ライフサイエンスコーパス: interband

1 he NELF-B and NELF-D subunits at hundreds of interbands.

2 under visible light, which was attributed to interband absorption.

3 truly metallic nanotubes but show excitonic interband absorption.

4 into a pattern of bands (afferent dense) and interband (afferent sparse) spaces that encompasses the

5 ed to study a new class of hamiltonians with interband and atom-molecule couplings.

6 ing which state filling induced bleaching of interband and exciton transitions curiously more than do

7 ganization of the chromosome by deleting the interband and fusing 3C7 with 3C6.

8 it large ultrafast nonlinearities under both interband and intraband excitations.

9 localizes to Drosophila polytene chromosome interbands and phosphorylates histone H3 at interphase,

10 The Drosophila CHD1 localizes to the interbands and puffs of the polytene chromosomes, which

11 o less condensed, hypoacetylated euchromatic interbands and was absent from moderately condensed, hyp

12 D1 localizes to sites of extended chromatin (interbands) and regions associated with high transcripti

13 y parameters where findings indicate minimal interband Auger recombination.

14 rared absorption, an extensive bleach of the interband band-edge absorption, and a complete quenching

15 The interband cascade laser differs from any other class of

16 The interband cascade laser is consequently the most attract

17 simulations demonstrating that all previous interband cascade laser performance has suffered from a

18 on spectroscopy (OF-CEAS) using mid-infrared interband cascade lasers (ICLs) is a sensitive technique

19 s the MsEph receptor is expressed by midline interband cells that are normally inhibitory to migratio

20 which the effective mass appears to diverge, interband coupling vanishes, and a local-moment state ap

21 arance of multiple plateaus indicates strong interband couplings involving multiple single-particle b

22 ch high power factors via a delayed onset of interband crossing.

23 Kerr effect, we detect and identify over 18 interband cyclotron resonances (CR) that are associated

24 small intraband Drude conductivity near the interband edge.

25 n unexpected behaviour that points to strong interband electron-electron scattering processes that co

26 xtraction by coupling photons generated from interband electronic transition to phonon polariton mode

27 encapsulated species also shifts the near-IR interband electronic transitions to lower energy by more

28 at into electricity and rejecting entropy by interband emission.

29 This is attributed to the interband excitation of BiVO4, which is unfavourable for

30 e for low band gap semiconductors, for which interband excitations occur in wavelength regions that o

31 3D topological insulator Bi2Se3 due to bulk interband excitations.

32 ntraband transition, a bleach of the visible interband exciton transitions, and a quench of the narro

33 lators, topological boundaries, and polytene interbands extends across the genome, and we therefore p

34 located at the boundaries between bands and interbands in polytene chromosomes.

35 on-coupling strength from the pi*-interlayer interband interaction.

36 A pol II in some but not all of the nonpuff, interband loci.

37 We report interband magneto-optical spectra for single-walled carb

38 pidly along the bands (but not onto adjacent interband musculature) and then complete their different

39 s between them correspond with the bands and interbands of polytene chromosomes of Drosophila.

40 asm, and to several transcriptionally active interbands of polytene chromosomes.

41 roperties is explained by the suppression of interband optical transitions and a small intraband Drud

42 The interband optical transitions cover a wide, technologica

43 otoactivation (internal photoemission versus interband photoexcitation followed by electron transfer)

44 phasing, intraband relaxation, trapping, and interband recombination of free and trapped charge carri

45 fact that it localizes properly to polytene interband regions and that it contains both kinase domai

46 in which decompaction of boundary-insulator-interband regions drives the organization of interphase

47 s show that JIL-1 localizes to the gene-rich interband regions of larval polytene chromosomes and is

48 ophila localizes specifically to euchromatic interband regions of polytene chromosomes and is enriche

49 distributed filopodia onto both the band and interband regions of the midgut surface.

50 lements and the locations of mapped polytene interband regions.

51 gut, but the neurons strictly avoid adjacent interband regions.

52 fa(swb) is located in the interband separating polytene band 3C7, which contains N

53 ction segregates into a pattern of bands and interband spaces, and by P12 adult-like, afferent-dense

54 pamin had the opposite effects on intra- and interband synchronization.

55 increased intraband synchrony and decreased interband synchrony, whereas apamin had the opposite eff

56 tion splitting the Ru-H2 complex involves an interband transition in RuO2 which effectively diminishe

57 ement around 490 nm, which is ascribed to an interband transition.

58 This gate dependence of interband transitions adds a valuable dimension for opti

59 electronic effects, related to the nature of interband transitions and band edge localization under p

60 the combination of bulk charge carriers from interband transitions and surface charge carriers of the

61 troscopy, we find that they also have strong interband transitions and that their optical transitions

62 nanotubes is used to verify the energies of interband transitions and validate the spectral assignme

63 We show that interband transitions associated with the superlattice m

64 We show that the CPGE can arise from interband transitions at the metal contacts to silicon n

65 om temperature is observed, arising from the interband transitions between the subbands of 2D InAs na

66 nce quantum, AQ = pialpha/nc for each set of interband transitions in a 2D semiconductor, where alpha

67 d based on existing models that include only interband transitions in ferromagnetic metals.

68 nocrystals (NCs) are characterized by strong interband transitions in the blue part of the spectral r

69 is sufficient to remove all vestiges of the interband transitions in the infrared spectrum.

70 ons, producing hotter electrons in gold, but interband transitions remain dominant.

71 Interband tunnelling of carriers through a forbidden ene