface defect scattering of surface plasmon polaritons: mirrors and light emitters. Appl Phys Lett 73:3509–3511\nSánchez-Gil JA, Maradudin AA (1999) Near-field and far-field scattering of surface plasmon polaritons by one-dimensional surface defects. Phys Rev B 60:8359–8367\nSánchez-Gil JA, Maradudin AA (2003) Resonant scattering of surface plasmon polariton pulses by nanoscale metal defects. Opt Lett 28:2255–2257\nSánchez-Gil JA, Maradudin AA (2004) Dynamic near-field calculations of surface-plasmon polariton pulses resonantly scattered at sub-micron metal defects. Opt Express 12:883–894\nSánchez-Gil JA, Maradudin AA (2005) Surface plasmon polariton scattering from a finite array of nano grooves\u002Fridges: efficient mirrors. Appl Phys Lett 86(1–3):251106\nMaradudin AA (1994) An impedance boundary condition for a rough surface, pp. 33–45. Topics in Condensed Matter Physics, ed. M.P. Das. Nova Science Publishers, New York\nNikitin AY, López-Tejeira F, Martín-Moreno L (2007) Scattering of surface plasmon polaritons by one-dimensional inhomogeneities. Phys Rev B75(1–8):035–129\nLeskova TA, Maradudin AAE, García-Guerrero E, Méndez ER (2010) The scattering of surface plasmon polaritons by nanoscale surface defects. Fiz Nizkh Temperatur 36:1022–1029\nChremmos I (2010) Magnetic field integral equation analysis of surface plasmon scattering by rectangular dielectric channel discontinuities. J Opt Soc Am A27:85–94\nBrucoli G, Martín-Moreno L (2011) Comparative study of surface plasmon scattering by shallow ridges and grooves. Phys Rev B 83(1–11):045–422\nBrucoli G, Martín-Moreno L (2011) Effect of defect depth on surface plasmon scattering by subwavelength surface defects. Phys Rev B 83(1–10):075–433\nKuttge MF, García de Abajo J, Polman A (2009) How grooves reflect and confine surface plasmon polaritons. Opt Express 17:10385–10392\nPolanco J, Fitzgerald RM, Maradudin AA (2013) Scattering of surface plasmon polaritons by one-dimensional surface defects. Phys Rev B 87:155417–155430\nNikitin AY, Martín-Moreno L (2007) Scattering coefficients of surface plasmon polaritons impinging at oblique incidence onto one-dimensional surface relief defects. Phys Rev B 75(1–4):081–405\nPetit R, Cadilhac M (1996) Sur la diffraction d’une onde plane par un réseau infiniment conducteur. C R Acad Sci B 262:468–471\nMillar RF (1969) On the Rayleigh assumption in scattering by a periodic surface. Proc Camb Philos Soc 65:773–791\nHill NR, Celli V (1978) Limits of convergence of the Rayleigh method for surface scattering. Phys Rev B 17:2478–2481\nVan den Berg PM, Fokkema JT (1979) The Rayleigh hypothesis in the theory of reflection by a grating. J Opt Soc Am 69:27–31\nVan den Berg PM, Fokkema JT (1980) The Rayleigh hypothesis in the theory of diffraction by a perturbation in a plane surface. Radio Sci 15:723–732\nSchlup WA (1984) On the convergence of the Rayleigh ansatz for hard-wall scattering on arbitrary periodic surface profiles. J Phys A: Math Gen 17:2607–2619\nDeSanto JA (1981) Scattering from a perfectly reflecting arbitrary periodic surface: an exact theory. Radio Sci 16:1315–1326\nPaulick TC (1990) Applicability of the Rayleigh hypothesis to real materials. Phys Rev B 42:2801–2824\nMillar RF (1973) The Rayleigh hypothesis and a related least-squares solution to scattering problems for periodic surfaces and other scatterers. Radio Sci 8:785–796\nRayleigh L (1896) The theory of sound, vol II, 2nd. MacMillan, London, pp 89, 297–311\nBrown GC, Celli V, Haller M, Marvin A (1984) Vector theory of light scattering from a rough surface: Unitary and reciprocal expansions. Surf Sci 136:381–397\nMaradudin AA, Mills DL (1976) The attenuation of Rayleigh surface waves by surface roughness. Ann Phys (N. Y.) 100:262–309. Appendix D\nPress WH, Teukolsky SA, Vetterling WT, Flannery BP (1992) Numerical recipes. Cambridge University Press, Cambridge, UK, pp 109–110\nPress WH, Teukolsky SA, Vetterling WT, Flannery BP (1992) Numerical recipes, Cambridge University Press, Cambridge, UK. Chapter 2",{"VOID":2180},"10.1007\u002Fs11468-015-9913-6","https:\u002F\u002Flink.springer.com\u002Farticle\u002F10.1007\u002Fs11468-015-9913-6",[2183,2198,2213],{"id":2184,"sortIndex":20,"researcher":19,"roles":2185,"affiliations":2186,"properties":2195,"displayName":2197,"givenName":19,"familyName":19},"5f2ea290-d890-49ac-baaf-80531d91607c",[1023],[2187],{"id":2188,"sortIndex":20,"affiliation":2189,"properties":19},"a1d40eb8-6471-4143-a185-843860c405d9",{"id":2188,"createTime":19,"updateTime":19,"relativeEntities":2190,"slug":19,"properties":2191,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":2194,"statistic":19},[],{"title":2192},{"VI":2193},"Department of Mathematics, University of Texas, El Paso, USA",[],{"title":2196},{"VI":2197},"J. 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Fitzgerald",{"id":2214,"sortIndex":293,"researcher":19,"roles":2215,"affiliations":2216,"properties":2228,"displayName":2230,"givenName":19,"familyName":19},"0a1c8977-c124-4efe-922f-b7116d81c304",[1023],[2217],{"id":2218,"sortIndex":20,"affiliation":2219,"properties":2225},"a080a1f9-21a6-4e14-800a-00039397123a",{"id":2218,"createTime":19,"updateTime":19,"relativeEntities":2220,"slug":19,"properties":2221,"entityType":19,"verifyStatus":19,"verifyTime":19,"verifyNote":19,"languages":19,"translateLanguages":19,"viewCount":19,"url":19,"parentIds":2224,"statistic":19},[],{"title":2222},{"VI":2223},"Department of Physics and Astronomy, University of California, Irvine, U.S.A.",[],{"title":2226},{"VI":2227},"Department of Physics and Astronomy, University of California, Irvine, USA",{"title":2229},{"VI":2230},"A. A. 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Multiple SPP modes were distinguished from waveguide modes in optical absorption for p-polarized plane wave. The degree of localization of multiple SPP waves was investigated by calculation of the time-averaged Poynting vector. The results showed that the long-range and short-range SPP waves can simultaneously be excited at both interfaces of metal core in this proposed structure which may be used in a broad range of sensing applications.",{"EN":2304},"Excitation of Multiple Surface Plasmon-Polaritons by a Metal Layer Inserted in an Equichiral Sculptured Thin Film",{"VOID":2306},"Polo JA, Lakhtakia A (2011) Surface electromagnetic waves: a review. Laser and Photonics Rev 5(2):234–246. https:\u002F\u002Fdoi.org\u002F10.1002\u002Flpor.200900050\nSwiontek SE, Pulsifer DP, Lakhtakia A (2013) Optical sensing of analytes in aqueous solutions with a multiple surface-plasmon-polariton-wave platform. Sci Rep 3(1):1409. https:\u002F\u002Fdoi.org\u002F10.1038\u002Fsrep01409\nPulsifer DP, Lakhtakia A (2009) Multiple surface plasmon polariton waves .Electron Lett 45:1137–1138. https:\u002F\u002Fdoi.org\u002F10.1049\u002Fel.2009.2049\nMackay TG, Lakhtakia A (2012) Modeling chiral sculptured thin films as platforms for surface-plasmonic-polaritonic optical sensing. IEEE Sensors J 12(2):273–280. https:\u002F\u002Fdoi.org\u002F10.1109\u002FJSEN.2010.2067448\nMotyka MA, Lakhtakia A (2008) Multiple trains of same-color surface plasmon-polaritons guided by the planar interface of a metal and a sculptured nematic thin film. Journal of Nanophotonics 2(1):021910. https:\u002F\u002Fdoi.org\u002F10.1117\u002F1.3033757\nFaryad M, Lakhtakia A (2011) Grating-coupled excitation of multiple surface plasmon-polariton waves. Phys Rev A 84(3):033852. https:\u002F\u002Fdoi.org\u002F10.1103\u002FPhysRevA.84.033852\nRobbie K, Brett MJ (1997) Sculptured thin films and glancing angle deposition: growth mechanics and applications. J Vac Sci Technol A 15(3):1460–1465. https:\u002F\u002Fdoi.org\u002F10.1116\u002F1.580562\nRobbie K, Sit JC, Brett MJ (1998) Advanced techniques for glancing angle deposition. J Vac Sci Technol B 16(3):1115. https:\u002F\u002Fdoi.org\u002F10.1116\u002F1.590019\nRobbie K, Brett MJ, Lakhtakia A (1996) Chiral sculptured thin films. Nature 384(6610):616. https:\u002F\u002Fdoi.org\u002F10.1038\u002F384616a0\nHodgkinson IJ, Lakhtakia A, hong Wu Q, Silva LD, McCall MW (2004) Ambichiral, equichiral and finely chiral layered structures. Opt Commun 239(4-6):353–358. https:\u002F\u002Fdoi.org\u002F10.1016\u002Fj.optcom.2004.06.005\nvan Popta AC, Brett MJ, Sit JC (2005) Double-handed circular Bragg phenomena in polygonal helix thin films. J Appl Phys 98(8):083517. https:\u002F\u002Fdoi.org\u002F10.1063\u002F1.2115092\nMackay TG, Polo JA, Lakhtakia A (2013) Electromagnetic surface waves: a modern perspective. Elsevier, Waltham\nFaryad M, Lakhtakia A (2011) Propagation of surface waves and waveguide modes guided by a dielectric slab inserted in a sculptured nematic thin film. Phys Rev A 83(1):013814. https:\u002F\u002Fdoi.org\u002F10.1103\u002FPhysRevA.83.013814\nKrenn JR, Weeber J-C (2004) Surface plasmon polaritons in metal stripes and wires. Phil Trans R Soc Lond A 362:739–756 https:\u002F\u002Fdoi.org\u002F10.1098\u002Frsta.2003.1344\nSarid D (1981) Long-range surface-plasma waves on very thin metal films. Phys Rev Lett 47:1927–1930 https:\u002F\u002Fdoi.org\u002F10.1103\u002FPhysRevLett.47.1927\nSarid D, Challener WA (2010) Modern introduction to surface plasmons: theory, Mathematica modeling and applications. University Press, Cambridge. https:\u002F\u002Fdoi.org\u002F10.1017\u002FCBO9781139194846\nBerini P (2009) Long-range surface plasmon polaritons. Adv Opt Photon 1(3):484. https:\u002F\u002Fdoi.org\u002F10.1364\u002FAOP.1.000484\nLakhtakia A, Messier R (1997) Sculptured thin films - I. Concepts. Mater Res Innov 1(3):145–148. https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs100190050032\nMessier R, Lakhtakia A (1999) Sculptured thin films — II. Experiments and applications. Mater Res Innov 2:217–222 https:\u002F\u002Fdoi.org\u002F10.1007\u002Fs100190050088\nFuzi Y, Sambles J, Bradberry GW (1991) Long-range surface modes supported by thin films. Phys Rev B 44:5855 https:\u002F\u002Fdoi.org\u002F10.1103\u002FPhysRevB.44.5855\nFaryad M, Lakhtakia A (2010) Surface plasmon–polariton wave propagation guided by a metal slab in a sculptured nematic thin film. J Opt 12(8):085102. https:\u002F\u002Fdoi.org\u002F10.1088\u002F2040-8978\u002F12\u002F8\u002F085102\nPolo JA, Mackay TG, Lakhtakia A (2011) Mapping multiple surface-plasmon-polariton-wave modes at the interface of a metal and a chiral sculptured thin film. J Opt SocAm B 28(11):2656. https:\u002F\u002Fdoi.org\u002F10.1364\u002FJOSAB.28.002656\nQuail JC, Rako JG, Simon HJ (1983) Long-range surface-plasmon modes in silver and aluminum films. OptLett 8:377–379 https:\u002F\u002Fdoi.org\u002F10.1364\u002FOL.8.000377\nCraig AE, Olson GA, Sarid D (1983) Experimental observation of the long-range surface-plasmon polariton. Opt.Lett 8(7):380–382. https:\u002F\u002Fdoi.org\u002F10.1364\u002FOL.8.000380\nDohi H, Kuwamura Y, Fukui M, Tada O (1984) Long-range surface Plasmon Polaritons in metal films bounded by similar-refractive-index materials. J Phys Soc Jpn 53(536):2828–2832 https:\u002F\u002Fdoi.org\u002F10.1143\u002FJPSJ.53.2828\nPulsifer DP, Faryad M, Lakhtakia A (2013) Observation of the Dyakonov-Tamm wave. Phys RevLett 111(538):243902 https:\u002F\u002Fdoi.org\u002F10.1103\u002FPhysRevLett.111.243902\nHodgkinson I, Hong Wu Q, Hazel J (1998) Empirical equations for the principal refractive indices and column angle of obliquely deposited films of tantalum oxide, titanium oxide, and zirconium oxide. Appl Opt 37:2653–2659 https:\u002F\u002Fdoi.org\u002F10.1364\u002FAO.37.002653\nLakhtakia A, Jen Y-J, Lin C-F (2009) Multiple trains of same-color surface plasmonpolaritons guided by the planar interface of a metal and a sculptured nematic thin film. Part III: experimental evidence.J Nanophotonics 3:033506. https:\u002F\u002Fdoi.org\u002F10.1117\u002F1.3249629\nGospodyn J, Sit JC (2006) Characterization of dielectric columnar thin films by variable angle Mueller matrix and spectroscopic ellipsometry. 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