Monodomain High-Aspect-Ratio 2D and 3D Ordered Porous Alumina Structures with Independently Controlled Pore Spacing and Diameter

2007 ◽  
Vol 19 (7) ◽  
pp. 988-992 ◽  
Author(s):  
R. Krishnan ◽  
C. V. Thompson
2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Mana Iwai ◽  
Tatsuya Kikuchi ◽  
Ryosuke O. Suzuki

AbstractHigh-aspect ratio ordered nanomaterial arrays exhibit several unique physicochemical and optical properties. Porous anodic aluminum oxide (AAO) is one of the most typical ordered porous structures and can be easily fabricated by applying an electrochemical anodizing process to Al. However, the dimensional and structural controllability of conventional porous AAOs is limited to a narrow range because there are only a few electrolytes that work in this process. Here, we provide a novel anodizing method using an alkaline electrolyte, sodium tetraborate (Na2B4O7), for the fabrication of a high-aspect ratio, self-ordered nanospike porous AAO structure. This self-ordered porous AAO structure possesses a wide range of the interpore distance under a new anodizing regime, and highly ordered porous AAO structures can be fabricated using pre-nanotexturing of Al. The vertical pore walls of porous AAOs have unique nanospikes measuring several tens of nanometers in periodicity, and we demonstrate that AAO can be used as a template for the fabrication of nanomaterials with a large surface area. We also reveal that stable anodizing without the occurrence of oxide burning and the subsequent formation of uniform self-ordered AAO structures can be achieved on complicated three-dimensional substrates.


2016 ◽  
Vol 7 ◽  
pp. 1709-1717 ◽  
Author(s):  
Alla I Vorobjova ◽  
Dmitry L Shimanovich ◽  
Kazimir I Yanushkevich ◽  
Sergej L Prischepa ◽  
Elena A Outkina

The comparative analysis of the electrochemical deposition of Ni and Ni–Fe nanowires (NWs) into ordered porous alumina templates is presented. The method developed allows for obtaining NWs of 50 ± 5 nm in diameter and 25 μm in length, i.e., with an aspect ratio of 500. XRD data demonstrate the polycrystalline nature of Ni and Ni–Fe in a face-centered cubic close-packed lattice. Both fabricated materials, Ni and Ni–Fe, have shown ferromagnetic properties. The specific magnetization value of Ni–Fe NWs in the alumina template is higher than that of the Ni sample and bulk Ni, also the Curie temperature of the Ni–Fe sample (790 K) is higher than that of the Ni sample one or bulk Ni.


2012 ◽  
Vol 5 (1) ◽  
pp. 72-79 ◽  
Author(s):  
Jaime Martín ◽  
Cristina V. Manzano ◽  
Olga Caballero-Calero ◽  
Marisol Martín-González

2014 ◽  
Vol 53 (7) ◽  
pp. 075201 ◽  
Author(s):  
Kazuyuki Nishio ◽  
Suguru Tagawa ◽  
Takashi Yanagishita ◽  
Hideki Masuda

2000 ◽  
Vol 39 (Part 2, No. 10B) ◽  
pp. L1039-L1041 ◽  
Author(s):  
Hideki Masuda ◽  
Masayuki Ohya ◽  
Kazuyuki Nishio ◽  
Hidetaka Asoh ◽  
Masashi Nakao ◽  
...  

RSC Advances ◽  
2021 ◽  
Vol 11 (4) ◽  
pp. 2096-2102
Author(s):  
Takashi Yanagishita ◽  
Tomohiro Hayakawa ◽  
Toshiaki Kondo ◽  
Hideki Masuda

Ni micropillar array with high aspect ratio prepared using anodic porous alumina.


Sensors ◽  
2021 ◽  
Vol 22 (1) ◽  
pp. 172
Author(s):  
Oleg Kameshkov ◽  
Vasily Gerasimov ◽  
Boris Knyazev

Terahertz surface plasmon resonance (SPR) sensors have been regarded as a promising technology in biomedicine due to their real-time, label-free, and ultrasensitive monitoring features. Different authors have suggested a lot of SPR sensors, including those based on 2D and 3D metamaterials, subwavelength gratings, graphene, and graphene nanotube, as well as others. However, one of the traditional approaches to realize high sensitivity SPR sensors based on metal diffraction gratings has been studied poorly in the terahertz frequency range. In this article, a linear metal rectangular diffraction grating with high aspect ratio is studied. The influence of the grating structure parameters on the sensor sensitivity is simulated. Effects arising from different ratios of depth and width were discovered and explained. The results show that the sensitivity can be increased to 2.26 THz/RIU when the refractive index range of the gas to measure is between 1 and 1.002 with the resolution 5×10−5 RIU.


Nano Letters ◽  
2005 ◽  
Vol 5 (8) ◽  
pp. 1603-1606 ◽  
Author(s):  
Anders Johansson ◽  
Erika Widenkvist ◽  
Jun Lu ◽  
Mats Boman ◽  
Ulf Jansson

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