X-ray reflectivity investigation of near-surface density changes induced in Al–Au multilayers by high-current ion beam bombardment

Author(s):  
A. Markwitz ◽  
F. Prokert ◽  
M. Waldschmidt ◽  
G. Demortier
2005 ◽  
Vol 04 (03) ◽  
pp. 269-286 ◽  
Author(s):  
F. WATT ◽  
A. A. BETTIOL ◽  
J. A. VAN KAN ◽  
E. J. TEO ◽  
M. B. H. BREESE

To overcome the diffraction constraints of traditional optical lithography, the next generation lithographies (NGLs) will utilize any one or more of EUV (extreme ultraviolet), X-ray, electron or ion beam technologies to produce sub-100 nm features. Perhaps the most under-developed and under-rated is the utilization of ions for lithographic purposes. All three ion beam techniques, FIB (Focused Ion Beam), Proton Beam Writing (p-beam writing) and Ion Projection Lithography (IPL) have now breached the technologically difficult 100 nm barrier, and are now capable of fabricating structures at the nanoscale. FIB, p-beam writing and IPL have the flexibility and potential to become leading contenders as NGLs. The three ion beam techniques have widely different attributes, and as such have their own strengths, niche areas and application areas. The physical principles underlying ion beam interactions with materials are described, together with a comparison with other lithographic techniques (electron beam writing and EUV/X-ray lithography). IPL follows the traditional lines of lithography, utilizing large area masks through which a pattern is replicated in resist material which can be used to modify the near-surface properties. In IPL, the complete absence of diffraction effects coupled with ability to tailor the depth of ion penetration to suit the resist thickness or the depth of modification are prime characteristics of this technique, as is the ability to pattern a large area in a single brief irradiation exposure without any wet processing steps. p-beam writing and FIB are direct write (maskless) processes, which for a long time have been considered too slow for mass production. However, these two techniques may have some distinct advantages when used in combination with nanoimprinting and pattern transfer. FIB can produce master stamps in any material, and p-beam writing is ideal for producing three-dimensional high-aspect ratio metallic stamps of precise geometry. The transfer of large scale patterns using nanoimprinting represents a technique of high potential for the mass production of a new generation of high area, high density, low dimensional structures. Finally a cross section of applications are chosen to demonstrate the potential of these new generation ion beam nanolithographies.


2021 ◽  
Vol 2064 (1) ◽  
pp. 012092
Author(s):  
A E Ligachev ◽  
M V Zhidkov ◽  
S A Sorokin ◽  
G V Potemkin ◽  
Yu R Kolobov

Abstract Effect of the pulsed soft X-ray fluxes (PSXF) on the surface topography of metals (Mg and Cu) has been investigated. Soft pulse X-ray irradiation (energy quanta of 0.1-1.0 keV) were carried out on a high-current MIG generator. The sample of magnesium was located at a distance of 10 cm from the X-ray source. Since the distance to the sample significantly exceeded the size of the X-ray beam, it can be assumed that the density of the X-ray radiation flow to the magnesium sample was uniform. The duration of the radiation pulse was 100 ns, and the radiation energy density in the pulse varied from 13 to 19 J/cm2. As a result of melting under the action of PSXF of the near-surface layer of metals and subsequent solidification, a wavy relief is formed on their surface. Defects in the form of craters, which usually occur after the impact of a powerful pulsed ion flow on metals, were not detected.


2013 ◽  
Vol 46 (2) ◽  
pp. 505-511 ◽  
Author(s):  
B. Khanbabaee ◽  
A. Biermanns ◽  
S. Facsko ◽  
J. Grenzer ◽  
U. Pietsch

This article reports on surface density variations that are accompanied by ion-beam-induced pattern formation processes on Si. The density profiles perpendicular to Si(100) surfaces were investigated after off-normal implantation with 5 keV Fe+ions at fluences ranging from 1 × 1016to 5 × 1017 ions cm−2. Ripple formation was observed for ion fluences above 1 × 1016 ions cm−2. X-ray reflectivity (XRR) revealed the formation of a nanometre subsurface layer with incorporated Fe. Using XRR, no major dependence of the surface density on the ion fluence could be found. In order to improve the surface sensitivity, extremely asymmetric X-ray diffraction was applied. Depth profiling was achieved by measuring X-ray rocking curves as a function of the decreasing incidence angle down to 0° using this noncoplanar scattering geometry. The density information was extracted from the dynamical Bragg shift of the diffraction peak caused by refraction of the X-ray beam at the air–sample interface. Simulations based on the dynamical theory of X-ray diffraction revealed a decrease of density for increasing ion fluence in a region close to the surface, caused by the amorphization and surface roughening.


2005 ◽  
Vol 98 (3) ◽  
pp. 033517 ◽  
Author(s):  
R. Klockenkämper ◽  
M. Becker ◽  
A. von Bohlen ◽  
H. W. Becker ◽  
H. Krzyzanowska ◽  
...  

1993 ◽  
Vol 321 ◽  
Author(s):  
E. D. Specht ◽  
D. A. Walko ◽  
S. J. Zinkle

ABSTRACTAt cryogenic temperatures, the accumulation of vacancy-interstitial pairs in Al2O3 from atomic displacements associated with ion implantation produces amorphization. At room temperature, these pairs recombine, and amorphization occurs only at high doses. X-ray reflectivity measurements show that amorphization of the surface of Al2O3 implanted at room temperature with 160 keV Cr+ ions is preceded by a progressive reduction in near-surface density. Monte Carlo simulations show that this density reduction can be accounted for by high-energy-transfer collisions which knock atoms deep into the target, leaving widely separated vacancies and interstitials, which do not recombine. Electron Microscopy shows that at least some of these vacancies condense into voids. We propose that this reduction in near-surface density can lead to amorphization at high doses. We present simple approximations for the density reduction expected for different ions and targets.


2013 ◽  
Vol 19 (S4) ◽  
pp. 95-96
Author(s):  
L.C. Alves ◽  
V. Corregidor ◽  
T. Pinheiro ◽  
L. Ferreira

Ion Beam Analytical techniques (IBA) using MeV charged particles are powerful techniques for the study of different type of samples in several science fields such as Material Science, microelectronics or biology/biomedicine due to its fine sensitivity, versatility and “non-destructive” characteristics. The possibility of beam focusing and beam scanning adds spatial resolution down to the dm level and imaging capabilities then allowing the IBA techniques to become microscopy techniques.In the Nuclear Microprobe installed at IST/ITN several IBA techniques can be routinely used for materials characterization, the most common ones being PIXE (Particle Induced X-ray Emission), RBS (Rutherford Backscattering Spectrometry) and STIM (Scanning Transmission Ion Microscopy). Whether through their independent or combined use the most important thing of these techniques is the complementary information that they can grant. As any other X-ray spectroscopic technique pPIXE can also provide elemental identification (for Z>12) but further present their spatial distribution in the sample as well as, for thin biological samples (<20 <m), calculate their areal mass density. RBS on the other hand is able to probe sample in depth then allowing obtaining, for instance, elemental depth profile and at the same time sample matrix areal mass density. The combined use of PIXE and RBS then allows determining elemental concentration for thin biological samples. For the mentioned thin biological samples the ion beam energy loss when crossing them (base of the STIM technique), contains information on their density or thickness allowing unique information on its structure and morphology.Advantages and draw backs can always be taken into account when comparing with similar or competitive techniques. This is the case of PIXE and SEM-EDS which is quite unfavorable for PIXE in the case of image spatial resolution, but quite favorable if elemental sensitivity is considered. Due to the much lower X-ray spectrum background, detection limits for PIXE reach the tg/g level.As an example of application, some of the results obtained for PE-g-HEMA films are here shown. To allow their utilization as biomaterials for biomedical applications (e.g. drug delivery) apart from the needed mechanical properties and surface characteristics, biocompatibility of these materials is of fundamental importance. Regarding biocompatibility one important parameter to be assessed is its cytotoxicity that strongly depends on the contamination level at the surface. As shown in Fig. 1, MeV ion beam microscopy not only can provide major and trace element spatial distribution (combining PIXE and RBS data) but also valuable information on its near-surface structure (STIM). Furthermore, quantitative elemental analysis can be performed through the analysis of the PIXE spectra with sensitivity down to the rg/g level as also revealed in Figure 1.V. Corregidor acknowledges the funding support from the FCT-Ciência program.


1993 ◽  
Vol 316 ◽  
Author(s):  
E.D. Specht ◽  
D.A. Walko ◽  
S.J. Zinkle

ABSTRACTAt cryogenic temperatures, the accumulation of vacancy-interstitial pairs in Al2O3 from atomic displacements associated with ion implantation produces amorphization. At room temperature, these pairs recombine, and amorphization occurs only at high doses. X-ray reflectivity measurements show that amorphization of the surface of Al2O3 implanted at room temperature with 160 keV Cr+ ions is preceded by a progressive reduction in near-surface density. Monte Carlo simulations show that this density reduction can be accounted for by high-energy-transfer collisions which knock atoms deep into the target, leaving widely separated vacancies and interstitials, which do not recombine. Electron microscopy shows that at least some of these vacancies condense into voids. We propose that this reduction in near-surface density can lead to amorphization at high doses. We present simple approximations for the density reduction expected for different ions and targets.


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