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 teraction of single QDs with highly confined optical modes.

4 rection locking in the excitation of surface optical modes.

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

6 tive optomechanical coupling between the two optical modes.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

31 These optical modes, including unusually low-frequency twistin

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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