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21.
In order to test the accuracy of the eigenvectors associated with the ionic motions which one gets from the Breathing Shell Model (BSM) of Schröder in NaI the nuclear quadrupole relaxation times have been calculated as function of temperature at both Na23 and I127 sites and these are compared with the experimental results. 相似文献
22.
Amy Sangster Diane Knight Richard Farrell Angela Bedard‐Haughn 《Rapid communications in mass spectrometry : RCM》2010,24(19):2791-2798
Both the quantity and quality of plant residues can impact soil properties and processes. Isotopic tracers can be used to trace plant residue decomposition if the tracer is homogeneously distributed throughout the plant. Continuous labeling will homogeneously label plants but is not widely accessible because elaborate equipment is needed. In order to determine if the more accessible repeat‐pulse labeling method could be used to trace plant residue decomposition, this labeling procedure was employed using 13CO2 to enrich field pea and canola plants in a controlled environment. Plants were exposed weekly to pulses of 33 atom% 13CO2 and grown to maturity. The distribution of the label throughout the plant parts (roots, stem, leaves, and pod) and biochemical fractions (ADF and ADL) was determined. The label was not homogeneously distributed throughout the plant; in particular, the pod fractions were less enriched than other fractions indicating the importance of continuing labeling well into plant maturity for pod‐producing plants. The ADL fraction was also less enriched than the ADF fraction. Because of the heterogeneity of the label throughout the plant, caution should be applied when using the repeat‐pulse method to trace the fate of 13C‐labeled residues in the soil. However, root contributions to below‐ground C were successfully determined from the repeat‐pulse labeled root material, as was 13C enrichment of soil within the top 15 cm. Canola contributed more above‐ and below‐ground residue C than field pea; however, canola was also higher in ADF and ADL fractions indicating a more recalcitrant residue. Copyright © 2010 John Wiley & Sons, Ltd. 相似文献
23.
Sangster T Spence M Sinclair P Payne R Smith C 《Rapid communications in mass spectrometry : RCM》2004,18(12):1361-1364
Ion suppression is a well-known phenomenon in electrospray ionization (ESI) mass spectrometry. These suppression effects have been shown to adversely affect the accuracy and precision of quantitative bioanalytical methods using ion spray. Such suppression effects have not been as well defined in atmospheric pressure chemical ionization (APCI) and there is some debate whether these effects actually occur in the ionization process using APCI. Here an example is described where clear ion suppression was observed during studies on a model compound and three metabolites using APCI liquid chromatography/tandem mass spectrometry (LC/MS/MS). 相似文献
24.
Li CK Séguin FH Frenje JA Rygg JR Petrasso RD Town RP Amendt PA Hatchett SP Landen OL Mackinnon AJ Patel PK Tabak M Knauer JP Sangster TC Smalyuk VA 《Physical review letters》2007,99(1):015001
Monoenergetic proton radiography was used to make the first measurements of the long-time-scale dynamics and evolution of megagauss laser-plasma-generated magnetic field structures. While a 1-ns 10(14) W/cm2 laser beam is on, the field structure expands in tandem with a hemispherical plasma bubble, maintaining a rigorous 2D cylindrical symmetry. With the laser off, the bubble continues to expand as the field decays; however, the outer field structure becomes distinctly asymmetric, indicating instability. Similarly, localized asymmetry growth in the bubble interior indicates another kind of instability. 2D LASNEX hydrosimulations qualitatively match the cylindrically averaged post-laser plasma evolution but even then it underpredicts the field dissipation rate and of course completely misses the 3D asymmetry growth. 相似文献
25.
Casey DT Frenje JA Johnson MG Manuel MJ Rinderknecht HG Sinenian N Séguin FH Li CK Petrasso RD Radha PB Delettrez JA Glebov VY Meyerhofer DD Sangster TC McNabb DP Amendt PA Boyd RN Rygg JR Herrmann HW Kim YH Bacher AD 《Physical review letters》2012,108(7):075002
Measurements of the D(d,p)T (dd) and T(t,2n)(4)He (tt) reaction yields have been compared with those of the D(t,n)(4)He (dt) reaction yield, using deuterium-tritium gas-filled inertial confinement fusion capsule implosions. In these experiments, carried out on the OMEGA laser, absolute spectral measurements of dd protons and tt neutrons were obtained. From these measurements, it was concluded that the dd yield is anomalously low and the tt yield is anomalously high relative to the dt yield, an observation that we conjecture to be caused by a stratification of the fuel in the implosion core. This effect may be present in ignition experiments planned on the National Ignition Facility. 相似文献
26.
Sangster TC Goncharov VN Radha PB Smalyuk VA Betti R Craxton RS Delettrez JA Edgell DH Glebov VY Harding DR Jacobs-Perkins D Knauer JP Marshall FJ McCrory RL McKenty PW Meyerhofer DD Regan SP Seka W Short RW Skupsky S Soures JM Stoeckl C Yaakobi B Shvarts D Frenje JA Li CK Petrasso RD Séguin FH 《Physical review letters》2008,100(18):185006
The first observation of ignition-relevant areal-density deuterium from implosions of capsules with cryogenic fuel layers at ignition-relevant adiabats is reported. The experiments were performed on the 60-beam, 30-kJUV OMEGA Laser System [T. R. Boehly, Opt. Commun. 133, 495 (1997)10.1016/S0030-4018(96)00325-2]. Neutron-averaged areal densities of 202+/-7 mg/cm2 and 182+/-7 mg/cm2 (corresponding to estimated peak fuel densities in excess of 100 g/cm3) were inferred using an 18-kJ direct-drive pulse designed to put the converging fuel on an adiabat of 2.5. These areal densities are in good agreement with the predictions of hydrodynamic simulations indicating that the fuel adiabat can be accurately controlled under ignition-relevant conditions. 相似文献
27.
D. F. Sangster 《Journal of Radioanalytical and Nuclear Chemistry》1993,171(1):75-82
A segment on radiation chemistry should be included in every course on nuclear science because of its unique role and its being relatively far removed from nuclear explosives. Experience of courses at different levels is outlined. Particular attention is given to the use of radiation chemical techniques in the training of postgraduate research students.Honorary AINSE Fellow, formely Post Retirement Fellow, ANSTO Isotope Technology. 相似文献
28.
Nilson PM Davies JR Theobald W Jaanimagi PA Mileham C Jungquist RK Stoeckl C Begishev IA Solodov AA Myatt JF Zuegel JD Sangster TC Betti R Meyerhofer DD 《Physical review letters》2012,108(8):085002
Time-resolved K(α) spectroscopy has been used to infer the hot-electron equilibration dynamics in high-intensity laser interactions with picosecond pulses and thin-foil solid targets. The measured K(α)-emission pulse width increases from ~3 to 6 ps for laser intensities from ~10(18) to 10(19) W/cm(2). Collisional energy-transfer model calculations suggest that hot electrons with mean energies from ~0.8 to 2 MeV are contained inside the target. The inferred mean hot-electron energies are broadly consistent with ponderomotive scaling over the relevant intensity range. 相似文献
29.
Sangster TP Wingate JE Burton L Teichert F Wilson ID 《Rapid communications in mass spectrometry : RCM》2007,21(18):2965-2970
Sources of analytical variation in high-performance liquid chromatography/mass spectrometry (HPLC/MS), such as changes in retention, mass accuracy or signal intensity, have been investigated to assess their importance as a variable in the metabonomic analysis of human urine. In this study chromatographic retention and mass accuracy were found to be quite reproducible with the most significant source of analytical variation in the data sets obtained being the result of changes in detector response. Depending on the signal intensity threshold used to define the presence of a peak a sample component could be present in some replicate injections and absent in others within the same run. The implementation of a more sophisticated data software analysis package was found to greatly reduce the impact of detector response variability resulting in improved data analysis. 相似文献
30.
S.P. Regan B. Yaakobi T.R. Boehly R. Epstein J.A. Delettrez V.Yu. Glebov V.N. Goncharov P.A. Jaanimagi J.P. Knauer F.J. Marshall R.L. McCrory D.D. Meyerhofer P.B. Radha T.C. Sangster V.A. Smalyuk J. Soures C. Stoeckl R.C. Mancini D.A. Haynes L. Welser-Sherrill H. Sawada 《High Energy Density Physics》2009,5(4):234-243
High-energy-density plasmas created in laser-fusion experiments are diagnosed with X-ray spectroscopy. Hans Griem, considered the father of modern plasma spectroscopy, provided an excellent foundation for this research. He studied the effect of plasma particles, in particular the fast-moving free electrons, on the Stark-broadening of spectral line shapes in plasmas [H. Griem, Phys. Rev. 125 (1962) 177]. Over the last three decades, X-ray spectroscopy has been used to record the remarkable progress made in inertial confinement fusion research. Four areas of X-ray spectroscopy for laser-fusion experiments are highlighted in this paper: Kα emission spectroscopy to diagnose target preheat by suprathermal electrons, Stark-broadened K-shell emissions of mid-Z elements to diagnose compressed densities and temperatures of implosion cores, K- and L-shell absorption spectroscopy to diagnose the relatively cold imploding shell (the “piston”) that does not emit X rays, and multispectral monochromatic imaging of implosions to diagnose core temperature and density profiles. The seminal research leading to the original X-ray spectroscopy experiments in these areas will be discussed and compared to current state-of-the-art measurements. 相似文献