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Half-Lives of Superheavy Nuclei in Z=113 Alpha Decay Chain
DONG Jian-Min, ZHANG Hong-Fei, ZUO Wei, LI Jun-Qing
Chin. Phys. Lett. 2008, 25 (12):
4230-4232
.
The generalized liquid drop model (GLDM), including the proximity effects and centrifugal potential, and the cluster model with Cosh potential are used to study the half-lives of some Z=113 isotopes and their α-decay products. The experimental half-lives of 284113, 283113, 282113 and their α-decay products are well reproduced by the two models when zero angular momenta transfer is assumed. For 278113 and its α-decay products, both the GLDM and the cluster model could provide satisfactory results if we assume the α particle carry five units of angular momenta, which indicates that possible nonzero angular momenta transfer and need further experimental measurements with high precision. Finally, we show that half-lives of α-decay are quite sensitive to the angular momentum transfers, and a formula could be used to describe the correlation between α-decay half-life and angular momentum transfer successfully.
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Optical Potential Parameters of Weakly Bound Nuclear System 17F+13C
AN Guang-Peng, LIN Cheng-Jian, ZHANG Huan-Qiao, LIU Zu-Hua, YANG Feng, ZHANG Gao-Long, ZHANG Chun-Lei, WU Zhen-Dong, JIA Fei, JIA Hui-Ming, XUXin-Xing, BAI Chun-Lin, YU Ning
Chin. Phys. Lett. 2008, 25 (12):
4237-4239
.
Elastic scattering angular distributions of the 14N+16O system and the angular distributions of transfer reaction 16O(14N,13C)17F at ELab=76.2MeV and 57MeV have been measured and calculated by means of the exact finite-range distorted-wave Born approximation with the PTOLEMY code. The optical potential parameters for the weakly bound nuclear system 17F+13C have been deduced and applied to analyse the elastic scattering angular distributions of the similar systems 17F+12C and 17F+14N which are taken from literature. The result shows that the transfer reaction with stable projectile and target combination can be used as an alternative method to extract the optical potential parameters for the weakly bound nuclear system.
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Interesting Features of n2D Rydberg Series Fine-Structure Splittings along the Sodium-Like Isoelectronic Sequence
WANG Xiao-Lu, LIU Ling-Tao, GAO Xiang, SHEN Chun, LI Jia-Ming,
Chin. Phys. Lett. 2008, 25 (12):
4244-4247
.
Using a simplified multi-configuration Dirac--Fock (SMCDF) scheme based on the multi-configuration Dirac--Fock (MCDF) theory, we study the systematic variations of the fine-structure splittings of n2D3/2,5/2 Rydberg series along the sodium-like isoelectronic sequence, i.e. the fine-structure orderings vary with increasing atomic number Z. The competition between the spin-orbit interactions and the exchange interactions due to relativistic effects of the nd orbital wavefunctions well explain such variations. Furthermore, the effect of Breit interactions which plays the secondary role is studied.
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Semiclassical Calculations of Autoionization Rate for Lithium Atoms in Parallel Electric and Magnetic Fields
LIN Sheng-Lu, ZHOU Hui, XU Xue-You, JIA Zheng-Mao, DENG Shan-Hong
Chin. Phys. Lett. 2008, 25 (12):
4251-4254
.
By using a semiclassical method, we present theoretical computations of the ionization rate of Rydberg lithium atoms in parallel electric and magnetic fields with different scaled energies above the classical saddle point. The yielded irregular pulse trains of the escape electrons are recorded as a function of emission time, which allows for relating themselves to the terms of the recurrence periods of the photoabsorption. This fact turns to illustrate the dynamic mechanism how the electron pulses are stochastically generated. Comparing our computations with previous investigation results, we can deduce that the complicated chaos under consideration here consists of two kinds of self-similar fractal structures which correspond to the contributions of the applied magnetic field and the core scattering events. Furthermore, the effect of the magnetic field plays a major role in the profile of the autoionization rate curves, while the contribution of the core scattering is critical for specifying the positions of the pulse peaks.
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Interaction of O3+ Ions with Al2O3 Nanocapillaries
CHEN Xi-Meng, WANG Jun, WANG Xing-An, SUN Guang-Zhi, CHEN Yi-Feng, XIFa-Yuan, SAHO Jian-Xiong, CUI Ying, DING Bao-Wei, XU Jun-Kui, LOU Feng-Jun, YIN Yong-Zhi, ZHOU Chun-Lin, QIU Xi-Yu
Chin. Phys. Lett. 2008, 25 (12):
4255-4257
.
We investigate angular distributions of the transmitted 60keV and 120keV O3+ ions through nanocapillaries with 50nm diameter and 10μm length. The experimental results are in agreement with the `guiding effect' found by Stolterfoht et al. For different tilted angles of the nanocapillary membrane with respect to the beam, the angular distributions of the transmitted ions are measured by a one-dimensional micro-channel plate (MCP) detector. Moreover, the dependence of this guiding effect on the projectile energy is studied.
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Effects of Pumping Sizes on THz Radiation Based on Ultrashort Light Pulse Optical Rectification for High Spatial Resolution T-Ray Imaging
XU Shi-Xiang, DAI Xiao-Ming, YANG Xiao-Hua, LI Jing-Zhen
Chin. Phys. Lett. 2008, 25 (12):
4262-4265
.
We present our experimental studies on the effects of the pumping sizes on THz radiation based on ultrashort light pulse optical rectification for high spatial resolution T-Ray imaging. Our experiments show that high spatial resolution T-ray imaging requires both thin THz emitter and sample, and rigorous tolerance of the gap between the sample and the emitter, as well as small pumping size which usually much smaller compared with THz wavelength. Such a small pumping size results in dramatic decrease of the THz wave power, which originates from strong diffraction of THz wave, the depolarization of the focused tightly pumping beam, the spatial filtering of the emitter exit-surface, and the strong phase-mismatching between the pumping and the high spatial Fourier components of the THz signal, rather than two-photon absorption
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Interaction of Triply-Dressing Electromagnetically Induced Transparency in Five-level Folding Atomic System
LI Chang-Biao, NIE Zhi-Qiang, ZHANG Wei-Feng, ZHANG Yan-Peng, SONG Jian-Ping, LI Yuan-Yuan, LU Ke-Qing
Chin. Phys. Lett. 2008, 25 (12):
4266-4270
.
We consider a five-level atomic folding system, which involve two kinds of dressing mechanisms (the nested-cascade and the sequential-cascade) in interaction of three-dressing fields, the numerical results show that three-dressing fields are interchangeable under certain conditions, which can be considered as two four-level sub-system configurations a nested-cascade N configuration and a sequential-cascade inverted-Y configuration).
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A Continuously Tunable Erbium-Doped Fibre Laser Using Tunable Fibre Bragg Gratings and Optical Circulator
LIU Peng, , YAN Feng-Ping, LI Jian, WANG Lin, NING Ti-Gang, GONG Tao-Rong, JIAN Shui-Sheng,
Chin. Phys. Lett. 2008, 25 (12):
4276-4279
.
A continuously tunable erbium-doped fibre laser (TEDFL) based on tunable fibre Bragger grating (TFBG) and a three-port optical circulator (OC) is proposed and demonstrated. The OC acts as a 100%-reflective mirror. A strain-induced uniform fibre Bragger grating (FBG) which functions as a partial-reflecting mirror is implemented in the linear cavity. By applying axial strain onto the TFBG, a continuously tunable lasing output can be realized. The wavelength tuning range covers approximately 7.00nm in C band (from 1543.6161 to 1550.3307nm). The side mode suppression ratio (SMSR) is better than 50dB, and the 3dB bandwidth of the laser is less than 0.01nm. Moreover, an array waveguide grating (AWG) is inserted into the cavity for wavelength preselecting, and a 50km transmission experiment was performed using our TEDFL at a 10Gb/s modulation rate.
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Self-Starting Passively Mode-Locked Er3+/Yb3+ Codoped Phosphate Glass All-Fibre Ring Laser
LUO Zhi-Chao, XU Wen-Cheng, SONG Chuang-Xing, LUO Ai-Ping, GAO Yu-Xin, XU Shan-Hui, YANG Zhong-Min, CHEN Wei-Cheng
Chin. Phys. Lett. 2008, 25 (12):
4280-4282
.
A self-starting, passively mode-locked all-fibre ring laser based on the homemade Er3+/Yb3+ codoped phosphate glass fibre is reported. Dual-pump sources were used to achieve the mode-locked operation in the experiment. The fundamental mode-locked pulse repetition rate is 10.67MHz. The pulse duration, assumed as the fit of hyperbolic secant pulse shape, is 5.82ps. We also observe the multi-pulse output of the fibre laser.
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Conical Emission Patterns by Femtosecond Pulses with Different Spectral Bandwidths
LI Yue-Xun, ZENG Zhi-Nan, GE Xiao-Chun, CHEN Xiao-Wei, LI Ru-Xin, XUZhi-Zhan
Chin. Phys. Lett. 2008, 25 (12):
4296-4299
.
Different conical emission (CE) patterns are obtained experimentally at various incident powers and beam sizes of pump laser pulses with pulse durations of 7fs, 44fs and 100fs. The results show that it is the incident power but not the incident power density that determines a certain CE pattern. In addition, the critical powers for similar CE patterns are nearly the same for the laser pulses with the same spectral bandwidth. Furthermore, as far as a certain CE pattern is concerned, the wider the spectral bandwidth of pump laser pulse is, the higher the critical power is. This will hopefully provide new insights for the generation of CE pattern in optical medium.
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Guiding of 60keV O6+ Ions through Nanocapillaries in an Uncoated Al2O3 Membrane
CHEN Xi-Meng, XI Fa-Yuan, QIU Xi-Yu0, SHAO Jian-Xiong, CUI Ying, SUNGuang-Zhi, WANG Jun, CHEN Yi-Feng, LIU Hui-Ping, YIN Yong-Zhi, LOU Feng-Jun, WANG Xing-An, XU Jun-Kui, ZHOU Chun-Lin
Chin. Phys. Lett. 2008, 25 (12):
4348-4351
.
We measure the transmission of O6+ ions with a higher energy of 60 keV (in turn a higher value of Ep/q) through capillaries in an uncoated Al2O3 membrane, and obtain agreements with previously reported results in general angular distribution of the transmitted ions and the transmission profile width variation with capillary tilt angle. The transmission fractions as a function of the tilt angle can be fitted to the semi-empirical Gaussian-like function well. Due to using uncoated capillary membrane, our ψc is larger than that using gold-coated one, in spite of our larger value of Ep/q, which suggests a larger equilibrium charge Q∞ in our experiment.
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Theoretical Study of Compressibility and Thermoelasticity of LaNi5-xAlx (x=0.3, 0.5 and 1.0)
CHEN Dong, XIAO Qi-Min, ZHAO Ying-Lu, XIONG Bao-Ku, YU Ben-Hai, SHI De-Heng
Chin. Phys. Lett. 2008, 25 (12):
4352-4355
.
The compressibility, the temperature dependence of bulk modulus, the pressure dependence of normalized volume V/V0, thermal expansion coefficient and Debye temperature of LaNi5-xAlx compounds are successfully obtained using the first-principles plane-wave pseudopotential (PW-PP) method, the EOSFIT6.0 software and the quasi-harmonic Debye model. The rapid decrease of relative lattice constant a/a0 shows that the deformation is easier in directions normal to the c-axis than that along it. The relationships between bulk modulus B and pressure at different temperatures are also analysed. It is found that the bulk modulus B increases monotonically with increasing pressure. Moreover, the pressure dependences of thermal expansion and Debye temperature are also successfully obtained. The calculated results are in agreement with the experimental data.
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Effect of Nitridation on Morphology, Structural Properties and Stress of AlN Films
HU Wei-Guo, JIAO Chun-Mei, WEI Hong-Yuan, ZHANG Pan-Feng, KANG Ting-Ting, ZHANG Ri-Qing, LIU Xiang-Lin
Chin. Phys. Lett. 2008, 25 (12):
4364-4367
.
We investigate effects of nitridation on AlN morphology, structural properties and stress. It is found that 3min nitridation can prominently improve AlN crystal structure, and slightly smooth the surface morphology. However, 10min nitridation degrades out-of-plane crystal structure and surface morphology instead. Additionally, 3-min nitridation introduces more tensile stress (1.5GPa) in AlN films, which can be attributed to the weaker islands 2D coalescent. Nitridation for 10min can introduce more defects, or even forms polycrystallinity interlayer, which relaxes the stress. Thus, the stress in AlN with 10min nitridation decreases to -0.2GPa compressive stress.
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Achieving Thin Films with Micro/Nano-Scale Controllable Morphology by Glancing Angle Deposition Technique
JIANG Shao-Ji, WANG Chao-Yi, TANG Ji-Jia, HU Lin-Xin
Chin. Phys. Lett. 2008, 25 (12):
4368-4370
.
We demonstrate that thin films with micro/nanometre controllable morphology can be fabricated by the glancing angle deposition (GLAD) technique which is a physical vapour deposition technique. In this technique, there are parameters which determine the morphology of the thin films: the incident angle, ratio of the deposition rate with respect to the substrate rotation rate, nature of the material being deposited, etc. We fabricate the morphology of column, pillar, helices, zigzag and study the parameters which determine morphology by given some examples of SEM.
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Multiple Nodeless Superconducting Gaps in (Ba0.6K0.4)Fe2As2 Superconductor from Angle-Resolved Photoemission Spectroscopy
ZHAO Lin, LIU Hai-Yun, ZHANG Wen-Tao, MENG Jian-Qiao, JIA Xiao-Wen, LIU Guo-Dong, DONG Xiao-Li, CHEN Gen-Fu, LUO Jian-Lin, WANG Nan-Lin, LU Wei, WANG Gui-Ling, ZHOU Yong, ZHU Yong, WANG Xiao-Yang, XU Zu-Yan, CHEN Chuang-Tian, ZHOU Xing-Jiang
Chin. Phys. Lett. 2008, 25 (12):
4402-4405
.
High resolution angle-resolved photoemission measurements have been carried out to study the superconducting gap in the (Ba0.6K0.4)Fe2As2 superconductor with Tc=35 K. Two hole-like Fermi surface sheets around the Γ point exhibit different superconducting gaps. The inner Fermi surface sheet shows larger (10~12 meV) and slightly momentum-dependent gap while the outer one has smaller (7~8meV) and nearly isotropic gap. The lack of gap node in both Fermi surface sheets favours s-wave superconducting gap symmetry. Superconducting gap opening is also observed at the M(π,π) point. The two Fermi surface spots near the M point are gapped below Tc but the gap persists above Tc. The rich and detailed superconducting gap information will provide key insights and constraints in understanding pairing mechanism in the iron-based superconductors.
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Effects of Parameter Modulation on Near-Field Imaging in Photonic Crystal Consisting of Alternately Left-Handed Material and Right-Handed Material
WANG Qiong, YAN Chang-Chun, ZHANG Ling-Ling, CUI Yi-Ping
Chin. Phys. Lett. 2008, 25 (12):
4417-4420
.
By means of the transfer-matrix method, the effects of parameter modulation on the quality of near-field imaging in one-dimensional photonic crystal consisting of alternately left-handed material and right-handed material are investigated. Based on analyses of the recovery rate and phase shift, the results show that the imaging quality is not obviously affected by the minor changes of layer thickness. In addition, by modulating the material parameters of the left-handed material, it is found that for both the real part and the imaginary part, the system is more sensitive to the permeability than the permittivity for the TE wave. For the TM wave, it is reverse. These properties are very useful to fabricate left-handed material photonic crystals in practice.
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Optimized Performances of Thick Film Organic Lighting-Emitting Diodes
WANG Xiu-Ru, ZHANG Zhi-Qiang, MA Dong-Ge, SUN Run-Guang
Chin. Phys. Lett. 2008, 25 (12):
4425-4427
.
The performance of organic light-emitting diodes (OLEDs) with thick film is optimized. The alternative vanadium oxide (V2O5) and N,N'-di(naphthalene-1-yl)-N,N'-diphenyl-benzidine (NPB) layers are used to enhance holes in the emissive region, and 4,7-dipheny-1,10-phenanthroline (Bphen) doped 8-tris-hydroxyquinoline aluminium (Alq3) is used to enhance electrons in the emissive region, thus ITO/V2O5 (8nm)/NPB (52nm)/V2O5 (8nm)/NPB (52nm)/Alq3 (30 and 45nm)/Alq3:Bphen (30wt%, 30 and 45nm)/LiF (1nm)/Al (120nm) devices are fabricated. The thick-film devices show the turn-on voltage of about 3V and the maximal power efficiency of 4.5lm/W, which is 1.46 times higher than the conventional thin-film OLEDs.
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Evolution of Luminescence with Shell's Thickness in Colloidal CdSe/CdS Core/Shell Quantum Dots
LIANG Da-Shun, SHEN Li, WANG Zhi-Bing, CUI Yi-Ping, ZHANG Jia-Yu, YE Yong-Hong
Chin. Phys. Lett. 2008, 25 (12):
4431-4434
.
We synthesize colloidal CdSe/CdS core/shell quantum dots with different shell thicknesses, and there are five samples including CdSe core dots, and CdSe/CdS core/shell dots with 1-4 CdS layers. X-ray diffraction and Raman measurements indicate that the stress in CdSe core becomes stronger with the increasing shell thickness, and the optical measurements show that when the shell becomes thicker, the photoluminescence quantum yield is enhanced, and the radiative decay is also expedited. The temperature-dependent optical spectra are measured. The relation between the microstructure and the optical properties is discussed.
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Sub-diffraction-Limit Imaging in Optical Hyperlens
HU Ji-Gang, , WANG-Pei, LU Yong-Hua, MING Hai, CHEN Chun-Chong, CHEN Jun-Xue,
Chin. Phys. Lett. 2008, 25 (12):
4439-4441
.
Sub-diffraction-limit imaging in the optical hyperlens based on cylindrical metamaterials is studied. Some parameters of hyperlens, such as the dispersive relation and the divergence angle of imaging, are numerically analysed with the ray trajectory method and effective medium theory. The dependence of imaging properties on dielectric constant is discussed. As a result, a 0° divergence angle is obtained for the best imaging effect. This work will be helpful for the design, structure fabrication and resolution improvement of the optical hyperlens.
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Influence of Dopants in ZnO Films on Defects
PENG Cheng-Xiao, WENG Hui-Min, ZHANG Yang, MA Xing-Ping, YE Bang-Jiao
Chin. Phys. Lett. 2008, 25 (12):
4442-4445
.
The influence of dopants in ZnO films on defects is investigated by slow positron annihilation technique. The results show S that parameters meet SAl>Sun>SAg for Al-doped ZnO films, undoped and Ag-doped ZnO films. Zinc vacancies are found in all ZnO films with different dopants. According to S parameter and the same defect type, it can be induced that the zinc vacancy concentration is the highest in the Al-doped ZnO film, and it is the least in the Ag-doped ZnO film. When Al atoms are doped in the ZnO films grown on silicon substrates, Zn vacancies increase as compared to the undoped and Ag-doped ZnO films. The dopant concentration could determine the position of Fermi level in materials, while defect formation energy of zinc vacancy strongly depends on the position of Fermi level, so its concentration varies with dopant element and dopant concentration.
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Growth of Highly Conductive n-Type Al0.7Ga0.3N Film by Using AlN Buffer with Periodical Variation of V / III Ratio
ZHANG Jie, GUO Li-Wei, XING Zhi-Gang, GE Bing-Hui, DING Guo-Jian, PENG Ming-Zeng, JIA Hai-Qiang, ZHOU Jun-Ming, CHEN Hong
Chin. Phys. Lett. 2008, 25 (12):
4449-4452
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High quality and highly conductive n-type Al0.7Ga0.3N films are obtained by using AlN multi-step layers (MSL) with periodical variation of V/III ratios by low-pressure metalorganic chemical vapour deposition (LP-MOCVD). The full-width at half-maximum (FWHM) of (0002) and (10-15) rocking curves of the Si-doped Al0.7Ga0.3N layer are 519 and 625 arcsec, respectively. Room temperature (RT) Hall measurement shows a free electron concentration of 2.9×1019cm-3, and mobility of 17.8cm2V-1s-1, corresponding to a resistivity of 0.0121Ωcm. High conductivity of the Si-doped AlGaN film with such high Al mole fraction is mainly contributed by a remarkable reduction of threading dislocations (TDs) in AlGaN layer. The TD reducing mechanism in AlN MSL growth with periodical variation of V / III ratio is discussed in detail.
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Effect of Aspect Ratio Distribution on Localized Surface Plasmon Resonance Extinction Spectrum of Gold Nanorods
TAO Jun, LU Yong-Hua, ZHENG Rong-Sheng, LIN Kai-Qun, XIE Zhi-Guo, LUO Zhao-Feng, LI Sheng-Li, WANG Pei, MING Hai
Chin. Phys. Lett. 2008, 25 (12):
4459-4462
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Gold nanorods with different aspect ratios are prepared in micells using a seeded growth method. Their extinction spectra are observed with an UV-visible spectrophotometer and analysed theoretically. It is known that there are two plasmon resonance peaks for gold nanorod corresponding to transverse and longitudinal plasmon resonance respectively. Moreover, the longitudinal plasmon resonance peak shifts to long wavelength when we increase the aspect ratio determined from TEM. Especially, we model the extinction spectrum using Gans' theory and compare it with our experimental result. Considering the aspect radios distribution of gold nanorods, it is found that longitudinal plasmon resonance peak will be wider than the nanorods with single aspect ratio, which is consistent with our experimental result. In addition, the effect of dielectric constant of surrounding medium is considered.
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Preparation and Size Characterization of Silver Nanoparticles Produced by Femtosecond Laser Ablation in Water
BIAN Fei, ZHANG Xin-Zheng, WANG Zhen-Hua, WU Qiang, HU Hao, XU Jing-Jun
Chin. Phys. Lett. 2008, 25 (12):
4463-4465
.
Femtosecond laser ablation of silver plate placed in water is used to produce nanoparticle suspension. The method is easy to operate and the suspension is relatively stable. The optical properties and the size distribution of the suspension are studied with UV-vis absorption spectroscopy and dynamic light scattering, respectively. The shape of the nanoparticles is investigated by an atomic force microscope, which is near spherical. There are two kinds of nanoparticles, small particles with diameter about 35nm, and large particles with diameter about 120nm.
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Growth, Antimony Incorporation Behaviour and Beryllium Doping of GaAs1-ySby Grown on GaAs by Molecular Beam Epitaxy
GAO Han-Chao, WANG Wen-Xin, JIANG Zhong-Wei, LIU Jian, YANG Cheng-Liang, WU Dian-Zhong, ZHOU Jun-Ming, CHEN Hong
Chin. Phys. Lett. 2008, 25 (12):
4466-4468
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A series of GaAs1-ySby epilayers are grown on GaAs substrates under different growth conditions. Different antimony compositions of samples with beryllium doping are obtained. A non-equilibrium thermodynamics model is used to calibrate and fit the Sb composition. Activation energy of 0.37eV for the dissociation process of Sb4 molecules is obtained. Carrier mobility and concentration of samples are influenced by the Sb composition. Quasi-qualitative analysis of mobility is used to explain the relations among Sb composition, carrier mobility and concentration. High resolution x-ray diffraction (HRXRD) rocking curves and Hall effects measurements are used to determine the crystal quality, carrier mobility and concentration.
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Synthesis, Characterization of 9,9'-Bianthracene and Fabrication of 9,9'-Bianthracene Field-Effect Transistors
LI Jian-Feng, CHANG Wen-Li, TAO Chun-Lan, OU Gu-Ping, ZHANG Fu-Jia
Chin. Phys. Lett. 2008, 25 (12):
4476-4479
.
We synthesize and purify 9,9'-bianthracene with the purity up to 96.4 %. The electronic and crystallographic structures of 9,9'-bianthracene are studied. The results of a joint experimental investigation based on a combination of x-ray diffraction (XRD) spectra, hydrogen nuclear magnetic (HNMR) spectra, infrared absorption (FT-IR) spectra, and mass spectra (MS) of 9,9'-bianthracene are obtained. The uniform compact film is observed by an atomic-force microscope (AFM). Organic field effect transistors (OFETs) with an active layer based on the synthesized 9,9'-bianthracene are fabricated for the first time. Its field-effect mobility is as large as 0.067cm2/(V12539;s) and the on/off ratio is above 5×104. The result demonstrates that the oligomerization of a small semiconductor molecule is an effective method to develop high-mobility organic semiconductors.
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88 articles
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