Relevant bibliographies by topics / Sub band

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  1. Journal articles
  2. Dissertations / Theses
  3. Books
  4. Book chapters
  5. Conference papers
  6. Reports

Academic literature on the topic 'Sub band'

Author: Grafiati
Published: 4 June 2021
Last updated: 21 February 2023

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Journal articles on the topic "Sub band"

1

Yu, Guiqiang, Lu Wen, Guoyu Luo, and Yan Wang. "Band structures and topological properties of twisted bilayer MoTe2 and WSe2." Physica Scripta 96, no. 12 (December 1, 2021): 125874. http://dx.doi.org/10.1088/1402-4896/ac4192.

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Abstract We calculate the electronic band structures and topological properties of twisted homobilayer transition metal dichalcogenides(t-TMDs), in particular, bilayer MoTe2 and WSe2 based on a low-energy effective continuum model. We systematically show how the twist angle, vertical electric field and pressure modify the band structures of t-TMDs, often accompanied by topological transitions.We find the variation of topological transitions mainly take place in a limited range of parameters. The electric field can efficiently tune the energy of the topmost second valence band to motify the Chern numbers of the topmost three valance bands. The topological property of the topmost first valance band can be modified by electric field and pressure, but doesn’t depend on twist angle. We show the band gap between the topmost second and third valance bands that both change from non-trivial to trivial closes at κ − -point of the moiré Brillouin zone.
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Wang, Zhi Long, Shi Qin Wang, Nin Yao, and Xing Min Wei. "VUV-Photoluminescence Properties of (Gd, La)2O2CO3: Eu3+." Advanced Materials Research 1052 (October 2014): 203–6. http://dx.doi.org/10.4028/www.scientific.net/amr.1052.203.

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(Gd,La)2-x O2CO3:Eux3+(0.01 ≤x≤0.04) were synthesized via a flux method at 400°C, and their photoluminescence properties under vacuum ultraviolet (VUV) excitation were examined. The excitation spectra showed two bands in the region from 125 nm to 300 nm, the first band centered at 190 nm was ascribed to absorption of related CO32- complex, and the second broad band centered at 246nm and 278nm in Gd2O2CO3:Eu3+ was ascribed to the charge transfer band of O2-→ Eu3+. Series samples exhibited red emission at around 611 nm under vacuum ultraviolet excitation corresponding to the 5D0→ 7F2.transition of Eu3+.
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Kaewjaeng, Siriprapa, Smit Insiripong, Hong Joo Kim, Utumma Maghanemi, Suchart Kothan, S. Ruengsri, and Jakrapong Kaewkhao. "Optical and Luminescence Properties of Pr3+ in Gd2O3-CaO-SiO2-B2O3 Glasses." Key Engineering Materials 675-676 (January 2016): 359–63. http://dx.doi.org/10.4028/www.scientific.net/kem.675-676.359.

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This paper reports on the results concerning optical absorption and luminescence properties of 25Gd2O3-10CaO-10SiO2-(55-x) B2O3-xPr2O3 (where x is 0.0, 0.5, 1.0, 1.5, 2.0 and 2.5 mol %) have been synthesized by melting and quenching process. The locations of the absorption peak observed are investigated for the first time. It is shown that the f-f transitions in the studied glasses are allowed by distortions of Pr3+ ions. Seven absorption bands corresponding to the 3H4 → 3P2, 1I6+3P1, 1D2, 1G4, 3F4, 3F3 and 3F2, respectively absorption bands peaked at 459,483,575,1011,1418,1513 and 1931 nm. The luminescence intensity of Pr3+ doped glass under excited at 459 and 483 nm, the emission band under excited at 459 nm wavelengths emission centered at 542 nm (3P0→3H5), 602 nm (1D2→3H4), 646 nm (3P0→3F2) and 689 nm (1D2→3H5) .The emission bands with 483 nm excitation wavelength, the emission band centered at 532 nm (3P1→3H5), 602 nm (1D2→3H4), 646 nm (3P0→3F2) and 725 nm (3P0→3F4), respectively. The present paper brings out the results pertaining to the studies carried out on different structural and optical absorption in UV-VIS-NIR region are also measured and discussed in term of energy levels, energy band gap and emission spectra of Pr3+ ions doped in Gd2O3-CaO-SiO2-B2O3 glasses.
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He, Ling, Wei Min Sun, Yu Tian Ding, and Yu Hua Wang. "Synthesis and Photoluminescence Properties of the Novel Red Phosphor Gd2MoB2O9: Eu." Advanced Materials Research 311-313 (August 2011): 1327–31. http://dx.doi.org/10.4028/www.scientific.net/amr.311-313.1327.

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A novel phosphor, Gd2MoB2O9:Eu3+ has been synthesized by solid-state reaction and its photoluminescence in UV-VUV range are investigated. A sharp excitation band is observed in the region of 120–135 nm, which is related to the charge-transfer (CT) band of Gd3+. The broad band around 135–160 nm can be assigned to the BO3 host absorption. The broad bands around 248 nm are assigned to the CT band of Eu3+-O2-. The phosphors emit strong red luminescence centered at about 591 nm, 614 nm and 626 nm due to the5D0–7F1 and 5D0–7F2 transitions of Eu3+. The main emission peak under 254 and 147 nm excitations also shows different shifts with increasing Eu3+ concentration. This could be due to the different luminescence sites selected at high doping concentrations of Eu3+. Gd2MoB2O9:Eu3+ shows the pure red emission under both 254 and 147 nm excitations.
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Xia, Xinyi, Nahid Sultan Al-Mamun, Chaker Fares, Aman Haque, Fan Ren, Anna Hassa, Holger von Wenckstern, Marius Grundmann, and S. J. Pearton. "Band Alignment of Al2O3 on α-(AlxGa1-x)2O3." ECS Journal of Solid State Science and Technology 11, no. 2 (February 1, 2022): 025006. http://dx.doi.org/10.1149/2162-8777/ac546f.

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X Ray Photoelectron Spectroscopy was used to measure valence band offsets for Al2O3 deposited by Atomic Layer Deposition on α-(AlxGa1-x)2O3 alloys over a wide range of Al contents, x, from 0.26–0.74, corresponding to a bandgap range from 5.8–7 eV. These alloys were grown by Pulsed Laser Deposition. The band alignments were type I (nested) at x <0.5, with valence band offsets 0.13 eV for x = 0.26 and x = 0.46. At higher Al contents, the band alignment was a staggered alignment, with valence band offsets of − 0.07 eV for x = 0.58 and −0.17 for x = 0.74, ie. negative valence band offsets in both cases. The conduction band offsets are also small at these high Al contents, being only 0.07 eV at x = 0.74. The wide bandgap of the α-(AlxGa1-x)2O3 alloys makes it difficult to find dielectrics with nested band alignments over the entire composition range.
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He, Da Wei, Fang Shen, Xin Li, Peng Zhi Lu, and Yong Sheng Wang. "Luminescence Properties of LnZr(BO3)2:Re (Ln=Ba, Sr; Re=Eu, Ce,Tb)." Key Engineering Materials 368-372 (February 2008): 369–71. http://dx.doi.org/10.4028/www.scientific.net/kem.368-372.369.

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The excitation spectrum of BaZr(BO3)2:Eu3+ is composed of two broad bands. One band in the range from 120 nm to 170 nm is attributed to the borate groups, and the other band at 230 nm is due to the charge-transfer state (CTS) of the Eu3+ ion. The excitation spectrum of BaZr(BO3)2:Tb3+consists of one broad band in the range from 120 nm to 170 nm and the bands peaking at 226 nm, 245 nm and 272 nm respectively. The former is also attributed to the absorption of the BO3 groups. The latter correspond to the 4f8-4f75d transition of Tb3+.Main peak of the host absorption moves about 30 nm to high energy region as Sr2+ replaces Ba2+ partially.
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Смагин, В. П., А. А. Исаева, and Н. С. Еремина. "Фотолюминесценция квантовых точек Zn-=SUB=-1-x-y-=/SUB=-Cu-=SUB=-x-=/SUB=-Eu-=SUB=-y-=/SUB=-S/EuL-=SUB=-3-=/SUB=- в полиакрилатной матрице." Журнал технической физики 128, no. 5 (2020): 651. http://dx.doi.org/10.21883/os.2020.05.49326.326-19.

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Zinc sulfide is one of the most popular luminescent semiconductors of group A(II)B(VI). Doping ZnS quantum dots with Ln3+ ions makes it possible to form nanoscale structures in a semiconductor matrix containing isolated centers of narrow-band luminescence. The introduction of quantum dots into the acrylate matrix further stabilizes the particles and allows them to form their morphology. Nanoscale structures of Zn1-x-yCuxEuyS/EuL3, where L − trifluoroacetate are anions, were synthesized by the method of emerging reagents in situ in the medium of methyl methacrylate (MMA). ZnS doping was performed by simultaneous introduction of soluble precursors of zinc sulfide, as well as copper and europium trifluoroacetates into the acrylate reaction mixture. Polymer optically transparent compositions of PMMA/Zn1-x-yCuxEuyS/EuL3 were obtained by radical polymerization of MMA in the block. The excitation of luminescence of compositions is associated with Interzone electron transitions in ZnS, with a system of levels that form alloying ions in the forbidden zone of ZnS, as well as with their own energy absorption by Eu3+ ions. Broadband luminescence of compositions is caused by intracrystalline defects formed in ZnS during doping. Narrow-band luminescence occurs as a result OF 5D0→7Fj electronic transitions in Eu3+ ions associated with quantum dots, as well as being in the polymer matrix independently of them. The transfer of energy from the donor levels of the semiconductor matrix to the levels of Eu3+ ions, followed by its release in the form of luminescence, was confirmed by the imposition of absorption bands doped with ZnS and excitation bands of luminescence compositions, as well as an increase in the intensity of narrow-band luminescence of Eu3+ ions while reducing the intensity of a wide band of recombination luminescence of doped ZnS. A decrease in the intensity of the ZnS recombination luminescence band with an increase in the concentration of Eu3+ >1.0∙10-3 mol/L ions is also associated with the formation of a layer of complex europium compounds on the particle surface that prevent the passage of exciting radiation to the particle core.
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Omehe, Nnamdi, and Divine Ojuh. "The Electronic Band Structure and Vibrational Properties of Cubic BxIn1-xN Alloy." Applied Mechanics and Materials 446-447 (November 2013): 98–103. http://dx.doi.org/10.4028/www.scientific.net/amm.446-447.98.

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We have performed the electronic and phonon band structures of BxIn1-xN for various concentration of Boron using the pseudopotential method. The electronic band structure calculation was done using the GW approximation while the phonon band structure was done using the density functional perturbation theory. All calculations were done within the frame work of the density functional theory (DFT). From our calculations, the direct band gap for B0.25In0.75N, B0.5In0.5N and B0.75In0.25N were found to be 0.024eV, 2.2 eV and 6.01 eV respectively while the indirect band gap obtained were 0.59 eV, 3.24 eV and 6.9 eV. For the phonon calculations, it was also observed that an increase in the Boron content results in corresponding increase in the frequency of the topmost LO at the zone centre. For B0.25In0.75N, B0.5In0.5N and B0.75In0.25N, the topmost LO obtained were 735 cm-1, 885 cm-1 and 1105 cm-1 respectively. We also saw that as the Boron concentration decreases, the number of optical bands across which the acoustic bands overlap increases.
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Nieken, Rachel, Anna Roche, Fateme Mahdikhanysarvejahany, Takashi Taniguchi, Kenji Watanabe, Michael R. Koehler, David G. Mandrus, John Schaibley, and Brian J. LeRoy. "Direct STM measurements of R-type and H-type twisted MoSe2/WSe2." APL Materials 10, no. 3 (March 1, 2022): 031107. http://dx.doi.org/10.1063/5.0084358.

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When semiconducting transition metal dichalcogenide heterostructures are stacked, the twist angle and lattice mismatch lead to a periodic moiré potential. As the angle between the layers changes, so do the electronic properties. As the angle approaches 0° or 60°, interesting characteristics and properties, such as modulations in the band edges, flat bands, and confinement, are predicted to occur. Here, we report scanning tunneling microscopy and spectroscopy measurements on the bandgaps and band modulations in MoSe2/WSe2 heterostructures with near 0° rotation (R-type) and near 60° rotation (H-type). We find a modulation of the bandgap for both stacking configurations with a larger modulation for R-type than for H-type as predicted by theory. Furthermore, local density of states images show that electrons are localized differently at the valence band and conduction band edges.
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Zeng, Wei, Qi Jun Liu, and Zheng Tang Liu. "Structural, Electronic and Optical Properties of S-Doped Anatase TiO2." Applied Mechanics and Materials 727-728 (January 2015): 79–82. http://dx.doi.org/10.4028/www.scientific.net/amm.727-728.79.

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Structural, electronic and optical properties of S-doped anatase TiO2 have been investigated using the first-principles density-functional theory. The band structure and density of states show that the band gap of anatase TiO2 narrows due to the presence of the S-3p energy level in the top of the valence bands. Compared with the optical absorption edge of the undoped anatase TiO2, the optical absorption edge of S-doped anatase TiO2 shifts to a lower energy, which indicates that S-doped anatase TiO2 can be used for visible-light absorption applications.
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Dissertations / Theses on the topic "Sub band"

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VASCONCELLOS, EDMAR DA COSTA. "SUB-BAND IMAGE CODING." PONTIFÍCIA UNIVERSIDADE CATÓLICA DO RIO DE JANEIRO, 1994. http://www.maxwell.vrac.puc-rio.br/Busca_etds.php?strSecao=resultado&nrSeq=8635@1.

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COORDENAÇÃO DE APERFEIÇOAMENTO DO PESSOAL DE ENSINO SUPERIOR
Este trabalho aborda o problema da compressão de imagens explorando a técnica de codificação por sub-bandas(SBB). Como estrutura básica, usada na primeira parte do trabalho, tem-se a divisão da imagem em 16 sub-bandas buscando replicar os resultados de woods [1]. As componentes das 16 SBB são quantizadas e codificadas, e bits são alocados às SBB usando como critério a minimização do erro médio quadrático. Os quantizadores são projetados segundo uma distribuição Gaussiana Generalizada. Neste processo de codificação, a sub-banda de mais baixa freqüência é codificada com DPCM, enquanto as demais SBB são codificadas por PCM. Como inovação, é proposto o uso do algoritmo de Lempel-Ziv na codificação sem perdas (compactação) das sub-bandas quantizadas. Na compactação são empregados os algoritmos de Huffman e LZW (modificação do LZA). Os resultados das simulações são apresentados em termos da taxa (bits/pixel) versus relação sinal ruído de pico e em termos de analise subjetiva das imagens reconstruídas. Os resultados obtidos indicam um desempenho de compressão superior quanto o algoritmo de Huffman é usado, comparado com o algoritmo LZW. A melhoria de desempenho, na técnica de decomposição em sub-bandas, observada com o algoritmo de Huffman foi superior (2dB acima). Todavia, tendo em vista as vantagens da universalidade do algoritmo de Lempel-Ziv, deve-se continuar a investigar o seu desempenho implementado de forma diferente do explorado neste trabalho.
This work focus on the problem of image compression, with exploring the techniques of subband coding. The basic structure, used in the sirst part of this tesis, encompass the uniform decomposition of the image into 16 subbands. This procedure aims at reproducing the reults of Woods [1]. The component of the 16 subbands are quatized and coded and bits are optimally allocated among the subbands to minimize the mean-squared error. The quantizers desingned match the Generelized Gaussian Distribuition, which model the subband components. In the coding process, the lowest subband is DPCM coded while the higher subbands are coded with PCM. As an innovation, it is proposed the use of the algorithm LZW for coding without error (compaction) the quantized subbands. In the compactation process, the Huffamn and LZW algorithms are used. The simulation results are presented in terms of rate (bits/pel) versus peak signal-to-noise and subjective quality. The performance of the subband decomposition tecnique obtained with the Huffamn´s algorithm is about 2dB better than that obtained with the LZW. The universality of the Lempel-Ziv algorithm is, however, an advantage that leads us to think that further investigation should still be pursued.
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Simoncelli, Eero Peter. "Orthogonal sub-band image transforms." Thesis, Massachusetts Institute of Technology, 1988. http://hdl.handle.net/1721.1/14758.

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RILA, LUCIANO. "SUB-BAND CODING OF IMAGES USING INTER-BAND VECTOR QUANTIZATION." PONTIFÍCIA UNIVERSIDADE CATÓLICA DO RIO DE JANEIRO, 1993. http://www.maxwell.vrac.puc-rio.br/Busca_etds.php?strSecao=resultado&nrSeq=8746@1.

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CONSELHO NACIONAL DE DESENVOLVIMENTO CIENTÍFICO E TECNOLÓGICO
Neste trabalho são examinados métodos de codificação de imagens em sub-bandas utilizando quantização vetorial inter-bandas para faixas abaixo de 1 bit/pixel. O espectro de freqüências da imagem é decomposto em 16 sub-bandas uniformes através de um banco de filtros espelhados em quadratura bi-dimensionais. As amostras dos sinais das 16 sub-bandas são usadas para compor um vetor de 16 componentes que, posteriormente, é codificado por um esquema de quantização vetorial (QV). Com o objetivo de reduzir a complexidade e o espaço de memória, são investigadas duas estruturas de quantização vetorial. Uma delas utiliza QV particionada, com o objetivo não só de reduzir a complexidade, como também de explorar as propriedades espectrais. A outra realiza a quantização vetorial direta, enquanto a complexidade é reduzida significativamente. Resultados de simulações são apresentados para as taxas de 0,50 bit/pixel, 0,63 bit/pixel e 0,75 bit/pixel. Uma análise comparativa mostra que o desempenho dos dois esquemas é comparável ao que utiliza quantização vetorial direta, enquanto a complexidade é reduzida significativamente. Resultados de simulações mostram ainda que, a taxas abaixo de 1 bit/pixel, não é recomendável o uso de QV inter-bandas particionada com alocação de bits adaptativa, nem de QV inter-bandas multi-estágios com busca em árvore. A técnica QV inter-bandas quando a sub-banda dominante é codificada separadamente através de um quantizador vetorial intra-banda. Considera-se a decomposição do espectro de freqüências em 16 sub-bandas uniformes e em 13 sub-bandas. Para a decomposição em 16 sub-bandas, esse esquema apresenta desempenho comparável à QV inter-bandas direta e complexidade equivalente à QV inter-bandas multi- estágios.
In this thesis sub-band coding of images using inter-band vector quantization is examined at rates below 1 bit/pixel. The image spectrum is decomposed into 16 uniform bands using 2-D separable quadrature mirror filters. These 16 bands are used to create 16-dimension vectores, which are coded using vector quantization (VQ). In order to reduce the computational complexity and the storage requirements, two vector quantization structures are considered. One approach is to split the vectors not only to reduce complexity but also to exploit spectral properties of the data image. In the order approach the vector quantization is done in multiple stages. Simulation results are presented at rates of 0,50 bit/pixel, 0,63 bit/pixel and 0,75 bit/pixel. A comparative analysis shows that the performance of the two systems is comparable to the basic coding structure, while the complexity is significantly reduced. Simulation results also show that split VQ with adaptive bit allocation and multi-stage VQ with tree search are not recommended at these rates. The best trade-off between complexity and performance is achieved with the inter-band multi-stage VQ scheme using the sequential search procedure. At last, the use of inter- band VQ is examined when the dominant sub-band is separately coded using intra-band VQ. When the image spectrum is decomposed into 16 bands, this scheme has a performance comparable to the basic coding structure while the complexity and storage reduction is equivalent to the inter-band multi-stage VQ technique.
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Bhuvanendran, Nilesh. "SUB-OPTIMAL ULTRA-WIDE BAND RECEIVERS." Master's thesis, University of Central Florida, 2004. http://digital.library.ucf.edu/cdm/ref/collection/ETD/id/4469.

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Ultra-wide Band (UWB) has sparked a lot of interest lately from the industry and academia. The growing capacity of the wireless industry is requires a new communication system that satisfies the high data rate which does not interfere with existing RF systems. UWB promises to be this new technology. UWB also promises low power, low cost and fexibility. The UWB Channel opens up a huge new wireless channel with Giga Hertz Capacities as well as the highest spatial capacities measured in bits per hertz per square meter. When properly implemented UWB channel can share spectrum with traditional radio systems without causing harmful interference. In this thesis we studied and compared several reduced complexity sub-optimal Ultra-Wide Band receivers. These receivers include auto correlation receiver, the square value detector and the absolute value detector are studied. We consider OOK and PPM modulation schemes. We examine these schemes and the receivers on Gaussian and UWB indoor channels. We compare the performance with optimal receivers. A transmitter receiver system using 0.1us pulses implemented using existing hardware. A packet consisting of 24 bits were transmitted and the received signal could be verified in real time using a vector signal analyzer. The results show sub-optimal receivers provide a better trade off between robust, complexity and performance.
M.S.
Department of Electrical and Computer Engineering
Engineering and Computer Science
Electrical and Computer Engineering
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Romano, Pasquale. "Vector quantization for spatiotemporal sub-band coding." Thesis, Massachusetts Institute of Technology, 1989. http://hdl.handle.net/1721.1/69708.

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Song, Sewoong 1954. "Structural sub-band decomposition for adaptive filters." Thesis, The University of Arizona, 1990. http://hdl.handle.net/10150/291831.

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The theory of structural sub-band decomposition of an FIR filters is extended to adaptive filters. It is shown that this sub-band decomposition is equivalent to the transform of input data by orthogonal matrices, of which the Walsh-Hadamard Transform (WHT) is a special case. Thus, the proposed method is a generalization of the transform domain adaptive filtering (TDAF) using WHT, which is already known to enhance the convergence speed of adaptive filters. Furthermore, our method yields one possible hardware implementation of the fast WHT. The convergence behavior of the proposed sub-band adaptive filters is simulated using the Least Mean Squares (LMS) and Recursive Least Squares (RLS) algorithms. The results show the faster convergence speed of the proposed adaptive filters compared to conventional adaptive filters.
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Punya, Atchara. "Quasiparticle self-consistent GW band structures of III-N, II-IV-N2 semiconductors and band offsets." Case Western Reserve University School of Graduate Studies / OhioLINK, 2014. http://rave.ohiolink.edu/etdc/view?acc_num=case1380888317.

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Lefebvre, Pierre D. "Adaptive multiple sub-band common mode RFI suppression." Thesis, National Library of Canada = Bibliothèque nationale du Canada, 2001. http://www.collectionscanada.ca/obj/s4/f2/dsk3/ftp04/MQ58475.pdf.

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Zemouri, Rachid. "Data compression of speech using sub-band coding." Thesis, University of Newcastle Upon Tyne, 1991. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.316094.

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Fischer, Stefan [Verfasser], and Eicke [Akademischer Betreuer] Weber. "Upconversion of sub-band-gap photons for silicon solar cells = Hochkonversion von sub-band-gap Photonen zur Effizienzsteigerung von Silicium-Solarzellen." Freiburg : Universität, 2014. http://d-nb.info/1123480982/34.

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Books on the topic "Sub band"

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Sauer, Ken. Sub-band/transform compression of video sequences: Final report. Notre Dame, Ind: Dept. of Electrical Engineering, University of Notre Dame, 1992.

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Sauer, Ken. Sub-band/transform compression of video sequences: Final report. Notre Dame, Ind: Dept. of Electrical Engineering, University of Notre Dame, 1992.

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McGirr, J. T. G.722 sub-band ADPCM coding algorithm with statistical framing synchronisation. [s.l: The Author], 1997.

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Agency, Radiocommunications. MPT 1347 radio interface specification: For commercial trunked networks operating in Band III, sub-bands 1 and 2. London: RA, 1991.

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Williamson, Charles A. Studies on the rapid and quantitative sub-band separation and characterization of creatine kinase for in vitro diagnostic use. Sudbury, Ont: Laurentian University, 1987.

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Petroni, Giulio. Sgarbo a Sgarbi e la sua band. [Roma?]: Dalia, 2002.

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Lensink, Robert. Structural adjustment in sub-Saharan Africa. London: Longman, 1996.

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Gelbard, E. Measuring financial development in Sub-Saharan Africa. [Washington, D.C.]: International Monetary Fund, African Department, 1999.

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Sirleaf, Ellen Johnson. The outlook for commercial bank lending to Sub-Saharan Africa. Washington (1818 H St., NW, Washington 20433): International Economics Dept., World Bank, 1991.

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Covarrubias, Alvaro J. Lending for electric power in Sub-Saharan Africa. Washington, D.C: World Bank, 1996.

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Book chapters on the topic "Sub band"

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Moreau, Nicolas. "Sub-band Transform Coding." In Tools for Signal Compression, 37–52. Hoboken, NJ USA: John Wiley & Sons, Inc., 2013. http://dx.doi.org/10.1002/9781118616611.ch3.

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Dai, Y. D., M. J. Hu, L. L. Guo, M. H. Cao, and H. X. Liu. "The Band Structure Analysis of the Hybrid Compound (C4H9NH3)2Gel4." In Solid State Phenomena, 51–54. Stafa: Trans Tech Publications Ltd., 2006. http://dx.doi.org/10.4028/3-908451-18-3.51.

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Lu, Tie Cheng, Xue Jun Wang, Bing Xun Cheng, Qiang Hu, and Shao Bo Dun. "Novel Visible-Band Transparent Ceramic Laser Material Mn:MgAl2O4." In Key Engineering Materials, 1229–32. Stafa: Trans Tech Publications Ltd., 2007. http://dx.doi.org/10.4028/0-87849-410-3.1229.

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Cho, Jae-Won, Ha-Joong Park, Young Huh, Hyun-Yeol Chung, and Ho-Youl Jung. "Echo Watermarking in Sub-band Domain." In Digital Watermarking, 447–55. Berlin, Heidelberg: Springer Berlin Heidelberg, 2004. http://dx.doi.org/10.1007/978-3-540-24624-4_35.

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Malu, Siddharth Savyasachi, Abhirup Datta, and Peter Timbie. "Fizeau Interferometers: Extracting Sub-band Information." In Computers and Devices for Communication, 359–62. Singapore: Springer Singapore, 2021. http://dx.doi.org/10.1007/978-981-15-8366-7_52.

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Kim, Yu Jin, Seong Jin Hwang, and Hyung Sun Kim. "Microwave Dielectric Properties of LTCC Materials Consisting of BaO-TiO2-SiO2-Al2O3 Glass - BaNd2Ti5O14 Ceramic Composites." In Materials Science Forum, 506–9. Stafa: Trans Tech Publications Ltd., 2005. http://dx.doi.org/10.4028/0-87849-966-0.506.

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Singh, Abhishek, and Narendra Ahuja. "Super-Resolution Using Sub-Band Self-Similarity." In Computer Vision -- ACCV 2014, 552–68. Cham: Springer International Publishing, 2015. http://dx.doi.org/10.1007/978-3-319-16808-1_37.

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Hossen, Abdulnasir, and Ulrich Heute. "General Sub-Band DCT: Fast Approximate Adaptive Algorithm." In Signal Analysis and Prediction, 47–56. Boston, MA: Birkhäuser Boston, 1998. http://dx.doi.org/10.1007/978-1-4612-1768-8_3.

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Stein, Dalton, He-Wen-Xuan Li, and David Chelidze. "Sub-Band Decomposition Based-Linear Normal Mode Identification." In Topics in Modal Analysis & Parameter Identification, Volume 8, 141–44. Cham: Springer International Publishing, 2012. http://dx.doi.org/10.1007/978-3-031-05445-7_16.

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Hou, Limin, Juanmin Xie, and Su Xie. "Sub-band Main Peak Frequency Application for Speaker Identification." In Biometric Recognition, 180–85. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-25449-9_23.

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Conference papers on the topic "Sub band"

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Nasersharif, Babak, and Ahmad Akbari. "Sub-band weighted projection measure for robust sub-band speech recognition." In Interspeech 2005. ISCA: ISCA, 2005. http://dx.doi.org/10.21437/interspeech.2005-225.

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Kuroda, T., and N. Mori. "Resonant Enhancement of Band-to-band Tuneling in In-plane MoS2/WS2 Heterojunctions." In 2017 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2017. http://dx.doi.org/10.7567/ssdm.2017.j-3-05.

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Iida, R., S. H. Kim, M. Yokoyama, N. Taoka, S. H. Lee, M. Takenaka, and S. Takagi. "Device characteristics of planar-type In0.53Ga0.47As channel band-to-band tunneling MOSFETs." In 2011 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2011. http://dx.doi.org/10.7567/ssdm.2011.d-4-1.

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Nair, Jinesh P., Debarati Sen, Sujit Jos, and Arun Naniyat. "Sub-sampled OFDM based sub-band ultra-wideband system." In 2012 IEEE Wireless Communications and Networking Conference (WCNC). IEEE, 2012. http://dx.doi.org/10.1109/wcnc.2012.6214416.

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Pincemin, E., Y. Jaouen, G. Froc, A. Poudoullec, N. Nicolas, M. Song, P. Gravey, M. Van der Keur, J. Karaki, and M. Morvan. "Multi-band OFDM Transmission with Sub-band Optical Switching." In 39th European Conference and Exhibition on Optical Communication (ECOC 2013). Institution of Engineering and Technology, 2013. http://dx.doi.org/10.1049/cp.2013.1527.

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Kaddour, Abdul-Sattar, and Stavros V. Georgakopoulos. "A Dual-Band Transmitarray Antenna with Independent Beam Control at Ka Band." In 2022 IEEE Texas Symposium on Wireless and Microwave Circuits and Systems (WMCS). IEEE, 2022. http://dx.doi.org/10.1109/wmcs55582.2022.9866157.

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Yamada, Y., and Y. Kanemitsu. "Phonon-Assisted Band-to-Band Luminescence and Carrier Recombination Processes in SrTiO3." In 2011 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2011. http://dx.doi.org/10.7567/ssdm.2011.p-9-4.

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Smets, Q., A. S. Verhulst, R. Rooyackers, C. Merckling, D. Lin, E. Simoen, A. Alian, et al. "In0.53Ga0.47As Diodes for Band-to-Band Tunneling Calibration and n- and p-LineTFET performance prediction." In 2013 International Conference on Solid State Devices and Materials. The Japan Society of Applied Physics, 2013. http://dx.doi.org/10.7567/ssdm.2013.d-7-4.

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Molla, Mahlet, and Emmanouil Kioupakis. "Thermodynamics and Band Structure of ScxAl1-xN." In 2022 Compound Semiconductor Week (CSW). IEEE, 2022. http://dx.doi.org/10.1109/csw55288.2022.9930119.

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Woo Sang Lee, Kyung Soon Park, Byoung Moo Lee, Young Joong Yoon, Joon-ho So, and Woo Young Song. "X-band TM/sub 01/-TE/sub 11/ mode converter." In IEEE Antennas and Propagation Society Symposium, 2004. IEEE, 2004. http://dx.doi.org/10.1109/aps.2004.1330481.

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Reports on the topic "Sub band"

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David A. Smith. A Multiple-Channel Sub-Band Transient Detection System. Office of Scientific and Technical Information (OSTI), November 1998. http://dx.doi.org/10.2172/3059.

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Sullivan, G. A search for. nu. sub. mu. yields. nu. sub e oscillations in a wide band neutrino beam. Office of Scientific and Technical Information (OSTI), January 1990. http://dx.doi.org/10.2172/7165939.

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Zollner, S., C. M. Herzinger, J. A. Woollam, S. S. Iyer, A. P. Powell, and K. Eberl. Spectroscopic ellipsometry and band structure of Si{sub 1{minus}y}C{sub y} alloys grown pseudomorphically on Si (001). Office of Scientific and Technical Information (OSTI), October 1995. http://dx.doi.org/10.2172/106645.

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Rock, Janice C., Tracy D. Hudson, Brandon Wolfson, Daniel Lawrence, Brandon Pillans, Andrew R. Brown, Louis A. Coryell, and Richard A. Milburn. Design, Fabrication, and Evaluation of a MEMS-Based, Ka-Band, 16-Element Sub-Array. Fort Belvoir, VA: Defense Technical Information Center, November 2009. http://dx.doi.org/10.21236/ada508549.

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Pines, Mark, Arieh Bar, David A. Carrino, Arnold I. Caplan, and James A. Dennis. Extracellular Matrix Molecules of the Eggshell as Related to Eggshell Quality. United States Department of Agriculture, 1997. http://dx.doi.org/10.32747/1997.7575270.bard.

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Abstract:
The extracellular matrix of the mineralizing eggshell contains molecules hypothesized to be regulators biomineralization. To study eggshell matrix molecules, a bank of monoclonal antibodies was generated that bound demineralized eggshell matrix or localized to oviduct epithelium. Immunofluorescence staining revealed several staining patterns for antibodies that recognized secretory cells: staining for a majority of columnar lining cells, staining for a minor sub-set of columnar lining cells, intensified staining within epithelial crypts, and staining of the entire tubular gland. Western blotting with the antibody Epi2 on eggshell matrix showed binding to molecules with the apparent molecular weight of eggshell matrix dermatan sulfate proteoglycan (eggshell DSPG) (Carrino, et al., 1997). Immunoblots of cyanogen bromide-cleaved eggshell DSPG revealed broad band of reactivity that shifted to 25 kDa after chondroitinase digestion; indicating that the Epi2 binding site is located on a fragment which contains dermatan sulfate side chains. Immunogold labeling showed that Epi2 binds to secretory vesicles within the non-ciliated cells of the columnar epithelium, while the antibodies Tg1 and Tg2 bind to secretory vesicles of tubular gland cells. Immunogold labeling of demineralized shell matrix showed binding of Epi2, Tg1, and Tg2 to the matrix of the palisades layer, and showed little reactivity to other regions of the shell matrix. Quantification of the immunogold particles within the eggshell matrix revealed that antibodies Epi2 and Tg1 bind all calcified regions equally while antibody Tg2 has a greater affinity for the baseplate region of the calcium reserve assembly.
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Ryasnyanskiy, Aleksandr. Narrow band laser source for efficient 3He polarization. Office of Scientific and Technical Information (OSTI), February 2018. http://dx.doi.org/10.2172/1434619.

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Lauritsen, T., T. L. Khoo, and R. G. Henry. Spins of superdeformed band in {sup 192}Hg. Office of Scientific and Technical Information (OSTI), August 1995. http://dx.doi.org/10.2172/166302.

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Brinkman, M. J. Decay of the {sup 194}Pb superdeformed band. Office of Scientific and Technical Information (OSTI), December 1994. http://dx.doi.org/10.2172/82246.

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Lindroos, M., A. Bansil, K. Gofron, J. C. Campuzano, H. Ding, R. Liu, and B. W. Veal. Signature of the CuO{sub 2} plane related bands in YBa{sub 2}Cu{sub 3}O{sub 6.9} as seen by angle-resolved photoemission. Office of Scientific and Technical Information (OSTI), September 1992. http://dx.doi.org/10.2172/10158490.

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Ahmad, I., D. Blumenthal, and M. P. Carpenter. Lifetimes of an excited superdeformed band in {sup 192}Hg. Office of Scientific and Technical Information (OSTI), August 1995. http://dx.doi.org/10.2172/166318.

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