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The Journal of Neuroscience, December 15, 2001, 21(24):9877-9887
Role of Calcium, Glutamate Neurotransmission, and Nitric Oxide in
Spreading Acidification and Depression in the Cerebellar Cortex
Gang
Chen,
Robert L.
Dunbar,
Wangcai
Gao, and
Timothy J.
Ebner
Department of Neuroscience, University of Minnesota, Minneapolis,
Minnesota 55455
 |
ABSTRACT |
This study investigated the mechanisms underlying the recently
reported fast spreading acidification and transient depression in the
cerebellar cortex in vivo. Spreading acidification was evoked by surface stimulation in the rat and mouse cerebellar cortex
stained with the pH-sensitive dye neutral red and monitored using
epifluorescent imaging. The probability of evoking spreading acidification was dependent on stimulation parameters; greater frequency and/or greater amplitude were more effective. Although activation of the parallel fibers defined the geometry of the spread,
their activation alone was not sufficient, because blocking synaptic
transmission with low Ca2+ prevented spreading
acidification. Increased postsynaptic excitability was also a major
factor. Application of either AMPA or metabotropic glutamate receptor
antagonists reduced the likelihood of evoking spreading acidification,
but stronger stimulation intensities were still effective. Conversely,
superfusion with GABA receptor antagonists decreased the threshold for
evoking spreading acidification. Blocking nitric oxide synthase (NOS)
increased the threshold for spreading acidification, and nitric oxide
donors lowered the threshold. However, spreading acidification could be
evoked in neuronal NOS-deficient mice
(B6;129S-Nos1tm1plh). The depression in cortical
excitability that accompanies spreading acidification occurred in the
presence of AMPA and metabotropic glutamate receptor antagonists and
NOS inhibitors. These findings suggest that spreading acidification is
dependent on extracellular Ca2+ and glutamate
neurotransmission with a contribution from both AMPA and metabotropic
glutamate receptors and is modulated by nitric oxide. Therefore,
spreading acidification involves both presynaptic and postsynaptic
mechanisms. We hypothesize that a regenerative process, i.e., a
nonpassive process, is operative that uses the cortical architecture to
account for the high speed of propagation.
Key words:
cerebellum; calcium; glutamate; nitric oxide; optical
imaging; neutral red; rat; transgenic mouse; spreading depression; calcium waves
 |
INTRODUCTION |
Several types of propagating waves
of activity occur in the CNS. Classic spreading depression (SD)
of Leao is characterized by a slowly propagating wave of neuronal and
glial depolarization with large shifts in the ionic gradients that
leads to a profound loss of spontaneous and evoked neuronal activity
(Leao, 1944
; Ochs, 1962
; Lauritzen and Nicholson, 1988
). Astrocytic gap
junctions have been implicated as a possible route for SD propagation
(Largo et al., 1997
; Martins-Ferreira et al., 2000
). Calcium waves in neuronal-glial cultures and in vitro preparations have been
shown to propagate either via glial coupling by gap junctions or an extracellular messenger (Yoon et al., 1996
; Newman and Zahs, 1997
; Guthrie et al., 1999
). Both pathophysiological processes and signaling mechanisms have been ascribed to these propagated activities (Lauritzen and Nicholson, 1988
; Cornell-Bell et al., 1990
; Somjen et al., 1992
;
Newman and Zahs 1997
).
Recently we described a novel form of propagated activity in the rat
cerebellar cortex in vivo based on optical imaging of pH
changes using neutral red (Chen et al., 1999a
). Surface stimulation was
shown to evoke a "parallel fiber-like" beam of activity (Chen et
al., 1998
, 1999a
; Hanson et al., 2000
). In some animals, this beam of
optical activity spread anteriorly and posteriorly across the folium, a
phenomenon referred to as spreading acidification. Transient but
powerful depression of both presynaptic and postsynaptic activity
accompanies spreading acidification. With an average propagation speed
of 450 µm/sec and peak speeds as high as 1100 µm/sec, spreading
acidification travels much faster than other known forms of propagated
activity, including SD at 20-150 µm/sec (Leao, 1944
; Nicholson et
al., 1978
; Somjen et al., 1992
) and calcium waves at 25-100 µm/sec
(Newman and Zahs, 1997
; Kunkler and Kraig, 1998
; Martins-Ferreira et
al., 2000
). Other unique characteristics of this propagated activity
include a stable extracellular DC potential, no change in blood vessel
diameter, and repeatability at short intervals (Chen et al., 1999a
).
Also differentiating this spreading phenomenon from classic SD is its
occurrence in the cerebellum without radical substitution of the ionic
makeup of the extracellular environment (Nicholson and Kraig, 1975
;
Tobiasz and Nicholson, 1982
).
The initial study described and characterized the basic
properties of this propagating acidification and depression (Chen et
al., 1999a
). The goal of the present study was to gain insights into
underlying mechanisms by evaluating the effective stimulation parameters, contribution of presynaptic and postsynaptic components, involvement of various neurotransmitters and receptors, and the role of
extracellular or intercellular messengers, or both. This study
demonstrates that both presynaptic and postsynaptic structures are
involved and that extracellular Ca2+, AMPA
receptors, metabotropic glutamate receptors (mGluRs), and nitric oxide
(NO) all contribute. Purinergic receptors are unlikely to be involved.
Parts of this paper have been published previously in abstract form
(Chen et al., 1999b
).
 |
MATERIALS AND METHODS |
Animal preparation. All animal experimentation was
approved by the Institutional Animal Care and Use Committee of the
University of Minnesota and conducted in conformity with the National
Institutes of Health Guide for the Care and Use of Laboratory
Animals. Experimental details on the animal preparation and
optical imaging techniques have been provided in previous publications
(Chen et al., 1998
; Hanson et al., 2000
) and therefore are only briefly
described here. Adult Sprague Dawley rats (Harlan, Indianapolis, IN) of either sex (200-400 gm) were anesthetized by intramuscular injection of a solution of ketamine (60 mg/kg) and xylazine (3 mg/kg). The trachea was cannulated for artificial respiration, as was the jugular
vein for the administration of fluids. Body temperature was
feedback-regulated. The electrocardiogram was monitored to assess the
depth of anesthesia, allowing anesthetic to be supplemented as needed.
After a craniotomy and creation of a watertight chamber of acrylic
around Crus I and II, the exposed surface was stained by superfusion
with a 10 mM solution of neutral red
(3-amino-m-dimethylamino-2-methylphenazine hydrochloride;
Sigma, St. Louis, MO) for 2-3 hr. An intravenous injection of neutral
red (1 ml at 35 mM) was used to supplement the
bath staining. After staining, the neutral red solution in the chamber
was thoroughly and repeatedly washed out, and the chamber was refilled
with Ringer's solution. The chamber was periodically rinsed with fresh
normal Ringer's solution that was repeatedly gassed with 95%
O2 and 5% CO2 to maintain
a stable pH of 7.4 in the chamber and in the interstitial environment
of the cerebellum.
Transgenic mice with an NO synthase (NOS) gene mutation were also used.
A breeding pair of mice homozygous for a targeted mutation
(B6;129S-Nos1tm1plh) disrupting the neuronal NOS
gene was obtained from JAX mice (Bar Harbor, ME). These animals were
bred and the offspring were used in these experiments when they reached
20-40 gm. The surgical and experimental procedures were similar to
those used in the rat, with the required scaling of the stereotaxic
apparatus, physiological monitoring, and respiratory control system
needed for the mouse. Also, an intraperitoneal injection of neutral red
(0.3-0.6 ml, 35 mM) was used to augment and
prolong the staining of the cerebellar cortex.
Electrical stimulation and electrophysiological monitoring
techniques. Parallel fiber stimulation was delivered by a tungsten microelectrode (1-3 M
) placed just below the cerebellar surface. The stimulation parameters consisted of a train of stimuli delivered at
5-75 Hz for 2-20 sec. Individual stimuli had pulse durations of
100-300 µsec and amplitudes of 100-300 µA. Stimulation intensity including frequency and amplitude were varied in some experiments to
evaluate the dependence of spreading acidification on stimulation parameters. In some experiments, extracellular recordings of the evoked
field potentials were obtained with glass microelectrodes (2 M NaCl, 2-5 M
) using conventional electrophysiological
techniques (Chen et al., 1998
, 1999a
). The field potentials were
digitized (50 kHz), averaged on-line, and stored for additional
off-line analysis.
To evaluate the excitability of the cerebellar cortex in relation to
the spreading optical response, extracellular field potentials were
recorded simultaneously with the acquisition of the images. Two
stimulation electrodes were placed on the surface. The first electrode
was used to evoke spreading acidification, and the second electrode
placed anterior to the first was used to activate a test group of
parallel fibers for assessing the excitability of the cerebellar
circuit. The resultant parallel fiber volley
(positive-negative-positive deflection;
P1-N1-P2
components) and postsynaptic response (longer latency negative
deflection; N2 component) were recorded "on
beam" relative to the second stimulation electrode (Eccles et al.,
1967
; Chen et al., 1999a
). The capture of each image was synchronized with the field potential recordings. The amplitude of
P1 to N1 was used as a
measure of parallel fiber excitability, and the amplitude of
N2 was used as a measure of the postsynaptic
response. In several experiments we also examined the field potentials
evoked as a function of stimulation frequency and amplitude. Of
interest was the accumulative effect of the stimulus train required to evoke spread; therefore, the "summed" field potential evoked by the
initial 1 sec of the train was used. Because at higher stimulus frequencies the field potentials invariably decreased in size with
time, this provided a measure of the accumulated response to the
stimulus train. Both the presynaptic and postsynaptic components were determined.
Optical imaging. After staining while still mounted in the
stereotaxic frame, the animal was placed on a large stage with precision x and y translation. Modified Zeiss
(Thornwood, NY) optics for epifluorescence imaging was mounted above
the animal. Using a stabilized xenon-mercury light source, the
excitation light was passed through a bandpass filter (546 ± 10 nm) while emitted light passed through a long-pass filter (
620 nm).
The cutoff wavelength of the dichroic mirror placed between the
excitation and emission filters was 580 nm. Images were taken with
cooled CCD cameras (PXL-37 with 512 × 512 pixels or Quantix 57 with 530 × 512 pixels, both with 12 bit digitization; Roper
Scientific, Tucson, AZ). The resolution using the PXL-37 camera was
reduced to 170 × 170 by binning pixels on the CCD chip, and when
using a 2× objective, the final image resolution was 14 × 14 µm. The resolution using the Quantix 57 camera was reduced to
176 × 170 by binning pixels on the CCD chip, and when using a 2×
objective, the final image resolution was 13 × 13 µm. The
camera was focused 100-300 µm below the surface of the cerebellar cortex.
The experimental protocol included obtaining a sequence of images. This
sequence consisted of a series of 20 "background" fluorescence
images, followed by a surface stimulation for 2-10 sec. During and
after the stimulation, a second series of images was acquired. The
entire sequence usually consisted of 320-820 images, and each image
was acquired with an integration time (camera exposure time) of 70-120
msec. The time between images was 40-50 msec for the PXL-37 camera and
<0.1 msec for the Quantix 57 camera. No frame averaging was
undertaken. Quantification of the optical signal in each image in the
series, Fi, was based on the net
fluorescence change as a function of the background fluorescence,
FB; that is,
F = (Fi
FB)/FB.
The average of the 20 background frames was used as
FB. Then the average
F
in regions of interest was determined. For most experiments, the region
of interest was the folium stimulated. In some experiments, several
regions of interest were defined at various locations, and the average
F in each region was determined. Figure display was based
on the subtraction of FB from the
entire sequence of images, Fi, and
displaying the resultant images.
Pharmacological manipulations and drugs. To gain insights
into the neurotransmitter systems involved in the spreading optical response, various receptor antagonists were applied to the cerebellar cortex. To alter the production of NO, a nitric oxide synthase inhibitor and NO donor were used. To examine whether the optical signals were attributable to swelling of cellular processes or the
accompanying reduction in extracellular space (Holthoff and Witte,
1996
), furosemide, a blocker of anion transport (Ransom et al., 1985
;
Holthoff and Witte, 1996
; Muller and Somjen, 1999
), was used. For most
compounds, stock solutions (1-10 mM) were made in saline,
stored at
20°C and diluted to the required concentration in normal
Ringer's solution before each experiment. If required, the solution
was prepared fresh on the day of use. All drugs were applied to the
exposed cerebellar surface by superfusion of the drug solution in the
chamber. If needed, drugs were removed by repeated washout of the
chamber with normal Ringer's solution. For repeated testing of a
pharmacological agent or different agents, separate animals were used.
The number of animals reported for each drug refers to experiments
performed in different animals.
(RS)-
-Methyl-4-carboxyphenylglycine (MCPG) and
(RS)-
-methylserine-O-phosphate (MPPG) were
purchased from Tocris Cookson Inc. (Ballwin, MO). Neutral red,
N-nitro-L-arginine (NLA), furosemide, and suramin were purchased from Sigma (St. Louis, MO). The following drugs were obtained from Research Biochemicals (Natick, MA):
L(+)-2-amino-3-phosphonopropionic acid (AP-3),
D(
)-2-amino-5-phosphonopentanoic acid
(AP-5), (
)-bicuculline methiodide,
1(S),9(R)-(bicuculline),
6-cyano-7-nitroquinoxaline-2,3-dione disodium (CNQX),
pyridoxal-phosphate-6-azophenyl-2',4'-disulfonic acid tetrasodium
(PPADS), (±)-3-amino-2-(4-chlorophenyl)-2-hydorxy-propylsulfonic acid
(saclofen), S-nitroso-N-acetylpenicillanine
(SNAP), and tetrodotoxin (TTX).
 |
RESULTS |
Spreading acidification and depression: dependence on stimulus
parameters and neuronal activation
Electrical stimulation of the cerebellar cortex with a brief train
of pulses evoked a narrow beam of increased fluorescence transversely
across the folium (Fig.
1A). This beam-like
activity is attributable to the activation of a bundle of parallel
fibers and their postsynaptic targets and in large part is attributable to the resulting intracellular acidification (Chen et al., 1996
, 1998
).
In some preparations, this activity propagated throughout the folium
and into neighboring folia (Fig. 1A). In this
example, at ~6.1 sec from the onset of stimulation, the optical
response began to spread orthogonally to the parallel fiber beam moving rapidly across the surface of the folium. By 6.6 sec, the optical signal had reached the posterior edge of Crus IIa, and by 6.9 sec, it
had reached the anterior edge. The propagation speed across Crus IIa
was 782 µm/sec. After an additional delay of 7.5 sec attributable to
traversing the intrasulcal distance, the optical response spread to the
anterior edge of the neighboring folium, Crus IIb (Fig.
1A, 14.1). The optical signal then spread
rapidly across the surface of Crus IIb, reaching its posterior boundary within 22.0 sec.

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Figure 1.
Propagation of the optical response in Crus IIa
and b. A, Series of optical images (stimulation minus
background) illustrating the effect of surface stimulation (150 µA,
150 µsec pulses at 10 Hz for 10 sec). The first image
is a background image and also shows the position of the stimulating
electrode (see B, C). Numbers are the
times in seconds relative to the onset of stimulation. Different time
intervals are shown to highlight different aspects of the propagation.
B, C, Background images of the folia and the regions of
interest (boxes with numbers or
letters) at which the fluorescence changes were
measured. Boxes were selected to show the propagation
parasagittally across the folia in B and transversely
within a folium in C. D, Intensity of
optical response as percentage of
F/F as a function of time for the
regions of interest in B. E, Intensity of
optical response as percentage of F/F
as a function of time for the regions of interest in C.
For this and the following figures, the bar beneath the
x-axis denotes time of stimulation. The orientation of
the image and scale bar are as indicated.
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Several 10 × 10 pixel regions of interest were selected in the
parasagittal plane (Fig. 1B) and in the transverse
plane (Fig. 1C) to illustrate the amplitude
(
F/F) and time course of the optical
signal (Fig. 1D,E). During the first 6 sec of the
stimulus train and before the onset of spreading acidification, the
optical signal was ~0.5% (
F/F) and
remained confined to a beam ~250 µm in width in the middle of the
folium. Once the optical signal spread, it increased to 30%
F/F (regions of interest near the center of
Crus IIa). The fluorescence remained elevated at this level over the
next 60 sec, although the stimulus train had ended (Fig.
1D). The long delays in the arrival of the optical
signal in Crus IIb and the rapid but persistent increase in
fluorescence are also evident in the plots of
F/F. Within Crus IIa, the spread of the
optical signal was initiated nearly simultaneously along the parallel
fiber beam (Fig. 1E).
Stimulus frequency and amplitude were important factors in determining
whether spreading acidification was initiated, with more intense
stimulation increasing the likelihood of spreading acidification. As
shown in Figure 2A,
increasing the amplitude of stimulation from 150 to 250 µA increased
the intensity of the optical beam, but spreading acidification was not
evoked until the stimulation amplitude reached 300 µA.
Similarly, increasing the stimulation frequency from 10 to 15 Hz
enhanced the initial optical beam, but spreading was not evoked until
the stimulation frequency was increased to 20 Hz. Increasing the
duration of the stimulus train had a similar effect, with
longer-duration trains more likely to result in spreading acidification
(data not shown). The probability of evoking spread as a function of
stimulation frequency and amplitude is summarized in Figure
2B. The data are based on a subset of 51 animals in
which stimulation frequency or amplitude was adjusted to produce
spreading acidification. In general, greater stimulation intensity
increased the probability of evoking spreading acidification. In these
animals, spreading acidification was invariably evoked with the
stimulation frequencies of 40-50 Hz and amplitudes of 250-300 µA.
However, in some animals, spreading acidification could not be evoked
regardless of the stimulation parameters. Spreading acidification was
observed in 100 of 145 animals (69%), an occurrence rate similar to
that reported previously (Chen et al., 1999a
).

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Figure 2.
Relationship between stimulation parameters and
optical electrophysiological responses. A, Effect of
stimulation amplitude and frequency on the optical response. Top
row, Effect of amplitude. At the same stimulation frequency (10 Hz for 5 sec), when amplitude was changed from 200 to 250 µA, the
evoked optical response was enhanced, and at 300 µA, spread was
evoked. Note that the decrease in fluorescence at the site of the
stimulating electrode is accentuated by increasing stimulation
amplitude. Bottom row, Effect of stimulation frequency.
Layout is similar to the top row, except that
stimulation frequency was varied as indicated. Stimulation amplitude
and duration were constant (250 µA and 2 sec). B,
Relationship between the probability of evoking spreading acidification
and stimulation frequency and amplitude. Data were obtained from 215 experiments in 51 animals in which spread was evoked at some
combination of stimulation parameters. C, Effects of
stimulation intensities on accumulative field potentials. Normalized
accumulative field potentials as a function of stimulation amplitude
(top, at 50 Hz) and stimulation frequency
(bottom, at 100 µA) are shown.
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More intense stimulation evoked a larger total presynaptic and
postsynaptic response over the stimulation period. As shown for the
representative example in Figure 2C, increasing the
stimulation amplitude from 100 to 300 µA, while holding stimulation
frequency constant, led to a progressive increase in both the
presynaptic and postsynaptic components of the summed extracellular
field potential. A similar increase in the summed field potential was observed with increasing stimulus frequency from 10 to 50 Hz while holding amplitude constant (Fig. 2C).
Dependence on presynaptic and postsynaptic activation
A fundamental question is whether spreading acidification occurs
with only the activation of the parallel fibers, i.e., the presynaptic
elements. To block synaptic transmission as completely as possible, the
chamber was filled with nominally
Ca2+-free Ringer's solution (0 Ca2+, 2 mM
Mg2+, and 2 mM EGTA) for 30 min. Surface stimulation in normal Ringer's solution (control)
produced a typical beam of increased fluorescence that subsequently
spread throughout the folium (Fig.
3A,F). After superfusion with nominally Ca2+-free
Ringer's solution, spreading acidification was not evoked either at
the same stimulus parameter (Fig. 3B) or with increasing stimulation frequency (Fig. 3C,D). Electrophysiological
recordings (Fig. 3G) show that N2 of
the field potential was abolished, whereas P1-N1 was unaffected. The
weaker optical beam at the same stimulation parameters after
superfusion with nominally Ca2+-free
Ringer's solution (Fig. 3, compare A and B) is
attributable to the block of synaptic transmission and is consistent
with our previous finding that both presynaptic and postsynaptic
elements contribute to the optical signal (Chen et al., 1998
). After
return to normal Ringer's solution, stimulation at the original
parameters evoked spreading acidification (Fig. 3E).
Although the amplitude and extent of the spreading acidification were
reduced after washout, the temporal profile of optical signal reveals a
similar, rapid increase at spread onset (Fig. 3F).
The partial recovery of the spreading acidification likely reflects the
loss of the dye attributable to repeated washing and the failure to
completely restore the extracellular environment. Similar results were
obtained in four animals in which nominally
Ca2+-free Ringer's solution was used.
Stimulation up to 100 Hz and 400 µA did not evoke spreading
acidification. Therefore, extracellular Ca2+ is a requirement, and activation of
only parallel fibers is insufficient to produce spreading
acidification.

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Figure 3.
Effect of nominally Ca2+-free
Ringer's solution (0 Ca2+, 2 mM
Mg2+, and 2 mM EGTA) on spreading
acidification. A, Sequence of images showing the
spreading acidification evoked by surface stimulation (200 µA, 15 Hz
for 5 sec). B-D, Attempts to evoke spreading
acidification in the presence of nominally Ca2+-free
Ringer's solution. The results of three different stimulation
frequencies are shown. E, After return to normal
Ringer's solution, stimulation at 20 Hz evoked spreading
acidification. F, Change in fluorescence
( F/F) as a function of time for
each series. G, Field potential recordings in normal
Ringer's solution, nominally Ca2+-free Ringer's
solution, and after washout. Arrow, Stimulation onset;
gap in the record, stimulus artifact removed.
H, Effect of TTX on spreading acidification. In normal
Ringer's solution, the spreading acidification is evident but is
abolished by the application of TTX (10 µM).
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Evoking spreading acidification required the activation of neurons and
functioning voltage-gated Na+ channels. An
example is shown in Figure 3H, in which surface stimulation
failed to evoke either an optical beam or spreading acidification
regardless of stimulus parameters after superfusion of Ringer's
solution containing 10 µM TTX. A complete block
of spreading acidification with TTX was observed in four animals. Therefore, spreading acidification is dependent on neuronal activation, and local depolarization of neurons or glia directly around the electrode site is not capable of evoking spreading acidification. This
finding also suggests that the activation of a bundle of parallel
fibers contributes to the generation and the geometry of spreading acidification.
Involvement of glutamate receptors
A series of experiments were performed to evaluate the dependence
of spreading acidification on non-NMDA, NMDA, and mGluRs. When the
competitive AMPA glutamate receptor antagonist CNQX was added to the
Ringer's solution, the threshold for spreading acidification increased. As shown for the example in Figure
4, surface stimulation produced the
characteristic beam and spreading response with a peak
F/F of ~17% (Fig. 4A).
After application of 50 µM CNQX, stimulation at
the same parameters did not evoke spreading acidification. Note that
the amplitude of the initial beam was reduced ~60% but not
completely abolished, also consistent with our previous finding that
both presynaptic and postsynaptic elements contribute to the optical
response (Chen et al., 1998
). Field potential recordings reveal a
complete loss of the postsynaptic negativity, with no effect on the
parallel fiber volley (Fig. 4B). Increasing
stimulation frequency to 30 Hz did not evoke spreading acidification,
whereas stimulation at 40 Hz did (Fig. 4A), although
the amplitude was attenuated. After washout of the CNQX, surface
stimulation at 20 Hz evoked spreading acidification (data not shown).
In three additional animals, CNQX blocked spreading acidification, but increasing the stimulation intensity (current, frequency, or duration) evoked spreading acidification. These findings show that the increase in postsynaptic excitability mediated via AMPA receptors contributes to
spreading acidification.

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Figure 4.
Effect of glutamate antagonists on spreading
acidification. A, Change in fluorescence as a function
of time in normal Ringer's solution and in normal Ringer's solution
containing 50 µM CNQX. The latter includes series of
three stimulation frequencies as indicated. In normal Ringer's
solution, spreading acidification was evoked at 20 Hz; after the
application of CNQX (50 µM), spreading acidification was
evoked at 40 Hz but not 20 or 30 Hz. Stimulation amplitude and duration
were kept constant (300 µA, 20 Hz for 10 sec). B,
Field potential recordings in normal Ringer's solution and after
application of CNQX. C, Similar layout as in
A, but MCPG (1 mM) was applied.
D, Field potential recordings in normal Ringer's
solution and after application of MCPG. E, Similar
layout as in A, but a combination of both AMPA and mGluR
antagonists was used. These GluR blockers included 20 µM
CNQX, 1 mM MCPG, and 1 mM MPPG.
F, Field potential recordings in normal Ringer's
solution and after application of GluR blockers.
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Metabotropic glutamate receptors, particularly the
mGluR1 subtype, are found on Purkinje cells
(Martin et al., 1992
) and produce significant excitatory currents in
response to high stimulus frequencies (Batchelor et al., 1994
; Finch
and Augustine, 1998
; Takechi et al., 1998
). Activation of these
receptors triggers several intracellular signaling cascades including
release of intracellular calcium via inositol-1,4,5-triphosphate (Finch
and Augustine, 1998
). Because evoking spreading acidification was
dependent on stimulation frequency (Fig. 2), the role of metabotropic
glutamate receptors was evaluated by using the mGluR antagonist MCPG.
As shown in Figure 4, C and D, surface
stimulation initially evoked a beam-like optical response that spread.
Thirty minutes after the application of MCPG, surface stimulation using
the same parameters failed to produce spreading acidification. However,
spreading acidification was evoked when the stimulation frequency was
increased to 40 Hz (Fig. 4C), albeit diminished in amplitude
and speed as discussed above. The field potential recordings reveal
identical electrophysiological responses before and after the
application of MCPG (Fig. 4D). As a demonstration of
its efficacy, MCPG reduced the intensity of the initial beam-like optical response evoked by surface stimulation. In experiments in which
the MCPG was washed out, spread was evoked at the original stimulation
parameters. Similar results were obtained in three animals in which
MCPG prevented spreading acidification at the control stimulation
parameters, but increasing the stimulation frequency to 40 or 50 Hz did
evoke spreading acidification. These results indicate that activation
of postsynaptic mGluRs contributes to spreading acidification, similar
to that of AMPA receptor.
In three additional animals, the mGluR antagonist MPPG was also used.
MPPG blocks mGluR4-type receptors that are found
presynaptically on the parallel fibers (Mateos et al., 1998
). MPPG had
no effect on the spread (data not shown).
To determine the effect of blocking ionotropic and metabotropic
glutamate receptors at the parallel fiber-Purkinje cell synapse, AMPA
and mGluR antagonists were applied together to determine whether
blocking both AMPA and metabotropic receptors completely prevented
spreading acidification. As shown in Figure 4E, this combination of glutamate antagonists increased the threshold for spreading acidification. However, increasing the stimulation frequency to 50 Hz evoked spreading acidification. Field potential recordings reveal a complete loss of the postsynaptic negativity, with no effect
on the parallel fiber volley (Fig. 4F). Similar
findings were obtained in four animals. Therefore, additional
mechanisms are likely involved in spreading acidification.
Additionally, NMDA glutamate receptor antagonists AP-3 (100 µM, three animals) and AP-5 (100 µM, three
animals) had no significant effect on spreading acidification, a
finding not unexpected, because the ketamine at the doses used in the
anesthetic would have blocked NMDA receptors (Lang, 2001
). Furthermore,
Purkinje cells in the adult rat cerebellum do not have NMDA receptors
(Farrant and Cull-Candy, 1991
).
Involvement of GABAergic neurotransmission
The parallel fibers synaptically activate several inhibitory
interneurons, including the basket and stellate cells, which in turn
have Purkinje cells as their postsynaptic target (Eccles et al., 1967
).
Also, Purkinje cell axon collaterals inhibit other Purkinje cells. Both
the inhibitory interneurons and Purkinje cells use GABA as their
neurotransmitter (Ito, 1984
). Because AMPA and mGluR antagonists
increased the threshold for evoking spread, it would be expected that
blocking GABAergic transmission would lower the threshold. This
prediction was confirmed in experiments in which both
GABAA and GABAB receptor
antagonists (bicuculline and saclofen, respectively) were added to the
Ringer's solution (Fig. 5). Initially,
stimulation at 20 Hz evoked an optical beam but did not produce spread.
After addition of the GABA blockers, the beam evoked by surface
stimulation at 20 Hz increased in width and intensity and subsequently
spread (Fig. 5A). After the GABA blockers, the presynaptic
component of the field potential recordings was identical, and there
was a small increase in the postsynaptic response (Fig. 5B).
Similar findings were obtained in three animals, in which the GABA
blockers reduced the threshold for spreading acidification.

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Figure 5.
Effects of GABA blockade on spreading
acidification. A, Change in fluorescence as a function
of time in normal Ringer's solution and in normal Ringer's solution
containing GABA blockers. The same stimulation parameters were used for
both conditions (300 µA, 20 Hz for 5 sec). GABA blockers included 100 µM bicuculline and 250 µM saclofen.
B, Field potential recordings in normal Ringer's
solution and after application of GABA blockers.
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Involvement of nitric oxide
How does spreading acidification and depression propagate? One
possible mechanism is that a diffusible substance is released in the
extracellular space. A potential candidate for such an extracellular
messenger is NO, which is generated in the cerebellar cortex after
surface stimulation (Shibuki and Kimura, 1997
; Kimura et al., 1998
).
The target of NO, guanyl cyclase, is primarily localized in cerebellar
Purkinje cells (Ariano et al., 1982
; Boxall and Garthwaite, 1996
). The
involvement of NO was assessed using the NOS inhibitor NLA. After
evoking spreading acidification with surface stimulation at 10 Hz (Fig.
6A), the cerebellar
cortex was superfused with Ringer's solution containing 1 mM NLA. Stimulation at 10 and 20 Hz evoked only a
beam. Spreading acidification, albeit reduced in amplitude and speed,
was only evoked when the stimulation frequency was increased to 30 Hz.
NLA had no effect on the field potential recordings (Fig.
6B), as reported previously (Iadecola et al., 1995
).
Similar results were observed in six animals.

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Figure 6.
Relationship between NO production and spreading
acidification. A, Effect of the NOS inhibitor NLA on
spreading acidification. Change in fluorescence is shown as a function
of time for series in normal Ringer's solution and in normal Ringer's
solution containing 1 mM NLA. The latter includes series of
three stimulation frequencies as indicated. In normal Ringer's
solution, spreading acidification was evoked at 10 Hz; after the
application of NLA, spreading acidification was evoked at 30 Hz
but not 10 or 20 Hz. Stimulation amplitude and duration (200 µA,
10 Hz for 5 sec) were kept constant. B, Field potential
recordings in normal Ringer's solution and after application of NLA.
C, Effect of the NO donor SNAP on spreading
acidification. Change in fluorescence is shown as a function of time
for series in normal Ringer's solution and in normal Ringer's
solution containing 2 mM SNAP. Surface stimulation (300 µA, 20 Hz for 10 sec) produced a strong beam-like optical response
but not spreading acidification. After the application of SNAP,
spreading acidification was evoked. D, Field potential
recordings in normal Ringer's solution and after application of
SNAP.
|
|
To further examine the contribution of NO to spreading acidification,
the effect of the NO donor SNAP was determined. As described above,
spreading was evoked in 69% of the animals. SNAP was added to the
Ringer's solution in experiments in which spreading acidification could not be evoked regardless of the stimulation intensity. An example
is shown in Figure 6C, in which intense surface stimulation produced a strong, wide, beam-like optical response that failed to
spread. After superfusion with 2 mM
SNAP, the same stimulus parameters evoked an optical beam that
propagated throughout the folium. Similar results were observed in four
animals. The field potential recordings were not altered by the
application of SNAP (Fig. 6D). These results
demonstrate that NO is a modulator of spreading acidification.
Antagonists of AMPA and mGlu receptors and NOS blockers all increased
the threshold for evoking spreading acidification but individually did
not completely prevent spread (Figs. 4-6). Therefore, we evaluated
whether blocking glutamate transmission and NOS in combination could
eliminate spread. As shown in Figure 7,
the combination of CNQX (20 µM), MCPG (2 mM),
and NLA (1 mM) completely blocked spreading acidification
regardless of the stimulation parameters (Fig. 7A). With the
presence of these blockers, spread could not be evoked with stimulation
frequencies as high as 75 Hz, but spread was evoked again at 40 Hz
after the washout of the blockers. As expected, these blockers result
in a complete loss of the postsynaptic negativity with no effect on the
parallel fiber volley (Fig. 7B). Similar results were found
in three animals.

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Figure 7.
Effect of AMPA antagonists, mGluR antagonists, and
NOS inhibitor on spreading acidification. A, Change in
fluorescence as a function of time for series obtained in normal
Ringer's solution, in normal Ringer's solution containing the
blockers (20 µM CNQX, 2 mM MCPG, and 1 mM NLA), and after washout of the blockers. In normal
Ringer's solution, spreading acidification was evoked at 40 Hz; after
the application of the blockers, spreading acidification was not evoked
even at higher frequencies (50 and 75 Hz) but was again evoked at 40 Hz
after washout of the blockers. Stimulation amplitude and duration were
kept constant (200 µA, 200 msec, 20 Hz for 5 sec). B,
Field potential recordings in normal Ringer's solution and after
application of the blockers.
|
|
Last, we investigated whether spreading acidification could be evoked
in transgenic mice with a targeted mutation
(B6;129S-Nos1tm1plh) disrupting the neuronal nitric
oxide synthase gene (Huang et al., 1993
). In wild-type mice, surface
stimulation evoked spreading acidification identical to that in rats
(data not shown). In the NOS-deficient mouse, spreading acidification
was evoked by surface stimulation in normal Ringer's solution (Fig.
8A,C). The intensity and propagation speed (559 ± 87 µm/sec) were similar to the
spreading acidification evoked in wild type animals. Spread was evoked
in the four NOS-deficient mice evaluated. In the NOS-deficient mice, we
also evaluated the effect of NLA in an additional four experiments. After application of 1 mM NLA, surface
stimulation evoked spreading acidification; albeit the initiation was
delayed, and the slope of spread decreased (Fig.
8B,C). When taken together with the results using the
NOS inhibitor and NO donor, the data suggest that NO modulates
spreading acidification. Furthermore, because NLA is a general NOS
inhibitor, non-neuronal NOS isoforms (Dawson et al., 1998
) may play a
role in spreading acidification.

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Figure 8.
Spreading acidification evoked in neuronal
NOS-deficient mice. A, Sequence of images showing
beam-like optical response to surface stimulation (100 µA, 10 Hz for
10 sec) in normal Ringer's solution. B, Sequence of
images showing spread evoked in the presence of NLA (1 mM).
C, Change in fluorescence as a function of time for each
series in A and B.
|
|
Spreading acidification was accompanied by a transient decrease in the
excitability of the parallel fibers and their postsynaptic targets
(Chen et al., 1999a
). In that initial report, we described complete
suppression of both the parallel fiber volley and the postsynaptic
component. Additional experiments have revealed that the depression in
excitability need not be complete, as shown in Figure
9. In this example, as the increased
fluorescence spread across the folia, there was a transient reduction
in the parallel fiber volley
(P1-N1) and a complete
suppression of the postsynaptic component (N2;
Fig. 9A). The parallel fiber volley was reduced to ~50%
of the control during the initial phase of spreading acidification and
the reduction lasted ~20 sec (Fig. 9B). The postsynaptic
component (N2) was completely suppressed for
~50 sec and recovered to 95% of baseline at 105 sec. The suppression
in the postsynaptic response mirrored the increase in fluorescence.
However, P1-N1 completely recovered to normal before the optical signal reached its peak, and
N2 almost completely recovered when the optical
signal had returned to 50% of its peak. In four animals, the maximal
depression of P1-N1
averaged 70%, lasted 5 sec, and recovered in 25 sec. Similarly for
N2, the maximal depression averaged 100%, lasted 64 sec, and recovered in 112 sec. This coupling between spreading acidification and decreased excitability was also observed in the
presence of CNQX (Fig. 9C; only
P1-N1 depression recorded), MCPG (Fig. 9D), and NLA (Fig. 9E). The duration
of depression was longer in the latter two experiments, reflecting the
longer spreading acidification manifested by the longer time course of optical responses.

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Figure 9.
Relationship between the optical response and
neuronal excitability. In this experiment, the optical response evoked
by the first stimulation electrode and field potentials evoked by the
second stimulation electrode were simultaneously recorded, as detailed
in Materials and Methods. A, Field potentials at
selected times (top right corner, in seconds) during
spreading acidification. B, Normalized optical signal
( F/F) in a 10 × 10 pixel
region centered at the tip of the recording electrode and
P1-N1 (parallel fiber volley) and
N2 (postsynaptic response) as a function of time. The times
of field potentials in A are indicated on the plot of
the optical signal. C-E, same layout as in
B, but the responses were obtained in the presence of
CNQX (20 µM), MCPG (1 mM), and NLA (1 mM), respectively. Note that there is no N2
component in C, because the postsynaptic response is
completely blocked by CNQX.
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Role of ATP, purinergic receptors, and furosemide
It has been shown that ATP acts as the extracellular messenger for
Ca2+ waves in mouse cortical astrocyte
cultures (Guthrie et al., 1999
). Because ATP neurotransmission occurs
in the cerebellar cortex, and purinergic receptors are abundant on
Purkinje cells (Mateo et al., 1998
), the possible involvement of ATP in
spreading acidification was of interest. We evaluated the role of
purinergic neurotransmission by blocking P2X purinergic receptors with
the antagonist PPADS. As shown in Figure
10A, superfusion with
1 mM PPADS did not affect the spreading
acidification evoked by surface stimulation. In four additional
animals, PPADS failed to block or alter the threshold to evoke
spreading acidification. A similar result was obtained with suramin, a
general antagonist of P2X and P2Y receptors (data not shown). We also
evaluated the effectiveness of these antagonists by microinjecting
adenosine into the molecular layer, which evoked a strong increase in
epifluorescence. This increase was blocked by the purinergic
antagonists (data not shown). These results suggest that purinergic
neurotransmission does not play an essential role, and ATP does not act
as an extracellular messenger in the propagation of spreading
acidification.

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Figure 10.
Effect of PPADS and furosemide on spreading
acidification. A, Change in fluorescence as a function
of time for series in normal Ringer's solution and in normal Ringer's
solution containing 1 mM PPADS. Surface stimulation: 200 µA, 20 Hz for 2 sec. B, After topical application of 1 mM furosemide for 45 min, spreading acidification could
still be evoked by surface stimulation (300 µA, 30 Hz for 10 sec).
|
|
Neuronal activity results in a reduction in the extracellular space and
an increase in neuronal and glial volume. This cellular swelling
subsequently leads to the increase of light transmittance through
tissue (Ransom et al., 1985
; Holthoff and Witte, 1996
). We have
demonstrated previously that neutral red-based epifluorescence signals
are primarily modulated by pH changes and that extracellular space
changes do not produce this optical signal (Chen et al., 1998
). Still,
it was important to determine whether volume changes were the source of
the optical signals observed during spreading acidification. Therefore,
furosemide, an anion transport inhibitor known to block the
extracellular space and cellular volume changes, was used (Ransom et
al., 1985
; Holthoff and Witte, 1996
; Muller and Somjen, 1999
). After
the application of furosemide (2 mM) for 45-60 min,
surface stimulation still evoked a spreading acidification (Fig.
10B). We did observe that furosemide (1-2
mM) was toxic to the cerebellar cortex,
depressing the field potentials (data not shown) and eliminating all
potentials at higher doses. Similar results were obtained in six
different animals.
 |
DISCUSSION |
Optical imaging has been used to monitor SD, calcium waves, and
related phenomena (Yoon et al., 1996
; Newman and Zahs, 1997
; Guthrie et
al., 1999
; Muller and Somjen, 1999
). The optical signals in this study
were derived from neutral red, a widely used indicator of intracellular
pH (Kogure et al., 1980
; LaManna, 1987
). Although one cannot exclude
contributions from other sources to the optical signals, these are
probably limited. As discussed previously (Chen et al., 1999a
),
membrane-associated effects, changes in ion concentrations, and voltage
sensitivity are not likely to contribute (Cohen et al., 1974
; LaManna,
1987
). In the cerebellum, the increase in fluorescence primarily
reflects neuronal intracellular acidification (Chen et al., 1998
). Our
initial report showed that volume changes alone did not produce these
epifluorescent optical signals (Chen et al., 1998
). When coupled
with the present results using furosemide, this suggests that cellular
swelling associated with neuronal activity is not the source of the
optical signals observed during spreading acidification. However, the
electrophysiological and pharmacological results reveal a complex set
of events underlying spreading acidification and depression.
Differences with classic spreading depression
Our original study documented several differences between
spreading acidification and depression and classic SD (Chen et al., 1999a
). The present study revealed three additional differences. First,
activation of NMDA glutamate receptors are critical for evoking SD in
the cerebral cortex, whereas non-NMDA receptors are not (Gorelova et
al., 1987
; Lauritzen and Hansen, 1992
). The converse was found for
spreading acidification in the cerebellum. Blocking NMDA receptors had
no effect, whereas blocking AMPA receptors with CNQX raised the
threshold for spreading acidification. Second, the accompanying
depression of neuronal activity need not be complete and can be brief,
lasting 1-2 min. In SD, the depression is more prolonged and complete
(Kraig and Nicholson, 1978
; Lauritzen and Nicholson, 1988
). Third, some
variants of SD can be evoked in 0 Ca2+
(Basarsky et al., 1998
; Bahar et al., 2000
), and spreading
acidification cannot. Therefore, spreading acidification and SD differ
both phenomenologically and mechanistically.
Presynaptic and postsynaptic contributions
Activation of parallel fibers alone did not evoke spreading
acidification, as demonstrated by the nominally
Ca2+-free experiments. This finding
suggests that spreading acidification is dependent on activation of the
postsynaptic targets of the parallel fibers: Purkinje cells and
interneurons. Consistent with this observation is that blocking AMPA
receptors, mGluRs, or both raised the threshold for evoking spreading
acidification. The latter class of receptors not only increases
intracellular Ca2+ but also produces
significant excitatory postsynaptic currents when activated at high
frequencies (Finch and Augustine, 1998
; Takechi et al., 1998
). Also,
NOS blockers raised the threshold for spreading acidification, and the
primary target of NO is the guanyl cyclase in Purkinje cells (Ariano et
al., 1982
; Boxall and Garthwaite, 1996
). Blocking
GABAA and GABAB receptors
lowered the threshold for spreading acidification, and the primary
target of these inhibitory networks is the Purkinje cell. Therefore, spreading acidification is dependent on the activation of postsynaptic structures, including Purkinje cells.
However, the presynaptic elements contribute to spreading
acidification. First, blocking conduction along the parallel fibers with TTX prevented spread. Second, the geometry of the activated parallel fibers and cerebellar cortical circuitry defines the spatial
structure of spreading acidification. As shown in Figure 1, spreading
acidification is initiated nearly simultaneously along the parallel
fiber beam evoked by surface stimulation (Chen et al., 1999a
).
Therefore, initiation of spreading acidification is not limited to the
site of stimulation but occurs along the entire length of the activated
parallel fibers.
In addition to its postsynaptic actions, high-frequency
stimulation of parallel fibers evokes presynaptic mechanisms that could
contribute to spreading acidification. NO release from parallel fibers
has a marked frequency dependence, and high-frequency stimulation potentiates the release of NO (Shibuki and Kimura, 1997
; Kimura et al.,
1998
). High-frequency stimulation of parallel fibers also results in
long-term potentiation of glutamate release (Salin et al., 1996
). These
effects are consistent with the observation that high-frequency
stimulation was effective in evoking spreading acidification and argue
for an important role for the parallel fibers.
Therefore, spreading acidification in the cerebellar cortex is a
multifactorial process involving glutamate neurotransmission and
modulated by NO. Blocking or interfering with these elements in
isolation did not prevent spreading acidification but only increased
the threshold. However, AMPA and mGluR antagonists and NOS inhibitors
in combination completely blocked spreading acidification. It remains
to be determined whether these factors converge on a common element or
signaling pathway. The removal of extracellular Ca2+ prevented spread. However, the role
of Ca2+ is difficult to pinpoint, because
increased intracellular Ca2+ is involved
in a multitude of signal pathways and cellular processes.
The increased acidification may be attributable to several factors,
including (1) increased intracellular Ca2+
and the associated release of H+ from
internal storage sites (Paalasmaa et al., 1994
), (2)
glutamate-mediated H+ influx (Chen and
Chesler, 1992
), (3) GABA channel-mediated
HCO
efflux (Kaila et al., 1990
), and (4)
metabolic production of CO2 and lactic acid
(Siesjo and Wieloch, 1985
). The first two possibilities are consistent
with the combined effects of nominally Ca2+-free Ringer's solution and glutamate
receptor antagonists. Although the optical signal is argued to reflect
intracellular pH changes, this does not imply that changes in
extracellular pH are not occurring. The well documented coupling
between intracellular and extracellular pH (Chesler, 1990
) would
predict that extracellular shifts in pH accompany spreading acidification.
Depression of the cerebellar cortical excitability was found to
accompany spreading depression in the presence of AMPA and mGluR
antagonists and NOS inhibitors. Therefore, the depression and
acidification are highly coupled. The acidification could also
contribute to the depression, because a decrease in pH depresses voltage-gated sodium channel conductance (Tombaugh and Somjen, 1996
)
and attenuates glutamate receptor channel conductance (Traynelis and
Gull-Candy, 1991
). Other potential factors are an increase in
intracellular Ca2+ and NO production.
Increases in intracellular Ca2+ can induce
several cascades that lead to depression of AMPA receptors (for review,
see Linden, 1994
). NO elevates the endogenous level of cGMP, inhibiting
presynaptic Ca2+ currents and
neurotransmitter release (Boulton et al., 1994
). Therefore, several
mechanisms could underlie the presynaptic and postsynaptic depression.
Postulated mechanism of propagation and significance
A major question is how spreading acidification propagates
from cell to cell at these relatively high speeds. Calcium waves and SD
in the retina (Martins-Ferreira et al., 2000
) as well as SD in the
cerebral cortex (Aitken et al., 1998
) propagate via glial gap
junctions. An extracellular messenger, ATP, has been implicated in the
spread of calcium waves in cultures of cortical astrocytes (Guthrie et
al., 1999
). These events are rather slow and rely on passive diffusion,
although Ca2+ waves that precede classic
spreading depression propagate at >100 µm/sec (Kunkler and Kraig,
1998
). Furthermore, both calcium waves (Newman and Zahs, 1997
; Guthrie
et al., 1999
) and SD, including SD in the cerebellar cortex, propagate
radially from the site of initiation (Chen et al., 1999a
). In contrast
to SD, spreading acidification propagates at relatively high speed and
spreads orthogonally to the activated parallel fibers. Therefore, we
postulate that spreading acidification involves a regenerative, i.e.,
nonpassive, process that uses the underlying parasagittal aspects of
cerebellar architecture such as the basket cell axons (Eccles et al.,
1967
; Ito, 1984
).
Of interest is whether spreading acidification in the cerebellar cortex
involves an extracellular and intercellular messenger. One candidate
evaluated, ATP, is highly unlikely, because the threshold for spreading
acidification is not increased by purinergic receptor blockers. The
second candidate evaluated, NO, is produced by activation of parallel
fibers (Shibuki and Kimura, 1997
; Kimura et al., 1998
) and has as a
target guanyl cyclase in Purkinje cells and in the parallel fibers
themselves (Ariano et al., 1982
). Blocking NO production raises the
threshold for spreading acidification and completely blocks spread in
the presence of AMPA and mGluR antagonists. Conversely, an NO donor
facilitates spread. However, NO is clearly not the only mechanism,
because spreading acidification was evoked in the neuronal
NOS-deficient mouse. An important caveat is that other sources of NO,
including non-neuronal isoforms of NOS, may still be operative (Dawson
et al., 1998
). Given this caveat, the role of NO may be its effect on
neuronal excitability and not as an intercellular agent.
An important avenue for future investigations is to determine
whether glia-glia or neuronal-glia interactions, or both, contribute to
spreading acidification. In the cerebellar cortex, glial gap junctions
are abundant and strongly coupled, and for Bergmann glia, the coupling
is perpendicular to the parallel fibers (Lee et al., 1994
; Muller et
al., 1996
). Repetitive parallel fiber stimulation increases
intracellular calcium in Bergmann glia (Grosche et al., 1999
; Kulik et
al., 1999
) that triggers the release of glutamate, which in turn
modulates the excitability of neighboring neurons (Parpura et al.,
1994
; Bezzi et al., 1998
; Rouach et al., 2000
) and further increases
intracellular calcium via both activation of ionotropic glutamate
receptors and the inositol-1,4,5-triphosphate pathway (Kirischuk et
al., 1999
). Therefore, a positive feedback loop exists that could
contribute to the propagation of spreading acidification.
The significance of spreading acidification and depression remains
undefined. Our working hypothesis is that this represents a
pathophysiological phenomenon that could acutely disrupt cerebellar function. An intriguing speculation is that spreading acidification is
involved in the episodic ataxias, channelopathies in which the clinical
complex includes an acute, transient cerebellar dysfunction (Browne et
al., 1994
; Ophoff et al., 1996
).
 |
FOOTNOTES |
Received May 23, 2001; revised Sept. 20, 2001; accepted Oct. 1, 2001.
This work was supported by National Institutes of Health Grant
P01-NS31318. We thank Yanhua Pan for animal preparation, Mike L. McPhee
for expert graphics, and Brigitte Welter and Linda King for help in
preparing this manuscript.
Correspondence should be addressed to Dr. Timothy J. Ebner, Department
of Neuroscience, University of Minnesota, Lions Research Building, 2001 Sixth Street Southeast, 421, Minneapolis, MN 55455. E-mail:
ebner001{at}umn.edu.
 |
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