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1  times as set by photon counting statistics (shot noise).
2 value expected from classical physics (i.e., shot noise).
3 dB) than the classical value associated with shot noise.
4 ollection, ICAM substantially reduces source shot noise.
5 ise minimum set by quantum mechanical photon shot noise.
6               This yields images impaired by shot noise.
7 measurement field, termed radiation pressure shot noise.
8 pear larger than the SD expected from photon shot noise.
9 uracy was predominantly limited by molecular shot noise.
10 dual peaks in large excess of that caused by shot noise.
11 merous pixels and low ion counts, leading to shot noise.
12                             By measuring the shot noise, a consequence of charge quantization, in sup
13                               The effects of shot noise, acceptor polarization, and FRET efficiency o
14  outside the superconducting gap region, the shot noise agrees quantitatively with independent tunnel
15 ted to the dependence on the photon detector shot noise, allowing a limit of detection of 0.14 nM for
16 mRNA synthesis noise is composed of wideband shot noise and band-limited operator binding generated n
17                               We discuss how shot noise and heterogeneity among the transition rates
18              We find that in addition to the shot noise and the noise associated with correlated mole
19 tally limited to the millimolar level due to shot noise and the small modulation depth.
20 erate in domains in which independent noise (shot noise and/or thermal noise) can overwhelm physiolog
21        Lifetime readout is limited by photon shot noise, and the method provides strong rejection of
22 with superior readout with respect to photon shot noise are needed to increase the sensitivity furthe
23  qubit, our results uniquely identify photon shot noise as limiting T2 in contemporary qubits based o
24 the noise is consistent with expectations of shot noise at a fixed electronic temperature.
25  analysis is ultimately limited by molecular shot noise at low concentrations and by concentration-in
26 y, this capability is limited only by photon shot noise, but in practice depends on additional parame
27  flux excitation can overcome photon-limited shot noise, but photobleaching and photodamage restrict
28  and their associated tracks propagated from shot noise, camera artifacts, pixelation, background and
29 gigahertz 3-decibel bandwidth with a maximum shot noise clearance of 12 decibels and shot noise clear
30 imum shot noise clearance of 12 decibels and shot noise clearance out to 26.5 gigahertz, when measure
31 luding asymmetric frequency pulls and photon shot noise dephasing, under varying degrees of nonrecipr
32 on time of 100 ms, corresponding to a single-shot noise-equivalent field of 4.6 kV m(1), using a puls
33  Here, we propose to use the photon-assisted shot noise for on-chip radiation detection.
34 pendence of the small excess width above the shot noise for the FRET efficiency distributions may res
35                           Here, we show that shot noise from other emitters and error propagation com
36                                    Recently, shot noise has been shown to be an inherent part of all
37  self-supervised deep learning algorithm for shot noise image filtering (DeepSNiF).
38                          We show that photon shot noise in the signal readout is currently a limiting
39      When compared with conventional metals, shot noise in these nanowires is strongly suppressed.
40 lication of a century-old result describing "shot noise" in an electronic system repairs the deficien
41 ncorporation of point spread function-shaped shot noise into the variance term in the Fisher matrix y
42 and when measurement imprecision from photon shot noise is balanced against disturbance from measurem
43         Deep within the superconducting gap, shot noise is greatly enhanced, reminiscent of multiple
44                         The resulting photon shot noise is mitigated using a dynamical decoupling pro
45              Here, we show that the enhanced shot noise, known from Josephson junctions with two supe
46 ance at only 2 times the fundamental quantum shot-noise level and provides the record sensitivity in
47                                       As the shot-noise level of the power spectrum is consistent wit
48 s that reduce fluorescence detection to near shot-noise levels.
49 rms phase measurement sensitivity beyond the shot noise limit.
50 have a sensitivity of 0.3 ppb in the photon (shot) noise limit.
51  promises a measurement precision beyond the shot-noise limit (SNL) by taking advantage of the infini
52 ton flux, which is voltage imaging below the shot-noise limit.
53  respectively, compared with the single-pass shot-noise limit.
54 low 1 per cavity mode volume near the photon shot-noise limit.
55 signal-to-noise ratio nearly 3 dB beyond the shot-noise limit.
56  detector, which operates beyond the quantum shot-noise limit.
57 tly track weak returning pulse trains at the shot-noise limit.
58 eak value amplification enables reaching the shot-noise-limit of sensitivity, which is difficult for
59 ectly, thereby overcoming the optical photon shot noise limitations of conventional fluorescence read
60 nt of light reaching the detector because of shot noise limitations.
61 of the number of photons in the spot for the shot noise limited case and as the inverse of the number
62 at a photon detector is capable of achieving shot noise limited performance without using the balance
63                         We show that, in any shot noise limited situation, the optimum signal-to-nois
64 lmost 3-orders-of-magnitude improvement over shot-noise limited direct imaging.
65 of a nanomechanical oscillator with a nearly shot-noise limited microwave interferometer.
66            Second, leveraging the platform's shot-noise limited performance and using a model DNA-AuN
67 s high temporal and spectral resolution with shot-noise limited performance, allowing for the label-f
68  stimulated Raman scattering microscope with shot-noise limited sensitivity and an imaging speed up t
69  dominant fixed-structure noise and obtain a shot-noise limited spectrum.
70 Through simulations, we demonstrate that the shot noise-limited precisions of the lateral and axial m
71 w that, for the far-from-resonance case, the shot noise-limited signal/noise ratio depends on the loc
72 water-subtracted lysozyme spectrum was still shot-noise-limited and essentially free of nonrandom noi
73 enic photodetector(6), capable of delivering shot-noise-limited microwave signals directly at millike
74 ference and the power of signal averaging in shot-noise-limited operation In our latest work, we have
75 sing RNA dilutions show this device achieves shot-noise-limited performance in quantifying single mol
76 egmentation of spiking cells compared to the shot-noise-limited performance of single pixels.
77 xtract the miniscule intensity increase with shot-noise-limited sensitivity by using a lock-in amplif
78                        Our system achieves a shot-noise-limited sensitivity of about -105 dB at a ref
79 ng photon detectors have prevented achieving shot-noise-limited sensitivity without using balanced-de
80 hm (DeepVID) for inferring fluorescence from shot-noise-limited signals.
81 this article, we present a highly sensitive, shot-noise-limited, and ruggedized Raman signal acquisit
82                                    We report shot-noise-limited, high-bandwidth measurements of Brown
83 R estimation theory and address its photonic shot-noise limits depicting information-theoretic bounds
84  This is within a factor of 2 of theoretical shot-noise limits.
85  of performance were within a factor of 2 of shot-noise limits.
86  13C/12C ratios were within a factor of 2 of shot-noise limits.
87                                          Our shot noise measurements reveal that heat flux displays a
88                                        Using shot-noise measurements in an SIS junction induced in an
89 lexity, from predominantly functional ones ('shot-noise' models) to those with more detailed physiolo
90                          Moreover, molecular shot noise, not thermal voltage noise, is the basis of t
91            Based on the principles of photon shot noise occurring in low light level fluorescence mic
92 observed noise level was attributable to the shot noise of the detectors.
93 nfrared probe laser pulse, is limited by the shot noise of the latter.
94           Here we report measurements of the shot noise of tunnelling current in high-quality La(2-x)
95       However, incorporating photon-counting shot noise often leads to moderate-to-high uncertainty i
96                                              Shot noise on the number of detected photons substantial
97                 We demonstrate the effect of shot noise on the precision of the measurements as well
98 ect this quantum phenomenon by measuring sub-shot-noise optical squeezing.
99  electronic interactions can be found in the shot noise or higher statistical moments of a direct cur
100          This noise, commonly referred to as shot noise or projection noise, gives rise to the standa
101 ure an e/3 tunneling charge and show that DC shot noise overestimates charge below ~100 mK.
102  present time-domain HOM and Photon-Assisted Shot Noise (PASN) measurements at nu = 2/3 to probe edge
103 gnatures in the dependence of photo-assisted shot noise (PASN) on voltage V when irradiating contacts
104 , leading to current partition and quantized shot-noise plateaus similar to those of conductance, whe
105                       Here, we show that the shot noise, proportional to the dark current, dominates
106                                              Shot noise reference doses in the range from 820 to 1,70
107 iption and show that the previously reported shot noise representation is exact at all mRNA populatio
108 upling to the radiation, the photon-assisted shot noise response is shown to be independent on the na
109 ing inference in spite of the extremely high shot noise (SNR ~ 1).
110 mbined with the squeezed state technique for shot noise suppression, this interferometer promises fur
111 alized leaky integrate-and-fire neurons with shot-noise synapses.
112  to noise ratio (SNR) statistics due to high shot noise that is associated with low photon count in a
113 s reduce the position uncertainty created by shot noise (the photon-counting error caused by the quan
114 ppendix In the presence of experimental-like shot noise, the precision of the SPIFF-based correction
115    We show that the dynamics transition from shot noise to chaos as the photon rate increases and tha
116                                  We measured shot noise to probe the granularity of the current-carry
117 ght power with excess noise increased by 0.5 shot noise unit.
118 vity for phase measurement is limited by the shot noise, which can be suppressed with squeezed states
119       Averaging over biological, thermal and shot noise with 100's to 1000's of FOV enables unbiased
120 erize four separate noise contributions: (1) shot noise with Fano factor close to unity due to holes

 
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