True Atomic Resolution Imaging on Semiconductor Surfaces with Noncontact Atomic Force Microscopy

1996 ◽  
Vol 442 ◽  
Author(s):  
Y. Sugawara ◽  
H. Ueyama ◽  
T. Uchihashi ◽  
M. Ohta ◽  
Y. Yanase ◽  
...  

AbstractThe constant vibration mode and the constant excitation mode in noncontact atomic force microscopy were compared to investigate the force interaction between tip and surface. As a result, we found that the constant excitation mode is much more gentle than the constant vibration mode. We also succeeded in atomic resolution imaging on InP(110) surface not only in the noncontact region but in the contact region for the first time. Furthermore, we found the discontinuity of the force gradient curve on reactive Si(111)7×7 reconstructed surface. We proposed a model to explain the discontinuity with the crossover between the physical and chemical bonding interaction.

2000 ◽  
Vol 39 (Part 2, No. 2A) ◽  
pp. L113-L115 ◽  
Author(s):  
Kousuke Yokoyama ◽  
Taketoshi Ochi ◽  
Akira Yoshimoto ◽  
Yasuhiro Sugawara ◽  
Seizo Morita

1997 ◽  
Vol 113-114 ◽  
pp. 364-370 ◽  
Author(s):  
Yasuhiro Sugawara ◽  
Hitoshi Ueyama ◽  
Takayuki Uchihashi ◽  
Masahiro Ohta ◽  
Seizo Morita ◽  
...  

1997 ◽  
Vol 04 (05) ◽  
pp. 1025-1029 ◽  
Author(s):  
R. LÜTHI ◽  
E. MEYER ◽  
M. BAMMERLIN ◽  
A. BARATOFF ◽  
L. HOWALD ◽  
...  

In this note we report the first observation of salient features of the Si(111)(7×7) reconstructed surface across monatomic steps by dynamic atomic force microscopy (AFM) in ultrahigh vacuum (UHV). Simultaneous measurements of the resonance frequency shift Δf of the Si cantilever and of the mean tunneling current [Formula: see text] from the cleaned Si tip indicate a restricted range for stable imaging with true atomic resolution. The corresponding characteristics vs. distance reveal why feedback control via Δf is problematic, whereas it is as successful as in conventional STM via [Formula: see text]. Furthermore, local dissipation (energy loss of 10-14 W) through individual atoms is observed and explained by the coupling of the surface atoms to phonons.


2016 ◽  
Vol 27 (41) ◽  
pp. 415709 ◽  
Author(s):  
John Tracey ◽  
Keisuke Miyazawa ◽  
Peter Spijker ◽  
Kazuki Miyata ◽  
Bernhard Reischl ◽  
...  

2012 ◽  
Vol 51 (8S3) ◽  
pp. 08KB09 ◽  
Author(s):  
Yuki Araki ◽  
Katsuo Tsukamoto ◽  
Noriaki Oyabu ◽  
Kei Kobayashi ◽  
Hirofumi Yamada

2002 ◽  
Vol 188 (3-4) ◽  
pp. 272-278 ◽  
Author(s):  
S. Araragi ◽  
A. Yoshimoto ◽  
N. Nakata ◽  
Y. Sugawara ◽  
S. Morita

2020 ◽  
Vol 11 ◽  
pp. 443-449
Author(s):  
Daiki Katsube ◽  
Shoki Ojima ◽  
Eiichi Inami ◽  
Masayuki Abe

The structure of the rutile TiO2(110)-(1 × 2) reconstructed surface is a phase induced by oxygen reduction. There is ongoing debate about the (1 × 2) reconstruction, because it cannot be clarified whether the (1 × 2) structure is formed over a wide area or only locally using macroscopic analysis methods such as diffraction. We used non-contact atomic force microscopy, scanning tunneling microscopy, and low-energy electron diffraction at room temperature to characterize the surface. Ti2O3 rows appeared as bright spots in both NC-AFM and STM images observed in the same area. High-resolution NC-AFM images revealed that the rutile TiO2(110)-(1 × 2) reconstructed surface is composed of two domains with different types of asymmetric rows.


Sign in / Sign up

Export Citation Format

Share Document