ライフサイエンスコーパス: optical mode

1 exchanged between the matter states and the optical mode.

2 ateral dimensions of both the device and the optical mode.

3 to emit one photon at a time into a desired optical mode.

4 , or applicability for alkaline solutions in optical mode.

5 spatial profile and scale invariance of the optical mode.

6 study noise and correlation between multiple optical modes.

7 r than the dissipation rates of the acoustic/optical modes.

8 tunably non-Gaussian, partially self-healing optical modes.

9 l platform to study the properties of hybrid optical modes.

10 ve waves typically consist of an ensemble of optical modes.

11 teraction of single QDs with highly confined optical modes.

12 rection locking in the excitation of surface optical modes.

13 tive optomechanical coupling between the two optical modes.

14 e transfer of optical fields between the two optical modes.

15 oup-index in hybrid plasmonic with nanoscale optical modes.

16 nanometre-scale plasmonic lasers, generating optical modes a hundred times smaller than the diffracti

17 involves the zero-point fluctuations of the optical mode (a.k.a. vacuum field) and the molecular tra

18 The instrument has two ion optical modes: a single-reflection configuration offers

19 agg reflectors (DBRs) host, besides confined optical modes, also mechanical resonances due to stop ba

20 olves the distribution of entangled pairs of optical modes among many quantum memories stationed alon

21 e structure that confines both a propagating optical mode and an electrically excitable breathing-mod

22 ward correlation between the first localized optical mode and maximum BP temperature for disordered m

23 The excited optical mode and resulting wavefront control are both lo

24 guide, maximizing their interaction with the optical mode and thus increasing sensitivity by a factor

25 rk mode, which is a superposition of the two optical modes and is decoupled from the mechanical oscil

26 isofrequency contours-feature large-momenta optical modes and wave confinement that make them promis

27 ew measurements, regardless of the number of optical modes, and provides a practical and robust solut

28 ns are sensitive to defect scattering, while optical modes are insensitive to small voids.

29 Quantum properties of optical modes are typically assessed by observing their

30 oustic phonons and the same electron-coupled optical modes as in the unit cell.

31 We identify the inflation of low-energy optical modes as the main responsible for the appearance

32 of the resonator geometry for supporting an optical mode associated with a quasi-bound state in the

33 The sensor supported five optical modes at 442 nm and three at 633 nm.

34 agating optical fields or multiple localized optical modes at distances.

35 ar cells is limited due to a small number of optical modes available in the thin-film slab.

36 and realised the metasurface to support two optical modes both with sharp Fano resonances that exhib

37 enerate entanglement between two propagating optical modes, by coupling them to the same, cryogenic m

38 In this framework, the network optical modes can be designed via the network connectivi

39 requirement for non-linear couplings between optical modes containing few photons.

40 based on implementing a quantum bit with two optical modes containing one photon.

41 s the way towards a more general idea of all-optical mode control.

42 de optical fibre for lensless microscopy and optical mode conversion.

43 Coupling vibrational transitions to resonant optical modes creates vibrational polaritons shifted fro

44 On the basis of optical mode degeneracy, we break time-reversal symmetry

45 low-optical losses make interaction with the optical mode difficult.

46 ge relocation, similar to a soft (transverse optical) mode driven phase transition between the ferro-

47 -phonon coupling to specific fully symmetric optical modes during the buildup of a three-dimensional

48 al limit can be substantially surpassed when optical modes exhibit deep-subwavelength-scale field con

49 In the long wavelength limit these optical modes exhibit longitudinal-transverse splitting,

50 A further low energy optical mode exists at ~12 cm(-1) that originates from d

51 tructure was operated in both electrical and optical mode for of tryptophan enantiomers (D-/L-Trp).

52 store the quantum information encoded on the optical modes for times that are long compared to the di

53 ire etching of thin-film LN, and uses hybrid optical modes formed by bonding LN to planarized silicon

54 h molecules are strongly-coupled to the same optical mode, forming so-called "hybrid" polaritons.

55 ellipsometry, we observe red shifting of the optical modes from local bonding distortion.

56 By watching the spectral shifts of optical modes from nanoparticles used to precoat these s

57 Tracking the variation of the Si optical mode in and around the QD, we observe the nanosc

58 probed by the evanescent field of the guided optical mode in the device.

59 ve realized such a dark mode by coupling two optical modes in a silica resonator to one of its mechan

60 ng between circularly and linearly polarized optical modes in our device.

61 e simultaneous confinement of mechanical and optical modes in periodic structures can lead to greatly

62 Due to the availability of multiple optical modes in the tunable open cavity, it seamlessly

63 density of states of, and coupling between, optical modes in ultralow-loss waveguides and resonators

64 These optical modes, including unusually low-frequency twistin

65 the circular polarization components of the optical modes induced by photonic RD SOC is observed exp

66 spaced metal nanoparticles that convert the optical mode into non-radiating surface plasmons.

67 ls, in which the behavior of highly confined optical modes is intertwined with quantum phenomena, are

68 n an optomechanical system, where one of the optical modes is strongly driven into chaotic motion and

69 es, which is directly correlated to measured optical mode lifetimes.

70 the electric and magnetic intensities of the optical modes localized in a photonic crystal nanocavity

71 , a weakly polar semiconductor with dominant optical-mode long-range e-ph interactions.

72 work, the presence of localized interfacial optical modes mediate thermal conductance across these i

73 romagnetic fields suggested the existence of optical modes more selective than circularly polarized p

74 ilar frequency, but by using an intermediary optical mode, non-degenerate modes can interact and be i

75 pillar array through the folded longitudinal optical mode, obtaining a clear spectral anti-crossing.

76 An optical mode of a compact Fabry-Perot resonator detects

77 g pulsed laser light to excite a colocalized optical mode of the cavity, we measured the internal aco

78 alled 2D chirality by strong coupling of the optical modes of (high finesse) achiral Fabry-Perot cavi

79 brational bands of solute and solvent to the optical modes of a Fabry-Perot cavity (vibrational stron

80 such structures by strongly coupling them to optical modes of Fabry-Perot type cavities.

81 iderations for the Brillouin process require optical modes of nearby frequencies but with different w

82 multiple absorption peaks from acoustic and optical modes of spin interaction between adjacent magne

83 ed to phonon scattering by the low-frequency optical modes of the side chains.

84 bers is modal dispersion, in which different optical modes propagate at different velocities and the

85 s of the two systems, e.g., linewidth of the optical modes, refractive index sensitivity and figure-o

86 evels of disorder are unable to localize the optical modes residing near the Dirac point.

87 gh reconnection events, where the additional optical modes resulting from the interactions with the t

88 Here we show that all-optical, mode-selective manipulation of the crystal latt

89 However, such lasers are restricted, both in optical mode size and physical device dimension, to bein

90 ty to a modulated structure arises from soft optical modes that is controlled by the octahedrally coo

91 um state composed of four spatially distinct optical modes that share one photon, a so-called W state

92 waves with an evolutionary competition among optical modes, the speckle field develops a single, high

93 y in a wide class of systems that couple two optical modes to a mechanical mode, highlighting the imp

94 onators, which introduce a dense spectrum of optical modes to enable dispersive phase compensation.

95 Here we rely on high-order transverse optical modes to relax this limitation and report the ex

96 ield, as they carry the potential to squeeze optical modes to spaces significantly below the diffract

97 rface plasmons and a previously unidentified optical mode type called absorption-induced scattering.

98 enables the formation of chiral and tunable optical modes upon the application of an external magnet

99 n and transfers chaos to other weakly driven optical modes via a common mechanical resonator.

100 ent coupling to photonic cavities having the optical mode volume close to or below the diffraction li

101 multaneous control of the radiation loss and optical mode volumes, we show that both requirements can

102 grated mode multiplexers to address separate optical modes, we show that circulators and narrowband f

103 mode works as a common force acting on each optical mode, which, thus, enables the synchronization o

104 tonic crystal waveguides that can support an optical mode with a submicrometre cross-section.

105 strong anharmonic coupling of the low energy optical modes with acoustic modes causes damping of heat

106 motions, broadband light can travel between optical modes with different angular momenta within a fe

107 versible conversion of spin splitting of the optical modes with different energies, leading to an opt

108 e a threshold for lasing as characterized by optical modes with instrument-limited linewidths.

109 tifying the large anharmonic coupling of the optical modes with the ligand layers and rationalize the

110 des, in a single laser beam, about a million optical modes with very narrow linewidths and absolute f

111 en light-harvesting complexes and a confined optical mode within a metallic optical microcavity.

112 fundamentally limited by the large number of optical modes within the ultrasound focus.