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1.
Summary NAD(P)H fluorescence emission spectra are recorded from single living cells, by a recently developed multichannel microspectrofluorometric technique, in correlation with the intracellular microelectrophoretic addition of substrate (i. e., glucose-6-P). These spectra may be used as a reference basis in establishing the critical parameters to be followed when the same studies are extended to a variety of cells, submitted to various drug effects or physical treatments. The sum-spectra corresponding to channel by channel (wavelength by wavelength) summation of spectra obtained from various cells within a series, before and after addition of substrate, and their difference spectrum may be normalized and evaluated comparatively. The NAD(P)H emission maximum prior to addition of substrate seems to present a mixture of dehydrogenase-bound and free coenzyme. There is a suggestion that immediately after substrate, i. e., at 5 sec, an increase in free NADH is first observed. While the overall changes in fluorescence intensity associated with substrate are quite large (50–150% increase), the counts (i. e., an expression of photons) associated with shifts in the emission maximum (free vs. bound NAD(P)H changes) are at times barely above noise. Rapid microspectrofluorometry provides in principle the most direct approach for the identification of coenzyme bound to various dehydrogenases in single living cells, but further improvements in spectral resolution and signal-to-noise ratio are required, for a better definition of the spectral shifts which may be observed.
Zusammenfassung Mit Hilfe einer kürzlich entwickelten Mehrkanal-Mikrospektrofluorometer-Methode wurden von einzelnen lebenden Zellen nach intrazellulär mikroelektrophoretischer Substratzugabe (z. B. Glucose-6-P) NAD(P)H Fluoreszenz-Emissionsspektren aufgenommen. Diese Spektren können als Vergleichsbasis bei der Festsetzung der entscheidenden Parameter verwendet werden, wenn die gleichen Untersuchungen auf eine Reihe von Zellen ausgedehnt werden sollen, die verschiedenen Medikamenteffekten oder physikalischer Behandlung ausgesetzt werden. Die Summenspektren, die der kanalmäßigen (wellenlängenmäßigen) Summierung der Spektren von verschiedenen Zellen innerhalb einer Serie, vor und nach Substratzugabe entsprechen, sowie ihre Differenzspektren können normalisiert und vergleichsweise ausgewertet werden. Das NAD(P)H-Emissionsmaximum vor der Substratzugabe scheint ein Gemisch von freiem und dehydrogenasegebundenem Coenzym darzustellen. Unmittelbar nach Substratzugabe (d. h. nach 5 sec) ist ein Anstieg an freiem NADH das erste Mal zu beobachten. Während die mit dem Substrat einhergehenden Gesamtveränderungen der Fluoreszenzintensität recht groß sind (50–150% Anstieg), sind die Impulse (als Effekt der Photonen), die mit einer Verschiebung im Emissionsmaximum verbunden sind (Veränderungen von freiem und gebundenem NAD(P)H) zu manchen Zeiten kaum höher als das Rauschen. Die rasche Mikrospektrofluorometrie stellt im Prinzip die direkteste Methode zur Identifizierung von Coenzymen dar, die an verschiedenen Dehydrogenasen in einzelnen lebenden Zellen gebunden sind. Weitere Verbesserungen der Spektralauflösung und der Empfindlichkeit (signal-to-noise ratio) sind notwendig, um die Spektralverschiebungen, die beobachtet werden, besser auswerten zu können.相似文献
2.
G. J. Bengtsson K. Hansen J. Larsson W. Schade S. Svanberg 《Zeitschrift für Physik D Atoms, Molecules and Clusters》1991,22(1):397-399
Radiative lifetimes were determined for two short-lived states in neutral nitrogen. Following photo-dissociation and two-photon excitation employing the same UV source, excitation to higher states was performed with a distributed feedback dye laser (DFDL). The lifetimes were found to be τ(2p 24d 4 D 7/2)=17(3) ns and τ(2p 25s 4 P 5/2)=22(3) ns. 相似文献
3.
Aihara H Alston-Garnjost M Avery RE Barbaro-Galtieri A Barker AR Barnes AV Barnett BA Bauer DA Bengtsson H Bintinger DL Bobbink GJ Bolognese TS Bross AD Buchanan CD Buijs A Cain MP Caldwell DO Clark AR Cowan GD Crane DA Dahl OI Derby KA Eastman JJ Eberhard PH Eisner AM Enomoto R Erné FC Fujii T Gary JW Gorn W Hauptman JM Hofmann W Huth JE Hylen J Kamae T Kaye HS Kees KH Kenney RW Kerth LT Ko W Koda RI Kofler RR Kwong KK Lander RL Langeveld WG Layter JG Linde FL Lindsey CS Loken SC Lu A Lu X 《Physical review letters》1986,57(8):945-948
4.
V. Barci H. El-Samman A. Gizon J. Gizon R. Kossakowski B. M. Nyako T. Vertse S. Elfström D. Jerrestam W. Klamra Th. Lindblad T. Bengtsson 《Zeitschrift für Physik A Hadrons and Nuclei》1986,325(4):399-404
The effective moment of inertiaI eff (2) of132Ce,134Nd and136Nd produced in40Ar induced reactions has been deduced from continuumγ-ray spectra measured by sum spectrometer methods. Results concerning the deformation of these nuclei are obtained by comparison of the experimental data and calculations in the frame of a cranking Nilsson — Strutinsky model. 相似文献
5.
H.A. Michelsen F. Liu B.F. Kock H. Bladh A. Boiarciuc M. Charwath T. Dreier R. Hadef M. Hofmann J. Reimann S. Will P.-E. Bengtsson H. Bockhorn F. Foucher K.-P. Geigle C. Mounaïm-Rousselle C. Schulz R. Stirn B. Tribalet R. Suntz 《Applied physics. B, Lasers and optics》2007,87(3):503-521
We have performed a comparison of ten models that predict the temporal behavior of laser-induced incandescence (LII) of soot.
In this paper we present a summary of the models and comparisons of calculated temperatures, diameters, signals, and energy-balance
terms. The models were run assuming laser heating at 532 nm at fluences of 0.05 and 0.70 J/cm2 with a laser temporal profile provided. Calculations were performed for a single primary particle with a diameter of 30 nm
at an ambient temperature of 1800 K and a pressure of 1 bar. Preliminary calculations were performed with a fully constrained
model. The comparison of unconstrained models demonstrates a wide spread in calculated LII signals. Many of the differences
can be attributed to the values of a few important parameters, such as the refractive-index function E(m) and thermal and
mass accommodation coefficients. Constraining these parameters brings most of the models into much better agreement with each
other, particularly for the low-fluence case. Agreement among models is not as good for the high-fluence case, even when selected
parameters are constrained. The reason for greater variability in model results at high fluence appears to be related to solution
approaches to mass and heat loss by sublimation.
PACS 65.80.+n; 78.20.Nv; 42.62.-b; 44.05.+e 相似文献
6.
Aihara H Alston-Garnjost M Bakken JA Barbaro-Galtieri A Barnes AV Barnett BA Bengtsson H Blumenfeld BJ Bross AD Buchanan CD Chamberlain O Chien C Clark AR Cordier A Dahl OI Day CT Derby KA Eberhard PH Fancher DL Fujii H Fujii T Gabioud B Gary JW Gorn W Hadley NJ Hauptman JM Hofmann W Huth JE Hylen J Kamae T Kaye HS Kenney RW Kerth LT Koda RI Kofler RR Kwong KK Layter JG Lindsey CS Loken SC Lu X Lynch GR Madansky L Madaras RJ Maruyama K Marx JN Matthews JA Melnikoff SO Moses W Nemethy P 《Physical review letters》1985,54(4):270-273
7.
8.
Jan E. Åman Ingemar Bengtsson Narit Pidokrajt 《General Relativity and Gravitation》2006,38(8):1305-1315
The Hessian of either the entropy or the energy function can be regarded as a metric on a Gibbs surface. For two parameter families of asymptotically flat black holes in arbitrary dimension one or the other of these metrics are flat, and the state space is a flat wedge. The mathematical reason for this is traced back to the scale invariance of the Einstein–Maxwell equations. The picture of state space that we obtain makes some properties such as the occurence of divergent specific heats transparent.Supported by VR. 相似文献
9.
Ragnar Bengtsson 《Hyperfine Interactions》1992,75(1-4):3-22
A survey is made of new regions of nuclei, which may become accessible to nuclear orientation experiments as the on-line technique
matures. Basic nuclear properties that can be investigated by means of nuclear orientation are briefly reviewed. Examples
of systematic use of nuclear moments for revealing nuclear properties are given as is an example of of the combined use of
low-spin nuclear orientation data and high-spin heavy-ion reaction data. 相似文献
10.
M. Mamor Y. Fu O. Nur M. Willander S. Bengtsson 《Applied Physics A: Materials Science & Processing》2001,72(5):633-637
We investigate, both experimentally and theoretically, current and capacitance (I–V/C–V) characteristics and the device performance
of Si/SiO2/Si single-barrier varactor diodes (SBVs). Two diodes were fabricated with different SiO2 layer thicknesses using the state-of-the-art wafer bonding technique. The devices have very low leakage currents (about 5×10-2 and 1.8×10-2 mA/mm2) and intrinsic capacitance levels of typically 1.5 and 50 nF/mm2 for diodes with 5-nm and 20-nm oxide layers, respectively. With the present device physical parameters (25-mm2 device area, 760-μm modulation layer thickness and ≈1015-cm-3 doping level), the estimated cut-off frequency is about 5×107 Hz. With the physical parameters of the present existing III–V triplers, the cut-off frequency of our Si-based SBV can be
as high as 0.5 THz.
Received: 9 February 2001 / Accepted: 9 February 2001 / Published online: 23 March 2001 相似文献