ライフサイエンスコーパス: shot noise

1 times as set by photon counting statistics (shot noise).

2 This yields images impaired by shot noise.

3 measurement field, termed radiation pressure shot noise.

4 pear larger than the SD expected from photon shot noise.

5 uracy was predominantly limited by molecular shot noise.

6 dual peaks in large excess of that caused by shot noise.

7 ise minimum set by quantum mechanical photon shot noise.

8 The effects of shot noise, acceptor polarization, and FRET efficiency o

9 ted to the dependence on the photon detector shot noise, allowing a limit of detection of 0.14 nM for

10 mRNA synthesis noise is composed of wideband shot noise and band-limited operator binding generated n

11 We discuss how shot noise and heterogeneity among the transition rates

12 We find that in addition to the shot noise and the noise associated with correlated mole

13 with superior readout with respect to photon shot noise are needed to increase the sensitivity furthe

14 qubit, our results uniquely identify photon shot noise as limiting T2 in contemporary qubits based o

15 the noise is consistent with expectations of shot noise at a fixed electronic temperature.

16 analysis is ultimately limited by molecular shot noise at low concentrations and by concentration-in

17 Here, we propose to use the photon-assisted shot noise for on-chip radiation detection.

18 pendence of the small excess width above the shot noise for the FRET efficiency distributions may res

19 Here, we show that shot noise from other emitters and error propagation com

20 We show that photon shot noise in the signal readout is currently a limiting

21 ncorporation of point spread function-shaped shot noise into the variance term in the Fisher matrix y

22 and when measurement imprecision from photon shot noise is balanced against disturbance from measurem

23 The resulting photon shot noise is mitigated using a dynamical decoupling pro

24 ance at only 2 times the fundamental quantum shot-noise level and provides the record sensitivity in

25 As the shot-noise level of the power spectrum is consistent wit

26 rms phase measurement sensitivity beyond the shot noise limit.

27 have a sensitivity of 0.3 ppb in the photon (shot) noise limit.

28 low 1 per cavity mode volume near the photon shot-noise limit.

29 respectively, compared with the single-pass shot-noise limit.

30 nt of light reaching the detector because of shot noise limitations.

31 of the number of photons in the spot for the shot noise limited case and as the inverse of the number

32 at a photon detector is capable of achieving shot noise limited performance without using the balance

33 of a nanomechanical oscillator with a nearly shot-noise limited microwave interferometer.

34 stimulated Raman scattering microscope with shot-noise limited sensitivity and an imaging speed up t

35 dominant fixed-structure noise and obtain a shot-noise limited spectrum.

36 w that, for the far-from-resonance case, the shot noise-limited signal/noise ratio depends on the loc

37 water-subtracted lysozyme spectrum was still shot-noise-limited and essentially free of nonrandom noi

38 sing RNA dilutions show this device achieves shot-noise-limited performance in quantifying single mol

39 xtract the miniscule intensity increase with shot-noise-limited sensitivity by using a lock-in amplif

40 Our system achieves a shot-noise-limited sensitivity of about -105 dB at a ref

41 ng photon detectors have prevented achieving shot-noise-limited sensitivity without using balanced-de

42 this article, we present a highly sensitive, shot-noise-limited, and ruggedized Raman signal acquisit

43 We report shot-noise-limited, high-bandwidth measurements of Brown

44 This is within a factor of 2 of theoretical shot-noise limits.

45 of performance were within a factor of 2 of shot-noise limits.

46 13C/12C ratios were within a factor of 2 of shot-noise limits.

47 Using shot-noise measurements in an SIS junction induced in an

48 lexity, from predominantly functional ones ('shot-noise' models) to those with more detailed physiolo

49 Moreover, molecular shot noise, not thermal voltage noise, is the basis of t

50 Based on the principles of photon shot noise occurring in low light level fluorescence mic

51 observed noise level was attributable to the shot noise of the detectors.

52 Shot noise on the number of detected photons substantial

53 ect this quantum phenomenon by measuring sub-shot-noise optical squeezing.

54 electronic interactions can be found in the shot noise or higher statistical moments of a direct cur

55 This noise, commonly referred to as shot noise or projection noise, gives rise to the standa

56 , leading to current partition and quantized shot-noise plateaus similar to those of conductance, whe

57 iption and show that the previously reported shot noise representation is exact at all mRNA populatio

58 upling to the radiation, the photon-assisted shot noise response is shown to be independent on the na

59 mbined with the squeezed state technique for shot noise suppression, this interferometer promises fur

60 alized leaky integrate-and-fire neurons with shot-noise synapses.

61 to noise ratio (SNR) statistics due to high shot noise that is associated with low photon count in a

62 ppendix In the presence of experimental-like shot noise, the precision of the SPIFF-based correction

63 We show that the dynamics transition from shot noise to chaos as the photon rate increases and tha

64 vity for phase measurement is limited by the shot noise, which can be suppressed with squeezed states

65 Averaging over biological, thermal and shot noise with 100's to 1000's of FOV enables unbiased