ライフサイエンスコーパス: numerical aperture

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 elements to enable even larger diameters and numerical apertures.

5 Using a high numerical aperture (1.4 NA) oil immersion objective, axi

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

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

8 c and dual-polarization edge detection, with numerical apertures above 0.35 and spectral bandwidths o

9 The individual microlenses maintain a high numerical aperture and are used to create digital light

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

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

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

13 d microscope is considered determined by the numerical aperture and wavelength of light, approximatel

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

15 so-called 4Pi geometry doubles the available numerical aperture, and coupling this with interferometr

16 a the excitation intensity, epi-illumination numerical aperture, and integration time.

17 ystems with high focusing efficiencies, high numerical apertures, and low chromatic focusing errors,

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

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

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

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

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

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

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

25 les and their performance for designing high numerical aperture devices is not well quantified.

26 ent metasurface designs in implementing high numerical aperture devices.

27 s accompanied by performance metrics-such as numerical aperture, efficiency, isotropy, and polarizati

28 of designing a cavity for coupling to a low numerical aperture fibre in the near field.

29 The requirement of high numerical aperture for sub-surface ablation, in addition

30 rger nerves, focusing lenses would require a numerical aperture [Formula: see text].

31 fficient value of 4), extended the synthetic numerical aperture from 0.41 to 0.99, and provided a two

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

33 The metalens exhibits a numerical aperture greater than 1.0, enabling efficient

34 ves having a high-enough detection aperture (numerical aperture >n(2)) and be separated in the back f

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

36 ith visible light in combination with a high numerical aperture is non-trivial.

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

38 Here, we present a high-numerical aperture, lens-based resonator that pushes the

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

40 Among them, the 400-mum diameter, 0.02-numerical-aperture metalens is used to demonstrate full-

41 for the estimation of the efficiency of high numerical aperture metasurfaces.

42 chieved for 15mum thick, 90mum diameter, 0.3 numerical aperture microlenses.

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

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

45 ve all obstructing hardware - ideal for high-numerical-aperture microscopy.

46 anar THz optical elements, namely (i) a high Numerical Aperture (N.A.), broadband aberration rectifie

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

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

49 in critical power and decrease in transition numerical aperture (NA) is predicted to occur with a dro

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

51 lution, enabled by the integration of a high numerical aperture (NA) objective lens (NA = 0.64) and t

52 th at 532 nm and detection optics with a 0.6 numerical aperture (NA) objective lens, this value repre

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

54 ns are limited by the requirements for large numerical aperture (NA) objectives, fluorescence intermi

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

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

57 with a long working distance (WD) and a high numerical aperture (NA).

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

59 olithography, as they uniquely feature large numerical apertures (NAs), immersion media compatibility

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

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

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

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

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

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

66 er that utilizes a gravity-driven flow, high numerical aperture objective, and micrometer-sized flow

67 With a confocal microscope and a 40x/1.3 numerical aperture objective, we achieved a uniform sub-

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

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

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

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

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

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

74 ence from the constituent atoms using a high-numerical-aperture objective.

75 However, these methods rely on high numerical aperture objectives and cannot resolve crowded

76 ution of wide-field images acquired with low-numerical-aperture objectives, matching the resolution t

77 g the resolution that is acquired using high-numerical-aperture objectives.

78 a single layer of TiO(2) nanofins and has a numerical aperture of 0.2 with a diameter of 26.4 um.

79 h an average efficiency of 77.1%-88.5% and a numerical aperture of 0.24-0.1.

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

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

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

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

84 experimentally demonstrate a metalens with a numerical aperture of 0.78 and a measured focusing effic

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

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

87 that the presence of absorption and the high numerical aperture of infrared microscopes does not expl

88 system that was limited in resolution by the numerical aperture of its objective lens.

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

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

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

92 er, its spatial resolution is limited by the numerical aperture of the imaging objective and the scat

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

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

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

96 an improve the effective brightfield imaging numerical aperture of the objectives from 0.23 to 0.3, a

97 e wavelength of the used wave packet and the numerical aperture of the optical system.

98 of 16 mum, 66 mum, 200 mum, and 400 mum, and numerical apertures of 0.27, 0.11, 0.04, and 0.02, respe

99 nstrated diffraction limited performance for numerical apertures of 0.27, 0.11, and 0.06, with averag

100 h a 10-millimeter focal length that supports numerical apertures of up to 0.05 and used it to focus u

101 A high numerical aperture oil-immersion objective was used to a

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

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

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

105 These high numerical aperture optics enable to distinguish sample l

106 ke most previous techniques, here we use low numerical aperture optics resulting in long manipulation

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

108 Owing to its high numerical aperture optics, this microscope achieves late

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

110 roorganisms, using very low laser powers and numerical aperture optics.

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

112 metalenses working in the visible with high numerical aperture, poly-chromatic focusing, and large d

113 band stop filters, beam deflectors and high numerical aperture radial lenses with measured quality f

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

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

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

117 Numerical apertures upwards of 0.47 are also achieved at

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