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First published online February 29, 2008
Journal of Experimental Biology 211, 844-851 (2008)
Published by The Company of Biologists 2008
doi: 10.1242/jeb.012179
Visual sensitivity in the crepuscular owl butterfly Caligo memnon and the diurnal blue morpho Morpho peleides: a clue to explain the evolution of nocturnal apposition eyes?
Lund University, Department of Cell and Organism Biology, Helgonavägen 3, S-22362 Lund, Sweden
* Author for correspondence (e-mail: rikard.frederiksen{at}cob.lu.se)
Accepted 21 January 2008
| Summary |
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is similar in both species, and acceptance angles, 
,
are only marginally larger in C. memnon. Moreover, temporal resolution is only
a little coarser in C. memnon compared to M. peleides. Using
a model for sensitivity, we found that the eyes of C. memnon are
about four times as light-sensitive as those of M. peleides in the
frontal visual field, much of this difference being due to the larger facet
diameters found in C. memnon. In summary, greater visual sensitivity
has evolved in C. memnon than in M. peleides, showing that
adaptations that improve sensitivity can be found not only in nocturnal
apposition eyes, but also on a smaller scale in crepuscular apposition
eyes.
Key words: visual sensitivity, crepuscular vision, apposition eye, Nymphalidae
| INTRODUCTION |
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Visual systems are known to show considerable flexibility during the
evolution of adaptations that optimise them for a particular light environment
(Cronin et al., 1994
;
Cheroske et al., 2006
). Life in
dim light, for instance, is particularly challenging to the visual system
(Warrant, 2004
). The light
intensity on a moonless night is over a hundred million times lower than on a
bright sunny day (Warrant and McIntyre,
1992
). To deal with this extreme range of intensities several eye
designs, of various sensitivities, have evolved. This is clearly seen in the
compound eyes of insects. Two basic eye designs are found: superposition eyes
and apposition eyes. There are several subtypes and variations in these two
designs (Nilsson, 1990
), but
the type of eye that is found in a typical day-active insect is the focal
apposition eye. Each rhabdom receives light from a single facet lens, and the
apposition eye is thus best suited to insects active in bright conditions.
Crepuscular (dusk- and dawn-active) and nocturnal insects, such as moths, many
beetles and even some butterflies [Hedyloidea
(Yack et al., 2007
)],
typically have superposition eyes that have evolved to capture as much of the
available light as possible. This is achieved by increasing the effective
aperture and allowing light from large numbers of corneal facet lenses to be
focused onto one rhabdom.
There are, however, interesting exceptions. Diurnal superposition eyes have
been reported from several groups of lepidoptera [e.g. Sphingidae
(Exner, 1891
;
Warrant et al., 1999
) and
Hesperiidae (Swihart, 1969
;
Horridge et al., 1972
)] and
beetles [e.g. dung beetles (McIntyre and
Caveney, 1985
)], and there are nocturnal and crepuscular insects
that have retained apposition eyes as they evolved a life in dimmer and dimmer
light (Warrant et al., 2004
;
Kelber et al., 2006
).
However, irrespective of eye design, there are adaptations that tune visual
systems to specific light intensity windows. For instance, the superposition
eye of the diurnal hummingbird hawkmoth Macroglossum stellatarum is
highly resolved (Warrant et al.,
1999
) and has a considerably smaller superposition aperture
(composed of fewer corneal facet lenses) than found in the nocturnal elephant
hawkmoth Deilephila elpenor
(Kelber et al., 2002
). In
nocturnal insects with apposition eyes, adaptations for increased sensitivity
can likewise be found. The nocturnal halictid bee Megalopta genalis,
for instance, is an insect with apposition eyes that is active at intensities
about ten times dimmer than starlight
(Warrant et al., 2004
;
Kelber et al., 2006
). In order
to achieve this, M. genalis has enlarged facets and rhabdoms, as well
as compromised spatial and temporal resolution, all of which favour increased
sensitivity (Warrant et al.,
2004
; Greiner et al.,
2004
).
There are also many crepuscular insects with apposition eyes. Do these insects, active at intermediate light intensities, also possess important adaptations that improve visual sensitivity in dim light, but on a smaller scale? If so, do these adaptations reveal anything about the evolutionary transition from a diurnal to a nocturnal lifestyle?
To explore these questions we have examined the anatomical, optical and
physiological parameters that determine visual sensitivity in two similarly
sized and closely related (Wahlberg et
al., 2003
; Freitas and Brown,
2004
) species of nymphalid butterflies from the neotropical
rainforests of Central America – the crepuscular owl butterfly
Caligo memnon and the diurnal blue morpho Morpho peleides.
Like all papilionoid butterflies, both species possess afocal apposition eyes
(Nilsson et al., 1984
;
van Hateren and Nilsson, 1987
;
Nilsson et al., 1988
), a
design best suited for bright light and in many respects intermediate between
the focal apposition design and the superposition design: as in superposition
eyes, their lens systems possess graded refractive-index elements
(Nilsson et al., 1988
). The
interesting difference between the two species is that C. memnon is
active at dawn and sometimes at dusk (Malo
and Willis, 1961
; Srygley,
1994
), when the luminance is 2–4 orders of magnitude dimmer
than daylight, while M. peleides is active only during the day
(Young, 1982
;
DeVries, 1987
).
| MATERIALS AND METHODS |
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Electrophysiology
In preparation for electrophysiology we removed the wings of the butterfly
and inserted it in a tube made of a plastic pipette tip with the small end
sliced off to accommodate the head of the butterfly. Only the head of the
animal was allowed to protrude through the hole. The animal was fixed to this
tube with a tiny amount of 50:50 mixture of bee's wax and violin resin melted
onto the mouthparts (proboscis and labial palps) and the dorsal and ventral
sides of the head as well as the antennae. The tube containing the animal was
attached to a holder on a magnet stand with the aid of dental wax. The
indifferent electrode, consisting of a thin silver wire, was inserted through
a hole made between the eyes and fixed in position with the same wax mixture
used to fix the animal to the plastic tube. A small, approximately
ten-facets-wide, triangular hole was cut in the ventral portion of the eye and
sealed with Vaseline. After fixation and dissection, we mounted the magnet
stand in the centre of the electrophysiology apparatus. The animal was placed
with its anterior end facing upwards and the angular position of the animal
was noted carefully. Finally the electrode was inserted through the hole in
the eye.
The electrophysiology apparatus contained one stimulating section and one recording section, all controlled by a Macintosh computer and LabVIEW 2.2.1 software (National Instruments, Austin, TX, USA). White stimulus light was produced by a Nikon XPS-100 xenon arc lamp. The light was directed through a series of filter wheels and a shutter (UniBlitz T132 shutterdriver/timer; Rochester, NY, USA) before reaching the animal through a quartz light guide. Neutral density filters controlled the intensity of the stimulus and interference filters controlled the wavelength of the stimulating light. The shutter regulated the stimulus light pulse length. The end of the light guide was held in a goniometer arm that allowed the stimulating light to be placed at any position in the visual field of the animal. The stimulus could thus be moved in known angular steps throughout the visual field of the eye. When recording from a photoreceptor we could therefore note its exact position, in terms of latitude and longitude, on an imaginary sphere around the animal. The stimulating end of the light guide had a diameter of 100 µm, and was positioned 115 mm away from the centre of the goniometer arm, making the stimulus a point source subtending a width of 0.050°. Surrounding the point source was a light-adapting device consisting of a set of 15 white LEDs (EL333UWC, Everlight Electronics, Taipei, Taiwan) illuminating a circular plastic diffuser disc with a 40 mm diameter.
For recording we used glass (borosilicate) microelectrodes filled with 2
mol l–1 potassium acetate (200–300 M
resistance
in vivo). The electrode was inserted into the hole in the ventral
part of the eye using a Märzhäuser PM10 (Wetzlar-Steindorf, Germany)
piezo-driven micromanipulator. The electrical responses were amplified on a
Biologic VF180 (Claix, France) microelectrode amplifier. Mains noise was
eliminated using a HumBug, from Quest Scientific (North Vancouver, BC,
Canada). The amplified signal was low-pass filtered at 400 Hz and digitised
into a Macintosh computer using LabVIEW 2.2.1 software (National
Instruments).
All electrophysiological experiments were performed in a laboratory at a temperature range of 23–25°C. Dark adaptation was performed by switching off all the lights in the room (resulting in a light intensity of 3.5x10–4 cd m–2). For light adaptation we used a background illumination of 200 cd m–2. Light and dark adaptation were maintained for at least 30 min prior to recording, and often longer.
Penetration of a photoreceptor cell was indicated by a drop in the baseline of 40–60 mV and depolarising responses to a flashlight. Once a photoreceptor was penetrated, we moved the goniometer arm so that the point source was positioned on the visual axis of the cell. This was indicated by the direction from which the maximum electrical response was generated. Following this we recorded the V–logI curve, the spectral sensitivity, the impulse response and the angular sensitivity of the cell. The sampling frequency was 2.5 kHz in all experiments.
The V–logI curve was plotted from the cell's
responses to a series of 40 ms long pulses of white light of increasing
intensity, with the point source aligned with the cell's optical axis. The
spectral sensitivity was recorded from the cell by stimulation with a series
of 40 ms light pulses at different wavelengths. The interference filters used
in this experiment had peak transmissions separated by 50 nm and ranged from
350 nm to 700 nm. The band-pass of the interference filters was 40 nm. Because
of the broad band-pass of the interference filters the spectral sensitivity
function could not be measured exactly. Nevertheless, it gave a good
estimation of the wavelength range where the cell was maximally sensitive.
Although we occasionally penetrated cells that were maximally sensitive in the
blue and UV range of the spectrum, the vast majority of the cells were
`green-sensitive' with a sensitivity peak at around 550 nm. Only these cells
were used for further experiments, since these are considered to be the part
of the pathway for contrast and luminance vision in insects
(Osorio and Vorobyev, 2005
).
Following the measurement of spectral sensitivity, the impulse response was
recorded. The shutter was set to deliver 2 ms light pulses and the neutral
density filters were adjusted to give a dim stimulus that resulted in a
2–3 mV depolarising response in the cell. Responses from 100 pulses were
recorded and averaged from each cell. Lastly, we recorded the angular
sensitivity function of the cell. The shutter was reset to deliver 40 ms
flashes and the neutral density filters were adjusted to an intensity that
resulted in the cell giving a depolarising electrical response of 50–75%
of maximum. The point source was displaced from the cell's optical axis
outside the visual field. During the recording, the stimulus was moved in
known angular steps across the visual field. At each step one stimulus flash
was delivered and the electrical response of the cell was recorded. When
recording from C. memnon we used 0.5° steps and 0.25° steps
from M. peleides. The responses were converted to equivalent
intensities through the V–logI curve and the
sensitivities at each angular step were calculated.
In total, 33 cells from nine individuals of C. memnon and 28 cells from six individuals of M. peleides were used for electrophysiology. Of these, only cells with a spectral sensitivity maximum of about 550 nm, and a maximum response of at least 30 mV, were used for analysis of the impulse response and angular sensitivity function. We also rejected all cells that did not have symmetrical angular sensitivity functions, since an asymmetrical angular sensitivity function may indicate damaged optics or an artificial double cell recording. The final number of cells used for analysis was 11 (9 dark-adapted recordings and 6 light-adapted recordings) from C. memnon and 12 (10 dark-adapted recordings and 6 light-adapted recordings) from M. peleides.
Maps of interommatidial angles
We made two eye maps of males of each species using standard methods
(Land and Eckert, 1985
;
Rutowski and Warrant, 2002
).
Briefly, the animal was mounted in a plastic tube in the same way as in the
preparation for electrophysiology. The left eye was dusted with chalk dust
particles that were used as landmarks in the analysis. We placed and centered
the preparation in a goniometer that in turn was placed under a microscope
adapted for orthodromic illumination: an axial light source illuminates the
insect eye with white light that is reflected by the mirror-like tapetum below
the retina. This reflection is seen as a `bright pseudopupil', a brightly lit
spot on the eye surface facing upwards into the microscope, light that is not
absorbed by the photopigments.
A magnified image of the eye, with pseudopupil and landmarks, was taken at the central front of the butterfly's visual field (latitude=0°, longitude=0°). We changed the angular position of the goniometer in 10° steps of latitude and longitude and took a new image at each. The procedure was repeated until the limits of the goniometer were reached (latitudes 80°, –80° and longitudes 80°, –80°). From the images the facet diameters were measured to produce an additional map with isolines of facet diameters. The local interommatidial angle was calculated by counting the number of facet rows (in x, y and z-axis) that the pseudopupil moves between the angular steps. This data was used to make a map with isolines of interommatidial angle.
Histology
Living animals were decapitated and the eyes were removed from the head and
put into fixative for 24 h. We used a fixative made of 90 ml ethanol (80%), 5
ml concentrated acetic acid and 5 ml formalin (40%). Following fixation, the
eyes were dehydrated in an ethanol series (70% 2x20 min, 96% 2x20
min, 100% 2x30 min) and then put in a series of acetone mixed with Epon
(Poly/Bed® 812, Polysciences, Eppelheim, Germany) plastic (acetone
2x30 min, 2:1 acetone/Epon 1 h, 1:1 acetone/Epon over night, 1:2
acetone/Epon over day, and pure Epon over night). The eyes were embedded in
new Epon and polymerised for 48 h at 60°C. We cut 2 µm thick sections
for light microscopy using a LKB Bromma 11800 pyramitome (Bromma, Sweden) with
a glass knife. From the sections we measured the rhabdom length in the frontal
visual field from two eyes in each species using five sections from each
eye.
In preparation for transmission electron microscopy, the animals were dissected in the same way as for light microscopy. The eyes were fixed in 2% paraformaldehyde, 2.5% glutaraldehyde and 2% sucrose in a 0.15 mol l–1 sodium cacodylate buffer, pH 7.2, for 12 h. After the fixation the eyes were rinsed in 0.15 mol l–1 sodium cacodylate buffer and postfixed in 1% osmium tetroxide (in the same buffer as above) and then rinsed again. The dehydration and embedding process was the same as for the light microscopy preparation. Thin sections (0.05 µm) were cut using a Leica Ultracut UCT ultratome (Wetzlar, Germany) with a diamond knife and mounted on grids for transmission electron microscopy. The sections were stained with uranyl acetate (3%, 30 min) and lead citrate (1%, 4 min). The microscope used was a Jeol JEM-1230 (Tokyo, Japan). Photographs of the rhabdoms of both species were taken and the rhabdom diameter measured.
For scanning electron microscopy we used air-dried specimens that were mounted on stubs and sputter coated with gold/palladium (Polaron SC7640 sputter coater; Quorum Technologies Ltd, Ringmer, E. Sussex, UK) at 1.2 kV, 11 mA and 0.03 mbar (3 Pa). The microscope used was a Jeol JSM-5600 LV scanning electron microscope. Photographs of the surface of the eyes of both species were taken for eye-size comparison.
| RESULTS |
|---|
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Rhabdom diameters are larger in C. memnon (3.9±0.2 µm,
Fig. 3A) than in M.
peleides (2.0±0.1 µm, Fig.
3B). Wide rhabdom diameters can potentially increase sensitivity
by increasing the solid angle
(
d2/4f2 steradians) of visual
space that is viewed by the receptor (where d is the rhabdom
diameter, and f is the focal length). A larger solid angle
contributes to a higher sensitivity but worsens spatial resolution
(Kirschfeld, 1974
;
Land, 1981
;
Warrant, 2004
).
|

, is
a convenient measure to quantify spatial resolution. C. memnon has slightly broader ASFs than M. peleides (Table 1). In both species the smallest acceptance angles (Fig. 4) were found near the equator of the visual field, 10° to 20° lateral of anterior. This is also an area of small interommatidial angles and large facet diameters (Fig. 1).
|
|
So far we have mentioned the parameters that determine the spatial
resolution and sensitivity of a single rhabdom. To get the full picture, the
visual sampling density of the eye, defined by the interommatidial angle

, the angular spacing between two neighbouring ommatidia, must
also be considered. The interommatidial angle is defined by the ratio of the
facet diameter D, to the radius of curvature R of the eye
[D/R rad (Land,
1981
)].
Both species have interommatidial angles that are in the same size range (about 1–2°, depending on position in the eye), but the distribution pattern in the visual field is rather different (Fig. 1). The visual field of C. memnon has a frontal acute zone 10–30° ventral of the equator. M. peleides, on the other hand, has a visual streak along the equator of the visual field where the largest facets are also found. Both species have the smallest interommatidial angles in the anterior part of the eye, about 10–20° ventral of the equator.
Temporal resolution
The impulse response is the cell's response to a very short and dim flash
of light that elicits an electrical response similar to that of one photon (a
photon bump). The half-width, or integration time
t, of the
impulse response is a good measure of the temporal resolution of an eye
(Pinter, 1972
;
Howard et al., 1984
).
Both species show considerably lower temporal resolution in the
dark-adapted state than in the light-adapted state, both in terms of
time-to-peak
p (the time from the stimulus onset to the
maximal response amplitude) and
t
(Table 1). Moreover, C.
memnon has longer integration times and times-to-peak than M.
peleides in the dark-adapted state. In the light-adapted state, the
difference is minor (Fig. 5,
Table 1).
|
The power falls off at lower frequencies in C. memnon (fc,LA=30.7±2.3 Hz, fc,DA=18.9±7.0 Hz) than in M. peleides (fc,LA=37.0±4.0 Hz, fc,DA=18.2±5.3 Hz). This is due to the wide and skewed dark-adapted impulse response (Fig. 5) in C. memnon. The difference between the species is, however, small.
Sensitivity
Several optical and physiological parameters contribute to the sensitivity
of an eye. In order to obtain a more complete picture we calculated the
sensitivity S (µm2sr) of the eyes in C. memnon
and M. peleides (Kirshfeld, 1974;
Land, 1981
;
Warrant and Nilsson, 1998
):
![]() | (1) |

(Warrant,
1999
|
The calculations show that C. memnon (S=1.3 µm2sr) is about 3.3 times as sensitive as M. peleides (S=0.4 µm2sr). If we also account for the 1.2 times longer integration time (Table 1) in Caligo's photoreceptors, we end up with a sensitivity difference of about four times between the species.
| DISCUSSION |
|---|
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Morphology, optics and spatial resolution
Perhaps the most evident adaptation for crepuscular vision in C.
memnon is its enlarged facets. The optical sensitivity increases with the
lens diameter squared, D2 [the lens area:
D2/4 (Kirschfeld,
1974
; Land,
1981
)]. If we compare the facet diameters of C. memnon
with those of M. peleides, in the eye region of highest resolution,
we find that the facet diameters alone account for a doubling of the optical
sensitivity (482/342=2). It is clear that it is the
large eye size of C. memnon (Fig.
2) that allows sensitive vision whilst maintaining reasonably high
visual acuity (Figs 1,
4). If we use our data to
calculate a local radius of curvature (R=D/
) in
the eye region of highest spatial resolution, we find that C. memnon
(R=3.4 mm) has a local radius of curvature that is 1.8x greater
than that in M. peleides (R=1.9 mm). Since the
interommatidial angle is very similar in the two butterfly species, the
doubled sensitivity due to enlarged facets in C. memnon is mostly due
to its very large eyes (Fig.
2). Because an enlargement in eye size and aperture size increases
sensitivity while maintaining high acuity, we believe that this is likely to
have happened early in the evolution towards increased sensitivity in
crepuscular insects. Such enlargements of eye and aperture size have also been
reported from other crepuscular and nocturnal insects with apposition eyes
(Warrant et al., 2004
) as well
as from insects with superposition eyes
(McIntyre and Caveney, 1998
).
Moreover, they have also been reported from nocturnal vertebrates such as
birds (Brooke et al., 1999
;
Thomas et al., 2006
;
Hall and Ross, 2007
) and
primates (Kay and Kirk, 2000
;
Kirk, 2004
), suggesting that a
relative enlargement of eye size is a common evolutionary strategy in animals
adapted for reliable vision in dim light. The size of the eye cannot, of
course, increase indefinitely but is eventually limited by developmental
constraints and opposing selection forces, for instance, limited energy
resources (Laughlin et al.,
1998
). Thus, at some point in the evolution of nocturnality, eye
enlargement will cease; acuity is then likely to be sacrificed in order to
achieve higher sensitivity. This sacrifice in acuity in the service of higher
sensitivity can result from the evolution of one or more of the following
three morphological strategies: (1) further increases in facet diameter (that
will decrease the sampling density), (2) increases in rhabdom diameter (that
will widen the acceptance angle) or (3) spatial summation of signals from
groups of several photoreceptors.
Interestingly, different strategies or combinations of different strategies
have been reported from different species. The nocturnal bee Megalopta
genalis, for instance, uses a combination of all of them
(Warrant et al., 2004
). The
nocturnal wasp Apoica pallens has large eyes but with many ommatidia,
all with small corneal facet lenses. Their rhabdoms, however, are very wide
and this, together with their large numbers of small facets, implies the
likelihood of spatial summation (Greiner,
2005
). In Caligo memnon, the eyes, facets and rhabdoms
are all larger than in Morpho peleides, suggesting that this
scaling-up of eye size should lead to improvements in sensitivity without
compromising spatial resolution. As we discuss below, this is indeed the case,
but further slight improvements in sensitivity have also occurred via
modest increases in acceptance angle.
C. memnon has a rhabdom diameter, d, about twice as wide
as that in M. peleides (Fig.
3). Wide rhabdoms increase sensitivity by increasing the
acceptance angle [approximated by d/f
(Stavenga, 2004a
;
Stavenga, 2004b
)]. The
mismatch between the small difference in electrophysiologically measured
acceptance angles (Fig. 4) and
the large difference in rhabdom diameters can be explained by a large local
radius of curvature, R, in the eye of C. memnon
(Fig. 2) and its
correspondingly longer focal length, f. However, the focal length is
very difficult to measure optically because of the complex graded refractive
index lens system of afocal apposition eyes. Electrophysiologically measured
acceptance angles are therefore a much more reliable measure of the eye's
resolution and sensitivity than what can be predicted from the ratio of the
rhabdom diameter and focal length.
We found somewhat wider acceptance angles in C. memnon than in
M. peleides, indicating more sensitive eyes in the former
(Fig. 4). The difference,
however, is not as great as one might expect. The dark-adapted apposition eyes
of the nocturnal bee Megalopta genalis, for instance, have much wider
acceptance angles: 
DA=5.6°
(Warrant et al., 2004
). This
species is active at intensities several orders of magnitude dimmer than those
in which C. memnon is active, and its much wider acceptance angles
(due to much wider rhabdoms) reflect its need for greater visual sensitivity.
Perhaps a more relevant comparison is with other lepidopteran apposition eyes.
The acceptance angles of both species investigated here are similar to, or
smaller than, those of other day active butterflies
(Land, 1990
). We must
therefore conclude that in terms of acceptance angles alone, improvements in
sensitivity are modest in C. memnon (1.7 times), suggesting that it
has been important for this species to maintain high acuity.
A similar pattern is seen in the maps of interommatidial angles
(Fig. 1): compared to other
butterflies neither of the species have exceptionally large interommatidial
angles (Stavenga et al.,
2001
). These, moreover, should follow the acceptance angles in
order to provide an optimal sampling (
/
=2) of the
image (Snyder, 1977
;
Snyder et al., 1977
;
Land, 1997
). We calculated the
sampling ratio (
/
) for C. memnon and M.
peleides in the frontal visual field and found that in the diurnal M.
peleides (
LA/
=1.1 and

DA/
=1.8) the light adapted value is very
close to the average for insects [
LA/
=1.07
(Land, 1997
)]. C.
memnon, on the other hand, has larger sampling ratios
(
LA/
=1.4 and

DA/
=2.6). The oversampling in the
dark-adapted eye of C. memnon will increase photon capture and
produce a brighter image. The trade-off between sensitivity and spatial
resolution becomes evident once again: acuity must be sacrificed to achieve a
greater sensitivity.
Thus, if during evolution the angular sensitivity functions widen more
quickly than the ommatidial sampling density coarsens, the image will be
oversampled and thus brighter. An already oversampled image will suffer little
from a degradation in acuity caused by an eventual spatial summation at a
later stage of processing such as the lamina
(Warrant et al., 2004
;
Greiner et al., 2005
): spatial
resolution cannot be further coarsened by an equally wide summation of
photoreceptor signals, but sensitivity and visual reliability, on the other
hand, can be greatly improved. We have no evidence as yet, however, of spatial
summation in the lamina of C. memnon.
As we have discussed in the previous paragraphs, C. memnon
achieves most of its sensitivity through its enlarged eyes and corneal facet
lenses. Visual acuity is obviously important to Caligo, but without
sufficient sensitivity the eyes will not capture enough light to exploit this
acuity (Warrant and McIntyre,
1992
). What might the relatively high acuity be used for? During
reproduction, male Caligo gather at `hot spots' for lekking. Although
chemical cues have been suggested to be important in the courtship display
(Wasserthal and Wasserthal,
1977
), vision could also play an important role, in particular for
landmark detection when navigating to the lekking site
(Srygley and Penz, 1999
).
Vision might also be important for detecting conspecifics during perching
behaviour. There are, however, no previous studies that definitely link
reproductive behaviour in Caligo to its visual system.
Morpho, on the other hand, has a more mobile reproductive behaviour
and does not aggregate on hot spots for lekking
(Young and Muyshondt, 1973
).
Colour and contrast cues seem to be important for the courtship display in
Morpho (Young, 1971
),
and this can be part of the explanation as to why this species has high
acuity. However, these differences in reproductive behaviour between the two
species cannot on their own satisfactorily explain the differences in their
visual systems.
Temporal resolution
Compared to M. peleides, does C. memnon have adaptations
for crepuscular vision in terms of temporal resolution?
Photoreceptors of nocturnal and crepuscular animals have been shown to have
slower impulse responses with longer integration times (
t)
than those of diurnal animals with the same type of eye (e.g.
Warrant et al., 2004
). There
is also a trade-off between photoreceptor sensitivity and temporal resolution
(Warrant and McIntyre, 1992
).
Low temporal resolution – from impulse responses with long integration
times – means a compromised bandwidth in the frequency response and a
lower corner frequency, properties that result in increased motion blur at
high angular velocities. High frequency noise is attenuated, however, and
reliability is improved, at lower frequencies
(Laughlin, 1996
).
Although the dark-adapted impulse response of C. memnon is slower
than that of M. peleides (Table
1; Fig. 5), it is
not by any means slow compared to other insects. A similar pattern is seen in
the power spectra of the two species: power falls off at slightly lower
frequencies in C. memnon, indicating a somewhat more pronounced
low-pass filtering of the visual signal and a greater reliability at lower
frequencies. However, it is very likely that other factors apart from light
intensity alone have had a large impact on the evolution of light-response
dynamics in the two butterfly species studied here
(Howard et al., 1984
;
Laughlin and Weckström,
1993
).
Sensitivity
Apart from the much enlarged facet diameters found in C. memnon,
the individual optical, anatomical and physiological properties of vision that
influence visual sensitivity do not seem to contribute much on their own.
Nevertheless, their combined effects make the eyes of C. memnon about
four times as sensitive as those of M. peleides. Supporting this,
Järemo Jonson et al. (Järemo
Jonson et al., 1998
) found that the pupil mechanism in the closely
related C. eurolochus closes at about one log unit dimmer intensities
compared to diurnal butterflies and thus indicates a more sensitive eye in the
former.
This difference in sensitivity can at first thought appear to be minor,
considering that there is a difference in ambient intensity of 2–4
orders of magnitude between the activity peaks of the two species. We do not
know, however, if either of the species regularly experiences microhabitats of
higher or dimmer light intensity than what is considered to be their `normal'
intensity window. Nor do we yet know whether C. memnon increases
sensitivity further by employing neural summation, a strategy likely to be
used by nocturnal bees (Warrant et al.,
2004
).
If we compare the calculated sensitivities of the butterflies to other
diurnal and nocturnal insects, we find that M. peleides
(S=0.4 µm2sr) has a sensitivity similar to the honeybee
Apis mellifera [S=0.1 µm2sr
(Greiner et al., 2004
)]. C.
memnon's sensitivity (S=1.3 µm2sr) is not as great
as that of the nocturnal bee Megalopta genalis [S=2.7
µm2sr (Greiner et al.,
2004
)] or the elephant hawkmoth Deilephila elpenor
[superposition eye, S=69 µm2sr
(Warrant, 2004
)], but it is
well above that of the honeybee. This shows that adaptations that improve
sensitivity can be found not only in nocturnal apposition eyes, but also on a
smaller scale in crepuscular apposition eyes.
Concluding remarks
We conclude that the visual systems of crepuscular insects have evolved
adaptations that improve visual reliability in dim light. The most important
adaptations found in the species we studied are the enlarged facets allowed by
a greater total eye size. Our data strongly suggest that the visual systems of
insects are sufficiently flexible to evolve to be matched and optimised for a
particular intensity window, a conclusion also recently drawn for closely
related ants (Greiner et al.,
2007
).
| Acknowledgments |
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