ライフサイエンスコーパス: octave

1 the octave and the cycle of notes within the octave.

2 anged from close to one octave to about 1/12 octave.

3 -frequency roll-off of approximately -8.4 dB/octave.

4 developed using the open-source software GNU Octave.

5 de a continuous conversion bandwidth over an octave.

6 hat contain notes spread unevenly across the octave.

7 e dyads, triads, and tetrads within a single octave.

8 ferent frequencies, varying by as much as an octave.

9 to less than approximately one eighth of an octave.

10 , and 2.0 cpd and a spatial bandwidth of 1.0 octave.

11 e conditioning stimuli was < approximately 1 octave.

12 oss sounds that differed in frequency by two octaves.

13 frequency (BF) shifts downwards by about 0.5 octaves.

14 spatial or temporal frequency separation in octaves.

15 d uniform supercontinuum, extending over 2.5 octaves.

16 ide band of frequencies, spanning over three octaves.

17 ion, have wider frequency tuning than +/-1/6 octaves.

18 ation, resulting in a total bandwidth of 1.6 octaves (137-407 THz).

19 hertz generation and detection spanning four octaves (200 GHz to > 3 THz).

20 perceived distance in response to monaural 1 octave 4 kHz noise source sounds presented at distances

21 nded to reproduce notes an integer number of octaves above or below the heard tones, Amazonians did n

22 Ambient noise was analysed in third octave and decade bands and further investigated using g

23 Versions are available in Octave and Java (with a graphical user interface).

24 was evaluated on spectral levels (one-third octave and one- twelfth octave band).

25 tuned the optical-driver frequency by a full octave and show that the predicted super-resolution mani

26 n the keyboard, these are illustrated by the octave and the cycle of notes within the octave.

27 d broad spectral tuning (approximately three octaves) and were excitatory in the contralateral ear, i

28 Common Lisp, Java, Python, Perl, MATLAB and Octave, and includes many features that facilitate adopt

29 e shifted downwards in frequency by nearly 1 octave, and the maximum phase lags amounted to only 180

30 nes <2 kHz, SFOAE amplification extended two octaves apical of CF, which highlights that different vi

31 t comb-like optical spectra spanning several octaves are a chief ingredient in the emerging field of

32 ng white-noise masking notch-filtered +/-1/6 octaves around the tone center frequencies.

33 substantially to DeltaCF approximately 0.62 octave at 24 weeks.

34 p misalignment of DeltaCF approximately 1.27 octaves at 6 weeks after overstimulation decreases subst

35 PCT; or decrease in near stereoacuity of >=2 octaves, at any masked examination; or reoperation witho

36 2-h exposure to 100-dB sound pressure level octave band (8 to 16 kHz) noise results in no permanent

37 ctive noise profiles, based on decibel-A and octave band assessments.

38 SSwap in Experiment 3 used octave band noise (2-4, 4-8, 8-16, or 16-32 kHz) and sep

39 We used octave band noise (8--16 kHz) at three levels (106, 112,

40 A separate group of chimeras was exposed to octave band noise (8-16 kHz for 2 hours) 2 weeks after t

41 days before and 3 days after a 3 hour 4 kHz octave band noise at 117 dB (SPL).

42 ne plus tempol and exposed to 120 dB SPL one-octave band noise centered at 4 kHz for 5 h.

43 rised recreational vessels can elevate third-octave band noise centred at 0.125, 2 and 16 kHz by 47-5

44 nts, CBA/CaJ mice were exposed to an intense octave band of noise (8-16 kHz) at 100 dB SPL for 2 hr,

45 The noise exposure was an 8kHz octave band of noise at 105dB SPL for 4h.

46 al levels (one-third octave and one- twelfth octave band).

47 The noise exposure (4-kHz octave band, 115 dB SPL, 5 h) created permanent threshol

48 ale guinea pigs were exposed to noise (4 kHz octave band, 115 dB SPL, 5 h).

49 udes comparable to those of responses to 1/3 octave band-pass noise.

50 ersonal noise measurements and environmental octave-band analyses were performed to divide subjects i

51 n Vglut3(WT) and Vglut3 (+/-) mice, 8-16 kHz octave-band noise exposure at 100 dB sound pressure leve

52 en 68.3 and 96.31 dB re 1 muPa(2) across 1/3 octave bands (13 Hz-16 kHz), with peaks in February and

53 sing the decibel-A scale and at each of nine octave bands at each bedspace.

54 ed from 81.5-95.5 dB re 1 muPa for one-third octave bands from 63-500 Hz.

55 rimentally, spanning from 125 Hz to 4 kHz (6 octave bands), covering the majority of the audible freq

56 To date, octave bandwidth (25-50 THz) single-channel links have b

57 ) for both narrowband tonal carriers and two-octave bandwidth noise carriers in the auditory core of

58 ventional horn antennas over greater than an octave bandwidth with negligible loss and advance the st

59 f cochlear amplification usually peaked ~1/2 octave basal of the CF region.

60 teristic frequency (CF) place and within one octave basal of the CF.

61 chlear amplification typically extended ~1.5 octaves basal of CF, and the data are consistent with co

62 claimed that SFOAE components originate many octaves basal of CF.

63 mbrane at a frequency approximately one-half octave below CF, in accordance with the experimental dat

64 en the mask was presented at approximately 1 octave below the test spatial frequency.

65 iments revealed, however, that the peak at 1 octave below the test was mediated by image size and/or

66 The OC motion at approximately 2-6 octaves below the characteristic frequency of the region

67 rner frequencies around 3 kHz- more than 2.5 octaves below the frequencies the OHCs are expected to a

68 e of the compression mode at about one-third octave beyond the best frequency.

69 nm in these structures, we generated a multi-octave broadband SC spectrum ranging from 1.5 um-25 um a

70 ure tone trajectory as small as 1/24th of an octave, comparable to what has been reported in primates

71 nd near) or near stereoacuity criterion (>=2-octave decrease from best previous measure).

72 re measured over headphones for STM (2cycles/octave density, 4-Hz rate) applied to an 85-dB SPL, 2-kH

73 multiple frequency bands (1) at exactly one octave distance from each other, (2) at multiple harmoni

74 Intriguingly, this "octave effect" not only occurs for physically presented

75 correlated with similarity-based measures of octave equivalence as well as the ability to match the a

76 ts on the limits of pitch, but indicate that octave equivalence may be culturally contingent, plausib

77 picosecond frequency combs tunable beyond an octave extending from 1.5 up to 3.3 mum with femtojoule-

78 diffuser lens to 2.3 +/- 0.7 and 3.5 +/- 0.8 octaves for the intermediate and strongest diffuser lens

79 difference increased systematically from 0.6 octaves for the weakest diffuser lens to 2.3 +/- 0.7 and

80 s designed exhibiting a bandwidth of several octaves for use in both multi-band plasmonic resonance-e

81 The results confirmed that the peak at 1 octave from the test still occurred when the potential f

82 2) near stereoacuity decreased by at least 2 octaves from baseline, both assessed by a masked examine

83 pecific aspects of music perception (such as octave generalization), as well as studies that investig

84 sensory alteration defined as change of >=2 octaves (>=0.6 log arcsec).

85 n acuity adjusted for age was reduced by 1.2 octaves in isolated infantile nystagmus and by 1.7 to 2.

86 olated infantile nystagmus and by 1.7 to 2.5 octaves in nystagmus with associated sensory defect.

87 d diverse stimulus preferences spanning five octaves in spatial and temporal frequency.

88 In the OCTAVE Induction 1 and 2 trials, 598 and 541 patients, r

89 In the OCTAVE Induction 1 and 2 trials, the rates of overall in

90 In the OCTAVE Induction 1 trial, remission at 8 weeks occurred

91 8.2% in the placebo group (P=0.007); in the OCTAVE Induction 2 trial, remission occurred in 16.6% ve

92 In addition, we developed a Matlab/Octave interface for fast metabolic modeling.

93 ed to generalize to frequencies separated by octave intervals both lesser and greater than the CS.

94 ated music using pitch intervals that divide octaves into the 12 tones of the chromatic scale.

95 plain prominent perceptual phenomena such as octave invariance.

96 avelength-multiplexed operation spanning 2/3 octave is also demonstrated in a single device.

97 y, coherent terahertz radiation spanning 2.8-octaves is achieved from 330 GHz to 2.3 THz, with ~20 GH

98 75-2400 nm), covering slightly more than two octaves is demonstrated.

99 rithm is implemented with scripts written in octave, linux shell and perl.

100 , 1.23+/-0.417 octaves; medium, 1.41+/-0.593 octaves; low, 1.52+/-0.475 octaves; mean +/- SD).

101 tiated at a frequency approximately one-half octave lower than the CF.

102 ponses in adult gerbils: BF was more than an octave lower, the steep slopes of the phase vs. frequenc

103 he pitch of IIRN[-] for the same delay is an octave lower.

104 a-broadband radiation (extending over more 5 octaves) making a great challenge to reach resolution li

105 ium, 1.41+/-0.593 octaves; low, 1.52+/-0.475 octaves; mean +/- SD).

106 of stimulus presentation (high, 1.23+/-0.417 octaves; medium, 1.41+/-0.593 octaves; low, 1.52+/-0.475

107 to pure tones of 2, 8, 16, or 32 kHz or half-octave noise bands centered on 2, 8, or 32 kHz at 80-120

108 localization of narrow-band (one-sixth of an octave) noise bursts presented from sources along the mi

109 with characteristic lag time of ~27 days per octave of length scales; transfer across 50 km peaks in

110 t a characteristic lag-time of ~ 40 days per octave of length-scales such that in both hemispheres, K

111 nse of individual optical antennas across an octave of the visible to near-infrared spectrum.

112 ead to future on-chip circulators over multi-octaves of frequency.

113 ld-resolved optical signal analysis spanning octaves of spectra in a monolithic device without the ne

114 dband electromagnetic signal analysis across octaves of spectrum using a single local oscillator.

115 s sensitive to and controllable by the super-octave optical field.

116 g acuity (across all five test ages) was 0.5 octave or better in 57% of eyes and 1.0 octave or better

117 (3.5-, 4.5-, and 5.5-year test ages) was 0.5 octave or better in 71% of eyes and 1.0 octave or better

118 0.5 octave or better in 57% of eyes and 1.0 octave or better in 85% of eyes.

119 0.5 octave or better in 71% of eyes and 1.0 octave or better in 93% of eyes.

120 ity difference, interobserver agreement of 1 octave or better was found in 88% of clinical subjects a

121 Interobserver agreement of 1 octave or better was found in 91% of the monocular and 9

122 unit's characteristic frequency was tuned an octave or more away from the test frequency.

123 In any given subject, there was a 1- to 2-octave range in acuity estimates over the 8 seconds of s

124 oad spectral selectivity over a four-to-five octave range.

125 ttention involves multiple pass-bands around octave-related frequencies above and below the cued tone

126 esults suggest neural interactions combining octave-related frequencies, likely located in nonprimary

127 om exposure to natural vibrations containing octave-related spectral peaks, e.g., as produced by voca

128 s covering more than 6 octaves with only 0.2 octave resolution.

129 Here, multi-octave SC generation in a gas-filled hollow-core antires

130 ded by noisy spatio-chromatic filters at one octave separations, which are either circularly symmetri

131 This implies that the half-octave shift in mammalian hearing is an epiphenomenon of

132 the effects of five musical transformations: octave shift, permutation, transposition, inversion, and

133 fer optical Kerr nonlinearity for generating octave soliton combs and quadratic nonlinearity for enab

134 Here, microcombs of more than two-octave span (450 nm to 2,008 nm) is demonstrated through

135 rged as a promising solution, owing to their octave spanning bandwidths, the ability to achieve group

136 lative-phase between two halves of the multi-octave spanning spectrum, and the overall carrier-envelo

137 ive polarization transformation over a broad octave-spanning bandwidth.

138 hat future dispersion engineering can enable octave-spanning combs.

139 Finally, KIS of an octave-spanning DKS exhibits enhancement of the opposite

140 millimetre wave synthesis(10-13) and unlock octave-spanning EO combs.

141 he complete coherent energy transfer between octave-spanning mid-infrared waveforms and vibrating mol

142 Our results represent the first octave-spanning tunable source in nanophotonics extendin

143 trate plasma-driven undulator radiation with octave-spanning tuneability at discrete wavelengths reac

144 monstrate generation and guidance of a three-octave spectral comb, spanning wavelengths from 325 to 2

145 tion of solitons with features including 1.5-octave spectral span, dual dispersive waves, and sub-ter

146 uneable active metasurfaces with record half-octave spectral tuning range and large optical contrast

147 nib-treated patients achieved remission with OCTAVE Sustain baseline MES of 0 versus 1 (61.9% vs. 36.

148 In the OCTAVE Sustain trial, 593 patients who had a clinical re

149 In the OCTAVE Sustain trial, remission at 52 weeks occurred in

150 In the OCTAVE Sustain trial, the rate of serious infection was

151 eving efficacy endpoints at Week 24 or 52 of OCTAVE Sustain was evaluated by baseline MES following 8

152 At Week 52 of OCTAVE Sustain, a numerically higher proportion of tofac

153 and safety in the 52-week maintenance study, OCTAVE Sustain, by baseline Mayo endoscopic subscore (ME

154 ination thresholds changed from close to one octave to about 1/12 octave.

155 nowledge can just type one command in Matlab/Octave to perform personalized metabolic modeling.

156 In this work, we demonstrate a compact octave tunable narrowband channel-select filter with a s

157 The cortical distance representing a given octave was similar, yet response frequency resolution wa

158 erification is demonstrated over an almost 5-octave wavelength range at 266, 1800, 4000 and 8000 nm b

159 2 nm (at - 30 dB), which corresponds to 0.83 octaves, when using the TM(10) waveguide mode.

160 Over a range of frequencies at least an octave wide, the depth is independent of frequency.

161 ic tuning in many cells was at least 1.5-2.0 octaves wide and, on average, was more than twice as wid

162 infrared dispersive waves, embedded in a 4.7-octave-wide supercontinuum that uniquely reaches simulta

163 equency from 1 to 3.5 kHz, doubling once per octave with peak tuning sharpness from 3.5 to 4 kHz.

164 ith a wide range of SFs covering more than 6 octaves with only 0.2 octave resolution.

165 quency of PVNs to higher frequency by a full octave, with no significant effect on average best frequ

166 wing formats: SBML, BioPAX, SBGN-ML, Matlab, Octave, XPP, GPML, Dot, MDL and APM.