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. 2010 Dec 8;30(49):16679–16691. doi: 10.1523/JNEUROSCI.3644-09.2010

Table 1.

Time constants of LFD, LFDAR, and PTPLFD were obtained by fitting mean amplitude values of IPSC (I) at any stimulus from n experiments (see Materials and Methods)

Stim. n ωfast (%) τfast (s) ωI (%) τI (s) ωII (%) τII (min)
LFD low P S 9 54.6 ± 4.9 54.5 ± 6.9 45.4 ± 2.3 8.9 ± 1.0
LFD high P S 7 51.9 ± 3.3 39.1 ± 9.7 48.1 ± 5.5 8.1 ± 0.9
Stat. with LFD low P * * NS NS
LFD low P + ApSynAla S 4 64.3 ± 2.1 39.1 ± 7.1 35.7 ± 3.9 10.2 ± 2.8
Stat. versus LFD low P * NS NS NS
LFD low P + PKAi6-22 S 4 57.2 ± 3.8 18.7 ± 2.9 42.8 ± 3.9 6.8 ± 1.7
Stat. with LFD low P NS ** NS NS
LFD high P PP 10 43.3 ± 4.1 26.8 ± 4.5 56.7 ± 5.8 10.4 ± 1.1
LFDAR rest 10 s PP 4 100 1.2 ± 0.2
LFDAR rest 15 s PP 4 100 1.6 ± 0.4
LFDAR rest 20 s PP 6 85.8 ± 5.8 1.0 ± 0.1 14.2 ± 2.0 19.8 ± 6.1
Stat. with LFD high P NS
LFDAR rest 40 s PP 5 86.3 ± 13.5 1.5 ± 0.2 13.7 ± 1.7 70.8 ± 12.0
Stat. with LFD high P **
LFDAR rest 60 s PP 4 76.7 ± 9.7 1.4 ± 0.4 23.3 ± 10.3 34.3 ± 10.2
Stat. with LFD high P NS
LFDAR rest 90 s PP 6 69.0 ± 12.0 1.0 ± 0.2 18.4 ± 7.8 13.2 ± 3.9 12.6 ± 0.6 2.3 ± 0.6
Stat. with LFD high P NS ***
LFDAR rest 120 s PP 5 65.0 ± 12.2 1.4 ± 0.2 22.1 ± 6.0 24.3 ± 8.3 12.1 ± 0.5 2.2 ± 0.1
Stat. with LFD high P NS **
LFDAR rest 240 s PP 4 63.1 ± 3.6 1.6 ± 0.4 23.3 ± 6.1 22.8 ± 5.5 13.6 ± 1.4 3.4 ± 0.3
Stat. with LFD high P NS **
LFDAR rest 900 s PP 7 49.0 ± 8.9 1.3 ± 0.2 29.2 ± 6.1 17.8 ± 2.7 21.8 ± 3.0 4.3 ± 0.3
Stat. with LFD high P NS ***
PTPLFD rest 20 s PP 5 60.3 ± 12.7 1.0 ± 0.1 27.7 ± 5.3 6.6 ± 0.1 12.0 ± 2.7 5.5 ± 0.8
Stat. with LFD high P ** **
PTPLFD rest 120 s PP 3 59.1 ± 6.9 1.6 ± 0.4 26.1 ± 4.1 9.4 ± 3.8 14.8 ± 2.7 3.4 ± 1.2
Stat. with LFD high P ** **
Stat. with PTPLFD rest 20 s NS NS NS NS

Low P and high P correspond to [Ca2+]/[Mg2+]e = 0.42 and [Ca2+]/[Mg2+]e = 2.1, respectively. LFDAR and PTPLFD were probed at [Ca2+]/[Mg2+]e = 2.1. LFD, LFDAR, and PTPLFD were probed using either a single stimulus (denoted as S) or a paired-pulse stimulation (interval, 40 ms; denoted as “PP”). The statistical differences (mentioned as “Stat.”) in the weights (ωI and ωII) and in the time constants (τI and τII) of the exponential decays were tested for two different conditions using either the t test or the Mann–Whitney rank sum test. The statistical difference in τfast calculated during LFDAR and PTPLFD at any rest period was probed using a one-way ANOVA. This test did not detect any statistical difference in τfast (p = 0.64).

*p < 0.05,

**p < 0.01, and

***p < 0.001. NS denotes no significant difference (i.e., p > 0.05).