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1.
质子交换膜燃料电池(PEMFC)作为一种清洁、高效的能源转化装置,已经备受学术界与产业界的关注.然而,高活性、高稳定性与低成本的铂基阴极氧还原(ORR)电催化剂的缺乏,严重限制PEMFC的大规模商业化应用.为提高贵金属铂的电催化性能,核壳纳米结构的研究受到广范关注.然而,核壳纳米结构的制备过程通常需要采用有机前驱体、表面活性剂与较高的反应温度,导致大多核壳结构制备方法的大规模应用受到限制.我们在室温下无表面活性剂与高沸点溶剂的参与下,通过钯表面吸附的解离的氢原子来还原K_2PtCl_4,得到Pd_核@Pt_壳纳米结构.通过改变加入K_2PtCl_4的量,可以成功控制壳的厚度;通过透射电子显微镜(TEM)观察得知,我们制备了铂壳厚度分别为0.45,0.75,0.9 nm的核壳结构.Pd_核@Pt_壳纳米结构的良好的纳米晶体结构与外延生长模式,通过高分辨透射电子显微镜(HRTEM)与能量色散谱仪(EDS)得到证实.同时,所制备Pd_核@Pt_壳样品的核壳结构通过高角环形暗场-扫描透射-元素分布(HAADF-STEM-EDX)表征方法,得到证实.X射线粉末衍射(XRD)表征证实,样品Pd_核@Pt_壳并无单独的Pd或Pt衍射峰出现,而是表现出良好的同种晶相结构;相对于单质Pt,样品中Pd核的存在导致Pd_核@Pt_壳核壳结构表现出一定程度的晶格紧缩.X射线光电子能谱(XPS)表明,钯核的存在导致铂壳的电子结合能增大,并且当铂壳厚度增大到一定程度后,核壳结构引起的电子效应维持不变.通过XPS分峰拟合可知,Pd_核@Pt_壳结构中零价态的铂含量均在80%以上,并且零价态的铂含量随着铂壳层厚度的增大而增大.采用电感耦合等离子体(ICP)与XPS,发现铂的表面富集现象,并且铂表面富集现象随着铂壳层厚度的增大而增大.在半电池中,经过循环伏安扫描活化,Pd_核@Pt_壳表现出明显的铂的氢吸附与脱附特征峰,再次证明了铂壳层的成功包覆.Pd_核@Pt_壳纳米颗粒表现出优于Pt/C(JM)的面积比活性、质量比活性及电化学稳定性.核壳结构的良好的ORR电催化性能,来源于催化剂表面含氧物种吸附强度的减弱;上述现象归因于钯核与铂壳之间的电子效应与晶格应力效应.此处简易、清洁的核壳结构制备方法也可以用来在温和条件下制备Ni_核@Pt_壳等核壳结构.  相似文献   

2.
金晟中  张爱清 《应用化学》2018,35(2):239-244
采用连续多元醇法,以RuCl3·xH2O和PtCl2为前驱体,乙二醇为还原剂,聚乙烯吡咯烷酮为稳定剂的反应体系,并通过调节PtCl2用量和还原温度成功制备了壳层厚度约为1.5个Pt原子层的单分散Ru@Pt核壳结构纳米粒子,利用透射电子显微镜(TEM)、X射线衍射仪(XRD)、X射线光电子能谱仪(XPS)等分析方法对其微观结构、粒径分布、晶型结构、物相组成进行了表征。 结果表明,该纳米粒子分布均匀且基本为球形,平均粒径约为3.57 nm,其中内核直径约为2.49 nm,外壳厚度约为0.55 nm,壳层金属Pt具有很好的晶型,Pt原子主要为{111}晶面,内核金属Ru与外壳金属Pt互相产生了电子效应使Pt的衍射峰和Ru、Pt的电子结合能产生了一定偏移,并初步研究了有效控制该核壳结构纳米粒子壳层厚度和增强核与壳两种金属之间电子效应的因素,使其有望在催化等领域发挥潜在的应用价值。  相似文献   

3.
铂原子单层的核壳结构催化剂因其高效的铂原子利用率和优异铂质量活性而广泛应用于燃料电池领域.在该系列材料中,钯@铂核壳催化剂具有更优于纯铂的氧还原(ORR)催化活性,因而拥有较好的应用前景.但由于钯原子在热力学上更倾向于富集到材料表面,钯@铂核壳催化剂的催化稳定性及原子扩散的途径需要更深入的研究.本文探究了热处理条件对钯@铂核壳结构稳定性的破坏,并确定了原子扩散对催化活性的影响.原位扫描透射电子显微镜-电子能量损失谱(STEM-EELS)证明了在250 oC的氩气氛围中,钯@铂纳米颗粒中原本清晰可见的1–2原子铂壳层已经消失,并伴随着颗粒表面钯铂合金化的形成.因钯金属可以吸收氢气而导致晶格间距的展宽,钯@铂核壳结构的破坏也可以通过氢气氛围中的原位X射线衍射谱中(111)衍射峰的展宽和位移进行判断.对钯@铂核壳纳米催化剂进行一系列温度的热处理结果显示,核壳结构的破坏在200 oC左右开始,并于200–300 oC之间急剧发生.一氧化碳电化学氧化脱附实验表明,热处理之后的核壳催化剂表面的一氧化碳氧化峰位置发生了明显的正移,也证明了热处理之后催化剂表面电子结构的变化.核壳结构改变对催化活性的影响也通过旋转圆盘电极进行了测量.相比于未经处理的样品, 200 oC处理之后的钯@铂核壳催化剂在0.9 V电位处的质量活性损失了约37%.进一步提高热处理温度至300 oC之后,钯@铂核壳催化剂的质量活性只有初始状态的44%.本文揭示核壳结构中因热处理而导致的原子扩散现象,并为燃料电池中核壳催化剂的应用及膜电极的制备工艺条件提供了参考.  相似文献   

4.
制备并表征了原子分散的模型体系:氧化铈负载的Pt-Co核壳催化剂.采用超高真空物理气相沉积法制备了有序CeO2(111)膜上的Pt@Co和Co@Pt核壳纳米结构,并用同步辐射光电子能谱和共振光发射光谱对其进行了研究.在低Co覆盖率(0.5 ML)下Co在CeO2(111)上沉积生成Co-CeO2(111)固溶体,然后在更高Co覆盖率下生长为金属Co纳米粒子.Pt@Co和Co@Pt两种模型结构在300-500 K温度范围内都能稳定地抗烧结.在500 K退火后, Pt@Co纳米结构含有接近纯的钴壳,而Co@Pt中的铂壳部分被金属钴覆盖.在550 K以上,在Pt@Co和Co@Pt纳米结构中近表面区域的重新排序中产生了次表层的Pt Co合金和富铂外壳.对于Co@Pt纳米粒子,近表面区域的化学有序性取决于沉积铂壳的初始厚度.无论初始铂壳的厚度如何,在有氧存在下对Co@Pt纳米结构进行退火,都会导致Pt-Co合金的分解以及Co的氧化.Co的逐步氧化与吸附质诱导的Co偏析共同导致在负载的Co@Pt纳米结构表面形成厚的Co O层.这一过程伴随着CeO2(111)薄膜的裂解,以及在550K以上氧气中退火后CeO2包裹氧化的Co@Pt纳米结构.很明显,于不同温度下在氧气和氢气的氧化-还原循环过程中,无论铂的初始厚度是多少,负载的Co@Pt纳米颗粒的结构和化学成分的变化主要是由氧化所致,而还原处理的影响则很小.  相似文献   

5.
应用晶种生长法制得金纳米立方体,Aucore-Pdshell和Aucore-Pdshell-Ptcluster电催化剂,通过改变溶液的H2PdCl4和H2PtCl6的用量以控制Pdshell的厚度和Ptcluster的覆盖度.采用扫描电镜(SEM)、透射电镜(TEM)观察了金纳米立方体的表面结构.利用循环伏安法(CV)研究了不同Pd层厚度的立方体形Aucore-Pdshell纳米粒子和不同Pt岛覆盖度的立方体形Aucore-Pdshell-Ptcluster纳米粒子对甲酸氧化的电催化性能.结果表明,与立方体形Aucore-Pdshell纳米粒子相比,"核-壳-岛"结构的立方体形Aucore-Pdshell-Ptcluster纳米粒子对甲酸的电氧化具有更高活性.当Pd壳层厚度为3层,Pt岛覆盖度为0.5时,电催化活性最高.  相似文献   

6.
本文控制合成一维方向生长的直径为1.5 nm,长度为11.8 nm的超细Pd纳米线,结合欠电位沉积方法在其表面制备了不同Pt原子层的Pd@Pt核壳结构纳米电催化剂. 高分辨透射电镜和光电子能谱结果证实了这种核壳结构及Pt在Pd纳米线上的均匀分布. 相比于商业化Pt黑催化剂,该核壳结构电催化剂对酸性介质中的氧气还原反应呈现了较高的电催化活性和增强的耐久性. 显著增强的耐久性可归属于催化剂一维结构的稳定性.  相似文献   

7.
在质子交换膜燃料电池(PEMFC)中,由于阴极氧还原反应(ORR)速率缓慢,因此开发高效的ORR催化剂是实现燃料电池商业化的关键. 世界各地的研究人员在提高催化剂活性和耐久性方面做出了不懈的努力. 目前,铂基催化剂仍然是商业应用上的首选,为开发实用的低铂氧还原催化剂,研究人员开展了大量的研究. 本文说明了ORR反应遇到的挑战,并介绍了近年来铂基氧还原催化剂的研究进展,具体包括ORR机理、铂核壳结构、一维纳米Pt催化剂和其他的代表性工作.  相似文献   

8.
光化学合成Au核@Pd壳复合纳米粒子及其表征   总被引:1,自引:0,他引:1  
在PEG-丙酮溶液体系中, 采用紫外光辐射还原Au(Ⅲ), Pd(Ⅱ)离子混合物和以Au晶种为核、紫外光辐射还原Pd(Ⅱ)使其沉积在Au晶种表面上这两种方法, 合成了Au核@Pd壳复合纳米粒子. 通过改变Au(Ⅲ)离子或Au晶种对Pd(Ⅱ)离子的摩尔比调节复合粒子的尺寸和Pd壳厚度, 分别获得了直径范围为5.6~4.6 nm和4.6~6.2 nm的复合粒子. 利用UV-Vis吸收光谱、TEM、HR-TEM和XPS等表征手段, 证明了合成的纳米粒子为核-壳复合结构. 研究了Au@Pd纳米粒子的直径随溶液中Au(Ⅲ)/Pd(Ⅱ)摩尔比的改变而变化的规律; 对Au核向Pd壳的供电子作用以及复合粒子的光化学形成机理进行了讨论.  相似文献   

9.
本实验利用铜的欠电位沉积技术,在旋转圆盘电极上以碳负载的钯纳米颗粒为核,制备铂单原子层核壳结构催化剂. 电化学测试用于表征不同Nafion含量的添加对于核壳结构催化剂制备的影响. 实验证明,Nafion的存在会影响铜的欠电位沉积,铂与铜的置换反应,并决定最终制备的核壳结构催化剂的氧还原催化反应的活性. 当催化剂薄层中Nafion的含量低于5%的时候,添加Nafion不但可以帮助催化剂附着在旋转圆盘电极表面,而且可以保证制备的催化剂具有较好的氧还原反应催化活性. 在H2SO4溶液中,钯纳米颗粒的表面存在特殊的阴离子吸/脱附电化学信号峰,这些信号峰可以用来监测Nafion含量对于铂单原子层核壳结构催化剂制备的影响.  相似文献   

10.
铂原子单层的核壳结构催化剂因其高效的铂原子利用率和优异铂质量活性而广泛应用于燃料电池领域.在该系列材料中,钯@铂核壳催化剂具有更优于纯铂的氧还原(ORR)催化活性,因而拥有较好的应用前景.但由于钯原子在热力学上更倾向于富集到材料表面,钯@铂核壳催化剂的催化稳定性及原子扩散的途径需要更深入的研究.本文探究了热处理条件对钯@铂核壳结构稳定性的破坏,并确定了原子扩散对催化活性的影响.原位扫描透射电子显微镜-电子能量损失谱(STEM-EELS)证明了在250 oC的氩气氛围中,钯@铂纳米颗粒中原本清晰可见的1–2原子铂壳层已经消失,并伴随着颗粒表面钯铂合金化的形成.因钯金属可以吸收氢气而导致晶格间距的展宽,钯@铂核壳结构的破坏也可以通过氢气氛围中的原位X射线衍射谱中(111)衍射峰的展宽和位移进行判断.对钯@铂核壳纳米催化剂进行一系列温度的热处理结果显示,核壳结构的破坏在200 oC左右开始,并于200–300 oC之间急剧发生.一氧化碳电化学氧化脱附实验表明,热处理之后的核壳催化剂表面的一氧化碳氧化峰位置发生了明显的正移,也证明了热处理之后催化剂表面电子结构的变化.核壳结构改变对催化活性的影响也通过旋转圆盘电极进行了测量.相比于未经处理的样品, 200 oC处理之后的钯@铂核壳催化剂在0.9 V电位处的质量活性损失了约37%.进一步提高热处理温度至300 oC之后,钯@铂核壳催化剂的质量活性只有初始状态的44%.本文揭示核壳结构中因热处理而导致的原子扩散现象,并为燃料电池中核壳催化剂的应用及膜电极的制备工艺条件提供了参考.  相似文献   

11.
Heterogeneous Au-Pt nanostructures have been synthesized using a sacrificial template-based approach. Typically, monodispersed Au nanoparticles are prepared first, followed by Ag coating to form core-shell Au-Ag nanoparticles. Next, the galvanic replacement reaction between Ag shells and an aqueous H(2)PtCl(6) solution, whose chemical reaction can be described as 4Ag + PtCl(6)(2-)→ Pt + 4AgCl + 2Cl(-), is carried out at room temperature. Pure Ag shell is transformed into a shell made of Ag/Pt alloy by galvanic replacement. The AgCl formed simultaneously roughens the surface of alloy Ag-Pt shells, which can be manipulated to create a porous Pt surface for oxygen reduction reaction. Finally, Ag and AgCl are removed from core-shell Au-Ag/Pt nanoparticles using bis(p-sulfonatophenyl)phenylphosphane dihydrate dipotassium salt to produce heterogeneous Au-Pt nanostructures. The heterogeneous Au-Pt nanostructures have displayed superior catalytic activity towards oxygen reduction in direct methanol fuel cells because of the electronic coupling effect between the inner-placed Au core and the Pt shell.  相似文献   

12.
采用电化学方法在铟锡氧化物(ITO)导电玻璃基底上制备了高度有序的ZnO纳米管阵列,然后在ZnO纳米管阵列上电化学沉积Cu2O纳米晶颗粒,获得了一维有序Cu2O/ZnO核壳式纳米阵列结构,通过控制Cu2O纳米晶的沉积电量得到不同厚度的Cu2O壳层,并对该核壳式纳米阵列的形貌和结构进行了分析. 以Cu2O/ZnO一维核壳式纳米阵列结构为光电极组装全固态纳米结构太阳电池,研究了Cu2O壳层厚度对光电极光吸收性能、光电性能以及组装电池光伏性能的影响,优化了电池中对电极材料的喷金厚度. 结果表明,以Cu2O沉积电量为1.5 C的Cu2O/ZnO为光活性层,以4 mA电流下真空镀金20~25 min的铜基底为对电极组装的简易太阳电池最高可获得0.013%的光电转换效率.  相似文献   

13.
The water-soluble Ag/Pt core-shell nanoparticles were prepared by deposition Pt over Ag colloidal seeds with the seed-growth method using K2PtCl4 with trisodium citrate as reduced agent. The Ag:Pt ratio is varied from 9:1 to 1:3 for synthesizing Pt shell layer of different thickness. A remarkable shift and broadening of Ag surface plasmon band around 410 nm was observed. The contrast of TEM images of Ag/Pt colloids has been obtained. Various techniques, such as transmission electron microscopy (TEM), UV-vis absorption and resonance light-scattering spectroscopy were used to characterize nanoparticles. The data of TEM, UV-vis and resonance light-scattering spectrum all confirm formation of Ag/Pt core-shell nanoparticles. Resonance light-scattering and emission spectrum show the Ag and Ag/Pt core-shell nanoparticles have a nonlinear light-scattering characteristic.  相似文献   

14.
In this work, we utilize the galvanic displacement synthesis and make it a general and efficient method for the preparation of Au-M (M = Au, Pd, and Pt) core-shell nanostructures with porous shells, which consist of multilayer nanoparticles. The method is generally applicable to the preparation of Au-Au, Au-Pd, and Au-Pt core-shell nanostructures with typical porous shells. Moreover, the Au-Au isomeric core-shell nanostructure is reported for the first time. The lower oxidation states of Au(I), Pd(II), and Pt(II) are supposed to contribute to the formation of porous core-shell nanostructures instead of yolk-shell nanostructures. The electrocatalytic ethanol oxidation and oxygen reduction reaction (ORR) performance of porous Au-Pd core-shell nanostructures are assessed as a typical example for the investigation of the advantages of the obtained core-shell nanostructures. As expected, the Au-Pd core-shell nanostructure indeed exhibits a significantly reduced overpotential (the peak potential is shifted in the positive direction by 44?mV and 32?mV), a much improved CO tolerance (I(f)/I(b) is 3.6 and 1.63 times higher), and an enhanced catalytic stability in comparison with Pd nanoparticles and Pt/C catalysts. Thus, porous Au-M (M = Au, Pd, and Pt) core-shell nanostructures may provide many opportunities in the fields of organic catalysis, direct alcohol fuel cells, surface-enhanced Raman scattering, and so forth.  相似文献   

15.
以Au粒子(55nm)为核,抗坏血酸为还原剂,将不同量的Pt沉积在Au核上,制得可控壳层厚度(0.3~6nm)的Pt包Au纳米粒子(Aucore@Ptshell).用紫外-可见吸收光谱、扫描电镜(SEM)、透射电镜(TEM)和电化学循环伏安法等观测Aucore@Ptshell纳米粒子的表面形貌、结构和性能.另以SCN-为探针,考察了Pt壳厚度对Aucore@Ptshell纳米粒子SERS信号的影响.结果表明,SCN-离子的SERS信号强度随Pt壳厚度的增加呈指数衰减,当Pt壳厚度为1.4nm时,Aucore@Ptshel纳米粒子表现出铂良好的电化学性能,又具有较强的SERS活性.  相似文献   

16.
The sensitivities of five different core-shell nanostructures were investigated towards changes in the refractive index of the surrounding medium. The shift of the localized surface plasmon resonance (LSPR) maximum served as a measure of the (respective) sensitivity. Thus, gold-silver core-shell nanoparticles (NPs) were prepared with different shell thicknesses in a two-step chemical process without the use of any (possibly disturbing) surfactants. The measurements were supported by ultramicroscopic images in order to size the resulting core-shell structures. When compared to sensitivities of nanostructures reported in the literature with those of the (roughly spherical) gold-silver core-shell NPs, the latter showed comparable (or even higher) sensitivities than gold nanorods. The experimental finding is supported by theoretical calculation of optical properties of such core-shell NP. Extinction spectra of ideal spherical and deformed core-shell NPs with various core/shell sizes were calculated, and the presence of an optimal silver shell thickness with increased sensitivity was confirmed. This effect is explained by the existence of two overlapping plasmon bands in the NP, which change their relative intensity upon change of refractive index. Results of this research show a possibility of improving LSPR sensor by adding an extra metallic layer of certain thickness.  相似文献   

17.
何圣超  费兆阳  李雷  孙博  冯新振  季伟捷 《催化学报》2013,34(11):2098-2109
采用简便的“先核后壳”和“先壳后核”途径制备了M@SiO2 (M=Ag, Au, Pt)核壳结构. 采用“先核后壳”途径时,金属内核可以控制在6 -9 nmm, 粒径分布均匀, SiO2壳层织构可调. 该途径制备过程简便, 无需高速离心分离, 可有效节约制备成本. 由该途径制得的Au@mSiO2中纳米Au的热稳定性高, 经550 ℃空气焙烧后仍能保持高的CO氧化性能(T100=235 ℃). 由“先壳后核”途径制得的核壳结构内核金属粒子也可以控制在< 10 nmm, 粒径分布均匀, 且SiO2壳层孔隙率可以预调, 即使在液相中也可有效消除对硝基苯酚反应物分子的扩散限制, 并于室温下将其还原为对氨基苯酚. 两种途径所得的核壳结构均呈高单分散态. 使用含有不同有机官能团的硅源可对介孔SiO2壳层进行进一步改性, 拓展应用领域, 因而具有很好的潜在应用前景.  相似文献   

18.
A new process has been developed for the synthesis of nanocrystalline niobium oxide and niobium diboride using an amorphous niobium precursor obtained via the solvothermal route. On varying the ratio of niobium precursor to boron and the reaction conditions, pure phases of nanostructured niobium oxides (Nb(2)O(5), NbO(2)), niobium diboride (NbB(2)) and core-shell nanostructures of NbB(2)@Nb(2)O(5) could be obtained at normal pressure and low temperature of 1300 °C compared to a temperature of 1650 °C normally used. The above borothermal process involves the in situ generation of B(2)O(2) to yield either oxide or diboride. The niobium oxides and borides have been characterized in detail by XRD, HRTEM and EDX studies. The core-shell structure has been investigated by XPS depth profiling, EFTEM and EELS (especially to characterize the presence of boron and the shell thickness). The niobium diboride nanorods (with high aspect ratio) show a superconducting transition with the T(c) of 6.4 K. In the core-shell of NbB(2)@Nb(2)O(5), the superconductivity of NbB(2) is masked by the niobium oxide shell and hence no superconductivity was observed. The above methodology has the benefits of realizing both oxides and borides of niobium in nanocrystalline form, in high purity and at much lower temperatures.  相似文献   

19.
Silica-metal nanostructures consisting of silica cores and metal nanoshells attract a lot of attention because of their unique properties and potential applications ranging from catalysis and biosensing to optical devices and medicine. The important feature of these nanostructures is the possibility of controlling their properties by the variation of their geometry, shell morphology and shell material. This review is devoted to silica-noble metal core-shell nanostructures; specifically, it outlines the main methods used for the preparation and surface modification of silica particles and presents the major strategies for the formation of metal nanoshells on the modified silica particles. A special emphasis is given to the St?ber method, which is relatively simple, effective and well verified for the synthesis of large and highly uniform silica particles (with diameters from 100 nm to a few microns). Next, the surface chemistry of these particles is discussed with a special focus on the attachment of specific organic groups such as aminopropyl or mercaptopropyl groups, which interact strongly with metal species. Finally, the synthesis, characterization and application of various silica-metal core-shell nanostructures are reviewed, especially in relation to the siliceous cores with gold or silver nanoshells. Nowadays, gold is most often used metal for the formation of nanoshells due to its beneficial properties for many applications. However, other metals such as silver, platinum, palladium, nickel and copper were also used for fabrication of core-shell nanostructures. Silica-metal nanostructures can be prepared using various methods, for instance, (i) growth of metal nanoshells on the siliceous cores with deposited metal nanoparticles, (ii) reduction of metal species accompanied by precipitation of metal nanoparticles on the modified silica cores, and (iii) formation of metal nanoshells under ultrasonic conditions. A special emphasis is given to the seed-mediated growth, where metal nanoshells are formed on the modified silica cores with deposited metal nanoparticles. This strategy assures a good control of the nanoshell thickness as well as its surface properties.  相似文献   

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