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deacetylation,的相关文献在2001年到2022年内共计194篇,主要集中在数学、物理学、化学 等领域,其中期刊论文194篇、相关期刊6种,包括中国地产市场、中国科学、世界胃肠病学杂志:英文版等; deacetylation,的相关文献由273位作者贡献,包括WANG、ZHANG、LI等。

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deacetylation,

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    • Pan Cao; Qian Chen; Chun-Xia Shi; Lu-Wen Wang; Zuo-Jiong Gong
    • 摘要: BACKGROUND The occurrence and development of acute liver failure(ALF)is closely related to a series of inflammatory reactions,such as the production of reactive oxygen species(ROS).Hypoxia inducible factor 1α(HIF-1α)is a key factor that regulates oxygen homeostasis and redox,and the stability of HIF-1αis related to the ROS level regulated by Sirtuin(Sirt)family.The activation of Sirt1 will lead to a powerful antioxidant defense system and therapeutic effects in liver disease.However,little is known about the relationship between HIF-1αand Sirt1 in the process of ALF and the molecular mechanism.AIM To investigate whether HIF-1αmay be a target of Sirt1 deacetylation and what the effects on ALF are.METHODS Mice were administrated lipopolysaccharide(LPS)/D-gal and exposed to hypoxic conditions as animal model,and resveratrol was used as an activator of Sirt1.The cellular model was established with L02 cells stimulated by LPS.N-acetyl-Lcysteine was used to remove ROS,and the expression of Sirt1 was inhibited by nicotinamide.Western blotting was used to detect Sirt1 and HIF-1αactivity and related protein expression.The possible signaling pathways involved were analyzed by immunofluorescent staining,co-immunoprecipitation,dihydroethidium staining,and Western blotting.RESULTS Compared with mice stimulated with LPS alone,the expression of Sirt1 decreased,the level of HIF-1αacetylation increased in hypoxic mice,and the levels of carbonic anhydrase 9 and Bcl-2-adenovirus E1B interacting protein 3 increased significantly,which was regulated by HIF-1α,indicating an increase of HIF-1αactivity.Under hypoxia,the down-regulation of Sirt1 activated and acetylated HIF-1αin L02 cells.The inhibition of Sirt1 significantly aggravated this effect and the massive production of ROS.The regulation of ROS was partly through peroxisome proliferatoractivated receptor alpha or AMP-activated protein kinase.Resveratrol,a Sirt1 activator,effectively relieved ALF aggravated by hypoxia,the production of ROS,and cell apoptosis.It also induced the deacetylation of HIF-1αand inhibited the activity of HIF-1α.CONCLUSION Sirt1 may have a protective effect on ALF by inducing HIF-1α deacetylation to reduce ROS.
    • Malinda Syifa Yusharani; Stenley; Harmami; Ita Ulfin; Suprapto Suprapto; Yatim Lailun Ni’mah
    • 摘要: Water-Soluble Chitosan(WSC)has been sucessfuly synthesized from squid pens waste.The synthesis of chitosan from chitin was carried out by optimization of deacetylation temperature and time.Chitin was obtained from squid pens waste by demineralization and deproteinization process.HCl 7%was used for demineralization and NaOH 10%at 60°C was applied for deproteinization process.Deacetylation reaction was carried out at varied temperatures i.e.,60°C,70°C,80°C,90°C and 100°C in NaOH 50%solution for 10 hours.Deacetylation reaction time were varied for 2 hours,4 hours,6 hours,8 hours,and 10 hours.The crude chitosan obtained then reacted with H2O230%to depolymerize.The synthesis product obtained then characterized by FTIR.The result of squid chitin yield was 33.9%.The optimum temperature and time of chitosan deacetylation process were 90°C for 8 hours as indicated by the value of deacetylation degree(DD)that equal to 83.94%at optimum temperature and 82.22%at optimum reaction time.The percentage of WSC yield at optimum temperature(90°C)and optimum time(8 hours)were 27.59%and 23.16%,respectively.WSC solubility test was done in water and HCl 0,1N.The solubility of 2.8325 mg/mL and 0.8125 mg/mL were obtained in acid medium and water medium,respectively.
    • Sunday Anthony Akolo; Abulsalami Sanni Kovo
    • 摘要: Chitosan synthesized locally with a degree of deacetylation 71% and chitosan with a degree of deacetylation 68% from Sigma Aldrich were used to investigate adsorption of Cu2+ ion in aqueous solution. The results obtained from equilibrium isotherm adsorption studies of Cu2+ ion were an-alyzed in five adsorption models namely: Langmuir, Freundlich, Temkin, Elovich and Dubin- Ra-dushkevich. The isotherms equation was indicated to be well fitted to Langmuir, Freundlich, Temkin and Elovich under the concentration range studied. The kinetic parameters were evaluated utilizing the pseudo-first-order and pseudo-second-order equations, and the adsorption kinetics followed the mechanism of the pseudo-second-order equation for all systems studied, evidencing chemical sorption as the rate-limiting step of adsorption mechanism and not involving a mass transfer in solution. The FTIR studies revealed that the greater sorption of heavy metal was attributed to the large number of primary amine groups available on the surfaces of the chitosan and the abundant carboxyl groups on chitosan.
    • Domenico Mastrangelo; Cosimo Loré; Giovanni Grasso
    • 摘要: The aim of the present review is to give new insights into the pathogenesis of retinoblastoma, by applying the principles of Epigenetics to the analysis of clinical, epidemiological, and biological data concerning the disease. As an emerging new scientific approach linking the genome to the environment, Epigenetics, as applied to the interpretation of clinical, epidemiological and biological data in retinoblastoma, can not only explain the inconsistencies of the mutational (“two hit”) model, but also open new outstanding scenarios in the fields of diagnosis, treatment and prevention of this eye tumour. This review is both a collection of literature data arguing against the role of the mutational (“two hit”) model in the genesis of retinoblastoma, and a documented evaluation of how the Epigenetic, rather than the genetic model fit the variegated phenotypic expression of the disease. The epigenetic model in the genesis of retinoblastoma, proposed herein, emphasizes the role of environment and the interaction of the environment with the genome, in generating reti-noblastoma in young children. Environmental toxicants, including radiations, wrong diets, and infectious diseases, among others, all play a major role in conditioning the degree of DNA methylation in embryos and foetuses during pregnancy, thus leading to stable, functional alterations of the genome, which, on the other hand, can be also transmit-ted from generation to generation, thus mimicking a hereditary disease. An accurate analysis of the currently available literature on both retinoblastoma and Epigenetics, coupled with the knowledge of the variegated phenotypic expression of the disease, can easily lead to the conclusion that retinoblastoma is an epigenetic, rather than a genetic disease.
    • CHEN; Ya; nli
    • 摘要: [1]Padilla. P, Hatfield, W. E., Correlation between π-orbital overlap and conductivity in bis-phthalocyaninato lanthanides, Inorg. Chim. Acta, 1991,185:131.[2]Passard, M., Blanc, J. P., Malaysson, C., Gaseous oxidation and compensation reduction of lutetium bis-phthalocyanine and lutetium phthalo-naphthalocyanine films, Thin Solid Films, 1995, 271: 8,[3]Besbes. S., Plichon, V., Simon, J. et al., Electromism of octaalkoxymethyl-substituted lutetium diphthalocyanine, J. Electroanal. Chem., 1987, 237:61.[4]Petty. M., Lovett, D. R., O'Connor, J. M., Electrochromism in ytterbium bisphthalocyanine-(steafic acid or cadmium stearate)films deposited by the Langmuir-Blodgett technique, Thin Solid Films, 1989, 179: 387.[5]Souto, J.. Aroca, R.. DeSaja, J. A., Gas adsorption and electrical conductivity of Langmuir-Blodgett films of terbium bisphthalocyanine, J. Phys. Chem., 1994, 98: 8998.[6]Rroca, R.. Bolourchi, H., Battisti, D. et al., Gas adsorption and electrical properties of two Langmuir-Blodgett layers of cerium bisphthalocyanine, Langmuir, 1993, 9: 3138.[7]Konami, H., Hatano, M., Kobayashi, N., Redox potentials of a series of lanthanide-bisphthalocyanine sandwich complexes, Chem. Phys. Lett.. 1990, 165: 397.[8]Koike. N.. Uekusa, H., Ohashi, Y., Relationship between the skew angle and interplanar distance in four bis (phthalocyaninato) lanthanide (Ⅲ) tetrabutyl-ammonium salts ([Nbu"4][Ln"Pc2]; Ln = Nd, Gd, Ho, Lu), Inorg. Chem., 1996, 35:5798.[9]Dennis. K. P. N., Jiang, J., Sandwich-type heteroleptic phthalocyaninato and porphyrinato metal complexes, Chem. Soc. Rev.. 1997, 26: 433.[10]Jiang. J., Liu, W., Poon, Ka-Wo. et al., Synthesis, spectroscopic, and electrochemical properties of rare earth double-deckers with tetra(teft-butyl) 2,3-naphthalocyaninato ligands, Eur. J, Inorg. Chem., 2000: 205.[11]Jiang, J.. Llew, R., Dennis, P. et al., Raman spectroscopic characteristics of phthalocyanine and naphthalocyanine in sandwich-type (na)phthalocyaninato and porphyrinato rare earth complexes, Polyhedron, 2000, 19:1381.[12]Jiang. J.. Kasuga, K., Dennis, P. et al., Supramolecular Photosensitive and Electroactive Materials, New York: Academic Press. 2001. 113-210.[13]Van Nostrum. C. F., Nolte, R. J. M., Functional supramolecular material: self-assembly of phthalocyanines and porphyraszines. Chem. Commun., 1996: 2385.[14]Liu. Y., Shigehara, K., Yamada, A., Purification of lutetium diphthalocyanine and electrochromism of its Langmuir-Blodgett films, Thin Solid Films, 1989, 179: 303.[15]Liu. Y.. Shigehara, K., Hara, M. et al., Electrochemistry and electrochromic behavior of Langmuir-Blodgett films of octakis-substituted rare-earth metal diphthalocyanines, J. Am. Chem. Soc., 1991,113: 440.[16]Jones, R., Hunter, R. A., Davidson, K., Ordered Langmuir-Blodgett films of a substituted lutetium bisphthalocyanine, Thin Solid Films,1994, 250: 249.[17]Jones, R., Krier, A., Davidosn, K., Structure electrical conductivity and electrochromism in thin film of substituted and unsubstituted lanthanide bisphthalocyanines, Thin Solid Films, 1997, 298: 228.[18]Qian, D. -J., Liu, H. -G., Jiang, J., Monolayers and Langmuir-Blodgett films of (phthalocyaninato)(tetra-4-pyridylporphyrinato) cerium double-decker heteto complex, Colloids and Surfaces A, 2000,163:191.[19]Honig, E. P., Hengst, J. H. T., Engelsen, D. D., Langmuir-Blodgett deposition ratios, J. Colloid Interface Sci., 1973, 45:92.[20]Smolenyak, P., Peterson, R., Nesesny, K. et al., Highly ordered thin films of octasubstituted phthalocyanines, J. Am. Chem.Soc., 1999, 121: 8628.[21]Kasha, M., Rawls, H. R., E1-Bayoumi, M. A., The excition model in molecular spectroscopy, Pure Appl. Chem., 1965, 11: 371.[22]Fujiki, M., Tabei, H., Kurihara, T., Self-assembling features of soluble nickel phthalocyanines, J. Phys. Chem., 1988, 92:1281.[23]Osburn, E. J., Chau, L. -K., Chen, S. -Y. et al., Novel amphiphilic phthalocyanines: Formation of Langmuir-Blodgett and cast thin films, Langmuir, 1996, 12: 4784.[24]Yoneyama, M., Sugi, M., Saito, M. et al., Photoelectric properties of copper phthalocyanine Langmuir-Blodgett film, Jpn. J. Appl. Phys., 1986, 25: 961.[25]
    • ZHENG; Jian
    • 摘要: [1]Braginskii,S.I.,Transport processes in a plasma,in Reviews of Plasma Physics,Vol.1,New York:Consultants Bureau,1965,205-311.[2]Ono,M.,Kulsrud,R.M.,Frequency and damping of ion acoustic waves,Phys.Fluids,1975,18(10):1287-1293.[3]Randall,C.J.,Effect of ion collisionality on ion-acoustic waves,Phys.Fluids,1982,25(12):2231-2233.[4]Tracy,M.D.,Williams,E.A.,Estabrook,K.G.et al.,Eigenvalue solution for the ion-collisional effects on ion-acoustic and entropy waves,Phys.Fluids,1993,B5(5):1430.[5]Bell,A.R.,Electron energy transport in ion waves and its relevance to laser produced plasmas,Phys.Fluids,1983,26(1):279-284.[6]Epperlein,E.M.,Short,R.W.,Simon,A.,Damping of ion-acoustic waves in the presence of electron-ion collisions,Phys.Rev.Lett.,1992,69(12):1765-1768.[7]Epperlein,E.M.,Effect of electron collisions on ion-acoustic waves and heat flow,Phys.Plasmas,1994,1(1):109-115.[8]Bychenkov,V.Y.,Myatt,J.,Rozmus,W.et al.,Quasihydrodynamic description of ion acoustic waves in a collisional plasmas,Phys.Plasmas,1994,1(8):2419-2429.[9]Bychenkov,V.Y.,Myatt,J.,Rozmus,W.et al.,Ion acoustic waves in plasmas with collisional electrons,Phys.Rev.E,1994,50(6):5134-5137.[10]Bychenkov,V.Y.,Rozmus,W.,Tikhonchuk,V.T.et al.,Nonlocal electron transport in a plasma,Phys.Rev.Lett.,1995,75(24):4405-4408.[11]Zhang,Y.Q.et al.,Density fluctuation spectra of a collision-dominated plasma measured by light scattering,Phys.Rev.Lett.,1989,62(16):1848-1851.[12]Hinton,F.L.,Collisional transport in plasma,in Handbook of Plasma Physics,Vol.1,Amsterdam:North-Holland,1983,147-199.[13]Zheng Jian,Yu Changxuan,A numerical approach to the frequencies and damping rates of ion-acoustic waves in ion-collisional plasmas,Chin.Phys.Lett.,1999,16(12):905-907.[14]Hammett,G.W.,Perkins,F.,Fluid moment models for Landau damping with application to the ion-temperature-gradient instability,Phys.Rev.Lett.,1990,64(25):3019-3022.
    • GUO; Maozheng
    • 摘要: [1]Martin Schecher,The Fucik spectrum,Indiana University Mathematics Journal,1994,43(4):1139-1157.[2]Dancer,E.N.,Remarks on jumping nonlinearities,in Topics in Nonlinear Analysis (eds.Escher,Simonett),Basel:Birkhauser,1999,101-116.[3]Dancer,E.N.,Du Yihong,Existence of changing sign solutions for semilinear problems with jumping nonlinearities at zero,Proceedings of the Royal Society of Edinburgh,1994,124A:1165-1176.[4]Dancer,E.N.,Du Yihong,Multiple solutions of some semilinear elliptic equations via generalized conley index,Journal of Mathematical Analysis and Applications,1995,189:848-871.[5]Li Shujie,Zhang Zhitao,Sign-changing solutions and multiple solutions theorems for semilinear elliptic boundary value problems with jumping nonlinearities,Acta Mathematica Sinica,2000,16(1):113-122.[6]Chang Kung-ching,Li Shujie,Liu Jiaquan,Remarks on multiple solutions for asymptotically linear elliptic boundary value problems.Topological methods for Nonlinear Analysis,Journal of the Juliusz Schauder Center,1994,3:179-187.[7]Alfonso Castro,Jorge Cossio,Multiple solutions for a nonlinear Dirichlet problem,SIAM J.Math.Anal.,1994,25(6):1554-1561.[8]Alfonso Castro,Jorge Cossio,John M.Neuberger,A sign-changing solution for a superlinear Dirichlet problem,Rocky Mountain J.M.,1997,27:1041-1053.[9]Alfonso Castro,Jorge Cossio,John M.Neuberger,A minimax principle,index of the critical point,and existence of sign-changing solutions to Elliptic boundary value problems,E.J.Diff.Eqn.,1998 (2):1-18.[10]Thomas Bartsch,Wang Zhiqiang,On the existence of sign-changing solutions for semilinear Dirichlet problems,Topological Methods in Nonlinear Analysis,Journal of the Juliusz Schauder Center,1996,(7):115-131.[11]Li Shujie,Zhang Zhitao,Multiple solutions theorems for semilinear elliptic boundary value problems with resonance at infinity,Discrete and Continuous Dynamical System,1999,5(3):489-493.[12]Mawhin,J.,Willem,M.,Critical Point Theory and Hamiltonian Systems,New York:Springer-Verlag,1989.[13]Chang Kung-ching,A variant mountain pass lemma,Science in China,Ser.A (in Chinese),1983,(4):306-317.[14]Chang Kung-ching,Infinite Dimentional Morse Theory and Multiple Solutions Problems,Basel:Birkhauser,1993.[15]Whyburn,G.T.,Topological Analysis,Princeton:Princeton University Press,1958.[16]Liu Zhaoli,A topological property of the boundary of bounded open sets in R2,Journal of Shandong University,1994,29(3):299-303.[17]Dancer,E.N.,Du Yihong,On sign-changing solutions of certain semilinear elliptic problems,Appl.Anal.,1995,56:193-206.
    • CHEN; Fan
    • 摘要: [1]Hirata,K.,Yamamoto,K.,Iijinma,J.et al.,Tunneling measurements on superconductor/insulator/superconductor junctions using single-crystal YBa2Cu3O7-x thin films,Appl.Phys.Lett.,1990,56(7):683-685.[2]Kingston,J.J.,Wellstood,F.C.,Lerch,P.et al.,Multilayer YBa2Cu3Ox-SrTiO3-YBa2Cu3Ox films for insulating crossovers,Appl.Phys.Lett.,1990,56(2):189-191.[3]Grundler,D.,Krumme,J.P.,David,B.et al.,YBa2Cu3O7 ramp-type junctions and superconducting quantum interference devices with an ultra thin barrier of NdGaO3,Appl.Phys.Lett.,1994,65(14):1841-1843.[4]Yang Guozhen,Lu Huibin,Chen Zhenghao et al.,Laser molecular beam epitaxy system and its key technologies,Science in China (in Chinese),Ser.A,1998,28(3):260-265.[5]Wang Ning,Lu Huibin,Chen,W.Z.et al.,Morphology and microstructure of BaTiO3/SrTiO3 superlattices grown on SrTiO3 by laser molecular-beam epitaxy,Appl.Phys.Lett.,1999,75(22):3464-3466.[6]Chen Li-Chyng,Particulates generated by pulsed laser ablation,in Pulsed Laser Deposition of Thin Films (eds.Chrisey,D.B.,Hulber,G.K.),New York:John Wiley & Sons,Inc.,1994,167-198.[7]Wang,H.S.,Dietsche,W.,Eissler,D.et al.,Molecular beam epitaxial growth and structure properties of DyBa2Cu3O7-y,J.Crys.Growth,1993,126:565-577.[8]Kita,R.,Hase,T.,Itti,R.et al.,Synthesis of CuO films using mass-separated,low-energy O+ ion beams,Appl.Phys.Lett.,1992,60(21):2684-2685.[9]Lu Huibin,Zhou Yueliang,Yang Guozhen et al.,Active gas source for thin film preparation,Chinese Patent (in Chinese),1996,No.ZL 96219046.2.[10]Wang Jing,Chen Fan,Zhao Tong et al.,Fabrication of high stable DC-SQUIDS with L-MBE YBCO thin films,Chinese Journal of Low Temperature Physics (in Chinese),1999,21(1):13-16.
    • LU; Yonghao
    • 摘要: [1]Otsuka,K.,Kubo,H.,Wayman,C.M.,Diffuse electron scattering and “streaming” effect,Metall.Trans.A,1981,12:595-605.[2]Otsuka,K.,Wayman,C.M.,Kubo,H.,Diffuse electron scattering in β-phase alloys,Metall.Trans.A,1978,9:1075-1085.[3]Singh,J.,Chen,H.,Wayman,C.M.,Transformation sequence in a Cu-Al-Ni shape memory alloy at elevated temperatures,Metall.Trans.A,1986,17:65-72.[4]Sun,Y.S.,Lorimer,G.W.,Ridley,N.,Microstructure and its development in Cu-Al-Ni alloys,Metall.Trans.A,1990,21:575-588.[5]Miyazaki,S.,Kawai,T.,Otsuka,K.,On the origin of intergranular fracture in β phase shape memory alloys,Scripta Metall.,1982,16:431-436.[6]Otsuka,K.,Wayman,C.M.,Naka,K.et al.,Superelasticity effects and stress-induced martensitic transformations in Cu-Al-Ni alloys,Acta Metall.,1976,24:207-226.[7]Otsuka,K.,Sakamoto,H.,Shimizu,K.,Successive stress-induced martensitic transformations and associated transformation pseudoelasticity in Cu-Al-Ni alloys,Acta Metall.,1979,27:585-600.[8]Shield,T.W.,Orientation dependence of the pseudoelastic behavior of single crystal of Cu-Al-Ni in tension,J.Mech.Phys.Solids,1995,43(6):869-895.[9]Sun,Q.P.,Zhang,X.Y.,Xu,T.,Experimental study of martensitic transformation in single shape memory alloy,Adv.Solids Mech.,1997,7:155-162.[10]Chen,Q.Z.,Chu,W.Y.,Hsiao,C.M.,In-situ TEM observation of nucleation and bluntness of nanocrack in 310 stainless steel,Acta Metall.Mater.,1995,43:4371-4376.[11]Chu,W.Y.,Gao,K.W.,Wang,Y.B.et al.,Nucleating and propagation of nanocrack in dislocation free zone in brittle material,Science in China,Ser.A,1995,38(14):1501-1509.[12]Chen,Q.Z.,Gao,K.W.,Gu,B.et al.,Nucleating,blunting and propagation of A nanocrack in DFZ of thin crystals,Fatigue Frac.Eng.Mater.Stru.,1996,21:1415-1423.[13]Nishiyama,Z.,Stacking faults in the martensite of Cu-Al alloy,Journal of the Physical Society of Japan,1965,20:1192-1121.[14]Lovey,F.C.,Van Tendeloo,G.,Van Landuyt,J.et al.,HREM imaging condition for stacking sequences in 18R martensite of Cu-Al alloys,Scripta Metall.,1985,19:1223-1228.[15]Takezawa,K.,Shindo,T.,Sato,S.,Shape memory effect in β1-CuZnAl alloys,Scripta Metall.,1976,10:13-18.[16]Saburi,T.,Wayman,C.M.,Crystallographic similarities in shape memory martensites,Acta Metall.,1979,27:979-995.[17]Adachi,K.,Perkins,J.,Deformation of martensite in a polystalline Cu-Zn-Al alloy,Metall.Trans.,1986,17:945-959.[18]Miyazaki,S.,Totsuka,K.,Development of shape memory alloys,ISIJ International,1989,29(5):353.[19]Chu,W.Y.,An Introduction to Fracture Mechanics (in Chinese),Beijing:Science and Technology Press,1979,4.
    • HU; Qiya
    • 摘要: [1]Carstensen,C.,Gwinner,J.,FEM and BEM coupling for a nonlinear transmission problem with Signorini contact,SIAM J.Numer.Anal.,1997,34(6):1845-1864.[2]Costabel,M.,Stephan,E.,Coupling of finite and boundary element methods for an elastoplastic interface problem,SIAM J.Numer.Anal.,1990,27(4):1212-1226.[3]Kikuchi,N.,Oden,J.,Contact problem in elasticity:a study of variational inequalities and finite element methods,Philadelphia,SIAM,1988.[4]Necas,J.,Introduction to the Theory of Nonlinear Elliptic Equations,Text 52,Leipzig:Teubner,1983.[5]Carstensen,C.,Interface problem in holonomic elastoplasticity,Math.Methods Appl.Sci.,1993,16(11):819-835.[6]Gatica,G.,Hsiao,G.,On the coupled BEM and FEM or a nonlinear exterior Dirichlet problem in R2,Numer.Math.,1992,61(2):171-214.[7]Mund,P.,Stephan,E.,An adaptive two-level method for the coupling of nonlinear FEM-BEM equations,SIAM J.Numer.Anal.,1999,36(3):1001-1021.[8]Meddahi,S.,An optimal iterative process for the Johnson-Nedelec method of coupling boundary and finite elements,SIAM J.Numer.Anal.,1998,35(4):1393-1415.[9]Yu,D.,The Mathematical Theory of the Natural Boundary Element Methods (in Chinese),Beijing:Science Press,1993.[10]Lions,J.,Magenes,E.,Non-homogeneous Boundary Value Problems and Applications,Vol.I,Berlin-Heidelberg-New York:Springer-Verlag,1972.[11]Zenisek,A.,Nonlinear Elliptic and Evolution Problems and Their Finite Element Approximations,London:Academic Press,1990.[12]Costabel,M.,Boundary integral operators on Lipschitz domains:Elementary results,SIAM J.Numer.Math.Anal.,1988,19(2):613-626.
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