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 l deformation vibrations and the first Ir-Ir overtone.

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

6 o of these signals is close to unity for all overtones.

7 y, the corn spectra were divided into second overtones (1100-1388 nm), first overtones (1390-1852 nm)

8 into second overtones (1100-1388 nm), first overtones (1390-1852 nm), and combinations (1852-2498 nm

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

10 e results with those obtained by the bilayer overtone analysis of membrane binding demonstrates a pro

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

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

13 5 mM for glucose models generated from first overtone and combination spectra, respectively.

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

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

16 have visualized mode profiles of individual overtones and analyzed higher-order transverse spurious

17 ate coupling of the NH stretching modes with overtones and combination bands of CH stretching and NH

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

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

20 the spectral sub-regions under the scope of overtones and combinations has not been performed.

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

22 ifts, Deltaf/n, are similar on the different overtones and that the shifts in half bandwidth, DeltaGa

23 twist, intermolecular stretch, donor torsion overtone, and in-plane and out-of-plane librational mode

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

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

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

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

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

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

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

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

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

33 ing at a rate matching the frequency of high-overtone bulk acoustic resonances(18), resonant build-up

34 actuator couples microwave signals to a high-overtone bulk acoustic resonator defined by the silica c

35 ng super-high-frequency (3 - 30 GHz) lateral overtone bulk acoustic resonator with unprecedented spat

36 ptic modulation is realized by exciting high-overtone bulk acoustic wave resonances (HBAR) in the pho

37 The multi-mode composite high-overtone bulk acoustic wave resonator (HBAR) is a popula

38 We account for vibrational CT-EL overtones by selectively measuring the dominant vibratio

39 es primarily due to differences in the first overtone CH stretching region between 1650 and 1720 nm,

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

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

42 al tract to narrowly focus the harmonics (or overtones) emanating from their vocal cords.

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

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

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

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

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

48 This highlights the overtone frequency comb as the straightforward future fo

49 ellulose structure, and N-H stretching first overtone from amide/protein structures.

50 The LO phonon and its overtones geometrically distort neighboring NV centers,

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

52 te a frequency comb consisting of mechanical overtones (integer multiples) of a single eigenfrequency

53 t mass derived from QCM independently of the overtone is about 10 times the Sauerbrey (inertial) mass

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

55 A novel overtone mobility spectrometry (OMS) instrument utilizin

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

57 Frequency differences between overtone modes-large separations-probe stellar density(2

58 h the Sauerbrey prediction, meaning that the overtone-normalized frequency shifts, Deltaf/n, are simi

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

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

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

62 wet mass with the particle coverage and the overtone number.

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

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

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

66 ds are assigned as the fundamental and first overtone of the H(2)O-H(-) vibrational stretching mode,

67 e O-H stretching fundamental and the bending overtone of the nearest neighboring water molecule.

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

69 electrophoretic force on the membrane at the overtones of a membrane's motion.

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

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

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

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

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

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

76 es, plots of /(- f) versus - f/n (with n the overtone order) show almost straight lines.

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

78 Here, we present an overtone photothermal (OPT) microscopy technique that of

79 soft contact regime, where the higher-number overtones produce a negligible QCM signal.

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

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

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

83 le probe for local heat detection in the C-H overtone region.

84 n (2130-2190 nm, 3 bands), whereas the first overtones region was the best for predicting starch (145

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

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

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

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

89 These overtones share a fixed frequency and phase relation, an

90 tions included tonal sounds with and without overtones, sounds of burst-pulse character, graded sound

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

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

93 each solute from both combination and first overtone spectra.

94 Vibrational overtone spectroscopy of molecules is a powerful tool fo

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

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

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

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

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

100 associated with C-H and O-H stretching first overtone, typical of the cellulose structure, and N-H st

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

102 d by the near-IR induced excitation of an OH-overtone vibration.

103 to hundreds of terahertz for fundamental and overtone vibrational and electronic transitions-possibly

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

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

106 e frequency and bandwidth shifts for various overtones were measured as a function of time.