silver 2003.pdf - Alice
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R EPORTS<br />
High-Probability Uniquantal<br />
Transmission at Excitatory<br />
Synapses in Barrel Cortex<br />
R. Angus Silver, 1 *† Joachim Lübke, 2 Bert Sakmann, 3<br />
Dirk Feldmeyer 3 *<br />
The number of vesicles released at excitatory synapses and the number of<br />
release sites per synaptic connection are key determinants of information<br />
processing in the cortex, yet they remain uncertain. Here we show that the<br />
number of functional release sites and the number of anatomically identified<br />
synaptic contacts are equal at connections between spiny stellate and<br />
pyramidal cells in rat barrel cortex. Moreover, our results indicate that the<br />
amount of transmitter released per synaptic contact is independent of<br />
release probability and the intrinsic release probability is high. These properties<br />
suggest that connections between layer 4and layer 2/3 are tuned for<br />
reliable transmission of spatially distributed, timing-based signals.<br />
Synaptic weight is thought to be a primary<br />
determinant of neural computation. According<br />
to the quantal hypothesis (1, 2) the efficacy<br />
of a connection is determined by the<br />
product of the probability of release, the number<br />
of release sites, and the size of the<br />
postsynaptic response to a quantum of transmitter.<br />
Quantal parameters determine how<br />
reliably information is transmitted (3, 4),<br />
with higher rates of information transfer possible<br />
at connections with larger numbers of<br />
release sites and higher (sustained) release<br />
probabilities (3). However, basic synaptic<br />
properties, such as number of functional and<br />
anatomical release sites per connection and<br />
the release probability per site, remain uncertain<br />
at most cortical synapses. Moreover, the<br />
number of vesicles released at individual synaptic<br />
contacts is controversial. Correlation of<br />
functional release sites and anatomically<br />
1<br />
Department of Physiology, University College London,<br />
Gower Street, London WC1E 6BT, U.K. 2 Forschungszentrum<br />
Jülich GmbH, Institut für Medizin,<br />
D-52425 Jülich, Germany. 3 Max-Planck Institut für<br />
Medizinische Forschung, Abteilung Zellphysiologie,<br />
Jahnstrasse 29, D-69120 Heidelberg, Germany.<br />
*These authors contributed equally to the work.<br />
†To whom correspondence should be addressed. E-<br />
mail: a.<strong>silver</strong>@ucl.ac.uk<br />
Fig. 1. EPSP recordings from an L4 to L2/3 cell pair in rat barrel cortex under different release<br />
probability conditions at 36°C. (A) Current protocols for AP stimulation in the presynaptic<br />
spiny stellate cell (top trace) and for testing input resistance stability in postsynaptic pyramidal<br />
cell (second trace). Third trace shows the AP in the spiny stellate cell. The bottom trace shows<br />
voltage responses to current injection followed by individual EPSPs (gray lines) and the mean<br />
EPSP (black line) in the postsynaptic pyramidal cell. (B) Mean EPSPs recorded in different<br />
extracellular Ca 2 and Mg 2 concentrations at a potential of –73 mV. (C) Input resistance<br />
during different extracellular Ca 2 and Mg 2 concentrations.<br />
Fig. 2. Quantal parameters estimated<br />
from evoked EPSPs under low probability<br />
conditions. (A) The top trace<br />
shows the mean action potential<br />
evoked by a brief depolarizing current<br />
pulse at –72 mV; the bottom trace<br />
shows 14 individual EPSPs (gray<br />
lines), the mean of the 44 EPSP successes<br />
(black solid line), and the mean<br />
of the 279 failures (dashed line) recorded<br />
at –72 mV in 1 mM [Ca 2 ]<br />
and 5 mM [Mg 2 ]. (B) The amplitude<br />
histogram of EPSPs (bins) and scaled<br />
baseline noise (dashed line). The coefficient<br />
of variation of the quantal<br />
EPSP amplitude (CV Q<br />
)was calculated from the background-subtracted<br />
variance. (C) Relation between the variance of the EPSP peak<br />
amplitude (corrected for background variance) and mean peak EPSP<br />
amplitude for an individual L4 to L2/3 cell pair. Each data point shows<br />
a different probability condition. Error bars indicate the theoretical<br />
standard error in the estimate of the variance. Solid line shows the fit<br />
to a multinomial model giving Q 0.09 mV, N F<br />
5.25 and <br />
19800.<br />
www.sciencemag.org SCIENCE VOL 302 12 DECEMBER 2003 1981
R EPORTS<br />
identified synaptic contacts in inhibitory neurons<br />
of goldfish lead to the hypothesis that a<br />
maximum of one vesicle is released per active<br />
zone (“the single vesicle hypothesis”)<br />
(5). This hypothesis was subsequently supported<br />
at connections between hippocampal<br />
pyramidal cells and interneurons (6). However,<br />
recent studies indicate that the concentration<br />
of glutamate in the synaptic cleft changes<br />
with release probability, which implies that<br />
multiple vesicles are released at each synaptic<br />
contact per action potential (AP) (7, 8).<br />
We investigated the number of functional<br />
and anatomical release sites, the release probability,<br />
and the mode of release at synaptic<br />
connections between pairs of layer 4 (L4) and<br />
layer 2/3 (L2/3) excitatory neurons in rat<br />
barrel cortex. Paired whole-cell recordings<br />
were made from acute slices from 17- to<br />
23-day-old rats at near-physiological temperature<br />
(9, 10). In the presence of 2 mM [Ca 2 ]<br />
and N-methyl-D-aspartate (NMDA) receptor<br />
antagonists, single APs in L4 spiny neurons<br />
evoked unitary excitatory postsynaptic potentials<br />
(EPSPs) in L2/3 pyramidal cells with a<br />
mean peak amplitude of 0.54 0.06 mV at<br />
–70 mV (n 32 cells; Fig. 1A). When<br />
stimulated at low frequency (0.1 to 0.033<br />
Hz), EPSP amplitudes remained stable for<br />
long periods (2 to 3 hours). The amplitude<br />
of unitary EPSPs could be increased (in eight<br />
of nine cells) or reduced by altering the<br />
[Ca 2 ] and [Mg 2 ], which suggests that<br />
transmitter release probability was not maximal<br />
under our control conditions (Fig. 1B).<br />
Such alterations in the [Ca 2 ]/[Mg 2 ] ratio<br />
had little effect on the input resistance, and<br />
thus on the voltage response to a given synaptic<br />
conductance (Fig. 1C).<br />
We first determined the mean postsynaptic<br />
response to a single quantum of<br />
transmitter (Q) by evoking release under conditions<br />
of low release probability. In the presence<br />
of 1 mM extracellular Ca 2 , the proportion<br />
of presynaptic APs that failed to release<br />
transmitter was high (0.82 0.02; 0.8 to 1.0<br />
mM Ca 2 ; n 5), and thus, the vast majority<br />
of the EPSPs were single quantal events (Fig.<br />
2A) (10). Quantal EPSPs were identified on<br />
the basis of their characteristic shape, after<br />
each trace was digitally filtered. We checked<br />
that small-amplitude EPSPs were not missed<br />
by averaging the failures (Fig. 2A). On average,<br />
the mean amplitude of quantal EPSPs<br />
was 0.15 0.02 mV at –70 mV (n 5<br />
cells). The mean number of quanta contributing<br />
to the evoked EPSP (quantal content)<br />
under control conditions (2 mM Ca 2 ) was<br />
thus 3.6.<br />
The number of quantal events generated<br />
per synaptic contact can be determined by<br />
comparing the number of sites that can generate<br />
a quantal event (functional release sites,<br />
N F<br />
) and the number of anatomically identified<br />
synaptic contacts (N A<br />
). Because the<br />
quantal content does not provide information<br />
about N F<br />
or about the average release probability<br />
across these sites (P R<br />
), we estimated<br />
these quantal parameters by applying multiple-probability<br />
fluctuation analysis (MPFA)<br />
(11, 12), also known as variance-mean analysis<br />
(13). We first estimated the total nonuniformity<br />
in Q from amplitudes of quantal<br />
EPSPs under low P R<br />
conditions, using the<br />
same peak and baseline measurement windows<br />
used for MPFA (Fig. 2B) (10). This<br />
gave a coefficient of variation (standard deviation/mean;<br />
CV Q<br />
0.43 0.06; n 5<br />
cells) similar to that reported for other excitatory<br />
synapses (11, 14). The variability in<br />
quantal size at an individual release site (intrasite<br />
variability) has been measured directly<br />
at single site cerebellar synapses at physiological<br />
temperature (CV QI<br />
0.21) (15). If we<br />
assume the same value for intrasite quantal<br />
variability at L4 to L2/3 synapses (see verification<br />
below), the variation arising from<br />
differences in the mean quantal amplitude<br />
across sites (intersite variability) can be calculated<br />
(CV QII<br />
0.37) from the total quantal<br />
variability (10). These estimates of quantal<br />
Fig. 3. Relation between the number of anatomically<br />
identified synaptic contacts and functional<br />
release sites. (A) Camera lucida reconstruction of<br />
a cell pair, L4 stellate cell with L2/3 pyramidal<br />
cell. The soma and dendrites of the presynaptic L4<br />
cell are given in red, the axonal arbor in blue. The<br />
somatodendritic configuration of the postsynaptic<br />
L2/3 pyramidal cell is given in black, the axonal<br />
arbor in green. Lower inset shows the distribution<br />
of putative, light microscopically identified synaptic contacts. (B) Variance-mean plot and<br />
multinomial fit for the cell pair shown in (A), where Q and N F are the estimated quantal size<br />
and number of functional release sites, respectively. (C) Electron micrographs (EMs) of the<br />
synaptic contacts identified by light microscopy in (A), where the letters next to the blue dots<br />
in (A) indicate the position of each EM image shown in (C). Labeling in (C): b, presynaptic<br />
bouton with clearly visible synaptic vesicles; d, postsynaptic dendrites.<br />
1982<br />
12 DECEMBER 2003 VOL 302 SCIENCE www.sciencemag.org
R EPORTS<br />
variability were used to constrain a nonuniform<br />
quantal model, which allowed more<br />
accurate estimates of Q, N F<br />
, and P R<br />
.<br />
Time-stable epochs of EPSP amplitudes<br />
were identified for each release probability<br />
condition with a Spearman rank-order analysis<br />
(15). The mean and variance of the peak<br />
amplitude were calculated and corrected for<br />
deviations in driving force from –70 mV,<br />
with an assumed reversal potential for AMPA<br />
receptors of 0 mV (9). EPSP variance-mean<br />
plots were constructed after subtracting background<br />
variance and were fit with a multinomial<br />
model with fixed values of quantal variance<br />
(10); goodness of fit was assessed with<br />
the chi-square test. A variance-mean plot and<br />
multinomial fit are shown in Fig. 2C that<br />
gave a Q of 0.09 mV and an estimate of 5.3<br />
functional release sites for this cell pair. The<br />
mean Q varied little across cell pairs (0.14 <br />
0.02, n 9) and was not significantly different<br />
from that measured directly from quantal<br />
EPSPs under low P R<br />
conditions (P 0.55,<br />
unpaired t test, unequal variance). The N F<br />
across cells was 5.1 0.9 (n 9) and varied<br />
between 2.3 and 6.5 except for one outlying<br />
cell in which N F<br />
11.1 (the mean value<br />
excluding this cell was 4.4 0.5, n 8).<br />
Simulations suggest that part of the variance<br />
in N F<br />
for the eight clustered cells arose from<br />
uncertainty in estimating the variance from a<br />
limited number of EPSPs (10). Under control<br />
conditions, the P R<br />
at each site was high<br />
(0.79 0.04 in 2 mM Ca 2 , n 9), consistent<br />
with a previous study (16). An upper<br />
limit for the quantal variability at an individual<br />
site was calculated by dividing the variance<br />
remaining when P R<br />
was maximal<br />
(1.02 0.05, n 9) by N F<br />
. This gave a value<br />
of CV QI<br />
close to that assumed from measurements<br />
at single-site synapses (0.26 0.02<br />
versus 0.21) (15). Estimation of the coefficient<br />
of variation of release probability across<br />
sites gave a value (0.28 0.07 in 2 mM<br />
Ca 2 , n 9), similar to that obtained in<br />
hippocampal synapses in culture (17).<br />
Anatomical identification of axondendrite<br />
intersections with high-resolution<br />
light microscopy of biocytin-filled cell pairs<br />
(10) indicated between four and six putative<br />
synaptic contacts per connection located on<br />
the proximal dendritic segments of the<br />
postsynaptic neuron (blue dots, Fig. 3A, inset).<br />
Across cells, an average of 4.6 0.2<br />
(n 14) putative synaptic connections were<br />
found, a value not significantly different from<br />
Fig. 4. Fractional block of the EPSP by low-affinity glutamate antagonists is independent of release<br />
probability. (A) The upper trace shows the presynaptic APs in a L4 spiny neuron; middle traces show<br />
mean EPSPs recorded in 2 mM Ca 2 ,1mMMg 2 under control conditions and in 1 mM -DGG (red<br />
trace). The bottom trace shows mean EPSPs recorded in 1.25 mM Ca 2 under control conditions<br />
(blue) and in 1 mM -DGG (green). (B) Plot of EPSP amplitudes as a function of time through the<br />
experiment. (C) EPSPs in (A) normalized to the peak of the first control EPSPs. (D) Relation<br />
between percentage block of the EPSP and extracellular [Ca 2 ] for 0.5 mM kynurenic acid and<br />
1mM-DGG.<br />
the N F<br />
(P 0.58 unpaired t test, unequal<br />
variance). In four cell pairs, we were able to<br />
recover the anatomy after performing quantal<br />
analysis. A camera lucida reconstruction of a<br />
cell pair is shown in Fig. 3, for which we<br />
estimated an N F<br />
of 5.5 and an N A<br />
of 5 (Fig. 3,<br />
A and B). For cell pairs in which both quantal<br />
analysis and anatomical reconstruction were<br />
performed, N F<br />
and N A<br />
were not significantly<br />
different (P 0.21, paired t test, n 4; table<br />
S1). We further examined whether these<br />
close appositions were indeed synaptic contacts<br />
by making serial ultrathin sections<br />
through the entire dendritic domain of the<br />
postsynaptic neuron and examining them at<br />
the electron microscopic (EM) level. Synaptic<br />
contacts were identified on the basis of a<br />
clear presynaptic bouton-like structure containing<br />
closely packed synaptic vesicles together<br />
with closely apposing (20 nm) preand<br />
postsynaptic membranes (Fig. 3C). The<br />
presence of electron-dense biocytin reaction<br />
product both pre- and postsynaptically and<br />
the long duration of the recordings precluded<br />
the use of other anatomical identifiers such as<br />
the pre- and postsynaptic densities. Full EM<br />
analysis of two quantal analysis pairs of neurons<br />
and one additional cell confirmed identification<br />
of 13 out of 14 putative synaptic<br />
contacts, which gave a detection rate close to<br />
that observed at other cortical synapses (18,<br />
19). Synaptic contacts were located directly<br />
on dendritic shafts (Fig. 3C) and occasionally<br />
on spines. Applying the observed optical detection<br />
rate for synaptic contacts (93%)<br />
across the four pairs of neurons, we estimated<br />
N F<br />
/N A<br />
to be 0.90 0.16, which suggests a<br />
one-to-one relation between these synaptic<br />
properties (table S1).<br />
The all-or-none behavior of excitatory synapses<br />
could arise either presynaptically, from the<br />
release of a single quantum per AP, or postsynaptically,<br />
from saturation of postsynaptic receptors<br />
(20, 21) following multivesicular release<br />
(22, 23). We therefore examined whether the<br />
cleft glutamate concentration changes with P R<br />
by assaying the level of block of the EPSPs by<br />
low-affinity glutamate receptor antagonists (7,<br />
12, 24). The effect of 1 mM -d-glutamylglycine<br />
(-DGG) on the mean EPSPs recorded from a<br />
cell pair in normal Ca 2 (2 mM) and in the<br />
presence of a low Ca 2 (1.25 mM) concentration<br />
is shown in Fig. 4, A and B. Normalization to the<br />
first EPSP amplitude illustrates that the fractional<br />
block of the EPSP by -DGG was similar<br />
under these two conditions (Fig. 4C). On average,<br />
the fractional block of the EPSP by -DGG<br />
was not significantly different in 2 mM Ca 2<br />
and 1.25 mM Ca 2 (66 6% and 60 5%,<br />
respectively; P 0.43; n 5). Moreover, the<br />
paired-pulse ratio in 2 mM Ca 2 was unchanged<br />
in the presence of -DGG (0.59 to 0.52, P <br />
0.36; n 10), which indicates a similar fractional<br />
block on each pulse. We tested these results<br />
further by carrying out a series of experiments<br />
www.sciencemag.org SCIENCE VOL 302 12 DECEMBER 2003 1983
R EPORTS<br />
using kynurenic acid, a different rapidly equilibrating<br />
antagonist. As for -DGG, the fractional<br />
block of the EPSP by kynurenic acid was not<br />
significantly different in 2 mM Ca 2 and 1.25<br />
mM Ca 2 (55 3% and 53 6%, respectively;<br />
P 0.61; n 4; Fig. 4D). Our results contrast<br />
with the substantial increase in the level of block<br />
of excitatory postsynaptic currents (EPSCs) by<br />
-DGG and kynurenic acid at the climbing fiber,<br />
as the release probability was lowered (7) from a<br />
similar initial value (11). The fact that rapidly<br />
equilibrating competitive antagonists are equally<br />
effective at blocking the EPSP when P R<br />
was<br />
reduced by a factor of 4 suggests that the concentration<br />
of transmitter in the synaptic cleft,<br />
following release, is independent of P R<br />
at L4 to<br />
L2/3 synapses. These results indicate that each<br />
excitatory synaptic contact releases a single<br />
quantum of glutamate (probably one vesicle but<br />
could be a group of vesicles whose number is<br />
independent of P R<br />
) and operates independently,<br />
in an all-or-none manner.<br />
The high P R<br />
at L4 to L2/3 synapses is well<br />
suited to promote reliable transmission of the<br />
one (76%) or two spikes that whisker stimulation<br />
usually evokes in L4 cells in vivo (25),<br />
because short-term depression becomes significant<br />
during longer bursts of L4 activity [Fig.<br />
4A and (9)]. The depression of high P R<br />
synapses,<br />
together with the precise synaptic latency<br />
between L4 and L2/3 (1 to 3 ms) and rapid<br />
EPSP kinetics (9), may also be important for<br />
maintaining and strengthening L4 to L2/3 synapses,<br />
because this connection exhibits a spiketiming–based<br />
plasticity rule with a narrow coincidence<br />
window (26). Curiously, the small<br />
numbers of release sites, all-or-none uniquantal<br />
signaling and small quantal size are likely to<br />
endow an individual L4 to L2/3 connection<br />
with a relatively low capacity for transmitting<br />
information. These properties contrast with<br />
synapses in the retina, where large numbers of<br />
release sites (200) and graded transmission<br />
allow high information transmission rates (27).<br />
Moreover, transmission is finely tuned because<br />
only 10% of the 300 to 400 spiny stellate cells<br />
that innervate an individual L2/3 pyramidal cell<br />
fire synchronously, within 15 ms of single<br />
whisker stimulation (25), close to the minimum<br />
number required for a pyramidal cell to reach<br />
voltage threshold (9). Our results suggest that<br />
the functional and anatomical properties of L4<br />
to L2/3 synaptic connections are well adapted<br />
for efficient, timing-based distributed signaling.<br />
References and Notes<br />
1. B. Katz, The Release of Neural Transmitter Substances<br />
(Liverpool Univ. Press, Liverpool, 1969).<br />
2. D. Vere-Jones, Aust. J. Stat. 8, 53 (1966).<br />
3. A. Zador, J. Neurophysiol. 79, 1219 (1998).<br />
4. M. London, A. Schreibman, M. Häusser, M. E. Larkum,<br />
I. Segev, Nature Neurosci. 5, 332 (2002).<br />
5. H. Korn, A. Triller, A. Mallet, D. S. Faber, Science 213,<br />
898 (1981).<br />
6. A. I. Gulyas et al., Nature 366, 683 (1993).<br />
7. J. I. Wadiche, C. E. Jahr, Neuron 32, 301 (2001).<br />
8. T. G. Oertner, B. L. Sabatini, E. A. Nimchinsky, K.<br />
Svoboda, Nature Neurosci 5, 657 (2002).<br />
9. D. Feldmeyer, J. Lübke, R. A. Silver, B. Sakmann,<br />
J. Physiol. (London) 538, 803 (2002).<br />
10. Methods, table S1, and references are available as<br />
supporting online material on Science Online.<br />
11. R. A. Silver, A. Momiyama, S. G. Cull-Candy, J. Physiol.<br />
(London) 510, 881 (1998).<br />
12. J. D. Clements, R. A. Silver, Trends Neurosci 23, 105 (2000).<br />
13. C. A. Reid, J. D. Clements, J. Physiol. (London) 518,<br />
121 (1999).<br />
14. J. M. Bekkers, J. D. Clements, J. Physiol. (London) 516,<br />
227 (1999).<br />
15. R. A. Silver, S. G. Cull-Candy, T. Takahashi, J. Physiol.<br />
(London) 494, 231 (1996).<br />
16. M. A. Castro-Alamancos, B. W. Connors, Proc. Natl.<br />
Acad. Sci. U.S.A. 94, 4161 (1997).<br />
17. V. N. Murthy, T. J. Sejnowski, C. F. Stevens, Neuron<br />
18, 599 (1997).<br />
18. H. Markram, J. Lübke, M. Frotscher, A. Roth, B. Sakmann,<br />
J. Physiol. (London) 500, 409 (1997).<br />
19. J. Lübke, A. Roth, D. Feldmeyer, B. Sakmann, Cereb.<br />
Cortex 13, 1051 (2003).<br />
20. J. J. Jack, S. J. Redman, K. Wong, J. Physiol. (London)<br />
321, 65 (1981).<br />
21. P. Jonas, G. Major, B. Sakmann, J. Physiol. (London)<br />
472, 615 (1993).<br />
22. R. A. Silver, in Central Synapses: Quantal Mechanisms<br />
and Plasticity, D. S. Faber, H. Korn, S. J. Redman, S. M.<br />
Thompson, and J. S. Altman, Eds., 4th Human Frontier<br />
Science Workshop, Strasbourg, France, 22 to 24 April<br />
1997 (Human Frontier Science Program, Strasbourg,<br />
France, 1998), pp. 130–139.<br />
23. K. A. Foster, A. C. Kreitzer, W. G. Regehr, Neuron 35,<br />
1115 (2002).<br />
24. J. S. Diamond, C. E. Jahr, J. Neurosci. 17, 4672 (1997).<br />
25. M. Brecht, B. Sakmann, J. Physiol. (London) 543, 49<br />
(2002).<br />
26. D. E. Feldman, Neuron 27, 45 (2000).<br />
27. S. B. Laughlin, R. R. de Ruyter van Steveninck, J. C.<br />
Anderson, Nature Neurosci. 1, 36 (1998).<br />
28. Supported by the Max-Planck Society and the Wellcome<br />
Trust. R.A.S. is in receipt of a Wellcome Trust<br />
Senior Fellowship. We thank A. Roth and C. Saviane<br />
for help with simulations; D. Attwell, D. DiGregorio,<br />
M. Farrant, S. Mitchell, T. Nielsen, and I. Vida for<br />
comments on the manuscript; and N. Nestel and B.<br />
Joch for technical assistance.<br />
Supporting Online Material<br />
www.sciencemag.org/cgi/content/full/302/5652/1981/DC1<br />
Materials and Methods<br />
Table S1<br />
References<br />
23 May 2003; accepted 15 October 2003<br />
Anterior-Posterior Guidance of<br />
Commissural Axons by<br />
Wnt-Frizzled Signaling<br />
Anna I. Lyuksyutova, 2 Chin-Chun Lu, 1 Nancy Milanesio, 1<br />
Leslie A. King, 2 Nini Guo, 4 Yanshu Wang, 4 Jeremy Nathans, 4<br />
Marc Tessier-Lavigne, 5 * Yimin Zou 1,2,3 †<br />
Commissural neurons in the mammalian dorsal spinal cord send axons ventrally<br />
toward the floor plate, where they cross the midline and turn anteriorly toward the<br />
brain; a gradient of chemoattractant(s) inside the spinal cord controls this turning.<br />
In rodents, several Wnt proteins stimulate the extension of commissural axons after<br />
midline crossing (postcrossing). We found that Wnt4 messenger RNA is expressed<br />
in a decreasing anterior-to-posterior gradient in the floor plate, and that a directed<br />
source of Wnt4protein attracted postcrossing commissural axons. Commissural<br />
axons in mice lacking the Wnt receptor Frizzled3 displayed anterior-posterior<br />
guidance defects after midline crossing. Thus, Wnt-Frizzled signaling guides commissural<br />
axons along the anterior-posterior axis of the spinal cord.<br />
Axonal connections are patterned along the<br />
anterior-posterior (A-P) and dorsal-ventral<br />
(D-V ) neuraxes. Guidance molecules that<br />
play essential roles in the D-V guidance of<br />
axons have been identified, whereas the nature<br />
of the A-P guidance cues has remained<br />
an enigma (1, 2). The dorsal spinal cord<br />
commissural neurons form several ascending<br />
somatosensory pathways. During embryonic<br />
development, they project axons to the ventral<br />
midline (Fig. 1A). At the floor plate,<br />
commissural axons cross the midline, enter<br />
the contralateral side of the spinal cord, and<br />
make a sharp anterior turn toward the brain<br />
(Fig. 1B) (3). The initial ventral growth of the<br />
commissural axons is directed by a collaboration<br />
of two chemoattractants, netrin-1 (4–<br />
6) and Sonic hedgehog (Shh) (7), and chemorepellents<br />
of the bone morphogenetic protein<br />
(BMP) family (8). As the axons cross the<br />
midline, they lose responsiveness to these<br />
chemoattractants (9) but gain responsiveness<br />
to several chemorepellents, including Slit and<br />
semaphorin proteins (10), which guide axons<br />
from the D-V axis into the A-P axis (10).<br />
To determine why axons turn in an anterior<br />
direction, we studied the turning of commissural<br />
axons after midline crossing in “open-book” spi-<br />
1<br />
Department of Neurobiology, Pharmacology and Physiology,<br />
2 Committee on Developmental Biology, 3 Committee<br />
on Neurobiology, University of Chicago, Chicago, IL 60637,<br />
USA. 4 Departments of Molecular Biology and Ophthalmology,<br />
Howard Hughes Medical Institute, Johns Hopkins<br />
Medical School, Baltimore, MD 21205, USA. 5 Department<br />
of Biological Sciences, Howard Hughes Medical Institute,<br />
Stanford University, Stanford, CA 94305, USA.<br />
*Present address: Genentech Inc., South San Francisco,<br />
CA 94080, USA.<br />
†To whom correspondence should be addressed. E-<br />
mail: yzou@bsd.uchicago.edu<br />
1984<br />
12 DECEMBER 2003 VOL 302 SCIENCE www.sciencemag.org