ライフサイエンスコーパス: absorption edge

1 e backbone yields a sharp longest wavelength absorption edge.

2 ponses at 1064 and 532 nm and a short 180 nm absorption edge.

3 structure range beyond the onset of the iron absorption edge.

4 s diffraction (MAD) applied to the bromine K-absorption edge.

5 ow-energy polaritons and a steepening of the absorption edge.

6 lastic x-ray scattering study at the Ru L(3) absorption edge.

7 solution to distinguish individual elemental absorption edges.

8 fluorescence setup at certain energies near absorption edges.

9 has permitted XAS studies at both Cu and Se absorption edges.

10 neously probes the I-4d and Br-3d core-level absorption edges.

11 ayer compounds exhibit a blue shift in their absorption edge (0.6-1.2 eV), due to the quantum confine

12 unds generate a very large blue shift in the absorption edge (1.0-2.0 eV) due to the strong QCE.

13 5 x KDP (600 x alpha-SiO2), and the shortest absorption edge (250 nm) of reported materials with a st

14 single pulse streaking reaching the carbon K-absorption edge (284 eV) by utilizing intense two-cycle

15 (n=2) has a much longer carrier lifetime and absorption edge (580 nm, 2.13 eV) in comparison to DJP(n

16 ond lengths and Debye-Waller factors at each absorption edge allowed us to rule out simple models for

17 h those collected at energies near the X-ray absorption edge, aluminum is highlighted.

18 inent excitonic features at 3.22 eV near the absorption edge and additional optical transitions at hi

19 Through the comparison by iron K-edge x-ray absorption edge and extended fine structure analyses of

20 with NC n-doping, including a bleach at the absorption edge, appearance of a new IR absorption band,

21 Simultaneously, a new absorption edge appeared at 1.1 eV below the conduction

22 The capability of resolving the absorption edge applies to a wide range of research area

23 xpected to reveal strong modulation in their absorption edge as a function of selenium content, x(Se)

24 5)I(16) and a direct bandgap with an optical absorption edge at 2.0 eV.

25 The material exhibits a sharp optical absorption edge at 2.70 eV and a strong broad orange lig

26 g the absorption into the NIR region with an absorption edge at 998 nm.

27 The multilayer films only show a sharp absorption edge at about 250 nm, indicating a high trans

28 BaB2 O4 , respectively, and exhibits a short absorption edge below 200 nm.

29 that achieves the balance between a short UV absorption edge, below 190 nm, and a large SHG response,

30 ese new devices include precisely adjustable absorption edges between 0.87 and 1.03 eV, low ideality

31 ccurring on the high-energy side of an X-ray absorption edge, can be used to identify interatomic dis

32 data collected near the respective elemental absorption edges confirm metal substitution.

33 um efficiency data for wavelengths above the absorption edge, coupled with a strong sharp photolumine

34 We show that the shift of the main visible absorption edge does not constrain the point of band gap

35 The unusually intense 8983 eV Cu K-absorption edge feature in reduced and substrate-bound-r

36 he X-ray energy used coincides with an X-ray absorption edge in one of the constituent elements in th

37 ely distributed surface pigment with a sharp absorption edge in the red part of the visible spectrum,

38 ranging from 2.8 to 13.5 x KDP, and exhibit absorption edges in the mid- to deep-ultraviolet regime.

39 perimental UV/Vis measurements of the Tix Oy absorption edges in these species and reveal that molecu

40 The energy is chosen close to an X-ray absorption edge, in order to give the maximum contrast b

41 The position of the absorption edge indicates that this site is in the oxida

42 osphorene at energies that closely match the absorption edge, indicating that they are direct bandgap

43 t] Stokes shift regarding the fundamental QW absorption edge, indicating the exciton localisation ben

44 Specifically, absorption-edge irradiation of the 2D poly(arylenevinyle

45 ents can be clearly distinguished and the Ni absorption edge is identified.

46 ng X-ray scattering differences at elemental absorption edges, is developed to quantitatively determi

47 skitoids having direct bandgaps with optical absorption edges less than 2.2 eV.

48 ain concentration measurement using spectral absorption edge markers.

49 Control of the fundamental absorption edge of a quantum dot with an applied electri

50 n the photon energy is tuned to a core-level absorption edge of an atom neighboring the emitting atom

51 ith incident energy lower and close to the K absorption edge of both elements.

52 1.7 A resolution with a wavelength near the absorption edge of bromine.

53 via diffraction of a probe pulse tuned to an absorption edge of Gd.

54 two monochromatic images, above and below an absorption edge of interest.

55 constructions at X-ray energies around the L absorption edge of iron demonstrates the advantages of t

56 at near visible wavelengths well beyond the absorption edge of silicon.

57 Chemically reducing the helicenes shifts the absorption edge of the ECD spectra into the near-infrare

58 collected at the X-ray wavelengths near the absorption edge of the K-shell alpha electrons of seleni

59 er visible-light irradiation by shifting the absorption edge of TiO2 nanocrystals to a shorter wavele

60 In addition, short absorption edges of <200 and 208 nm for KMgCO3F and Cs9M

61 inations have been carried out at the K or L absorption edges of a variety of elements.

62 itional structure at the L(1), L(2) and L(3) absorption edges of gadolinium in gadolinium gallium gar

63 circular dichroism measurements at the N4,5 absorption edges of Gd to validate the high degree of ci

64 to specific interaction pathways around the absorption edges of ionic charge states.

65 on energies corresponding to the fundamental absorption edges of matter, which lie in the soft X-ray

66 r dichroic signals at the Fe K and Dy L 2, 3 absorption edges of the non-centrosymmetric structure wa

67 The optical excitonic features and absorption edges of the WSSe nanotubes do not vary linea

68 stigating the fine structure of the K- and L-absorption edges of various elements (carbon, calcium, o

69 nsity beam of X-rays at energies close to an absorption edge on inorganic surfaces in air.

70 We find that excitons created by near-absorption-edge photons are intrinsically bound states,

71 Moreover, when the X-ray absorption edge positions were extracted from each spect

72 ccur as the X-ray energy is varied across an absorption edge provide additional information that is l

73 Spectral features near the Cl K-absorption edge provide detailed information about the b

74 Merging of XAS data at the Cu and Se K-absorption edges provided additional details of the clus

75 ieved through operating above the two-photon absorption edge, representing one of the largest optical

76 The DFT simulations of the Mn 1s absorption edge reproduce the experimentally measured cu

77 X-ray absorption spectroscopy reveals an absorption edge shift of 1.65 eV in the Co L-edge upon r

78 purified enzyme using X-rays tuned to the Fe absorption edge show Fe partitions primarily to the beta

79 near edge structure (XANES) around the Pb-L3 absorption edge showed that Pb pigments and Pb soaps can

80 ints of a single atom, the L(2,3) and M(4,5) absorption edge signals for iron and terbium, respective

81 Quantification is achieved by employing absorption-edge synchrotron X-ray computed microtomograp

82 spectrum at 150 ps shows a red shift of the absorption edge that is consistent with an Fe(II) high-s

83 efficient, good electron mobility, and sharp absorption edges that are defined by the twisted molecul

84 rption in the ultraviolet spectrum and sharp absorption edges that rapidly decline upon entering the

85 e observed when exciting the acceptor at its absorption edge to a thermalized state.

86 erty of the refractive lens material near an absorption edge to make its fabrication practical.

87 to the excitonic photoluminescence near the absorption edge, we find a red-shifted, broadband (full-

88 ng incident x-ray energies close to the Se K-absorption edge, we have collected quantitative, 100-mic

89 The band gaps (estimated from the steep absorption edges) were found to be 2.31 eV for 1 (0D), 2

90 0 nm wavelength resides above the two-photon absorption edge, while still possessing large nonlineari

91 ross the vanadium L (2,3) and oxygen K x-ray absorption edges with nanometer-scale resolution.

92 -dependent studies at Br K and Pb L(3) X-ray absorption edges with refined ab initio simulations, whi