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J Neurophysiol (April 1, 2003). 10.1152/jn.00972.2002
Submitted on Submitted 28 October 2002; accepted in final form 5 December 2002
Department of Zoology, University of Washington, Seattle, Washington 98195
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ABSTRACT |
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Picken Bahrey, Heidi L. and William J. Moody. Early Development of Voltage-Gated Ion Currents and Firing Properties in Neurons of the Mouse Cerebral Cortex. J. Neurophysiol. 89: 1761-1773, 2003. Voltage- and current-clamp recordings were made from acute slices of mouse cerebral cortex from embryonic day 14 to postnatal day 17. We targeted cells in the migratory population of the embryonic intermediate zone (IZ) and in deep layers of embryonic and postnatal cortical plate (CP). IZ neurons maintain fairly consistent properties through the embryonic period, all expressing high-input resistance, inward Na+ currents and outward K+ currents, and none showing any hyperpolarization-activated currents. In CP neurons, several changes in physiological properties occur in the late embryonic and early postnatal period: inward Na+ current density is strongly upregulated while outward K+ current density remains almost unchanged, input resistance drops dramatically, and a hyperpolarization-activated current resembling Ih appears. As a result of these changes, the action potential becomes larger, shorter in duration, and its threshold shifts to more negative potentials. In addition, CP cells become capable of firing repetitively and an increasing fraction show spontaneous action potentials. This coordinated development of ion channel properties may help to time the occurrence of developmentally relevant spontaneous activity in the immature cortex.
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INTRODUCTION |
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Spontaneous electrical activity
plays a fundamental role in many aspects of nervous system development,
including DNA synthesis and cell cycle exit (Barish
1998
; Catalano et al. 1997
;
Dutton et al. 1993
; Fields 2001
;
LoTurco et al. 1995
), cell migration (Behar et
al. 2001
; Edgar and Price 2001
; Flint et
al. 1999
; Komuro and Rakic 1992
, 1993
, 1998
;
Maric et al. 2001
), formation and refinement of synaptic
connections (Catalano and Shatz 1998
; Herrmann and Shatz 1995
; O'Leary et al. 1994
;
Penn et al. 1998
; Shatz and Katz 1996
;
Shatz and Stryker 1988
), and development of mature ion
channel properties (Dallman et al. 1998
; Moody
1998
; Spitzer 1991
; Spitzer and Ribera
1998
). The existence and patterns of spontaneous activity in
any given neuron early in its development depend on both the input it
receives (from any existing synaptic inputs and the presence of
nonsynaptically released transmitters in the extracellular space)
(Haydar et al. 2000
; Owens et al. 1996
)
and on its intrinsic ion channel properties.
It has been well established in invertebrate and nonmammalian
vertebrate cells that the properties of ion channels present at early
stages of development can be quite different from those in the mature
state. These differences are critical in determining the existence of
spontaneous electrical activity and in regulating its ability to
mediate activity-dependent developmental events (Catalano et al.
1997
; Dallman et al. 1998
; Greaves et al.
1996
; Gu and Spitzer 1995
; Linsdell and
Moody 1995
; O'Dowd et al. 1988
; Wong et
al. 1993
). Because the properties and types of ion channels present in a cell can change rapidly during development, understanding the roles of immature ion channel properties in activity-dependent development has required detailed maps of ion channel development (Dallman et al. 1998
; Greaves et al.
1996
). Such maps have not been drawn for developing neurons of
the mammalian neocortex in sufficient detail to allow correlations to
be determined between the patterns of ion channel development and the
occurrence of critical developmental periods of spontaneous electrical
activity. Here, we report measurements in neurons of mouse sensorimotor cortex of input resistance (Rin),
inward Na+ current
(INa), outward
K+ current (IK),
and inwardly rectifying currents between embryonic day 14 (E14) and
postnatal day 17 (P17). Our results show that each of these properties
is regulated in a different way during embryonic and early postnatal
development and suggest that early postnatal periods of spontaneous
activity may in part be regulated by the developmental expression of
currents that support repetitive firing ability in individual neurons.
The neurons that populate the layers of the mammalian neocortex arise
in part from repeated divisions of precursors in the neocortical
ventricular zone (VZ), a proliferative population that in rodents
actively generates neuronal precursors during most of the latter third
of embryonic development (Luskin et al. 1988
;
Takahashi et al. 1994
). A secondary proliferative
population, responsible for generating most cortical glia, persists
much later in development (Goldman 1995
; Levers
et al. 2001
). During neurogenesis, which in mouse occurs
between about E11.5 and E17, depending on neocortical region, a
steadily increasing fraction of the proliferative population exits the
cell cycle in the VZ and migrates outward through the intermediate zone
(IZ) to final destinations in the cortical plate (CP) (Caviness
1982
; Shoukimas and Hinds 1978
; Sidman
and Rakic 1973
). Presumptive neurons that exit the cell cycle
at earlier days occupy the deeper cortical layers, and those that exit
later migrate through these to form the more superficial layers. This
radial migratory process appears to generate the pyramidal cell
population (Anderson et al. 1999
; Mione et al. 1997
; Tan et al. 1998
). More recent evidence
indicates that a large fraction, if not all, of the inhibitory
interneurons of the rodent cortex arise in the VZ of the ganglionic
eminencies, the precursors of the striatum in the adult animal
(Anderson et al. 1999
, 2001
; Parnavelas et al.
2000
).
In various studies of membrane properties of the embryonic rodent
neocortex, proliferating populations have been found to primarily
express voltage-gated K+,
Ca2+-activated K+ and small
Na+ conductances when input resistances are
sufficient to permit detection of small currents (Bulan et al.
1994
; Hallows and Tempel 1998
;
Martin-Moutot et al. 1987
; Mienville and Barker
1997
; Mienville et al. 1994
; Noctor et
al. 2002
; Picken Bahrey and Moody 2003
). Na+ currents then increase throughout development
as cells begin to migrate and differentiate (Couraud et al.
1986
; Hamill et al. 1991
; Huguenard et
al. 1988
; Luhmann et al. 2000
; Mienville
et al. 1994
; Picken Bahrey and Moody 2003
;
Villegas et al. 1994
). Changing levels of expression of
L-type, low- and high-voltage-activated (LVA and HVA)
Ca2+ currents (Lorenzon and Foehring
1995
; Tarasenko et al. 1998
), as well as
voltage-gated inactivating (IA) and
delayed rectifier K+ currents (Bekkers
2000
; Hamill et al. 1991
; Korngreen and
Sakmann 2000
; Mienville and Barker 1997
), occur
during both embryonic and postnatal development. Cells of the
developing cerebral cortex gain the ability to generate activity as
early as E18 (Hamill et al. 1991
; Luhmann et al.
1999
), and there is some evidence that both
Na+ and outward K+ currents
can be modulated by activity patterns (Desai et al. 1999
). Here we show that presumptive neurons migrating through the IZ have relatively consistent electrophysiological properties that
change very little with developmental stage: high-input resistance, delayed K+ currents, small inward
Na+ currents, and no hyperpolarization-activated
currents. After they enter the CP, however, these properties begin to
change. Input resistance drops dramatically by P12.
Na+ current density increases while
K+ current density remains constant. A slow,
hyperpolarization-activated current resembling
Ih appears abruptly at about P6.
During the period in the CP, neurons also gain the ability to fire
repetitive action potentials during long depolarizing stimuli, and many
begin to show spontaneous, repetitive action potentials.
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METHODS |
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Animals
Timed pregnant C57Bl/6 mice were obtained from ATL, Kent, WA.
Pregnant females were killed on gestational day 13-18 (E13-E18) by
CO2 inhalation according to National Institutes
of Health and institutional guidelines. Both uterine horns were
dissected out and placed in ice-cold prenatal artificial cerebral
spinal fluid [preACSF, which contained (mM) 119 NaCl, 2.5 KCl, 1.3 MgCl2, 2.5 CaCl2, 1 NaH2PO4, 26.2 NaHCO3, and 11 D-glucose
(Mooney et al. 1996
); unless otherwise noted, all
chemicals were obtained from Sigma, St. Louis, MO] bubbled with
carbogen (95% O2-5% CO2).
Pups were removed from the uterus and staged by visual inspection or crown to rump length, and cerebral cortices were dissected out and
placed in ice-cold preACSF, keeping intact the section from olfactory
lobes through a portion of the brain stem. Some brains were then
embedded in a 3% solution of Type IX-A Ultra-low temperature gelling
agarose in preACSF that had cooled below 32°C, and placed on ice
until the agarose was gelled. Others were mounted directly to a metal
pan for slicing.
Postnatal pups were killed according to institutional guidelines, and
cerebral cortices were removed to ice-cold postnatal ACSF [postACSF,
which contained (in mM) 115 NaCl, 4.3 KCl,
2CaCl2, 2 MgCl2, 0.28 MgSO4, 0.22 KH2PO4, 0.85 Na2HPO4, 27 NaHCO3, and 25 D-glucose
(Beier and Barish 2000
)] bubbled with carbogen.
Olfactory lobes and brain stem were removed, and cerebral cortices were mounted directly on a metal pan for slicing.
Coronal slices (200 µm) were cut using a Vibratome 1000 (Technical Products International, St. Louis, MO), removed from the agar if embedded, and allowed to recover in oxygenated room temperature preACSF or postACSF for 60-90 min before recording.
Voltage-clamp recordings
Pipets were pulled to a resistance of 8-12 M
from 50 µl
hematocrit glass capillary tubes using a Narishige two-stage puller (PP-83 and PP-830, Japan), coated with silicone elastomer (Sylgard 184;
Dow Corning, Midland, MI), and filled with potassium internal solution
[potassium methylsulfate, which contained (in mM) 113 KMSO4 (ICN Biomedicals), 20 KCl, 10 HEPES, 2, MgATP, 3 Na-ATP, and 0.2 Na-GTP, pH to 7.25; or potassium gluconate,
which contained (in mM) 100 KGluconate, 0.5 EGTA, 5 MgCl2, 40 HEPES, 2 Na-ATP, and 0.3 Na-GTP, pH to
7.25]. In a few cases 3,000 M
biotin dextran (2%; Molecular
Probes, Eugene, OR) or Neurobiotin (2%; Vector Laboratories,
Burlingame, CA) were added to the recording pipette for later
confirmation of cell morphology.
Voltage-clamp experiments were performed using the whole cell
patch-clamp technique (Hamill et al. 1981
). All
recordings were made at room temperature (24-26°C) in pre- or
postACSF. Slices from the somatosensory cortex were chosen for
recording and were placed in a 1.2-ml recording chamber and perfused at
a rate of 0.6 ml/min with carbogen bubbled pre- or postACSF.
Individual cell somas were visualized with an upright Axioskop (Zeiss,
Germany) using a water immersion ×63 objective with DIC optics (Fig.
1C). Cells within a region
200 µm dorsal to the striatal border were targeted prenatally and
within 300 µm dorsal to the caudatopallial angle postnatally. In
prenatal recordings, IZ cells located in the middle of the lateral IZ,
and CP cells located in the middle of that region were targeted (Fig.
1A). In postnatal recordings, cells with a pyramidal
morphology were targeted (Fig. 4A).
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Pipettes were lowered onto individual visualized cells, keeping
constant positive pressure to avoid clogging. Pressure was then turned
off when the cell was touched, and a seal >4 G
usually formed
within 2-10 s. A holding potential of
60 mV was applied, and brief
pulses of suction were applied until the membrane inside the pipette
ruptured. Recordings were made using a List EPC-7 (Heka Elektronik,
Lambrecht/Pfalz, Germany) or Axopatch 1-D (Axon Instruments, Foster
City, CA) amplifier. The resulting currents were filtered at 1 kHz and
recorded and analyzed using pCLAMP8 software (Axon Instruments).
Most cells were also held under current clamp to investigate activity.
Histology
Slices with cells filled with Neurobiotin or biotin dextran were
fixed in 4% paraformaldehyde in 0.1 M PBS (pH 7.2) for 1 h at
room temperature or overnight at 4°C. After four washes in PBS, the
slices were treated with 3% hydrogen peroxide for 10 min and rinsed in
0.3% Triton-X 100 in PBS (PBS-TX). Slices were incubated for 2 h
in an avidin-biotin horseradish peroxidase BSA solution (Vector
Laboratories ABC kit with 2% bovine serum albumin added) and again
washed four times in PBS-TX. Fills were developed with diaminobenzidine
and glucose oxidase,
glucose, NH4Cl, NiCl, and
dehydrated through an ethanol series. Slices were cleared using
cedarwood oil or xylene and mounted on slides in DPX (Fluka, Switzerland). Images were acquired with a ZVS3C75DE Digital Camera system (Zeiss) mounted on an Axioskop upright microscope with Optronics
software (Optronics, Goleta, CA). Images were stored using Adobe
Photoshop 6.0 (Adobe Systems, San Jose, CA).
Analysis methods
Input resistance (Rin) was
calculated from the average of responses to voltage pulses to ±10 and
±20 mV from
60 mV. A triangle wave voltage command was then played
to the cell, and capacitance measurements were calculated from the
amplitude of the resulting square-wave current (Moody and Bosma
1985
). Current density was calculated as peak current divided
by the capacitance of the cell. Kinetics of activation and inactivation
were determined by fitting exponential curves to the appropriate
portions of the current trace within pCLAMP8 software. Histograms were
created in Sigmaplot (SPSS Science, Chicago, IL), and statistics
(descriptive and Student's t-test) were done in Microsoft
Excel (Microsoft, Redmond, WA). Figure data are shown as means ± SE, with n values noted.
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RESULTS |
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Development of Na+ and K+ currents in IZ cells
We recorded from 103 IZ cells in animals aged E13 to E18 (see Fig.
1B). Mean input resistance of the IZ cells did not change significantly across embryonic days, ranging from 7,350 ± 2,594 M
at E16 (n = 17) to 4,085 ± 714 M
at E17
(n = 7; P = 0.44; Fig. 1D).
Capacitance also changed very little during these stages, although the
difference between the maximum value of 6 ± 1 pF at E17 and the
minimum of 4 ± 0.3 pF at E18 was marginally significant (P = 0.046; Fig. 1E). Our previous work
showed that in embryonic mouse cortex, dye coupling as seen in Fig.
1B is not associated with significant electrical coupling,
so that voltage-clamp measurements are accurate for the recorded cell
without resorting to uncoupling methods (Picken Bahrey and Moody
2003
).
In previous work (Picken Bahrey and Moody 2003
),
we showed that the amplitude of the inward Na+
current increased as presumptive neurons exit the cell cycle in the VZ
and migrate into the IZ. This implies that
INa amplitude is determined by
developmental stage of individual cells, i.e., by state of migration
and time since cell cycle exit, rather than by chronological age of the
embryo. If this is true, then mean INa
amplitude in IZ cells should be similar at different stages because the
IZ is a constantly changing population of cells that began migration at
a similar time interval following cell cycle exit.
As shown in Fig. 2A (also see insets Fig. 3E), INa amplitude was similar in IZ cells at most of these stages, with no significant differences between any pair of stages except E13 and E14-16 (E13: 24 ± 7 pA, n = 9; E14: 58 ± 6, n = 40; P = 0.02; data included only from cells with measurable INa). This indicates that presumptive neurons acquire functional INa as a result of individual differentiation and migration, not as a function of overall developmental time. Because capacitance of IZ cells did not vary during this period (Fig. 1E), INa density in IZ cells was also constant during this interval of development. There was, however, some variation in the fraction of IZ cells expressing detectable INa, decreasing from a high of 100% at E16 to a low of 67% at E18 (P = 0.021 by Fisher's exact test; Fig. 2B).
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The other major current in these cells is a delayed outward
K+ current, which is present in virtually all
cells at all stages (102/103), as it is in VZ cells (Picken
Bahrey and Moody 2003
; M. Albrieux, J. C. Platel, A. Dupuis, M. Villaz, and W. J. Moody, unpublished data). Unlike
INa, the mean amplitude of
IK decreases steadily by about 50%
between E13 and E18 (392 ± 62 pA at E13 to 157 ± 46 pA at
E18, n = 11 and 12, respectively; P = 0.008; Fig. 3, A and insets in E).
Because capacitance does not change during this period (see Fig.
1E), average IK density
declines similarly. In addition to the decrease in amplitude, the
activation kinetics of IK slowed
somewhat between E13 and E17 (E14: 0.9 ± 0.1 ms,
n = 41; vs. E17: 5.3 ± 1.4 ms, n = 5; P = 6.9 × 10-10; Fig.
3C). Neither the voltage dependence nor the inactivation of
the outward K+ current change during this time
(Fig. 3E).
Closer analysis of IK amplitudes suggests that the decrease in amplitude may represent a loss of cells with large IK amplitudes rather than a shift of the entire population to lower amplitudes. Figure 3, B and D, compares frequency histograms of IK amplitudes at E13-15 and E16-18. At the earlier stages, the distribution shows some indication of two populations, one centered around 150 pA and the other around 350 pA. At the later stages, the entire population is well described by a single distribution centered around the lower value of 150 pA with an almost complete absence of the high IK cells.
Development of Na+ and K+ currents in CP and deep layer pyramidal cells
The IZ is a continuously changing cell population, in which cells
present on different embryonic days share a common state of
differentiation. The preceding data indicate that this is reflected in
relatively static physiological properties. Once these cells take up
their positions in the layers of the forming cortical plate, however,
this situation changes. As developmental time progresses, CP cells
should continue to differentiate physiologically to gain the ability
for robust repetitive firing and to form the variety of firing types
characteristic of the mature cortex (Connors and Gutnick
1990
; Massengill et al. 1997
). To follow the
early stages of this process, we recorded from cortical cells at stages between E14 and P17, binning our data as follows: E14 (E13-14), E16
(E15-16), and E18 (E17-18) prenatally; P0 (P0-1), P2 (P2-3), P4
(P4-5), P6 (P6-7), P10 (P10-11), and P12 (P12-17) from postnatal cortex.
The same lateral region of the cortex was targeted at each stage, and cell type was noted, where possible. During embryonic stage recordings, we targeted cells in the mid-CP, with a few in the deeper parts of the developing CP. These cells are primarily cells of the early forming deeper layers but may include cells from the subplate or those of mid-layers still migrating through the deeper layers toward the pia. For postnatal recordings, we almost exclusively targeted pyramidal cells in the deeper layers by noting morphology under DIC optics. This morphology was confirmed in some cases by dye filling with a biotin-conjugated dextran (Fig. 4A).
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The input resistance of CP cells dropped dramatically, by about a
factor of 30, between E14 and P12 (Fig. 4B). This decrease occurred in two abrupt phases, one between E14 and E16 (E14:
17,065 ± 4,104 M
, n = 23; E16: 6,396 ± 1,502 M
, n = 20; P = 0.03), and
another between P2 and P6 (P2: 4,901 ± 1,403 M
,
n = 8; P6: 1,662 ± 823 M
, n = 18; P = 0.047). Except for the high value at E14, the
input resistances of CP cells in the embryonic and perinatal period
(E16-P2) are the same as those found in IZ cells (5,145 ± 554 M
; Fig. 4B, dashed line). By P12, CP input resistances have decreased by a factor of 10 from this value. This indicates that,
for the most part, cells that are migrating through the IZ in the
embryonic period maintain their resting membrane resistance as they
enter the CP and then subsequently acquire the low resting membrane
resistance characteristic of mature cortical neurons over their first 2 weeks of residence in the CP.
To test whether this decrease in input resistance could simply be a
function of cell growth, we measured capacitance of CP cells over the
same period of development (Fig. 4C). Capacitance showed a
substantial increase, beginning at about the time of birth, by a factor
of about 6 (E14: 6.7 ± 0.3 pF, n = 23; P10: 38.4 ± 6.8 pF, n = 12; P = 2.0 × 10
7). This increase in capacitance
is not large enough to account completely for the decrease in input
resistance and does not exactly match its time course. Therefore it is
likely that the decrease in resistance of CP cells during this period
is caused by a combination of growth and the insertion of new resting channels.
Over the same period of development, the amplitude of inward Na+ currents in CP cells increases by a factor of 10, from 72 ± 24 pA at E14 (n = 18) to values averaging about 800 pA between P2 and P12 (Figs. 5 and 7). (The apparent peak at P10 is not significantly different from values at P6 and P12). This increase is larger than the increase in capacitance over the same period, so Na+ current density shows a similar, though somewhat smaller, increase during this period (INa density is 14 + 5 pA/pF at E14, n = 16, and 83 + 30 pA/pF at P6, n = 13; P = 0.016). Although we also measured a slight negative shift in the activation voltage of INa during this period, it is likely that at later postnatal stages, when Na+ currents are quite large, voltage-clamp control is degraded sufficiently to make measurement of this difference unreliable. For the same reason, it is possible that our values for maximal INa at later stages are underestimates of the actual values.
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Delayed K+ currents showed a similar pattern of
increase in CP cells from E14 through P12. At E14,
IK amplitude (measured at +70 mV) was
327 ± 41 pA (n = 23), and by P12 had increased by about a factor of four to 1,198 ± 526 pA (n = 9;
P = 0.012 compared with E14; Figs.
6A and
7). Unlike the case for
INa, however, the IK increase was approximately the same
as the increase in capacitance, so that
IK density showed no significant
increase through the period from E14 to P12 (E14: 50 ± 6 pA/pF,
n = 22; P10: 65 ± 18 pA/pF, n = 9; P = 0.31). This indicates that the increases in IK amplitude during this period most
likely reflect cell growth and the proportionate insertion of
K+ channels. Differences in the time courses and
magnitudes of INa and
IK development are also seen at
earlier stages (Picken Bahrey and Moody 2003
) and thus
emphasize the different developmental control of these two types of
currents during early cortical development.
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Pyramidal cells of mature mouse cortex often express currents activated
by hyperpolarization, such as the nonselective cationic inward
rectifier, Ih (Fields et al.
2001
; Franz et al. 2000
). Our recordings in VZ
and IZ cells at embryonic stages, however, indicate that
hyperpolarization-activated currents are almost completely absent in
these populations (Picken Bahrey and Moody 2003
) (see
preceding text). In CP neurons, an
Ih-like current appears rather
abruptly near the end of the first postnatal week (Fig. 6B).
From E14 to P4, less than 10% of cells (3/41) showed any
hyperpolarization-activated currents (Fig. 6, B and
C). In those three cells, the current we recorded activated
slowly, showed inward tail currents at
60 mV and had a mean amplitude
of 38 ± 23 pA (measured at
120 mV). At P6, we observed a sudden
increase in the number of neurons expressing this current (70%; 20/28
between P6 and P12; Fig. 6, B and D), and a large
increase in the mean amplitude in cells with the current (101 ± 25 pA). This indicates that Ih is
almost exclusively a postnatal property of CP cells. Two cells at P8
showed a complete and reversible block in the presence of 5 mM cesium
(a blocker of Ih).
It is not easy to predict how the variety of changes in voltage-clamp properties of CP cells between E14 and P17 might translate into development of firing patterns. The large increase in INa accompanied by a stable IK should increase neuronal ability to generate action potentials. The large decrease in input resistance, however, might well degrade that ability. To measure firing properties directly, we recorded from CP cells at each stage under current-clamp conditions and measured their ability to generate action potentials after the termination of short depolarizing current pulses, their ability to fire repetitively during long stimuli, and the existence of spontaneous activity in the absence of applied current. These results are summarized in Figs. 8 and 9.
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At early embryonic stages, CP cells were very limited in their ability
to generate action potentials (Figs. 8 and 9A). At E14, for
example, only 31% (4/13) of cells generated an active response
(defined as a positive dV/dt) after the
termination of a short stimulus, a fraction only half as large as the
fraction of cells with detectable Na+ currents
measured in voltage clamp (65%). This discrepancy is probably due to
the long time constant of the cells at this stage shunting the
relatively rapid Na+ current. No cell at E14
showed spontaneous action potentials in the absence of stimuli. By the
later embryonic stages, a much larger fraction of cells responded to
stimuli with active responses. At E17-18, 80% (4/5) of cells were
capable of generating an active response following the termination of a
brief stimulus. These were broad responses with a high threshold
(
21 ± 3 mV, n = 7; Fig. 9, B and
C). Despite this change, however, no cells at any embryonic
stage showed any spontaneous action potential activity in the absence
of stimuli (resting potential was fairly depolarized:
40 ± 2 mV, n = 34), and none were capable of firing repetitive action potentials during a 150-ms stimulus (Figs. 8, E17, and 9D).
The large increases in INa
amplitude that occur perinatally (see Figs. 5 and 7) change this
situation considerably. By P0, 83% of cells generated an action
potential with a slightly shorter duration following the termination of
a short pulse, and two of eight cells tested were capable of firing
repetitively during a 150-ms depolarizing stimulus. These same two
cells also showed some spontaneous action potentials, apparently
resulting from postsynaptic potential (psp) like input on a resting
potential of
54 ± 5 mV (n = 14; Figs. 8,
P0, and 9D). Cells at P2 appeared to be similar
to P0 neurons in firing ability with 57% (4/7) generating action
potentials after a short pulse and 38% (3/8) both firing repetitively
during a 150-ms pulse and generating spontaneous spikes.
Although the percentage of cells generating an action potential after a short stimulus did not change from earlier postnatal stages (66%), at P6, we saw an increase in the fraction of cells generating repetitive action potentials during long pulses (83%). These action potentials were even shorter in duration than those at early postnatal stages (Fig. 9C). Only 25% of cells generated spontaneous action potentials, however.
At the latest stages, P10-P12, 100% of recorded cells generated
action potentials after a short stimulus at a threshold that had
dropped more than 10 mV, to
34 ± 3 mV (n = 12;
Fig. 9B). Almost 70% of recorded pyramidal neurons were
capable of repetitive firing during a long stimulus, and 65% fired
spontaneously, often in response to psp-like depolarizations on an
already depolarized resting potential (see Figs. 8, P10,
and 9B).
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DISCUSSION |
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To begin to understand how the patterns with which voltage-gated ion channels develop in the mammalian neocortex, we have measured Na+, delayed K+, and inwardly rectifying currents in neurons of the mouse sensorimotor cortex between E13 and P17. We concentrated on migratory presumptive neurons of the IZ from E13 to E18, and differentiating neurons of the cortical plate and deep cortical layers from E14 to P17. Our data indicate that all three types of currents, and cell input resistance, develop in different patterns during this interval.
The IZ represents a continuously changing population of cells that have
exited the cell cycle in the VZ recently and that are migrating to take
up their positions in the CP. Therefore IZ cells at E14 and E18, for
example, should be similar in developmental state but different in both
chronological age and in the cortical layer they are destined to
occupy. We found that IZ cells were almost identical in their
electrophysiological properties over the interval E13-E18. Cell input
resistance, capacitance, and INa
amplitudes did not vary significantly with stage. No IZ cells expressed
any hyperpolarization-activated currents. The only change we observed
was a steady decrease in IK amplitude
of about 50% between E13 and E18. This could arise in two ways. First,
a slight decrease in IK might occur as
cells migrate out of the VZ into the IZ. This could be true only at
later stages; however, because we have measured
IK in the VZ at E12, E13, and E14, and
mean amplitudes are not distinguishable from
IK amplitudes in E13-E15 IZ. A
progressively greater loss of IK as
cells exit the VZ at later and later stages, however, could indicate a
layer-specific level of IK expression, with cells fated to more superficial layers having smaller
IK amplitudes at least during
migration. Another possible explanation is that the presumptive
inhibitory interneurons that migrate from the ganglionic eminences into
the neocortical IZ (Anderson et al. 2001
; Marin
and Rubenstein 2001
; Parnavelas et al.
2000
) express different levels of
IK than do cells that arise locally in
the neocortical VZ. This explanation is consistent with our finding of
two populations of cells in the IZ defined by
IK amplitude. The first population,
with IK of around 150 pA, persists
from E13 to E18 and may represent the population of radially migrating neurons from the VZ. The second population, defined by their larger IK (300-800 pA), is present from E13
to E15, during the days of greatest migration of subpallial cells
destined for the developing cortex (Marin and Rubenstein
2001
), but disappears at later stages (see Fig. 3, B
and D). If this second population represents the GABAergic
interneurons migrating from the ganglionic eminences, their early
presence and later loss could easily explain the decline we see in
IK with developmental stage. Previous
findings by Hamill et al. (1991)
, showing that pyramidal
and nonpyramidal neurons in embryonic rat cortex express identical
Na+ current densities but different
K+ currents, are consistent with this possibility.
The CP presents a different population of cells than the IZ, being composed primarily of postmigratory neurons undergoing terminal neuronal differentiation. We concentrated on the deep layers of the CP and postnatal cortex that are formed earlier in development than the more superficial layers, allowing us to study a longer interval of development in a single population. The population is not entirely postmigratory, however, as migratory neurons destined for the more superficial layers transiently pass through those deeper layers.
We found a dramatic decrease
between 10- and 30-fold
in input
resistance over the interval E14 to P12 in CP cells. This decrease occurred in two stages, one between E14 and E16, the other between P2
and P4. A portion of the drop in input resistance may be due simply to
cell growth because capacitance decreases over the same period,
although by a much smaller amount. It is possible, however, that our
measurement of the increase in capacitance underestimates membrane
growth relative to input resistance measurements because capacitance is measured at considerably higher frequencies and thus
may measure a smaller fraction of actual surface area in cell processes
that are extending during this period. If we assume that the increase
in surface area does, in fact, account only for a portion of the input
resistance change, then the appearance of a new resting conductance
must be responsible for the remainder of this change. A
hyperpolarization-activated current (presumably Ih) appears postnatally in CP cells
(Fig. 6B). Although little of this current is activated at
the resting potential, the time course of its appearance is similar to
the drop in input resistance, and the appearance of even a small
resting conductance may have a large effect on cells that previously
had a very low resting conductance. We do also see a positive shift in
resting potential during the second postnatal week (see Fig.
9B), after a significant number of cells already express
Ih, so it is possible that even a
small contribution of Ih, with its
positive reversal potential, to an initially small resting conductance
could cause both the decrease in input resistance and the positive
shift in resting potential.
The second major change we see in CP cells is the very large increase
in amplitude of INa beginning at late
embryonic stages (Figs. 5 and 7). INa
increases by more than a factor of 10, much greater than the membrane
area increase during the same period. It is not clear whether this
represents the appearance of a new Na+ channel
subtype or an increase in density of the subtype already present
(Gong et al. 1999
; Yarowsky et al. 1991
;
Zhang et al. 2001
). Also beginning in the late embryonic
period, there is an increase in amplitude of the delayed outward
K+ current, although this change is much smaller
and can be accounted for simply by the increase in cell surface area.
Finally, we see the appearance of a hyperpolarization-activated
(inwardly rectifying) current in CP cells. This current appears
relatively late in comparison to the increases in
INa and
IK. Between E14 and P4, only very few
cells express this current. Between P4 and P6, there is a large
increase in the fraction of cells expressing this current so that from
P6 to P17, it can be detected in more than 80% of cells. This inward
current activates slowly on hyperpolarization, with very little current
passing positive to
70 mV (although there was measurable current at
voltages as positive as
50 mV in a few cells) and a voltage-dependent
time constant of about 330 ms at
90 mV and 180 ms at
120 mV.
Although we cannot definitively identify this current as
Ih, the kinetics and voltage
dependence are very similar to those published previously to describe
Ih (DiFrancesco et al.
1986
; McCormick and Pape 1990
; Spain et
al. 1987
), and block by Cs+ is a further
indication that this current is Ih.
These complex changes in channel expression in developing CP cells have profound effects on the firing properties of the cells. In embryonic stages, CP cells show relatively low levels of excitability. When active responses can be elicited (27% of embryonic CP cells overall), they tend to be small and long in duration (Figs. 8, E14 and E17, and 9C). The peaks of these responses are not sufficiently depolarized to activate a substantial fraction of the delayed K+ current, and combined with the long time constant of embryonic cells (due to their high-input resistances), this results in a prolongation of the falling phase the active response so that it follows the membrane time constant (see Fig. 8, E14-middle). None of our embryonic CP cells fired repetitively during long depolarizing stimuli. This does not, however, mean that embryonic CP cells do not fire repetitively in vivo. It is quite possible that these cells are subject to complex waveforms of depolarizing stimuli normally and that some of these can evoke different firing patterns than we see in response to simple square-wave depolarizations.
This situation changes after the perinatal period. The combination of
increasing Na+ and K+
current, decreased input resistance leading to faster time constants, and eventually, a more depolarized resting potential at the end of the
second postnatal week results in the appearance of more rapidly rising
and falling action potentials and repetitive firing ability.
Ih may also impart a slow
depolarization encouraging repetitive firing at these later stages
(Bender et al. 2001
; Luthi and McCormick
1998
; Moosmang et al. 1999
). Consistent with
this idea, we found that 78% of cells expressing
Ih generate evoked or spontaneous
AP's compared with only 37% of cells not expressing Ih (P = 0.0078 Fisher's exact test). An even greater difference exists between the
percentage of cells with Ih that
generate either evoked or spontaneous repetitive activity (72%) and
those without Ih (7%;
P = 3.5 × 10
6, Fisher's
exact test). In addition, current-clamp recordings made in the absence
of stimuli indicate that a steadily increasing fraction of postnatal
cells are normally firing repetitively (see Fig. 8, P2 and P10). This
latter conclusion, however, must be made with caution. Although the
ability to fire repetitively clearly develops during this early
postnatal period, we cannot be certain that the spontaneous activity we
observe is not secondary to depolarization induced by leakage currents
through the seal resistance. Although this leak should be less
important in the lower resistance postnatal cells than in the high
resistance embryonic cells, it still may interact with the more
negative threshold to induce activity in some cases. We believe that at
least some spontaneous activity is occurring normally, though, because
we have recorded activity on hyperpolarized baselines and because we
have observed spontaneous transient increases in intracellular
Ca2+ using optical methods in these cells in the
early postnatal period (unpublished observations).
Many of the developmental changes we have observed are summarized in
Fig. 10. Here, we take our data
(including that of Picken Bahrey and Moody 2003
) in VZ,
IZ, and CP cells between E14 and P17 to recreate a likely picture of
the development of ionic currents in a single cell as it divides in the
VZ, exits the cell cycle there at E14, migrates through the IZ, arrives
in the CP on E16, and then undergoes later neuronal differentiation. As
it proliferates, the presumptive neuron has very simple electrical
properties: a high-input resistance and outward
K+ current. On cell cycle exit, a second
conductance
a small Na+ current
appears and
begins to increase slowly as the cell migrates. This state continues
until the differentiating neuron arrives at the cortical plate. At this
point, several things happen. First, the cell begins to grow rapidly,
causing increases in Na+ and
K+ current and a decrease in
Rin. Na+ current
and Rin changes are larger than can be
explained by cell growth, however. Lagging slightly behind the increase
in INa and IK, is the initial expression and
increase of a third conductance, the inwardly rectifying cation current
Ih, possibly contributing to the
decrease in Rin. As the complexity of
this cell increases, with expression of
Ih and increases in
Na+ and K+ conductances,
the cell begins to mature electrically, gaining the ability to fire
repetitively.
|
The changing patterns of ion channel expression we observe put some
constraints on the likely generation of spontaneous activity during
early cortical development. If cortical neurons generate repetitive
bursts of action potentials that serve important developmental roles,
then they should be most likely to do so starting in the very early
postnatal period, rather than embryonically. This kind of activity has
in fact been observed in the early postnatal rat neocortex
(Garaschuk et al. 2000
). Although the exact time of onset of such activity has not yet been determined, it is likely that
the onset is limited by the ability of the individual neurons to fire
repetitively. The termination of such activity, however, is probably
determined by the nature of inputs to the cell or by the changing
depolarizing drive supplied by conductances active at the resting
potential because the intrinsic ability to fire repetitively lasts
throughout adulthood. Whatever exact role that intrinsic channel
expression in individual neurons plays in timing spontaneous activity,
it is clear that the changing patterns of channel expression must be
taken into account in describing how developing neurons generate such activity.
| |
ACKNOWLEDGMENTS |
|---|
We sincerely thank Drs. Martha Bosma and Douglas Currie for helpful scientific discussion.
This work was supported by National Institutes of Health Grant NS-38116 and a Royalty Research Fund Grant from the University of Washington to W. J. Moody and NIH Training Grant GM-07270 to H. L. Picken Bahrey.
| |
FOOTNOTES |
|---|
Address for reprint requests: W. J. Moody, Box 351800, Dept. of Zoology, University of Washington, Seattle, WA 98195 (E-mail: Profbill{at}u.washington.edu).
| |
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J Neurosci
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