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111.
In order to optimize the synthesis of BaCuO2, different modes were developed and estimated. Wet chemical powders produced by coprecipitation of oxalates or hydroxycarbonates were characterized and their reactivity is compared with the conventional ceramic process of firing a mixture of BaCO3 and CuO by DTA, XRD and IR-investigations. This becomes possible, because the decomposition of these chemical precursors to BaCO3 and CuO is finished up to 600 °C. Hence, the same reaction for the formation of BaCuO2 is monitored.  相似文献   
112.
113.
The Tungsten oxides WO3, W20O59, W18O49 and WO2 have been transported by TeCl4 in monocrystalline Form. W3O is not a equilibrium phase of the system, and therefore it is impossible to obtain this phase by CTR. The value of the lower phase boundary of tungsten trioxide is 2.96.  相似文献   
114.
Investigations on the Phase Diagram EuCl2–EuCl3 The phase diagram EuCl2–EuCl3 was determined by difference‐thermoanalysis and the barogram of the system was determined by total pressure measurements of different compositions in function of temperature. By the results the phase diagram was precised. Eu5Cl11 decomposes at 565 °C in to EuCl2,s and Eu4Cl9,s and shows a transition at 510 °C. Eu4Cl9 decomposes at 603 °C in to EuCl2,s and Eu14Cl33,s. Eu14Cl33 decomposes at 612 °C peritectically in EuCl2,s and a EuCl3‐rich melt. Eu14Cl33 shows two high temperature transition points at 570 °C and 580 °C. The endothermal effect of compositions near Eu14Cl33 was interpreted as an endothermal formation of this compound. The eutectikum was detected between Eu14Cl33 and EuCl3 to 60 ± 1 Mol‐% EuCl3 at 530 °C.  相似文献   
115.
Chemical Transport of Bismuth Oxide Halides BiOX (X = Cl, Br, I) with X2, HX and H2O, and Determination of the Molar Enthalpies of BiOX By comparison of calculated and experimental chemical transport behaviour of BiOX (X = Cl, Br, I) with X2, HX, and H2O it was shown, that we understand the transport of BiOCl, BiOBr and BiOI with X2 and HX in terms of the well known gaseous spezies in the systems. The existence of gaseous complexes Bi(OH)2X is be concluded from high transport rates of BiOX with water, and their enthalpies and entropies were derived. The molar enthalpies and standard entropies of BiOX were determined by low temperature Cp measurements. (Data see Inhaltsübersicht)  相似文献   
116.
The photochemistry of DNA systems is characterized by the ultraviolet (UV) absorption of π-stacked nucleobases, resulting in exciton states delocalized over several bases. As their relaxation sensitively depends on local stacking conformations, disentangling the ensuing electronic and structural dynamics has remained an experimental challenge, despite their fundamental role in protecting the genome from potentially harmful UV radiation. Here we use transient absorption and transient absorption anisotropy spectroscopy with broadband femtosecond deep-UV pulses (250–360 nm) to resolve the exciton dynamics of UV-excited adenosine single strands under physiological conditions. Due to the exceptional deep-UV bandwidth and polarization sensitivity of our experimental approach, we simultaneously resolve the population dynamics, charge-transfer (CT) character and conformational changes encoded in the UV transition dipoles of the π-stacked nucleotides. Whilst UV excitation forms fully charge-separated CT excitons in less than 0.3 ps, we find that most decay back to the ground state via a back-electron transfer. Based on the anisotropy measurements, we propose that this mechanism is accompanied by a structural relaxation of the photoexcited base-stack, involving an inter-base rotation of the nucleotides. Our results finally complete the exciton relaxation mechanism for adenosine single strands and offer a direct view into the coupling of electronic and structural dynamics in aggregated photochemical systems.

Despite its key role in DNA photochemistry, the decay mechanism of excitons in stacked bases has remained difficult to resolve. Ultrafast polarization spectroscopy now reveals a back-electron transfer and ultrafast base motions in adenosine strands.  相似文献   
117.
CVD-experiments in the system Cu O H Cl N result in the growth of Cu2O single crystals. The characteristic faces of the various forms are the {100} ones. A thermodynamic analysis permits to predict such conditions under which Cu2O is deposited without deposition of any other phases.  相似文献   
118.
A report is given on the transport behaviour of the equilibrium phases NbO2.417 to NbO2.483 and of niobium pentoxide during chemical transport with TeCl4. – It became apparent that phase-pure NbO2.417 and Nb2O5 are deposited from the investigated equilibrium phases. Chemical transport of the phases NbO2.453 to NbO2.483 produces a mixture of several phases. This indicates a strong inhibition of the equilibration in the starting solid. Chemical transport of the niobium pentoxide caused the deposition of monocrystals of the upper and lower phase boundary. The experimental behaviour agrees very well with the calculated results. Monocrystals of the niobium pentoxide forms H, M, N, B and P are deposited in a well identifiable manner by variation of the temperatures (T2, T1).  相似文献   
119.
The thermodynamic relationship between the transition metal dioxides and their tetrahalogenides is demonstrated, and a comprehensive survey on the thermodynamic values of the compounds is given. – All dioxides of the transition metals existing to 1000°C in the solid state are transportable by TeCl4. Only those dioxides are transported by TeBr4 which have corresponding oxide-bromides existing in the gaseous phase. – The forms of crystallographic growth are very similar. The favoured growth direction is [001], the crystal faces are {110}- and {100}-prisms, {101}- and {111}-pyramids, respectively.  相似文献   
120.
Thermal Behaviour and Crystal Structure of YAl3Cl12 We determined the thermodynamic data of YAl3Cl12 ΔH = ?739.9 ± 3 kcal/mol and S = 136.1 ± 4 cal/K · mol by total pressure measurements and ΔH = ?739.1 ± 1.6 kcal/mol by solution calorimetry. Using DTA-investigations we established the phase diagram in the system AlCl3–YCl3. The crystal structure was refined on the basis of single crystal data (P31 12; Z = 3; a = 1 046.8(2); c = 1 562.3(3) pm).  相似文献   
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