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 solution to distinguish individual elemental absorption edges.

6 fluorescence setup at certain energies near absorption edges.

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

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

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

10 5 x KDP (600 x alpha-SiO2), and the shortest absorption edge (250 nm) of reported materials with a st

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

34 1.7 A resolution with a wavelength near the absorption edge of bromine.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

60 0 nm wavelength resides above the two-photon absorption edge, while still possessing large nonlineari