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Preliminary Frequency Comparison of Two 40Ca+ Optical Frequency Standards
LIU Pei-Liang, HUANG Yao, BIAN Wu, SHAO Hu, QIAN Yuan, GUAN Hua, GAO Ke-Lin
Chin. Phys. Lett. 2014, 31 (11):
113702
.
DOI: 10.1088/0256-307X/31/11/113702
Frequency comparison is one of the most efficient ways to evaluate the performance of a frequency standard. Based on the pre-existing 40Ca+ optical frequency standard, we set up the second 40Ca+ optical frequency standard, which has been improved in the materials and structure of ion traps for better control of the magnetic field. After the compensation, the residual magnetic field at the position of the ion is adjusted to be ~500 nT with a long time jitter of ~10 nT, which is better than the pre-existing 40Ca+ optical frequency standard. We realize the '4-point-closed-loop locking' on the second 40Ca+ optical frequency standard after a series of preparatory works. Through half an hour of measurement time, the two frequency standards exhibited a stability of 2.1×10?13τ?1/2 and a relative frequency difference of 1.5 (2.9) Hz.
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Temperature Dependence of Emission Properties of Self-Assembled InGaN Quantum Dots
ZHAO Wan-Ru, WENG Guo-En, LIANG Ming-Ming, LI Zeng-Cheng, LIU Jian-Ping, ZHANG Jiang-Yong, ZHANG Bao-Ping
Chin. Phys. Lett. 2014, 31 (11):
114205
.
DOI: 10.1088/0256-307X/31/11/114205
Emission properties of self-assembled green-emitting InGaN quantum dots (QDs) grown on sapphire substrates by using metal organic chemical vapor deposition are studied by temperature-dependent photoluminescence (PL) measurements. As temperature increases (15–300 K), the PL peak energy shows an anomalous V-shaped (redshift–blueshift) variation instead of an S-shaped (redshift–blueshift–redshift) variation, as observed typically in green-emitting InGaN/GaN multi-quantum wells (MQWs). The PL full width at half maximum (FWHM) also shows a V-shaped (decrease–increase) variation. The temperature dependence of the PL peak energy and FWHM of QDs are well explained by a model similar to MQWs, in which carriers transferring in localized states play an important role, while the confinement energy of localized states in the QDs is significantly larger than that in MQWs. By analyzing the integrated PL intensity, the larger confinement energy of localized states in the QDs is estimated to be 105.9 meV, which is well explained by taking into account the band-gap shrinkage and carrier thermalization with temperature. It is also found that the nonradiative combination centers in QD samples are much less than those in QW samples with the same In content.
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Electron Beam Lithographic Pixelated Micropolarizer Array for Real-Time Phase Measurement
ZHANG Zhi-Gang, DONG Feng-Liang, CHENG Teng, QIAN Ke-Mao, QIU Kang, ZHANG Qing-Chuan, CHU Wei-Guo, WU Xiao-Ping
Chin. Phys. Lett. 2014, 31 (11):
114208
.
DOI: 10.1088/0256-307X/31/11/114208
Pixelated micropolarizer arrays (PMAs) have recently been used as key components to achieve real-time phase measurement. PMA fabrication by electron beam lithography and inductively coupled plasma-reactive ion etching is proposed in this work. A 320×240 aluminum PMA with 7.4 μm pitch is successfully fabricated by the proposed technique. The period of the grating is 140 nm, and the polarization directions of each of the 2×2 units are 0°, 45°, 90°, and 135°. The scanning electron microscopy and optical microscopy results show that the PMA has a good surface characteristic and polarization performances. When the PMA is applied to phase-shifting interferometry, four fringe patterns of different polarization directions are obtained from only one single frame image, and then the object wave phase is calculated in real time.
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Fourth-Order Spatial Correlation of Thermal Light
WEN Feng, ZHANG Xun, XUE Xin-Xin, SUN Jia, SONG Jian-Ping, ZHANG Yan-Peng
Chin. Phys. Lett. 2014, 31 (11):
114209
.
DOI: 10.1088/0256-307X/31/11/114209
We investigate the fourth-order spatial correlation properties of pseudo-thermal light in the photon counting regime, and apply the Klyshko advanced-wave picture to describe the process of four-photon coincidence counting measurement. We deduce the theory of a proof-of-principle four-photon coincidence counting configuration, and find that if the four randomly radiated photons come from the same radiation area and are indistinguishable in principle, the fourth-order correlation of them is 24 times larger than that when four photons come from different radiation areas. In addition, we also show that the higher-order spatial correlation function can be decomposed into multiple lower-order correlation functions, and the contrast and visibility of low-order correlation peaks are less than those of higher orders, while the resolutions all are identical. This study may be useful for better understanding the four-photon interference and multi-channel correlation imaging.
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Depression of the Superfluid Transition Temperature in 4He by a Heat Flow
YIN Liang, LIN Peng, QI Xin
Chin. Phys. Lett. 2014, 31 (11):
114401
.
DOI: 10.1088/0256-307X/31/11/114401
The depression of the superfluid transition temperature in He by a heat flow Q is studied. A small sealed cell with a capillary is introduced and a stable and flat superfluid transition temperature plateau is easily obtained by controlling the temperature of the variable-temperature platform and the bottom chamber of the sealed cell. Owing to the depression effect of the superfluid transition temperature by the heat flow, the heat flow through the capillary is changed by the temperature control to obtain multiple temperature plateaus of different heat flows. The thermometer self-heating effect, the residual heat leak of the 4.2 K environment, the temperature difference on the He II liquid column, the Kapiza thermal resistance between the liquid helium and the copper surface of the sealed cell, the temperature gradient of the sealed cell, the static pressure of the He II liquid column and other factors have influence on the depression effect and the influence is analyzed in detail. Twenty experiments of the depression of the superfluid transition temperature in 4He by heat flow are made with four sealed cells in one year. The formula of the superfluid transition temperature pressured by the heat flow is Tλ(Q)=?0.00000103Q+2.1769108, and covers the range 229≤Q≤6462 μW/cm2.
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Intruder Motion in Two-Dimensional Shaken Granular Beds
MA Huan-Ping, LV Yong-Jun, ZHENG Ning, LI Liang-Sheng, SHI Qing-Fan
Chin. Phys. Lett. 2014, 31 (11):
114501
.
DOI: 10.1088/0256-307X/31/11/114501
The dynamical behavior of an intruder immersed in a two-dimensional shaken granular bed is experimentally investigated. With two types of background particles, f– Γ phase diagrams depicting the intruder's motion are measured and compared. It is found that even with the same size and density ratio of the intruder to the background particles, the intruder exhibits a distinct behavior at given vibrational conditions: rising behavior in one granular bed; sinking behavior in another granular bed. We slightly tune the size and density ratio to confirm the reliability of the experimental results. In addition, we examine the influences of interstitial air, convection and the initial position on the intruder's motion, speculating that the opposite motion could be traced to the material properties of the background particles.
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Simulation of the Quasi-Monoenergetic Protons Generation by Parallel Laser Pulses Interaction with Foils
WANG Wei-Quan, YIN Yan, ZOU De-Bin, YU Tong-Pu, YANG Xiao-Hu, XU Han, YU Ming-Yang, MA Yan-Yun, ZHUO Hong-Bin, SHAO Fu-Qiu
Chin. Phys. Lett. 2014, 31 (11):
115201
.
DOI: 10.1088/0256-307X/31/11/115201
A new scheme of radiation pressure acceleration for generating high-quality protons by using two overlapping-parallel laser pulses is proposed. Particle-in-cell simulation shows that the overlapping of two pulses with identical Gaussian profiles in space and trapezoidal profiles in the time domain can result in a composite light pulse with a spatial profile suitable for stable acceleration of protons to high energies. At ~2.46×1021 W/cm2 intensity of the combination light pulse, a quasi-monoenergetic proton beam with peak energy ~200 MeV/nucleon, energy spread <15%, and divergency angle <4° is obtained, which is appropriate for tumor therapy. The proton beam quality can be controlled by adjusting the incidence points of two laser pulses.
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The Kinetic Theory of Growth of Zr-Sn Diffusion Layers on Zr55Cu30Al10Ni5 Metallic Glass
CHAI Kan, LIN Tie-Song, HE Peng, SUN Jian-Fei
Chin. Phys. Lett. 2014, 31 (11):
116102
.
DOI: 10.1088/0256-307X/31/11/116102
The growth kinetics of the intermetallic compound layer between molten pure Sn and ZrCu30Al10Ni5 bulk metallic glass (BMG) is mainly controlled by the diffusion mechanism at stage I at which the value of the time exponent is approximately 1/2, also there is unusual or unique stage II whose time exponent of the growth is suppressed to 1/3. It is deduced that phase transition such as nucleation, coalescence occurring in the vicinity of the interface of the diffusion layer within the BMG and the average size growing as one-third power of time, called the Lifshitz–Slezov law. A more elegant means of attack is based upon the Fokker–Planck approach, which permits us to calculate directly the probability of the distribution of steady-state thickness fluctuations. Physical implications of the analytical results also give the one-third power of time of distance scale. The transmission of Sn particles through a disorder system of the BMG, scattered by the local fluctuation levels, is the source of the time exponent from 1/2 to 1/3 as a macroscopic cumulative effect.
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Raman Spectrum of Epitaxial Graphene Grown on Ion Beam Illuminated 6H-SiC (0001)
ZHOU Zhi, HU Ying, SHAN Xin-Yan, LU Xing-Hua
Chin. Phys. Lett. 2014, 31 (11):
116801
.
DOI: 10.1088/0256-307X/31/11/116801
Patterning SiC substrates with focused ion beam for growth of confined graphene nanostructures is interesting for fabrication of graphene devices. However, by imposing an ion beam, the morphology of illuminated SiC substrate surface is inevitably damaged, which imposes significant effects on the subsequent growth of graphene. By using confocal Raman spectroscopy, we investigate the effects of ion beam illumination on the quality of graphene layers that are grown on 6H-SiC (0001) substrates with two different growth methods. With the first method, the 6H-SiC (0001) substrate is flash annealed in ultra-high vacuum. Prominent defects in graphene grown on illuminated areas are revealed by the emergence of Raman D peak. Significant changes in D peak intensity are observed with Ga+ ion fluence as low as 105 μm?2. To eliminate the damage from the ion beam illumination, hydrogen etching is employed in the second growth method, with which prominent improvement in the quality of crystalline graphene is revealed by its Raman features. The defect density is significantly reduced as inferred from the disappearance of D peak. The Raman shift of G peak and 2D peak indicates strain-released graphene layers as grown in such a method. Such results provide essential information for patterning graphene nano-devices.
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Semimetal Na3Bi Thin Film Grown on Double-Layer Graphene by Molecular Beam Epitaxy
WEN Jing, GUO Hua, YAN Chen-Hui, WANG Zhen-Yu, CHANG Kai, DENG Peng, ZHANG Teng, ZHANG Zhi-Dong, JI Shuai-Hua, WANG Li-Li, HE Ke, MA Xu-Cun, CHEN Xi, XUE Qi-Kun
Chin. Phys. Lett. 2014, 31 (11):
116802
.
DOI: 10.1088/0256-307X/31/11/116802
Atomically flat thin films of topological semimetal Na3Bi are grown on double-layer graphene formed on 6H–SiC(0001) substrates by molecular beam epitaxy. By combined techniques of molecular beam epitaxy, scanning tunneling microscopy and angle resolved photoelectron spectroscopy, the growth conditions for Na3Bi thin films on double-layer graphene are successfully established. The band structure of Na3Bi grown on graphene is mapped along Γ–M and Γ– K directions. Furthermore, the energy band of Na3Bi at higher energy is uncovered by doping Cs atoms on the surface.
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Energy Gap and Electron Effective Mass in Chlorine Halide Superconductor at High Pressure
R. Szczęśniak, D. Szczęśniak
Chin. Phys. Lett. 2014, 31 (11):
117401
.
DOI: 10.1088/0256-307X/31/11/117401
Dependences of the order parameter (Δ) and the electron effective mass (me?) on the temperature for the chlorine halide superconductor are determined in the present work. The high values of the pressure (p1=320 GPa and p2=360 GPa), for which the critical temperature is equal to [TC]p1=30.6 K and [TC]p2=41.5 K, are taken into consideration. It is found that the dependence of the order parameter on the temperature deviates from the predictions of the classical Bardeen–Cooper–Schrieffer theory, due to the existence of the significant strong-coupling and retardation effects. The values of the order parameter, for the temperature close to zero Kelvin, are equal to [Δ(0)]p1=4.89 meV and [Δ(0)]p2=6.82 meV. The obtained results allowed next to calculate the dimensionless ratio RΔ≡2Δ(0)/kBTC, which is equal to 3.71 and 3.81 in respect to p1 and p2. In the last step, it is proven that the electron effective mass is weakly dependent on the temperature in the area of the existence of the superconducting state and reaches its maximum at the critical temperature. For the considered values of the pressure, we obtain [me?]p1max=1.69me and [me?]p2max=1.78me, where the symbol me denotes the electron band mass.
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Method of Moments Based on Prior Knowledge for Solving Wide Angle EM Scattering Problems
CAO Xin-Yuan, CHEN Ming-Sheng, KONG Meng, ZHANG Liang, WU Xian-Liang
Chin. Phys. Lett. 2014, 31 (11):
118401
.
DOI: 10.1088/0256-307X/31/11/118401
Aiming at fast analysis of wide angle electromagnetic scattering problems, compressed sensing theory is introduced and applied, and a new kind of sparse representation of induced currents is constructed based on prior knowledge that originates from excitation vectors in method of moments. Using the new kind of sparse representation in conjugation with compressed sensing, one can recover unknown currents accurately with fewer measurements than some conventional sparse representations in mathematical sense. Hence, times of calculation by traditional method of moments used to obtain the required measurements can be reduced, which will improve the computational efficiency.
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LiF Thickness dependence of Electron Injection Models for Alq3/LiF/Al Cathode Structure
LIAN Jia-Rong, LUO Xi, CHEN Wei, SU Sheng-Xun, ZHAO Hong-Fei, LIU Si-Yang, XU Gui-wen, NIU Fang-Fang, ZENG Peng-Ju
Chin. Phys. Lett. 2014, 31 (11):
118501
.
DOI: 10.1088/0256-307X/31/11/118501
We present the experimental evidences showing that three different electron injection models play roles in Alq3 based organic light-emitting diodes in sequence when the thickness of LiF interlayer is changed. It is found that the device with a 0.2 nm LiF layer displays the largest current with declined luminescence. However, the one with a 0.6 nm LiF layer displays the second largest current and the highest luminescence of all. Combining with the photoluminescent test results, three models, namely chemical reaction at ternary interface, dipole effect at binary interface and tunneling enhancement effect, are expected to play roles in sequence when the LiF thickness is increased from 0 nm to 4 nm.
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Characteristics of Double Gamma-Ray Bursts
LIU Tong, SUN Mou-Yuan, HOU Shu-Jin, LI Ang, ZHANG Fu-Wen, GU Wei-Min, LU Ju-Fu
Chin. Phys. Lett. 2014, 31 (11):
119801
.
DOI: 10.1088/0256-307X/31/11/119801
Double gamma-ray bursts (DGRBs) have two well-separated sub-bursts in the main prompt emission and the typical time interval between them is in the hundreds of seconds. Among DGRBs, gamma-ray bursts (DGRBs) 110801A and 120716A are the ones with known redshifts. However, unlike GRB 110801A, we show that the two sub-bursts of GRB 120716A is severally similar to the short- and long-duration GRBs, thus it is difficult to explain the origin of GRB 120716A by the popular models on the central engine of GRBs. We suggest that some mechanisms of x-ray flares in GRBs, i.e., a post-merger millisecond pulsars or the jet precession in a black hole hyperaccretion system may produce the DGRB.
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42 articles
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