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31.
32.
James D. Scott Linda Chalker-Scott Alynda Empie Foreman Michael D'Angelo 《Photochemistry and photobiology》1999,70(3):308-313
Abstract The ability to avoid or tolerate UVB radiation (290–320 nm) probably reduces the quality of phytoplankton as food for zooplankton. Ultraviolet avoidance forces motile algae lower in the water column, reducing net primary productivity. Production of UV-absorbing compounds as a tolerance mechanism takes carbon and energy away from cell growth; these compounds are also less useful as food for herbivores. We assessed the food quality of UVB-irradiated Chlamydomonas reinhardtii Dang, by analysis of cohort life tables for the herbivore Daphnia pulex Leydig. Algal cultures were grown under fluorescent lights interspersed with UV bulbs (20°C, 16 h light: 8 h dark) and covered with either cellulose acetate (+UVB) or Mylar D (-UVB). After a 7 day UVB exposure, carotenoid levels of C. reinhardtii were significantly greater than in unexposed cultures; there were no significant differences in chlorophyll, lipid, protein or nonstructural carbohydrate levels. After an initial decrease in growth rate, UVB-exposed algae recovered and final growth rates of both cultures were similar after 7 days. Daphnia neonates were raised under optimal conditions (20°C, 16 h light:8 h dark) and fed either UVB-irradiated or control algae. Daphnia fed UVB-irradiated algae had significantly increased mortality, decreased growth rate at the time of first clutch production, delayed release of the first clutch and decreased overall fecundity (P < 0.05). Daphnia were also less efficient at clearing UVB-irradiated algae from the water column (17% removal in 18 h) when compared with Daphnia that grazed upon nonirradiated algae (85% removal in 18 h). These data suggest that even though UVB-irradiated algal populations can recover from their initial decline, their predators may not be able to utilize them as an effective food source. Therefore, the impacts of UVB radiation within 相似文献
33.
K. W. Foreman A. T. Phillips J. B. Rosen K. A. Dill 《Journal of computational chemistry》1999,20(14):1527-1532
We provide some tests of the convex global underestimator (CGU) algorithm, which aims to find global minima on funnel-shaped energy landscapes. We use two different potential functions—the reduced Lennard–Jones cluster potential, and the modified Sun protein folding potential, to compare the CGU algorithm with the simplest versions of the traditional trajectory-based search methods, simulated annealing (SA), and Monte Carlo (MC). For both potentials, the CGU reaches energies lower on the landscapes than both SA and MC, even when SA and MC are given the same number of starting points as in a full CGU run or when all methods are given the same amount of computer time. The CGU consistently finds the global minima of the Lennard–Jones potential for all cases with up to at least n=30 degrees of freedom. Finding the global or near-global minimum in the CGU method requires polynomial time [scaling between O(n3) and O(n4)], on average. ©1999 John Wiley & Sons, Inc. J Comput Chem 20: 1527–1532, 1999 相似文献
34.
Two mode-locked femtosecond fiber lasers, connected via a 7 km fiber link, are synchronized to an rms timing jitter of 19 fs, observed over the entire Nyquist bandwidth (half of the 93 MHz repetition frequency). This result is achieved in two steps. First, active cancellation of the fiber-transmission noise reduces timing jitter caused by path length fluctuations to a record level of 16 fs. Second, using a wide bandwidth interactivity actuator, the slave laser is synchronized to the incoming stable pulse train from the reference laser to within 10 fs. These results are confirmed by an optical cross-correlation measurement performed independently of the feedback loop operated in the microwave domain. 相似文献
35.
36.
We demonstrate a new experimental approach for flexible femtosecond pulse generation in the mid-IR by use of difference-frequency generation from two tightly synchronized Ti:sapphire lasers. The resultant mid-IR pulse train can be easily tuned, with an adjustable repetition frequency up to 100 MHz, a pulse energy of approximately 1.5 x 10(-13) J, and an intensity noise similar to that of the Ti:sapphire. Rapid switching of the mid-IR wavelength and programmable amplitude modulation are achieved by precision setting of the time delay between two original pulses. 相似文献
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38.
M. J. Plater B. M. De Silva M. R. St. J. Foreman W. T. A. Harrison 《Journal of Structural Chemistry》2016,57(6):1169-1175
The syntheses and crystal structures of two one-dimensional coordination polymers, [Mn(C5HO2F6)2(C16H20N2)] n (1) and [Mn(C5HO2F6)2(C20H20N2)] n (2), are described, where C5HO2F6 ? is the hexafluoro acetylacetonate anion, C16H20N2 is 1,6-bis(4-pyridyl)-hexane, and C20H20N2 is 1,4-bis[2-(3-pyridyl)ethyl]-benzene. In both phases, the metal ion lies on a crystallographic twofold axis and is coordinated by two chelating C5HO2F6 ? anions and two bridging bipyridyl ligands to generate a cis-MnN2O4 octahedron. The bridging ligands, which are completed by crystallographic inversion symmetry in both compounds, connect the metal nodes into zigzag [20 1 ] chains in 1 and contorted [001] chains in 2. Intrachain C–H???O interactions occur in 1 but not in 2, which may be correlated with the relative orientations of the ligands. Crystal data: 1, C26H22F12MnN2O4, M r = 709.40, monoclinic, C2/c (No. 15), a = 9.3475(2) Å, b = 16.6547(3) Å, c = 18.3649(4) Å, β = 91.1135(8)°, V = 2858.50(10) Å3, Z = 4, R(F) = 0.030, w R(F 2) = 0.075. 2, C30H22F12MnN2O4, M r = 757.44, monoclinic, C2/c (No. 15), a = 19.9198(2) Å, b = 10.6459(2) Å, c = 16.8185(3) Å, β = 119.8344(8)°, V = 3093.91(9) Å3, Z = 4, R(F) = 0.032, w R(F 2) = 0.078. 相似文献
39.
M. John Plater Mark R. St. J. Foreman Janet M. S. Skakle 《Journal of chemical crystallography》2000,30(8):535-537
The synthesis and molecular structure of the title compound are reported. The metal ion has a distorted octahedral geometry and is coordinated by two cis thiocyanate nitrogens, two trans pyridine nitrogens and two cis pyridazine nitrogens. The structure has an orthorhombic space group Pbcn with a = 12.9376(6) Å, b = 13.4312(7) Å, c = 18.8992(9) Å, V = 3284.1(3) Å3, and Z = 8. 相似文献
40.
Miranda KM Dutton AS Ridnour LA Foreman CA Ford E Paolocci N Katori T Tocchetti CG Mancardi D Thomas DD Espey MG Houk KN Fukuto JM Wink DA 《Journal of the American Chemical Society》2005,127(2):722-731
The recent determination that Angeli's salt may have clinical application as a nitrogen oxide donor for treatment of cardiovascular diseases such as heart failure has led to renewed interest in the mechanism and products of thermal decomposition of Angeli's salt under physiological conditions. In this report, several mechanisms are evaluated experimentally and by quantum mechanical calculations to determine whether HNO is in fact released from Angeli's salt in neutral, aerobic solution. The mechanism of product autoxidation is also considered. 相似文献