Table 4.

Characteristics of single cell responses from dark-adapted rods with and without Gγ 1

Dark current (pA)Dim flash time to peak (ms)τ rec (ms)aIntegration time (ms)Io (photons · μm−2)bCellular noise ς 2 (pA2)cAmplification constant (s−2)
1 −/−9.9 ± 0.9 (n = 12)102 ± 15 (n = 12)142 ± 15 (n = 12)193 ± 24 (n = 12)3991 ± 471 (n = 12)0.00927 ± 0.00336 (n = 9)0.367 ± 0.043 (n = 12)
WT13.6 ± 0.7 (n = 29)114 ± 6 (n = 19)174 ± 11 (n = 19)254 ± 19 (n = 19)59.4 ± 3.0 (n = 19)0.0575 ± 0.0199 (n = 8)8.87 ± 0.55 (n = 17)
  • aτrec was determined by fitting a single-exponential function to the final falling phase of the dim flash response.

  • bFlash strength (500 nm) that elicited a half-maximal response.

  • cNoise variance for individual cells was calculated by integrating difference (dark − light) power spectra over a bandwidth of 0.1–20 Hz. All other parameters were determined as by Krispel et al. (2003).