The surface topography of pyrolitic carbons and of gold thin films by scanning tunneling microscopy:grain boundaries and surface defects

Vacuum ◽  
1989 ◽  
Vol 39 (5) ◽  
pp. 526-527
2003 ◽  
Vol 10 (06) ◽  
pp. 903-908 ◽  
Author(s):  
L. L. MELO ◽  
M. C. SALVADORI ◽  
M. CATTANI

We have fabricated gold thin films by metal plasma ion deposition on silicon substrates. The roughness of these nanostructured films has been measured by scanning tunneling microscopy (STM) and we have determined the growth dynamics critical exponents. We have also measured the grain sizes as a function of the film thickness.


2000 ◽  
Vol 648 ◽  
Author(s):  
Jeffrey A. Stultz ◽  
Andrei Kolmakov ◽  
Xiaofeng Lai ◽  
Young Dok Kim ◽  
D. Wayne Goodman

AbstractMgO thin films having different defect densities are explored in this study using metastable impact electron spectroscopy (MIES), ultraviolet photoelectron spectroscopy (UPS), temperature programmed desorption (TPD), and scanning tunneling microscopy (STM). Surface point defects on MgO exhibit themselves in both the MIES and UPS spectra as a feature approximately 2 eV above the valance band, whereas extended defects are only observed spectroscopically as a broadening of the O 2p band. The interaction of NO and N2O with the MgO surface as a function of surface defect density is explored. Upon adsorption on MgO thin films at 100K, both NO and N2O show the development of three features which coincide with a standard gas phase N2O spectrum. The saturation coverage of N2O from NO adsorption increases with increasing defect density, indicating that defect sites are mainly responsible for N2O formation. STM images confirm the increase of thin film defect density upon thermal quenching.


1990 ◽  
Vol 8 (1) ◽  
pp. 459-463 ◽  
Author(s):  
A. D. Kent ◽  
I. Maggio‐Aprile ◽  
Ph. Niedermann ◽  
Ch. Renner ◽  
O/. Fischer

2005 ◽  
Vol 12 (05n06) ◽  
pp. 675-679 ◽  
Author(s):  
M. CATTANI ◽  
M. C. SALVADORI

Platinum and gold thin films have been fabricated by filtered vacuum arc deposition perpendicularly on rough silicon and glass substrates. Four sets of samples have been prepared with different thickness (d). Two sets were very thin films of Pt (1.31 ≤ d ≤ 11.66 nm ) and Au (1.77 ≤ d ≤ 10.46 nm ) and two sets were thicker films also of Pt (7 ≤ d ≤ 80 nm ) and Au (34 ≤ d ≤ 200 nm ). The roughness mean-square ω of the films have been measured, as a function of the film thickness d, by scanning tunneling microscopy (STM). We verified that the dynamical scaling relation ω(t) ~ tβ, where β is the growth exponent, is obeyed for the thicker films but it is not obeyed for the very thin films. These cases are analyzed taking into account the films growth theory.


Molecules ◽  
2021 ◽  
Vol 26 (15) ◽  
pp. 4439
Author(s):  
Shui-Yang Lien ◽  
Yu-Hao Chen ◽  
Wen-Ray Chen ◽  
Chuan-Hsi Liu ◽  
Chien-Jung Huang

In this study, adding CsPbI3 quantum dots to organic perovskite methylamine lead triiodide (CH3NH3PbI3) to form a doped perovskite film filmed by different temperatures was found to effectively reduce the formation of unsaturated metal Pb. Doping a small amount of CsPbI3 quantum dots could enhance thermal stability and improve surface defects. The electron mobility of the doped film was 2.5 times higher than the pristine film. This was a major breakthrough for inorganic quantum dot doped organic perovskite thin films.


2021 ◽  
Vol 724 ◽  
pp. 138598
Author(s):  
Linda AISSANI ◽  
Akram ALHUSSEIN ◽  
Abdelhak AYAD ◽  
Corinne NOUVEAU ◽  
Elia ZGHEIB ◽  
...  

2021 ◽  
Vol 22 (13) ◽  
pp. 6880
Author(s):  
Zilong Wang ◽  
Minlong Tao ◽  
Daxiao Yang ◽  
Zuo Li ◽  
Mingxia Shi ◽  
...  

We report an ultra-high vacuum low-temperature scanning tunneling microscopy (STM) study of the C60 monolayer grown on Cd(0001). Individual C60 molecules adsorbed on Cd(0001) may exhibit a bright or dim contrast in STM images. When deposited at low temperatures close to 100 K, C60 thin films present a curved structure to release strain due to dominant molecule–substrate interactions. Moreover, edge dislocation appears when two different wavy structures encounter each other, which has seldomly been observed in molecular self-assembly. When growth temperature rose, we found two forms of symmetric kagome lattice superstructures, 2 × 2 and 4 × 4, at room temperature (RT) and 310 K, respectively. The results provide new insight into the growth behavior of C60 films.


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