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Exact Vortex Clusters of Two-Dimensional Quantum Fluid with Harmonic Confinement
CHONG Gui-Shu, ZHANG Ling-Ling, HAI Wen-Hua
Chin. Phys. Lett. 2013, 30 (4):
040303
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DOI: 10.1088/0256-307X/30/4/040303
A family of exact analytical solutions of vortices in quantum fluid governed by a two-dimensional time-dependent Schr?dinger equation is presented, which describes different kinds of vortex structures. The dynamics of different vortex clusters, such as the single vortex, vortex pair, vortex dipole and vortex trimer in a two-dimensional quantum fluid are analytically studied based on these exact solutions. The time evolutions of the wave of such vortices are demonstrated, and the orbits of motion of singular points in the vortices are also explored. The interactions of vortices in many-vortex clusters are discussed. A repulsive interaction between vortices with the same topological charge, and inter-annihilation and inter-creation of vortices with opposite topological charge, are shown.
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Improvement of Controlled Bidirectional Quantum Direct Communication Using a GHZ State
YE Tian-Yu, JIANG Li-Zhen
Chin. Phys. Lett. 2013, 30 (4):
040305
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DOI: 10.1088/0256-307X/30/4/040305
The security of controlled bidirectional quantum direct communication using a GHZ state [ Chin. Phys. Lett. 23 (2006) 1680] is analyzed. It turns out that the MX protocol has the problem of definite information leakage, i.e., the first bit of a secret message from any communication party is always leaked out without any active attack after the controller's announcement of measurement results. We put forward two approaches to improve this. The first is to merely modify the encoding rule of the MX protocol, while the second is to use a Bell state as the quantum resource instead of a GHZ state. Both our approaches can ensure that all the bits of secret messages from two communication parties are not leaked out after the controller's announcement of measurement results. Moreover, the controlled bidirectional quantum secure direct communication protocol based on the second approach is more convenient to implement than the MX protocol, since it merely uses a Bell state as the quantum resource and only needs to perform the Bell-basis measurement.
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A Potassium Atom Four-Level Active Optical Clock Scheme
ZHANG Sheng-Nan, WANG Yan-Fei, ZHANG Tong-Gang, ZHUANG Wei, CHEN Jing-Biao
Chin. Phys. Lett. 2013, 30 (4):
040601
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DOI: 10.1088/0256-307X/30/4/040601
We present an active optical clock scheme with a four-level quantum potassium system. We calculate the population probabilities of each state using the density matrix. At the steady state, ρ33 and ρ55 are equal to 8.3% and 3.5%, respectively, and the population inversion between the 5S1/2 and 4P3/2 states is built up in the thermal potassium cell with a 404.7 nm pumping laser. According to the mechanism of the active optical clock, under the action of the 404.7 nm pumping laser, the scheme can output a 1252.2 nm quantum-limited-linewidth laser, which can be directly used as an active optical frequency standard.
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Finding a Way to Determine the Pion Distribution Amplitude from the Experimental Data
HUANG Tao, WU Xing-Gang, ZHONG Tao
Chin. Phys. Lett. 2013, 30 (4):
041201
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DOI: 10.1088/0256-307X/30/4/041201
It is believed that one can extract more accurate information of the pion distribution amplitude from the pion-photon transition form factor (TFF) due to the single pion in this process. However, the BABAR and Belle data of the pion-photon TFF have a big difference for Q2∈[15,40] GeV2, and at present, the pion DA can not be definitely determined from the pion-photon TFF. It is crucial to find the right pion DA behavior and to determine which data is more reliable. We perform a combined analysis of the most existing data of the processes involving pion by using a general model for the pion wavefunction/DA. Such a DA model can mimic all the existed pion DA behaviors, whose parameters can be fixed by the constraints from the processes π0→γγ, π→μν, and B→πl ν, etc. Especially, we examine the B →π transition form factors that provides another constraint to the parameter B in our DA model, which results in B∈[0.00,0.29]. This inversely shows that the predicted curve for the pion-photon TFF is between the BABAR and Belle data in the region Q2∈[15,40] GeV2. It will be tested by coming more accurate data in large Q2 region, and the definite behavior of pion DA can be concluded finally.
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Observation of New Isotope 131Ag via the Two-Step Fragmentation Technique
WANG He, N. Aoi, S. Takeuchi, M. Matsushita, P. Doornenbal, T. Motobayashi, D. Steppenbeck, K. Yoneda, K. Kobayashi, J. Lee, LIU Hong-Na, Y. Kondo, R. Yokoyama, H. Sakurai, YE Yan-Lin
Chin. Phys. Lett. 2013, 30 (4):
042501
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DOI: 10.1088/0256-307X/30/4/042501
We report on the first observation of the neutron-rich nucleus 131Ag. This isotope was produced via fragmentation reactions of intense secondary radioactive ion beams, including 134, 135Sn. The secondary beams were produced from induced fission reactions from a stable 238U beam at 345 MeV/nucleon. Secondary reaction residues were selected by the ZeroDegree spectrometer and identified by measuring their magnetic rigidity, time of flight, energy loss, and total kinetic energy.
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First Principles Study of Single Wall TiO2 Nanotubes Rolled by Anatase Monolayers
ZHANG Hai-Yang, DONG Shun-Le
Chin. Phys. Lett. 2013, 30 (4):
043102
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DOI: 10.1088/0256-307X/30/4/043102
Titanium dioxide (TiO2) nanotubes have been widely investigated for their potential applications in solar cells, hydrogen production, and catalysis. We study three types of TiO2 nanotubes constructed from anatase TiO2 monolayers with density functional-based tight binding methods employing the DFTB+ code. The dependences of the strain energies, structural and electronic properties on the radii of the tubes are investigated in the 3–10 ? range. In addition, the present calculations indicate that the electronic band gap of all types of TiO2 nanotubes is proportional to their diameters. Chiral (n,m) tubes have smaller band gaps than (n,0) and (m,0) tubes, which can be prepared for absorbing the visible spectrum of solar energy.
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The Probe Transmission Spectra of 87Rb in an Operating Magneto-Optical Trap in the Presence of an Ionizing Laser
LIU Long-Wei, JIA Feng-Dong, RUAN Ya-Ping, HUANG Wei, LV Shuang-Fei, XUE Ping, XU Xiang-Yuan, DAI Xing-Can, ZHONG Zhi-Ping
Chin. Phys. Lett. 2013, 30 (4):
043201
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DOI: 10.1088/0256-307X/30/4/043201
The influence of an ionizing laser on the pump-probe spectra of 87Rb over the transition 52S1/2,F=2 →52P3/2,F'=3 is experimentally studied in an operating magneto-optical trap. These spectral features, including gain peak, a dispersion-like structure and absorption peak, become weak as the intensity of the ionizing laser increases. Moreover, the profiles of the absorption peak and gain peak vary as the ionizing laser intensity changes. Such results indicate that there is more than one component in the two features and that each component has different dependences on the number of 87Rb atoms.
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The Collins Formula Applied in Optical Image Encryption
CHEN Lin-Fei, ZHAO Dao-Mu, MAO Hai-Dan, GE Fan, GUAN Rui-Xia
Chin. Phys. Lett. 2013, 30 (4):
044201
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DOI: 10.1088/0256-307X/30/4/044201
We propose a novel method for image encryption, which is realized by the Collins formula with the random shifting method. The Collins formula can denote different optical transforms by one expression with different ABCD elements. For a generalized optical system, the ABCD elements can be randomly chosen, so the keys are increased and the security of the system is strengthened. Finally, some computer simulations are given for different encryption systems to prove the possibilities. The encryption effect is good, and people without the correct keys can not obtain the information easily.
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Femtosecond Laser Pulses for Drilling the Shaped Micro-Hole of Turbine Blades
JIA Hai-Ni, YANG Xiao-Jun, ZHAO Wei, ZHAO Hua-Long, DU Xu, YANG Yong
Chin. Phys. Lett. 2013, 30 (4):
044202
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DOI: 10.1088/0256-307X/30/4/044202
We design a set of processing devices to drill the shaped holes of turbine blades by using a femtosecond laser which outputs 1064 nm 5 W pulses at 100 kHz, investigate the mechanism of the femtosecond laser interaction with metals, and demonstrate that ultrafast laser drilling has distinct strong points against electric spark and longer laser pulse processing. The advantages related to no recast layer, no thermal effect, no micro crack, high precision, and high processing efficiency are carried out.
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Two-Mode Steady-State Entanglement in a Four-Level Atomic System
PING Yun-Xia, ZHANG Chao-Min, CHEN Guang-Long, ZHU Peng-Fei, CHENG Ze
Chin. Phys. Lett. 2013, 30 (4):
044203
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DOI: 10.1088/0256-307X/30/4/044203
We investigate the continuous variable entanglement in a four-level atom according to the criterion proposed by Duan et al. [ Phys. Rev. Lett. 84 (2000) 2722]. The atomic coherence is introduced using two external classical driving fields. We study the steady-state entanglement of the system in the presence of losses, concluding that the creation of entangled states can be achievable under certain conditions.
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A Tunable Blue Light Source with Narrow Linewidth for Cold Atom Experiments
ZHAI Yue-Yang, FAN Bo, YANG Shi-Feng, ZHANG Yin, QI Xiang-Hui, ZHOU Xiao-Ji, CHEN Xu-Zong
Chin. Phys. Lett. 2013, 30 (4):
044209
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DOI: 10.1088/0256-307X/30/4/044209
We present a 397-nm frequency-doubling system with a quasi-phase-matched KTP crystal (PPKTP) which features tunable, narrow linewidth, high power, and excellent mechanical stability. Using 20-mm and 30-mm-long PPKTP crystals, we establish two experimental setups based on different external cavity parameters. By testing the beat signal of these two lasers, the linewidth for the system is measured to be less than 2.5 MHz. The maximum power of blue light can be achieved up to 40 mW. With these performance characteristics, the constructed blue laser system is useful for applications in cold atom physics and precision measurements.
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The Multi-Scale and the Multi-Fractality Properties of Speckles on Rough Screen Surfaces
ZHANG Mei-Na, LI Zhen-Hua, CHEN Xiao-Yi, LIU Chun-Xiang, TENG Shu-Yun, CHENG Chuan-Fu
Chin. Phys. Lett. 2013, 30 (4):
044210
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DOI: 10.1088/0256-307X/30/4/044210
With a microscopic imaging system composed of microscopic objective, lens and CCD, we observe the complicated structures in the speckle fields on the surface of a rough screen. It is found that such structures contain ridge stripes, large platform-like grains, and shivy grains, exhibiting multiple scales in size and multiple fractalities. Simulations shows these structures are formed by different parts of the rough surface. The experimental curve of the autocorrelation function of the speckle intensity includes the three parts of the central peak, the transition part and the long tail part. Using the sum of self-affine fractal models with different scales and fractalities, we propose theoretically a triple-scale autocorrelation function to describe the speckle field. Fit of this autocorrelation function to the experimental curve gives the values of such parameters as average speckle sizes and fractalities in different scales of the speckle structures.
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Particle-in-Cell Simulations of Fast Magnetic Reconnection in Laser-Plasma Interaction
ZHANG Ze-Chen, LU Quan-Ming, DONG Quan-Li, LU San, HUANG Can, WU Ming-Yu, SHENG Zheng-Ming, WANG Shui, ZHANG Jie
Chin. Phys. Lett. 2013, 30 (4):
045201
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DOI: 10.1088/0256-307X/30/4/045201
Recent experiments have observed magnetic reconnection in laser-produced high-energy-density (HED) plasma bubbles. We perform two-dimensional (2-D) particle-in-cell (PIC) simulations to investigate magnetic reconnection between two approaching HED plasma bubbles. It is found that the expanding velocity of the bubbles has a great influence on the process of magnetic reconnection. When the expanding velocity is small, a single X line reconnection is formed. However, when the expanding velocity is sufficiently large, we can observe a plasmoid in the vicinity of the X line. At the same time, the structures of the electromagnetic field in HED plasma reconnection are similar to that in Harris current sheet reconnection.
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In situ XAFS Investigation on Zincblende ZnS up to 31.7 GPa
YANG Jun, ZHU Feng, ZHANG Qian, WU Ye, WU Xiang, QIN Shan, DONG Jun-Cai, CHEN Dong-Liang
Chin. Phys. Lett. 2013, 30 (4):
046101
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DOI: 10.1088/0256-307X/30/4/046101
In situ high-pressure x-ray absorption fine structure (EXAFS) measurements on the Zn K-edge in zincblende ZnS are performed up to 31.7 GPa at room temperature using a synchrotron radiation x-ray re-focused by a polycapillary half-lens in the classic energy-scanning transmission mode. The present XAFS data illustrate that ZnS undergoes a phase transition from zincblende F43m to rocksalt Fm3m at 16.9 GPa, accompanied by the increase of the first shell coordination number of the absorption zinc atoms and the unit-cell volume collapse of ~14%. The isothermal equation of state of the F43m ZnS is well presented by the third-order Birch–Murnaghan equation of state with V0=158.6±0.8 ?3, B0=87±5 GPa and B0'=4 (fixed). The high-pressure behavior of ZnS from the XAFS spectra is consistent with the previous high-pressure XRD results. In addition, the present experimental method demonstrates that the large divergent x-ray micro-beam induced by a polycapillary half-lens can suppress effectively the glitches from single crystal diamond anvil and improve significantly the quality of the XAFS data, which will shed light on the high-pressure XAFS applications.
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CuO Nanoparticle Modified ZnO Nanorods with Improved Photocatalytic Activity
WEI Ang, XIONG Li, SUN Li, LIU Yan-Jun, LI Wei-Wei
Chin. Phys. Lett. 2013, 30 (4):
046202
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DOI: 10.1088/0256-307X/30/4/046202
Cupric oxide (CuO) nanoparticles were grown on zinc oxide (ZnO) nanorod (NR) arrays to form ZnO–CuO corn-like composites via a simple two step solution-based method. First, ZnO nanorods were grown on a glass substrate by the hydrothermal method. Afterwards, CuO crystals were photochemically deposited on ZnO NRs using ultraviolet (UV) light irradiation at room temperature. The density and size of CuO nanoparticles (NPs) on ZnO NRs can be controlled by the irradiation time of UV light. The structural and optical properties of ZnO–CuO nanocomposites were characterized by using various techniques such as UV-vis absorption spectroscopy, photoluminescence, scanning electron microscopy, energy dispersive x-ray spectroscopy, and x-ray diffraction. ZnO–CuO nanocomposites show an excellent improvement in photocatalytic characteristics compared to bare ZnO NRs.
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Electronic Band Structure and Optical Response of Spinel SnX2O4 (X = Mg, Zn) through Modified Becke–Johnson Potential
A. Manzar, G. Murtaza, R. Khenata, S. Muhammad, Hayatullah
Chin. Phys. Lett. 2013, 30 (4):
047401
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DOI: 10.1088/0256-307X/30/4/047401
The modified Becke–Johnson exchange potential approximation is applied to predict the band structure, optical parameters and electron density of SnMg2O4 and SnZn2O4. The local density approximation, generalized gradient approximation (GGA), EV-GGA significantly underestimate the direct band gap values compared to modified Becke–Johnson approximation. The band gap dependent optical parameters such as dielectric constant, index of refraction, reflectivity, and optical conductivity are calculated and analyzed. A prominent feature of cation replacement is observed and analyzed for these studied compounds. The replacement of the cation Mg by Zn leads to a significant reduction in the value of band gap and consequently affects its dependant optical parameters. This variation is of crucial importance for device fabrication in different regions of the spectrum.
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Room-Temperature Ferromagnetism in Fe/Sn-Codoped In2O3 Powders and Thin Films
JIANG Feng-Xian, XI Shi-Bo, MA Rong-Rong, QIN Xiu-Fang, FAN Xiao-Chen, ZHANG Min-Gang, ZHOU Jun-Qi, XU Xiao-Hong
Chin. Phys. Lett. 2013, 30 (4):
047501
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DOI: 10.1088/0256-307X/30/4/047501
Fe/Sn-codoped In2O3 powders and films are prepared by a vacuum annealing process and a pulsed laser deposition technique, respectively. The structural and magnetic properties of the samples are investigated. The obvious room-temperature ferromagnetism is observed in both (In0.92Fe0.05Sn0.03)2O3 powders and films, but their magnetic behaviors are very different. The ferromagnetism of the vacuum-annealed powders is partially due to precipitated Fe3O4 impurity. By contrast, the ferromagnetism of the films is intrinsic and does not originate from any magnetic impurity, as confirmed by the extensive x-ray absorption spectroscopy and magnetization studies.
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Electric and Magnetic Properties and Magnetoelectric Effect of the Ba0.8Sr0.2TiO3/CoFe2O4 Heterostructure Film by Radio-Frequency Magnetron Sputtering
WANG Ye-An, WANG Yun-Bo, RAO Wei, GAO Jun-Xiong, ZHOU Wen-Li, YU Jun
Chin. Phys. Lett. 2013, 30 (4):
047502
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DOI: 10.1088/0256-307X/30/4/047502
A Ba0.8Sr0.2TiO3/CoFe2O4 layered heterostructure film was grown on a Pt/TiO2/SiO2/Si substrate by rf-magnetron sputtering. X-ray diffraction shows that the film consists of perovskite Ba0.8Sr0.2TiO3 and spinel CoFe2O4 phases. The microstructures of the film were observed by a scanning electron microscope (SEM), showing good surface morphology and clear interfaces among the Ba0.8Sr0.2TiO3 film, the CoFe2O4 film and the substrate. The variations of dielectric properties with frequency of the heterostructure film are investigated. The heterostructure film simultaneously displays distinct ferroelectricity and ferromagnetism. Moreover, an obvious magnetoelectric coupling effect was observed in the heterostructure film with a maximum magnetoelectric voltage coefficient of 5.0 mV?cm?1Oe?1, which is about seven times larger than that of the Ba0.8Sr0.2TiO3/CoFe2O4 particulate composite ceramics in a previous report.
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57 articles
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