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The Journal of Neuroscience, February 1, 1998, 18(3):1171-1185
Neural Substrates for Species Recognition in the Time-Coding
Electrosensory Pathway of Mormyrid Electric Fish
Matthew A.
Friedman and
Carl D.
Hopkins
Section of Neurobiology and Behavior, Cornell University, Ithaca,
New York 14853
 |
ABSTRACT |
Mormyrid electric fish have species- and sex-typical electric organ
discharges (EODs). One class of tuberous electroreceptors, the
knollenorgans, plays a critical role in electric communication; one
function is species recognition of EOD waveforms. In this paper, we
describe cell types in the knollenorgan central pathway, which appear
responsible for analysis of the temporal patterns of spikes encoded by
the knollenorgans in response to EOD stimuli. Secondary sensory neurons
in the nucleus of the electrosensory lateral line lobe (NELL) act as
relays of peripheral responses. They fire a single phase-locked spike
to an outside positive-going voltage step. Axons from the NELL project
to the toral nucleus exterolateralis pars anterior (ELa). Immediately
after they enter the ELa, they send collaterals to terminate on one to
three ELa large cells and then continue in a lengthy neuronal pathway
that traverses the ELa several times. After a path length of up to 5 mm, the NELL axon terminates on as many as 70 ELa small cells. Thus the
large cells appear to be excited first, followed by the small cells,
with the intervening length of the axon serving as a delay line. The
large cells also respond with phase-locked spikes to voltage steps.
Large cell axons extend for ~1 mm and terminate on several small
cells within the ELa. The terminals are known to be GABAergic inputs
and are presumed inhibitory. We propose that small cells receive direct
inhibition from large cells and delayed excitation from NELL axons. The
small cells may act as anti-co-incidence detectors to analyze the
temporal structure of the EOD waveform.
Key words:
mormyrid; electric fish; knollenorgan; electroreception; time-coding; delay line; co-incidence detector
 |
INTRODUCTION |
Mormyrid electric fish communicate
using pulse-type electric organ discharges (EODs), generated by an
electric organ in the tail (Hopkins, 1986
; Kramer, 1990
; Moller, 1995
).
EODs can be species-, sex-, and individual-specific (Hopkins, 1981c
;
Hopkins and Bass, 1981
; Crawford, 1992
; Friedman and Hopkins, 1996
).
Fish can discriminate the species and sex of neighboring fish,
apparently based on the temporal structure of the EOD waveform,
although EODs may be less than 1 msec in duration (Hopkins, 1981c
;
Hopkins and Bass, 1981
; Graff and Kramer, 1992
). The EODs are detected by a specialized class of tuberous electroreceptors, called
knollenorgans (Hopkins, 1981b
, 1983
; Moller and Szabo, 1981
). In this
paper, we describe anatomical and physiological specializations of cell types in the knollenorgan pathway and how these cells may be involved in temporal analysis of the EOD waveform.
Figure 1 illustrates the knollenorgan
pathway. Knollenorgans are scattered over the skin of the head and the
dorsal and ventral midlines (Harder, 1968
). Knollenorgan afferents are
relayed through the nucleus of the electrosensory lateral line lobe
(NELL), which in turn project up to the nucleus medialis ventralis (MV)
and the nucleus exterolateralis pars anterior (ELa), where they end on
two cell types, large cells and small cells (Bell and Szabo, 1986
). ELa
large cells terminate with calyceal, GABA-ergic synapses onto ELa small
cells (Mugnaini and Maler, 1987a
; Amagai et al., 1998
), which in turn
project to the nucleus exterolateralis pars posterior (ELp)
(Haugedé-Carré, 1979
).

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Figure 1.
Brain anatomy and summary of the knollenorgan
pathway. A, Lateral view of brain of B.
brachyistius. The nucleus exterolateralis sits between the
valvula (VA) and the optic tectum
(OT). The ELa is whiter than the ELp,
because of its heavy myelin content. B, Summary of the
knollenorgan pathway. Knollenorgan afferents project to the NELL, which
in turn projects bilaterally to the ELa onto large and small cell
types. The NELL also sends collaterals to the MV.
C3, Cerebellar lobe 3; EGp,
eminentia granularis pars posterior; ELa, nucleus
exterolateralis pars anterior; ELL, electrosensory
lateral line lobe; ELp, nucleus exterolateralis pars
posterior; IL, inferior lobe; ll, lateral
lemniscus; mm, meso-mesencephalic tract;
MV, toral nucleus medialis ventralis; nALL, anterior lateral line nerve; NELL
nucleus of the ELL; nPLL, posterior lateral line nerve;
OB, olfactory bulb; op, optic nerve; SC, spinal cord; Tel, telencephalon;
TL, torus longitudinalis; VA, valvula
cerebelli. Scale bars: A, 1 mm; B, 250 µsec.
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The primary afferents, NELL cells, and ELa large cells all have large,
adendritic somata, heavily myelinated, thick axons, and large, mixed
electrotonic and chemical synapses (Bell and Russell, 1978
; Szabo et
al., 1983
; Mugnaini and Maler, 1987a
,b
; Bell and Grant, 1989
; Hopkins
et al., 1993
; Amagai et al., 1998
). Their responses are tightly
phase-locked to the stimulus with little temporal variation
("jitter"; Amagai et al., 1998
). They also can contain high levels
of calcium-binding proteins (Friedman and Kawasaki, 1997
). These
specializations are characteristic of other sensory systems that encode
the temporal structure of stimuli, so-called "time-coding pathways"
(Carr, 1986
, 1993
). Early stages in these pathways encode temporal
information using phase-locking, but higher stages typically convert to
a different coding form, such as the presence or magnitude of firing in
a subset of cells in a map, with an accompanying loss of the anatomical and physiological specializations.
Indeed, in the knollenorgan pathway, the ELa small cells lack these
specializations (Mugnaini and Maler, 1987a
). Because the ELa receives
bilateral input from the NELL, small cells could make temporal
comparisons between knollenorgan activity on the two sides of the body
(Szabo et al., 1983
). Hopkins and Bass (1981)
proposed that recognition
of EOD waveforms could be accomplished by comparing the difference in
response latencies between different regions of the body surface
presented with an EOD stimulus. Our results support the hypothesis that
ELa small cells measure EOD duration by comparing delayed, excitatory
input from an NELL cell with inhibitory input from an ELa large cell,
with the two inputs having receptive fields on different parts of the
body surface.
 |
MATERIALS AND METHODS |
This study used more than 50 individuals of two species of
mormyrid fish, Brienomyrus brachyistius (Gill, 1862
) and
B. niger (Günther, 1866
). Fish were imported from
commercial fish dealers, housed in 400 l tanks, kept on a 12 hr
light/dark cycle, and fed live blackworms. Water conductivity was
maintained at ~200-500 µS/cm. Some of the methods have been
described before (Amagai et al., 1998
).
We paralyzed fish and eliminated the EOD with flaxedil (10-20 µl of
2 mg/ml), providing continuous aerated water for respiration. We glued
a post to the skull to stabilize the head and opened a small hole over
the nucleus exterolateralis (Fig. 2).
During surgery, the fish was anesthetized with MS-222 (100-200 mg/l) and with 2% lidocaine applied to the surgical wound.

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Figure 2.
Experimental setup. Stimuli are delivered either
transverse or head-tail through carbon rod electrodes. The head is
steadied with a head holder glued to the skull. The health of the fish is monitored using a pair of electrodes next to the tail, which pick up
the spinal volley that would normally cause an electric organ
discharge.
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Intracellular recording. We used thin-wall (0.75 mm inner
diameter) borosilicate glass containing 2% biocytin dissolved in an
artificial intracellular solution ("Rose" solution, in
mM: 100 potassium acetate, 2 KCl, 1 MgCl2, 5 EGTA, 10 HEPES, and 20 KOH) (Rose and
Fortune, 1996
) (resistances 150-250 M
). In some experiments, we
used 5% lucifer yellow in 0.1 M LiCl, 2% biocytin in 2 M potassium acetate, or 2-3% neurobiotin in 3 M KCl.
We positioned microelectrodes using a Burleigh inchworm microdrive
(Burleigh Instruments, Fishers, NY) according to visual landmarks (Fig.
1A). We confirmed electrode position by the
short-latency responses of units to electrosensory stimuli. We aimed
for 15-20 mV spikes and
30 mV resting potentials for the best
fills.
Cellular responses were amplified (intracellular amplifier 707A, World
Precision Instruments, Sarasota, FL), low-pass-filtered at 10 kHz, and
digitized to computer disk at 20 kHz (AD1; Tucker-Davis Technologies,
Gainesville, FL). Responses were analyzed off-line using custom written
software. Latencies for action potentials and synaptic potentials were
measured to the point of maximum slope.
After recording from a cell, we attempted to fill it with dye by
passing positive-biased 2 Hz sinusoidal current. Large cell bodies
could be faintly labeled after 15-30 sec of filling, but a good fill
required >5 min.
Stimulus generation. We presented square pulse stimuli
(0.02-30 msec duration) with different amplitudes (0.1-300 mV/cm in 5 dB steps) and geometries, using a Tucker-Davis AP2 array processor, DA1
digital-to-analog device, and a PA4 programmable attenuator. Stimuli
were isolated using an audio transformer (Magnetek Triad, T-31X;
frequency response, flat ± 3 dB from 12 Hz to 40 kHz) and were
delivered into the tank using carbon electrodes (Fig. 1C). The positive electrode was on the fish's left side (Fig. 2). We calibrated the electric field with the fish absent.
We measured the one-to-one firing threshold for NELL cells and ELa
large cells in each polarity by stimulating at long durations at the
lowest intensity that yielded one-to-one firing. Then we shortened the
duration until the cell stopped firing, at which point we increased the
intensity in 5 dB steps until it fired one-to-one. For some fibers, no
response could be elicited for the shortest durations. Stimuli were
generally delivered at four to five per second. For the sake of filling
the cells with dye, we tried to characterize the cells in <2 min.
Tract tracing. We used broken-tipped microelectrodes (8-12
µm), filled with Mr 3000 or 10,000 biotinylated dextran amines [Molecular Probes, Eugene, OR; 7% in 0.7 M KCl and 0.03% Triton X-100 (Aldrich, St. Louis, MO)].
We verified electrode placement in the ELa or the ELp using field
potentials and injected dye with 0.7-1.3 µA of current for 1-5 min.
We allowed 4-6 hr for the dye to transport.
Histology. Before perfusion, we deeply anesthetized fish
with 0.05-0.1% MS-222. We perfused fish through the conus with 0.9% NaCl, followed by 4% buffered paraformaldehyde, and post-fixed the
brains overnight in paraformaldehyde and then in 4% paraformaldehyde plus 10% sucrose until it sank. We embedded the brains in 10% gelatin-10% sucrose, post-fixed overnight, and cut 50 µm frozen sections on a sliding microtome (American Optical Corp., Buffalo, NY).
The brains with tract-tracing injections were treated similarly, but
without the sucrose, and were cut at 60 µm by Vibratome (Pelco, Redding, CA). We visualized biotin-labeled cells with a protocol modified from that of Horikawa and Armstrong (1988)
(see Amagai et al.,
1998
). Sections were mounted on subbed slides, counterstained with
neutral red, dehydrated, and coverslipped under Permount (Fisher
Scientific, Rochester, NY) or DePeX (Bio/Medical Specialties, Inc.,
Santa Monica, CA).
Microscopy. We made camera lucida drawings of cells on a
Leitz DMRB microscope. Complete serial reconstruction was performed for
several cells by lining up segments of axons from one section with the
adjacent section. The exit position of an axon segment from a section
reliably predicted a nearby continuing axon segment in the next
section, and an axon segment that did not exit the section reliably
ended with a distinct terminal onto a counterstained cell body of
identifiable type. After axon assignments were made, axon segment
lengths were measured by walking a pair of calipers set to the
equivalent of 10 µm over the length of the traced axon. If a segment
entered and exited through opposite sides of the section, its true
length was estimated by assuming it took the shortest, straight
diagonal path through the section, and therefore:
 |
RESULTS |
Encoding characteristics of NELL axons and ELa large cells
Our results summarize recordings from >150 units in the ELa, most
of which were from NELL axons or ELa large cells, which had response
characteristics similar to knollenorgan primary afferents. These cells
were stimulated by either the rising edge or the falling edge of square
pulse stimuli. They fired spikes, usually singly, at 2.5-3 msec
latency with low jitter. One-to-one firing thresholds varied from 5 to
50 mV/cm.
Figure 3 illustrates these
characteristics for one NELL axon. This unit responded at its
one-to-one firing threshold (14 mV/cm) with a latency of 2.6 ± 0 msec (Fig. 3A). When the stimulus intensity was reduced to
8.0 mV/cm, the response probability decreased to 68% (13 of 19), and
the response latency and jitter increased to 2.84 ± 0.13 msec
(n = 13; range, 2.65-3.2 msec; Fig. 3B).
With a further reduction in stimulus intensity to 8 mV/cm (~5 dB), the unit was silent. If the intensity was increased above the one-to-one firing threshold, there was no change in first spike latency.

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Figure 3.
Traces from a contralateral NELL axon recorded in
the ELa. This recording typifies the most common type of unit recorded
in the ELa. The large deflections 1 msec from the beginning of the trace are stimulus artifact. A, Response at the
one-to-one firing threshold. Ten responses to a 0.05 msec, 14 mV/cm,
reverse polarity square pulse are overlaid. B, Responses
5 dB below the one-to-one firing threshold. The 19 stimulus
presentations of a 0.05 msec, 8.0 mV/cm, reverse polarity square pulse
are overlaid. C, D, Responses to reverse
(C) and normal (D) polarity
stimuli of 0.05, 0.6, and 1 msec durations.
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As seen in previous studies (Amagai et al., 1988
, 1993
, 1998
),
responses were phase-locked to one edge of the stimulus or the other.
The spike response of the unit in Figure 3 was phase-locked at a
latency of 2.6 msec to the leading edge of a reverse polarity stimulus
(left side negative; Fig. 3C) or to the falling edge of a
normal polarity stimulus (left side positive; Fig. 3D). From this polarity test, we predicted, and later confirmed by labeling the
cell with dye, that the receptive field was on the right
(contralateral) side of the fish. Most of the units we recorded from
were driven by contralateral inputs. Other units were driven by
ipsilateral (left) inputs, but these were less common.
We determined the one-to-one firing thresholds to transverse electric
fields for each unit over a range of square pulse durations (11 examples shown in Fig. 4). The thresholds
varied from 2-3 mV/cm to 200 mV/cm for different units. These numbers
were higher and more variable than receptor thresholds measured in
response to direct stimulation at the receptor pore (Bennett, 1965
;
Hopkins, 1981a
) and undoubtedly reflect the effect of stimulus geometry (see Yager and Hopkins, 1993
). Typically, the thresholds were constant
for square pulse stimuli with durations down to 0.1 msec. Some units
showed nearly constant thresholds down to 0.02 msec square pulse, but
for others the intensity had to be increased by 5 or 10 dB to achieve
one-to-one firing for the shortest durations. All units shown in Figure
4 were confirmed to be NELL axons or ELa large cells by intracellular
labeling. Two large cells are marked with circles. One large
cell (Fig. 4, open circles) could not be driven one-to-one,
and we suspect its receptive field was in an unfavorable location for
transverse stimuli. We could not distinguish between large cell
recordings and NELL axon recordings from their physiological properties
alone.

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Figure 4.
One-to-one firing thresholds for square pulses of
varying durations for 11 units recorded in the ELa. Solid
lines are fibers from contralateral-responding NELL cells, and
dotted lines are from ipsilateral-responding NELL cells.
The open and closed circles are two units
confirmed to be ELa large cells. Insets show the direction of current flow, normal polarity in A, and
reverse polarity in B.
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NELL afferent projection patterns
We successfully filled 30 afferent axons from the NELL with
biocytin. The fills were characterized by an axon projecting into the
ELa from the lateral lemniscus. Twenty-three axons ran in the
contralateral (ventral) lateral lemniscal bundle; five ran in the
ipsilateral (dorsal) lateral lemniscal bundle; and two could not be
determined. We labeled all the way to the soma in the NELL in eight
cases (e.g., Fig.
5A,B).
In 4 of the 30 cases, we saw a distinct bifurcation in the posterior
lateral lemniscus, with collaterals to both ipsilateral and
contralateral ELas (Fig. 5C). Because the axons were quite
faint at the bifurcation point in these four cases, the absence of a
collateral in the other 26 axons is inconclusive.

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Figure 5.
NELL cell. In this and all subsequent anatomical
figures, sections are cut horizontally (i.e., anterior is at
top), and the somata have been counterstained with
neutral red. A, Overview of the right NELL of B.
niger. Medial is to the left. The NELL is a long
tube of large round cells, just medial to the ampullary zone of the ELL
cortex. The area in the dotted box is enlarged in
B. B, NELL soma filled by intracellular injection into
ELa. The somata are large and adendritic. The arrow
indicates the labeled initial segment. A nearby unfilled cell,
counterstained with neutral red, is included for comparison.
C, Bifurcation of an NELL axon in the decussation of the
lateral lemniscus. The axon arrives from the lower right
and bifurcates (arrow), producing collateral fibers to
the contralateral (right branch) and ipsilateral
(left branch) ELas. Scale bars: A, 200 µm; B, 20 µm; C, 50 µm.
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In six well labeled NELL axons, we observed a collateral projection
into the medial ventral toral nucleus (Fig.
6, MV). All of the
axons that had MV terminals arose from the contralateral NELL, but
because the number of ipsilateral NELL axons labeled was small, we
cannot conclude that ipsilateral NELL axons do not terminate in the MV
also. The terminal arborizations are thin and diffuse, with
varicosities at intervals along their length (Fig.
6B). We saw two variants of this projection. In the
first variant, four NELL axons branched within the lemniscus, with the main trunk continuing dorsally toward the ELa and the thin branch turning ventrally and laterally toward the MV (Fig.
6D). In the second variant, two NELL axons diverted
from the lemniscus and crossed the dorsal MV, letting off intermittent
branches (Fig. 6B,C), before
continuing dorsally and laterally toward the ELa.

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Figure 6.
Terminals from intracellularly filled NELL cells
in the MV. A, Overview of the torus semicircularis. In
all subsequent figures, anterior is at top, and medial
is to the right. The MV is located ventral to the
nucleus exterolateralis, with the lateral lemniscus passing medially
and dorsally to it. A fiber from the NELL crossing the MV is indicated
by the arrow and is enlarged in B. B,
Closeup of the boxed area in A. An axon
from the NELL traverses the MV, with two branches visible at this plane
of section (large arrows). The axon within the MV is
thin, and there are small varicosities visible (small
arrows). C, Reconstruction from eight sections of the axon shown in A and B. The
terminal field is contained within two sections (100 µm)
D, Another NELL axon terminating in the MV,
reconstructed from three sections (150 µm). IG,
Isthmic granule nucleus; mm, meso-mesencephalic tract;
PE, preeminential nucleus; v, ventricle;
VP, ventral posterior nucleus. Scale bars: A, C,
D, 400 µm; B, 50 µm.
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In agreement with previous studies (Mugnaini and Maler, 1987a
), the
NELL axon projecting into the ELa is thick (2-4 µm; Fig. 7A). We observed two types of
terminals from these NELL axons. The first type was a large cup-like
terminal onto the soma of an ELa large cell. These terminals onto large
cells were located either immediately adjacent to the NELL axon (Fig.
7A) or off a thick, 10- to 80-µm-long collateral (Fig.
7B). The terminals onto large cells were 4-10 µm across,
compared with the large-cell soma diameter of 8-14 µm. The second
type of NELL axon terminal was a smaller bouton onto an ELa small cell.
These terminals generally occurred at the ends of branches off the axon
(Fig. 7C) or as en passant synapses along the
axon. Fibers with terminals onto small cells were <1 µm in diameter,
and terminal boutons were 1-2 µm across, compared with the small
cell soma diameter of 5-7 µm. In one case, we observed dye coupling
between the NELL axon and the small cell somata it contacted (Fig.
7C). This is consistent with the electron microscopic study
of Mugnaini and Maler (1987a)
, which found electrotonic synapses
between NELL axons and small cells.

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Figure 7.
Terminals from NELL cells in the ELa.
A, Nearby terminal from an intracellularly labeled NELL
axon onto an ELa large cell (arrow). B,
Distant terminal from an intracellularly labeled NELL axon onto an ELa
large cell (arrow). C, Terminals from an
intracellularly labeled NELL axon onto ELa small cells. The small cell
somata contacted (arrows) are distinctly grayer than the
surrounding red-counterstained small cells, which indicates dye
coupling. Scale bars: A, C, 20 µm; B,
50 µm.
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We made serial reconstructions of four NELL axons in ELa by connecting
83-206 segments of labeled axons across 12-15 serial sections. The
final reconstructions of two of them are shown in Figure
8. The paths described by the NELL axon
are quite complex, but it is possible to follow simple ones through the
nucleus. In Figure 8A, the axon enters ventrally from
the lateral lemniscus and goes laterally, where it branches to make a
terminal on a large cell (Fig. 8A, arrow). The main
branch then heads posteriorly and dorsally to the posterior margin of
the ELa, before turning laterally to the lateral edge of the ELa. Then
it heads to the anterior margin of the ELa, before doubling back
posteriorly and dropping ventrally to the bottom of the nucleus. Then
it curves laterally, anteriorly, and dorsally and splits into four
branches that go dorsally and anteriorly, laterally, posteriorly and
laterally, and posteriorly and medially. Some axons are even more
complex. The axon illustrated in Figure 8B winds
throughout the ELa covering anterior to posterior, lateral to medial,
and dorsal to ventral extents of the nucleus.

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Figure 8.
Sample reconstructed NELL terminal fields in ELa.
Somata of postsynaptic cells are indicated by gray
circles, and terminals onto large cells are indicated by
arrows. The cross-sectional area of ELa varies greatly
over the dorsal-ventral extent of ELa (Figs.
12E, 13D), so the outlines chosen
are taken from the sections that best encompass the entire
reconstruction. The dorsal and ventral positions of axon segments along
the main axon trunk are coded by the line thickness,
where dorsal is thick and ventral is
thin. Scale bars: 100 µm.
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Because ELa large cells and small cells are adendritic, it was possible
to identify terminals from these reconstructed NELL cells onto large
and small cells (Fig. 8). They appear to be distributed over the
entirety of the ELa, from anterior to posterior, lateral to medial, and
dorsal to ventral. There are, however, long lengths of axon over which
we found no terminals. The two axons reconstructed here arose from the
contralateral NELL, but we did not see any qualitative difference in
two ipsilaterally projecting axons.
We next examined the linear branching pattern of the NELL axons. We
measured the length of each traced axon segment and mapped the
measurements onto a linear graph. The four NELL axons shown in Figure
9 had total lengths of 5, 5.5, 6.5, and 7 mm from the position of the first terminal within the ELa. In each
case, the first terminal was onto an ELa large cell, which was early in the projection of the axon through the ELa. This was followed by a
second large cell terminal over the next 1 mm of axon (one cell had two
additional large cell terminals). Then the axon traveled 3.5-5 mm from
the last large cell terminal before branching widely and contacting a
large number of small cells. The four axons in Figure 9 had 33, 44, 72, and 65 total small cell terminals. Few small cells are contacted early
in the winding of the axon though the ELa. The four axons in Figure 9
contacted only 0, 16, 10, and 16 small cells, respectively, before the
final arborization (these counts represent 0, 36, 14, and 25% of the
total number of small cell terminals). Thus, the signal traveling up
the NELL axon arrives first at a few ELa large cells and then, after a long winding axon with few terminals, at a large number of ELa small
cells distributed across the whole nucleus.

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Figure 9.
Linear reconstructions of four NELL axons and one
large cell. All segment lengths were measured and aligned end to end.
The horizontal position of any branch or terminal indicates its
measured distance from the first large cell terminal or, for the ELa
large cell, its distance from the soma. Vertical spacing is for
clarity. Filled circles indicate terminals onto large
cells, and open circles indicate terminals onto small
cells. Sizes of terminals are not to scale. The numbers
of terminals are listed at the right.
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ELa large cell projection patterns
In B. brachyistius, the ELa large cell somata are
located mainly deep in the nucleus, that is medially, ventrally, and
posteriorly, where the lateral lemniscus enters the ELa. B. niger has many more large cells than B. brachyistius,
and they are distributed more toward the superficial parts of the ELa.
We obtained six good intracellular fills of ELa large cells. Each large
cell had a round soma (8-14 µm in diameter; Fig.
10A,B),
as well as numerous cup-shaped terminals around small cells (Fig.
10C). All of the large cells appeared to be adendritic; we
saw no dye-filled processes off the soma except the axon, and all
terminals that we observed on large cells were somatic. The initial
segment of the large cell is thin (
1 µm) for ~25 µm, at which
point it widens to 2-3 µm.

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Figure 10.
ELa large cells and terminal. A,
Large cell filled by mass injection in the ELa. The adendritic soma is
oval (9 × 14 µm). The axon widens to 2-3 µm ~24 µm from
the soma (arrow). B, Large cell filled by
intracellular injection. The soma is round and ~14 µm in diameter.
The initial segment is ~27 µm, before the axon thickens to ~3
µm (arrow). (The axon briefly travels out of the plane
of section.) C, Cup-shaped terminal from large cell. The
target small cell is visible in neutral red stain, although such cells
are frequently completely obscured by the terminal. Scale bars:
A, B, 50 µm; C, 20 µm.
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By comparison with the NELL axons, reconstructed ELa large cells
project directly to the terminal field, with few branches (Fig.
11). The terminals tend to be in
restricted areas, either bands or patches in parts of the ELa up to 1 mm away. For example, the terminals of the cell in Figure
11A lie close to the two main axon branches of the
cell. The terminals of the cell in Figure 11C lie in a
cluster ~300 µm across, next to the lateral edge of the ELa. In one
case, there was a small terminal field close to the soma onto other
large cells (Fig. 11B).

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Figure 11.
Reconstructed ELa large cells. Somata of
postsynaptic small cells are indicated by gray circles.
The dorsal and ventral positions of axon segments along the main axon
trunk are coded by the line thickness, where dorsal is
thick and ventral is thin. Scale bars: 100 µm.
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We quantitatively reconstructed one large cell (the cell in Fig.
11A, reconstructed in Fig. 9). The total axon length
was <1 mm, far less than the length of the NELL axons.
Small cell projection patterns
To trace small cell axons, we injected biotinylated dextrans into
the ELa and the ELp. Dextrans are apparently taken up by axons and
somata in the vicinity of the injection and then transported both
anterogradely and retrogradely. The injection sites using Mr 3000 biotinylated dextrans were fairly
compact, 100-150 µm in diameter.
Injections into the ELa
We performed seven successful injections into the ELa (Fig.
12A). We observed
labeling in ELa large cells, small cells, and cell bodies in the NELL.
We also found fibers in the ELp (Fig. 12B-D). The border between the ELa and
the ELp is characterized by a soma-sparse central region (Fig.
12B, thin part of dotted line)
through which most of the fibers from the ELa enter the ELp. From there
they fan out radially and proceed in almost a straight line to the most
distal edge of the ELp (Fig. 12C,D). The axons
show varicosities at intervals along their length, which are presumably
en passant synaptic contacts, but they do not appear to
contact ELp somata directly. No other anatomical specializations suggestive of synapses were observed.

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Figure 12.
Injections of biotinylated dextrans into
the ELa label small cell axons into the ELp. A, Overview
of the ELa and injection site. At this dorsal level, the ELp is not
visible. The injection site is ~150 µm in diameter.
B, Section ~450 µm ventral to A. The
border between the ELa and the ELp is somewhat indistinct toward the
center (narrow dotted line), where the small cell axons enter the ELp. The boxed areas are magnified in
C and D. C, Medial small cell fibers in
the ELp. The fibers travel mostly radially toward the medial edge of
the ELp. D, Posterior small cell fibers in the ELp. The
fibers travel mostly radially toward the back of the ELp.
E, Summary of two experiments in which biotinylated dextrans were injected into the ELa.
i-viii, Horizontal sections of the ELa
and the ELp over a dorsal-ventral series. The approximate positions of
the sections are indicated in the inset. Figure
legend continues. Circles in the ELa represent the injection sites, and fibers in the ELp are the resulting small cell projection. In the first
experiment, the lateral injection (dotted circle) gave rise to lateral fibers (dotted). In the second
experiment, the medial injection (solid circle) gave
rise to the medial fibers (solid). L,
Lateral toral nucleus; MD, medial dorsal nucleus; OT, optic tectum; Tel, telencephalon;
VA, valvula. Scale bars: A, 800 µm;
B, 200 µm; C, D, 50 µm;
E, 500 µm for reconstructions, 1 mm for the
inset.
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The small cell projection from the ELa to the ELp is topographically
mapped. Restricted injections in the ELa tend to project to a
restricted corresponding part of the ELp. The results of two
experiments from two different preparations are superimposed in Figure
12E. An injection of biotinylated dextrans into the
medial ELa (Fig. 12E, solid circle) anterogradely
labeled axons in the medial ELp (solid fibers), whereas an injection
into the lateral ELa (Fig. 12E, dotted circle)
labeled axons in the lateral ELa (dotted fibers).
Injections into the ELp
We verified the results of the injections into the ELa using
retrograde transport from focal injections in the ELp. We performed seven successful injections, retrogradely labeling exclusively small
cell somata in the ELa (Fig.
13A). After one injection we counted several hundred small cell somata. The small cell somata appear
adendritic and round (5-7 µm in diameter; Fig. 13B). The small cell axons are thin and are directed toward the center of the
border between the ELa and the ELp. The axons appear smooth within the
boundaries of the ELa but display varicosities once they cross the
border into the ELp.

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Figure 13.
Injections of biotinylated dextrans into the ELp
label small cell bodies in the ELa. A, Injection site in
the ELp. The injection site (ij) is fairly anterior.
Small cell bodies are labeled in the ELa, visible as dark
spots. B, Close-up of the boxed
area in A showing six small cell somata.
C, Section of the ELp 100 µm dorsal to the injection
site in A. Fibers projecting radially to the edge of the
ELp are more easily visible here. D, Summary of two
experiments injecting biotinylated dextrans into the ELp. i-viii, Horizontal sections of the ELa
and the ELp over a dorsal-ventral series. The approximate positions of
the sections are indicated in the inset.
Circles in the ELp represent the injection sites, and
symbols in the ELa are the positions of retrogradely
labeled small cell somata. In the first experiment, the lateral
injection (solid circle) retrogradely labels lateral
small cell somata ( ). In the second experiment, the medial injection
(dashed circle with + in the center) retrogradely
labeled medial small cell somata (+). Scale bars: A, 200 µm; B, 20 µm; C, 100 µm;
D, 500 µm for reconstructions, 1 mm for the
inset.
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Focal injections of dye into the ELp highlight the organization of
small cell axons running in parallel from the center of the boundary
between the ELa and the ELp to the distal margins of the ELp. The
injection in Figure 13A was made in the anterior, lateral
half of the ELp, but fibers are filled out to the lateral-posterior margin of the nucleus, seen more easily 100 µm dorsal to the
injection site (Fig. 13C). From this we see that small cell
axons travel through the injection site, pick up the dextran, and
transport it both retrogradely back to the small cell soma in the ELa
and anterogradely on to the furthest extent of the axonal arborization at the edge of the ELp. All injections in the ELp show a similar effect.
The topographic mapping of the ELa onto the ELp is illustrated in
Figure 13D. An injection of biotinylated dextrans in the medial ELp (circle with +) retrogradely labeled small cell
somata in the medial ELa (+), whereas an injection into the lateral ELp (open circle) labeled small cell somata in the lateral ELp
(Fig. 13D, circles).
Putative small cell responses
Although we were unable to obtain anatomical confirmation with
intracellular labeling, we present here data from five putative small
cell recordings. In each case, the electrode tip was within the ELa,
but the activity pattern differed from the NELL axons and ELa large
cells already described.
For the presumed small cell presented in Figure
14A, we observed
brief spontaneous potentials and long spontaneous potentials. The brief
potentials were 0.33 ± 0.04 msec long (measured at half-height; n = 10). Some brief potentials were separated by as
little as 0.4 msec (e.g., Fig. 14A,
arrows). Spontaneous long potentials were 2.45 ± 0.31 msec long (measured at half-height; n = 8).

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Figure 14.
Recordings in ELa that may be small cells.
Recordings in A and B are from one cell
and in C and D are from two more.
A, Eleven sample traces in response to a 15 msec reverse
polarity square pulse (bottom trace). The unit had high
spontaneous activity in addition to potentials phase-locked to the
downward and upward edges of the stimulus. The unit showed two types of
activity, a brief potential (1) and a long
potential (2). Pairs of brief potentials may be
separated by less than the spike refractory period
(arrows). B, Averaged traces of activity
revealing differing time dependence of phase-locked potentials. The
downward edge of all stimuli is followed by a large, long potential
(latency, 2.75 msec). The upward edge is followed first by a brief
potential (latency, 2.15 msec) and then by a long potential (visible in the top two traces). For shorter-duration stimuli, the
responses to the upward edge are obscured (third trace),
but the brief potential emerges before the response to the downward
edge at the shortest duration stimulus (bottom trace,
arrow). C, Sample traces showing the effect of
amplitude on brief and long potentials in a different cell from
A and B. D, Sample traces from another
cell showing hyperpolarizing long potentials. This cell was held for 7 sec. The stimulus was 0.25 msec. The arrows indicate
what may be a brief potential.
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In addition to the spontaneous potentials, Figure 14A
shows brief and long potentials that were phase-locked to the stimulus, as can be seen better after averaging (Fig. 14B).
There was a large, long potential phase-locked to the leading, downward
edge of the stimulus (that is, originating from the contralateral NELL;
Fig. 14B). The large, long potential had a latency of
2.75 msec, fast rise time (0.25 msec, 20-80%), and a half-height
duration of ~5 msec. There was also a brief potential phase-locked to
the trailing, upward edge of the stimulus (that is, originating from
the ipsilateral NELL), which was paired with a small, long potential
(Fig. 14B, top two traces, arrows). The
brief potential had a half-height duration of 0.4 msec and a latency of
2.15 msec. For very short stimuli, the brief potential appeared before
the large, long potential (Fig. 14B, bottom
trace, arrow). Thus the two stimulus edges are inducing different
potentials to this unit at different latencies. No spikes were seen in
this recording.
A second unit shown in Figure 14C also had brief and long
potentials triggered by electrosensory stimuli, but the thresholds for
these potentials differed, again indicating at least two different inputs to the unit. For high-amplitude stimuli (Fig. 14C,
top group of traces), only a long potential was
visible. As the stimulus amplitude decreased, the long potential
occasionally failed (Fig. 14C, second and
third groups of traces), but the brief potential persisted. At very low stimulus amplitudes, the brief potential also
became smaller (Fig. 14C, bottom group of
traces). This suggests that there are multiple inputs to
this cell, with different kinetics and different amplitude
sensitivities. Temporal sensitivity could not be adequately tested in
this cell.
We interpret these recordings as follows: the brief potentials are
fast, excitatory inputs through electrotonic synapses from NELL axons;
and the long potentials are IPSPs from the large cells, which have
become inverted as an artifact of the recording condition. We expect
that the brief potentials are synaptic inputs, not distant spikes,
because the delays between them can be shorter than a typical action
potential refractory period. The brief duration is consistent with
electrotonic input from NELL cells, which are the only cell type in ELa
known to make electrotonic synapses (Mugnaini and Maler, 1987a
).
Although the synapses from large cells onto small cells contain GABA
(Mugnaini and Maler, 1987a
), three units had long potentials that were
depolarizing (two shown in Fig. 14). Recordings from two more units had
long potentials that were hyperpolarizing (Fig. 14D),
neither of which appeared to cause any rebound excitation. We suspect
that the synaptic potential flipped from hyperpolarizing to
depolarizing because the cell was damaged, or chloride was leaking out
of the electrode (also see Bell and Grant, 1989
). In fact, in the unit
illustrated in Figure 14C, the long potential was
hyperpolarizing for the first few seconds of recording, before the
responses could be stored to disk.
 |
DISCUSSION |
We have shown detailed anatomical reconstructions of two major
cell types in the analysis of temporal information in the mormyrid electric communication pathway. The axons from the NELL terminate on
one or two ELa large cells first and then travel extensively throughout
the nucleus, before ending in a large number of terminals onto ELa
small cells. The projection pattern of ELa large cells onto the small
cells is comparatively direct. We suggest that the long winding of the
NELL axon constitutes a delay line. The conduction velocity from the
NELL to the ELa up the lateral lemniscus has been estimated at 15 m/sec
(Enger et al., 1976
). If this speed were maintained in the ELa, then
axon lengths of 3.5-7 mm between large cell terminals and small cell
terminals would correspond to delays of 230-460 µsec. This is almost
certainly an underestimate, because of the method used to measure the
total axon length and because the axon diameter in the ELa is
frequently thinner than in the lateral lemniscus, particularly in the
axon branches to small cells.
Assuming that spike generation in the ELa large cell is rapid through
the electrotonic junctions, and that they have the same conduction
velocity as the NELL axons, the time delay to their terminals (1 mm)
would be ~60 µsec. We estimate that the synaptic delay from the
large cell to the small cell is 300 µsec. Therefore, the difference
in arrival times at the small cell between NELL axon and ELa large cell
inputs could range from
130 to +100 µsec. For the cell we
identified as possibly a small cell (Fig.
14A,B), the difference in latencies
between brief (NELL?) and long (large cell?) potentials was 600 µsec, which is close to our estimated latency difference. The EOD
duration for B. niger is ~250 µsec (Fig.
1B), which suggests that the NELL axon delay line is
in the behaviorally relevant range for computing the duration of EOD
stimuli.
These data support the hypothesis that the small cells act as
anti-co-incidence detectors, such that direct excitatory input from the
NELL triggers a small cell to fire, unless it is blocked by inhibitory
input from the large cell (Fig.
15A). With the inhibitory input originating from a different receptive field (such as from the
opposite side of the body), the small cell response would be blocked
over a particular range of square pulse (and EOD) durations, which
would depend solely on the length of the NELL axonal delay and the
duration of the large cell IPSP (Fig. 15B). Clearly,
conduction delays from more distant parts of the body (which may be as
great as 1 msec; Bell and Grant, 1989
), and between ipsilateral and contralateral NELLs would affect the range of potentially measurable pulse durations. However, the sharpness of the field potential in the
ELa (Szabo et al., 1979
) suggests that they are at least partially
compensated. We saw preliminary evidence that the excitatory and
inhibitory inputs can arrive from separate receptive fields (Fig. 14).
Because there is a range of different length delay lines (Fig. 9),
different small cells may be sensitive to different delays (Fig.
15C). Each NELL axon and ELa large cell distributes its
activity throughout the nucleus, as if the population of ELa small
cells were comparing knollenorgan activity over the entire body
surface.

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Figure 15.
Model of small cell response. A,
Example of inputs to the small cell. The leading edge of the stimulus
triggers activity in a patch of knollenorgans on the right side of the
body, which is relayed through an NELL cell and then an ELa large cell,
finally terminating on an ELa small cell with an IPSP of duration
tipsp. The trailing edge of the stimulus
triggers activity in a patch of knollenorgans on the left side of the
body, which is relayed through an NELL cell, finally terminating on the
small cell with an EPSP after a relative delay
(tdelay). (These patches of
knollenorgans are also presumably compared by a second small cell in
which the right side passes through the delay line, and the left side
passes through the large cell.) B, Hypothesized response
probability of the small cell in A for different
duration stimuli. Reverse polarity stimuli are treated as negative
duration, because the downward edge precedes the upward edge. Four
points on the response probability graph are illustrated in
traces i-iv. The upward edge of the stimulus
(middle traces, i-iv) leads to an IPSP of duration tipsp (bottom traces), and
the downward edge leads to an EPSP at a relative delay of
tdelay (top traces). The
small cell fires for long-duration, reverse polarity stimuli
(i) but not when the pulse duration is short
enough for the IPSP to overwhelm the EPSP (ii).
Responses are blanked for short-duration, normal polarity stimuli
(iii), but if the duration of the normal polarity
stimulus is sufficiently long, the EPSP will occur after the IPSP ends (iv). The cutoff point depends on
tdelay, and the range of blanked durations depends on tipsp.
C, Duration sensitivity of a family of ELa small cells
with different NELL delay lines. Short-duration stimuli will cause few
small cells to fire. As duration increases, more small cells are
recruited.
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Thus, we propose that pulse duration is represented by the number of
ELa small cells that are activated. Because this representation relies
only on the presence of activity in a subset of cells, the preservation
of precise spike times is no longer necessary. The projection of the
ELa small cells into the ELp maintains their topographic organization,
and the ELp neurons have large dendritic arbors oriented perpendicular
to the incoming axons (M. A. Friedman and C. D. Hopkins,
unpublished observations), so ELp cells may be well suited to integrate
the activity of many small cells.
However, a simple count of the number of active cells does not give an
unequivocal estimate of the pulse duration. If the pulse amplitude were
increased, the number of activated knollenorgans and NELL axons would
increase, which would recruit more ELa small cells. To avoid this
ambiguity between amplitude and duration, it would also be necessary to
take into account the pattern of activated cells in the ELa. This
pattern is likely to be complex, because the course of the NELL axon
and its widespread terminal fields suggest that duration sensitivity is
not mapped simply across the ELa.
Spatial analysis of knollenorgan information
One critical function of the knollenorgan system not
discussed so far is passive electrolocation of conspecific EODs.
Behavioral tests have indicated that B. brachyistius aligns
its body along current lines to swim toward a dipole source (Schluger
and Hopkins, 1987
), and the knollenorgans are the most likely
electroreceptors subserving that function. In a wide range of taxa, the
optic tectum contains spatial maps of different sensory modalities
(e.g., Knudsen, 1982
; Bartels et al., 1990
; Bodznick, 1991
; Stein and
Meredith, 1993
) and may be involved in orientation (Knudsen et al.,
1987
). Knollenorgan input to the optic tectum comes from the MV
(Wulliman and Northcutt, 1990
).
As we have shown (Fig. 6), the NELL projection to the MV is quite
different from the ELa. The NELL axons in the MV are thinner, the
terminals are smaller, and they do not appear to end on MV somata.
These anatomical features suggest that precise temporal information is
lost in the MV. One possibility therefore is that the MV may play a
role in analysis, not of temporal features of the EOD waveform, but
rather of spatial features of the pattern of excitation on different
parts of the body surface, which could be a cue for orientation.
Because the MV also receives input from the ELp
(Haugedé-Carré, 1979
) (Friedman and Hopkins, unpublished observations), the MV may also play a role in analysis of EOD waveform
or interpulse interval.
Comparative considerations
Mormyrid EOD durations range from 60 µsec in
Pollimyrus adspersus (Crawford, 1992
) to 20 msec in
Campylomormyrus numenius (Lovell et al., 1997
). Although
knollenorgans are broadly tuned to the fish's own EOD (Bass and
Hopkins, 1980
, 1984
; Hopkins, 1983
), they respond to the EODs of other
species (Hopkins, 1986
). Our results imply that NELL cells and ELa
large cells also respond generally. The only target of the ELa small
cells is the ELp, in which Amagai (1998)
found a class of units that
are bandpass-tuned to square pulses, with the range of best durations
from 0.1 to 10 msec. Thus it appears that the ELp, and probably the
population of ELa small cells, is generalized to respond to EODs from a
number of species, rather than being specialized to respond solely to the EODs of its own species. For the longest duration square pulses and
EODs, the NELL axon probably could not serve as a long enough delay
line, even with slower axon conduction velocity and slower channel
kinetics. Long-duration species may be forced to use another time delay
mechanism, such as inhibitory rebound, as has been proposed for bat
echo ranging (Park and Pollak, 1993
; Saitoh and Suga, 1995
).
There is interspecific variation in the neuroanatomy of the
knollenorgan pathway, even in the two species studied here. B. niger has approximately three times as many NELL somata as
B. brachyistius, and it also has many more ELa large cells
(data not shown). In addition, the two species differ in
calcium-binding protein expression; in B. niger, the ELa
large cells contain high levels of calretinin, but in B. brachyistius, they do not (Friedman and Kawasaki, 1997
). These
differences are unexpected, because the EODs of the two species are of
approximately similar duration and peak power content. These
differences may reflect some greater dependence on precise temporal
information in B. niger, such as for individual recognition.
Greater attention to behavioral and neuroanatomical differences between
mormyrid species will be necessary.
Comparison with other time-coding systems
We note that the organization of the NELL axon input to the ELa
contrasts sharply with the tidy organization of the auditory time-coding systems of the barn owl and the chick. In these, the nucleus magnocellularis makes a clear delay line projection across the
nucleus laminaris, with ipsilateral and contralateral inputs taking
different routes (Young and Rubel, 1983
; Carr, 1986
; Carr and Konishi,
1990
), strongly reminiscent of the model of Jeffress (1948)
for
converting temporal information into a place code. The laminaris
neurons act as co-incidence detectors to determine interaural time
differences (Carr and Konishi, 1990
; Overholt et al., 1992
; Joseph and
Hyson, 1993
), by a mechanism apparently involving a rapidly activating,
outward rectifier suppressing responses to sustained, rather than
transient, synaptic input (Reyes et al., 1996
).
In the phase-coding electrosensory pathway of Eigenmannia, a
South American gymnotiform fish, the projection is not as organized as
in the barn owl and appears superficially more similar to the knollenorgan system. Spherical cells in the ELL receive input from
T-unit electroreceptors, which encode temporal characteristics of
electrosensory stimuli by precise spike times. The projection of the
spherical cell to giant cells and small cells in layer VI of the torus
semicircularis is spatially restricted (Carr et al., 1986b
), just as
the ELa large cell projection is restricted. The layer VI giant cell
projects widely (Carr et al., 1986a
,b
), just as the NELL axon projects
widely. The layer VI small cells are sensitive to timing differences
between direct spherical cell inputs and indirect giant cell inputs
(Heiligenberg and Rose, 1985
). The delay line is proposed to be the
small cell dendrite, and one possible mechanism of co-incidence
detection is proposed to be attributable to channel inactivation
(Lytton, 1991
).
Both the barn owl and Eigenmannia compare two excitatory
inputs, whereas the mormyrid knollenorgan system compares an excitatory input with an inhibitory input (Fig. 15). This represents a novel solution to the problem of co-incidence detection.
 |
FOOTNOTES |
Received June 9, 1997; revised Nov. 7, 1997; accepted Nov. 17, 1997.
This work was supported by National Institutes of Mental Health (NIMH)
Grant MH37972 to C.D.H., Training Grant MH15793 from NIMH, and GM07469
from National Institutes of Health to M.A.F. We thank Satoshi Amagai
and Garry Harned for help with the experiments, Phil Stoddard and
Calvin Wong for help with histological procedures, and Margie Nelson
for the drawing of the mormyrid brain. We thank Ron Harris-Warrick,
Walter Metzner, Masashi Kawasaki, and an anonymous reviewer for
comments on this manuscript.
Correspondence should be addressed to Matthew Friedman, Department of
Neurobiology, Harvard Medical School, 220 Longwood Avenue, Boston, MA
02115.
 |
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