ライフサイエンスコーパス: plane wave

コーパス検索結果 (１語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します

1 riance of the speed of light only applies to plane waves.

2 nsional stochastic model of random-direction plane waves.

3 smon modes that are difficult to excite with plane waves.

4 originate from fine interference of multiple plane waves.

5 oth near-field and far-field properties with plane wave and lumped port sources.

6 We present explicit solutions for plane waves and linear excitations, and identify the dif

7 ta-band activity is dominated by propagating plane waves and spatiotemporal structures, which we call

8 This activity consists of plane waves and spiral-like waves, as well as more compl

9 red from long, thin objects illuminated by a plane wave at any angle.

10 NMR with first-principles calculations using plane-wave basis sets.

11 In perfect crystals, normal modes are plane waves, but they can be complex in disordered syste

12 me but lose both longitudinal and transverse plane-wave character at a common energy near the Boson p

13 An 18-MHz linear array was used to acquire plane-wave data at absolute frame rates >/=10 kHz using

14 of theory, including both Gaussian-based and plane wave density functional theory (DFT), second-order

15 We present results of plane-wave density functional theory (DFT) based investi

16 as well as its surface mobility, by means of plane-wave density functional theory (DFT) calculations.

17 Employing a plane-wave density functional theory formalism, we inves

18 Plane-wave density functional theory has been applied in

19 P-dependent protein kinase are calculated by plane-wave density functional theory, starting from stru

20 a and phosphoric acid are investigated using plane-wave density functional theory.

21 electron full-potential linearized augmented plane wave (FLAPW) approach across various functionals f

22 with the full-potential linearized augmented plane wave (FLAPW) method show that the band gap increas

23 The plane waves have an average phase gradient of approximat

24 The normal modes take the form of plane waves hybridized with localized short wavelength f

25 switchable with the polarization of uniform, plane wave illumination, and its magnitude is comparable

26 ted for a quantitative analysis of SPR under plane-wave illumination and a finite-difference time-dom

27 Here, a plane-wave imaging method was used to obtain high-speed

28 des more selective than circularly polarized plane waves in preferentially exciting single enantiomer

29 eous unit cells can turn a normally incident plane wave into a self-accelerating beam on the prescrib

30 equilibrium Bose-Einstein distribution at in-plane wave number k parallel > 0 and a nonequilibrium co

31 ndles relatively simple light beams, such as plane waves or Gaussian beams.

32 lly periodic firing patterns are composed of plane waves (or bands) drawn from a discrete set of orie

33 The most familiar example is that of a plane wave propagating in free space.

34 , we obtained good agreement with theory for plane waves propagating in a direction perpendicular to

35 Plane waves propagating parallel to myocardial fibers pr

36 el to fibers (10.6 +/- 4.2 mm) compared with plane wave propagation (ie, without pivoting) parallel t

37 n be explained by a large decrease in the in-plane wave propagation length that occurs near the molec

38 ring reentry was compared with lambda during plane wave propagation transverse and longitudinal to ca

39 pic bidomain nature of cardiac tissue during plane wave propagation.

40 es chemical shift calculations that employ a plane-wave pseudopotential approach.

41 ping a spatially localized basis, compressed plane waves, that spans the eigenspace of a differential

42 The coupling of an electromagnetic plane wave to a thin conductor depends on the sheet cond

43 Our approach generalizes the concept of plane waves to an orthogonal real-space basis with multi

44 ce and that of the second mechanism is an in-plane wave vector matching when the Dirac points of the

45 r new wavelet formation after collision of a plane wave with an obstacle in an otherwise homogeneous

WebLSDに未収録の専門用語（用法）は "新規対訳" から投稿できます。