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Growth of Ni-Al alloys on Ni(111), from Al deposits of various thicknesses: (II) Formation of NiAl over a Ni3Al interfacial layer

机译:由各种厚度的Al沉积物在Ni(111)上生长Ni-Al合金:(II)在Ni3Al界面层上形成NiAl

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This paper describes the second part of a study devoted to the growth of thin Ni-Al alloys after deposition of Al on Ni(111). In the previous paper [S. Le Pevedic, D. Schmaus, C. Cohen, Surf. Sci. 600 (2006) 565] we have described the results obtained for ultra-thin Al deposits, leading, after annealing at 750 K, to an epitaxial layer of Ni3Al(111). In the present paper we show that this regime is only observed for Al deposits smaller than 8 X 10(15) Al/cm(2) and we describe the results obtained for Al deposits exceeding this critical thickness, up to 200 x 10(15) Al/cm(2). Al deposition was performed at low temperature (around 130 K) and the alloying process was followed in situ during subsequent annealing, by Auger electron spectroscopy, low energy electron diffraction and ion beam analysis-channeling measurements, in an ultra-high vacuum chamber connected to a Van de Graaff accelerator. We evidence the formation, after annealing at 750 K, of a crystallographically and chemically well-ordered NiAl(110) layer (whose thickness depends on the deposited Al amount), over a Ni3Al "interfacial" layer (whose thickness-about 18 (111) planes-is independent of rhe deposited Al amount). The NiAl over-layer is composed of three variants, at 120 degrees from each other in the surface plane, in relation with the respective symmetries of NiAl(l 10) and Ni3Al(111). The NiAl layer is relaxed (the lattice parameters of cc-B2 NiAl and fcc-Ll(2) Ni3Al differ markedly), and we have determined its epitaxial relationship. In the case of the thickest alloyed layer formed the results concerning the structure of the NiAl layer have been confirmed and refined by ex situ X-ray diffraction and information on its grain size has been obtained by ex situ Atomic Force Microscopy. The kinetics of the alloying process is complex. It corresponds to an heterogeneous growth leading, above the thin NiAl interfacial layer, to a mixture of At and NiAl over the whole Al film, up to the surface. The atomic diffusion is very limited in the NiAl phase that forms, and thus the progressive enrichment in Ni of the At film, i.e. of the mean Ni concentration, becomes slower and slower. As a consequence, alloying is observed to take place in a very broad temperature range between 300 K and 700 K. For annealing temperatures above 800 K, the alloyed layer is decomposed, Al atoms diffusing in the bulk of the substrate. (c) 2006 Elsevier B.V. All rights reserved.
机译:本文介绍了研究的第二部分,该研究致力于在Al(Ni)(111)上沉积Al后薄Ni-Al合金的生长。在以前的论文[S. Le Pevedic,D。Schmaus,C。Cohen,Surf。科学600(2006)565]我们描述了超薄Al沉积物的结果,该沉积物在750 K退火后导致Ni3Al(111)的外延层。在本文中,我们表明仅在小于8 X 10(15)Al / cm(2)的Al沉积物中观察到这种情况,并且我们描述了超过此临界厚度直至200 x 10(15)的Al沉积获得的结果Al / cm(2)。在低温(约130 K)下进行铝沉积,并在随后的退火过程中,通过俄歇电子能谱,低能电子衍射和离子束分析-通道测量,在与之相连的超高真空室内进行合金化工艺。 Van de Graaff加速器。我们证明了在750 K退火后,在Ni3Al“界面”层(其厚度约为18(111)上,在晶体学和化学上有序的NiAl(110)层(其厚度取决于所沉积的Al量)的形成。 )平面-与rhe沉积的Al量无关)。 NiAl覆盖层由三个变体组成,相对于NiAl(110)和Ni3Al(111)的各自对称性,它们在表面平面上彼此成120度。 NiAl层松弛(cc-B2 NiAl和fcc-Ll(2)Ni3Al的晶格参数明显不同),我们确定了其外延关系。在形成最厚的合金层的情况下,已通过异位X射线衍射确认并改进了与NiAl层结构有关的结果,并已通过异位原子力显微镜获得了有关其晶粒尺寸的信息。合金化过程的动力学很复杂。它对应于异质生长,导致在薄的NiAl界面层上方,导致整个Al膜上直至表面的At和NiAl的混合物。原子的扩散在所形成的NiAl相中非常有限,因此,At膜中Ni的逐渐富集,即平均Ni浓度,变得越来越慢。结果,观察到合金化发生在300 K至700 K的非常宽的温度范围内。对于高于800 K的退火温度,合金层被分解,Al原子扩散到整个基板中。 (c)2006 Elsevier B.V.保留所有权利。

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