ライフサイエンスコーパス: numerical aperture

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 to obtain due to steric constraints at high numerical aperture.

2 cond beams and a water objective with a high numerical aperture.

3 is, proved to be independent of focus and of numerical aperture.

4 Owing to optical aberrations and lower numerical apertures, a main class of microlens, gradient

5 We identify stray reflections and high-numerical aperture aberrations of the TIRF objective as

6 The requisite high numerical aperture and exogenous contrast agents that en

7 ethodology offers high design flexibility in numerical aperture and focal length, and is readily exte

8 ope objectives of low magnification have low numerical aperture and therefore have too little depth r

9 ity using concave fiber lenses with matching numerical apertures and diameters.

10 n that in the human eye because of its large numerical aperture (approximately 0.43).

11 The compatibility with the use of high numerical aperture (approximately 1.0) objectives is an

12 igh efficiency and small spot size (or large numerical aperture) are discussed.

13 ing to the use of objective lenses with high numerical aperture, brighter fluorophores and more sensi

14 gital micromirror device together with a low numerical aperture collecting system, we are able to pro

15 ace on probe emission and the effect of high numerical aperture collection of light.

16 n limited to use with low-magnification, low-numerical-aperture configurations.

17 s achieved by the use of a 1-mm-diameter 0.5 numerical aperture gradient index objective lens and one

18 field curvature correction that allows high numerical aperture imaging and near-diffraction-limited

19 h collection efficiency (48%+/-5% into a 0.4 numerical aperture lens, close to the theoretically pred

20 trum and to enable applications such as high numerical aperture lenses, color holograms, and wearable

21 hat allows imaging the particles with a high numerical aperture microscope objective.

22 le-photon avalanche diode (SPAD), and a high-numerical-aperture microscope objective mounted in an ep

23 ction of complex optical aberrations at high numerical aperture (NA) and a 14-ms update rate.

24 To demonstrate the concept, a 0.5 numerical aperture (NA) confocal fluorescence microscope

25 bwavelength resolution imaging requires high numerical aperture (NA) lenses, which are bulky and expe

26 ive based that employ expensive special high numerical aperture (NA) objectives or prism based that r

27 hip microscopy, such as the achievement of a numerical aperture (NA) of approximately 0.8-0.9 across

28 the optical system is directly linked to the numerical aperture (NA) of the microscope objective, whi

29 f specimens, performing very close to a high numerical-aperture (NA) benchtop microscope that is corr

30 cement is observed utilizing an intermediate numerical aperture objective (NA = 0.7), necessary for b

31 transverse plasmon absorption using a large numerical aperture objective as out-of-plane plasmon osc

32 smon resonance (SPR) microscope using a high numerical aperture objective from a commercially availab

33 e in which the specimen is coupled to a high numerical aperture objective lens by an immersion fluid.

34 ntenna is reversed and then gathered by high numerical aperture objective lenses.

35 Here we use a high numerical aperture objective that avoids all the limitat

36 nn configuration in a microscope with a high-numerical-aperture objective (1.45) together with confoc

37 We show that by using a high-numerical-aperture objective (1.65) and high-refractive-

38 t permits the use of a room-temperature high-numerical-aperture objective lens to image frozen sample

39 use the index-matching fluids used with high-numerical-aperture objective lenses can conduct heat fro

40 ting position detection methods require high-numerical-aperture objective lenses, which are bulky, ex

41 queous solution using an oil-immersion, high-numerical-aperture objective.

42 he field of view of an objective lens with a numerical aperture of 0.45.

43 zation insensitive metasurface lenses with a numerical aperture of 0.46, that focus light at 915 and

44 nstrument using a compact lens assembly with numerical aperture of 0.5 to achieve a working distance

45 on efficiency of 68% +/- 6% into a lens with numerical aperture of 0.65, and simultaneously exhibitin

46 bule in aqueous suspension and imaged with a numerical aperture of 1.4 had a peak retardance of 0.07

47 ely 24 mm(2) field-of-view with an effective numerical aperture of approximately 0.2.

48 lambda = 600 nm and an objective lens with a numerical aperture of NA = 1.49), limiting the resolutio

49 Conversely, injecting light over the full numerical aperture of the fiber results in light emissio

50 bda is the wavelength of light and NA is the numerical aperture of the illumination and imaging lense

51 eased when the filament was defocused or the numerical aperture of the imaging system was decreased.

52 ambda/NA (lambda = wavelength of light, NA = numerical aperture of the objective) and at the axial pl

53 ssion wavelength of the single molecule, the numerical aperture of the objective, the efficiency of t

54 orating these birefringent elements and high-numerical-aperture oil immersion objectives could outper

55 The optical system is completed by a low-numerical-aperture optic that can have a long working di

56 Microscope objective or high numerical aperture optical fiber were used for collectio

57 approximately 600 ps) are focused using high numerical aperture optics to submicrometer focal spots,

58 analyte are detected using inexpensive, low-numerical aperture optics.

59 eld from a photoreaction site formed by high-numerical-aperture optics, with positively charged (and

60 e-cell SIM through two approaches: ultrahigh numerical aperture SIM at 84-nanometer lateral resolutio

61 I and incorporating an objective with a high numerical aperture, spot sizes of 10-20 mum were readily

62 each point along the lens, leading to a high numerical aperture that is limited only by its extent.

63 collimation and collection by increasing the numerical aperture with a plano-convex hyper-hemispheric

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。