ライフサイエンスコーパス: overtone

1 e, low spectral density (i.e., less harmonic overtones).

2 at the frequency of the first NH stretching overtone.

3 d been thought to arise from the Trp 2 x W18 overtone.

4 s at the crystal's fundamental frequency and overtones.

5 single-beam spectra collected over the first overtone (6500-5500 cm(-1)) and the combination (5000-40

6 ctrochemical impedance spectroscopy, bilayer overtone analysis, neutron reflectometry, and molecular

7 Sample thickness set for the first overtone and combination spectra are 7.5 and 1.5 mm, res

8 5 mM for glucose models generated from first overtone and combination spectra, respectively.

9 lues for urea are 7.33 and 0.10 mM for first overtone and combination spectra, respectively.

10 ree of selectivity provided within the first overtone and combination spectral regions.

11 only been characterized previously by their overtones and combination bands.

12 and C-H and N-H stretching modes as well as overtones and combinations (>3000 cm(-1)).

13 the Raman excitation frequency, (b) exhibit overtones and combinations in the RR spectra, and (c) sh

14 es are performed over the combination, first-overtone, and short-wavelength spectral regions.

15 (H/D) oscillators revealed that aromatic C-D overtones anomalously quench the luminescence more than

16 OH stretching vibration and the H2O bending overtone are found--has precluded definitive identificat

17 noid electronic states with aromatic C-(H/D) overtones are evaluated quantitatively for different lan

18 nce of the normalized frequency shift on the overtones as well as a large dissipation, which is a cle

19 er (IL)-related phonon combination modes and overtones as well as their phonon self-energy renormaliz

20 )(CO(2)) (pft) at 518 cm(-)(1) and its first overtone at 1035 cm(-)(1), consistent with the structura

21 m (1300 nm, 1450 nm, and 1550 nm) in the 1st overtone band.

22 d H(2) isotopologues and consistencies among overtone bands that are well-described by the Buckingham

23 microscopy technique based on infrared laser overtone/combination band absorption to heat small ( app

24 tercept of the line that fits instantaneous, overtone-dependent QCM data on (delta/a, -Deltaf/n) coor

25 lses at a wavelength of 1.7 mum was used for overtone excitation of C-H bonds.

26 nol in small water clusters initiated by the overtone excitation of the hydroxyl group.

27 r in glioma progenitor cells, with practical overtones for therapy.

28 ial for CNS myelination, which has practical overtones for understanding CNS myelin disorders.

29 oduction mechanism where the fundamental and overtone frequencies of blue whale B calls can be well m

30 ed ion mobility, traveling wave, cyclic, and overtone instruments) using the equations described in t

31 A new means of acquiring overtone mobility spectrometry (OMS) data sets that allo

32 A novel overtone mobility spectrometry (OMS) instrument utilizin

33 is selection method of operation as selected overtone mobility spectrometry (SOMS).

34 llows distributions of ions for a prescribed overtone number is described.

35 quartz crystal microbalance with dissipation overtone number, frequencies of zero-crossing could be i

36 taf is the QCM frequency shift, and n is the overtone number.

37 the OD and OH stretch fundamental and first overtone of dilute HOD in ice Ih.

38 undamental symmetric stretch and the bending overtone of methylene; and 2), the carbonyl and peptide

39 the absorption coefficient of the stretching overtone of the aromatic C-H groups.

40 ing-stretching fundamental nu1 and the first overtone of the phenolic ring-deformation mode nu(16a),

41 el; and (e) hearing loss where many harmonic overtones of even moderately loud playing may become ina

42 We propose that excitation of vibrational overtones of H2SO4 and its hydrate in the near-infrared

43 arise from the coupling of the HOOP with the overtones of interacting water O-H vibrations.

44 It is shown that the characteristics for the overtones of these vibrational modes deviate substantial

45 essentially unmixed metal-metal stretch, and overtones of this vibration.

46 gy vibrational modes are readily assigned to overtone or combination bands or to fundamentals corresp

47 requency extents when the number of harmonic overtones per formant is low, suggesting that this is a

48 tive excitation of CH3CHOO in the CH stretch overtone region combined with sensitive OH detection rev

49 The model based on the first-overtone region is slightly degraded but still provides

50 ity to eliminate peaks from all but a single overtone region overcomes a significant limitation assoc

51 he models based on the combination and first-overtone regions are dominated by glucose absorption inf

52 c layers structures for switchable microwave overtone resonators, binary and quadrature phase-shift k

53 at the songs of most bird species follow the overtone series, our findings add to a small but growing

54 equency ratios derived from the harmonic (or overtone) series.

55 Such high SEP values for urea with first overtone spectra correspond to an inability to quantify

56 ion spectra and the other designed for first overtone spectra.

57 each solute from both combination and first overtone spectra.

58 Vibrational overtone spectroscopy of molecules is a powerful tool fo

59 lementary theory provides insights on the IR overtone spectrum, as well as vibrational excitations, s

60 ble to select different ions from a specific overtone that is resonant over a range of applied freque

61 enes that considers the D' peak by using its overtone the 2D'.

62 ndicates that this fast feature is due to an overtone transition of Zundel-like H(3)O(2)(-) states, w

63 n the near-infrared at about 1690 nm probing overtone transitions in acetone in a spectral region rel

64 lly, a priori knowledge via selection of the overtone used to separate ions makes it possible to dire

65 ource for high-speed excitation of molecular overtone vibrations.

66 based on the near-infrared spectrum of water overtones was constructed to accurately determine the vi