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The Journal of Neuroscience, August 1, 2001, 21(15):5574-5586
Subunit Interactions and AMPA Receptor Desensitization
Antoine
Robert1,
Stacey
N.
Irizarry1,
Thomas E.
Hughes2, and
James R.
Howe1
Departments of 1 Pharmacology and
2 Ophthalmology, Yale University School of Medicine, New
Haven, Connecticut 06520-8066
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ABSTRACT |
Most AMPA-type glutamate receptors (GluRs) exhibit rapid and
virtually complete desensitization when activated by glutamate, and at
some central synapses it is largely desensitization that determines the
decay of EPSCs. However, the mechanisms underlying the
conformation change that results in desensitization are not fully
understood. AMPA receptor subunits that contain a single amino acid
substitution have been shown to form homomeric channels that show
markedly reduced desensitization. We show here that the coexpression of
wild-type GluR1 with one such mutant, GluR1(L497Y), results in
heteromeric channels that show desensitization behavior that is
intermediate between wild-type and mutant homomers. The relative
amplitudes of the multiple exponential components present in the decay
of glutamate-evoked currents depended on the relative abundance of
wild-type and mutant subunits and were described by the combinatorial
distribution of the two types of subunits into tetrameric, but not
pentameric, assemblies. Our results are consistent with recent
structural data suggesting that AMPA receptors are tetrameric
assemblies composed of two dimers.
Key words:
glutamate; AMPA receptor; desensitization; subunit
interactions; allosteric; kinetics
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INTRODUCTION |
AMPA-type glutamate receptors
(GluRs) rapidly desensitize on exposure to glutamate, and the kinetics
of desensitization can determine the time course of synaptic events
(Jonas and Spruston, 1994 ; Jones and Westbrook, 1996 ; Otis et al.,
1996 ). Multiple regions within single AMPA receptor subunits have been
shown to influence the rate, extent, and pharmacological modulation of desensitization. Alternative splicing of the so-called flip/flop cassette has marked effects on the kinetics of desensitization (Sommer
et al., 1990 ; Mosbacher et al., 1994 ), as well as on allosteric modulation by cyclothiazide and aniracetam (Partin et al., 1993 , 1994 ,
1996 ). The flip and flop sequences are found in all AMPA receptor
subunits and are located within the extracellular loop just before the
third transmembrane segment. RNA editing at a site just upstream of the
flip/flop cassette affects recovery from desensitization (Lomeli et
al., 1994 ). Amino acids that affect desensitization are also located
within the proximal portion of the extracellular loop (the S2 domain)
(Mano et al., 1996 ). Finally, Stern-Bach et al. (1998) identified amino
acids in the S1 domain that when mutated reduce the rate and extent of
desensitization. Specifically, these latter authors showed that a
single leucine-to-tyrosine substitution (L507Y for GluR3 or L497Y for
GluR1) created subunits that form homomeric channels that do not appear
to desensitize.
Although the above studies have identified domains within individual
subunits that influence desensitization, the extent to which
subunit-subunit interactions play a role is less clear. Allosteric
models similar to those advanced to explain the behavior of tetrameric
hemoglobin (Monod et al., 1965 ) have been suggested to apply to AMPA
receptor desensitization (Partin et al., 1996 ). Such models imply,
among other things, that desensitization requires a concerted
conformational change involving all the subunits of the oligomeric
receptor and also that agonists bind with higher affinity to the
desensitized state of the receptor. Glutamate does appear to bind
preferentially to the desensitized form of the receptor (Trussell and
Fischbach, 1989 ; Patneau and Mayer, 1991 ; Colquhoun et al., 1992 ; Raman
and Trussell, 1992 ), and evidence for a concerted conformational change
comes from results showing that heteromeric assemblies of subunits with
different desensitization properties display phenotypes
indistinguishable from one of the "parent" subunits (Mosbacher et
al., 1994 ; Partin et al., 1994 ). Recently, however, the unitary
conductance of AMPA-type channels has been shown to depend on the
number of ligand molecules bound to the receptor (Rosenmund et al.,
1998 ; Smith and Howe, 2000 ). Because each subunit contains a single
agonist binding site, one interpretation of these results is that
individual subunits can gate independently.
We show here that the coexpression of wild-type
GluR1flip with the non-desensitizing
GluR1flip (L497Y) mutant results in what appears
to be intermediate desensitization behavior. The relative amplitudes of
the multiple components present in the decay of glutamate-evoked
currents depended on the relative abundance of wild-type and mutant
subunits. The results provide novel evidence that AMPA-type channels
are tetrameric assemblies, and our findings are consistent with recent
evidence suggesting that these assemblies are composed of two dimers.
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MATERIALS AND METHODS |
Cell culture. Human embryonic kidney (HEK) 293 cells
were plated onto 12 mm glass coverslips that had been coated with
poly-L-lysine (100 µg/ml) and were maintained
in humidified 95% O2/5%
CO2. The culture medium was modified Eagle's
medium (MEM; Life Technologies) containing 10% fetal bovine serum. HEK
293 cells were transiently transfected using Lipofectamine 2000 (Life
Technologies) with 0.2-0.6 µg of total cDNA per coverslip. The
solution used for transfection consisted of 100 µl of Opti-MEM medium
(Life Technologies), 3 µl of Lipofectamine 2000, 0.5 µg of a
reporter cDNA encoding the green fluorescent protein (GFP) in
pCMVsport, 0.1-1 µg of GluR1flip or
GluR1flip (L497Y), or both, in a
CMV-driven mammalian expression vector. The GluR1 plasmids were kindly
provided by Derek Bowie (Emory University, Atlanta, GA), who
introduced the L497Y mutation. The GluR1flip
construct (original cDNA from Peter Seeburg, MPI Medical Research,
Heidelberg, Germany) was modified previously by Mark Mayer and
Kathy Partin (National Institute of Child Health and Human Development,
National Institutes of Health, Bethesda, MD) to enhance
expression in mammalian cells. The transfection solution was first
incubated at room temperature for 15 min, and 25 µl of this solution
was added to each culture well. Electrophysiological recordings were
performed 24 hr after transfection.
Cerebellar culture. The cerebella of Sprague Dawley rat pups
(age 5-7 d) were removed and minced with a razor blade. Cells were
dissociated into the culture medium with a fire-polished Pasteur
pipette in the absence of enzymes. The resulting solution was then
filtered through a nylon mesh, and the cells were plated onto
acid-washed coverslips coated with poly-L-lysine
(400 µg/ml for 1 hr). The culture medium was DMEM containing 25 mM KCl and 10% fetal bovine serum. The
transfection technique was as described above. To minimize
glutamate-mediated toxicity,
1,2,3,4-tetrahydro-6-nitro-2,3-dioxo-benzo[f]quinoxaline-7-sulfonamide (NBQX; RBI/Sigma) was added at 1 µM to the
transfected cultures.
Electrophysiology. Whole-cell patch-clamp recordings and
recordings from excised outside-out patches were made with an EPC9 amplifier (HEKA). The cells were constantly superfused with normal external solution at a rate of 1 ml/min. Transfected cells were identified by epifluorescence imaging of GFP (Marshall et al., 1995 ).
Patch electrodes were pulled from thin-walled borosilicate glass with
inner filament (Warner) to an open resistance of 1-3 M . The series
resistance after going whole cell was 3-6 M . Given the size of the
peak currents in patches, the voltage errors were 5 mV at the holding
potential of 90 mV used for all recordings. We found that series
resistance compensation (60-80%) had no effect on the amplitude or
kinetics of the glutamate-evoked currents, but did often introduce
high-frequency noise; therefore it was not used in most recordings.
Most currents were analog low-pass filtered at 2.9 kHz (four-pole
Bessel-type, 3 dB) and written directly to the hard-drive of the
computer at a sampling rate of 30 kHz. For measurements of
deactivation, the half-power frequency of the low-pass filter was set
at 5 kHz, and the data were sampled at 100 kHz. All recordings were
performed at room temperature (20-22°C).
The external medium was (in mM): 150 NaCl, 3 KCl, 2 CaCl2, 1 MgCl2, 5 glucose,
and 10 HEPES (pH adjusted to 7.4 with NaOH). Pipettes were filled with
a solution containing (in mM): 120 CsF, 33 KOH, 2 MgCl2, 1 CaCl2, 0.1 spermine, 10 HEPES, and 11 EGTA (pH adjusted to 7.4 with CsOH).
Glutamate was added to the external solution. Cyclothiazide was
prepared in DMSO and diluted in external solution to a final
concentration of 100 µM (final DMSO concentration 0.5%).
All chemicals were purchased from Sigma (St. Louis, MO).
Fast perfusion. In most experiments, glutamate was applied
with a rapid perfusion system made from a pulled theta capillary. The
tip of the theta glass was cleanly broken with a diamond cutter to a
tip diameter of ~300 µm, and its septum was snapped back at the tip
with a sharp needle so that the flow of solution leaving the tip from
either side of the theta capillary overlapped. Four capillaries (outer
diameter 450 µm; Polymicro Technologies) were introduced into each
barrel at the back of the theta glass and secured with Sylgard (Dow
Corning). Each capillary was connected to plastic tubing that branched
to a solenoid valve (The Lee Company). The valves were opened and
closed by a analog-to-digital (A/D) interface (TIB 14, HEKA)
that was controlled by the acquisition software of the EPC9. The speed
of the solution exchanges obtained with this system was estimated with
an open patch pipette by measuring the current deflections induced by a
change in the NaCl concentration. The mean 10-90% rise times of the
open-tip responses were 275 ± 25 µsec (n = 5).
The valve-controlled system described above produced rapid solution
exchanges, but it did not allow us to make applications briefer than
~50 msec. For measurements of deactivation time constants, and for
experiments to determine the effect of cyclothiazide on peak currents,
glutamate was applied to excised patches using a theta glass pipette
mounted on a piezoelectric bimorph. The theta glass pipettes were
pulled and broken to a tip diameter of ~300 µm. The width of the
septum separating the two barrels was reduced by etching with
hydrofluoric acid to increase the sharpness of the interface created
between solutions flowing out of each barrel. Patches were positioned
near the solution interface, and the interface was moved by applying
voltage across the bimorph with a constant voltage source (Winston
Electronics Co.) that was triggered with one of the A/D outputs
on the EPC9. The voltage pulses were resistance-capacitive filtered to
minimize mechanical oscillations of the piezoelectric device. The
10-90% rise times of the open-tip responses obtained with this system
were 100-200 µsec, and glutamate applications as brief as 1 msec
could be delivered reproducibly.
Data analysis. The digitized records were transferred to
IGOR software (Wavemetrics). The decays of glutamate-evoked currents were fitted with functions consisting of the mixture of multiple exponential components and a steady-state plateau current. Usually 5-10 responses were averaged, and the fits were performed on the averaged currents. The segment of the decay to be fitted was defined by
placing cursors on the data trace, where the first cursor was placed
near the peak of the current and the other cursor ~700 msec after the
peak. Fits were performed by sequentially including from one to four
exponential components. At each stage, the quality of the fit was
evaluated by visual inspection of the residual current (obtained by
subtracting the fit from the data). If the residual current was not
flat, an additional exponential component was added. Two exponential
components and a plateau current gave adequate fits in a few cases, and
functions containing three exponentials were sufficient to obtain a
flat residual current in all cases. Not only did the inclusion of a
fourth component not improve the fits as assessed by visual inspection
of the residual currents, but repeated four-component fits of the same
data gave parameter values that were not reproducible. In most cases,
the amplitude of one component converged to a value near zero, two of
the time constants converged to very similar values, or one of the time constants converged to a value that was very brief or very long. Inclusion of a fourth component typically reduced the sum of squared deviations by <1% and rarely improved the goodness of fit
significantly as assessed by a standard test for comparison of nested
models (Horn, 1987 ). In contrast, repeated three-exponential fits of the same decays gave reproducible time constants and relative amplitudes, and the parameter values obtained were largely insensitive to the initial guesses. With the exception of some of the results obtained at mutant/wild-type ratios of 1:6 and 3:1, the
three-exponential fits were significantly better than those obtained
with two-exponential components.
The recovery from desensitization was estimated with two-pulse
protocols in which a constant 100 msec application of 500 µM glutamate was followed by test pulses applied at
variable intervals. Each two-pulse protocol was separated by a 5 sec
interval to allow complete recovery from desensitization. The decays of
the currents evoked by the test pulses were fitted as described above,
and the amplitudes of the fast and intermediate exponential components were plotted as a function of recovery time. Each set of data was
fitted with a single exponential function:
It/I = 1 exp((t offset)/ rec), where
It is the amplitude of the current for a given
test pulse, I is the amplitude of
the corresponding component for the current evoked by the constant
prepulse application, t is the interpulse
interval, and rec is the time
constant of the exponential recovery. The single exponential fits to
the recovery data did not extrapolate back to zero time. Thus the
additional variable, offset, was included in the fits and
subtracted from all recovery times. This offset may reflect slight
delays in the complete removal of glutamate after switching back to
control solution at the end of the prepulse application. To minimize
this offset, we used 500 µM glutamate for the
recovery experiments instead of the higher concentration (5 mM) used in most experiments.
Fluctuation analysis of steady-state currents evoked by a range of
glutamate concentrations was used to estimate the unitary conductance
and open probability of GluR1flip (L497Y)
homomeric channels. These results were compared with the corresponding
results obtained for wild-type GluR1flip channels
in the presence of 100 µM cyclothiazide (to slow
desensitization). Values for the current variance were obtained from
spectral density analysis of steady-state currents evoked at different
glutamate concentrations, and these values were plotted against the
corresponding mean currents to give estimates of
Popen and the apparent unitary
conductance ( noise). For these experiments,
the data were sampled at 9.4 kHz and low-pass filtered at 2 kHz. Power
spectra were obtained and fitted with bi-Lorentzian functions as
described previously (Howe, 1996 ).
It was assumed that the assembly of wild-type and mutant subunits was
random and combinatorial. The probabilities for each possible
stoichiometric combination of wild-type and mutant subunits were
calculated from the binomial relationship:
Pj = (N!/(j!(N j)!))(pmut)j(1 pmut)N j,
where Pj is the probability that a channel
composed of N subunits will contain j mutant
subunits, and pmut is the amount of
GluR1flip (L497Y) cDNA as a proportion of the
total GluR-encoding cDNA (wild type plus mutant) used for the
transfection. For each wild-type/mutant cDNA ratio studied, the results
were compared with the stoichiometric predictions for channels
containing N = 4 and N = 5 subunits
(tetramers and pentamers, respectively). Similar calculations were
done, assuming that the channels assembled first as dimers, to obtain the probabilities that a channel contained at least one dimer in which
both subunits were the L497Y mutant.
Simulated glutamate-evoked currents were generated using QUB software
(Qin et al., 1996 , 1997 ). The kinetics of the simulated currents were
analyzed as described above in IGOR. The rate constants and parameter
values used for the simulations are given in Results or in the legends
to the appropriate figures. The experimental results in Figures
5C, 6A, and 7B are shown as
mean ± SD; all other results are given as mean ± SEM.
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RESULTS |
Desensitization of GluR1flip and GluR1flip
(L497Y) homomeric channels
The transient transfection of HEK 293 cells with the cDNAs
encoding the GluR1flip and the
GluR1flip (L497Y) subunits resulted in high-level
expression of each type of homomeric channel. This facilitated our
studies of desensitization kinetics because we were able to measure
large ensemble currents in outside-out patches from transfected cells.
Although the superfusion systems used produced solution exchanges of
<300 µsec, the rise times of whole-cell currents were much slower
(2-5 msec), presumably because of diffusion barriers. Therefore,
although qualitatively similar data were obtained from whole-cell
recordings, all quantitative analysis reported here was limited to
results obtained in outside-out patches in which the rise times of the
currents were <500 µsec.
Typical currents evoked by 5 mM glutamate in outside-out
patches are shown in Figure 1. Currents
through wild-type GluR1flip homomers showed rapid
and virtually complete desensitization. Although the decay of the
currents proceeded largely monophasically, we found that these decays
were consistently better fitted by two, rather than one, exponential
component. Figure 1Aa shows the current evoked by the
sustained application of 5 mM glutamate in a
patch from a GluR1flip-transfected cell. The
two-exponential fit is superposed on the data, and the corresponding
residual current is also shown. An expanded view of the same current
with the best single exponential fit superposed is shown in Figure 1Ab. As was the case in all patches studied, single
exponential fits failed to describe well the tail of the
glutamate-evoked currents and also gave significant residual current
near the peak response. The source of the small slower component is
uncertain, but we believe it arose because a few of the receptors in
the patches had restricted access to the agonist because of physical barriers to diffusion. To limit the effect of this small tail on the
time constants measured for the major component of decay, the slow
component was routinely included in the fitting. On average, the
currents through GluR1flip homomers decayed with
a large fast component ( f = 2.24 ± 0.12 msec; 98-99.5% of the total current amplitude; n = 8 patches) and a much smaller component with a time constant that varied
between 9 and 22 msec. The sustained component of the currents was very
small, averaging only 0.23 ± 0.09% of the total peak amplitude
(n = 8).

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Figure 1.
Desensitization kinetics of wild-type
GluR1flip and GluR1flip (L497Y).
Aa, Current elicited by the rapid and sustained
application of 5 mM glutamate (bar) in an
outside-out patch from a HEK 293 cell transfected with wild-type
GluR1flip. The bi-exponential fit (smooth solid
line) to the decay of the current, as well as the residual
trace (res; obtained by subtracting the recording from
the fit), are shown. The fit gave time constants of 2.25 and 14 msec
for the two components. The amplitude of the fast component was 99% of
the total peak current. Ab, Enlargement of the same
current fitted with a single exponential. Note that the fit is poor in
the tail of the current, as well as the presence of substantial
residual current near the peak. Ba, Response to 5 mM glutamate in a patch from a cell expressing
GluR1flip (L497Y). The single-exponential fit to the decay
and the corresponding residual current are shown. Bb,
The rises of the currents in A
(GluR1flip) and B
[GluR1flip (L497Y)] are superposed after the peak
amplitudes are scaled. Note that the rises are virtually
identical.
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Typical currents evoked by glutamate pulses in patches from cells
expressing GluR1flip (L497Y) channels are
illustrated in Figure 1B. As shown by Stern-Bach et
al. (1998) , these channels generate a sustained current that does not
show the rapid decay that is characteristic of wild-type AMPA
receptor-mediated currents. However, in each of the seven patches
analyzed here, the glutamate-activated currents did show some decay,
albeit slow and incomplete (Fig. 1Ba). Single
exponential fits to these decays gave a mean time constant of 111 ± 13 msec; the mean amplitude of the sustained plateau current was
86 ± 2% of the peak amplitude (n = 7). It is
therefore likely that some residual desensitization is still present in
the mutant channels.
The L497Y mutation did not appear to affect the speed of activation.
The currents in Figure 1, A and Ba, have been
normalized and superposed in Figure 1Bb to illustrate
the similar rise of the currents through wild-type and mutant channels.
Heteromeric channels display intermediate
desensitization kinetics
To determine the relative dominance of the wild-type and mutant
phenotypes, we recorded currents activated by 5 mM
glutamate in outside-out patches from HEK 293 cells that were
cotransfected with equal amounts of the plasmids encoding
GluR1flip and GluR1flip (L497Y). A typical example of the recordings obtained in these experiments is presented in Figure 2. In
each of six patches, three exponential components were required to
obtain adequate fits to the decays of the glutamate-activated currents.
The three individual components are shown in Figure
2B as dotted lines. The mean values
obtained for the time constant of the fast
( f), intermediate
( i), and slow ( s)
components were 3.94 ± 0.14, 19.5 ± 1.2, and 94 ± 10 msec, with respective amplitudes of 31 ± 1.6, 30 ± 1.2, and
12 ± 1.6% of the total peak current (n = 6 patches). At this 1:1 DNA ratio, the sustained current represented 27 ± 2.1% of the total current. Because the slow component
decayed with a time constant that was indistinguishable from that of
homomeric GluR1flip (L497Y) channels (Fig.
1Ba), the slowly decaying component and the sustained
current were treated as a single desensitization phenotype, which is
hereafter referred to as the slow component.

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Figure 2.
Coexpression of GluR1flip and
GluR1flip (L497Y) gives an intermediate component of decay.
Aa, Current elicited by 5 mM glutamate
(bar) in a patch from a cell transiently cotransfected
with equal amounts of wild-type GluR1flip and the
GluR1flip (L497Y) mutant. The decay of the current contains
three resolvable exponential components. The triple exponential fit
(smooth solid line) and the corresponding residual
current (res) are shown. Ab, The same
current and the fit are shown on an expanded time scale, together with
each of the individual exponential components (dotted
lines). The three components decay at fast
(f; f = 3.72 msec),
intermediate (i; i = 19.5 msec), and
slow (s; s = 97 msec) rates. The
slow component of decay and the steady-state plateau current are
treated as a single component. Each of the three components represents
approximately one-third of the total current.
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The results of these coexpression experiments indicated that the
channel population generated by mixing wild-type and non-desensitizing subunits displays three distinct phenotypes that are characterized by
different rates and extents of desensitization. Under conditions in
which the expression of the two types of subunits is approximately equal (1:1 cDNA ratio), the three components that are distinguishable in the decay of large ensemble currents have similar amplitudes. Approximately one-third of the channels desensitize with a rapid time
course that is slightly slower than that of homomeric wild-type channels, approximately one-third desensitize at a rate
( i 20 msec) that is intermediate between
wild-type and mutant homomers, and the remaining one-third desensitize
incompletely and at a rate that is similar to that of homomeric mutant channels.
The amplitude of each phenotype depends on the ratio of wild-type
and mutant cDNAs
One interpretation of the results obtained in the coexpression
experiments is that the rate and extent of desensitization depends on
the stoichiometry of wild-type and mutant subunits in individual
channel assemblies. To investigate this possibility further, we tested
different mutant/wild-type cDNA ratios to vary the relative abundance
of mutant and wild-type subunits. With the exception of the L497Y
mutation, the expression plasmids used in our experiments were
identical. Figure 3 shows typical results obtained in outside-out patches from cells transfected with cDNA mixtures at mutant/wild-type ratios of 1:6 (A), 1:3
(B), and 3:1 (C). Each panel of
Figure 3 shows the current evoked by a 700 msec application of 5 mM glutamate, the fit to its decay, and the
corresponding residual current. The insets show the same
recordings on an expanded time scale with the individual components
(fast, intermediate, and slow) that were detected in the decays shown as dotted lines.

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Figure 3.
The relative amplitudes of the fast,
intermediate, and slow components of decay vary systematically with the
ratio of wild-type and mutant cDNAs. Aa,
Glutamate-evoked current in a patch from a cell cotransfected with
plasmids encoding GluR1flip (L497Y) and
GluR1flip at a cDNA ratio of 1:6. The decay of the current
was fitted with two exponential components and a small sustained
current. The fit (smooth solid line) and the residual
current (res) are shown. Ab, Same trace
as in Aa on an enlarged time scale together with the
three individual components (dotted lines). The values
for f and i are given. B,
Same as A, except that the cell from which the patch was
excised was cotransfected with GluR1flip (L497Y) and
GluR1flip cDNAs at a ratio of 1:3. C, Same
as A, except that the transfection mixture contained
GluR1flip (L497Y) and GluR1flip cDNAs at a
ratio of 3:1. Note that there is no fast component of decay. The time
constants obtained for the fast and intermediate components are given
in each panel.
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Three main findings were evident from the coexpression experiments.
First, as the mutant/wild-type cDNA ratio was systematically increased,
the relative amplitude of the fast component of decay decreased and the
relative amplitude of the slow component increased. At a
mutant/wild-type ratio of 3:1, the fast component was very small or
absent. Second, concomitant with these changes, the time constant of
the fast component became gradually slower. Third, at each cDNA ratio
tested, there was a component of decay that proceeded with a time
constant of ~20 msec. The fits to the currents evoked in patches from
cells transfected with mutant and wild-type cDNAs at a ratio of 1:6
gave mean f and i
values of 3.04 ± 0.08 and 22.3 ± 1.6 msec, respectively
(n = 7). The relative amplitudes (as a proportion of
the total peak current) were 0.90 ± 0.02 for the fast component,
0.08 ± 0.01 for the intermediate component, and 0.02 ± 0.004 for the slow component. In the experiments in which a 1:3
mutant/wild-type ratio was used, we found f = 3.52 ± 0.10, i = 20.2 ± 1.6, and
s = 117 ± 10 msec (n = 5). The relative amplitudes were 0.66 ± 0.04 for the fast
component of decay, 0.17 ± 0.02 for the intermediate component,
and 0.085 ± 0.001 for the slow plus sustained current. The
results from the experiments using a mutant/wild-type ratio of 3:1 gave
mean i and s values of 18.4 ± 1.2 and 121 ± 8 msec, respectively
(n = 5). The relative amplitudes of the intermediate
and slow components were 0.19 ± 0.02 and 0.81 ± 0.02.
Comparison of the results with combinatorial predictions
The results above show that the relative amplitudes of the three
components distinguished in the decay of currents evoked by sustained
applications of glutamate changed in a graded fashion as the
mutant/wild-type cDNA ratio was altered. To test further the hypothesis
that the three components arise from channels with different
stoichiometries of mutant and wild-type subunits, we calculated
the proportions of each possible subunit combination, assuming that
channel assembly is combinatorial.
The combinatorial analysis that we performed rests on several
simplifying assumptions. First, we assumed that the relative abundance
of wild-type and mutant subunits accurately reflects the ratio of the
two cDNAs used for the transfection. Because the expression levels were
high, and the two cDNA constructs were identical except for the point
mutation, we believe that this assumption is reasonable. Second, our
analysis assumed that the point mutation does not affect subunit
assembly. Although this assumption is untested, the levels of
expression seen when each cDNA was expressed alone were similar, and
some channel properties, e.g., the apparent rate of activation, were
unaltered by the mutation.
The combinatorial analysis also assumes that the unitary conductance
and probability of channel opening were similar for wild-type and
mutant channels. It has been shown that the corresponding leucine-to-tyrosine mutation in GluR3 (L507Y) does not alter either the
main conductance level or the open probability
(Popen) of homomeric channels formed
from this subunit (Rosenmund et al., 1998 ; Stern-Bach et al., 1998 ). We
performed fluctuation analysis of steady-state currents over a range of
five to seven glutamate concentrations to estimate the unitary
conductance and Popen of homomeric
GluR1flip (L497Y) channels. These results were
compared with the corresponding results obtained for wild-type
GluR1flip channels in the presence of 100 µM cyclothiazide (to slow desensitization). At
saturating agonist concentrations, the noise
values obtained for both types of homomeric channels were similar
(wild-type GluR1: 24.9 ± 1.7 pS, n = 7; GluR1
(L497Y): 24.6 ± 1.9 pS, n = 4), and the
Popen was 0.8-0.9. These
Popen values are similar to the
corresponding values for the peak
Popen of wild-type GluR1 channels with
intact desensitization (Banke et al., 2000 ).
Finally, our combinatorial analysis implicitly assumed that the
channels in the excised patches are representative of the population
expressed in a given cell. The patches used for the analysis gave peak
inward currents that were always >300 pA and were typically ~1 nA
(at the routine holding potential of 90 mV). Given the unitary
conductance of GluR1 channels (Derkach et al., 1999 ; Banke et al.,
2000 ; this paper), the peak currents all correspond to more (usually
much more) than 150 channels open simultaneously, which is a
sufficient number to be representative.
With the above assumptions, the probability of each possible
wild-type/mutant stoichiometry can be predicted from the binomial equation (see Materials and Methods). The calculated probabilities for
the possible wild-type and mutant subunit combinations are given in
Figure 4 for each of the four
mutant/wild-type cDNA ratios investigated. Figure 4A
gives the combinatorial predictions assuming that the receptor is a
tetramer, whereas the probabilities in Figure 4B
assume the channel is a pentamer. These probabilities can then be
compared with the relative amplitudes of the three exponential
components distinguished in the current decays. If AMPA receptors are
tetramers, the results obtained with a 1:1 cDNA ratio (approximately
equal amounts of fast, intermediate, and slow current) can be accounted
for if the rapidly decaying component corresponds to channels
containing three or four wild-type subunits (0.25 + 0.06 = 0.31),
the intermediate component corresponds to channels with two wild-type
and two mutant subunits [0.37 (Fig. 4A, shaded
row)], and the slow component arises from channels with three or
four mutant subunits (0.06 + 0.25 = 0.31). This partitioning of
the probabilities also matches well our observation that the relative
amplitude of the intermediate component is similar for mutant/wild-type
ratios of 1:3 and 3:1 (0.17 and 0.19 vs 0.21 predicted). The relative
amplitude of the intermediate component at a mutant/wild-type ratio of
1:6 also agrees with the predictions (0.08 observed vs 0.09 predicted).

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Figure 4.
The results support the idea that AMPA receptors
are tetramers. A, Table showing the probability of
occurrence of each possible subunit combination if the channels are
tetramers for the different cDNA ratios examined. Each
row corresponds to channels with a different number of
mutant subunits (0, 1, 2,
3, 4) as indicated. The
shaded row corresponds to channels containing two mutant
subunits and predicts well the measured relative amplitude of the
intermediate component. The relative proportions of the fast component
of desensitization match well the predicted proportion of channels
containing no or one mutant subunit. The relative proportions of the
slow component match well with the sum of homomeric mutants and
channels containing one wild-type subunit. B,
Probability of occurrence of all subunit combinations if the channels
are pentamers. No partitioning of the subunit combinations matches the
proportion of fast, intermediate, and slow phenotypes over the range of
cDNA ratios tested.
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In contrast to the results obtained assuming the channel is a tetramer,
there is no partitioning of the probabilities in Figure 4B (channels assumed to be pentamers) that matches
well the relative amplitudes of the three components over the range of
cDNA ratios tested. This is so despite the fact that there are more
ways to partition the results, which might be expected to increase the chance of a spurious match. In particular, there is no partitioning that can account for the roughly equal amplitudes of each component at
a cDNA ratio of 1:1, nor our observation that the amplitude of the
intermediate component was similar at mutant/wild-type ratios of 1:3
and 3:1. For example, if the intermediate component is identified with
channel assemblies containing three mutant subunits [(Fig.
4B, shaded row) 0.31 probability at a 1:1
ratio], then it is predicted that the fast component should be more
than twice the amplitude of the slow component (0.5 vs 0.19). This way
of partitioning the pentameric probabilities also predicts that the
intermediate component should have been very small (0.02) at a
mutant/wild-type ratio of 1:6 and that the relative amplitudes of the
intermediate component at cDNA ratios of 1:3 and 3:1 should have
differed substantially (0.26 vs 0.09). None of these predictions is
borne out by the results.
The above comparisons indicate that the results can be accounted for if
the channels are tetramers and the three distinguishable components
correspond to channel assemblies with different stoichiometries of
mutant and wild-type subunits. As noted, this analysis rests on the
assumption that the relative amplitude of each component accurately
reflects the relative abundance of the corresponding channel
population. The rise of the currents was substantially faster than the
decays, even for the fast component, making it unlikely that we were
significantly underestimating the peak amplitudes because the solution
exchanges were insufficiently fast. However, because desensitization
appears to proceed via closed states (Vyklicky et al., 1991 ; Raman and
Trussell, 1992 , 1995 ), some channels are expected to desensitize
without ever opening, and the proportion that do is likely to depend on
the rate constant for entry into desensitization. To estimate the
extent to which this might confound the analysis, we recorded
glutamate-evoked currents in the absence and presence of cyclothiazide,
a drug that appears to reduce the rate at which AMPA-type channels
enter into desensitization (Partin et al., 1996 ). Because we found that
cyclothiazide caused a modest rundown of the peak currents evoked by
prolonged glutamate applications, these experiments were made with a
piezoelectric system that allowed us to make glutamate applications of
10 msec or less.
Responses to brief applications of 5 mM glutamate in the
absence and presence of 100 µM cyclothiazide are shown in
Figure 5A. The currents were
measured in the same patch from a cell transfected with wild-type
GluR1flip. In each of four patches studied,
cyclothiazide caused an increase in the peak current through homomeric
wild-type channels (mean percentage increase 34 ± 2%;
n = 4). This result is predicted for models of the type
shown in Figure 6D,
where activation and desensitization occur independently from the same closed state. Although the available results are insufficient to define
some of the rate constants for the model in Figure
6D, at high agonist concentrations the channels spend
most of their time in fully liganded states, and this model predicts
behavior similar to simpler models proposed previously. Simulations of channel activity evoked by 5 mM glutamate (using
the model in Fig. 6D) showed that the decay of
wild-type currents during sustained applications of glutamate could be
reproduced with values for channel opening ( 4)
and channel closing ( 4) of 7000 s 1
and 2550 s 1
and rate constants for entry into and exit from desensitization of 2000 s 1
( 4) and 1 s 1
( 4). As shown in Figure 5B, these
values also gave the observed amount of potentiation by cyclothiazide
if it was assumed that the effect of cyclothiazide was solely to reduce
the rate of entry into desensitization ( 4 = 1 s 1) (Partin
et al., 1996 ). Also shown in Figure 5B are simulated currents that give decay time constants that mimic the intermediate and
slow components detected in the coexpression experiments. The
simulations predict that the peak of the intermediate component more
closely approaches that generated by the same number of homomeric mutant channels, because it was necessary to reduce
4 to slow the decay of this component to the
extent observed experimentally. The results of the simulation analysis
suggest that the peak amplitudes of the fast and intermediate
components underestimate the proportion of channels underlying these
phenotypes because significant numbers of channels enter
desensitization without opening.

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Figure 5.
The effect of cyclothiazide and comparison of the
results with combinatorial predictions. A, Currents
evoked by 5 mM glutamate in a patch from a cell transected
with wild-type GluR1flip. Preexposure of the patch to
cyclothiazide (100 µM) greatly slows desensitization and
potentiates the peak current amplitude. B, Simulated
currents generated with the model shown in Figure
6D in response to a sustained application of 5 mM glutamate. The number of channels was set to 1000 for
each simulation. The analysis was performed to estimate the extent to
which the peak current amplitude underestimated the number of channels
as the result of some channels desensitizing without ever opening. The
trace labeled 1 mimics the kinetics of wild-type
GluR1flip homomers. The following values were used for the
rate constants: k1 = 1 × 107 M 1
s 1,
k-1 = 7000 s 1, 4 = 7000 s 1, 4 = 2550 s 1,
4 = 2000 s 1, 4 = 1 s 1. These values reproduced the
rise time (10-90% = 180 µsec), desensitization ( = 2.2 msec, 0.25% plateau current), and deactivation kinetics
( deact = 0.7 msec) (Fig. 6C) of
wild-type channels and gave an EC50 value of ~800
µM. The results were largely insensitive to the values of
the other rate constants. The and values for partially liganded
states were set to the corresponding values for the fully liganded
state. The conductance of the open states with one, two, and three
agonist molecules bound were taken to be 0.25, 0.5, and 0.75 of the
value of the fully liganded state. It was assumed that glutamate bound
with 100-fold higher affinity to desensitized channel states
(k1 = k2,
k 2 = 70 s 1), and the and values
for partially liganded states were set to maintain microscopic
reversibility. The trace labeled 3 was obtained with
4 = 1 s 1
and mimics the effect of cyclothiazide on wild-type channels. The trace
labeled 2 mimics the decay of the intermediate component
( = 20 msec) and was obtained by setting 4 = 400 s 1 and
4 = 1400 s 1. The trace labeled
4 mimics the decay of the slow component ( = 100 msec, 90% plateau current) and was obtained by setting
4 = 200 s 1,
4 = 80 s 1,
and 4 = 15 s 1. These values gave a
deact of 9 msec, which is similar to the value measured
for homomeric mutant channels (Fig. 6C). Note that the
peak wild-type and intermediate currents (traces 1 and
2) reach only 65 and 88% of the amplitude of the slow
component (trace 4), although the number of
channels was set to 1000 for each simulation. C, The
relative amplitudes of the three components fast ( ), intermediate
( ), and slow ( ), at the four cDNA ratios tested. Each
point is the mean value from measurements made in five
to seven patches. The bars indicate the SD, some of which were less than half the symbol height. The
black curves show the summed probability of homomeric
GluR1flip channels and channels with one
GluR1flip (L497Y) subunit (solid line), the
probability that channels will contain two GluR1flip
(L497Y) subunits (dotted line), and the summed
probability of having homomeric GluR1flip (L497Y) and
channels with one wild-type GluR1flip subunit
(dashed line). The probabilities are plotted as a
function of the proportion of wild-type subunits present, assuming that
the subunit assemblies are tetramers. The gray curves
show the corresponding probabilities after adjusting the results for
the fast and intermediate components (for missing channels that never
open) using the relative amplitudes of the peak currents predicted from
the simulated results in B (fast and intermediate
components underestimated by 35 and 12%, respectively, relative to the
slow component).
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Figure 6.
The results are consistent with the conclusion
that AMPA receptors are dimers of dimers. A, The
relative amplitude of the slow component is plotted as a function of
the proportion of wild-type cDNA included in the transfection mixture.
Each point is the mean value from measurements made in
five to seven patches. The bars indicate the SD. The black
curve shows the expected proportion of tetramers that contain
at least one dimer with two mutant subunits. The gray
curve shows the corresponding prediction after correcting for
missing channels that never open using the simulated data in Figure
5B. B, Diagram illustrating the
partitioning of tetrameric assemblies assumed to display wild-type and
mutant desensitization for the combinatorial analysis shown in
A. C, Deactivation kinetics of wild-type
GluR1flip (left) and homomeric
GluR1flip (L497Y) channels (right). The
currents were evoked by 1 msec applications (bars) of 5 mM glutamate. The decays of the currents (dotted
traces) were fitted with single exponential functions
(solid curves) with the indicated time constants.
Da, Possible kinetic scheme illustrating some general
features of AMPA receptor activation and desensitization suggested by
previous work. It is assumed that the channel is a tetramer where each
subunit can bind a single agonist molecule (A)
and can exist in three distinct conformations: closed
(C), open (O), and
desensitized (D). The states in the top
row are open, those in the middle row are
closed, and those in the bottom row are desensitized.
For closed and desensitized states, each subunit is constrained to
adopt the same conformation. The affinity of agonist binding is higher
affinity to desensitized states than to closed states
(k 2/k2 < k 1/k1).
The top two rows represent one of the models tested by
Smith et al. (2000) that incorporates evidence for
concentration-dependent substate gating and the presence of as many as
four discrete open levels for some native AMPA receptors. The notation
of the open states implies that individual subunits gate independently.
For simplicity, it is assumed that binding is not cooperative, that
binding and unbinding do not occur when the channel is open, that
transitions between nonadjacent states do not occur, and that the
probability of opening from state C4 is zero.
Db, Enlarged view of the scheme showing the portion of
the model most relevant to our results.
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Figure 5C is a plot of the mean relative amplitudes of the
fast, intermediate, and slow components of desensitization as a function of the proportion of wild-type cDNA included in the
transfection mixture. The smooth curves show the respective
probabilities that channel assemblies will contain 0 or 1, 2, and 3 or
4 mutant subunits, assuming that the channels are tetramers. The
black curves show the combinatorial predictions. The
gray curves show the result of correcting the combinatorial
predictions for the likely underestimation of the fast and intermediate
components that would occur if some channels desensitize without ever
opening. There is good agreement between the combinatorial predictions
and the results at each cDNA ratio tested, supporting the notion that
the kinetically distinct components of desensitization arise from
channels with different numbers of mutant subunits. Although the
cyclothiazide results suggest that the peak fast and intermediate
currents underestimate the number of channels by ~35 and 12%,
respectively, this is predicted to have only modest effects on the
results. The potential influence of such errors is greatest when all
three components are of similar amplitude.
Although we believe that the combinatorial analysis supports the view
that AMPA receptors are tetramers, two further observations are worthy
of emphasis. First, the time constant of the fast component detected in
the coexpression experiments was slower than the corresponding value
measured for homomeric wild-type channels ( f = 2.24 msec), and it became increasingly slower as the relative amount of
mutant cDNA was increased ( f = 3.04, 3.52, and
3.94 msec for mutant/wild-type ratios of 1:6, 1:3, and 1:1). Each of
the mean f values measured in the coexpression
experiments was significantly greater than the
f measured for wild-type channels
(p < 0.001; one-way ANOVA), and the
f values for the 1:3 and 1:1 ratios were
greater than the value of 3.04 msec obtained at a wild-type/mutant
ratio of 1:6 (p < 0.05). Second, although there
is good agreement in Figure 5C between the predictions and
the results, at each cDNA ratio studied the slow component is slightly
larger than predicted and the intermediate component is too small. One
way to resolve this small, but consistent, discrepancy is to assume
that the channels underlying the intermediate component also generate
some of the plateau current. However, new structural data suggest an
alternative interpretation of the results.
The results are consistent with dimeric
subunit assembly
Armstrong and Gouaux (2000) recently published additional x-ray
crystallographic data on the structure of the ligand binding domain of
GluR2 and showed that the binding domains crystallize as dimers.
Strikingly, two of the residues participating in intersubunit interactions are L483 (L497 for GluR1) and the aspargine residue (N754)
that is critical for conferring flop-like sensitivity to cyclothiazide
(N750 for GluR1) (Partin et al., 1995 ). L483 forms a hydrophobic
cluster with residues in the flip/flop domain on the adjacent protomer.
Because the dimer exhibits twofold symmetry, the L483 residues on
adjacent protomers create two spatially distinct connections.
Although Armstrong and Gouaux (2000) were careful to emphasize that
their results could reflect a crystal-packing artifact, if AMPA
receptor assembly proceeds via the formation of dimers, then all
tetrameric assemblies with two mutant subunits are not identical. In
one-third of such assemblies the two mutant subunits will be in the
same dimer, whereas in the others each dimer will contain one mutant
subunit. Figure 6A compares the results with the
combinatorial predictions when it was assumed that all tetramers containing at least one mutant dimer (both subunits with the L497Y mutation) were non-desensitizing, whereas the extent to which other
heteromeric channels desensitized was indistinguishable from wild-type
homomers (Fig. 6B). As can be seen, the relative amplitude of the slow component agrees well with the proportion of
channels that contains at least one mutant dimer at each cDNA ratio
tested (Fig. 6A). Correction for missing channels
that never open (gray curve) produces even better
agreement. Thus the size of the slow component can be accounted for if
it is assumed that the non-desensitizing phenotype of
GluR1flip (L497Y) is dominant, but that this
dominance requires that at least one dimer in the tetramer contains two
mutant subunits.
Slow desensitization versus slow deactivation
Although the "dominant dimer" interpretation accounts for the
dependence of the size of the slow component on the relative abundance
of wild-type and mutant subunits, it does not explain the intermediate
component of decay. However, as emphasized by Partin et al. (1996) , the
decay of AMPA receptor currents in the continuous presence of agonist
is determined by the rate of both deactivation and desensitization.
Previous work on wild-type GluR1 homomers has given deactivation time
constants of ~0.8 msec (Partin et al., 1996 ). In contrast, the
deactivation rate of homomeric GluR1flip (L497Y)
channels is much slower. Figure 6C illustrates the decay of
currents through wild-type and mutant homomers after termination of a 1 msec application of 5 mM glutamate. The decays have been fitted with single exponential functions that give time constants that differ by more than an order of magnitude. On average, the mean time constant of deactivation was 0.68 ± 0.07 msec for wild-type channels and 8.9 ± 0.9 msec for channels carrying the L497Y mutation (n = 5 and 4 patches, respectively).
Thus, in addition to altering desensitization, the L497Y mutation also
produces a ~13-fold slowing of deactivation.
Two commonly agreed upon features in previously published models of
AMPA receptor kinetics are that desensitization occurs exclusively from
closed states and that the rate constant for channel opening is greater
than the rate constant for entry into desensitization (Vyklicky et al.,
1991 ; Raman and Trussell, 1992 , 1995 ; Partin et al., 1996 ). Figure
6D illustrates a kinetic scheme that incorporates
these features and extends them to account for concentration-dependent
substate gating and the accumulating evidence that AMPA
receptors are tetramers (Mano and Teichberg, 1998 ; Rosenmund et al.,
1998 ; Smith and Howe, 2000 ). In this scheme, the observed decay during
a sustained application of a saturating concentration of agonist will
be determined not just by the rate constant for entry into
desensitization ( 4) but also by the length of
individual openings (1/ 4) and the average
number of times the channel opens before desensitization occurs.
Comparisons of the time constants of deactivation and desensitization
for various AMPA-type channels suggest that, on average, the fully
liganded receptor will open and close multiple times before it
desensitizes (Partin et al., 1996 ). Depending on the relative values of
k 1, 4, and 4, it is also possible that the apparent
slowing of deactivation might reflect a decrease in the rate of entry
into desensitization ( 4).
To gain some insight into the effect of the L497Y on the various
microscopic rate constants that could influence operational measurements of the time constants of deactivation and desensitization, we performed channel simulations and systematically altered the rate
constants for transitions into and out of fully liganded channel
states. The analysis indicated that the slowing of deactivation could
be largely accounted for if it was assumed that it arose from
alterations in 4, the rate constant for
channel closure. In contrast, independent alterations in
k-1, 4, and
4 failed to reproduce the results. For
example, slowing 4 to the extent required to
reproduce the mutant desensitization phenotype resulted in virtually no
change in deactivation, and increasing 4 to an extent sufficient to slow both deactivation and desensitization produced activation time courses that were unrealistic. Alterations in
k 1 that markedly slowed
desensitization gave biphasic deactivation decays caused by the
interspersion of substate openings between sequential unbinding steps.
In contrast, reducing 4 by a factor of 13 not
only accounted for the slowing of deactivation in the L497Y mutant
channels, but it slowed the decay of the current during a sustained
application of glutamate to a similar extent. We have not measured the
deactivation rate for the intermediate component of decay. However, if
the slowing of deactivation depends on the stoichiometry of wild-type
and mutant subunits, then this would largely explain the appearance of
the intermediate component. If channels containing a single mutant
subunit deactivate somewhat more slowly than wild-type channels, the
apparent slowing of the fast component of decay could reflect the
increasing (but unresolved) contribution of this slower component as
the relative abundance of mutant subunit was increased. To test this
latter idea, we generated decays that contained four components and
then fit them with only three exponentials. We found that the slowing
of the fast time constant of desensitization could be reproduced if it was assumed that the currents through channels containing one mutant
subunit decay with a time constant of ~4 msec (twofold reduction in
4).
Intermediate channels recover faster from desensitization
It has been proposed that the entry into, and recovery from,
desensitization may proceed via different paths (Patneau and Mayer,
1991 ; Jonas, 1993 ; Raman and Trussell, 1995 ). To test whether the
inclusion of the mutant subunit in receptor assemblies also altered the
rate of recovery from desensitization, we compared the speed of
recovery of the intermediate and fast components. For these
experiments, we used patches from cells transfected with mutant and
wild-type cDNAs at a ratio of 1:3, which showed substantial fast and
intermediate components in their decays. Patches were conditioned with
an application of glutamate (0.5 mM for 100 msec), and then
a second application was delivered at varying times after the
conditioning pulse.
A typical example of the results obtained in these experiments is shown
in Figure 7A. The decays of
the currents evoked by the conditioning and test pulses were each
fitted with three exponential components. The amplitudes of the fast
and intermediate components in the decay of the current evoked by the
test pulse were then expressed as a proportion of the amplitude of the
corresponding component in the decay of the current evoked by the
conditioning pulse. Figure 7B shows a plot of the relative
amplitudes of the fast and intermediate components as a function of
recovery time, where each point is the mean value obtained from five
patches. Single exponential fits to each set of results gave recovery
time constants ( rec) of 154 msec for the fast
current and 51 msec for the intermediate current. The apparent offset
(see Materials and Methods) was similar for both sets of data (19 and
21 msec). Because the intermediate component of decay appears to arise
from channels that contain two mutant subunits, the data from the
two-pulse experiments suggest that these channels also recover from
desensitization faster than wild-type channels.

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Figure 7.
The intermediate component recovers faster from
desensitization and shows reduced apparent affinity for glutamate.
A, Six consecutive sweeps obtained in a patch from a
cell that was cotransfected with GluR1flip (L497Y) and
GluR1flip cDNAs at a ratio of 1:3. Glutamate (0.5 mM) was applied for 100 msec, and then a second application
was made at a varying interval (40, 80, 120, 150, 200, 300 msec). The
decays of the currents evoked by the second application of each pair
were fitted with three exponential components, and their amplitudes
were expressed as a proportion of the corresponding component in the
decay of the current evoked by the preceding conditioning pulse.
B, Graph showing the recovery from desensitization of
the fast ( ) and the intermediate ( ) components. Each
point is the mean from five different patches (bars
indicate SD). Each set of results was fitted with a single exponential
function. The fits did not extrapolate to zero time. This apparent
offset was estimated from the fit and was subtracted from all recovery
times. C, Percentage inhibition of peak currents through
wild-type GluR1flip channels ( ) are plotted as a
function of glutamate concentration and compared with the corresponding
results for the intermediate component detected in coexpression
experiments ( ). Each point is the mean value obtained
from five patches (bars indicate SD). Each data set was fitted with a
Hill-type equation with the maximal inhibition constrained to 100%. In
the coexpression experiments, glutamate concentrations above 10 µM produced significant channel activation. The fits gave
IC50 values of 0.89 µM for the wild-type
channels and 4.30 µM for the channels underlying the
intermediate component of decay. D, Currents in a patch
from a cell transfected with GluR1flip (L497Y) and
GluR1flip at a cDNA ratio of 1:3. The records are responses
to 5 mM glutamate before and during preincubation with 2 µM glutamate. The three-exponential fits to the decays
(smooth solid lines) are superposed on the currents, and
the dotted lines show the intermediate component
obtained from each fit. Note that preincubation with glutamate reduces
the amplitude of the fast component more than it does the amplitude of
the intermediate component (71 and 30% inhibition,
respectively).
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At high agonist concentrations, recovery from desensitization could
occur directly to non-desensitized states or it might proceed initially
via unbinding transitions, with exit from desensitization only
occurring after agonist has dissociated from one or more subunits. Thus
the somewhat faster recovery of the intermediate component could either
reflect modest destabilization of desensitized channel states (increase
in 4) (Fig. 6D) or a
decreased affinity of glutamate binding to these states (increase in
k 2). To distinguish between these
two possibilities, we determined the apparent affinity of glutamate for
desensitized channel states. As reported by others (Trussell and
Fischbach, 1989 ; Colquhoun et al., 1992 ; Raman and Trussell, 1992 ),
preincubation of wild-type channels with low concentrations of
glutamate (which do not cause detectable channel activation) produces
significant desensitization, as assessed by depression of the currents
evoked by subsequent glutamate applications. The data in Figure
7C gave an IC50 value of 0.89 µM for glutamate depression of glutamate-evoked
currents through wild-type GluR1flip channels (n = 4 patches). The corresponding value measured for the intermediate
component of decay was 4.3 µM
(n = 5 patches). An example of the preincubation
results obtained in one of the patches is shown in Figure
7D. Preincubation of the patch with 2 µM glutamate resulted in a substantial
reduction in the fast component of decay with much less effect on the
amplitude of the intermediate component. The results support the
conclusion that the desensitized states of channels underlying the
intermediate component exhibit four- to fivefold lower affinity for
glutamate (compared with wild-type channels), and they suggest that
this reduced affinity is why the channels recover faster from desensitization.
The expression of GluR1flip (L497Y) in neurons also
gives an intermediate phenotype
From studies in oocytes, Thalhammer et al. (1999) concluded that
the L497Y mutation is dominant, the presence of a single mutant subunit
being sufficient to render various types of heteromeric AMPA receptors
non-desensitizing. This conclusion appears at odds with our results.
Therefore, to determine whether the intermediate desensitization
behavior that we observed after coexpression of GluR1flip with GluR1flip
(L497Y) was unique to channels containing exclusively flip versions of
GluR1, we expressed the GluR1flip (L497Y) subunit
in cerebellar granule cell neurons. Primary cultures of rat cerebellum
were maintained in vitro for 6-8 d and transiently transfected with GluR1flip (L497Y). Granule cells
expressing the mutant subunit (identified by coexpressing the GFP)
represented 1-2% of the total number of cells per coverslip. The
decay kinetics of responses to glutamate (2 mM)
were determined in patches pulled from transfected granule cells and
compared with the kinetics of responses obtained in patches from
untransfected cells on the same coverslip.
Typical currents evoked by the application of 2 mM
glutamate in patches from control and transfected cells are shown in
Figure 8. As illustrated in Figure
8A, currents in patches pulled from control cells
showed rapid and virtually complete desensitization. The decays of
these currents contained two exponential components. The fits to
results obtained in eight control patches gave mean time constants for
these components of 1.05 ± 0.09 and 3.82 ± 0.15 msec. On
average, the amplitude of the fast and slower components represented
66 ± 1.4 and 34 ± 1.8% of the total peak current. Granule
cells express predominantly the GluR2 and GluR4 subunits (Monyer et
al., 1991 ). The time constant of the fast component ( 1 msec) agrees well with the corresponding value for channels containing
the GluR4flop subunit (with or without GluR2),
whereas the slower component ( 4 msec) is similar to the
desensitization rate of channels that contain
GluR4flip (with or without the flop version of
GluR2) (Mosbacher et al., 1994 ). Thus the fast and slow components
likely arise from channels containing the flop and flip versions of
GluR4, respectively. None of the patches gave plateau currents that
were >1% of the total peak current.

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Figure 8.
The assembly of GluR1flip (L497Y) with
native subunits also generates intermediate desensitization.
Aa, Current activated by glutamate (2 mM) in
an outside-out patch from a control granule cell maintained in culture
for 7 d. The decay of the current was fitted with a function
consisting of two exponentials (smooth solid line).
Ab, Same current on an expanded time scale with the
individual components superposed (dotted lines). The
time constants of the two components are given on the figure.
Ba, Current activated by 2 mM glutamate in a
patch from a granule cell that was maintained in vitro
for 7 d and transiently transfected 24 hr before with
GluR1flip (L497Y). The decay of the current was fitted with
a function consisting of three exponentials and a sustained current
(smooth solid line). Bb, The current, the
fit, and the three individual exponential components are shown on an
enlarged time scale. The time constants for the fast and intermediate
components are given. Note that the fast component is slower than the
fast component in the control neuron.
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As shown in Figure 8B, the currents evoked by
glutamate in patches pulled from neurons expressing the
GluR1flip (L497Y) subunit displayed a large
sustained component that was clearly not present in the patches pulled
from control granule cells. The decays of these currents contained
three exponential components with time constants of 3.61 ± 0.24, 26.5 ± 2.4, and 180 ± 20 msec (n = 5 patches). In all the patches, both the slow component (including the
plateau current) and the intermediate component represented >20% of
the total peak current. The similarity of the intermediate component of
decay in transfected neurons to the intermediate component seen in the
cotransfection experiments strongly supports the conclusion that it
arises from heteromeric assembly of GluR1flip (L497Y) with native AMPA receptor subunits. Indeed, the decays of the
responses in transfected neurons also showed a slowing of the fast
component of decay, and they were strikingly similar to those observed
in HEK 293 cells (compare Figs. 3 and 8). This similarity suggests that
our observations with recombinant channels are not restricted to GluR1
homomeric channels, nor are they likely to be unique to channels
composed solely of flip splice variants.
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DISCUSSION |
The coexpression of GluR1flip with the
non-desensitizing mutant subunit GluR1flip
(L497Y) produced channels that appear to desensitize at three
kinetically distinct rates, one of which is intermediate between that
of wild-type and mutant homomeric channels. The relative amplitudes of
the three components were described well by simple combinatorial
predictions if the channels were assumed to be tetramers. In contrast,
there was no partitioning of the combinatorial probabilities that
accounted well for the results if the channels were assumed to be pentamers.
Allosteric models of desensitization and subunit dominance
Allosteric models of the Monod-Wyman-Changeaux (MWC) type (Monod
et al., 1965 ) have been advanced to explain the behavior of various ion
channels. Here allosteric implies, among other things, that each
subunit in the oligomer can exist in at least two distinct
conformations, all subunits are constrained to adopt the same
conformation, and the ligand binds to one subunit conformation with
higher affinity than to the others (for review, see Colquhoun, 1998 ).
It has been noted that the desensitization of AMPA receptors shows
features reminiscent of such allosteric models. First, concentrations
of glutamate insufficient to activate AMPA receptors can produce nearly
complete AMPA receptor desensitization (Trussell and Fischbach, 1989 ;
Patneau and Mayer, 1991 ; Colquhoun et al., 1992 ; Raman and Trussell,
1992 ), supporting the idea that glutamate binds with highest affinity
to the desensitized form of the receptor. Second, evidence supporting a
concerted conformational change comes from results showing that some
desensitization phenotypes are dominant in heteromeric assemblies. For
example, the GluR4flop subunit determines the
rate of desensitization in heteromeric channels (Mosbacher et al.,
1994 ), and the presence of a single flip-type subunit appears
sufficient to confer flip-type sensitivity to cyclothiazide (Partin et
al., 1994 , 1995 ).
One interpretation of our results is that the rate and extent of
desensitization titrates with the number of non-desensitizing subunits.
Although this interpretation conflicts with the notion of subunit
dominance, graded stoichiometric changes do not necessarily argue
against allosteric mechanisms. If the conformational change corresponding to desensitization is concerted, then it might become less likely as the number of "reluctant" subunits in the oligomer is increased and thereby result in a progressive slowing of the rate at
which the population of channels desensitizes.
The results are described just as well, however, by the "dominant
dimer" analysis presented in Figure 6. This interpretation is
consistent with recent structural data (Armstrong and Gouaux, 2000 ) and
also better reconciles our results with the evidence described above
for subunit dominance. If this view is correct, then the decay of the
intermediate component must be largely the result of the slowing of
deactivation. Our simulation results suggest that the decay of the
intermediate component can be accounted for with only modest changes in
the rate constant for entry into desensitization
( 4 decreased less than twofold) if it is
assumed that channels with one mutant subunit in each dimer deactivate sixfold more slowly than wild-type channels. Although this
result somewhat supports the dominant dimer hypothesis, at
present our results do not allow us to exclude other interpretations.
The crystallographic data on the ligand binding domain of GluR2
demonstrate that the dimers show twofold symmetry (Armstrong and
Gouaux, 2000 ). If AMPA receptors display similar symmetry, then they
would be expected to form tetramers in which the protomers associate
exclusively via isologous and symmetrical interactions. As pointed out
by Monod et al. (1965) in their seminal paper on allosteric
transitions, in such symmetrical oligomers each protomer is subject to
the same quaternary constraints, and therefore all protomers are likely
to adopt the same conformation.
The L497Y mutation appears to destabilize desensitized states
Although the slowing of deactivation accounts substantially for
the intermediate component of decay, it cannot account for the
substantial plateau current generated by channels containing three or
four mutant subunits. This greatly reduced steady-state desensitization
must reflect alterations in the rate constants for entry into, or
recovery from, desensitized channel states. The L497Y mutation in GluR1
does not remove desensitization completely. Currents through homomeric
mutant channels decayed with a time constant of ~100 msec to 85-90%
of their peak amplitude (Fig. 1Ba). We found that
reproducing this phenotype in channel simulations required substantial
changes in the values of both 4 and
4 (~15-fold). Indeed this analysis suggests
that it is the increased rate of exit from desensitization that is
largely responsible for the "non-desensitizing" phenotype, because
the channels still enter desensitization frequently, but they return
from desensitization nearly as often.
Armstrong and Gouaux (2000) suggested that the leucine-to-tyrosine
mutation studied here might stabilize interactions between adjacent
protomers [see also Partin (2001) ]. In each protomer, the two
globular domains surrounding the glutamate receptor binding pocket are
thought to close around the ligand in "venus flytrap" models of
ligand receptor binding (for review, see Dingledine et al., 1999 ; Howe,
1999 ). Interestingly, the amount of domain closure is ligand dependent,
being smallest for antagonists, intermediate for the partial and
incompletely desensitizing agonist kainate, and greatest for full and
strongly desensitizing agonists such as glutamate and AMPA (Armstrong
et al., 1998 ; Armstrong and Gouaux, 2000 ). By strengthening
intersubunit interactions, the L497Y mutation might restrict domain
closure within individual subunits. If this is true, and the L497Y
mutation speeds escape from desensitized states, then domain closure
may not initiate desensitization but rather stabilize the resulting
nonconducting conformations.
Effects on apparent affinity
For cyclic models of the type shown in Figure
6D, it is expected that altering desensitization will
alter binding affinity (and vice versa). This is so because to maintain
microscopic reversibility the / ratios for adjacent paths must
differ by the difference in the equilibrium dissociation constants for
binding to closed versus desensitized states [for example:
( 4/ 4)/( 3/ 3) = (k 1/k1)/(k 2/k2) (Fig. 6D)]. In line with these expectations,
cyclothiazide both removes desensitization and markedly increases the
apparent affinity of agonists for non-desensitized closed states
(Patneau et al., 1993 ; Yamada and Tang, 1993 ; Kessler et al., 1996 ).
Previous studies also suggest that the extent of desensitization (as
assessed by the ratio of the peak to plateau current) increases with
agonist concentration (Geoffroy et al., 1991 ; Vyklicky et al.,
1991 ).
The EC50 value that we determined for glutamate
activation of homomeric GluR1flip (L497Y)
channels (28 µM; data not shown) is ~30-fold smaller
than the corresponding value for wild-type GluR1 channels when
desensitization is intact (Partin et al., 1996 ; A. Robert and J. R. Howe, unpublished observations). Our results also suggest that the
inclusion of L497Y subunits in heteromeric assemblies reduces the
affinity with which glutamate binds to desensitized channel states
(Fig. 7C). Thus the L497Y mutation both reduces
desensitization and results in changes in relative affinity that are
qualitatively those expected for allosteric schemes. How tightly
alterations in desensitization are necessarily linked to alterations in
agonist binding affinity, and how our results relate to the
concentration dependence of desensitization, are questions that require
further investigation.
The intermediate component of decay showed hastened recovery from
desensitization, and the apparent affinity of glutamate for
desensitized channel states was reduced to a similar extent as recovery
from these states was speeded. These results suggest that unbinding
steps precede exit from desensitization for the channels underlying the
fast and intermediate components. Studies on native channels support a
similar conclusion (Patneau and Mayer, 1991 ).
Allosteric versus subunit independent gating
Our results support the idea that AMPA receptor desensitization
proceeds via an allosteric mechanism, and they provide functional evidence consistent with dimeric receptor assembly. AMPA receptors also
show concentration-dependent substate gating (Rosenmund et al., 1998 ;
Smith and Howe, 2000 ), a property shared by cyclic nucleotide-gated
(CNG) channels (Ruiz and Karpen, 1997 ). Interestingly, it appears that
CNG channels also behave as dimers of dimers and obey allosteric gating
mechanisms, but for CNG channels it is activation, not desensitization,
that is described by modified MWC schemes (Liu et al., 1998 ; but see
Ruiz and Karpen, 1999 ).
Individual AMPA receptors show as many as four conductance levels, the
frequency of occurrence of which depends on the number of subunits
occupied by agonist (Smith and Howe, 2000 ; Smith et al., 2000 ). One
interpretation of these results, and the staircase behavior described
by Rosenmund et al. (1998) , is that individual subunits gate
independently of the state of the other subunits in the tetramer. Thus
activation may differ fundamentally from desensitization, the latter
being a process that appears to require a concerted conformational
change involving all four subunits (or both dimers). That activation
and desensitization are distinct and separable processes is implicit in
previous kinetic schemes (Raman and Trussell, 1995 ; Partin et al.,
1996 ) and was also a main conclusion of the mutagenesis work of
Stern-Bach et al. (1998) .
 |
FOOTNOTES |
Received Feb. 14, 2001; revised May 9, 2001; accepted May 21, 2001.
This work was supported by National Institutes of Health Grant NS
37904. We thank Derek Bowie for providing the GluR1 constructs.
Correspondence should be addressed to James R. Howe, Department of
Pharmacology, Yale University School of Medicine, 333 Cedar Street, New
Haven, CT 06520-8066. E-mail: james.howe{at}yale.edu.
 |
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M.-L. He, T.-a. Koshimizu, M. Tomic', and S. S. Stojilkovic
Purinergic P2X2 Receptor Desensitization Depends on Coupling between Ectodomain and C-Terminal Domain
Mol. Pharmacol.,
November 1, 2002;
62(5):
1187 - 1197.
[Abstract]
[Full Text]
[PDF]
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P. Legendre, E. Muller, C. I. Badiu, J. Meier, C. Vannier, and A. Triller
Desensitization of Homomeric alpha 1 Glycine Receptor Increases with Receptor Density
Mol. Pharmacol.,
October 1, 2002;
62(4):
817 - 827.
[Abstract]
[Full Text]
[PDF]
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D. Bowie and G. D. Lange
Functional Stoichiometry of Glutamate Receptor Desensitization
J. Neurosci.,
May 1, 2002;
22(9):
3392 - 3403.
[Abstract]
[Full Text]
[PDF]
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