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991.
Li Hao 《Journal of Graph Theory》1989,13(3):313-322
Ore proved in 1960 that if G is a graph of order n and the sum of the degrees of any pair of nonadjacent vertices is at least n, then G has a hamiltonian cycle. In 1986, Li Hao and Zhu Yongjin showed that if n ? 20 and the minimum degree δ is at least 5, then the graph G above contains at least two edge disjoint hamiltonian cycles. The result of this paper is that if n ? 2δ2, then for any 3 ? l1 ? l2 ? ? ? lk ? n, 1 = k = [(δ - 1)/2], such graph has K edge disjoint cycles with lengths l1, l2…lk, respectively. In particular, when l1 = l2 = ? = lk = n and k = [(δ - 1)/2], the graph contains [(δ - 1)/2] edge disjoint hamiltonian cycles. 相似文献
992.
Shih Hsi Chu Zhi Hao Chen Zun Yao Weng Elizabeth C. Rowe Edward Chu Ming-Yu Wang Chu 《Journal of heterocyclic chemistry》1987,24(4):989-995
Amino analogs of BAU (5-benzylacyclouridine) and BBAU (5-benzyloxybenzylacyclouridine) and their 2′-hydroxymethyl derivatives were synthesized for evaluation as inhibitors of uridine phosphorylase and hence potential cancer chemotherapeutic agents. Both aminomethyl analogs were found to be potent inhibitors of this enzyme and good potentiators of the anti-tumor action of FUdR. 相似文献
993.
Zhi‐guo Zhang Ji‐bing Yuan Huai‐jun Tang Hao Tang Li‐na Wang Ke‐Li Zhang 《Journal of polymer science. Part A, Polymer chemistry》2009,47(1):210-221
A novel nonconjugated copolymer (PVKEu) with carbazole segments and phenanthroline [Eu(β‐diketonate)3] moieties was synthesized via free radical copolymerization, and characterized by FTIR, 1H NMR spectroscopy, GPC, ICP, and elemental analysis. The copolymer exhibited good solubility, as well as good thermal stability and high glass transition temperature. The photoluminescence (PL) of this polymer in solution and in solid film has been studied. A multi‐layer device with the configuration of ITO/PEDOT: PSS (40 nm)/PVKEu (70 nm)/BCP (15 nm)/AlQ3 (30 nm)/LiF/Al exhibited nearly monochromatic red emission at 615 nm and voltage‐independent spectral stability. Our results suggest that enhancing the ligand‐mediated energy transfer between the matrix polymer and europium complex is a potential method to improve the electroluminescence performance of the Eu‐chelated polymers. © 2008 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 47: 210–221, 2009 相似文献
994.
Yanfeng Zhang Hao Liu Hefei Dong Changhua Li Shiyong Liu 《Journal of polymer science. Part A, Polymer chemistry》2009,47(6):1636-1650
Amphiphilic ABC miktoarm star terpolymers consisting of polystyrene, poly(ε‐caprolactone), and poly(N‐isopropylacrylamide) arms, PS(‐b‐PNIPAM)‐b‐PCL, were synthesized via a combination of atom transfer radical polymerization, ring‐opening polymerization (ROP), and click chemistry. Difunctional PS bearing an alkynyl and a primary hydroxyl moiety at the chain end, PS‐alknyl‐OH, was prepared by reacting azido‐terminated PS with an excess of 3,5‐bis(propargyloxy)benzyl alcohol (BPBA) under click conditions. The subsequent ROP of ε‐caprolactone using PS‐alknyl‐OH macroinitiator afforded PS(‐alkynyl)‐b‐PCL copolymer bearing an alkynyl moiety at the diblock junction point. Target PS(‐b‐PNIPAM)‐b‐PCL amphiphilic ABC miktoarm star terpolymers were then prepared via click reaction between PS(‐alkynyl)‐b‐PCL and an excess of azido‐terminated PNIPAM (PNIPAM‐N3). The removal of excess PNIPAM‐N3 was accomplished by “clicking” onto alkynyl‐functionalized Wang resin. All the intermediate and final products were characterized by gel permeation chromatography, 1H NMR, and FTIR. In aqueous solution, the obtained amphiphilic ABC miktoarm star terpolymer self‐assembles into micelles possessing mixed PS/PCL cores and thermoresponsive shells, which were further characterized by dynamic laser light scattering and transmission electron microscopy. © 2009 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem 47: 1636–1650, 2009 相似文献
995.
We present nonlinear spectra of four-level ladder cesium atoms employing 6 S1/2→6 P3/2→7 S1/2→30 P3/2 scheme of a room temperature vapor cell.A coupling laser drives Rydberg transition,a dressing laser couples two intermediate levels,and a probe laser optically probes the nonlinear spectra via electromagnetically induced transparency(EIT).Nonlinear spectra are detected as a function of coupling laser frequency.The observed spectra exhibit an enhanced absorption(EA) signal at coupling laser resonance to Rydberg transition and enhanced transmission(ET) signals at detunings to the transition.We define the enhanced absorption(transmission) strength,HEA(HET),and distance between two ET peaks,γET,to describe the spectral feature of the four-level atoms.The enhanced absorption signal HEA is found to have a maximum value when we vary the dressing laser Rabi frequency Ωd,corresponding Rabi frequency is defined as a separatrix point,ΩdSe.The values of ΩdSe and further η=ΩdSe/Ωc are found to depend on the probe and coupling Rabi frequency but not the atomic density.Based on ΩdSe,the spectra can be separated into two regimes,weak and strong dressing ranges,Ωd≤ΩdSe and Ωd≥QdSe,respectively.The spectroscopies display different features at these two regimes.A four-level theoretical model is developed that agrees well with the experimental results in terms of the probe-beam absorption behavior of Rabi frequency-dependent dressed states. 相似文献
996.
The analysis of the LHCb data on \begin{document}$X(6900)$\end{document} ![]()
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found in the di-\begin{document}$J/\psi$\end{document} ![]()
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system was performed using a momentum-dependent Flatté-like parameterization. The use of the pole counting rule and spectral density function sum rule provides consistent evidence that both confining and molecular states are possible. Alternatively, the nature of \begin{document}$X(6900)$\end{document} ![]()
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cannot be distinguished if only the di-\begin{document}$J/\psi$\end{document} ![]()
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experimental data with current statistics are available. Nevertheless, we found that the lowest state in the di-\begin{document}$J/\psi$\end{document} ![]()
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system likely has the same quantum numbers as \begin{document}$X(6900)$\end{document} ![]()
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, and \begin{document}$X(6900)$\end{document} ![]()
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is probably not interpreted as a \begin{document}$J/\psi-\psi(2S)$\end{document} ![]()
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molecular state. 相似文献
997.
Zheng Chenglong Li Jie Li Jitao Yue Zhen Wang Silei Li Mengyao Zhao Hongliang Hao Xuanruo Zang Huaping Zhang Yating Yao Jianquan 《中国科学:物理学 力学 天文学(英文版)》2021,64(11):1-12
The usage of full-color imaging in digital pathology produces significant results. Compared with a grayscale image or a pseudocolor image containing contrast information, a full-color image can identify and detect the target object better with color texture information. Fourier ptychographic microscopy(FPM) is a high-throughput computational imaging technique that breaks the tradeoff between high resolution(HR) and a large field of view. It also eliminates the artifacts of scanning and stitching in digital pathology and improves its imaging efficiency. However, the conventional full-color digital pathology based on FPM is still time-consuming because of the repeated experiments with tri-wavelengths. A color transfer FPM approach termed "CFPM" was reported. The color texture information of a low-resolution full-color pathologic image is directly transferred to the HR grayscale FPM image captured by only a single wavelength. Both of the color space of FPM based on the standard CIE-XYZ color model and the display based on the standard RGB color space were established. Different FPM colorization schemes were analyzed and compared with 30 biological samples. Three types of evaluation approaches were provided, including the root-mean-square error(RMSE), the difference maps, and the image histogram cosine similarity. The average RMSE values of the conventional method and CFPM compared with the ground truth were 5.3% and 5.7%, respectively. Therefore, the reconstruction time is significantly reduced by 2/3 with the sacrifice of precision of only 0.4%. The CFPM method is also compatible with advanced fast FPM approaches to further reduce computation time. 相似文献
998.
Lei Pang Yingjuan Shao Wenqi Zhong Hao Liu 《Proceedings of the Combustion Institute》2021,38(3):4121-4129
Oxy-coal combustion with pressurized fluidized beds has recently emerged as a promising carbon capture and storage (CCS) technology for coal-fired power plants. Although a large number of energy efficiency analyses have shown that an increase in combustion pressure can further increase the net plant efficiency, there are few experimental studies of pressurized oxy-coal combustion conducted on fluidized bed combustors/boilers with continuous coal feeding. In this study, oxy-coal combustion experiments with lignite and anthracite were conducted with a 30 kWth pressurized fluidized bed combustor within the pressure range of 0.1 MPa to 0.4 MPa. The investigation focused on the elucidation of the impacts of combustion pressure on the combustion performance, pollutant emissions and desulfurization of oxy-coal combustion in fluidized beds. The results showed that an increase in pressure increased the combustion efficiency and combustion rate of coal particles, and the promoting effect of pressure increase was more significant for the high rank coal with smaller particle size and the high O2 concentration atmosphere. For both coals, NOx emissions decreased with pressure but N2O emissions increased with pressure and accounted for a considerable part of the nitrogen oxide pollutants under high pressure oxy-coal combustion conditions. The pressure had insignificant impact on the SO2 emissions of oxy-coal combustion but an increase in pressure enhanced the direct desulfurization of limestone. 相似文献
999.
先前报道的2,7-二苯芴酮具有不寻常的,伴随150 nm荧光红移的聚集诱导发光现象. 通过重复实验,发现这种异常行为由合成的2,7-二苯芴酮中少量2,7-二苯芴(DPF)造成. 固态纯2,7-二苯芴酮分子在528 nm处确实有强烈的荧光,是在二氯甲烷稀溶液中的4∽5倍(542 nm),但在固体中是蓝移而不是红移. 合成的2,7-二苯芴酮固体的荧光增强和波长红移现象由少量2,7-二苯芴杂质造成. 在稀溶液中,2,7-二苯芴的荧光远强于2,7-二苯芴酮且波长较短,当2,7-二苯芴酮中含有痕量(约1%)2,7-二苯芴时,主要的荧光峰来自于2,7-二苯芴. 因为2,7-二苯芴的吸收峰与2,7-二苯芴酮重叠,所以2,7-二苯芴的电子能可以转移到2,7-二苯芴酮上. 随着浓度的增加,因为2,7-二苯芴与周围2,7-二苯芴酮分子的距离更近,能量转移会变快. 这造成了2,7-二苯芴的荧光猝灭(356和372 nm)和2,7-二苯芴酮的荧光增强(溶液中542 nm,固体中528 nm). 因此,在高浓度溶液或者固体中,仅有542或528 nm的荧光峰出现,356和372 nm 处荧光峰消失. 相似文献
1000.