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词汇 example_english_spectrum
释义

Examples of spectrum


These examples are from corpora and from sources on the web. Any opinions in the examples do not represent the opinion of the Cambridge Dictionary editors or of Cambridge University Press or its licensors.
The spectra are in relative units and thus provide a comparison of the intensities of different emission bands.
More specifically, power spectra are computed for each of the 12 electrode sites to examine power in various frequency bands.
Each filter introduces a peak in the magnitude spectra determined by the pass-band centre frequency and by the formant bandwidth.
I will now look at the formant spectra (or modes) of the durations for each protagonist.
The perceptual dimensions underlying similarity judgments between pairs of timbres are based on the amplitude pattern of the spectra.
The spectra can be roughly approximated by single temperature distributions for each intensity.
A common sense approach to peak picking in two-, three-, and four-dimensional spectra using automatic computer analysis of contour diagrams.
In this way, we can quantitatively assess the uncertainties associated with distinguishing between glasses and certain phyllosilicates in thermal infrared spectra of multimineralic materials.
One of the major limitations in this direction is the difficulty of predicting or measuring two-photon absorption spectra of the fluorescent molecules used.
Also, we observe that there is no qualitative change in the spectra when the sign of the chirp is changed while its magnitude is not.
However, based on the current experiments, these lamps do not appear to be able to produce smooth and easily interpretable spectra of plants under stress.
Variance of the distributions of energy levels and of the transition arrays in atomic spectra.
The spectra have been corrected for a background signal present in oxidized hygrogenosomes, and are adjusted to the same protein concentration.
We obtain the dispersion relations and the frequency spectra of these waves separately by using linear approximations.
The emission spectra corresponding to these two kinds of beam movement are quite different.
A sample of 622 daylight spectra was taken, and subjected to an eigenvector analysis.
X-ray spectra from high intensity subpicosecond laser produced plasmas.
Simple technique for measurement of energy spectra of ions from laser produced plasma.
In fact, the laser spectra obtained after the laser-gas interaction region are time-integrated.
The ionization 0 dissociation mechanism can be studied by observing the fragmentation patterns in the mass spectra obtained.
The other peaks in the spectra are salt adducts and other contaminants that are not representative of the presence of additional oligomers.
Variations within the electrorotational spectra of fertilized eggs are also reported and such variability may be due to structural changes during embryonation.
The radiative proper ties and emitted spectra are computed self-consistently with respect to the emitter structure and the per turbers.
The infrared spectra of the aminoacrylonitrile, both in the gas and condensed phases, were recorded in the range 500-4000 cmx1.
The corresponding ion of mass 166 is omitted throughout the spectra.
From these spectra it is possible to follow the absorbance of each polyyne species after irradiation.
The spectra were recorded in the wavelength region 200-400 nm.
We would like also to study the dynamic effect on the observed spectra.
Timbrally, all gongs produce inharmonic spectra, but the three types of gongs used in this piece feature different spectral characteristics.
Fully automated sequence/specific resonance assignment of hetero/nuclear protein spectra.
Determination of protein secondary structure using factor analysis of infrared spectra.
Particularly interesting is the contribution of an a-helix to the spectra of lysozyme and a-lactalbumin.
The solid, dashed and dash-dotted lines illustrate the spectra obtained by us with a = 2.5, a = 3.5 and a = 1.5, respectively.
The stability criterion and the characteristic oscillation frequency of the zonal flow are determined in terms of the spectra of turbulent fluctuations.
Figure 4 shows, comparatively, the obtained electrostatic and magnetic fluctuation spectra.
The abstracted thematic statements were further organized into nine thematic sections: three corresponding sections in each of the three spiritual health spectrums.
The reader who wants to know something about oceanic geoid mapping or wave spectra, for example, will need to look elsewhere.
They correspond to the measured spectra 6a, 6b, and 6c.
The values of the electron beam energy and energy spread were fixed and equal to the values obtained from the multiple fits to the spectra.
Decomposition of measured spectra into individual spectral lines represents an example of a global optimization problem, which cannot be efficiently solved by traditional techniques.
Spectromorphology here is a broad concept, but it can be described as the perceptual analysis of time-varying aural spectra.
As a result, continuous inharmonic spectra have a tendency to disperse into streams.
At the most extreme end of this continuum is a sine tone (with no spectra), while at the other end is noise.
We have used a combination of techniques for determining parameters that enable model outputs to closely match the time-varying spectra of original acoustic sounds.
In section 4 we repor t the spectra observed and discuss their detailed features.
Five spectra (or dimensions) of psychopathology were assessed: depression, anxiety, substance dependence, persistent antisocial behaviour, and psychosis.
The sensitivity of the emission spectra to the electron temperature, the atom number density, and the presence of hot electrons has been explored.
88 strength of these lines decreases, so that the hollow atom transitions make relatively little contribution to the emission spectra seen at the final time.
An analytical expression for electron spectra needs additional studies.
We describe in the following the general elaboration procedure that applies to all spectra.
Finally, it is shown how frequency spectra and the development of instabilities are changed by increasing the strength of the external magnetic field.
Moreover, well-separated poloidal modes give rise to displaced spectra, so that part of the bounce integral is to be excluded when evaluating the dielectric response.
Furthermore, the individual terms contributing to the transfer spectra were studied.
The present study focuses on the degeneracy of spectra between point and continuum, or continuum and continuum which has never been treated so far.
Accordingly, it is of practical interest to examine the wave spectra that span from long to short wavelengths.
The process was repeated until all spectra had been predicted in this manner.
The problem is especially acute for metameric reflectances, which have different spectra that match under one light but not under another.
Detection of pulmonary vascular disease in infants using input impedance spectra.
Particular attention will be paid to the case where one of the spectra is pure point.
After introducing the dynamical systems and discussing their basic topological features, we will focus on studying the relationship between these two spectra.
The normalized power spectra are shown on a linear scale in figure 22.
On the spectra of randomly perturbed expanding maps.
The spectra were then calculated and ensemble averaged over the 100 records (200 degrees of freedom).
Reynolds number for the runs whose spectra are shown in figure 12.
Power spectra were obtained by averaging sampled records over many periods of oscillation.
One-dimensional energy spectra were obtained in the 30, 100 and 300ppm solutions with the conical hot-film probe.
However, quantitative comparison is required in order to definitely determine whether the spectra are identical to those in the pure solvent.
To get better comparisons with experiment, one-dimensional spectra must be plotted.
In this analysis complete energy-transfer spectra for many different times will be given first.
Cross-correlated spectra confirm that the flow is non-axisymmetric.
We study multifractal spectra of a simple class of interval transformations with a neutral fixed point.
At 8 cmx1 spectral resolution, the quality of spectra is quite similar to that at 4 cmx1 resolution.
They have much harder photon spectra but also a lower rate and lower total energy.
The inverse reflectance spectra can be equated with emittance spectra in most cases.
Dotted and dashed-dotted lines respectively respresent the model and the data spectra.
Other parameters, including receiver gain, were adjusted to obtain the most resolved spectra.
Both spectra are the result of the superposition of two triplets.
In this paper we test two simple hypotheses: (1) that -diversity has a stronger influence than - diversity on pollen spectra.
427 ratio in men with photopigment spectra derived from genetics.
Separate axon diameter spectra were determined at different locations in cross sections of the two specimens.
All reflectance spectra were sampled at 10-nm intervals, from 410 nm to 710 nm.
Simple exponential functions describing the absorbance bands of visual pigment spectra.
They are merely a consequence of the asymmetries in surface reflecting properties induced by the limited way biological photoreceptors sample physical spectra.
Composing with spectra would place music outside the world of linear time (p. 40), and precisely this would connect music with spiritual experience.
Therefore, it is expected that it can change the spectra of volume and surface waves in degenerate and nondegenerate plasmas.
The original signals being measured in time, these observational spectra are measured in frequency.
Now we formulate and prove several lemmas concerning the actions with absolutely continuous spectrums.
The dipole moments of all the protonated molecules are large enough for the radio spectra to be seen.
The emission spectra of the impacts were observed with high-speed spectrometers.
The general philosophy is to derive appropriate scaling factors by adjusting the calculated spectra to the spectroscopic values of a number of representative molecules.
Recorded spectra were the result of absorption and scattering.
However, the spectra have been roughly normalized so that the most intense bands in each are similar in intensity, for comparison purposes.
However, those spectra, in addition, contain large portions of power within considerably higher frequencies, which cannot be explained by the one-dimensional model.
The latter is consistent with the saddle-shaped spectra, which suggest the presence of excess argon.
The spectra obtained with the turbulent pipe flow nozzle, in general, resembled those obtained with the shorter nozzles.
Examining the electronics, we see that the system frequency response was limited by the low-pass filter used to prevent aliasing of the spectra.
The kinematical properties leading to such spectra are discussed.
The spectra viewed at an angle of 608 to the target were analyzed to estimate the profiles of different characteristics within the plasma.
Since the flow is inhomogeneous in the radial direction, radial spectra cannot be calculated.
We first checked that the frequency obtained in the spectra only depends on the rotation rate and the stratification and not on the experimental procedure.
These examples are from corpora and from sources on the web. Any opinions in the examples do not represent the opinion of the Cambridge Dictionary editors or of Cambridge University Press or its licensors.
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