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The Journal of Neuroscience, June 1, 1998, 18(11):4314-4324
The Papilla Neglecta of Turtles: A Detector of Head Rotations
with Unique Sensory Coding Properties
Alan M.
Brichta1 and
Jay M.
Goldberg2
Departments of 1 Surgery (Otolaryngology, Head and Neck
Surgery) and 2 Pharmacological and Physiological Sciences,
University of Chicago, Chicago, Illinois 60637
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ABSTRACT |
The turtle papilla neglecta (PN) is a small organ lying in the
ventrolateral utricular wall between the posterior crista (PC) and the
utriculosaccular foramen. Innervated by a branch of the posterior
ampullary nerve, the organ is covered by a cupula extending only a
small distance into the endolymphatic space. Although most rotation-sensitive units in the posterior division of the eighth nerve
have sensory coding properties expected of PC fibers, a few have unique
properties. Intra-axonal labeling studies show that the former are PC
units and the latter are PN units. PC units are maximally responsive to
head rotations in the posterior canal plane and are sensitive to a
combination of angular velocity and angular acceleration. PN units
respond maximally to pitch rotations and are sensitive to a combination
of angular acceleration and angular jerk. A maximal response to pitches
can be related to the location of the PN, which allows it to sample
endolymph flow from both vertical semicircular canals. Differences in
response dynamics may reflect macromechanics. Because the cupula of
each vertical canal occludes the endolymphatic space, its displacement should be proportional to endolymph displacement. In contrast, the PN
cupula is probably coupled to endolymph flow by viscous forces, in
which case its displacement should be proportional to endolymph
velocity. In many vertebrates, the PN is similar to that seen in
turtles in its location and in the size and shape of its cupula, which
suggests that its function in these other species is also similar.
Key words:
vestibular nerve; membranous labyrinth; papilla neglecta; posterior crista; cupula; endolymph; sensory coding; macromechanics
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INTRODUCTION |
The papilla neglecta (PN) is a
labyrinthine organ present in fish, reptiles, birds, and some mammals
and innervated by a branch of the nerve supplying the posterior crista
(PC) (Baird, 1974 ; Lewis et al., 1985 ). In most vertebrates, the
papilla is a small, oval-shaped organ with 20-200 hair cells, covered
by a cupula, and located in the ventrolateral wall of the utriculus
between the posterior crista and the utriculosaccular foramen. A
different arrangement is seen in elasmobranchs, where the papilla or
macula as it is sometimes called is situated in or near a duct
connecting the posterior canal with the sacculus (Baird, 1974 ;
Corwin, 1978 ). In addition, the papilla in some elasmobranchs is
large, containing anywhere from 2500 to 260,000 hair cells (Corwin,
1978 ). Within amphibians, a papilla neglecta is present in apodans but
not in urodeles or anurans (Baird, 1974 ; Lombard and Bolt, 1979 ;
Fritzsch and Wake, 1988 ). It has been proposed that the papilla
neglecta in the latter animals has been transformed into the amphibian papilla, an auditory organ peculiar to amphibians (for review, see
Fritzsch and Wake, 1988 ).
Physiological studies in elasmobranchs indicate that the papilla
neglecta is sensitive to vibratory and auditory stimuli (Lowenstein and
Roberts, 1951 ; Fay et al., 1975 ; Corwin, 1981 ). Its function in other
species is unknown. We became interested in the organ while recording
from the posterior division of the eighth nerve in turtles. Most
rotation-sensitive afferents we encountered had sensory coding
properties similar to fibers innervating the posterior crista in other
species (Blanks and Precht, 1976 ). The units were maximally responsive
to head rotations in the plane of the posterior semicircular canal and
were sensitive to some combination of angular velocity and angular
acceleration. In addition, a few rotation-sensitive units had unique
properties, unlike any that had previously been described. The unusual
units responded maximally to rotations in the pitch plane, rather than
in the plane of one of the three semicircular canals. In addition, the
sensitivity of the unusual units fell between angular acceleration and
angular jerk. Although it has long been established that the response
dynamics of canal afferents depart from the expected velocity-sensitive
macromechanics of the semicircular canals (Fernández and
Goldberg, 1971 ), the departure in the unusual units was much larger
than had ever been encountered (Baird et al., 1988 ; Honrubia et al.,
1989 ; Boyle et al., 1991 ). Their unique properties suggested that the
unusual units innervated an organ other than a crista. The suggestion was confirmed by intra-axonal labeling, which showed that the more
typical units innervated the posterior crista, whereas the atypical
units supplied the papilla neglecta.
In this paper, we describe the morphology of the turtle PN, summarize
evidence identifying the atypical units as innervating this organ, and
compare the response properties of PN and PC afferents. We then
consider how the directional properties and response dynamics of PN
afferents are related to the location of the organ and to the size and
shape of its cupula.
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MATERIALS AND METHODS |
Animals. We used red-eared turtles,
Pseudemys (Trachemys) scripta
elegans, of either sex, weighing 150-350 gm with carapace lengths of 10-13 cm.
Anatomical procedures. Animals were killed by decapitation;
skin and soft tissue attached to the mandible were removed; and the
head was split midsagitally. The two half-heads were immersed in cool
(10°C) turtle Ringer's solution (in mM: 130 NaCl2, 4 KCl, 2.2 MgCl2, 2.8 CaCl2, and 5 HEPES, pH 7.6) (Art and Fettiplace, 1984 ). The brain and cranial nerves were removed, and the membranous labyrinth was exposed. The half-head was then placed in cool fixative containing 3% paraformaldehyde, 3% glutaraldehyde, and 3% sucrose in
0.1 M cacodylate buffer. In some cases, immersion fixation was supplemented by intralabyrinthine perfusion with the same fixative.
The ear was excised and transferred to fresh fixative for at least 2 hr, after which the membranous labyrinth was dissected free, rinsed in
0.1 M cacodylate buffer, post-fixed in 1% OsO4 for 1 hr, and then rinsed in buffer. At this point, tissue intended for
scanning electron microscopy went through four steps of the Osmium-Thiocarbohydrazide-Osmium method (Kelley et al., 1973 ). Specimens were then transferred through a series of graded ethanol concentrations.
Scanning and light microscopy. After ethanol dehydration,
tissue was dried using Peldri II (Ted Pella, Inc.) for scanning microscopy or plastic embedded for light microscopy. Tissue intended for scanning microscopy was sputter-coated with gold-palladium and
examined in a JEOL 840A scanning electron microscope. Plastic-embedded specimens were sectioned at 1-2 µm with a diamond histoknife on an
LKB-Wallac (Gaithersburg, MD) ultratome. Sections were transferred to
glass slides, stained with Richardson's solution (1% azure II, 2%
methylene blue, and 2% sodium borate) on a hot plate, and coverslipped.
Confocal microscopy. To visualize the cupulae of the PC and
the PN, unfixed labyrinths were injected with 0.1 ml
fluorescein-labeled wheat germ agglutinin (FITC-WGA) (Vector
Laboratories, Burlingame, CA). Combined with a fluorescent marker, WGA
lectin provides an effective staining method of the cupula, otoconia,
and otoconial membrane (Gil-Loyzaga et al., 1985 ). Within 10 min of the
injection into the common crus the cupulae showed an intense
florescence, whereas the surrounding tissue became only slightly
fluorescent. Small windows were cut into the membranous labyrinth to
provide unimpeded views. Care was taken not to dislodge the cupulae.
Fluorescent images were captured using a Molecular Dynamics (Sunnyvale,
CA) 2000 confocal microscope.
Surgical and recording procedures. A method similar to that
described by Crawford and Fettiplace (1978) was followed. After decapitation the head was midsagittally sectioned, and the left half-head was placed into fresh turtle Ringer's solution. To expose the dorsal surface of the posterior division of the eighth nerve, the
brainstem was blocked at the levels of the trigeminal nerve rostrally
and the glossopharyngeal nerve caudally and then pivoted 90° around
the seventh and eighth nerves. The isolated half-head was placed on its
lateral surface in a recording chamber. A moist gas mixture (95%
O2 and 5% CO2) was passed over the
preparation throughout the experiment. The recording chamber was
attached to a superstructure on a rotating device, the motion of which was controlled by a velocity servomechanism (Inland 823). By tilting the superstructure, the preparation could be placed in any desired orientation with respect to the rotation axis. Recording
microelectrodes were advanced by a screw micrometer drive attached to
the top of the recording chamber. For extracellular recordings,
micropipettes were filled with 3 M NaCl (20-40 M
impedance). Intra-axonal labeling was done with bevelled micropipettes
containing 4% biocytin (Molecular Probes, Eugene, OR) in 0.5 M KCl and 0.05 M Tris, pH 7.4, (40-80 M
impedance).
Physiological testing. Recordings were made from the
posterior division of the eighth nerve. Sensitivity to rotations,
tilts, and other linear forces was tested as in preceding studies
(Goldberg and Fernández, 1975 ). Acoustic sensitivity was examined
with 100-800 Hz tones delivered from a loudspeaker with intensities of
70-90 dB re: 0.0002 dyne/cm2 as measured by a sound
level meter placed near the preparation (Brüel and Kjær model
2203). Vibration sensitivity was tested by tapping the superstructure.
When monitored with an accelerometer (Brüel & Kjær model 4333),
the taps consisted of 100 Hz oscillations decaying over 10-20 cycles
with peak accelerations near ±1 g. Only rotation-sensitive units were
studied in detail because, as described in Results, they were the only
fibers found to innervate the PC and PN.
Rotation-sensitive units were characterized as follows. The head was
kept in a position so that the horizontal (rotation) plane corresponded
to the pitch plane of the specimen, 45° from the posterior canal
plane. A 5 sec sample of background discharge was recorded, as was the
response to a 0.3 Hz sinusoidal head rotation. In some units, responses
were obtained to rotational sinusoids at frequencies spaced a
half-decade apart from 0.1 to 3.0 Hz. Peak head velocities could be as
high as 160°/sec (0.1 Hz), 80°/sec (0.3 Hz), 40°/sec (1.0 Hz),
and 20°/sec (3.0 Hz). The number of cycles ranged from eight (0.1 Hz)
to 256 (3.0 Hz). Care was taken to keep the rotation amplitude
sufficiently small so that the responses appeared linear with no signs
of excitatory saturation and, in units with an appreciable background
discharge, no inhibitory silencing. Fourier analysis was used to
extract the fundamental component of the response. A similar analysis was done on the head velocity signal from the tachometer of the servomechanism. Gains were obtained as the ratio of the response amplitude (in spikes per second) to the head velocity amplitude (in
degrees per second). For the phase (in degrees), the head velocity
phase was subtracted from the response phase; positive phases
correspond to phase leads. Further testing was only done on
extracellularly recorded units.
Some units were studied with velocity trapezoids, consisting of a
stationary period (T1), an ascending velocity ramp (T2), a velocity
plateau (T3), a descending velocity ramp (T4), and a final stationary
period (T5); T1 = T3 = T5 = 5 sec; T2 = T4 = 1 or 2 sec. Responses to 8-100 consecutive rotations were averaged. Maximum velocities used were 40°/sec for 1 sec ramps and 80°/sec for 2 sec ramps. Actual velocities were set to keep each unit within a
linear range and were as small as 2.5°/sec.
Directional properties of units were determined by comparing the
responses to 0.3 or 1.0 Hz rotation sinusoids with the head in
different tilt positions relative to the rotation plane.
Intracellular labeling. After physiological testing, impaled
axons were iontophoretically injected with biocytin. Injection currents
were 5 nA, alternating every 500 msec between anodal and cathodal
steps. Every 30 sec the resting potential and the size of the action
potential were measured. Biocytin injections continued for a total of
10 min (50 nA · min) or until the resting potential fell below 10
mV. We did not attempt to label more than one rotation-sensitive
afferent per animal. After a minimum of 2 hr, the tissue was fixed with
2.5% paraformaldehyde and 2.5% glutaraldehyde in 0.1 M
phosphate buffer, pH 7.4. The membranous labyrinth and attached nerve
branches and brainstem were dissected in toto and placed in
fresh fixative overnight, moved to a 30% sucrose solution in phosphate
buffer for 12 hr, and then embedded in 12% gelatin. The block was
hardened in fresh fixative containing 30% sucrose for not <4 hr,
rinsed in fresh 30% phosphate buffer, and serially sectioned at 40 µm on a freezing microtome. To visualize biocytin, sections were
incubated in a solution of avidin-biotin-HRP complex (1:50 dilution,
Vector) and 0.1% Triton X-100 in 0.1 M phosphate buffer,
pH 7.4, for 3 hr, followed by a presoak in 0.05% diaminobenzidine for
30 min to which 0.03% H2O2 was added for 4 min. The sections were rinsed, mounted, dehydrated through graded concentrations of ethanol, and then coverslipped.
Labeled material was examined with a 100× oil immersion,
planapochromatic objective (numerical aperture, 1.3) under bright-field illumination. Axons and peripheral arborizations were drawn from serial
sections with the aid of a drawing tube (total magnification, 1650×).
Inversion of fractional transfer functions. We needed to
obtain the time-domain responses corresponding to a transfer function consisting of a conventional part,
H1(s) = s/(s + )(s + ), multiplied by a fractional operator,
H2(s) = sk. From elementary methods, the inverse
of H1(s) is
h1(t) = [1/( )][
exp( t) exp( t)]. The
time-domain equivalent of sk is a fractional
derivative, so the overall transfer function has a time-domain
representation, h(t) = dkh1(t)/dtk.
The fractional derivative of an exponential,
dkexp(±
t)/dtk = [exp(±
t)/xk] *( k, ± t), where * is the entire incomplete function, which was evaluated from its series expansion (Oldham and Spanier, 1974 ; Spanier and Oldham, 1987 ).
Normalized measures of discharge regularity. The coefficient
of variation (cv), which provides a measure of discharge regularity, is
a function of discharge rate (Goldberg and Fernández, 1971 ; Goldberg et al., 1984 ). To obtain a normalized cv independent of
discharge rate, we followed a previously described procedure (Goldberg
et al., 1984 ) and calculated a normalized cv*, the cv appropriate to a
discharge rate of 20 spikes/sec. This rate was chosen because it was
near the mean value obtained from a large sample of rotation-sensitive
units.
Determination of response vectors. Responses to 0.3 or 1.0 Hz sinusoidal head rotations were compared after the preparation had
been tilted to each of several positions from our standard position.
Two tilt planes were used. The first or xy plane explored rotations ranging from pure pitch (x-axis) to pure roll
(y-axis). Rotations in the xz plane
included pure pitch (x-axis) and pure yaw
(z-axis). The gains and phases to the various rotations were used to calculate a response vector of unit length,
Vmax = (x, y, z), giving the
orientation with respect to the head of the rotation axis leading to
maximal responses (Hess and Angelaki, 1993 ). Positive values of the
Vmax coordinates indicate excitation by downward
pitches (x), leftward (ipsilateral) rolls
(y), and counterclockwise (leftward or ipsilateral)
yaws (z).
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RESULTS |
Structure of the papilla neglecta
In turtles, the PN is an epithelial mound lying in the
ventrolateral wall of the utriculus, anterior to the PC and immediately posterior to the utriculosaccular foramen and the entrance of the
horizontal canal duct (Figs. 1,
PN; 2A,B).
The mound consists of a neuroepithelium, surrounded by a transitional
epithelium (Fig. 2C). A small nerve branch arising from the
dorsal surface of the posterior ampullary nerve, midway along its
length innervates the neuroepithelium (Fig. 1B).
There are 20-30 myelinated nerve fibers in the PN branch (mean ± SD, 26 ± 4; n = 5) and these range in diameter
from 1.8 to 8 µm. In comparison, there are ~800 fibers innervating
the PC (Brichta and Peterson, 1994 ).

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Figure 1.
Medial view of the turtle membranous labyrinth and
eighth nerve stained for myelin with Sudan Black B (Rasmussen, 1961 ).
A, B, arrowhead, Location
of the papilla neglecta (PN) in the ventrolateral
wall of the posterior utriculus, below the common crus
(C), anterior to the posterior crista
(PC), and posterior to the utriculosaccular foramen (*).
Arrow points to the small branch of the posterior
ampullary nerve innervating the PN. A, Anterior crista;
B, basilar papilla; H, horizontal crista;
L, lagena; S, sacculus;
PC, posterior crista; U, utriculus. Scale
bars: A, 1 mm; B, 250 µm.
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Figure 2.
A, B, Scanning electron micrographs
of the posterior crista (PC) and papilla neglecta
(PN). A, arrowhead, Location of
the PN in the wall of the utriculus, posterior to the
utriculosaccular foramen (*). The entrance of horizontal canal duct
(H) into the utriculus is indicated by
the arrow. B, PN is a mound consisting of a
neuroepithelium surrounded by a transitional epithelium. Hair bundles
have been partially removed by ultrasonication to allow an unimpeded
view of the epithelial surface. C, Semithin section of
the PN. The organ consists of transitional cells, supporting cells, and
hair cells. In this section only type II hair cells are observed. Scale
bars: A, 100 µm;
B, C, 50 µm.
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The neuroepithelium was visualized in scanning electron micrographs
(Fig. 2A,B), in which it measured 100 × 150 × 25 µm and contained 175-225 hair cells (Fig.
2B). Hair bundles have a nearly identical
orientation, similar to that seen in the PC. The kinocilium is located
on the side of the hair cell facing toward the posterior canal ampulla
and away from the utriculus. As discerned in semithin sections (Fig.
2C), most PN hair cells are cylindrically shaped and are
presumed to be type II cells. In semithin sections of the PC,
type I hair cells can be recognized because their basolateral surfaces
are surrounded by calyx endings. Presumed type I cells were not seen in
two serially examined PN.
FITC-WGA was used to visualize the PC (Fig.
3A) and the PN cupulae (Fig.
3B). As is especially clear in Figure 3B, the
cupulae were intensely stained by the lectin, whereas the surrounding epithelium was barely fluorescent. Consistent with previous accounts (Steinhausen, 1931 ; Hillman and McLaren, 1979 ), the PC cupula extends
from the crista to the ampullary roof and occludes the endolymphatic
space (Fig. 3A). In contrast, the PN cupula reaches only
60-70 µm into the utricular lumen (Fig. 3B) the diameter of which is 500 µm (Fig. 1A,B). Because the PN
cupula does not occlude the lumen, endolymph is free to move over and
around it. Otoconia are not present on or near either cupula.

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Figure 3.
Confocal images of the cupulae of the PC and PN
stained with FITC-WGA. Each image represents a superimposition of 20 (A) and 8 (B) confocal
sections taken at steps of 5 µm. A, PC cupula extends
from the crista surface (bottom) to the ampullary roof
(top, arrowheads), forming a partition occluding
endolymph flow within the posterior ampulla. Less florescence is seen
over the middle of the PC (*), where the cupula is relatively thin.
B, PN cupula is 35 µm at its thickest point
(arrowhead) and may be seen to protrude into the
endolymphatic space from the wall of the utricular sac (*). When the
height of the neuroepithelium is considered (Fig. 2C),
the cupula extends 60-70 µm into the lumen of the posterior
utriculus. Scale bars: A, B, 50 µm.
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Labeling of physiologically characterized axons
A total of 58 rotation-sensitive units were labeled in the present
study. Of these, 54 innervated the PC, and four supplied the PN.
Informal testing (see Materials and Methods) indicated that
rotation-sensitive units did not respond to head tilts, to centrifugal
forces, or to auditory or vibrational stimulation. No
rotation-sensitive unit was traced to any other organ innervated by the
posterior division of the eighth nerve, including the lagena, the
saccular macula, or the basilar papilla. Another 40 auditory, vibration-sensitive, and/or tilt-sensitive units were labeled. None of
them went to the PC or the PN.
As illustrated by an intracellularly labeled axon (Fig.
4B), PN fibers are
concentrated on the dorsomedial surface of the ampullary nerve. On
reaching the PN branch, they turn sharply in a dorsal direction to exit
the main nerve. In contrast, PC fibers (Fig. 4A)
continue along the posterior ampullary nerve to reach the posterior
crista. Only two of the four labeled PN fibers were sufficiently
labeled to reconstruct their terminal arbors within the papilla. An
example is seen in Figure 4C. As was also the case for the
other reconstructed arbor, there was an extensive terminal tree
containing bouton endings and innervating a large fraction of the
neuroepithelium. A description of the labeled PC units will be
presented elsewhere (A. M. Brichta and J. M. Goldberg,
unpublished observations).

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Figure 4.
Reconstructions of two rotation-sensitive axons,
intracellularly labeled with biocytin. A, This axon
follows the posterior ampullary nerve to the posterior crista
(PC). As was the case for another 53 labeled fibers
traced to the PC, the axon was sensitive to a combination of angular
velocity and angular acceleration. B, This axon leaves
the posterior ampullary nerve and runs in a small nerve branch to the
papilla neglecta (PN). A total of four labeled
fibers traced to the PN were sensitive to a combination of angular
acceleration and angular jerk. C, Reconstruction of the
terminal field of the axon in B. The terminal field
extends almost the entire length of the PN. Scale bars:
A, B, 20 µm.
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Identification and discharge properties of PN and PC fibers
In addition to the 58 labeled units, there were 585 extracellularly recorded, rotation-sensitive units in the study. All of them were tested with 0.3 Hz sinusoidal head rotations (Fig.
5). Extracellular units fell into two
distinct groups, a low-phase group with phase leads 91° and a
high-phase group with phase leads 104°. Identification of the
low-phase group as PC units and the high-phase group as PN units is
based on the phases of labeled units. In particular, phases of the 54 labeled PC units ranged from 5-91°; those of the four labeled PN
units, from 125-146°. The bimodal shape of the extracellular
distribution reinforces the conclusion. Among the extracellular units,
the high-phase group made up 33 of 585 or 5.6% of the extracellular
sample, slightly larger than the 3.1% expected from the relative
numbers of PN and PC fibers.

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Figure 5.
Based on the phase of their response to 0.3 Hz
sinusoidal rotations, axons in the posterior ampullary nerve can be
distinguished into two groups: low phase group ( 91°, dashed
outline, n = 552) and high phase group
( 104°, solid outline, n = 33).
Intra-axonally labeled fibers traced to the posterior crista
(PC) fell into the low-phase group (light
shading, n = 54), whereas labeled fibers
traced to the papilla neglecta (PN) fell into the
high-phase group (n = 4, dark
shading).
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PN and PC fibers had similar background discharges with mean (±SD)
values for the extracellular samples of 18.3 ± 12.7 (PC units)
and 19.2 ± 9.8 spikes/sec (PN units). The normalized cv* varied
from <0.2 to 1.0 in both groups. In other populations (Baird et al.,
1988 ; Honrubia et al., 1989 ), including the present PC population
(Brichta and Goldberg, 1996 ), rotational gain and phase both increase
with cv*. The same is true for PN units. Gains at 0.3 Hz were fit by a
power law, gain = a (cv*)b, with
a = 0.65 ± 0.16 spikes per sec/degrees per sec
and b = 0.91 ± 0.29 (n = 31;
p < 0.005). Phases at the same frequency were fit by a
semilogarithmic relation, phase = a + b
log10cv*, with a = 148.1 ± 3.8° and
b = 18.8 ± 10.9° (p < 0.10). Although they were not included in the calculations, points for
the four labeled PN units were close to the regression lines. Points
for the extracellular PN units did not fall into distinct groups based on their cv*, gain, or phase.
Response dynamics
PC and PN units differ in their response dynamics. This can be
seen in Figure 6, which compares Bode
plots for 18 PN and 13 PC units. The frequency range only extends down
to 0.1 Hz, because many PN units became virtually unresponsive at lower
frequencies. Results were available for PC units at lower frequencies,
typically down to 0.01 Hz.

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Figure 6.
Responses of PC (dashed lines,
n = 13) and PN (solid lines,
n = 18) units to sinusoidal head rotations, 0.1-3
Hz. Individual units are characterized by their gains in spikes per
second/degrees per second (A,
B) and phase leads re: head velocity in degrees
(C). PN units became insensitive at frequencies
<0.1 Hz. A, Gains of PN units increase ~100-fold as
frequency increases from 0.1 to 3 Hz. B, In contrast,
gains of PC units increase <10-fold over the same frequency range.
C, Throughout the frequency range, PN phases are larger
and more tightly distributed than PC phases. PN phases decline by 50°
between 0.3 and 3 Hz. A similar frequency-dependent decline is seen in
those PC units with large phases at 0.1 and 0.3 Hz. For other PC units,
phase remains nearly constant >0.3 Hz. D, The ratio of
gains at 0.1 Hz and 1.0 Hz is plotted versus the phase lead at 0.3 Hz.
Straight line, Expected relation for a fractional
(sk) operator with
letters indicating the points corresponding to velocity
(k = 0, V), acceleration
(k = 1, A), and jerk
(k = 2, J) sensitivity.
intra, extra, Intracellularly labeled and
extracellularly recorded units, respectively.
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Response dynamics are relatively uniform in PN units. This is indicated
by the similarity in their gain slopes when plotted in double
logarithmic coordinates (Fig. 6A) and by the
similarity in their phases at single frequencies (Fig. 6C).
For almost all PN units, gain increases 100- to 150-fold between 0.1 and 3 Hz, and phase curves vary by only 30° at any particular
frequency. In contrast, the gain slopes of PC units vary eightfold, and
their phase curves differ by almost 90° at 0.1 and 0.3 Hz (Fig.
6B,C). The phase leads of PN units decline as
frequency increases (Fig. 6C). Most PC units reach a nearly
constant phase at frequencies of 0.3 Hz. The only PC units to show a
frequency-dependent phase decline are units with large phase leads at
0.1 and 0.3 Hz.
Data from Figure 6A-C are replotted in Figure
6D in terms of the relation between the gain slopes
and phases for individual units. Most of the points fall close to the
straight line expected of fractional (sk)
operators. The points corresponding to angular velocity
(V), angular acceleration
(A), and angular jerk (J)
encoding are indicated. PN units encode between A and
J, whereas PC units encode between V and
A (Fig. 6D). To verify this
interpretation, we used rotation trapezoids with 1 or 2 sec ramps.
Figure 7 shows responses for three PC
units (Fig. 7A-C) and two PN units (Fig. 7D,E).
The first PC unit (Fig. 7A) is velocity-sensitive. Responses
during the ramps grow linearly, paralleling angular velocity, and
response declines during the following constant velocity periods are
exponential and slow. The second PC unit (Fig. 7B) encodes
between V and A. During the leading (excitatory)
ramp, the response curve is concave downward; during the trailing
(inhibitory) ramp, it is concave upward. On transition to constant
velocity, responses return rapidly to the baseline, and there is a
suggestion of a response reversal. These trends are exaggerated in the
third PC unit (Fig. 7C), which encodes near A.
Responses rapidly approach their maxima during the ramps and response
reversals are evident after the ramps. Trends are even more exaggerated
in the two PN units (Fig. 7D,E). Maximum responses occur
during the first 0.1 sec bin of each ramp, and the response declines to
10-25% of maximum during the next 0.9 sec. Immediately after each
ramp, the response reverses and rapidly approaches the baseline from
the opposite direction.

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Figure 7.
Rotation trapezoids with 1 sec leading and
trailing ramps (bars, horizontal axes)
were used to study response dynamics of PC (A, B, C) and
PN (D, E) units. Shaded histograms,
Actual responses; curved lines, best-fitting trapezoid
responses obtained by inverting text equation 1. The three PC units are
arranged to show sensitivities ranging from near velocity to near
acceleration. A, Velocity-sensitive PC unit has a
response most closely resembling the velocity trapezoid.
B, PC unit encoding midway between velocity and
acceleration. C, Near acceleration-sensitive PC unit the
response of which parallels differentiated version of velocity
trapezoid. D, E, Two PN units encode
between acceleration and jerk. F, Comparison of
fractional exponent (k) values giving
best-fitting trapezoid responses and the 0.3 Hz sinusoidal phases for
13 units. Solid symbols, PN; open
symbols, PC. Circles, 1 sec ramps;
squares, 2 sec ramps. For one PN unit, trapezoids with 1 sec and 2 sec ramps were both tested. Straight line,
Expected relation between k (ordinate)
and sinusoidal phase (abscissa) derived from text
Equation 1.
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Actual responses were compared with theoretical responses obtained by
inverting the transfer function:
|
(1a)
|
where
|
(1b)
|
gV is a midband velocity gain,
TP(s) is a second-order torsion pendulum model
with = 0.39 sec 1 and = 75 sec 1, and sk is a
fractional velocity operator. To determine , we used a subset of the
PC units with the smallest phase leads and found the frequency at which
their mean phase curve crossed 45°. was taken to be the lowest
rate constant of the series solution to the Navier-Stokes
equation for a circular tube of radius, a. The formula is = j0,12 /a2,
where j0,1 = 2.4048 is the first zero of the
J0 Bessel function (Batchelor, 1967 , p. 194);
= 1 × 10 2 cm2/sec is
the kinematic viscosity of endolymph, which can be assumed equal to
that of water (Money et al., 1971 ). To account for variations in the
radius, was calculated as the average for 20 equally spaced points
around the entire posterior canal ring.
In fitting individual responses, only gV and
k were allowed to vary. Equation 1 provides reasonably good
fits to the trapezoid responses (Fig. 7) with the possible exception
that the reversed responses of Figure 7, B and C,
are underestimated. Of particular interest are the values of
k providing best fits, because these exponents provide a
convenient way to summarize the response dynamics of different units.
In particular, k = 0 corresponds to V
encoding; k = 0.5, halfway between V and
A encoding; k = 1.0 corresponds to
A encoding; and k = 1.5, halfway between A
and J encoding.
Trapezoid data were available for 10 PC and three PN units. Figure
7F compares the values of k, determined by
fitting the trapezoid responses of the 13 units, to the phases of their
0.3 Hz sinusoidal responses. The straight line is the relation expected from Equation 1. The values of k for PC units range from
near zero to 0.8; those for the three PN units average 1.47 (range, 1.37-1.55). Results are consistent with the conclusion that PC units
encode between V and A, whereas PN units encode
halfway between A and J.
Directional properties
The directional properties of PN and PC units differed. This can
be seen by comparing the sinusoidal responses of two such units for
xy tilts between 0° (pure pitch) and 90° (pure roll) (Fig. 8). The reversal point for the PC
unit is near 50°, whereas that for the PN unit is >90°. Combining
the xy results (Fig. 8) with xz results (data not
shown) allowed us to compute Vmax response vectors for the two units. Normalized (x, y, z) coordinates were ( 0.74, 0.65, 0.17) for the PC unit. The signs of the x and
y components imply that the unit was excited by upward
pitches and ipsilateral rolls. x and y
coordinates are almost equal in size, indicating that the unit was
almost equally sensitive to pitch and roll rotations; the small size of
the z component implies a weak sensitivity of yaw rotations.
The vector is nearly orthogonal to the plane of the posterior canal
(Fig. 9A). It follows that the
PC unit is maximally sensitive to rotations near the canal plane.

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Figure 8.
Responses of a PC unit
(A-C) and a PN unit (F-H)
as the preparation was tilted so that a 1 Hz sinusoidal rotation was a
pitch at 0° tilt and a roll at 90° tilt. The response reverses
polarity near 50° in the PC unit and between 90 and 120° in the PN
unit. Responses were collected along two orthogonal tilt axes. The
corresponding gains and phases were used to calculate response vectors
for each unit. D, E, Normalized gains and phases of the
responses plotted as a function of tilt angle for the two units. Gain
is normalized to unity and phase to 0° when the rotation axis and the
calculated response vector coincide. Curves are expected
gains and phases calculated from best-fitting response vectors.
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Figure 9.
Response vectors for eight PN (solid
lines) and 25 PC units (dashed lines) from left
ear. Each vector indicates a head-fixed rotation axis. Rotations in the
plane perpendicular to the axis give maximal responses for the
particular unit. Excitatory directions obtained from the right-hand
rule with all vectors pointing away from head. Thick
lines inside head (top), Silhouette of the two
vertical canals. A, Orientation of vectors in the
horizontal plane indicate relative sensitivities to rotations around
pitch (X) and roll
(Y) axes. PC units respond to rotations in
the plane of the posterior canal and are almost equally excited by
ipsilateral rolls and upward pitches. PN units respond to rotations in
the pitch plane and are excited by upward pitches. B,
Orientation of vectors indicate relative sensitivities to rotations
around pitch (X) and yaw
(Z) axes. Both PC and PN units are much more
sensitive to pitches. Although the yaw sensitivity is small for both
groups, PC units may be excited by ipsilateral and PN units by
contralateral yaw rotations.
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Coordinates for the PN unit were ( 0.91, 0.14, 0.39). The large
size of the x (compared with the y) component
means that the unit is much more sensitive to pitches than to rolls.
Nose-up pitches are excitatory. A large yaw (z) sensitivity
was peculiar to this and to another PN unit encountered in the same
preparation.
Directional properties were determined in eight PN units and 25 PC
units. Rotations in both the xy and xz planes
were studied in 13 units (seven PN and six PC) and in one or the other
plane in another 20 units (one PN and 19 PC). Results for the 13 units studied in both planes gave the following mean (±SE)
Vmax coordinates of ( 0.721 ± 0.022, 0.673 ± 0.016, 0.168 ± 0.024) for PC units and
( 0.989 ± 0.025, 0.050 ± 0.114, 0.127 ± 0.087) for
PN units. All 33 units were used in constructing vector diagrams (Fig.
9A,B). The orientation of its response vector in the
horizontal (xy) plane reflects the relative sensitivities of
each unit to pitches and rolls (Fig. 9A) The ratio of pitch
to roll sensitivity had a mean (±SE) of 1.1 ± 0.10 for 16 PC
units and 7.4 ± 1.9 for eight PN units. Relative sensitivities to
pitch and yaw rotations, indicated by the vector orientations in the
frontal (xz) plane, are similar for the two groups of units,
but the groups differ in the signs of their z components
(Fig. 9B). Mean (±SE) angles with the horizontal in the
xz plane were 16.1 ± 2.2° (11 PC units) and
7.7 ± 4.9° (seven PN units). The negative mean value for the
PN units, although suggesting that they might be excited by
contralateral yaws, is small and not statistically significant
(t test, p > 0.2)
 |
DISCUSSION |
Although the PN is widely distributed among vertebrates, its
function has remained obscure. Previous functional studies had been
confined to elasmobranchs, in which the PN is a vibratory or auditory
organ (Lowenstein and Roberts, 1951 ; Fay et al., 1975 ; Corwin, 1981 ).
In contrast, our study shows that the PN in turtles resembles the PC
(and the other two cristae) in detecting angular head rotations,
although at the same time differing from the cristae in its response
dynamics and directional properties. In the following sections, we
relate the distinctive properties of the turtle PN to its location and
to the size and shape of its cupula. This puts us in a position to
speculate about the function of the organ in other vertebrates in which
there is relevant morphological, but no functional, information.
Response dynamics
PC afferents respond to some combination of angular velocity and
angular acceleration, whereas PN units encode almost halfway between
angular acceleration and angular jerk. To a first approximation, PN
responses can be considered a differentiated version of PC responses.
We now argue that the differences in response dynamics can be explained
by the macromechanics governing the bulk displacements of the two
cupulae. The PC cupula extends to the vault of the ampulla, thereby
occluding the ampullary lumen. Angular head movements result in an
oppositely directed motion of the endolymph within the posterior canal
and a pressure difference across the PC cupula. Assuming that there is
no bulging of the ampullary walls, fluid continuity requires that the
bulk displacements of the PC cupula and the endolymph are equal. From
its location and size, the PN cupula should stick into the endolymph
fluid stream without occluding it. The cupula is assumed to be
displaced by fluid flow originating in the vertical semicircular canals
(see Directional properties). Fluid forces are likely to be viscous and
these should be proportional to fluid velocity. Assuming the elastic
restoring forces were acting on the PN cupula, its displacement would
be proportional to fluid velocity and hence, would be a differentiated
version of PC cupular displacement.
To consider these ideas in more detail, we used a model (Fig.
10, VN) originally
developed by van Netten (1991) (van Netten and Kroese, 1987 ) to account
for the dynamics of cupular motion in lateral line canal organs. The
fluid force acting on the cupula is calculated from Stokes' analysis
of fluid flow past a vibrating sphere. It is assumed that the only
restoring force on the cupula is its elastic coupling to the
neuroepithelium, presumably contributed by the bending stiffness of the
hair bundles. The VN transfer function gives PN cupular displacement
relative to endolymph displacement. To obtain a transfer function (PM)
relating PN cupular displacement to angular head velocity, we multiply
VN by TP, the transfer function (see Eq. 1) relating endolymph flow in
the semicircular canals to head velocity. The overall model for PN
cupular displacement is PM = VN * TP.

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Figure 10.
Mean Bode plots for three unit samples are
compared with three theoretical transfer functions. Unit samples: all
PC bouton units (n = 30), the PC bouton units with
the largest phase leads at 0.3 Hz (n = 7), and PN
units (n = 18). Theoretical transfer functions:
TP (torsion-pendulum model), Expected endolymph
displacement for semicircular canals re: angular head velocity (see
Equation 1b in Results for parameters). VN, expected PN
cupular displacement re: endolymph displacement, was calculated from
Equation 15 (van Netten, 1991 ) with viscosity, µ = 1.0 × 10 2 gm/cm · sec, density, = 1.0 gm/cm3; PN cupular radius, a = 6 × 10 3 cm; and PN cupular elasticity,
S = 26 dynes/cm. PM, Expected
displacement of PN cupula re: angular head velocity was obtained from
PM = TP * VN.
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Figure 10 compares the behavior of the PM model with the mean
response dynamics of PN afferents. Over the frequency range, 0.01-3
Hz, VN can be simulated by an sk
operator, k = 1.05, so that PM is close to a
differentiated version of TP. The PN afferent gain curve is steeper and
the PN afferent phase lead is larger than predicted from PM. Similar
discrepancies are seen between PC afferent discharge and TP, the
expected mechanical response of the PC cupula. Presumably, the
discrepancies for both organs reflect transduction stages between
macromechanics and afferent discharge (Baird et al., 1988 ; Boyle et
al., 1991 ). In the case of the mean PC curve based on all bouton
afferents (Fig. 10), the discrepancy can be described by an
sk operator, k = 0.27, which predicts a constant phase discrepancy of 24° across
frequencies. For PN units and for the most phasic PC bouton units, an
sk operator will not suffice, because
phase discrepancies decline with increasing frequency. Because their
phase curves parallel one another, it might be supposed that similar
transduction mechanisms are responsible for the discrepancies in PN and
the most phasic PC units.
Directional properties
The PN is located between the entrances of the anterior and
posterior ampullae into the utriculus and immediately underneath the
crus commune (Figs. 1, 11). Because of
its location, the PN is in the direct line of endolymph flow from the
anterior canal (AC) and posterior canal (PC). A maximal response to
pitches is easily explained. During pitches the AC and PC flows will
reinforce one another (Fig. 11A), whereas during
rolls the two flows will cancel (Fig. 11B). Hair
bundle orientation is consistent with both the PN and PC being excited
by upward pitches. The PN is relatively insensitive to yaw rotations. A
possible reason is that the horizontal canal (HC) duct joins the
utriculus in front of the PN, so the latter is not particularly well
located to sample HC endolymph flow. Figure 11C illustrates
ipsilateral (utriculofugal) HC endolymph flow during contralateral yaw
rotations. The flow should displace the PN cupula in an excitatory
(posterior) direction as the streamlines spread out from the HC canal
duct into the enlarged space of the utriculus. Consistent with this
prediction, our data suggest that contralateral yaws have a small
excitatory effect on PN units.

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Figure 11.
The papilla neglecta (PN)
is suitably positioned to detect flow from both the anterior
(AC) and posterior (PC) vertical canals,
seen in silhouette in A and B.
Arrows with open arrowheads, top, Head
rotations. Solid-headed arrows inside membranous
labyrinth, Directions of endolymph flow. Shaded circle,
Location of PN. A, An upward pitch leads to
utriculopetal flow in AC and utriculofugal flow in PC. The AC is
inhibited, and the PC is excited. AC and PC flows are in same direction
in vicinity of PN. Because the hair bundle orientation is the same for
the PN and PC, the PN is excited. B, Contralateral roll
leads to utriculopetal flow in both the AC and PC. Both canals are
inhibited. AC and PC flows are in opposite directions near PN and
should cancel. C, Flow in the horizontal canal
(HC) during a contralateral yaw. The posterior ampulla
and crista are seen below. Because of its location posterior to the
entrance of the horizontal canal duct into the utriculus, the PN is not
in the direct line of endolymph flow. Nevertheless, streamlines
entering the utriculus may displace the PN cupula in a posterior
(excitatory) direction.
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Although the scheme summarized in Figure 11 is plausible, there is a
need for experimental confirmation of the proposed relation between the
pitch sensitivity of the PN and endolymph flow in the two vertical
canals.
Comparative considerations
In turtles, the PN is sensitive to rotational head movements in
the pitch plane and encodes between angular acceleration and jerk. Two
features appear to determine these properties. First, a location
between the anterior and posterior ampullae allows the organ to sample
fluid flows from both vertical canals and thus to respond to rotations
in a plane symmetrically disposed to the AC and PC planes. The other
feature, a cupula that can sample fluid flow without occluding it, is
considered essential for the organ to encode between angular
acceleration and jerk. Both features are present in bony fish,
reptiles, birds, and some mammals (Baird, 1974 ; Lewis et al., 1985 ),
suggesting that the PN in these animals functions as it does in
turtles. Among cartilaginous fish, a similar arrangement is found in
Chimaera but not in elasmobranches (Baird, 1974 ; Corwin,
1978 ). In the latter species, the location of the PN is such that it is
unlikely to sample fluid flow from any canal. Not surprisingly, the PN
of sharks and rays has an entirely different function, involving
sensitivity to vibratory or acoustic stimuli (for review, see Corwin,
1981 ). Correlated with the difference in function, the PN in
elasmobranches can be much larger than in other vertebrates (Corwin,
1978 ), its cupula occludes the endolymphatic space (Vilstrup, 1951 ),
and there are specializations in the parietal cartilage that may
facilitate the delivery of acoustic energy to the ear (Corwin,
1981 ).
A PN is found in several mammals, but is apparently absent in some
species (for review, see Lewis et al., 1985 ). Among mammals, it has
been best described in the cat, in which it is quite similar in
location, size, and shape to the organ found in lower vertebrates (Gacek, 1961 ; Montandon et al., 1970 ; Hoshino and Kodama, 1976 ). The
incidence of a PN in humans is difficult to evaluate from the
literature. A PN was found in 17 of 223 temporal bones (Okano et al.,
1978 ), but most of the material in this and other human studies was not
serially examined, in which case the PN could have been missed because
of its small size. Two other facts about the human PN deserve comment.
First, it is located in the posterior ampulla instead of in the
utriculus (Montandon et al., 1970 ; Okano et al., 1978 ). Second, the
human PN is not always innervated by a separate branch of the posterior
ampullary nerve and in some cases a separate branch innervates both the
PN and a part of the PC (Okano et al., 1978 ). Based on these two
considerations, it has been suggested that the PN is incorporated into
the PC in some subjects (Montandon et al., 1970 ). In such an
arrangement, the PN would most likely lose its unusual properties,
including its maximal responses to pitches and its distinctive response dynamics. Before this conclusion is reached, however, it would be
prudent to confirm that a separate PN is absent in a substantial fraction of humans.
Despite its small size, the PN has kept essentially the same structure
in bony fish, reptiles, birds, and some mammals. Its evolutionary
persistence suggests that it plays a distinctive role in vestibular
processing. The present study shows that the organ in the turtle has
unique sensory coding properties. Even so, it remains unclear how the
PN innervation could make an impact on central processing when the PC
innervation outnumbers it by 30:1 in the turtle and 100:1 in the cat.
The numeric disparity would suggest that the central projections of the
PN are also unique.
 |
FOOTNOTES |
Received Dec. 10, 1997; revised March 5, 1998; accepted March 10, 1998.
This work was supported by National Institutes of Health Grant DC
02058. At the start of the research, A.M.B. was a Postdoctoral Fellow
of the National Institutes of Health. We thank Drs. Bernd Fritzsch,
Richard D. Rabbitt, and Anna Lysakowski for helpful comments on a
previous version of this paper and Dr. Ellengene Peterson for the use
of a confocal microscope at Ohio University.
Correspondence should be addressed to Dr. Alan M. Brichta, Department
of Surgery (Otolaryngology, Head and Neck Surgery), University of
Chicago, 5841 South Maryland Avenue, Chicago, IL 60637.
 |
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