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1 Departments of Pediatrics, and Neurology and Neurosurgery, McGill University and the Neuropeptide Physiology Laboratory, McGill University-Montreal Children's Hospital Research Institute, Montreal, Quebec, Canada H3H 1P3; and 2 Department of Biological Chemistry, Weizmann Institute of Science, Rehovot, Israel 76100
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ABSTRACT |
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Growth hormone (GH) induces growth in animals and humans and also has important metabolic functions. The GH neuroendocrine axis consists of a signaling cascade from the hypothalamus to the pituitary, the liver, and peripheral tissues, including two major feedback mechanisms. GH is secreted from the pituitary into the circulating blood according to the effect on the somatotrophs of two hypothalamic peptides, GH-releasing hormone (GHRH) and its antagonist, somatostatin (SRIF). The typical GH profile in the male rat shows secretory episodes every 3.3 h, which are subdivided into two peaks. Focusing on the mechanisms for generation of this ultradian GH rhythm, we simulated the time course of GH secretion under a variety of conditions. The model that we propose is based on feedback of GH on its own release mediated both by GH receptors on SRIF neurons in the brain and by a delayed SRIF release into both the brain and portal blood. SRIF, with a resultant periodicity of 3.3 h, affects both the somatotroph cells in the pituitary and the GHRH neurons in the hypothalamus. The secretion of GHRH is postulated to occur in an ~1-h rhythm modulated by the level of SRIF in the hypothalamus. The model predicts a possible mechanism for the feminization of the male GH rhythm by sex steroids and vice versa, and suggests experiments that might reveal the proposed intrinsic 1-h GHRH rhythm.
somatostatin; growth hormone-releasing hormone; hypothalamus; growth hormone receptor; mathematical model
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INTRODUCTION |
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GROWTH HORMONE (GH) is secreted in a pulsatile manner from the pituitary gland, resulting in an oscillating time course of GH concentration in the circulating blood. In the adult male rat, the regular time course of GH is characterized by biphasic secretion episodes every 3.3 h separated by intervening trough periods with undetectable basal levels (39). The secretion is governed by the two hypothalamic neuropeptides, GH-releasing hormone (GHRH) and somatostatin (SRIF), which have stimulatory and inhibitory effects, respectively, on GH release. SRIF neurons are located in the periventricular nucleus (PVN), as well as in the arcuate nucleus (ARC), of the hypothalamus, whereas GHRH cells predominantly reside in the ARC. The axons of these neurons course to the median eminence where they release the neurohormones into the portal blood. GH exerts a negative feedback on its own secretion at the level of the hypothalamus by regulating the secretion of SRIF (short loop feedback). In the liver, GH regulates the secretion of insulin-like growth factors (IGF-I and IGF-II), which exert growth-promoting effects in peripheral tissues; IGF-I and IGF-II constitute the long loop feedback of the GH neuroendocrine axis by suppressing GH release at the level of the pituitary and/or hypothalamus (for reviews, see Refs. 14 and 35).
Although many experiments were performed to elucidate the interrelationship between SRIF and GHRH in GH regulation, the mechanisms underlying normal pulsatile GH secretion remain obscure. Chen et al. (10) derived an elaborate model involving eight differential equations and five arbitrary feedback functions, which was too complex to explain the actual function of the system. We address the problem using a model that focuses on the generation of the 3.3-h rhythm of GH secretion. Due to the time scale examined, short-term alterations were assumed to be in pseudoequilibrium with the relevant variables, whereas long-term effects were treated as constants. This allows us to propose a model of the ultradian rhythm of GH secretion using only two differential equations: one for GH and one for SRIF. GHRH is assumed to be generated independently of GH and possesses an intrinsic rhythm with a mean period of ~1 h. We found that the major feedback mechanism for generation of the 3.3-h rhythm is the short feedback loop via SRIF. The release of SRIF due to GH is delayed, which reflects the kinetics of the signaling pathway in these cells. SRIF, with a resultant periodicity of 3.3 h, affects both the somatotroph cells in the pituitary and the GHRH neurons in the hypothalamus. The inclusion of two sites of SRIF action in this model resolves experimental results that have so far eluded explanation. The model also predicts a possible mechanism for the change of the male GH rhythm into the female pattern by sex steroids and vice versa, and it suggests experiments that might reveal the proposed intrinsic 1-h GHRH rhythm.
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METHODS |
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Basis of the Model
Pituitary GH secretion. The interrelationship of SRIF and GHRH in GH regulation at the level of the pituitary was investigated using an adult rat model. From these experiments, Tannenbaum and Ling (38) postulated that SRIF and GHRH are released in reciprocal 3- to 4-h cycles from the hypothalamus into the hypophyseal portal blood to generate the ultradian GH rhythm. These conclusions were corroborated by measuring the concentrations of immunoreactive GHRH and SRIF in hypophyseal portal plasma (30). Our model is based on these well-established findings.
GH feedback via SRIF. GH given centrally (34) or peripherally (44) suppresses the spontaneous bursts of GH in the rat. Experimental evidence indicates that the feedback effect of GH on its own secretion is exerted by increasing hypothalamic SRIF release into the portal blood (11). In vitro studies show that the pituitary gland is not the site of GH feedback inhibition (20). The GH feedback effect also results in a high-frequency pulse train of GH (~1 h), unmasked by injecting SRIF antibody (Ab) after GH treatment (21), suggesting that the GH rhythm is generated by an intrinsic high-frequency (~1 h) GHRH release.
Mediation of GH feedback by GH receptors on SRIF cells. GH receptor (GHR) transcripts have been found to colocalize with SRIF transcripts in the PVN (5). Because there is experimental evidence that GH does not affect GHRH cells in the ARC (25), we assume that the feedback of GH is mediated via GHR on SRIF neurons. The binding of GH to its receptor results in a dimerization of GHR and activates a variety of signaling molecules (7). Central injection of GH increases SRIF release into portal blood with a delay of 40-80 min (11), which is determined by the above-mentioned signaling cascade. In the simulations, we used a generally accepted model for the GHR turnover (1, 16).
Further mediation of GH feedback by SRIF receptors in brain. Evidence has been provided for the association of SRIF receptors with a subpopulation of GHRH-containing ARC neurons (3, 23, 41), implying direct regulation of the GHRH hypothalamo-hypophyseal system by SRIF. In addition, ultradian oscillation in SRIF binding within the ARC in synchrony with the pattern of GH secretion has been shown (36). These results suggest that the feedback of GH on GHRH neurons in the ARC is mediated via SRIF, at least on the timescale of a secretion episode.
Long loop feedback involving IGFs. Although there is convincing in vitro evidence that the IGFs affect GH secretion (2), the effect of the IGFs in vivo is still poorly understood. At the level of the brain, it appears that a synergistic interaction of IGF-I and IGF-II is required to reduce the amplitude of GH pulses 2-3 h after injection (15). Furthermore, no modification of plasma IGF-I levels was observed after acute or chronic GH administration (21), indicating that GH-induced negative feedback can operate independently of changes in IGF-I. We assume that the IGFs are involved in a feedback loop but that it is not essential for generation of the 3.3-h rhythm of GH.
Male-female dimorphism. In adult rats, there is a striking sex difference in the pulsatile pattern of GH secretion. In contrast to the regular 3.3-h periodicity in the male, females exhibit more frequent, irregular, low-amplitude GH pulses with an elevated baseline (see Ref. 19 for review). The level of GHR in the liver is lower in males than in females (31). It has been postulated that, in the female rat, SRIF release into portal blood is continuous, whereas GHRH release is erratic with a high frequency (12, 27). Administration of the female sex steroid estradiol to male rats converts the male GH rhythm to a female-like pattern (28), whereas, conversely, the male sex steroid testosterone masculinizes the female GH secretory profile (35). Because the high-frequency pattern of GH secretion is observed in the female rat, we used the transition between the male and female GH profiles to justify the assumed intrinsic 1-h rhythm of GHRH in the male rat.
GH secretagogues. A novel class of synthetic compounds with potent GH-releasing activity, termed GH secretagogues (GHSs), has been described (4, 33). The cellular mechanisms involved in the actions of GHSs are different from those of GHRH (33). A receptor for GHS (GHS-R) has been cloned recently (18), and there is anatomic evidence that the GHS-R is expressed by GHRH neurons (37), suggesting that an additional neuroendocrine pathway may exist to regulate pulsatile GH secretion. However, the endogenous ligand for GHS-R has not, as yet, been identified. Thus GHS is not included in the model.
Description of the Model
Mathematical implementation. The scheme of the model used for the simulation is presented in Fig. 1. The numbering convention refers to SRIF as species 1, GHRH as species 2, GH as species 3, and GH receptors as species 4. The symbol A refers to the hypothalamus, B to the portal blood or pituitary, and C to the circulation. Concentrations are denoted by c, with an appropriate subscript to indicate the species and superscript to indicate the zone. All concentrations are time dependent, unless they are doubly subscripted, in which case they are parameters of the model with assigned values (see Table 1).
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(1) |
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(2) |
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(3) |
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(4) |
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(5) |
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(6) |
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(7) |
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(8) |
and
are receptor functions, and
k4,i, k4,ri, and
k4,d are the rate constants for internalization,
reinsertion of GHR, and dissociation of GH, respectively. The binding
constant is denoted by Ka, and c4,tot
is the total amount of GHR in the hypothalamus. For the male and female
parameter sets, the dependence of internalized receptors on GH
normalized by c4,tot is shown in Fig. 2, inset.
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with respect to
the concentration of internalized receptors (11, 34). Furthermore,
is taken to represent the sum of all delays in the GH feedback loop
(26); including the fast clearance observed for SRIF, its time course
is given by
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(9) |
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(10) |
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(11) |
denotes the partition coefficient.
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RESULTS |
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Simulations and Comparisons with Experiments
Calculations. Simulations of time-dependent concentrations of SRIF, GHRH, and GH were performed using the Euler algorithm with a time step of 0.01 min. Figures 3-6 do not show the initial transient, and the zero point of the time window presented was shifted to match the experimental conditions. Note that the two differential equations describe a "limit cycle," which is independent of initial conditions after the initial transient.
Parameters. The differential equation system was calibrated in such a way that the simulated concentrations are comparable to measured values. Hence the release rate constants are given in nanograms per milliliter per minute for GH and picograms per milliliter per minute for SRIF. They were chosen to reproduce physiological concentrations. In contrast, the clearance rate constants were calculated according to the measured half-life. For GH, we used a half-life of 8-10 min (9), and, for SRIF, we used a value of 0.5 min (10). The amplitude variation of GHRH and the maximal amount of SRIF in the portal blood correspond to experimental findings (30).
The generation of the GHRH pulse train requires the parameters T, the distance between two pulses, and T1, the duration of secretion. To estimate these parameters, we performed a time series analysis of typical normal GH profiles of six different rats with two secretion episodes each. It revealed a periodicity of the GH secretory episodes of 201 ± 11 min, and if the secretion period was composed of two consecutive GH pulses the peak-to-peak distance was found to be 59 ± 15 min. The periodicity T was adjusted to 50 min to simulate the 3.3-h (200 min) rhythm of the GH profile. The time of increasing GH concentration was considered to be due to secretion events. Thus we obtained a secretion time period of 20 ± 9 min for the first peak and 21 ± 7 min for the second peak. In accordance with the time series analysis, a secretion duration of T1 = 20 min was used. This value was corroborated using the deconvolution algorithm developed by Veldhuis et al. (42) on five GH profiles (data not shown). The delay between the increase of GH in the brain and the rise of SRIF in the portal circulation,
, was estimated by several authors (11,
34, 44) to lie within 40-80 min. The value
= 62 min imposed on
the feedback in the simulation was chosen such that, first, at low
levels of SRIF, the secretion of GH is induced by more than one GHRH
pulse (
> 50 min) and, second, on increasing levels of SRIF, the
second pulse of GHRH is cut off, resulting in a lower GH peak amplitude
(
< 70 min).
The Hill coefficient n3 (Eq. 5) was
determined by fitting a Hill function to an experimental data set (24)
that shows the GH response curve induced by different amounts of GHRH.
This yielded a Hill coefficient of approximately two. SRIF acts via a
similar second messenger mechanism on the somatotrophs, leading to the assumption of equal Hill coefficients of the two neuropeptides at the
pituitary (n2 = 2). The dense network of SRIF
neurons in the ARC suggests a high degree of cooperativity and is
represented in the simulation by a Hill coefficient
n1 = 4. If the value of n1 is
less than four, adequate suppression of GHRH release by SRIF cannot be attained.
The thresholds and the two parameters of the receptor function were
chosen arbitrarily to fit experimental data. The partition coefficient
lies between zero and one. A summary of the parameter values used
is given in Table 1. An examination of the
sensitivity of the system to the parameter values showed that it is
insensitive to small changes in all of the parameters shown in Table 1
except the Hill functions (provided that the constraints on the time constants are fulfilled). However, increasing the Hill coefficients decreases the sensitivity to the thresholds.
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Unperturbed GH rhythm. The simulated time courses of the unperturbed SRIF, GHRH, and GH rhythms in the male rat compared with experimental GH data are presented in Fig. 3. The simulated GH bursts exhibit a periodicity of 3.3 h, and each burst is subdivided into two GH pulses separated by 50 min. The duration of the nadir period is ~90 min with almost undetectable GH levels.
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Perturbation by exogenous GHRH. The male rat shows a synchronized GH rhythm so that administration of exogenous GHRH during a GH secretory episode results in an amplified GH peak, whereas during a trough period the response is negligible (38). Injections of GHRH were modeled, and the simulations as well as the experimental result are presented in Fig. 4. The model shows two high GH peaks at 1100 and 1500 (Fig. 4C). The suppression of the GH response to GHRH at 1300, due to the high level of SRIF, fits well with the experimental data. The extended tail of GH secretion after the peak at 1100 and the increased level of GH preceding the peak at 1500 are due to endogenous pulses of GHRH.
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Perturbation by human GH. By administering exogenous human (h) GH, the periodicity of endogenous rat GH can be changed reproducibly. The response due to hGH perturbation is a suppression of the GH pulses and a prolongation of the GH trough period by ~1.5 h (21). The effects of the GH negative feedback loop are presented in Fig. 5. The injection of hGH at 0800 results in a shift of the spontaneous GH burst, which appears at ~1230 (Fig. 5, C and D). In addition, the GH peak amplitudes are often reduced while the system returns to the normal rhythm (21). The change in periodicity is not due to the high peak amplitude of hGH (~400 ng/ml) but to the slower decay of hGH in the circulating blood. This causes a long tail in the SRIF surge (Fig. 5A) that suppresses GH pulses for 1.5 h. The elevated SRIF level in the recovery phase of GH reduces the GHRH pulses and diminishes the amplitude of GH secretion.
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Feminizing the male rhythm.
Despite the different GH periodicities in male (3.3 h) and female (~1
h) rats, the regulatory mechanisms (Fig. 1) are probably the same since
the ~1-h rhythm of the female can be detected within the GH secretory
episode of the male. The transformation of a male GH profile into a
female profile is presented in Fig. 6. By
introducing a 1,000-fold increase in the product
c4,tot,
to make the receptor function almost independent of GH (see
APPENDIX), and by increasing the ratio
to eight (see
Table 1), which adjusts the SRIF level (see APPENDIX), the
simulations exhibit a GH profile similar to that observed in the
feminized male rat (28). According to the simulations, the feminized GH
rhythm is generated by an almost constant release of SRIF into the
hypothalamus (Fig. 6A), where it reduces the GHRH peak
amplitudes, and into the portal circulation, resulting in partly sealed
somatotrophs. Consequently, the GH peak amplitude is much smaller
compared with the normal male profile, and the system exhibits the
intrinsic 1-h rhythm (Fig. 6C). The characteristic properties
of the GH pattern in the feminized male rat, i.e., lower peak
amplitude, 1-h periodicity, and an elevated baseline, are well
represented by the simulations.
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DISCUSSION |
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GH is essential for normal body growth and metabolism in both animals and humans. Hence, an understanding of the mode of generation of the GH secretion profile is of physiological and pathophysiological importance.
Based on experimental results, we modeled the GH neuroendocrine axis as a combination of a linear pathway that describes the sequential signaling between GHRH and GH and a cyclic pathway involving the feedback of GH on its own release via GH receptors on SRIF neurons in the hypothalamus. The GHRH-GH axis is based on an intrinsic 1-h rhythm while the SRIF-GH cycle yields the 3.3-h periodicity. The ultradian GH rhythm observed in the male rat is obtained by modulating the 1-h GHRH rhythm with an overall 3.3-h periodicity of SRIF release into both the brain and portal blood.
The 3.3-h GH rhythm is composed of the following components. Starting
at the beginning of a secretion period, the concentration of SRIF
increases after a delay of 62 min and remains at a high level for 70 min, i.e., the duration of two pulses. Thereafter, SRIF follows the
decay of GH in the circulation until the latter declines below the 1%
threshold after 63 min
(5 × 1/k3,cl). This yields a total
of 195 min, so the next pulse of GHRH (after 200 min) induces the
release of GH and the cycle starts again. To obtain a 3.3-h rhythm, an
integral number of GHRH pulses must occur within 200 min. Because the
delay time
and the clearance rate constant
k3,cl are fixed parameters of the system, the 3.3-h rhythm can be disrupted either by changing the duration of the high
level of GH in the circulation (e.g., administration of hGH) or by
altering the parameters of the feedback function (resulting in a
decreased sensitivity of SRIF to GH as in the case of the male-female transition).
The intriguing fact that the 3.3-h GH rhythm is conserved after an intravenous injection of SRIF-Ab with an elevated baseline (27) can be readily explained in terms of the model. SRIF-Ab is assumed to neutralize SRIF only at the level of the pituitary but not at the level of the hypothalamus (due to the blood-brain barrier). In the absence of SRIF in the pituitary, the GH profile in the circulation represents the GHRH pulses in the portal blood. Because the feedback of GH on hypothalamic SRIF release is not distorted by the perturbation, a rise in circulating GH still results in an increase of SRIF after the delay, which in turn suppresses GHRH pulses at the level of the hypothalamus. Therefore, the 3.3-h periodicity of SRIF in the brain remains conserved.
The model is designed so that release of GH can only be induced by GHRH. It follows that administration of GHRH-Ab results in an undetectable level of GH in the circulation, as observed in many experiments (27, 43).
The hypothesis of an intrinsic 1-h rhythm generated by GHRH neurons is based on the following arguments. In the male rat, a high-frequency pattern of GH is often observed in perturbation studies (13, 21), which is similar to that seen within a GH secretory episode. Because the GH profile in blood shows a periodicity of 3.3 h, it is unlikely that the high frequency of the GHRH pulses is generated by a GH feedback loop. It remains possible that the high-frequency GHRH profile is the result of mutual activation or inhibition between GHRH and SRIF neurons in the brain. Unfortunately, such a mechanism appears to require Hill coefficients greater than seven (10), which are usually not observed in biology. Thus we arrived at a 1-h rhythm intrinsic to a black box system involving GHRH neurons, which could be the result of a feedback circuit within the GHRH neuronal network (17) or via other neuropeptides such as the putative GHS (4, 33) and neuropeptide Y (8).
The model predicts a possible mechanism for the change of the male GH
rhythm into the female pattern by sex steroids and vice versa. The
transition was obtained by an appropriate change of the parameters
(
,
c4,tot) of the receptor function (see Fig. 2).
The latter becomes independent of GH on sufficiently increasing
c4,tot, which can be achieved by a higher binding
constant or by increasing the number of GHR; indeed, there is
experimental evidence that the total amount of GHR is elevated in the
female rat (31). Therefore, intravenous administration of hGH to a female rat has no effect on the rat GH profile (6) (the feedback of GH
is disrupted), and the system gives a constant response to hourly
injections of GHRH (12, 27) (constant SRIF release).
There is no doubt that pulsatility in GH secretion is important for
growth (32). The typical GH profile shows two frequencies, namely the
3.3-h periodicity of the GH secretory episodes and the 1-h rhythm
within the episodes. In the model, the origin of the multiple peaks per
GH episode is the time delay
. If
were <50 min, only one GH
peak per period would be observed. Therefore, one might speculate that
the double peak within a secretion episode is due to an intrinsic
limiting parameter (
), whereas the 3.3-h periodicity is the result
of an evolutionary process to optimize growth.
Finally, the model suggests two experiments that might reveal the 1-h rhythm of GHRH neurons. Disrupting the feedback of GH on its own release (which entails the obliteration of internalized receptors) should cause the profile of GH in the circulation to show a 1-h periodicity according to the pulses of GHRH in the portal blood, since release of SRIF ceases. Indeed, Pellegrini et al. (29) recently demonstrated that central administration of a GHR mRNA antisense increases the pulsatility of GH and decreases hypothalamic SRIF expression. Second, antagonizing the activity of SRIF in the hypothalamus and in the pituitary, using a pure SRIF antagonist, should result in a 1-h rhythm of GH secretion in the circulating blood. This experiment is now in progress.
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APPENDIX |
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Derivation of the Receptor Function (cA4)
In general, it is assumed that two receptors bind to one GH molecule to activate the signaling pathway within the cell. Assuming the total amount of receptors, c4,tot, is constant, the kinetic equations corresponding to the model shown in Fig. 2 read
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(A1) |
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(A2) |
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(A3) |
The following two interesting limits of Eq. 6 should be noted:
1) if cC3 tends to zero, it can
readily be shown that cA4 tends to zero as
well, and 2) if
c4,tot tends to infinity, the
value of cA4/c4,tot becomes
constant and independent of the GH concentration
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(A4) |
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ACKNOWLEDGEMENTS |
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This work was supported by Grant MT-6837 (to G. S. Tannenbaum) from the Medical Research Council of Canada. G. S. Tannenbaum is a Chercheur de Carrière of the Fonds de la recherche en santé de Québec. C. Wagner is the recipient of postdoctoral fellowship awards from The Swiss National Foundation and the Ciba-Geigy-Jubilaeumsstiftung.
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FOOTNOTES |
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Present address of C. Wagner: Biozentrum, University of Basel, Dept. of Biophysical Chemistry, Klingelbergstrasse 70, CH-4056 Basel, Switzerland.
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. §1734 solely to indicate this fact.
Address for reprint requests: G. S. Tannenbaum, Neuropeptide Physiology Laboratory, McGill University-Montreal Children's Hospital Research Institute, 2300 Tupper St., Montreal, Quebec, Canada H3H 1P3.
Received 22 May 1998; accepted in final form 21 August 1998.
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