Room-Temperature Reaction between Laser Chemical Vapor Deposited Selenium and Some Metals

2004 ◽  
Vol 16 (18) ◽  
pp. 3439-3445 ◽  
Author(s):  
Akihiko Ouchi ◽  
Zdeněk Bastl ◽  
Jaroslav Boháček ◽  
Hideo Orita ◽  
Koji Miyazaki ◽  
...  
ChemInform ◽  
2004 ◽  
Vol 35 (44) ◽  
Author(s):  
Akihiko Ouchi ◽  
Zdenek Bastl ◽  
Jaroslav Bohacek ◽  
Hideo Orita ◽  
Koji Miyazaki ◽  
...  

2016 ◽  
Vol 2016 ◽  
pp. 1-6 ◽  
Author(s):  
W. J. Liu ◽  
L. Chen ◽  
P. Zhou ◽  
Q. Q. Sun ◽  
H. L. Lu ◽  
...  

We demonstrated a flash memory device with chemical-vapor-deposited graphene as a charge trapping layer. It was found that the average RMS roughness of block oxide on graphene storage layer can be significantly reduced from 5.9 nm to 0.5 nm by inserting a seed metal layer, which was verified by AFM measurements. The memory window is 5.6 V for a dual sweep of ±12 V at room temperature. Moreover, a reduced hysteresis at the low temperature was observed, indicative of water molecules or −OH groups between graphene and dielectric playing an important role in memory windows.


2011 ◽  
Vol 1282 ◽  
Author(s):  
Shuji Kiyohara ◽  
Masaya Kumagai ◽  
Yoshio Taguchi ◽  
Yoshinari Sugiyama ◽  
Yukiko Omata ◽  
...  

ABSTRACTWe have investigated the nanopatterning of chemical vapor deposited (CVD) diamond films in room-temperature nanoimprint lithography (RT-NIL), using a diamond nanodot mold. We have proposed the use of polysiloxane as an electron beam (EB) mask and RT-imprint resist materials. The diamond molds of cylinder dot using the RT-NIL process were fabricated with polysiloxane oxide mask in EB lithography technology. The dot in minimum diameter is 500 nm. The pitch between the dots is 2 μm, and dot has a height of about 600 nm. It was found that the optimum imprinting conditions for the RT-NIL : time from spin-coating to imprinting t1 of 1 min , pressure time t2 of 5 min, imprinting pressure P of 0.5 MPa. The imprint depth obtained after the press under their conditions was 500 nm. We carried out the RT-NIL process for the fabrication of diamond nanopit arrays, using the diamond nanodot molds that we developed. The resulting diamond nanopit arrays with 500 nm-diameter and 200 nm-depth after the electron cyclotron resonance (ECR) oxygen ion beam etching were fabricated. The diameter of diamond nanopit arrays was in good agreement with that of the diamond nanodot mold.


2017 ◽  
Vol 404 ◽  
pp. 357-363 ◽  
Author(s):  
Yotsarayuth Seekaew ◽  
Ditsayut Phokharatkul ◽  
Anurat Wisitsoraat ◽  
Chatchawal Wongchoosuk

2012 ◽  
Vol 1395 ◽  
Author(s):  
Shuji Kiyohara ◽  
Chigaya Ito ◽  
Ippei Ishikawa ◽  
Hirofumi Takikawa ◽  
Yoshio Taguchi ◽  
...  

ABSTRACTWe have proposed the use of glass-like carbon (GC), as mold material because the 27-maximum etching selectivity of polysiloxane film against GC, which was approximately sixtimes larger than that of polysiloxane film against chemical vapor deposited (CVD) diamond film. We have investigated the fabrication of diamond nanopit arrays by room-temperature curing nanoimprint lithography (RTC-NIL) using GC mold, as applications to the emitter and the micro-gear. The polysiloxane has in the state of sticky liquid at room-temperature and negative-exposure characteristic. Therefore, the polysiloxane was used as RTC-imprint resist material, and also used as electron beam (EB) resist (oxide mask) material in EB lithography. We have fabricated the cylindrical GC nanodot mold with 500 nm-diameter, 600 nm-height and 2 μm-pitch. We carried out RTC-NIL using GC mold under the following optimum conditions: time from spin-coating to imprint of 1 min, imprinting pressure of 0.5 MPa and imprinting time of 5min. Then, we have processed the diamond film with an electron cyclotron resonance (ECR) oxygen ion shower. We have fabricated diamond nanopit array with 250 nm-depth and 500 nm-diameter. The diameter of diamond nanopit pattern was in good agreement with that of GC mold. Moreover, the depth of the diamond nanopit patterns fabricated by RTC-NIL using cylindrical GC mold was three times larger than that using conical diamond mold.


2004 ◽  
Vol 828 ◽  
Author(s):  
S. G. Wang ◽  
P. J. Sellin ◽  
A. Lohstroh ◽  
M. E. Özsan

ABSTRACTWe report a study of pulse shapes of a radiation detector with a sandwich structure fabricated from chemical vapor deposited (CVD) polycrystalline diamond. The pulse shapes were recorded at room temperature using 5.486 MeV alpha particles from 241Am source. Only “fast” component was observed in the electron predominated pulses, whereas both “fast” and “slow” components were obtained in the hole predominated pulses, suggesting that electron charge drift is prompt and no detrapping occurred. In contrast, hole charge drift is slower than expected and trapping-detrapping took place during hole travel process.


1995 ◽  
Vol 391 ◽  
Author(s):  
Jin Lee ◽  
Qing Ma ◽  
Thomas Marieb ◽  
Anne S. Mack ◽  
Harry Fujimoto ◽  
...  

AbstractWe have studied stress states in chemical vapor deposited (CVD) tungsten (W) for both blanket films and lines, to understand better the mechanical implications of intrinsic stress for interconnection structures. Since W has a low mobility at its deposition temperature, a very large intrinsic stress develops during deposition. Intrinsic strains in blanket W films were measured with an X-ray technique. The measured strains correspond to a biaxial tensile stress of the order of 1 GPa. This result was used to provide an initial strain input in a finite element calculation to obtain intrinsic stress states in W lines. SEM observation of cross sections of the metal lines enabled us to determine the growth pattern of the W, and infer the boundary conditions during growth. Finite Element Method (FEM) calculations of the room temperature stress in the lines, including both intrinsic and thermal components, are in good agreement with X-ray determinations.


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