|
|
||||||||
J Neurophysiol (March 1, 2003). 10.1152/jn.00909.2002
Submitted on Submitted 11 October 2002; accepted in final form 13 October 2002
1Department of Mechanical Engineering, University of Rome `La Sapienza', 00184 Rome, Italy; and 2Department of Academic Computing and 3Department of Physiology, University of Massachusetts Medical School, Worcester, Massachusetts 01655
| |
ABSTRACT |
|---|
|
|
|---|
Del Prete, Zaccaria, Stephen P. Baker, and Peter Grigg. Stretch Responses of Cutaneous RA Afferent Neurons in Mouse Hairy Skin. J. Neurophysiol. 89: 1649-1659, 2003. Rapidly adapting (RA), stretch-sensitive neurons were recorded in vitro, using an isolated preparation of skin and nerve from mouse hindlimb. The skin was stretched uniaxially using a pseudo-Gaussian noise stimulus. Loads and displacements were recorded as were spike responses of single RA afferent neurons. The goal was to determine what components of the mechanical stimulus were associated with spike responses. The association between stimuli and spike responses was measured using multiple logistic regression. Spike responses were strongly associated with the rate of change of stress and weakly associated with the rate of change of strain and with stress. There was no association between spike responses and strain. There were significant memory effects associated with each variable, and memory effects differed for each variable. The maximal effect of the rate of change of stress was observed 8-12 ms prior to a spike.
| |
INTRODUCTION |
|---|
|
|
|---|
Mechanical sensing by
cells is a widespread phenomenon. Mechanical stimuli can evoke cellular
responses that range from channel opening (Bostel et al.
2002
; Brakemeier et al. 2002
; Zou et al. 2002
) to changes in gene expression (Ohki et al.
2002
). When mechanical stimuli are applied to tissues they can
produce very complex internal states. For example, stretching skin can
simultaneously produce tensile, compressive, and shear stresses and
strains. This makes it difficult to identify which components of stress
or strain actually stimulate a cell. Furthermore, mechanical variables
such as tensile stress and strain along a particular direction are confounded; i.e., they are related to each other through the
constitutive properties of the tissue. To determine whether a neuron is
driven by one variable versus another, it is necessary to decouple
them, i.e., to cause one variable to change independently of the other. Two strategies have been developed to accomplish this, and both have
shown that responses of mechanoreceptor neurons are associated with
stress variables rather than strain. One strategy involved the use of
biaxial stimuli to study cutaneous SA2 neurons that are highly
directionally selective (Grigg 1996
). In that
experiment, the skin was stretched along the preferred direction of an
SA2 afferent, and stress and strain along that direction were decoupled by simultaneously stretching along the orthogonal direction. Multiple correlation analysis was used to show that the neurons were
preferentially sensitive to tensile stress rather than strain along the
neuron's preferred direction. Similar experiments on receptors found
in the joint capsule have yielded similar findings (Khalsa et
al. 1996
). A second approach (Fuller et al.
1991
) utilized the viscoelastic properties of soft tissues to
decouple stress and strain variables. Dynamic stretch of viscoelastic
materials causes a phase shift between stress and strain variables,
thus decoupling those variables. Joint capsule tissue was stretched
dynamically, and conditional probability distribution
(transinformation) analysis was used to test for associations between
stimulus patterns and spike responses. It was found that
mechanoreceptor responses were more closely related to stress than to strain.
Other studies (Ge and Khalsa 2002
; Khalsa et al.
1997
; Looft 1994
; Pubols 1990
)
have applied mechanical stimuli to mechanoreceptor neurons such as SA1
and mechanical nociceptor neurons. They recorded stress and strain
variables along with neuronal responses and showed that neural
responses had a stronger linear relationship with stress than with
strain variables. In contrast, Pubols (1990)
found a
stronger relationship between neuronal responses and strain than stress.
In an earlier study from this laboratory (Del Prete and Grigg
1998
), the responses of rat cutaneous rapidly adapting (RA) afferents were studied using dynamic stretch stimuli. Associations between spikes and tensile stress and strain were sought using cross-correlation analysis. In that experiment, stress and strain were
confounded, and while cross-correlation showed a stronger association
between spikes and tensile stress than with tensile strain, it was not
possible to determine the individual effect of either variable.
The present study, similar to our earlier study in rats, was designed
to determine the mechanical sensitivity of stretch activated, RA
mechanoreceptors in mouse skin. In the present experiment, we have
applied uniaxial stretch stimuli to isolated specimens of skin
harvested from control mice, and we have recorded spike responses from
single RA afferent neurons. In this experiment, stress and strain are
decoupled from each other on a very short time scale (i.e., on the
order of milliseconds). On that time scale it was not possible to
characterize neural responses in terms of a continuous frequency
measure. Therefore standard forms of correlation analysis were not
suitable for use (Sanger 2002
). When the output variable
is binary, then the multiple correlation method of choice is multiple
logistic regression (MLR), which allows for the modeling of a binary
(dichotomous) outcome as a function of a set of candidate stimulus
variables. This method allows the determination of the independent
effect of a variable by controlling for the other variables in the
model (Hosmer and Lemeshow 1989
). Logistic regression is
widely used in clinical trials and epidemiology, applications in which
it is used to model the binary dependent variable (incidence of disease
or death) as a function of categorical and continuous variables (risk
factors). Here, we describe its use in analyzing the binary dependent
variable (spikes) as a function of a set of experimentally controlled
continuous independent variables (tensile stress and strain and their
rates of change).
| |
METHODS |
|---|
|
|
|---|
Cutaneous afferent neurons were recorded in an in vitro preparation of isolated skin and nerve that was harvested from the mouse hindlimb. Individual afferent neurons were recorded while the skin was subjected to dynamic, uniaxial stretch stimuli using a linear actuator.
Adult C57BL6 mice, of either sex, with a body mass of 20-22 g, were anesthetized with 35 mg/kg ip Nembutal. A skin specimen of approximately 10 × 6 mm was excised from the hindlimb along with a length of its associated cutaneous nerve. The geometry of the specimen and its location on the hindlimb are shown in Fig. 1A.
|
Marks were placed on the skin while it was in situ, and the distances
between the marks were noted. The specimen was removed from the leg,
and maintained in vitro in an apparatus. The apparatus (Fig. 1,
B and C) consisted of a Lucite bath filled with
HEPES-buffered artificial interstitial fluid (Koltzenburg et al.
1997
) at pH 7.40 at room temperature (20°C).
The goal was to subject the skin to uniaxial loads, while maintaining a geometry that was as close as possible to its natural (i.e., in situ) geometry. The sample was fastened in the apparatus by its edges. One end of the skin specimen was gripped in a clamp (Fig. 1, B and C) that was anchored at one end of the bath. The gripping area of the clamp extended across the width of the sample. The opposite end of the specimen was coupled to a linear actuator. The actuator was coupled to the skin by a segment of suture material with a small hook (H) at its end. The hook engaged a plastic tab (P) (5 mm × 18 mm × 0.24 mm thick) that was glued to the edge of the skin. The plastic tab served to uniformly distribute the load applied by the hook over the width of the sample, thus avoiding stress concentrations. The string, hook, and plastic tab had a total mass of 22.5 mg; minimizing the mass attached to the actuator optimized its frequency response. The sides of the skin were anchored to the sides of the chamber using two short gold chains (GC) with hooks at their ends. The hooks were engaged in holes punched in the edges of the skin. The purpose of anchoring the edges of the sample was simply to maintain the width of the sample close to the in vivo dimensions. We extended the edges until the 5 × 10 mm strip between the fixed clamp and the plastic tab (between the dashed lines in Fig. 1B) had a geometry similar to that observed in situ. Neurons were sampled only in that strip.
It was assumed that stress and strain were both uniformly distributed
throughout the part of the skin sample within which neurons were
sampled. In support of this assumption, both the clamp and the plastic
tab extended across the entire width of the sample, to avoid stress
concentrations. Neurons were not sampled within 2 mm of either the
clamp or the tab. The hooks applied to the sides of the sample were
3
mm from the area within which neurons were sampled and gave no evidence
of sustaining any significant loads.
The actuator was an Aurora Scientific 305B lever system. This is a rotary servomotor that can be operated in force control mode. An aluminum arm, 28 mm long, was clamped on the motor shaft. Operating the motor through small angular displacements resulted in an approximately linear displacement of the tip of the arm. When operated in force control mode, the actuator caused the force applied to the tissue to follow a command (input) voltage. The Aurora controller outputted voltages that were proportional to actuator displacements and to the loads applied to the specimen. Length signal resolution was 1 µm and length signal linearity was ±0.5% over a range of 20 mm. Force resolution was 1 mN (100 mg) and force linearity was 0.2% of force change. Length and force step response time was 2 ms (1 to 99% critically damped).
The experimental design was based on the hypothesis that the neurons we
studied would respond to force (stress)-related variables rather than
displacement (strain)-related variables. Thus the actuator was run in a
force-controlled mode, and tensile load was the controlled variable.
The command signal to the actuator was a band-limited (0-100 Hz)
pseudo-Gaussian noise (PGN) signal, and the system response showed
significant power at frequencies
75 Hz. There were two reasons
for using a PGN signal. First, the neurons we studied were all rapidly
adapting, so a dynamic stimulus was required to activate them. Second,
our method of analysis was based on an approach similar to reverse
correlation (Eggermont et al. 1983
), in which
associations are sought between the spikes in a data record and the
ensemble of stimuli that precedes them. In order for this approach to
work it is necessary that the stimuli before the spike have a random
structure (Eggermont et al. 1983
).
The experimental design sought to decouple tensile stress and strain.
Since skin is viscoelastic (Silver et al. 2001
), dynamic stretching induces a phase shift between stress and strain variables. We quantified the phase shift between stress and strain using a method
(Hoffman and Grigg 2002
) in which a nonlinear model of the skin is determined as a set of second-order Wiener kernels that are
calculated from experimental stress and strain data. The model was used
to predict the phase relationship between stress and strain and
revealed that, at frequencies
50 Hz, stress led strain with a
phase shift of
15°.
The cutaneous nerve was pulled into a small oil-filled chamber (Fig. 1B) and treated briefly with a solution of collagenase (Worthington, CLS-1). It was subsequently dissected into small filaments using sharpened forceps. Filaments were placed on a gold wire recording electrode. The indifferent electrode was placed in the bath. Neuronal signals were amplified with an EG&G 113 amplifier. The output of the amplifier was filtered using a Riverbend Learning Filter, which digitally subtracts noise that is in phase with line frequency. Filaments were recorded while a search stimulus (a manual stretch) was applied to the skin. Dissection of filaments was continued until a clearly identifiable single unit was recorded. Criteria for single units were the consistency of the shape and amplitude of the waveform. A software template-matching system (Signal Processing Systems, Prospect, S. Australia) was used to detect spike responses during experimental runs. This system output a voltage pulse when a spike matched an appropriate template. The pulse triggered a counter on a National Instruments MIO-16E-4 data acquisition board. Following a spike, the counter output was set to 1.0 V for the duration of the sampling period. The counter output was sampled using the A/D converter, and the counter output was reset to 0 after each sampling period. Thus a "1" was collected in each sampling period in which a spike occurred. In sampling periods during which no spikes were observed, a "0" was collected. This method assumed that the neuron never fired more than 1 spike within any 2-ms period. We verified this by separately analyzing interspike intervals (e.g., see Fig. 2). All data:analog load and displacement signals from the Aurora controller, and the output of the counter (indicating spike/no spike) were sampled at 500 Hz using the MIO-16E-4 data acquisition board. Data were written into files as they were collected. Data collection runs were typically 60 s in duration, but occasionally were as long as 300 s. Intertrial intervals were typically 5 min but were longer after long-duration runs.
|
We attempted to determine the association between mechanical variables
measured in the skin and the spike responses of single neurons. The
loads applied to the skin sample and the resulting displacements were
directly measured. Under the assumption that stresses and strains were
uniformly distributed in the skin samples, loads
(F(t)) were used to calculate tensile stress
(
), using measures of cross section area of the skin (
= F(t)/area). Cross section area was measured at
the completion of experiments by polarizing microscopy of cross
sections cut with a cryostat, as described in Hoffman and Grigg
(2002)
. Displacements (l(t)) were used to
calculate the Lagrangian strain (
) using the expression (
= [l(t)
l0]/l0).
The resulting records of stress and strain were differentiated using
the expression in the following equation to obtain their rates of
change
|
(1) |
or
, respectively.
The four variables:
, d
/dt,
, and
d
/dt as well as all of the first-order interactions
between them:
×
,
× d
/dt,
× d
/dt,
× d
/dt,
× d
/dt, and d
/dt × d
/dt
were the independent variables (predictors) in the MLR data analysis.
Our strategy in selecting the terms in the model was to have it be
parsimonious, i.e., to include all the terms of direct interest, while
excluding terms that were either not significant or not physically
interpretable. All higher-order interactions were not included for
these reasons.
Relationships between predictors and dichotomous spikes were sought
using MLR. In the section below, we describe the considerations that
are relevant to using MLR in this application. The accompanying APPENDIX presents a formal, detailed treatment of
the use of logistic regression. Basically MLR works by fitting a
regression model on the probability of the event of interest, i.e., the
dichotomous outcome. This produces a slope (
) for each predictor
variable, the antilog of which is the estimate of the effect of that
predictor after controlling for other predictors. In this application,
the independent variables are recorded values of stress, strain, and their rates of change, and the outcome is binary (dichotomous), a set
of intervals that either contain a spike or do not and are represented
by zeros and ones, respectively. A segment of a typical data file is
shown for reference in Table 1. MLR
estimates the effect of the predictors in the left hand columns of
Table 1 on the probability of a spike.
|
As with all multivariate modeling methods, MLR does not control for, nor can it estimate, the effects of variables not included in the model. In particular, this experiment contains factors that can influence the outcome but are not included in the MLR model. Specifically, after each spike, the neuron has a recovery process that includes refractory periods, which influence the likelihood of a spike in subsequent sampling periods. This means that sampling periods following a spike are not independent.
We dealt with nonindependence caused by refractory behavior by using two separate strategies.
In strategy 1 we estimated the duration of the recovery period of the neuron, and excluded from the analysis all the data collected during it. This method ensured that the data that are subjected to analysis are recorded from a fully recovered neuron and hence independent of the sampling period before it contained a spike. The details of how we used this method are described in detail in the following text.
In strategy 2 the effect of nonindependence resulting from refractory behavior is to bias estimates of the effects of independent variables toward the null, i.e., toward finding no relationship between independent variables and spikes. For example, logistic regression estimates the effect of the predictors on the binary (0/1) outcome measure. At issue is that some of the zeros that are recorded might have been ones were it not for the effect of the neuronal refractory period. This results in reducing the strength of association between the predictors and the outcome and thus biases the result of the analysis against finding associations. Thus our strategy in this case was to take the data, as collected, and subject it to analysis using MLR.
To analyze results collected when the neurons were in a fully recovered
state, i.e., (strategy 1), we used published values (100 ms) for the
duration of the recovery period, including the subnormal and
supernormal periods, that follows each spike (McIntyre et al.
2002
). This is an extremely conservative estimate of neuronal recovery, since the excitability changes in the sub- and supernormal periods are small (McIntyre et al. 2002
). We selected
for analysis only those spikes that were preceded by 100 ms that were
free of spike responses. This ensured that the neuron was fully
recovered when a spike occurred.
Another strategy was to account for the effects of refractory periods
but not the supernormal and subnormal periods. To this end, we directly
measured the duration of refractory periods and excluded from analysis
all data collected when the neuron was refractory. The duration of the
refractory period was measured using a "hazard function"
(Gray 1967
). To create a hazard function, cutaneous RA
afferents were recorded while the skin was mechanically stimulated by
indenting it using a continuous, random input with a bandwidth of
0-100 Hz. The indentation stimulus activated cutaneous afferent
neurons that were typical of those that we describe under RESULTS. It is assumed that the stimulus will elicit spike
responses at all possible interspike intervals. The hazard function
(Fig. 2) is the conditional probability of observing a response at
different intervals between spikes. Six neurons were studied in this
fashion. The conditional probability of observing spikes reached a
plateau after 18 ms and remained constant thereafter (Fig. 2). Thus,
after 18 ms, a second spike is independent of the effects of a prior spike.
In summary, in those analyses in which we desired to obtain a totally unbiased estimate of the dependencies between predictors and spikes, we analyzed only those spikes that were preceded by 100 ms of zeros (i.e., no spikes). In analyses in which we wished to obtain a largely unbiased estimate of stimulus-response dependencies, we excluded data collected during the refractory period, i.e., for 18 ms after each spike. This latter strategy ensured that the outcomes that we analyzed represented the properties of a neuron in a largely recovered state; i.e., it ignored only the super- and subnormal periods. In other analyses we ignored the effects of recovery processes and included all data. The advantages and disadvantages of these analysis strategies are described in detail under DISCUSSION.
A reverse correlation design allows for the determination of system
memory. In the present experimental design, where sampling periods make
up a regular sequence (i.e., a time series), a stimulus presented
during a particular sampling period can influence the likelihood of a
response in a subsequent sampling period. This is an important
phenomenon known as system memory, in which an input variable at one
point in time has an effect on the probability of a spike occurring at
some point later in time. This can be determined for some memory time
t by subtracting the constant time t from the
time of occurrence of each spike in the data record, so as to create a
dummy output variable, which is termed "Lag" (Table 1). Shifting
the spikes up by one sampling period (i.e., Lag 2, Table 1) and then
performing MLR analysis on the resulting file effectively determines
whether there are any dependencies between stimuli in one sampling
period and a response in a subsequent sampling period. We used this
approach, known as lag analysis, to quantify memory. Dependencies were
determined between outcome responses and stimuli that preceded them by
50 ms.
In logistic regression, the strength of association between a stimulus
variable and the output variable is expressed in terms of an "odds
ratio." Odds ratios are tied to the units of the input variable and
represent the probability of the outcome event (i.e., the probability
of a spike response) that is associated with a one-unit change in a
predictor variable. In our experimental design, the input variables
(stress, strain, and their time derivatives) all have different units.
For example, stress is expressed in units of kPa, while
d
/dt has units of kPa/s. Similarly, the units of stress
and strain are different. For this reason, the odds ratios of our
predictor variables are not comparable in a direct and intuitive way.
We dealt with this problem by expressing magnitudes of stimuli as
normalized variables (i.e., standardized variables) (Steel and
Torrie 1981
), by subtracting the mean and dividing by the SD.
All predictors were approximately Gaussian in distribution, and the
resulting normalized variables had means = 0 and SD = 1. Values of odds ratios, calculated from these normalized data, were then
comparable inasmuch as they represented the probability of a spike,
associated with a change of 1 SD in the magnitude of the particular
variable. This allowed all four normalized variables to be represented
on the same nondimensional x-axis. Furthermore, interactions
terms, which are functions of two or more variables, are all
dimensionally reduced to functions of one variable, the SD.
All logistic regression analyses were run using SPSS version 9.0.
| |
RESULTS |
|---|
|
|
|---|
Thirty neurons were recorded in seven successful experiments.
Neurons were studied using PGN stimuli whose magnitude ranged from 1 to
120 kPa and had mean values of
40 kPa. These stresses resulted in
strains that ranged from 0.01 to 0.37. Typical stimuli, used for
studying all neurons, had magnitudes that ranged from 1 to 40 kPa, with
a mean value of about 20 kPa. In these runs, strains ranged from 0.01 to 0.13 with a mean value of 0.07. Figure 3 shows an example of raw (Fig.
3A) and normalized (Fig. 3, B and C)
data recorded from one neuron. As can be seen, spikes were relatively
sparse in these records. The number of spikes recorded in a 120-s
collection run ranged from 100 to as many as 1,000. The number of
spikes evoked by a particular PGN stimulus sequence increased with the
magnitude and bandwidth of the stimulus.
|
Figure 4 shows histograms of the spike
responses (black histograms) observed in a single run plotted versus
the distributions of the four main factors in the experiment (colored
histograms). Spikes were associated with a wide range of values of
and
and were associated primarily with large values of
d
/dt and d
/dt. It is important to note that
the histograms in Fig. 4 illustrate raw relationships, inasmuch as they
do not account for covariance between inputs. For example, similar
relationships are observed between
and
and between
d
/dt and d
/dt. These variables covary in
this experiment, and the representation in Fig. 4 does not allow for
the determination of the relative contributions made by (for example)
d
/dt and d
/dt. This question requires the
use of a multivariate method of analysis, for which we used MLR.
|
Normalized data were subjected to analysis with MLR. The logistic
regression analysis yielded a
value for each factor in the model
(see APPENDIX). The anti-log of the
values,
= e
, was used to calculate an
estimate of the odds ratio for each factor. Table
2 is an example of SPSS output including
odds ratios determined in a typical data run for one neuron.
|
It should be noted that the results in Table 2 reflect the association
between the spike responses and the input variables measured in the
same sampling period, i.e., when there is no memory. Memory effects
were explored by performing logistic regression analysis using the
offset (lag) spikes. We systematically varied the lag time from 0 to 50 ms in 2-ms increments and performed logistic regression analysis for
each lag time. The resulting
values were used to calculate odds
ratios for all the factors at each memory time. These are shown for one
neuron, based on analysis using strategy 1 (see METHODS) in
Fig. 5.
|
In the analysis depicted in Fig. 5, there were four variables with
significant effects on spikes: d
/dt,
,
d
/dt, and the interaction d
/dt ×
.
These variables had their effects at different memory times. There was
no effect of
in this (or for that matter in any) neuron. The
variable with the largest odds ratio was d
/dt, at a
memory time of 10 ms. The time at which the peak odds ratio was
observed for d
/dt varied between 8 and 12 ms between
different neurons and even between different runs for a single neuron.
The odds ratios for the interaction terms, while significant, were always small. None of the other interaction terms was significant. Odds
ratios were somewhat variable between different runs for a particular
neuron and between different neurons. This neuron was typical of the
whole sample in that d
/dt at a memory time of 10 ms was
most strongly associated with spikes.
Logistic regression analysis makes the assumption that outcomes are independent of each other. We ensured that this assumption was satisfied in the analysis of Fig. 5, by only including data in which spikes were preceded by 100 ms of silence. However, this strategy necessitated the exclusion of data from the analysis. To determine how great an effect was caused by the exclusion of data, we used data from a sample neuron and analyzed it using three strategies (outlined under METHODS). Two of three strategies involved eliminating different amounts of data, and one strategy was based on using all data. Results of these analyses are shown in Fig. 6. The results in Fig. 6A are based on analysis similar to that used for Fig. 5; namely, the only spikes that were included were those preceded by 100 ms with no spike activity. Figure 6B is based on analysis of all data except for data recorded when the neuron was refractory. To perform this analysis we excluded from analysis all data collected for 18 ms after each spike. The final strategy was to include all data (i.e., exclude nothing) in the analysis (Fig. 6C). Analysis based on this strategy yielded lower values for odds ratios.
|
To demonstrate the degree of consistency of response within one neuron, the neuron depicted in Fig. 6 was studied in nine different runs employing a variety of frequency bandwidths and stimulus amplitudes. All analyses were done following strategy 2, after removing refractory data (as in Fig. 6B). The odds ratios from all these runs were averaged together (Fig. 7); the error bars indicate the degree of consistency of the response within a single neuron.
|
To summarize the properties of the population of afferents and to show the consistency of response between afferents, we combined data from all neurons that were sampled (Fig. 8). When there were multiple runs for a single neuron, the odds ratios for those runs were averaged together as in Fig. 7. This provided the best estimate of the properties of each neuron. The resulting odds ratios for all (n = 30) individual neurons were then averaged together to create Fig. 8. It is important to note that the data that make up Fig. 8 were collected in different neurons, using stimuli of different magnitudes and with different bandwidths. All odds ratios were calculated using data that excluded refractory data. Thus this figure yields the best estimate of the relationship between stimuli and spike responses in these experiments.
|
To demonstrate the validity of the logistic regression analysis we used the following two methods:
1) Randomizing spikes. We wished to demonstrate that the
effects seen in the preceding figures (Figs. 5-7) represented the
association between the input variables and the spikes, rather than
being due to some unspecified process. Therefore we performed logistic regression analysis on the data set of Fig. 6 after randomizing (i.e.,
shuffling) the locations of spikes in the data file (Hung et al.
2002
). Results of this analysis are shown in Fig.
9. The analysis of randomized spikes
yielded an odds ratio for each factor in the analysis that was not
different from 1.0, which is the value expected when there is no
relationship between the input and output variables.
|
2) Predicting spikes based on the logistic regression model.
One way of validating a model is testing whether it can predict the
occurrence of spikes in other sets of data collected under similar
conditions. Since the odds ratios represent the change in the
probability of a spike caused by a particular stimulus, it was possible
to estimate the likelihood of observing a spike associated with
particular stimulus values. We made a prediction model based on the
odds ratios for a particular data set and used that model to predict
the occurrence of spikes in three different cases: predicting the
original data set, predicting randomized (shuffled) spikes, and
predicting spikes in another data set from another neuron. We used the
receiver operating characteristic (ROC) curve (Hanley
1989
) to quantify the goodness of the prediction in these three
cases (Fig. 10). The ROC curve shows
how the true prediction rate (the sensitivity) of a model relates to
the false-positive rate (100
specificity) predicted by the
model, as the prediction criterion value (cut point) is changed. If a
model has no predictive value, then, as the prediction criterion is
changed, correct predictions and false predictions are equally likely.
Hence a model with no predictive value is represented by the diagonal
line in the ROC curve.
|
The goodness with which a model makes predictions is quantified by the area under the ROC curve. The lack of any relationship is indicated by an area of 0.5, perfect predictions by an area of 1.0, and perfect incorrect prediction by an area of 0. The results of the ROC analyses are shown in Table 3.
|
| |
DISCUSSION |
|---|
|
|
|---|
The main goal of the experiment was to determine what components
of the mechanical stimulus were responsible for eliciting spike
responses. Mouse cutaneous RAs were shown to have a strong association
with the rate at which stress varies, d
/dt. However, there were also significant influences of
and d
/dt.
That neural responses were mainly driven by dynamic components of the
stimulus (i.e., d
/dt and d
/dt) was not
unexpected since the sample population consisted of RA afferents. Of
the two interaction terms that were significant, one
(d
/dt ×
) is proportional to the incremental area under the stress-strain curve and thus reflects strain energy. The odds ratio for this term was always small, indicating that, unlike
other systems (Grigg and Hoffman 1984
; Khalsa et
al. 1996
; Srinivasan and Dandekar 1996
), strain
energy does not appear to be an important determinant of the response
of these neurons. The fact that d
/dt ×
was
significant means that, similar to other afferents (Houk et al.
1981
; Rogers et al. 1996
), the effect of
d
/dt was dependent on the absolute value of
.
There were strong memory effects for all of the variables that were
associated with spike responses. The variable d
/dt, which had the strongest association with neural responses, had its maximal association with spike responses at a memory time of 8-12 ms; i.e.,
there was a delay of 8-12 ms between the stimulus and the response it
evoked. Memory associated with other variables had different time courses.
The presence of memory effects raises the question as to their origin.
Part of memory reflects time required for generator currents to reach
threshold and for sufficient current to accumulate for the initiation
of a spike. However, accumulation time has been estimated to be 0 ms in
muscle spindles (Schafer et al. 1999
) and would in any
event be expected to be very small in RA afferents. Conduction time
along the axon is also included in memory time. However, conduction
time is relatively short in these small preparations, in which the
distance from skin to electrode is usually 10 mm or less. Even at the
low (20°C) temperature at which the experiments were conducted, the
conduction time was still on the order of 1 ms. Since skin is a
fiber-reinforced composite material, memory time may be required for
reorientation of tissue constituents with load. However, it is still
unclear why different variables such as d
/dt,
, and
d
/dt would have their effects at different memory times.
Memory effects are an example of phenomena that may be illuminated by
experiments using mutant and gene-targeted mice that have altered skin
mechanical phenotypes.
While we have described the use of MLR for the analysis of responses of
RA afferents, we note that it can be used in the analysis of any system
in which spikes are the output. We (unpublished observations) have
applied MLR to previously published data (Fuller et al.
1991
) in which slowly adapting mechanoreceptors in cat knee
joint were studied with a PGN stretch stimulus. MLR revealed a
significant association with stress, similar to the results reported by
Fuller et al. (1991)
using transinformation analysis.
There are many aspects of these findings that remain unclear. It is widely but uncritically accepted that mechanically sensitive channels are activated by molecular deformations (i.e., strains). Yet it is not clear through what mechanism macroscopic stress can be coupled to neuronal activation, to the exclusion of macroscopic strain. It is hoped that further studies on mechanoreceptor neurons can elucidate these problems.
Logistic regression analysis presents both some potential problems and some palpable strengths in analysis of data from this experiment. Neuronal recovery periods pose the potential problem. A spike in a neuron is followed by a recovery period during which the neuron's excitability is altered: it is depressed during refractory periods and the subnormal period and is enhanced during the supernormal period. This means that there are times when outcome events are not independent of each other. This violates the assumption, commonly made in MLR, that outcome events are independent of each other.
It is possible to avoid violating this assumption by selecting data for
analysis. One way is to perform MLR analysis using only data that were
recorded when the neuron was in a fully recovered state. Since the
duration of the sub- and supernormal periods is on the order of 100 ms
(McIntyre et al. 2002
), this strategy involved including
in the analysis only those spikes that were preceded by
100 ms with
no spike responses. A typical data file contained large numbers of such
intervals. The data of Fig. 3 illustrate one such interval, prior to
the first spike in the figure. By analyzing only these data, we ensured
that both the refractory periods and the sub- and supernormal periods
from a preceding spike were completely finished when the next spike was elicited. The strength of this method is that it yields an unbiased estimate of the association between predictors and spikes. The downside
is that it is necessary to exclude data from analysis, and it limits
the characterization of neurons to effective frequencies of 10 Hz or
less. Analyses done in this fashion revealed a strong relationship
between d
/dt and spike responses, with the maximal memory
effect for d
/dt at around 10 ms.
A second way of analyzing the data involved excluding only the data
collected during the refractory periods (i.e., for 18 ms following each
spike). The rationale was that 1) we were able to measure
the duration of the refractory period, and 2) excitability changes during the sub- and supernormal periods are relatively small,
so that their effect on spike responses would be correspondingly small.
These analyses included data sampled when the recovery of the neuron
was complete except for any effect of subnormal and supernormal
periods. With this analysis strategy, the trade-off described in the
prior paragraph is somewhat different. Any effect of the subnormal and
supernormal periods is not accounted for, but, on the other hand, the
characterization of the neuron is now based on effective frequencies of
55 Hz. Importantly, these analyses yielded results that were
identical to those excluding sub- and supernormal periods, i.e., the
strongest association was with d
/dt, at a memory time of
about 10 ms.
A third way of analyzing the data was to include all data, including
those collected immediately following spike responses, in the analysis.
This means that there are instances in the data in which a
suprathreshold stimulus fails to elicit a spike because the neuron is
refractory. The stimulus will be associated with a "0" rather than
a "1" response, and this will lower the odds ratios for the
predictors. As above, a trade-off is still involved. In this case, an
additional factor-refractory behavior-is unaccounted for in the
analysis, while the characterization of the neuron is based on data
that impose no limitations of the frequency of neuronal response. These
analyses revealed that the association between stimuli and spikes was
highly similar to those seen in the analyses described above: the
strongest association was still with d
/dt, and the
maximal effect was seen at a memory time of 8-10 ms. The odds ratios
obtained in these analyses were smaller than those from the previous
analyses but were nonetheless highly significant. It should also be
noted that, while the effective neuronal frequency differs in these
strategies, the stimulus bandwidth is the same in all cases since this
refers to the stimuli during the period prior to the spikes.
Since there were differences in odds ratios measured with these
strategies, it is of interest to show the validity of the odds ratios.
The MLR method was validated with a prediction model that was based on
the odds ratios from the all-data analyses, which yielded the smallest
estimates of odds ratios. The prediction model was used to predict
spikes in either the same or different data sets. The prediction model
was very successful in predicting the actual spikes in experimental
data files, as evidenced by the ROC analyses. Thus, while our method of
analysis may violate an assumption that is commonly made in MLR, it
does not appear to substantially alter the effectiveness of the method
in our application. Furthermore, other studies have routinely used
nonrecovered neurons in experiments in which stimulus-response
relationships are characterized. Any study in which the responses of
cutaneous RA afferents are characterized using stimuli with a frequency content > 55 Hz (Gescheider et al. 2001
) is using
nonrecovered neurons.
While there are some limitations (discussed above) on the use of MLR in
this application, there are some important advantages to its use. It is
a powerful tool for dealing with data such as ours, in which binary
spike events are related to continuous predictor variables. By using
logistic regression, we avoid longstanding problems associated with
attempts to analyze spike train data using standard correlation
methods. In particular, logistic regression allows us to treat spikes
as discrete events (Victor and Purpura 1997
) rather than
transforming a series of discrete events into frequency values (see
Sanger 2002
). It is not necessary to assume that there
is a linear relationship between predictors and outcomes. In addition,
as a multivariate method, it allows for determining the effect of
individual variables that may be confounded, as well as of interactions
between them.
MLR quantifies the strength of association between an input variable
and the outcome variable in terms of odds ratios. An odds ratio relates
the likelihood of observing the outcome variable in terms of the units
of the predictor variable. A conceptually simple example involves the
association between the effect of smoking, in packs per day, on heart
disease. An odds ratio of 1.5 means that smoking 2 packs per day makes
heart disease 1.5 times more likely than smoking 1 pack per day. In the
present experiment, stimulus magnitudes were normalized to have a
mean = 0 and a SD of 1.0. Thus an odds ratio of 30 for
d
/dt means that a stimulus that is 1 SD unit greater than
the mean is 30 times more likely to elicit a spike than a stimulus
whose magnitude is equal to the mean. The absolute values of odds
ratios can vary for several reasons, including the amount of data in
the data set, the ratio of spikes to no spikes, and the presence of any unmeasured or uncontrolled predictors. Differences in odds ratios can
be quite important when, as in Fig. 5, components of a particular data
set are included in or excluded from the analysis. But, in general, the
magnitudes of odds ratios should be interpreted with some caution.
There are important guidelines for using MLR in applications such as
this. Most important is that the stimulus must have a random structure.
This is a requirement for any experimental design using reverse
correlation (Eggermont et al. 1983
). A random structure allows for all possible combinations of predictors to occur prior to a
spike. We accomplished this by using a PGN stimulus. The use of a PGN
input was also useful in that it allowed for expressing the magnitude
of stimuli in units of SDs. This made it possible to make comparisons
of the odds ratios for different predictors and interaction terms.
| |
APPENDIX |
|---|
|
|
|---|
is the
predicted value for the outcome and
x1, ... , xk are
values for k different predictor values, a linear regression
model for y for subject i might be:
i =
0 +
1x1 + ... +
kxk where
0 is the intercept and
1,
2, ... ,
k are the
effects of the k different predictor variables for one unit
of change in the predictor. Other ways to describe this are that
is the conditional mean for y
conditioning on x1, ... ,
xk or the expected value of y given x1, ... , xk, in
mathematical notation:
= E(y|
), where
is the vector x1, ... ,
xk. When outcomes are dichotomous it is
convenient to model them with dummy values of 1 when the outcome of
interest occurs and 0 otherwise. Conditional means of dichotomous
variables coded this way are then constrained to be between 0 and 1 in
a way similar to cumulative probability distributions. One cumulative probability distribution, the logistic distribution, lends itself particularly well to the modeling of dichotomous variables because it
is flexible and easy to use and also because its use lends itself to
biological interpretation (Hosmer and Lemeshow 1989
0,
1 are the regression coefficients (Hosmer and Lemeshow 1989
|
(A1) |
(x) represents the expected value for
y constrained between 0 and 1 or, equivalently, the
conditional mean of y given x, and where
x is the predictor or factor. However the "logit" transformation
|
(A2) |

to +
, properties that lend themselves to regression models.
Estimates of the coefficients
0 and
1 are made by fitting the model to the
experimental data using maximum likelihood estimation (Kleinbaum
et al. 1988
(x) of these coefficients, which is interpretable as an
estimate of the "odds ratio" for the factor x
|
(A3) |
|
(A4) |
is the vector of all the
physiologically meaningful factors listed above.
Since we had six interaction terms in our model, the expressions that
were used for calculating odds ratios were
|
(A5) |
|
(A6) |
|
(A7) |
|
(A8) |

is a function of three variables,
, 

| |
ACKNOWLEDGMENTS |
|---|
We thank S. Liberman for writing programs and P. Tilander and D. Robichaud for technical assistance.
This work was supported by National Institute of Neurological Disorders and Stroke Grant NS-10783.
| |
FOOTNOTES |
|---|
Address for reprint requests: P. Grigg, Department of Physiology, Room S4-245, University of Massachusetts Medical School, 55 Lake Avenue, Worcester MA 01655 (E-mail: Peter.Grigg{at}umassmed.edu).
| |
REFERENCES |
|---|
|
< |
|---|