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Supplemental InformationNestling polymorphism in a cuckoo-host system: a consequence of an escalating coevolutionary arms raceNozomu J. Sato, Keita D. Tanaka, Yuji Okahisa, Masato Yamamichi, Ralph Kuehn, Roman Gula, Keisuke Ueda, Jörn Theuerkauf
Supplemental Experimental ProceduresMaterials and Methods
Study Sites, Species and Measurements
We conducted field investigations at three sites on the main island (Grande Terre) of New Caledonia
during three breeding seasons (September-January) from 2011 to 2014: Parc provincial des Grandes
Fougères (main study site) and near surroundings (21°37’39.44” S, 165°45’41.75” E), approx. 40
km west (21°35’58.89” S, 165°23’55.61” E) of the main study site, and approx. 130 km northwest
(20°41’45.55” S, 164°59’38.41” E) of the main study site.
The fan-tailed gerygone Gerygone flavolateralis flavolateralis is a passerine bird of the
family Acanthizidae and an endemic subspecies to New Caledonia. The shining bronze-cuckoo
Chalcites lucidus layardi is a brood parasitic cuckoo of the family Cuculidae, and also an endemic
subspecies to New Caledonia. Both are abundant and widespread throughout Grande Terre year-
round, and the gerygone is exclusively parasitised by the bronze-cuckoo [S1].
To measure reflectance, we captured 32 gerygone chicks from 18 broods (dark: N = 5;
bright: N = 11; polymorphic: N = 2), out of which 22 were of the bright morph and 10 were of the
dark morph. We also captured 3 shining bronze-cuckoo chicks to measure reflectance, which all
were of the bright morph. We measured reflectance spectra of light from 300 nm to 700 nm
wavelengths from their skin (Figure S1a) using spectrophotometers (USB-2000 and Jaz-EL-200,
Ocean Optics, Dunedin, Florida, USA) with light irradiated by a deuterium-tungsten-halogen light
source (DT-MINI-2-GS, Ocean Optics, Dunedin, Florida, USA). Before measurements, we
calibrated the spectrometer with a diffuse reflectance standard (WS-1, Ocean Optics, Dunedin,
Florida, USA). Measurements were carried out in a film-changing bag (E-7041, Etsumi, Tokyo,
Japan) to block ambient light. While holding chicks by hand, we placed the probe vertically above
their skin, keeping an approximately 2-mm distance ensured by insulating tape winded around the
probe. To avoid injuring gerygone chicks, we conducted measurements when they were at least 3
days old, while cuckoo chicks were measured on the day of hatching before host parents ejected
them. We measured reflectance spectra of bare skin on the back of each chick twice (except for 4
chicks that we could only measure once). This usually took only few minutes, thereby avoiding
potential negative effects on chicks. From the 35 chicks, we obtained 66 reflectance spectra in total
(dark: n = 18; bright: n = 42; cuckoo: n = 6).
Because host parents were likely to eject cuckoo chicks, we artificially incubated 2 cuckoo
eggs to measure reflectance spectra of hatchlings (Mini Advance Incubator, Brinsea, Wiscombe,
North Somerset, UK). We conducted measurement for one cuckoo chick that hatched naturally in
the host nest before being ejected by the host. All artificially hatched cuckoo chicks were
reintroduced in the nearest active nest on the day of hatching in the case that the original nest was
depredated. We placed an artificial cuckoo egg in the nest at least 24 h before we replaced it with a
cuckoo chick.
Skin Colour Polymorphism in Chicks
There was neither a sign of colour polymorphism in adults nor a sign of assortative mating in
relation to the chick skin colour polymorphism in the gerygone since there were no detectable
differences in adult songs and plumages between parents of dark and bright chicks (authors’
unpublished data), which are known as indices of prezygotic isolation in birds [S2, S3]. Both dark
and bright gerygone chicks were found sympatric in all study sites.
The skin colour polymorphism of host chicks was most remarkable just after hatching, and
weakened with chick age (authors’ unpublished data). It became almost indistinguishable in chicks
of ca. 13-15 days of age. We occasionally measured reflectance from chicks older than 5 days (2
bright and 3 dark chicks in 3 nests), but not from chicks 10 days or older. The polymorphism was
not related to deformation of pigmentation such as albinism [9], since no bright chick had red irises
or a pinkish bill, or fibromelanosis [S4].
We have no evidence for sympatric polymorphism in the bronze-cuckoo but photo
evidence of a dark morph (Figure 1C) was published 35 years ago [S5] and taken in Parc
Provincial de la Rivière Bleue, approx. 100 km southeast of the main study site. Chick colour
polymorphism is known in the shining-bronze cuckoo, though in different subspecies, and
respective cuckoo morphs mimic chicks of respective hosts in different colours [7, 9, S6].
Avian Visual Model
Birds are thought to have two distinct pathways to perceive a colour, i.e., chromatic (hue) and
achromatic (luminance, or perceived lightness) [S7-S9]. We estimated both chromatic [S7] and
achromatic [S9] discrimination thresholds of the chick skin colours, respectively, based on the
Vorobyev-Osorio model [S7, S9]. Birds of the genus Gerygone have VS (violet-sensitive) vision
[S10]. However, because data of the visual performance of the study species were not available, we
applied hitherto available single-cone sensitivity of a VS-type bird, the wedge-tailed shearwater
Puffinus pacificus [S11], the double-cone sensitivity of the blue tit Cyanistes caeruleus [S12], and
the single-cone abundance in the posterior dorsal area of retina of the satin bowerbird
Ptilonorhynchus violaceus [S13], all phylogenetically closest to the gerygone among species with
available information.
We first calculated photon capture Qi with sensitivity of respective photoreceptors Ci(λ)
and measured reflectance spectra R(λ) according to the following equation:
Qi=∫300
700
R ( λ )⋅C i ( λ ).
We then calculated the colour discrimination threshold, i.e., just noticeable difference (jnd),
between a given pair of colours. Jnds were obtained from the following equations:
jnd hue=√ (ωUV ωS )2 ( Δf L−Δf M )2+(ωUV ωM )2 ( Δf L−Δf S)2+(ωUV ωL )2 ( Δf M−Δf S )2+ ¿
(ωS ωM )2 ( Δf L−Δf UV )2+(ωS ωL )2 ( Δf M −Δf UV )2+(ωM ωL )2 (Δf S− Δf UV )2 ¿(ωUV ωS ωM )2+ (ωUV ωS ωL )2+(ωUV ωM ωL )2+ (ωS ωM ωL )2
(S1a)for hue [S6], and
jnd luminance=ΔS=|Δf D
ωD|
(S1b)
for luminance [S7], where ∆f denotes the log ratio of photon captures of the focal pair of measured
colours by a given type of photoreceptors:
,and ω denotes the relative abundance of each single-cone type in the posterior dorsal area of the
retina, with incorporating the Weber fraction of 0.05, the conventionally adopted error rate (i.e.,
noise-to-signal ratio) in the Weber-Fechner law [S7]. Since fan-tailed gerygones build domed nests
in which the inside is dimly lit, we considered fluctuation of the number of photons captured by
cone cells (i.e., shot noise) as a relatively great quantal flux of 103 [S14]. We did not consider colour
constancy because the ambient light condition should be very similar for all chick types.
Statistics
We first calculated jnds between all possible combinations of measured colours for both hue and
luminance respectively based on equations S1a and S1b [S5, S7]. Next, we converted these jnds
into respective distance matrices, from which we calculated tridimensional coordinates through a
principal coordinate analysis (PCoA, or multi-dimensional scaling, MDS) [S15, S16].Each principal
coordinate consists of a set of data, each of which corresponds to each photospectral measurement,
and thus the total number of replicates analysed was n = 66. Each coordinate value indicates the
relative position of each datum among the whole dataset, i.e., distance from the centroid, on each
coordinate axis in its unit (jnd in this case) (see Figure S1d). Unlike jnd (i.e., psychophysical
distance), all coordinate values are geometrically independent of each other, and thus the dataset is
compatible with linear models [S15, S16]. Eigenvalues were used to assess the accuracy of primary
eigenvectors (i.e., first principal coordinates). The rationale underlying this procedure is illustrated
in [S15] and [S16].
We analysed the first principal coordinates for hue and luminance with linear mixed
models (LMMs), in which brood ID and nestling ID nested within brood were assigned as random
effects to avoid pseudoreplication [S15]. We assigned dummy variables [S16, S17] to each chick
type, i.e., dark chick, bright chick and cuckoo chick, and set bright chick as the intercept in the
LMMs. Representative values for respective chick types were calculated as the absolute value of the
difference of partial coefficient from the intercept, i.e., |cuckoo chick – bright chick| and |dark chick
– bright chick|. These values represent the perceivable difference of respective chick types from
bright chick on average, and thus can be interpreted as chromatic (hue) or achromatic (luminance)
discriminability [S15, S16]. We assumed jnd > 3 as discriminable by convention [S9]. Goodness of
fit was tested by the likelihood ratio (2) test.
For the analyses of the observed data, we conducted a contingency (2) test, a binomial
test, and a generalised linear model (GLM) with a likelihood-ratio (2) test. All statistical
procedures were conducted in R [S18]. PCoAs/MDSs were conducted with the cmdscale function,
setting the dimensional parameter k as 3 because jnds existed in a tridimensional colour space.
LMMs were conducted with the lmer function in the lme4 package [S19] and the GLM the glm.nb
function in the MASS package [S20]. Likelihood ratio tests were conducted with the Anova function
in the car package [S21]. Figure S1a was drawn with the aggplot function in the pavo package
[S22].
Population Genetics Model
We assumed 1-locus-2-allele complete dominance as the inheritance mechanism, which was most
probable in this case because the colour difference appeared to be discrete, as we have not observed
hatchlings of an ambiguous type. The observed frequency of within-nest polymorphism might be
biased or obscured in several ways: an inevitable bias caused by small brood sizes, i.e., no
polymorphism in single-chick broods irrespective of parental genotypes; an observational bias, i.e.,
before we found a nest, polymorphism in there might have already vanished due to randomly
caused partial brood mortality (including that caused by brood parasitism); and a small sample size.
To deal with such bias and uncertainty, we simulated stochastic distributions for expected
frequencies of phenotype, monomorphic brood of each morph, and polymorphic brood at Hardy-
Weinberg equilibrium. These values represent the frequency of phenotype and respective brood-
types, ideally obtainable in a limited number of observations and at a low average brood size of the
population when the population is at the equilibrium. We assumed genetic monogamy of parents
(i.e., chicks in a nest have the same genetic parents) and our observation to be random sampling for
simplicity.
On allele frequencies at even intervals, offspring phenotypes were randomly sampled
assuming a binomial distribution with coefficients for the emergence probabilities of respective
brood types based on equations described below. Parameter values were set at 33 for sample size
assuming a Poisson distribution, and set for brood size ranging from 1.525 to 3.350 in integer
assuming a uniform distribution (average 1.93), in reference to our observation (see Results). We
iterated the sampling 500 times in R [S18].
We extracted a pair of simulated samples of phenotype frequency, each assuming the dark
morph as either recessive or dominant, from samples in each iteration, among those which were
nearest to the observed phenotype frequency of chicks. The brood-type frequencies and allele
frequencies corresponding to the extracted phenotype frequencies were also extracted. We
compared the position (i.e., percentile) of the observed frequencies of phenotype and respective
brood-types within the corresponding simulated distributions of expected frequencies between
recessive and dominant (see Figure S2). These simulated percentiles were resampled with the
parametric bootstrapping method (iteration = 1000). The minimum requirement for Hardy-
Weinberg equilibrium here is that all the observed frequencies are simultaneously contained within
the corresponding simulated distributions respectively.
Equations for Population Genetics Model
When the genotype frequency in the parental generation is x for dominant homozygotes (AA), y for
heterozygotes (Aa), and z for recessive homozygotes (aa), the expected genotype frequency in the
offspring generation under Hardy-Weinberg equilibrium is X = , Y = , and
Z = , where X denotes dominant homozygotes, Y heterozygotes, and Z recessive
homozygotes; note that x + y + z = X + Y + Z = 1. The emergence of polymorphic broods is
potentially limited in those from parents of the Aa-Aa pair (both heterozygotes; y2) and the Aa-aa
pair (heterozygote and recessive homozygote; 2yz). However, the emergence of polymorphic broods
is also limited in situations that brood size, C, is two or greater, and thus, the emergence probability
of each brood type is:
bD: (S2a)
b
p: (S2b)
bm:
(S2c)
bR: z2 (S2d)
where bD denotes dominant monomorphic broods, bp polymorphic broods, bm monomorphic broods
of either from the potential mating combinations, and bR recessive monomorphic broods (Figure
S2a). bp and bm are complementary to each other and thus sum up to y2 + 2yz (“potential” in Figure
S2a); when C is 1, bp is always 0 and bm is always y2 + 2yz (Figure S2a).
Ethical Notes
We conducted fieldwork under permissions from Province Sud and Province Nord of New
Caledonia. No chick died because of our treatments. The research protocol complies with the
current laws in New Caledonia, and was approved by the Ethical Committee of Life-Sciences at
Rikkyo University in Tokyo, Japan, and the First Warsaw Local Ethics Committee for Animal
Experimentation in Warsaw, Poland.
Results
Colour Discriminability
We described the results for achromatic discriminability in the main text. The distribution of
measured colours (in hue) overlaps in the tetrachromatic colour space of VS birds irrespective of
chick types (Figure S1b, c). Eigenvalues of first principal coordinates were 3.00 (100% of variance
explained) for luminance and 2.47 (82% of variance explained) for hue (Figure S1d, e), and thus
they well represented the distribution of measured colours.
Chromatic discriminability for both dark host and (bright) cuckoo chicks was neither
greater than 3 on average nor statistically different from that for bright chick (intercept: 0.033, SE =
0.60) (Figure S1d, e): dark chick, 0.18 jnd (partial coefficient = -0.15, SE = 0.92), 21 = 0.027, P =
0.87; cuckoo chick, 1.69 jnd (partial coefficient = -1.65 SE = 1.50), 21 = 1.21, P = 0.27. These
results suggest that the colours of respective chick types are indiscernible in terms of hue.
Observed Frequencies
We found 149 gerygone nests over three breeding seasons. We found eggs in 68 nests, out of which
18 were parasitised, and 42 nests with chicks. We were not able to determine the skin colour in 9
nests because chicks were too old, and thus the skin colour was known from 33 nests, in which we
included parasitised nests. Out of them, 23 broods consisted only of bright chicks and 8 broods
exclusively of dark chicks, while 2 nests contained both types of chicks, one nest with 1 chick of
each morph, and the other with 1 bright and 2 dark chicks. The observed brood type frequency of
bright monomorphic, polymorphic, and dark monomorphic broods was 0.70:0.06:0.24 (Figure S2d-
f). The number of bright chicks was 39 and that of dark chicks 16 in total. The overall phenotype
frequency of bright and dark chicks was 0.71:0.29 (Figure S2c).
Out of 42 nests containing chicks, we could not reliably assess brood size in 12 nests due
to brood parasitism (3), unhatched eggs (3), egg disappearance (2), partial predation (1), the
location of the nest preventing close inspection (1), and clutch or brood reduction for unknown
reasons (2). The clutch and brood sizes were thus known from 50 and 30 non-parasitised nests,
respectively. The estimated mean clutch and brood sizes were 1.82 (log-linear coefficient: 0.60 SE =
0.11; GLM, family = negative binomial, link = log) and 1.93 (0.66 SE = 0.17) respectively, which
were not statistically different (21 = 0.13, P = 0.72). Frequencies of each size class did not differ
between egg and nestling stages as well (contingency test, 22 = 0.75, P = 0.69; Figure 1F).
We successfully monitored the transition from egg to nestling stages in 18 out of 30 non-
parasitised nests, of which brood size was consistent with clutch size in 10 nests. Among 8 nests of
clutch-brood size discordance, the causes of the discordance were unknown in 2 nests but known in
6 nests as above mentioned. After excluding these 6 nests, the probability of concordance, 10 out of
12 nests, was significantly greater than chance (one-sided binomial test, P = 0.019).
Observed Frequencies among the Expected Frequencies Inferred by Simulation
Assuming the dark morph to be dominant, all observed frequencies (red arrows in Figure S2c-f)
were within the range of simulated distributions for their corresponding expected frequencies (all
within 40-60%ile). In contrast, assuming the dark morph to be recessive, observed frequencies for
bright monomorphic and polymorphic broods greatly diverged from those expected (namely,
3.7%ile and 90.6%ile) (Figure S2c-f). This trend was consistent in the outcome of the parametric
bootstrap: mean percentiles were 4.6 and 90.3 respectively for bright monomorphic and
polymorphic broods if recessive, while those for bright monomorphic and polymorphic broods if
dominant were 39.3 and 55.0, respectively. The mean percentiles for the rest of frequencies were all
between 35%ile and 65%ile. These results suggest that the dominant dark morph is more consistent
with the assumption for Hardy-Weinberg equilibrium than the recessive one. The putative dark-
morph allele frequency was inferred at 0.63 (SD = 0.070) if recessive, and at 0.11 (SD = 0.035) if
dominant.
Cuckoo Chick Ejection by Host Parents
From more than 2000 h of video footage, we confirmed that all 8 cuckoo hatchlings that we found
in gerygone nests were ejected by host parents both from naturally parasitised nests and nests from
to which we introduced artificially incubated chicks (foster nests). Five out of 8 cuckoo chicks were
confirmed to be of the bright morph, 2 seemingly bright, and 1 was unidentified. Four out of 8 host
broods from these nests were composed only of bright chicks, 1 brood with only dark chicks, and 3
were unidentified. Two cuckoo chicks were fostered in 2 broods of the bright morph. The causes of
failure to identify the colour of chicks were ejection of cuckoo chicks by host parents, and failure of
eggs to hatch or predation of the host nests.
All parasitic eggs hatched earlier than host eggs, but host parents did not always eject
parasitic chicks before their own eggs hatched. Thus, cuckoo chicks coexisted with host hatchlings
in 2 nests (1 naturally parasitised and 1 fostered; both bright monomorphic broods). The shining
bronze-cuckoo is probably an evictor (a brood parasite whose chicks monopolise host nests by
evicting host eggs and chicks from the nests soon after hatching; Figure 1C) like Chalcites cuckoos
in other areas [4, 5, S1, S5]. We could however not confirm this because host parents ejected
cuckoo chicks soon after hatching (44 min. after hatching at the shortest). In foster nests, ejection
by host parents occurred later than in naturally parasitised nests (1 day after introduction at the
longest). We confirmed that host parents reared remaining host chicks until fledging (2 nests) or
until predation (3 nests), hence saving them from eviction by cuckoo chicks (c.f., [S6]).
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Supplemental Figures
Figure S1. a) Mean reflectance spectra from the skin of cuckoo chicks (green) and of both morphs
of gerygone chicks: bright (blue) and dark (red). Vertical widths in translucent colours represent
95% confidence intervals. b) Distribution of measured colours in the tetrachromatic colour space of
VS birds (b, c). Viewing angles are altered to illustrate the aspect of avian colour space that is
visible to humans (b) and that invisible to humans (c). Each apex indicates the coordinate for a
colour that stimulates solely the corresponding photoreceptor. First principal coordinates calculated
from distance matrices of pairwise hue jnds between all possible combinations of measured colours,
in relation to second principal coordinates (d), or chick types (e). Numbers represent the eigenvalue
of the first principal component, with the proportion of variances explained in parenthesis.
Figure S2. a) Expected brood-type frequency at Hardy-Weinberg equilibrium in relation to
recessive allele frequency, with a constant brood size C within population, according to the model
described in the supplementary text. y and z represent the frequencies of parental genotypes in
population, heterozygotes and recessive homozygotes, respectively. Red lines indicate the
frequencies of polymorphic broods (bp), and the blue line that of monomorphic broods (bm) among
the potential mating combinations (note that bp = potential – bm). b) Simulated expected frequencies
by the model in relation to recessive allele frequency. Line colours denote each brood type.
Horizontal lines indicate the observed frequencies of phenotype, assuming the dark morph as
dominant (solid) and as recessive (dashed); observed frequencies of brood types (red): polymorphic
(solid), dark monomorphic (dotted), and bright monomorphic broods (dashed). c-f Positions of the
observed frequencies (indicated by red arrows and percentile values) of respective categories among
the distributions of simulated expected frequencies, assuming the dark morph as dominant (shaded
bars) and as recessive (open bars): phenotype (c), dark monomorphic (d), bright monomorphic (e),
and polymorphic broods (f). Percentile values are underlined for dominant. Vertical lines indicate
the mean of simulated frequencies when assuming the dark-morph as dominant (dashed) and as
recessive (solid). Bin widths of all histograms were optimised by setting the breaks argument as
“Scott” for the hist function default in R [S18].