ライフサイエンスコーパス: reflector

1 esonant metasurface and a metallic thin-film reflector.

2 plasmonic structures and a distributed Bragg reflector.

3 ary of resonator and the "close" boundary of reflector.

4 lements, such as the all-angle acoustic back reflector.

5 r SOI structures without the use of any back-reflector.

6 in its ability to act as a structural light reflector.

7 tetrafluoroethylene (PTFE) cell as a diffuse reflector.

8 tandard solution and deposited onto a quartz reflector.

9 t spread function (PSF) was assessed off the reflector.

10 oscopy, radar, and frequency scanned antenna reflectors.

11 etic waves (directional emitter) without any reflectors.

12 d in layers, together acting as interference reflectors.

13 ng of ballistic energy carriers by pyramidal reflectors.

14 multimode cavity between two acoustic Bragg reflectors.

15 terference of light with intracellular Bragg reflectors.

16 d photoreceptors are positioned behind these reflectors.

17 vskite transition is too wide to cause sharp reflectors.

18 nside diameter: 5.5 m), reflected by a retro-reflector and recorded using a fast thermoelectrically c

19 ber of seismic observations, such as the D'' reflector and the high degree of seismic anisotropy with

20 h, we introduce an integrated photonic solar reflector and thermal emitter consisting of seven layers

21 of angle-switchable metagratings as splitter/reflector and transparent/opaque mirror.

22 ring methods to make direct analogues of the reflectors and anti-reflectors found in nature.

23 ectronic barriers to realize tunable plasmon reflectors and phase retarders in future graphene-based

24 ally applied as conducting circuits, plasmon reflectors and phase retarders.

25 to 2.7, allowing efficient distributed Bragg reflectors and waveguides to be fabricated.

26 ent densities of 25 mA/cm(2) with a backside reflector, and simulations further show that such stacki

27 eased at the 330-kilometer and 450-kilometer reflectors, and S-wave impedance decreased near 200 kilo

28 this unique synthesis platform include Bragg reflectors, antireflective coatings, and chiral metamate

29 to 18 kilometers near where the decollement reflector apparently terminates.

30 we interpret a negative-polarity sedimentary reflector approximately 500 meters above the subducting

31 Bracketing is possible with reflectors as close as 2.6 cm.

32 ove and below, respectively, reveal multiple reflectors beneath Central America and East Asia, two ar

33 The three-dimensional shape of this micro-reflector can be tuned as a function of time, vapor temp

34 ering nanopost on top of a distributed Bragg reflector, capable of providing a nearly 2pi nonlinear p

35 laser scanning microscope by placing a plane reflector close to the specimen.

36 Fish have evolved biogenic multilayer reflectors composed of stacks of intracellular anhydrous

37 into the iridocyte to form a potential Bragg reflector consisting of an array of narrow, parallel cha

38 abricating an all-dielectric omnidirectional reflector consisting of multilayer films.

39 Instead we argue that the seismic layer 2A reflector corresponds to an alteration boundary that can

40 This predecollement reflector corresponds to unusual prism structure, morpho

41 antum dots (QDs) in planar distributed Bragg reflector (DBR) cavity with an average position uncertai

42 Distributed Bragg reflectors (DBRs) are essential components for the devel

43 Planar microcavities with distributed Bragg reflectors (DBRs) host, besides confined optical modes,

44 ammogram and radiograph of the specimen, and reflector depth was measured on the mammogram.

45 ed increased distance between the target and reflector distance of greater than 1.0 cm (range, 1.1-2.

46 Mean mammographic target to reflector distance was 0.3 cm.

47 Target to reflector distance was measured on the mammogram and rad

48 d photonic properties, functioning as chiral reflector/filters and structural colour matrices.

49 ethylene glycol droplets, which act as micro-reflectors for fluorescent light.

50 bsorbers/emitters for visible light and good reflectors for IR light, which are desirable for efficie

51 direct analogues of the reflectors and anti-reflectors found in nature.

52 elocity structure, earthquake locations, and reflector geometry in northwest Washington state.

53 MIRUS system (S1) and 15 cm from the filter-Reflector group (S2).

54 i Scout (Cianna Medical, Aliso Viejo, Calif) reflector-guided localization and excision of breast les

55 uch as waveguides, lenses, beamsplitters and reflectors have been implemented by structuring metal su

56 Here we report a linearly polarizing reflector in a stomatopod crustacean that consists of 6-

57 backscatter coefficient and is the dominant reflector in rd retinas that lack photoreceptors.

58 al, it can be used to design omnidirectional reflectors in many frequency ranges of interest.

59 uctive interference from intracellular Bragg reflectors in specialized skin cells called iridocytes.

60 These protein-based reflectors in squids provide a marked example of nanofab

61 s 45-kilometer depth contour occur below the reflector, in the subducted oceanic mantle, consistent w

62 The reflector, interpreted to be the crust-mantle boundary (

63 An alternative hypothesis is that the reflector is associated with an alteration boundary with

64 We suggest that the observed sharp D'' reflector is caused by a rapid change in seismic anisotr

65 Here we show that, although the layer 2A reflector is imaged near the top of the sheeted dyke com

66 the formation rate and shapes of these micro-reflectors is presented, along with a ray tracing model

67 ed over young oceanic crust commonly image a reflector known as 'layer 2A', which is typically interp

68 ating distributed feedback-distributed Bragg reflector lasers.

69 the frequency bandwidth corresponding to the reflector loss at -10 dB was up to 5.8 GHz within the fr

70 defined at half peak height) was observed in reflector mode.

71 profiles and may be responsible for seismic reflectors observed at 1,000- to 1,400-km depth.

72 ed films, the transition from transmitter to reflector occurs when the sheet resistance is approximat

73 er can serve as a strong frequency-selective reflector of magnetic fields when operating in the near-

74 rating a hybrid conductive distributed Bragg reflector on the back side of the transparent conducting

75 ayed in nature result from either multilayer reflectors or linear diffraction gratings.

76 Metals are generally considered good reflectors over the entire electromagnetic spectrum up t

77 Twenty patients had two or three reflectors placed for bracketing or for localizing multi

78 and excision of breast lesions by analyzing reflector placement, localization, and removal, along wi

79 pathologic analysis helped verify target and reflector removal.

80 flexible upright waveguides and self-aligned reflectors, respectively.

81 lly consist of four packets of finely spaced reflectors separated by homogeneous interpacket regions

82 peptides are identified in the (+) ion MALDI reflector spectrum by the presence of [MH-H3PO4]+ and [M

83 ramid photonic crystal and a rear dielectric/reflector stack.

84 indicates that this condition obtains for a reflector that is a solid over fluid interface; it is no

85 The photograph shows a polymer reflector that mimics the colour and underlying molecula

86 zone is frequently identifiable as a smooth reflector that runs parallel to the sea floor.

87 how strong P-to-S converted reflections from reflectors that are aligned at a depth of approximately

88 wavelength dielectric layer closed by a gold reflector the highest absorptance is attainable at perpe

89 For a conical reflector, the cylindrical symmetry is echoed in an angu

90 ction respectively as a compact director and reflector, the second harmonic radiation is deflected 90

91 atmospheric pressure ion mobility orthogonal reflector time-of-flight mass spectrometer (IM(tof)MS) t

92 atmospheric pressure ion mobility orthogonal reflector time-of-flight mass spectrometer (IM(tof)MS) t

93 ion mobility spectrometry with an orthogonal reflector time-of-flight mass spectrometer to analyze ch

94 wise internally trapped light and multilayer reflectors to control the direction of light emission.

95 The reflector was simply constructed as a stack of nine alte

96 Based on these self-assembled micro-reflectors, we experimentally demonstrate ~2.5-3 fold en

97 Target and reflector were localized intraoperatively by one of two

98 The hybrid conductive distributed Bragg reflectors were designed to be transparent to the long-w

99 123 (100%; 95% CI: 96.4%, 100%) targets and reflectors were excised.

100 ies comparable to those of the best metallic reflectors were obtained.

101 ve, infrared-activated, electromagnetic wave reflectors were percutaneously inserted adjacent to or w

102 000 m using virtually any solid surface as a reflector, whilst also being highly portable.

103 e can reconcile seismic observation of a D'' reflector with recent experiments showing that the width

104 Laterally continuous weak reflectors with tens of kilometers of topography were de