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Negative and Superluminal Group Velocity Propagation with Narrow Pulse in a Coaxial Photonic Crystal
OU Xiao-Juan, ZHOU Wei, LI Lin, TENG Li-Hu, FENG Bao-Ying, ZHENG Sheng-Feng, WANG Feng-Wei
Chin. Phys. Lett. 2007, 24 (3):
624-627
.
We investigate the propagation of electric signal along a spatially periodic impedance mismatched transmission line group. Anomalous dispersion is caused by the periodically mismatched impedance structure and a forbidden band appears near 8MHz in transmission. The group velocity of the amplitude-modulated signal is augmented up to infinity, even -3.89c (c the speed of light in vacuum) in the forbidden region with the amplitude of the modulated signal increasing. When the carrier sinusoid signal is modulated in amplitude by the modulating sinusoid signal, of which the peak is superimposed with a narrow pulse at fivefold frequency, the superluminal group velocity also occurs. The experiment failed to show whether the propagation velocity of narrow pulse exceeds c or not.
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Rhythm Synchronization of Coupled Neurons with Temporal Coding Scheme
SHI Xia, LU Qi-Shao
Chin. Phys. Lett. 2007, 24 (3):
636-639
.
Encoding information by firing patterns is one of the basic neural functions, and synchronization is important collective behaviour of a group of coupled neurons. Taking account of two schemes for encoding information (that is, rate coding and temporal coding), rhythm synchronization of coupled neurons is studied. There are two types of rhythm synchronization of neurons: spike and burst synchronizations. Firstly, it is shown that the spike synchronization is equivalent to the phase synchronization for coupled neurons. Secondly, the similarity function of the slow variables of neurons, which have relevant to the bursting process, is proposed to judge the burst synchronization. It is also found that the burst synchronization can be achieved more easily than the spike synchronization, whatever the firing patterns of the neurons are. Hence the temporal encoding scheme, which is closely related to both the spike and burst synchronizations, is more comprehensive than the rate coding scheme in essence.
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Structures of Light Neutron-Rich Nuclei with Orbit--Orbit Coupling
GUO Yan-Qing, REN Zhong-Zhou,
Chin. Phys. Lett. 2007, 24 (3):
652-655
.
The properties of N=7, 8, 9 isotones with Z=4-8 are studied in the framework of the single-particle shell model. A tentative orbit--orbit coupling is introduced in the average nuclear potential. Calculations give a unified description of the structures of N=7,8,9 isotones. The neutron level inversion in N=7 and N=9 isotones is discussed. The ground-state level inversion in 11Be and 15C is reproduced. The inversion between 2s 1/2 and 1d 5/2 neutron levels in 14B and 13Be is predicted. The possible halo structures in N=7 and N=9 isotones are analysed. The numerical results confirm the one-neutron halo structures in 11Be(2s 1/2), 11Be(1p 1/2), 12B(2s 1/2), 13C(2s1/2),14B(2s1/2) and 15C(2s1/2). The study implies that the attempt of considering orbit--orbit interaction in the shell model may be a feasible way to explain the anomalous properties of exotic light nuclei.
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Sensitive Probe for Symmetry Potential
LIU Jian-Ye, , XIAO Guo-Qing, GUO Wen-Jun, REN Zhong-Zhou, ZUO Wei, LEE Xi-Guo,
Chin. Phys. Lett. 2007, 24 (3):
660-663
.
Based on both very obvious isospin effect of the neutron--proton number ratio of nucleon emissions (n/p) nucl on symmetry potential and (n/p) nucl's sensitive dependence on symmetry potential in the nuclear reactions induced by halo-neutron projectiles, compared to the same mass stable projectile, probing symmetry potential is investigated within the isospin-dependent quantum molecular dynamics with isospin and momentum-dependent interactions for different symmetry potentials U1sym and U2 sym. It is found that the neutron-halo projectile induces very obvious increase of (n/p) nucl and strengthens the dependence of (n/p) nucl on the symmetry potential for all the beam energies and impact parameters, compared to the same mass stable projectile under the same incident channel condition. Therefore (n/p) nucl induced by the neutron-halo projectile is a more favourable probe than the normal neutron-rich and neutron-poor projectiles for extracting the symmetry potential.
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Motional Stark Effect and Its Active Cancellation in Diamagnetic Spectrum of Barium
QUAN Wei, , LIU Hong-Ping, SHEN Li, , ZHAN Ming-Sheng,
Chin. Phys. Lett. 2007, 24 (3):
672-674
.
With time-of-flight and electric field ionization detection technique, we investigate the motional Stark effect for highly excited Rydberg barium in high magnetic field and its active cancellation experimentally. In the experiment, the atom beam is aligned at a small angle of 15° with respect to the magnetic field. The motional Stark effect cancellation is demonstrated on two sets of circularly polarized spectra in static magnetic field B=1.00000 Tesla and B=1.70000 Tesla, respectively, although the effect is very small (~3.5Vcm-1) in our apparatus configuration.
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Re-excited States in Conjugated Polymers
ZHANG Da-Cheng, LIU De-Sheng, MEI Liang-Mo, XIE Shi-Jie, SUN Xin
Chin. Phys. Lett. 2007, 24 (3):
698-701
.
We investigate the re-exciting process of a soliton, a polaron and a bipolaron in conjugated polymers. For a soliton case, the processes S0+ hυ=>S±+Pμ and S±+ hυ=>S0+P± will take place, where S0, S± and P±express a neutral soliton, charged solitons and charged polarons,respectively. For a polaron case, the processes P±+ hυ=> P^μ + BP±2 will occur, where BP±2 expresses a charged bipolaron with two electronic units. For a bipolaron case, the processes BP±2+ hυ=>P±+ P±and BP±2+hυ=> BP±2 +E0 are obtained.
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Large and Ultrafast Third-Order Nonlinear Optical Properties of Ge-S Based Chalcogenide Glasses
CHU Sai-Sai, WANG Shu-Feng, TAO Hai-Zheng, WANG Zhen-Wei, YANG Hong, LIN Chang-Gui, GONG Qi-Huang, ZHAO Xiu-Jian
Chin. Phys. Lett. 2007, 24 (3):
727-729
.
We report ultrafast third-order nonlinear optical (NLO) properties of several chalcogenide glasses GeSx (x=1.8, 2.0, 2.5) measured by femtosecond time-resolved optical Kerr gate technique at 820nm. The third-order nonlinear susceptibility of GeS 1.8 glass is determined to be as large as 1.41×10-12 esu, which is the maximum value of the third order nonlinear susceptibility χ(3) for the three compositions investigated. The symmetric Gauss profiles of optical Kerr signals reveal the nature of ultrafast nonlinear response of these samples, which are originated from the ultrafast polarization of the electron clouds. By detailed microstructural analysis of these glasses based on the chain-crossing model (CCM) and the random-covalent-network model (RCNM), it can be concluded that χ(3) value of GeSx glasses can be enhanced greatly by S--S covalent bonds or S3Ge--GeS3 ethane-like units.
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Femtosecond Third-Order Optical Nonlinearity of Au:Bi2O3 Nanocomposite Films
YOU Guan-Jun, ZHOU Peng, DONG Zhi-Wei, ZHANG Chun-Feng, CHEN Liang-Yao, QIAN Shi-Xiong
Chin. Phys. Lett. 2007, 24 (3):
730-733
.
Ultrafast third-order optical nonlinearities of the as-deposited and annealed Au:Bi2O3 nanocomposite films deposited by magnetron cosputtering are investigated by using femtosecond time-resolved optical Kerr effect (OKE) and pump--probe techniques. The third-order optical nonlinear susceptibility is estimated to be 2.6×10-10 esu and 1.8×10-9 esu at wavelength of 800nm, for the as-deposited and the annealed film, respectively. The OKE signal of the as-deposited film is nearly temporally symmetrical with a peak centred at zero delay time, which indicates the dominant contribution from intraband transition of conduction electrons. For the annealed film, the existence of a decay process in OKE signal implies the important contribution of hot electrons. These characteristics are in agreement with the hot electron dynamics observed in pump--probe measurement.
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In Vivo Monitoring of Neovascularization in Tumour Angiogenesis by Photoacoustic Tomography
XIANG Liang-Zhong, XING Da, GU Huai-Min, ZHOU Fei-Fan, YANG Di-Wu, ZENGLv-Ming, YANG Si-Hua
Chin. Phys. Lett. 2007, 24 (3):
751-754
.
Photoacoustic tomography (PAT) is presented to in vivo monitor neovascularization in tumour angiogenesis with high resolution and high contrast images in a rat. With a circular scan system, the photoacoustic signal, generated by laser pulses at a wavelength of 532nm from a Q-switched Nd:YAG laser, is captured by a hydrophone with a diameter of 1mm and a sensitivity of 850nV/Pa. The vascular structure around the rat tumour is imaged clearly, with optimal contrast, because blood has strong absorption near this wavelength. Serial noninvasive photoacoustic images of neovascularization in tumour angiogenesis are also obtained consecutively from a growing tumour implanted under the skin of a rat over a period of two weeks. This work demonstrates that PAT can potentially provide a powerful tool for tumour angiogenesis detection in cancer research. It will bring us closer to clinical applications for tumour diagnosis and treatment monitoring.
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Supersonic Turbulent Boundary Layer: DNS and RANS
XU Jing-Lei, MA Hui-Yang
Chin. Phys. Lett. 2007, 24 (3):
763-766
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We assess the performance of a few turbulence models for Reynolds averaged Navier--Stokes (RANS) simulation of supersonic boundary layers, compared to the direct numerical simulations (DNS) of supersonic flat-plate turbulent boundary layers, carried out by Gao et al. [Chin. Phys. Lett. 22(2005)1709] and Huang et al. [Sci. Chin.48(2005)614], as well as some available experimental data. The assessment is made for two test cases, with incoming Mach numbers and Reynolds numbers M = 2.25, Re = 365,000/in, and M = 4.5, Re =1.7×107/m, respectively. It is found that in the first case the prediction of RANS models agrees well with the DNS and the experimental data, while for the second case the agreement of the DNS models with experiment is less satisfactory. The compressibility effect on the RANS models is discussed.
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Dust Lattice Waves of Dusty Plasma Chain with an External Magnetic Field
SUN Xiao-Xia, WANG Chun-Hua, WANG Xiao-Gang,
Chin. Phys. Lett. 2007, 24 (3):
771-773
.
Dust lattice waves of a one-dimensional plasma crystal chain with an external magnetic field are investigated. When the magnetic field is in the vertical direction (θ=0), perpendicular to the chain, the vertical transverse mode is not affected, while the horizontal transverse mode is coupled with the longitudinal mode. In the high frequency range, we obtain an `upper-hybrid' dust lattice mode and in the low frequency range, we obtain a `lower-hybrid' dust lattice mode. Between the two modes, a `gap' is formed. When the magnetic field is oriented to the chain (θ=π/2), the longitudinal mode is not affected while both the horizontal and vertical transverse modes are shifted due to the effect of the magnetic field.
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Nitrogen and Silicon Co-Doping of Ge2Sb2Te5 Thin Films for Improving Phase Change Memory Performance
CAI Yan-Fei, ZHOU Peng, LIN Yin-Yin, TANG Ting-Ao, CHEN Liang-Yao, LI Jing, QIAO Bao-Wei, LAI Yun-Feng, FENG Jie, CAI Bing-Chu, CHEN Bomy
Chin. Phys. Lett. 2007, 24 (3):
781-783
.
Electrical properties and phase structures of (Si+N)-codoped Ge2Sb2Te5 (GST) for phase change memory are investigated to improve the memory erformance. Compared to the films with N or Si dopants only in previous reports, the (Si+N)-doped GST has a remarkable improvement of crystalline resistivity of about 104m Ωcm. The Fourier-transform infrared spectroscopy spectrum reveals the Si--N bonds formation in the film. X-ray diffraction patterns show that the grain size is reduced due to the crystallization inhibition of the amorphous GST by SiNx, which results in higher crystalline resistivity. This is very useful to reduce writing current for phase change memory applications.
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Mechanical Yielding and Strength Behaviour of OFHC Copper in Planar Shock Waves
CHEN Da-Nian, FAN Chun-Lei, HU Jin-Wei, WU Shan-Xing, WANG Huan-Ran, TAN Hua, YU Yu-Ying
Chin. Phys. Lett. 2007, 24 (3):
786-789
.
It is necessary to study the validation of strength models under planar shock loading in view of the fact that strength models for metals obtained at moderate strain rates are often used in the numerical simulations of shock wave phenomena. The variations of longitudinal stress, transverse stress and yield strength of oxygen-free high conductance (OFHC) copper with time under planar shock loading are obtained by using the manganin stress gauges and compared with the predicted results by the constructed seven constitutive models based on Y/G=constant and on G/B=constant (Y the yield strength, G the shear modulus, B the bulk modulus), respectively. It seems that the pressure, density, temperature and plastic strain dependence of the yield strength for OFHC copper under planar shock loading is essential to the constitutive description.
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Ge1Sb2Te4 Based Chalcogenide Random Access Memory Array Fabricated by 0.18-μm CMOS Technology
ZHANG Ting, SONG Zhi-Tang, FENG Gao-Ming, LIU Bo, WU Liang-Cai, FENG Song-Lin, CHEN Bomy
Chin. Phys. Lett. 2007, 24 (3):
790-792
.
Ge1Sb2Te4-based chalcogenide random access memory array, with a tungsten heating electrode of 260nm in diameter, is fabricated by 0.18-μm CMOS technology. Electrical performance of the device, as well as physical and electrical properties of Ge1Sb2Te4 thin film, is characterized. SET and RESET programming currents are 1.6 and 4.1mA, respectively, when pulse width is 100ns. Both the values are larger than those of the Ge2Sb2Te5-based ones with the same structure and contact size. Endurance up to 106 cycles with a resistance ratio of about 100 has been achieved.
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Electronic Structure of Si 1-x IVx/Si Superlattices on Si (001)
CHEN Jie, LÜ, Tie-Yu, HUANG Mei-Chun,
Chin. Phys. Lett. 2007, 24 (3):
811-813
.
We have preformed systematical ab initio studies of the structural and electronic properties of short-period Si 1-x IVx/Si/Si (x=0.125, 0.25, 0.5, IV=Ge, Sn) superlattices (SLs) grown along the [001] direction on bulk Si. The present calculations reveal that the Si 0.875 Ge 0.125/Si, Si 0.75 Ge 0.25/Si and Si 0.875 Ge 0.125/Si are the Γ-point direct bandgap semiconductors. The technological importance lies in the expectation that the direct gap Si 1-x IVx/Si/Si SLs may be used as components in integrated optoelectronic devices, in conjunction with the already well-established and highly advanced silicon technology.
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Structural and Thermodynamic Properties of Gallium Arsenide with Hexagonal Wurtzite Structure from First-Principles Analysis
CUI Hong-Ling, ZHANG Wei, CHENG Yan, CHEN Xiang-Rong,
Chin. Phys. Lett. 2007, 24 (3):
814-817
.
A first-principles plane wave method with the ultrasoft pseudopotential scheme in the frame of the generalized gradient approximation (GGA) is performed to calculate the lattice parameters, the bulk modulus B 0 and its pressure derivative B0' of the hexagonal wurtzite GaAs (w-GaAs) by the Cambridge serial total energy package (CASTEP). Our calculations show that the most stable structure of the w-GaAs corresponds to the axial ratio c/a=1.651 and the internal parameter u= 0.374, consistent with other theoretical results. Also, the thermodynamic properties of the w-GaAs are investigated from the quasi-harmonic Debye model. The dependences of the normalized lattice parameters a/a0, c/c0, the axial ratio c/a, the normalized volume V/V0, the heat capacity Cv and the thermal expansion α on pressure P and temperature T are also obtained successfully.
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Enhanced Efficiency of Polymer: Fullerene Bulk Heterojunction Solar Cells with the Insertion of Thin TiO2 Layer near the LiF/Al Electrode
LI Yan, HOU Yan-Bing, JIN Hui, SHI Quan-Min, LIU Jun, SUN Xin, CHANG Xiao-Wei
Chin. Phys. Lett. 2007, 24 (3):
818-821
.
The insertion layer of TiO2 between polymer-fullerene blend and LiF/Al electrode is used to enhance the short-circuit current I sc and fill factor (FF). The solar cell based on the blend of poly[2-methoxy-5-(2'-ethylhexyloxy)-1,4-phenylenevinylene] (MEH-PPV) and C60 with the modifying layer of TiO2 (about 20nm) shows the open-circuit Voc of about 0.62V, short circuit current Isc of about 2.35mA/cm2, filling factor FF of about 0.284, and the power conversion efficiency (PCE) of about 2.4% under monochromatic light (500nm) photoexcitation of about 17mW/cm 2. Compared to cells without the TiO2 layer, the power conversion efficiency increases by about 17.5%. Similar effect is also obtained in cells with the undoped MEH-PPV structure of ITO/PEDOT:PASS/MEH-PPV/(TiO2)LiF/Al. The improved solar cell performance can be attributed to enhanced carrier extraction efficiency at the active layer/electrode interfaces when TiO2 is inserted.
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Structural, Optical and Electrical Properties of ZnS/Porous Silicon Heterostructures
WANG Cai-Feng, LI Qing-Shan, LV Lei, ZHANG Li-Chun, QI Hong-Xia, CHEN Hou
Chin. Phys. Lett. 2007, 24 (3):
825-827
.
ZnS films are deposited by pulsed laser deposition on porous silicon (PS) substrates formed by electrochemical anodization of p-type (100) silicon wafer. Scanning electron microscope images reveal that the surface of ZnS films is unsmoothed, and there are some cracks in the ZnS films due to the roughness of the PS surface. The x-ray diffraction patterns show that the ZnS films on PS surface are grown in preferring orientation along cubic phase β-ZnS (111) direction. White light emission is obtained by combining the blue-green emission from ZnS films with the orange--red emission from PS layers. Based on the I--V characteristic, the ZnS/PS heterojunction exhibits the rectifying junction behaviour, and an ideality factor n is calculated to be 77 from the I--V plot.
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Navigation on Power-Law Small World Network with Incomplete Information
CHEN Jian-Zhen, ZHU Jian-Yang
Chin. Phys. Lett. 2007, 24 (3):
839-842
.
We investigate the navigation process on a variant of the Watts--Strogatz small-world network model with local information. In the network construction, each vertex of an N×N square lattice sends out a long-range link with probability p. The other end of the link falls on a randomly chosen vertex with probability proportional to r-α, where r is the lattice distance between the two vertices, and α≥0. The average actual path length, i.e. the expected number of steps for passing messages between randomly chosen vertex pairs, is found to scale as a power-law function of the network size Nβ, except when α is close to a specific value αmin, which gives the highest efficiency of message navigation. For a finite network, the exponent β epends on both α and p, and αmin drops to zero at a critical value of p which depends on N. When the network size goes to infinity, β depends only on α, and αmin is equal to the network dimensionality.
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72 articles
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