ライフサイエンスコーパス: dark current

1 devices to obtain high photocurrent and low dark current.

2 e crystal surface leakage current and device dark current.

3 all size features without degradation of the dark current.

4 and reduced single rod photosensitivity and dark currents.

5 was employed to reduce both bulk and surface dark currents.

6 n Mn-doped Ga2O3 thin films takes on a lower dark current, a higher sensitivity, and a faster photore

7 -/-) mouse rods also showed little change in dark current and a large and significant decrease in the

8 olar cell flash responses, suppressed inward dark current and decreased input conductance.

9 Recovery of dark current and flash sensitivity in individual intact

10 Somewhat surprisingly, dark current and light sensitivity were normal in indivi

11 ponses to appear light adapted, with reduced dark current and sensitivity and faster response kinetic

12 gous (D+/+) for this mutation have decreased dark current and sensitivity, reduced Ca(2+), and accele

13 demanding active ion transport maintains the dark current and where NO presumably activates guanylate

14 fied photodetectors have significantly lower dark-currents and higher on-currents.

15 over this wide spectral range and reduce the dark current (and noise) to values well below dark curre

16 mitting diodes a high response speed and low dark current, and they are widely used in communications

17 thin film X-ray diffraction result in a high dark current, and thus a low V(oc).

18 including sample/buffer rescaling, detector dark current, and, within a narrow range, hydration laye

19 ity of 0.31 A/W), 3 GHz bandwidth, and 30 nA dark current at a reverse bias of 30 V.

20 The induction of prolonged dark currents by intense blue light could be suppressed

21 espectively, were extracted from the forward dark current characteristics.

22 te flash induced a small amplitude prolonged dark current composed of discrete unitary currents simil

23 factors close to unity, and state-of-the-art dark current densities for Ge-based materials.

24 At -5 V reverse bias, the dark current densities of the diodes were measured to be

25 ived rods maintained near normal saturating (dark) current densities by developing abnormally high ra

26 double electron barrier design results in a dark current density of 6.3 x 10(-6) A/cm(2) at 77 K.

27 transport of majority carriers to reduce the dark current density of the device.

28 Steady-state dark current density versus applied potential and open c

29 elength infrared photodetectors with reduced dark current density were demonstrated.

30 is molecular design, we are able to suppress dark current density while retaining high responsivity i

31 The saturation dark current density, J(S), is an important factor in de

32 Dark current in nof cones is also normal, but it is inse

33 a few 10 s of %, few-GHz bandwidths, and low dark currents, in devices with loaded Qs in the range of

34 ed: capacitance, implied depletion width and dark current measurements as functions of applied bias a

35 trochemical impedance spectroscopy (EIS) and dark current measurements.

36 We recorded the dark current noise of individual salamander L cones.

37 ark current (and noise) to values well below dark currents obtained in narrow-band photodetectors mad

38 illumination, and therefore combines the low dark current of a photodiode and the high responsivity o

39 We explore the dependence of the dark current of C(60)-based organic photovoltaic (OPV) c

40 olymers, which can significantly depress the dark current of the polymer photodetectors with little a

41 water splitting over 5 mA cm(-2) before the dark current onset, which originated from the large surf

42 y high bandwidth, zero source-drain bias and dark current operation, and good internal quantum effici

43 rected responsivity (without contribution of dark current) reaches up to 85~88% (VIS) and 26~40% (NIR

44 ated from such mice, despite having a normal dark current, recovered from a light flash markedly fast

45 The initial rate of dark current recovery after 12% rhodopsin bleach was thr

46 We measured tonic activity in light and dark, current responses to changes in luminous intensity

47 noise component contributed 0.022 pA2 to the dark current, roughly equal to the discrete noise varian

48 kinetics of the recovery of the prestimulus dark current that are sensitive to duration and frequenc

49 reased metabolic demand associated with the "dark current." The inner retina had higher MEMRI activit

50 e dark events accounted for 73% of the total dark current variance in the native (A2) state and 46% i

51 inties because of the buffer subtraction and dark currents, we find excellent agreement to experiment

52 rber size, and the resulting capacitance and dark current, while maintaining high quantum efficiency.