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Multi-site Compact-Like Discrete Breather in Discrete One-Dimensional Monatomic Chains
XU Quan, TIAN Qiang
Chin. Phys. Lett. 2007, 24 (12):
3351-3355
.
Multi-site compact-like discrete breathers in discrete one-dimensional monatomic chains are investigated by discussing a generalized discrete one-dimensional monatomic model. We obtain that the two-site compact-like discrete breathers with codes σ ={ 0,... ,0,1,1,0,... ,0} and codes σ={0,... , 0,1,-1,0,... ,0} can exist in discrete one-dimensional monatomic chain with quartic on-site and inter-site potentials. However, the former can only exist in hard quartic on-site potential and cannot exist in soft quartic on-site potential, whereas the latter is just reversed. All of the two-site Compact-like discrete breathers with codes σ.={0,....,0,1,1,0,.... ,0} and σ ={0,... , 0,1,-1,0, .... ,0} cannot exist in a pure K4 chain.
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Design, Fabrication and Measurement of Ni/Ti Multilayer Used for Neutron Monochromator
ZHANG Zhong, WANG Zhan-Shan, ZHU Jing-Tao, WU Yong-Rong, MU Bao-Zhong, WANG Feng-Li, QIN Shu-Ji, CHEN Ling-Yan
Chin. Phys. Lett. 2007, 24 (12):
3365-3357
.
Ni/Ti multilayers, which can be used for neutron monochromators, are designed, fabricated and measured. Firstly, their reflectivities are simulated based on the Nevot--Croce model. Reflectivities of two Ni/Ti multilayer mirrors with periods d=10.3nm (M1) and d=7.8nm (M2) are calculated. In the calculation, the reflectivity of the Ni/Ti multilayer is taken as a function of the grazing angle with different roughness factors δ=1.0nm and delta=1.5nm. Secondly, these two multilayers are fabricated by the direct current magnetron sputtering technology. Thirdly their structures are characterized by small-angle x-ray diffraction. The roughness factors are fitted to be 0.68nm and 1.16nm for M1 and M2, respectively. Finally their reflective performances are measured on the V14 neutron beam line at the Berlin Neutron Scattering Centre (BENSC), Germany. The experimental data show that the grazing angle of the reflected neutron intensity peak increases, but the reflected neutron intensity decreases, with the decreasing periods of the multilayers.
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Angular Dispersion and Deflection Function for Heavy Ion Elastic Scattering
BAI Zhen, WANG Qi, HAN Jian-Long, XIAO Zhi-Gang, XU Hu-Shan, SUN Zhi-Yu, HU Zheng-Guo, ZHANG Xue-Ying, WANG Hong-Wei, MAO Rui-Shi, YUAN Xiao-Hua, XU Zhi-Guo, ZHANG Hong-Bin, XU Hua-Gen, QIHui-Rong, WANG Yue, JIA Fei, WU Li-Jie, DING Xian-Li, GAO Qi, GAO Hui, LI Song-Lin, LI Jun-Qing, ZHANG Ya-Peng, XIAO Guo-Qing, JIN Gen-Ming, REN Zhong-Zhou, ZHOU Shan-Gui, XU Wang, Fan Gong-Tao, ZHANG Shuang-Quan, PANG Dan-Yang, SERGEY Yu-Kun,
Chin. Phys. Lett. 2007, 24 (12):
3384-3387
.
The differential cross sections for elastic scattering products of 17F on 208Pb have been measured. The angular dispersion plots of ln(dσ/dθ) versus θ2 are obtained from the angular distribution of the elastic scattering differential cross sections. Systematical analysis on the angular dispersion for the available experimental data indicates that there is an angular dispersion turning angle at forward angular range within the grazing angle. This turning angle can be clarified as nuclear rainbow in classical deflection function. The exotic behaviour of the nuclear rainbow angle offers a new probe to investigate the halo and skin phenomena.
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Phenomenological Scaling of Rapidity Dependence for Anisotropic Flows in 25MeV/nucleon Ca+Ca by Quantum Molecular Dynamics Model
YAN Ting-Zhi, MA Yu-Gang, CAI Xiang-Zhou, FANG De-Qing, LUGuang-Cheng, SHEN Wen-Qing, TIAN Wen-Dong, WANG Hong-Wei, WANG Kun
Chin. Phys. Lett. 2007, 24 (12):
3388-3391
.
Anisotropic flows (v1, v2, v3 and v4) of light fragments up to the mass number 4 as a function of rapidity are studied for 25MeV/nucleon 40Ca + 40Ca at large impact parameters by a quantum molecular dynamics model. A phenomenological scaling behaviour of rapidity dependent flow parameters vn (n = 1, 2, 3 and 4) is found as a function of mass number plus a constant term, which may arise from the interplay of collective and random motions. In addition, v4v22 keeps to be almost independent of rapidity and remains a rough constant of 1/2 for all light fragments.
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Effects of Configuration Interaction on Dielectronic Recombination of Cu-Like Gold Ion through 3d+ e →4l'l'' Capture Process
MENG Fan-Chang, CHEN Chong-Yang, WANG Yan-Shen, ZOU Ya-Ming,
Chin. Phys. Lett. 2007, 24 (12):
3404-3407
.
Effects of configuration interaction on dielectronic recombination of Cu-like gold ions through the 3d+e → 4l'4l'' capture process are studied in the models of isolated configurations approximation, configuration mixing within 3d94s4l'4l'', and configuration mixing within 3d94l4l'4l'' (l≥0), employing a relativistic distorted-wave approximation. Nonresonant raditive stabilizing transitions and decays to autoionizing levels followed by radiative cascades, as well as resonant stabilizing transitions from the resonant levels, are taken into account. The additional mixing with 3d94l4l'4l'' (0<l≤ l'≤l''3) shifts slightly the peaks of cross section towards low energy. The rate coefficient at low temperature is dramatically changed. The rate coefficient at temperature above 100eV is enhanced by a factor between 26% and 13%.
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Interactions of Three Dual-Dressing Effects of Four-Wave Mixing in a Five-Level Atomic System
LI Pei-Zhe, NIE Zhi-Qiang, ZHANG Yan-Peng, JIANG-Tong, DU Yi-Gang, GAN Chen-Li, SONG Jian-Ping, LU Ke-Qing
Chin. Phys. Lett. 2007, 24 (12):
3420-3423
.
We study the four-wave mixing (FWM) in an opening five-level system with two dressing fields. There are three kinds of doubly dressing mechanisms (parallel cascade, sequential cascade, and nested cascade) in the system for doubly dressed four-wave mixing. These mechanisms reflect different correlations between two dressing fields and different effects of two dressing fields to the FWM. Investigation of these mechanisms is helpful to understand the generated high-order nonlinear optical signal dressed by multi-fields.
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(Ti,Al)N Film on Normalized T8 Carbon Tool Steel Prepared by Pulsed High Energy Density Plasma Technique
LIU Yuan-Fu, DENG Fu-Ping, HAN Jian-Min, XU Xiang-Yang, YANG Si-Ze, LIU Xiu-Bo
Chin. Phys. Lett. 2007, 24 (12):
3469-3472
.
Under optimized operating parameters, a hard and wear resistant (Ti,Al)N film is prepared on a normalized T8 carbon tool steel substrate by using pulsed high energy density plasma technique. Microstructure and composition of the film are analysed by x-ray diffraction, x-ray photoelectron spectroscopy, Auger electron spectroscopy and scanning electron microscopy. Hardness profile and tribological properties of the film are tested with nano-indenter and ring-on-ring wear tester, respectively. The tested results show that the microstructure of the film is dense and uniform and is mainly composed of (Ti,Al)N and AlN hard phases. A wide transition interface exists between the film and the normalized T8 carbon tool steel substrate. Thickness of the film is about 1000nm and mean hardness value of the film is about 26GPa. Under dry sliding wear test conditions, relative wear resistance of the (Ti,Al)N film is approximately 9 times higher than that of the hardened T8 carbon tool steel reference sample. Meanwhile, the (Ti,Al)N film has low and stable friction coefficient compared with the hardened T8 carbon tool steel reference sample.
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Structural and Magnetic Properties of Codoped ZnO based Diluted Magnetic Semiconductors
LI Bin-Bin, SHEN Hong-Lie, ZHANG Rong, XIU Xiang-Qiang, XIE Zhi
Chin. Phys. Lett. 2007, 24 (12):
3473-3476
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Zn1-xCoxO (x=0.01, 0.02, 0.05, 0.10 and 0.20) diluted magnetic semiconductors are prepared by the sol-gel method. The structural and magnetic properties of the samples are studied using x-ray diffraction (XRD), extended x-ray absorption fine structure (EXAFS) and superconducting quantum interference device (SQUID). The XRD patterns does not show any signal of precipitates that are different from wurtzite type ZnO when Co content is lower than x=0.10. An EXAFS technique for the Co K-edge has been employed to probe the local structures around Co atoms doped in ZnO powders by fluorescence mode. The simulation results for the first shell EXAFS signals indicate that Zn sites can be substituted by Co atoms when Co content is lower than x=0.05. The SQUID results show that the samples (x<0.05) exhibit clear hysteresis loops at 300K, and magnetization versus temperature from 5K to 350K at H=100,Oe for the sample x=0.02 shows that the samples have ferromagnetism above room temperature. A double-exchange mechanism is proposed to explain the ferromagnetic properties of the samples.
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Disc-Capped ZnO Nanocombs
LI Xin, XU Chun-Xiang, ZHU Guang-Ping, YANG Yi, LIU Jin-Ping, SUN Xiao-Wei, CUI Yi-Ping
Chin. Phys. Lett. 2007, 24 (12):
3495-3498
.
Nanocombs with a disc cap structure of ZnO have been synthesized on Si substrates by using pure Zinc powders as the source materials based on a vapour-phase transport process. The morphology and the microstructure are investigated by a scanning electron microscopy and x-ray diffraction. Based on the transmission electron microscopy and selected area electron diffraction analysis, the growth directions of three representative parts, nanoribbon stem, nanorod branch and nanodisc cap of the nanocomb are revealed. The growth mechanism of the disc-capped nanocombs is discussed based on the self-catalyzed vapour-liquid-solid process.
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Codoping of Potassium and Bromine in Carbon Nanotubes: A Density Functional Theory Study
XIAO Yang, YAN Xiao-Hong, DING Jian-Wen
Chin. Phys. Lett. 2007, 24 (12):
3506-3508
.
We investigate the co-doping of potassium and bromine in single-walled carbon nanotubes (SWCNTs) and double-walled carbon nanotubes (DWCNTs) based on density functional theory. In the co-doped (6,0) SWCNTs, the 4s electron of potassium is transferred to nanotube and Br, leading to the n-type feature of SWCNTs. When potassium is intercalated into inner tube and bromine is put on outer tube, the positive and negative charges reside on the outer and inner tubes of the (7,0)@(16,0) DWCNT, respectively. It is expected that DWCNTs would be an ideal candidate for p--n junction and diode applications.
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Influences of Pressure and Substrate Temperature on Epitaxial Growth of γ-Mg2SiO4 Thin Films on Si Substrates
KANG Lin, GAO Ju, XU Hua-Rong, ZHAO Shao-Qi, CHEN Hong, WU Pei-Heng
Chin. Phys. Lett. 2007, 24 (12):
3528-3531
.
An epitaxial γ-Mg2SiO4 thin film can be a good buffer between the Si ubstrate and some oxide thin films. For high temperature superconducting multilayer structures, hopefully it can be taken as an insulating layer to replace the widely used MgO film. To explore such possibilities, we carry out systematic studies on the influences of pressure and substrate temperature on the epitaxy of γ-Mg2SiO4 thin films grown on Si (100) substrates using rf magnetron sputtering with an Mg target of purity of 99.95 percent. With the substrate temperature kept at 500°C and the pressure changing from 10Pa to 15Pa, in the XRD spectra the γ-Mg2SiO4 (400) peak grows drastically while the MgO (200) peak is suppressed. Keeping the pressure at 15Pa and increasing the temperature from 500°C to 570°C further can improve the film epitaxy, while working at 780°C and 11Pa seems to give very good results. X-ray photoelectronic spectroscopy and Ф scan are used to characterize the stoichiometry, crystallinity, and in-plane growth of the samples.
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Phase Transition and High Piezoactivity of Sb Doped (Na0.53K0.435Li0.035)Nb0.94Ta0.06O3 Lead-Free Ceramics
QI Peng, WANG Jin-Feng, MING Bao-Quan, WANG Chun-Ming, LIANG Xing-Hua
Chin. Phys. Lett. 2007, 24 (12):
3535-3538
.
Lead-free piezoelectric ceramics with the composition of (Na0.53K0.435Li0.035)Nb0.94-xSbxTa0.06O3 (NKLNST) are synthesized by a conventional solid-state sintering process. An MPB-like region between orthorhombic and pseudocubic phases is found in this system. The density, piezoelectric and dielectric properties are enhanced greatly in this region. A composition (Na0.53K0.435Li0.035) (Nb0.86Sb0.08Ta0.06)O3 is found to have excellent electrical properties: d33=320pC/N, kp=49% and kt=43%, as well as relatively low loss, tan δ=4.2%, and high relative density higher than 96%, which indicate that this ceramics is a promising lead-free piezoceramics replacing for lead zirconate titanate.
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Polymer White-Light-Emitting Diodes with High Work Function Cathode Based on a Novel Phosphorescent Chelating Copolymer
XIONG Yan, ZHANG Yong, ZHOU Jian-Lin, PENG Jun-Biao, HUANG Wen-Bo, CAO Yong
Chin. Phys. Lett. 2007, 24 (12):
3547-3550
.
Polymer white-light-emitting diodes are fabricated based on the blend of poly[9,9-di-(2-% ethylhexyl)-fluorenyl-2,7-diyl]-end capped with polysilsesquioxane (PFO) and a chelating copolymer of poly[(9,9-bis(3'-(N,N-dimethylamino) propyl)-2,7-fluorene-alt-2,7-(9,9-dioctylfluorene))-co- [2,7-(9,9-dioctlyfluorene)-alt-5,5-bis(2-(4-methyl-1-naphtha-lene) pyridine-C2,N) iridium (III) acethylacetonate]] (PFN-NaIr). The device with the sole aluminium cathode is able to produce a comparably white electroluminescence efficiency of 1.31cd/A to that of the device using low work function cathodes (such as Ba, Ca, etc.). The CIE coordinates of the white light emission consisting of red, green and blue three components are nearly at (0.34, 0.35). The mechanism of the white light emission from the device with the Al cathode is investigated, which is related to the efficient injection of electrons through the interface of PFN-NaIr/Al.
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Effect of Crucibles on Qualities of Self-Seeded Aluminium Nitride Crystals Grown by Sublimation
HAN Qi-Feng, DUAN Cheng-Hong, QIU Kai, JI Chang-Jian, LI Xin-Hua, ZHONG Fei, YIN Zhi-Jun, CAO Xian-Cun, ZHOU Xiu-Ju, WANG Yu-Qi
Chin. Phys. Lett. 2007, 24 (12):
3555-3558
.
Self-seeded aluminium nitride (AlN) crystals are grown in tungsten and hot pressed boron nitride (HPBN) crucibles with different shapes by a sublimation method. The qualities of the AlN crystals are characterized by high-resolution transmission electronic microscopy (HRTEM), scanning electron microscopy (SEM) and Micro-Raman spectroscopy. The results indicate that the better quality crystals can be collected in conical tungsten crucible.
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Effect of Annealing Temperature on Electrical Properties of Ferroelectric Bi3.25La0.75Ti3O12 Capacitors
YAN Zheng, ZHANG Wei-Tao, WANG Yi, ZHANG Xin, LI Li, ZHAO Qing-Xun, DU Jun, LIU Bao-Ting
Chin. Phys. Lett. 2007, 24 (12):
3559-3562
.
Lanthanum-modified bismuth titanate (Bi3.25La0.75Ti3O12, BLT) thin films are fabricated on platinized Si wafers by the sol-gel method, and the effect of annealing temperatures ranging from 650°C to 800°C on the electrical properties of Pt/BLT/Pt capacitors are investigated. It is found that polarization and leakage current of BLT capacitors strongly depend on the annealing temperature although all the capacitors demonstrate very similar characteristics, except the value of polarization, in pulse-width dependence, retention, and fatigue. Remanent polarization increases with the increase of annealing temperature, and annealing temperature of 700°C can yield the largest remanent polarization, and then polarization decreases with increasing annealing temperature. For the 700°C annealed Pt/BLT/Pt capacitor, the remanent polarization 2Pr and the coercive field 2Ec, at an electric field of 226kV/cm, are 23.8μC/cm2 and 130kV/cm, respectively. Dielectric breakdown voltages of BLT films annealed at 750°C and 800°C are much lower than those annealed at 650°C and 700°C. At 100kV/cm, the leakage currents of BLT films prepared at 650°C and 700°C are only 1.5×10-6A/cm2 and 8.9×10-7A/cm2, espectively. Moreover, all the Pt/BLT/Pt capacitors exhibit excellent retention properties after a cumulative time of 1× m 104s and do not show any significant fatigue up to 1×1010 switching cycles at frequency of 1MHz.
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Effects of Different Dispersion Methods on the Microscopical Morphologyof TiO2 Film
LAN Xiao-Hua, YANG Shu-Qin, ZOU Yu, WANG Zhi-An, HUANG Ning-Kang
Chin. Phys. Lett. 2007, 24 (12):
3567-3569
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Nanocrystalline porous TiO2 films were prepared on conducting glass supports (ITO) by processed commercial TiO2 nanometre powder (P25). Three methods of physical dispersing for TiO2 powder, i.e. grinding, magnetic stirring, sonicleaning, were used to disperse TiO2 nanometre powder. Surface morphologies of TiO2 films were observed by optic-microscope and SEM. It is found that the surface morphologies of TiO2 films are determined not only by the dispersing methods but also by the percentage of TiO2 powder in the dispersing system. Different film morphologies can be obtained under the same preparation condition but with different dispersing methods. A lot of cracks exist on the film surface for which the TiO2 slurry is dispersed by grinding. Magnetic stirring leads to some white points and micro-holes on the film surface. Only a few of micro-holes can be observed on the film surface, in which the TiO2 slurry is dispersed by sonicleaning. Different surface morphologies can also be found with different thicknesses of TiO2 films. Different film thicknesses are due to different percentages of TiO2 powder in the slurry. The related mechanism leading to different features of the surface morphologies for the TiO2 films is discussed.
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Transport Properties of Binary Clusters
WAN Hai-Qing, ZHOU Yan-Hong, XU Ying
Chin. Phys. Lett. 2007, 24 (12):
3570-3573
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We present first-principles studies on the transport properties of small silicon and aluminium clusters: Al2, Si2, Al4 and AlSi sandwiched between two Al (100) electrodes. The variation of the equilibrium conductance as a function of contact distance for these two-probe systems is probed. Our results show that the transport properties are dependent on both the specific nanostructure and the separation distance between the central molecule and the electrodes. For equilibrium transport properties, the clusters with the similar structure show similar transmission spectra at large distances, the small difference can be explained by the electron filling. For current-voltage characteristics, all the clusters show the metallic behaviour at lower bias, however very different non-linear behaviour can be observed at higher bias. For AlSi and Al2, when the distance between the central cluster and the electrodes is 3.5AA, large negative differential resistance (NDR) can be found in the bias range 0.8V~1.4\,V.
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81 articles
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