All bats possess eyes that are of adaptive value. Echolocating bats have retinae dominated by rod photoreceptors and use dim light vision for navigation, and in rare cases for hunting. However, the visual detection threshold of insectivorous echolocating bats remains unknown. Here, we determined this threshold for the vespertilionid bat Myotis daubentonii. We show that for a green luminous target, M. daubentonii has a visual luminance threshold of 3.2(±0.9)×10−4 cd m−2, an intensity corresponding to the luminance of an open cloudless terrestrial habitat on a starlit night. Our results show that echolocating bats have good visual sensitivity, allowing them to see during their active periods. Together with previous results showing that M. daubentonii has poor visual acuity (∼0.6 cycles deg−1), this suggests that echolocating bats do not use vision to hunt but rather to orient themselves.

Vision is one of the most ubiquitous senses in the animal kingdom, and almost all animal species possess eyes for detecting light, ranging from simple pit eyes in clams to the more complex compound eyes of insects and the camera eyes of mammals (Land and Fernald, 1992; Land and Nilsson, 2012). However, while vision is most efficient in bright light, it is not limited to day-active animals (Warrant, 2008).

Most bats are nocturnal and use echolocation to navigate and forage, emitting high-frequency sound pulses, and localizing and identifying objects in their surroundings by the returning echoes (Griffin, 1958). Echolocation allows bats to forage in the complete absence of light, but nonetheless all echolocating bats have eyes. While the eyes of echolocating bats are small compared with those of non-echolocating bats (Thiagavel et al., 2018), it is clear that they have functional significance because (i) eyes are exceptionally costly to maintain (Niven and Laughlin, 2008) and as a consequence are reduced (Borghi et al., 2002) or even lost over evolutionary time if unused (Jeffrey et al., 2003), and (ii) there is strong purifying selection on the opsin genes in both echolocating and non-echolocating bats (Shen et al., 2010; Zhao et al., 2009). Echolocating bats have retinae dominated by rod photoreceptors (Suthers and Wallis, 1970), the photoreceptor class subserving dim-light vision in all vertebrates (Ahnelt and Kolb, 2000), indicating a strong adaptation to low-light conditions. However, the small size of echolocating bat eyes, both in relative terms and in absolute terms, does limit their visual sensitivity and resolution at low light intensities (Céchetto et al., 2020; Pettigrew et al., 1988; Thiagavel et al., 2018).

Visual acuity in echolocating bats appears to correlate with feeding ecology. Aerial hawking insectivorous bats have poorer visual acuity than both carnivorous and frugivorous gleaners, with values as low as 0.2 cycles deg−1 in the small aerial hawker Rhinolophus rouxi, compared with around 2 cycles deg−1 in the very large carnivorous gleaner Megaderma gigas (Pettigrew et al., 1988). However, the visual acuity of most aerial hawking bats is below 0.6 cycles deg−1, with one reported case at 1.3 cycles deg−1 (Bell and Fenton, 1986; Céchetto et al., 2020; Eklöf et al., 2014; Suthers, 1966). Functionally this means that they can detect 30–90 mm objects at 1 m distance under ideal conditions and it is generally accepted that this is insufficient to detect and track their insect prey (Eklöf et al., 2014). This is also likely to be the underlying drive for the evolution of echolocation, as the ancestral bat probably had the auditory capacity for echolocation but not the visual capacity for high-speed aerial pursuit of insects (Thiagavel et al., 2018). It is therefore generally held that aerial hawking insectivorous bats predominantly use their eyes for large-scale orientation and navigation (Barbour et al., 1966; Boonman and Jones, 2002; Buchler and Childs, 1982; Childs and Buchler, 1981; Davis and Barbour, 1965; Eklöf et al., 2014; Kugler et al., 2019).

However, the absolute visual thresholds of echolocating bats are still largely unknown (for a summary, see Table S1). A few studies have reported the lowest luminances allowing optomotor responses (e.g. 6×10−4 cd m−2 for Macrotus californicus and Antrozous pallidus: Bell and Fenton, 1986) or brightness discrimination (10−4 cd m−2 for Eptesicus fuscus: Ellins and Masterson, 1974), but while such measurements may function as a good proxy, they systematically underestimate absolute sensitivity because good acuity requires higher light levels (Cronin et al., 2014; Land and Nilsson, 2012). Liu et al. (2015) used flash-evoked visual potentials to measure absolute visual threshold in Taphozous melanopogon (Emballonuridae) and Rhinolophus affinis (Rhinolophodae): 2×10−4 and 1.2×10−2 cd m−2, respectively. But such measurements need to be ground-truthed against behavioural measures as they usually result in a higher threshold than obtained in behavioural experiments. The only behavioural measure of visual sensitivity that has been made in echolocating bats is for the nectar-feeding Glossophaga soricina – with a peak spectral sensitivity at 510 nm (green), visual threshold was obtained at an illuminance of about 7.6×109 photons cm−2 s−1 (Winter et al., 2003). Glossophaga soricina is a nectar-feeding bat that potentially uses vision (and particularly UV vision) to enhance contrast when detecting light reflected from flower petals (Guldberg and Atsatt, 1975; Horovitz and Cohen, 1972). Moreover, this family of bats (Phyllostomidae) have larger eyes relative to their body size than other insectivorous echolocating bats (Thiagavel et al., 2018).

Hence, the aim of our study was to behaviourally determine the visual detection threshold in an insectivorous echolocating bat. We hypothesized that non-gleaning insectivorous bats have poor acuity, but a relatively good visual sensitivity that allows large-scale orientation and navigation under open-sky conditions. To test this hypothesis, we used operand conditioning to determine the visual detection threshold of a vespertilionid bat for which we already have data on visual acuity: Myotis daubentonii (Céchetto et al., 2020). Myotis daubentonii is a small insectivorous bat (8–10 g) that hunts at low altitude over water. It starts hunting from around 30 min after sunset and continues for about 1–2 h (Rydell et al., 1996; Encarnação and Dietz, 2006).

Animals

We captured four adult male Myotis daubentonii (Kuhl 1817) in the vicinity of Odense in Denmark, with permission from the Danish Environmental Protection Agency (permit number: NST-3446-00001). The animals were kept on a reversed 8 h:16 h day:night cycle with a stable temperature of 20°C and 60% humidity and were released following experiments.

Apparatus

Experiments were conducted in a Y-maze, with a floor made of black felt, and walls made of aluminium painted with matt black paint. Both arms of the maze were covered with a black-painted aluminium roof and further covered with felt to prevent any exterior light from entering. The maze itself was in a small room that was completely dark during experiments.

Each arm measured 15 cm in length from the bifurcation point and was 12 cm wide and 12 cm high. The common arm also measured 15 cm in length and was 15 cm wide and 12 cm high (Fig. 1A). We used a small red headlight only when necessary and the computer screen was dimmed with a neutral density (ND) filter sheet of ND value 2.

Fig. 1.

Experimental setup. (A) Top view of the apparatus. At the end of each maze arm is a diffusing screen (light grey line), where the visual target would appear. Each pair of shutters consists of a real shutter (solid line) and a mock shutter (dashed line). The bifurcated liquid light guide (Uvitron UV21268) splits the light from the light source (LED) into two equal beams. The two filter wheels hold seven UV-VIS 12.5 mm diameter quartz neutral density (ND) filters. Laser triggers for detecting bat choices were produced using a laser diode (5 mW, 650 nm) that created a laser beam detected by an analog light sensor. The bat was detected when it broke the laser beam during approaches towards the light stimulus in a given arm. (B) The spectral radiance of the LED light source used for the stimulus measured from inside the maze arm after the diffusing paper with no ND filter in front of the light source.

Fig. 1.

Experimental setup. (A) Top view of the apparatus. At the end of each maze arm is a diffusing screen (light grey line), where the visual target would appear. Each pair of shutters consists of a real shutter (solid line) and a mock shutter (dashed line). The bifurcated liquid light guide (Uvitron UV21268) splits the light from the light source (LED) into two equal beams. The two filter wheels hold seven UV-VIS 12.5 mm diameter quartz neutral density (ND) filters. Laser triggers for detecting bat choices were produced using a laser diode (5 mW, 650 nm) that created a laser beam detected by an analog light sensor. The bat was detected when it broke the laser beam during approaches towards the light stimulus in a given arm. (B) The spectral radiance of the LED light source used for the stimulus measured from inside the maze arm after the diffusing paper with no ND filter in front of the light source.

The Y-maze was equipped with a broad green (peak 565 nm) LED light source (Broadcom HLMP-3950: RS Components #590-525) (spectrum shown in Fig. 1B; the spectrum was measured from the inside of the labyrinth arm after passing through the diffusing paper) and two custom-made filter wheels, containing seven 12.5 mm diameter UV-VIS quartz ND filters from Edmund Optics (with ND values of 0.3, 0.6, 0.9, 1.3, 2, 2.5, 3). The filter wheels were activated by servo motors (Parallax Standard Servo #900-00005) controlled by an Arduino Uno board. A 2-pole bifurcated liquid light guide (Uvitron UV2168) carried light to two diffusing filters (Lee filters 216 white diffusion) that, when illuminated, constituted the visual targets in each arm, each of which was round and had a diameter of 10 cm (Fig. 1B). Electronic shutters allowed the illuminated targets in each arm of the Y-maze to be turned on and off. Laser diodes (650 nm), with corresponding sensors (DFRobot LX1972), created a thin light beam across the interior of the Y-maze arm that, when broken, detected when a bat entered the arm to make its choice, thereby triggering the acquisition of that decision.

The different light intensities used (given as spectral radiance in mW m−2 sr−1 nm−1), created by a combination of one or two ND filters, are reported in Table 1. The first five light levels were measured using a Ramses hyperspectral radiometer (TriOS Optical Sensors). We used the given ND values of the filters to calculate the intensity of the dimmer light levels (beyond the range of the radiometer) as the radiometric measurements at brighter light levels did not differ from the calculated values. To convert spectral radiance into cd m−2 we used the following formula (BIPM, 2006; Johnsen, 2012):
formula
(1)
where E(λ) represents the photon energy spectrum, ŷ(λ) represents the scoptopic human spectral sensitivity curve and Δλ is the width (in nm) of the summation step used (in our case Δλ=10 nm). The wavelength limits of the summation (500–650 nm) were chosen to capture the radiance spectrum of our experimental target (Fig. 1B).
Table 1.

Light level steps used in the staircase procedure

Light level steps used in the staircase procedure
Light level steps used in the staircase procedure

Experimental protocol

We used a two-way forced choice paradigm (Kingdom, 2012) with a weighted staircase method (1 step down, 2 steps up) to determine the bats' detection threshold for green (∼560 nm) light.

The bats were trained to go towards the arm of the Y-maze where light was present. We used positive reinforcement with a bridging signal (i.e. a buzz sound classically conditioned to be associated with food) and rewards consisting of half mealworms (larvae of Tenebrio molitor). After each successful trial (Hit), the light level was decreased by one step, and in the case of an unsuccessful trial (Miss), the light level was increased by 2 steps (see Table 1). We used a weighted staircase method so that if a bat was lucky in guessing the arm with the light and thus moved towards light intensities under its threshold it would be faster for it to return to visible stimulus intensities, ensuring higher motivation and reward frequency (Garcia-Perez, 1998).

Each session ended after a pre-set number of trials depending on the bat's body mass before the experiment (usually around 30 trials); if the bat's body mass was high (above ∼9 g), the number of trials was reduced to ensure that the bat would finish the session. Each session started with a warm-up period, where the bat had to make four correct choices in a row for the intensity to start decreasing. This was to ensure the bat was under stimulus control, and that the bats were motivated enough by the reward to make choices and participate in the experiment. Each session also ended with a cool-down period with light intensity at the highest level (step 0 in Table 1) for the last four trials.

All recording sessions were double-blind such that neither the experimenter nor the animal could predict which arm would be illuminated for any given trial. We controlled the setup using an Arduino board controlled through serial communication using a custom-written program in Python 2.7.

At the beginning of each session, the bat was placed at the entrance to the Y-maze (Fig. 1A) and the experimenter started the first trial. The program then generated a pseudo-random sequence of stimulation in the left and right Y-maze arms so that the illumination would never be presented more than 3 times in a row in a given arm and that each arm was illuminated equally often (i.e. ∼50% of the time). The program then sent instructions to the Arduino board as to which arm should be lit and at what intensity. The Arduino board selected the correct set of filters (Fig. 1A), opened the shutter on the arm to be lit, and turned on the light source and two laser triggers on each arm of the maze. To avoid giving confounding auditory cues to the bats, each side had a real and a mock shutter that would always be activated on each trial so that there was sound on both sides for every trial.

The Arduino board then waited for the bat to make a choice (to cross one of the laser triggers). As soon as that happened, the light source was turned off and both shutters closed. If the bat chose correctly during the trial (Hit), the bridging signal played – the experimenter then gave the bat a reward and moved it back to the start of the maze. If the result of the trial was a Miss, the bat was simply moved back to the start of the maze. This was done using touch or, in some cases, indirect lighting from a dim red headlight. The Arduino board then sent the result of the trial (Hit or Miss) to the program and a new trial was started.

For the next trial, based on the outcome of the previous trial(s), the program determined at which intensity, and in which arm, the stimulus would next appear, and the process was repeated.

Statistical analysis

The results of each session were saved as a comma-separated file and then analysed using a custom-written Python script using Matplotlib (https://matplotlib.org/) and Scipy (https://scipy.org) packages. Because we used a staircase method, the number of trials where a given intensity was presented during a session could be quite low, especially at lower light intensities. Therefore, to estimate the probability of success at a given intensity as accurately as possible, we pooled results together from all sessions and calculated the probability of success for each intensity.

As the experiment used a two-way forced choice paradigm, if we had no data for a given intensity (i.e. the bat never reacted to that intensity) we set the probability to chance level (i.e. 0.5). We then used the Weibull cumulative distribution function, and least squares fitting, to generate a sigmoidal psychometric function (Kershaw, 1985; Wetherill and Levitt, 1965) that fitted the relationship between the probability of choice success P and the base-10 logarithm of target luminance I:
formula
(2)
where g is the expected probability of success at chance level (i.e. 0.5), and α and β control the slope of the function. The threshold was obtained by calculating the value of target luminance corresponding to a probability of success of 75% using the psychometric function previously calculated.

We also estimated the threshold by calculating the average intensity levels generating reversals (i.e. the trials where the bats missed).

We calculated visual thresholds using between 6 and 12 sessions and between 142 and 385 trials with an average of 239 trials for each of the four bats (Table S2). Measurements of psychometric functions for each of the bats revealed a median threshold (±median absolute deviation) of 3.2(±0.9)×10−4 cd m−2 (Fig. 2; Tables S2, S3). Likewise, when calculating the threshold using the average of reversals, we found a median threshold of 2.0(±0.3)×10−4 cd m−2.

Fig. 2.

Psychometric functions for the Daubenton's bats (Myotis daubentonii) used in this study. The probability of a correct choice is given as a function of the base-10 logarithm of luminance (cd m−2) for the four bats (A–D). Each data point (circles) represents the observed probability of a correct choice at that light level. The black curve is the best-fit Weibull density function (Eqn 2) describing the psychometric function. The dashed grey part of the line and grey circles represent where the probability was set to chance level (i.e. 0.5). Horizontal and vertical dashed lines indicate estimates of the intensity threshold (parameter α in the Weibull function).

Fig. 2.

Psychometric functions for the Daubenton's bats (Myotis daubentonii) used in this study. The probability of a correct choice is given as a function of the base-10 logarithm of luminance (cd m−2) for the four bats (A–D). Each data point (circles) represents the observed probability of a correct choice at that light level. The black curve is the best-fit Weibull density function (Eqn 2) describing the psychometric function. The dashed grey part of the line and grey circles represent where the probability was set to chance level (i.e. 0.5). Horizontal and vertical dashed lines indicate estimates of the intensity threshold (parameter α in the Weibull function).

We find a luminance threshold for M. daubentonii of 3.2(±0.9)×10−4 cd m−2 [2.0(±0.3)×10−4 cd m−2 based on average of reversals] for green light in the three most sensitive individuals, which is equivalent to the luminance of terrestrial objects in an open habitat under a moonless clear starlit sky (Warrant, 2008). This means that M. daubentonii should be fully capable of large-scale visual navigation and orientation under most natural conditions. However, with an estimated maximal acuity of 0.6 cycles deg−1, they are probably not capable of visually guided prey capture (Céchetto et al., 2020). Our results are consistent with existing knowledge on Macrotus californicus, A. pallidus and E. fuscus (Bell and Fenton, 1986; Ellins and Masterson, 1974). While these studies did not measure detection thresholds, the light levels measured that allow spatial vision and brightness discrimination are of the same order of magnitude as our measurements (6×10−4 cd m−2 for M. californicus and A. pallidus and 10−4 cd m−2 for E. fuscus). Compared with sensitivity measurements using visually evoked potentials, our results are on par with those obtained in Taphozous melanopogon (2×10−4 cd m−2) but are substantially lower than values obtained in Rhinolophus affinis (around 1.2×10−2 cd m−2: Liu et al., 2015). Given that emballonurids have much larger eyes than rhinolophids and vespertilionids (Thiagavel et al., 2018), visually evoked potentials may underestimate the visual threshold substantially, as we think it likely that R. affinis has a similar threshold to M. daubentonii while T. melanopogon could be more sensitive. In their study, Winter et al. (2003) find that G. soricina has a relatively low threshold for detecting both green and UV light. Although their results are not directly comparable to ours, they suggest that G. soricina has a sufficiently low visual threshold to permit foraging from flowers at night.

The broad green light source used in our study has a wavelength peak at 560 nm, which is higher than the peak sensitivity of rhodopsin (∼500 nm). Even though the emission spectrum widely overlapped the absorption spectrum of rhodopsin, had we had the possibility to use a light source that peaked at 500 nm it is likely that the detection threshold of M. daubentonii would have been slightly lower. Similarly, the use of a more natural stimulus may have yielded a lower threshold. Indeed, in mice it has been shown that visual performance is dependent on the ecological relevance of the stimulus (Hoy et al., 2016).

Nonetheless, this threshold indicates that the eyes of these bats are quite sensitive to light, although compared with flying foxes (family Pteropodidae) and other nocturnal mammals such as cats, the threshold is at least 3 orders of magnitude higher (i.e. less sensitive) to light (Gunter, 1951; Liu et al., 2015). In mice, whose eyes are slightly bigger than those of M. daubentonii (∼3.5 mm versus ∼1.5 mm), visual threshold is only about an order of magnitude lower (i.e. more sensitive) than that measured in M. daubentonii (De Tejada et al., 1997). While additional specializations, such as a tapetum lucidum (found in cats and many flying foxes), may account for part of this difference, it is likely that the substantially larger eyes and lower ocular F-number found in cats accounts for most of the difference. For example, the F-number of the cat's dark-adapted eye is 0.9 (Cronin et al., 2014) while in Myotis sodalis it is around 2.2 (calculated from Suthers and Wallis, 1970). This difference in F-number implies that the image formed on the retina of the cat is (2.2/0.9)2≈6 times brighter than the image formed on the retina of the bat.

In echolocating bats, visual acuity appears to be correlated with feeding ecology. For instance, acuity is higher in gleaners, which have comparably larger eyes, than in aerial hawking bats (Eklöf et al., 2014; Thiagavel et al., 2018; Veilleux and Kirk, 2014). Given the sparsity of visual detection threshold data for echolocating bats, it remains to be seen if visual sensitivity likewise correlates with feeding ecology. The inherent trade-off between acuity and sensitivity would indicate that, at least in small bats such as P. auritus and M. daubentonii, it is unlikely that both sensitivity and acuity can be maximized given their relatively and absolutely small eye size (Eklöf et al., 2014). However, in larger gleaners (or in families with larger eyes, e.g. phyllostomids or emballonurids: Thiagavel et al., 2018) sensitivity and acuity could both be high.

Our results have obvious implications for understanding vision in echolocating bats and afford us insight into how echolocating bats might use vision for navigation. But our results also have implications for conservation and habitat protection – with the urbanization of rural landscapes (Antrop, 2004), light pollution becomes another challenge that nocturnal animals must face. Indeed, light pollution has been shown to have an adverse effect on numerous bat species, ranging from general avoidance behaviour to changes in emergence behaviour, disruption of the circadian rhythm, disruption of hibernation and roost abandonment (Stone and Harris, 2015). In-depth knowledge of visual sensitivity in bat species adversely affected by light pollution should provide much needed data on how to efficiently mitigate such effects.

We dedicate this article to the late Professor Annemarie Surlykke, who made valuable contributions to this project.

Author contributions

Conceptualization: C.C., L.J., E.J.W.; Methodology: C.C., L.J.; Software: C.C.; Validation: C.C., L.J., E.J.W.; Formal analysis: C.C.; Investigation: C.C.; Resources: L.J.; Writing - original draft: C.C., L.J.; Writing - review & editing: C.C., L.J., E.J.W.; Visualization: C.C., L.J., E.J.W.; Supervision: L.J., E.J.W.; Project administration: L.J.; Funding acquisition: L.J.

Funding

This work was funded in part by the Human Frontier Science Program and by Danmarks Frie Forskningfond.

Data availability

All relevant data can be found within the article and its supplementary information.

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Competing interests

The authors declare no competing or financial interests.

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