Chengyi Xu
abcd
aDepartment of Mechanical and Materials Engineering, School of Engineering, University of Alabama at Birmingham, Birmingham, AL 35294, USA. E-mail: cxu@uab.edu
bNeuroengineering PhD Program, School of Engineering, University of Alabama at Birmingham, Birmingham, AL 35294, USA
cGraduate Biological Science Program, University of Alabama at Birmingham, Birmingham, AL 35294, USA
dComprehensive Neuroscience Center, Heersink School of Medicine, University of Alabama at Birmingham, Birmingham, AL 35294, USA
First published on 10th September 2025
Cephalopods (e.g., octopus, squid, and cuttlefish) are a class of soft-bodied marine invertebrates renowned for their ability to dynamically alter their color and appearance for camouflage in complex environments. Despite their popularity in human history and culture, the mechanisms underlying the dazzling visual feats displayed by cephalopod skin were not fully understood until recent decades. These feats are enabled by a synchronized orchestra of thousands to millions of dynamic bio-optical components embedded in the skin, each comprising highly evolved biological structures and a unique materials foundation, capable of unparalleled manipulation of incident light through neuromuscular or biochemical control. While our fundamental understanding of cephalopod optical biology and camouflage behaviors continues to evolve, it has already inspired numerous man-made technologies over the past decade with tunable optical functionalities across various spectral ranges. However, a comprehensive and up-to-date overview covering cephalopod camouflage tactics at the animal level, the underlying mechanisms at the organ and cellular levels, and the development of dynamic optical materials and systems derived from and inspired by cephalopod skin remains lacking and is highly needed. In this review, we summarize key recent advances in the optical biology of cephalopods and discuss how these insights have informed the design of dynamic, stimuli-responsive optical materials and systems. In addition, we provide our perspectives on future research directions in this rapidly growing field, with the aim to stimulate interdisciplinary research across cephalopod biology, materials science, and engineering domains.
Cephalopods share close ties with human beings from historical, cultural, and scientific perspectives. Early around 4000 years ago, ancient Chinese described the discovery of an unusual ‘ten-body’ fish in a classic geographical and cultural account called “The Classic of Mountains and Seas.”6 This mysterious ‘ten-body’ fish was later believed to be shallow-water squid that was known to have eight arms and two tentacles.6 Around 350 BCE, the Greek philosopher Aristotle described in his book “History of Animals” about cephalopods (Fig. 1A).7,8 Aristotle observed that octopuses and sepia cuttlefishes could render their body colors to match adjacent stones in the surrounding environments for hunting purposes, and they could perform similar color-changing tricks when alarmed.7,8 These two examples represented early written reports of cephalopods in human history and confirmed our ancestors’ direct observation and interaction with these animals. Indeed, cephalopods have served as inspiration sources for countless fictional mythologies and novels, such as the famous sea monster named Kraken in Scandinavian folklore (Fig. 1B) and the giant squid in Jules Verne's “Twenty Thousand Leagues under the Sea” (Fig. 1C).9–12 In addition, cephalopods are aesthetically appealing for their marvelous body forms and appearances, and they have been continuously stimulating the creation of numerous artworks, from ancient ceramic wares, as exemplified by a delicate octopus-patterned vase that was unearthed in Palaikastro (Fig. 1D),13 to paintings, as exemplified by Giuseppe Arcimboldo's “The Allegory of Water” from the Renaissance.14 Since around a century ago, cephalopods have also started to garner growing interest within the scientific community, with an extensive amount of research performed to explore and elucidate the evolutionary,15,16 physiological,17 structural,18 and ethological3,19 properties of these marine animals, which in turn have facilitated progress in other emerging areas such as neuroscience,20 bioelectronics,21 and robotics.22 Taken together, cephalopods have demonstrated enormous impacts on our culture and science along with human history.
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Fig. 1 Cephalopods in Human History. (A) A lost diagram of an octopus arm in Aristotle's book “History of Animals” (c. 350 BCE).7 The diagram was reconstructed by D’Arcy Thompson (1910 CE).8 (B) A drawing of an imaginary colossal octopus called the Kraken devouring a ship by Pierre Dénys de Montfort (1801 CE).10 (C) An illustration in Jules Verne's “Twenty Thousand Leagues Under the Sea” by Alphonse de Neuville and Édouard Riou (1870 CE), showing Captain Nemo viewing a giant squid from the Nautilus submarine.12 (D) A picture of an ancient octopus-patterned vase unearthed at Palaikastro, Greece (c. 1500 BCE).13 The picture was taken by Wolfgang Sauber (2009 CE). Parts A, B, and C are in the Public Domain and were reproduced via Wikimedia Commons. Part D was reproduced from an image by Wolfgang Sauber via Wikimedia Commons (Creative Commons Attribution-Share Alike 3.0). |
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Fig. 2 Cephalopod camouflage tactics at the animal level. (A) Color and patterning modulation. An S. officinalis cuttlefish adapting its body appearance to match different backgrounds, with the skin pattern changing from (i) uniform to (ii) mottled to (iii) disruptive.40 (iv) An Atlantic white-spotted octopus (Callistoctopus macropus) displaying a deimatic reddish pattern with sparsely distributed white spots.41 (v) A male Caribbean reef squid (Sepioteuthis sepioides) splitting its body pattern into two different halves to attract a female squid during mating activities.43 (vi) A flamboyant cuttlefish (Metasepia pfefferi) showing vivid skin coloration with constantly moving pigmentary stripes (known as passing clouds) on the dorsal side of the mantle.44 (B) Transparency modulation. (i) Pictures of a representative mesopelagic octopus (Japetella heathi) reversibly switching its body appearance between transparent and opaque states.46 (ii) Pictures of a representative glass squid (Taonius borealis) reversibly switching its body appearance between transparent and opaque states.46,47 (C) Contrast modulation. (i) Images of a blue-ringed octopus (Hapalochlaena lunulata) flashing blue rings and switching the body appearance from a low-contrast state (left) to a high-contrast state (right).48 (ii) Close-up images of an individual blue ring in the same octopus’ skin switching from a low-contrast state (left) to a high-contrast state (right).48 (iii) A schematic of the cross-sectional architecture of a blue ring, showing the arrangement of bright iridophores in the blue ring (br.ir.), surrounding chromatophore organs (ch.), and proximal muscles (m.). (iv) A confocal microscopy image of the cross-sectional architecture of a blue ring.49 (D) Symbiotic bioluminescence. A digital camera image of another Euprymna scolopes squid. The inset shows that bioluminescent bacteria (Vibrio fischeri) occupy and live inside a light organ that is located in the squid mantle.51 Note that the bioluminescent bacteria were colored in green for visualization. (E) Texture manipulation. (i) Images of an Australian giant cuttlefish (Sepia apama) reversibly changing its skin texture.55 Note that papillae can be expressed to form a highly textured skin surface. The images were taken by Roger Hanlon and reproduced with permission. (ii) Images of a common octopus (Octopus vulgaris) reversibly changing its skin texture and appearance.37 Note that the octopus can perform realistic 3D camouflage and perfectly blend itself into the undulating algae above the seafloor. (F) Behavioral Mimicry. (i) A mimic octopus swimming across the seafloor (bottom), mimicking the typical appearance and motion of a flatfish (top).61 (ii) A mimic octopus sitting still on the seafloor (bottom), resembling the typical posture of a sessile tube worm (top).62 (iii) A mimic octopus buried itself in a sand burrow with two long black-and-white banded arms undulating outside (bottom), mimicking the shape, pattern, and movement of a typical sea snake (top).61 (iv) A mimic octopus moving above the seafloor with all eight arms extended (bottom), resembling the typical body form of a lionfish (top).61 The images in Part A (i)–(iii) were reproduced with permission from Springer Nature (Copyright©2009). The image in Part A (iv) was taken by the SUBnormali Team and reproduced under the Creative Commons Attribution-Share Alike 3.0 Unported license via Wikimedia Commons. The image in Part A (v) was taken by Roger Hanlon and reproduced with permission. The image in Part A (vi) was taken by Silke Baron and reproduced under the Creative Commons Attribution 2.0 Generic license via Wikimedia Commons. The images in Part B (i) were reproduced with permission from Elsevier Ltd. (Copyright©2011). The images in Part B (ii) were obtained and reproduced with permission from the Monterey Bay Aquarium Research Institute. The images in Part C (i) and (ii) were reproduced with permission from New Atlantis WILD – YouTube under the Creative Commons Attribution (CC BY) license. The images in Part C (iii) and (iv) were reproduced with permission from The Company of Biologists Ltd (Copyright©2012). The images in Part D (i) and (ii) were taken by Roger Hanlon and reproduced with permission from Elsevier Ltd (Copyright©2007). The images in Part E were taken by Eric Stabb and reproduced with permission. The images in Part F (i), (iii) and (iv) were taken by Mark Norman and Roger Steene and reproduced with permission from the Royal Society (Copyright©2001), and the images in Part F (ii) were taken by Roger Hanlon and reproduced with permission from John Wiley and Sons (Copyright©2007). |
Besides camouflage, many cephalopods also use dynamic body patterning for a variety of other purposes, such as secondary defense mechanism, communication, and signaling.3,36 As one example, in cases where the primary defense mechanism (i.e., camouflage) fails, an Atlantic white-spotted octopus (Callistoctopus macropus) can suddenly change its body appearance into a high-contrast reddish pattern with sparsely distributed white spots (Fig. 2A(iv)).41 This dramatic deimatic display, as commonly seen in various animals, is effective to startle the predators and thus gain the octopus more time to expel ink and escape.42 As another example, a male Caribbean reef squid (Sepioteuthis sepioides) can split its body pattern into two strikingly different halves, with the right half appearing dark brown to attract a female squid and the left half appearing silvery-white to repel rival males (Fig. 2A(v)).43 Note that the half-bodied pattern can be rapidly flipped in seconds. As a third example, flamboyant cuttlefishes (Metasepia pfefferi) are famous for their vivid coloration with a series of pigmentary black stripes constantly moving across the body, which are known as ‘passing clouds’ (Fig. 2A(vi)).44 These eye-catching flashing patterns can send out warning (poisonous) signals to confuse or dismay potential predators, although, interestingly, the M. pfefferi cuttlefishes only produce neurotoxins at trace amounts. Altogether, these examples readily showcase cephalopods’ versatile abilities to change color and patterning under various circumstances.
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Fig. 3 Pigment-Rich Chromatophore Organs in Cephalopod Skin. (A) Chromatophore organs at different length scales (from left to right): (i) a digital camera image of a longfin inshore squid (Doryteuthis pealeii).65 The image was taken by Paloma T. Gonzalez-Bellido; (ii) a close-up image of the skin of a D. pealeii squid, showing a dense distribution of pigmentary chromatophores (dark colored spots).66 The image was taken by Minette Layne; (iii) a confocal microscope image of chromatophore organs, showing radial muscles and nerve bundles connected to the central elastic pigment-containing sacculus (P) of each individual chromatophore;70 (iv) a scanning electron microscope (SEM) image of the cross section of a chromatophore;68 (v) a close-up SEM image of closely packed pigment granules inside the same chromatophore.68 (B) A schematic of the reversible actuation of a chromatophore under direct neural control, showing a clear change in the areal coverage upon activation.71 (C) Optical microscopy images of the reversible actuation of a chromatophore in the skin of a D. pealeii squid, showing visible changes in both the areal coverage and pigmentary coloration upon activation.71 (D) Iridescence was seen in expanded chromatophores by changing the light illumination angle.73 (E) Autofluorescence confocal image of a chromatophore with the sheath cells highlighted in yellow.73 The pigment sac and muscle fibers (M) are enveloped by the sheath cells. (F) Confocal image of the sheath cell region showing abundant reflectin distribution inside, highlighted using a secondary antibody in green.73 The image in Part A (i) was reproduced with permission from the Company of Biologists Ltd. (Copyright©2014). The image in Part A (ii) was reproduced under the Creative Commons Attribution 2.0 Generic license via Wikimedia Commons. The image in Part A (iii) was reproduced with permission from John Wiley and Sons (Copyright©2013). The images in Part A (iv) and (v) were reproduced with permission from the Royal Society (Copyright©2014). The images in Parts B and C were reproduced with permission from John Wiley and Sons (Copyright©2013). The images in Parts D–F were reproduced with permission from Springer Nature (Copyright©2019). |
The optically active component of a chromatophore organ is chromatocyte, which consists of a central cytoelastic sacculus that encompasses packed pigment granules with diameters of hundreds of nanometers and varied sub-granular ultrastructures (Fig. 3A).67–70 A set of wedge-shaped radial muscles (15–25) are attached and anchored onto the highly deformable pigment-containing sacculus (Fig. 3A(iii)).3,31,67,71 Because cephalopod skin is highly innervated with nerve bundles, these radial muscles are subject to direct neural control from the central nervous system without the involvement of any synapse (Fig. 3A(iii)).3,31,67,71 At the resting state, the radial muscles are relaxed, and the sacculus is retracted into a tiny dot with the internal pigmentary granules closely packed in a small volume (Fig. 3B, left and Fig. 3C, left).71 Therefore, more light is allowed to transmit through the skin, and less is absorbed. At the activated state, the radial muscles are contracted, and the sacculus is radially pulled and expanded into a much larger area with the internal pigment granules spread out in a relatively sparse distribution (Fig. 3B, right and Fig. 3C, right).71 Therefore, less light is allowed to transmit through the skin, and more is absorbed. The size of the elastic pigment-containing sacculus can dramatically change upon activation, up to over 100 times, thus enabling a remarkable visible change in the overall pigmentary coloration.31 Note that this neuromuscular control of chromatophore organs in cephalopod skin is quite different from the function mechanism of common chromatophore cells found in fishes and reptiles, where pigmentary coloration is modulated by forming pigment aggregation/dispersion upon hormonal stimuli.72 In comparison, one obvious advantage of direct neuromuscular control is the rapid response of chromatophores, which can be instantly activated or deactivated within only hundreds of milliseconds.3,31,71 As a result, cephalopods are capable of changing color multiple times within only a few seconds, and thousands of chromatophores can be synchronously switched on and off in multiplexed formats to generate a variety of complex global patterns for dynamic camouflage in real time.
In a recent study, structural coloration was found in chromatophores in their expanded states, with iridescent patterns located precisely across the surfaces of all chromatophore color types (yellow, red, and brown) in both living squid and excised skin samples (Fig. 3D).73 These patterns are visible from specific view angles between 20° and 50°. For decades, such iridescence was mistakenly attributed to the underlying structurally colored iridophores; however, it has now been confirmed to originate from the sheath cells that envelope the chromatocytes.73 Within the sheath cells, reflectin protein aggregates were dispersed as small granule vesicles in a disordered fashion (Fig. 3E and F). According to a simplified optical model, one potential mechanism for this structural coloration might arise from multilayered structures between the sheath cell membranes and the thickness-tunable cytoplasm layers, which may further explain the observed color shifts upon chromatophore expansion.
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Fig. 4 Light-Reflecting Iridophore Cells in Cephalopod Skin. (A) Iridophore cells at different length scales (from left to right): (i) a digital camera image of a longfin inshore squid (Doryteuthis pealeii).74 (ii) a close-up image of the skin of a D. pealeii squid, showing sparsely distributed light-reflecting iridophore cells (bright spots).74 (iii) A cross-sectional transmission electron microscope (TEM) image of several iridophore cells from a different inshore squid (Doryteuthis opalescens);77 (iv) an SEM image of a portion of an iridophore from a D. opalescens squid;73 (v) a close-up SEM image of the surface of the same iridophore, showing a periodic arrangement of highly invaginated structures.77 (B) A confocal maximum-intensity projection image of fine neural structures (in red color) within an iridophore, confirming that iridophores are innervated.78 (C) An illustration of a proposed biochemical signaling cascade process that may contribute to iridophores’ tunable iridescence in response to acetylcholine (ACh).77 (D) Optical microscopy images of single iridophores in the skin of a D. pealeii squid displaying neurally tunable structure coloration from orange (left) to green (middle) to blue (right) in response to stimuli.78 The images in Part A (i) and (ii) were taken by Grayson Hanlon and reproduced with permission. The images in Part A (iii)–(v) and Part C were reproduced with permission from the National Academy of Sciences (Copyright©2013). Part B and D were reproduced with permission from the Royal Society (Copyright©2012). |
In most cephalopod species, iridophores are found to be physiologically static, i.e., their optical functionality is not responsive to external stimuli. However, there are exceptions in a few species, such as longfin inshore squid (Doryteuthis pealeii), where iridophores have been confirmed to exhibit tunable coloration.78 Experiments have demonstrated that these dynamic iridophores are often connected or terminated with nerve fibers, which indicates that the observed tunable iridescences are related to neurally mediated processes (Fig. 4B).78 The application of a neurotransmitter acetylcholine (ACh) triggers a biochemical signaling cascade process within the iridophore cells, initiating the phosphorylation of the constituent reflectin proteins in the alternating proteinaceous platelets and this neutralizing the initially cationic reflectin, leading to water outflux across the cell membrane (Fig. 4C).77 The resulting condensation of the proteinaceous platelets causes changes in the overall geometry, refractive index, and arrangement of the Bragg-reflector-like structures on the iridophore surface (Fig. 4C).77 Therefore, the iridophores can shift their reflectance peaks (i.e., colors) across a broad wavelength range within the visible region of the electromagnetic spectrum (Fig. 4D).78 Furthermore, the semi-permeable membrane that envelops the Bragg lamellae is thought to functionally serve as an “impedance-matched” amplifier to the stimuli-responsive reflectin assembly size.79 The response time of these tunable iridophores is usually between a few seconds and a few minutes, much slower compared to that of chromatophores.3,78
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Fig. 5 Light-scattering leucophore cells in cephalopod skin. (A) Leucophore cells at different length scales (from left to right): (i) a digital camera image of a European common cuttlefish (Sepia officinalis) on the sandy floor. (ii) a close-up image of the skin of an S. officinalis cuttlefish, featuring zebra-like bands with white regions that are mainly composed of leucophores;33 (iii) a cross-sectional SEM image of a fractured leucophore cell from an S. officinalis cuttlefish, featuring densely packed spherical leucosome particles within the cell;33 (iv) a close-up TEM image of spherical leucosome particles.33 (B) Optical microscopy images of a single leucophore from an S. officinalis cuttlefish displaying different colors when illuminated with lights at different wavelengths.33 (C) Digital camera images of tunable white stripe in the skin of a female Doryteuthis opalescens squid upon the stimuli of a neurotransmitter (ACh), featuring a gradual change in the appearance as indicated by the red cross.81 The image in Part A (i) was taken by Chengyi Xu and reproduced with permission. The images in Part A (ii)–(iv) and B were reproduced with permission from the IOP Publishing (Copyright©2018). The images in Part C were reproduced with permission from the Company of Biologists Ltd. (Copyright©2013). |
For a long time, leucophores were thought to be physiologically static, because no clear evidence of nerve or muscle connections was found in these cells.3 More recently, it was demonstrated that leucophores found in the dorsal mantle of female Doryteuthis opalescens squid are optically active upon the stimuli of a neurotransmitter (ACh) (Fig. 5C).81 The leucophore-based white stripes in these animals can dynamically switch their appearances from a highly transparent state to a diffusive white-colored state upon activation (Fig. 5C), as quantified by an over 15% increase in the broadband reflectance, and the whole process takes around three minutes.81 This finding represents one of the very few reported examples of tunable leucophores in any cephalopod species, and a comprehensive understanding of possible structural and molecular mechanisms behind such optical modulation remains limited.
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Fig. 6 Reflectin proteins derived from cephalopod skin as dynamic optical materials. (A) (i) The location of reflective and non-reflective tissues of an E. scolopes squid.83 (ii) A cross-sectional light micrograph of the light organ.83 (iii) and (iv) Transmission electron microscopy (TEM) images of the orange boxed region in (ii) at different magnifications, showing arrangements of reflective protein platelets.83 (v) Linear amino acid sequence of a full-length reflectin 1a isoform, showing repeated domains highlighted in different colors.83 (B) (i) An illustration of the fabrication of a reflectin 1a-based thin film on a rigid substrate by flow coating.85 (ii) Images of a reflectin 1a-based thin film reversibly changing the color from orange (left) to blue (right) upon the application of water vapor.85 (iii)–(v) SEM images of diffraction grating made from reflectin 1a, featuring tunable grating spacing; (vi) an optical microscope image of a highly amorphous fiber made from reflectin 1a; (vii) an SEM image of another amorphous fiber made from reflectin 1a with a much smaller diameter.85 (C) (i) Structural coloration, (ii) atomic force microscope (AFM) images of the surface topography, and (iii) normalized visible-to-near-IR reflectance spectra of monolayers composed of DBCO-conjugated reflectin B1 nanospheres with tunable sizes.98 The nanospheres were self-assembled and deposited on an azide-functionalized wafer via a Langmuir–Schaefer approach.98 (D) (i) Schematics of a RfA1-based protochromic device with the application of no bias (middle), a positive bias (left), and a negative bias (right) on the palladium hydride (PdHx) electrode, featuring a thickness change in the constituent RfA1 layer upon proton injection or extraction.99 (ii) Normalized reflectance spectra for a representative RfA1-based protochromic device before (green curve) and after (red curve) the application of a positive bias of +1.5 V on the PdHx electrode.99 (iii) Normalized reflectance spectra for a representative RfA1-based protochromic device before (green curve) and after (blue curve) the application of a negative bias of −1.5 V on the PdHx electrode.99 (E) Schematics of voltage-induced swelling and shrinkage of a reflectin film on a Pt working electrode, showing simultaneous changes in film thickness and refractive index for structural color modulation.101 (F) Schematics of photo-controlled electrostatic interactions between RfA1 and a multivalent AzoEDTA-based photoswitch with anionic end groups, showing reversible modulation of assembly size under different light wavelengths.103 (G) Schematics of a RfA1-expressed human cell before (left) and after (right) applications of chemical stimuli, featuring changes in the size, geometry, and arrangement of the RfA1 nano-aggerates within the cell, which lead to changes in light transmission and reflection. The actual transparency modulation of a cell-containing solution is shown by the optical images.104 Part A was reproduced with permission from Springer Nature (Copyright©2004). Part B was reproduced with permission from Springer Nature (Copyright©2007). Part C was reproduced with permission from the American Chemical Society (Copyright©2022). Part D was reproduced with permission from John Wiley and Sons (Copyright©2017). Part E was reproduced with permission from John Wiley and Sons (Copyright©2025). Part F was reproduced with permission from the Royal Society of Chemistry (Copyright©2024). Part G was reproduced with permission from Springer Nature (Copyright©2007). |
Reflectin-based optical materials | Gene origin | Material production | Device format | Device fabrication | Device substrate | External stimuli | Optical functionality | Ref. |
---|---|---|---|---|---|---|---|---|
Reflectin 1a | Euprymna scolopes | Escherichia coli (E. coli) expression | Thin films | Flow coating | Silicon (Si) | Chemical (water, methanol, ethanol vapors) | Change in reflectance (visible) | 85 |
Reflectin 1a | Euprymna scolopes | E. coli expression | Diffraction gratings | Dipping | Si | — | Interference-based optical gratings | 85 |
Reflectin 1a | Euprymna scolopes | E. coli expression | Fibers | Drawing from precipitates | — | — | Reduced optical scattering | 85 |
Reflectin-based peptide (refCBA) | Euprymna scolopes | E. coli expression | Thin films (multilayered) | Flow coating & spin-coating | Si | Chemical (water vapor) | Change in reflectance (visible) | 93 |
Reflectin 1b and derived peptides (e.g., 2CX4) | Euprymna scolopes | E. coli expression | Thin films | Flow coating | Si | Chemical (water vapor) | Change in reflectance (both specular and scattered components in the visible) | 94 |
Reflectin 2 | Sepia officinalis | E. coli expression | Thin films | Spin-coating | Si or glass | Chemical (water vapor) | Change in reflectance and transmittance (visible) | 95 |
Reflectin A1 | Doryteuthis pealeii | E. coli expression | Thin films | Doctor-blading | Graphene oxide-coated SiO2/Si | Chemical (water, acetic acid vapors) | Change in reflectance (visible to near-IR) | 96 |
Reflectin A1 | Doryteuthis pealeii | E. coli expression | Stretchable films | Doctor-blading | Fluorinated ethylene propylene (FEP) tape | Mechanical strain | Change in reflectance (visible to near-IR) | 97 |
Reflectin B1 (ligand conjugated) | Sepioteuthis lessioniana | E. coli expression | Thin films assembled by nanoparticles | Langmuir− Schaefer deposition & drop-casting | Azide-functionalized SiO2 | Chemical (water vapor) | Change in reflectance (visible to near-IR) | 98 |
Reflectin A1 | Doryteuthis pealeii | E. coli expression | Thin films | Drop-casting or dip-coating | SiO2/Si | Electrical bias | Change in reflectance (visible) | 99 |
Reflectin A1 | Doryteuthis opalescens | E. coli expression | Thin films | Drop-casting | Pt/Si | Electrical bias | Change in refractive index (632.8 nm) | 101 |
Reflectin A2 (phytochrome-doped) | Doryteuthis opalescens | E. coli expression | Thin films | Spin-coating | Si | Light | Change in reflectance (visible) | 102 |
Reflectin A1 (azoEDTA-coupled) | Doryteuthis opalescens | E. coli expression | Solution | Solution mixing | — | Light | Change in absorbance (visible) and turbidity | 103 |
Reflectin A1 | Doryteuthis pealeii | Human embryonic kidney (HEK) 293 cells | Cells dispersed in solution | Genetic transfection | — | Chemical (ionic strength of NaCl) | Change in transparency (Visible) | 104 |
In a pioneering study, Kramer et al. used flow coating to fabricate recombinantly expressed reflectin 1a into uniform thin films (Fig. 6B(i)).85 The film thickness was adjusted by changing the reflectin 1a solution concentration, which results in different structural colors governed by thin-film interference. A color shift was observed from blue to yellow upon exposure to water vapor, which was caused by an increase in film thickness due to swelling (Fig. 6B(ii)). The unique in vitro self-assembling properties of reflectin were further demonstrated through the formation of iridescent diffraction gratings with tunable micron-scale spacing via ionic liquid-facilitated phase separation, featuring defect-free patterns over several millimeters (Fig. 6B(iii)–(v)).85 Moreover, reflectins were drawn into fibers with tunable diameters using high-viscosity precipitates (Fig. 6B(vi) and (vii)), which exhibited a lack of crystallinity that can minimize unwanted scattering in optical applications.85 Similarly, both single-layer and multilayer reflectin derivatives (e.g., refCBA from reflectin 1a,93 2CX4 from reflectin 1b94) were shown to display thickness-dependent structural colors that can be modulated through exposure to water vapor. Besides thin-film interference, wavelength-dependent light scattering was found critical for the dynamic blue color displayed by reflectin films, driven by higher-order self-assembly in the presence of aromatic triggers.95
Further efforts have been made to extend the optical functionality of reflectin-based devices from the visible to the IR regions of the electromagnetic spectrum. This was achieved through more substantial modulation of film thickness via various external stimuli (e.g., chemical and mechanical) or tunable assembly sizes that red-shift the wavelength of constructive interference into the IR region. Phan et al. applied doctor blading to prepare thin films from a histidine-tagged reflectin A1 (RfA1) isoform on a negatively charged graphene oxide-coated silica substrate.96 Upon exposure to acetic acid vapor, the RfA1 film swelled, increasing its thickness from 207 nm to 394 nm, and thereby shifted its reflection peak from the visible (∼625 nm) to the near-IR (∼1200 nm) region.96 Moreover, the same RfA1 was directly coated onto flexible adhesive tape, which could be easily attached onto fabrics for camouflage use.97 The devices’ near-IR reflectance peaks were modulated by mechanically stretching the tape substrate, as the film thickness changed due to the strain-induced Poisson effect.97 In another study, spherical reflectin B1 nanoparticles were immobilized onto azide-functionalized substrates via dibenzocyclooctyne (DBCO)-sulfo-NHS ester-based ligands.98 These self-assembled nanoparticles exhibited tunable sizes ranging from 170 nm to 310 nm, allowing the reflectance peaks of the resulting films to shift from blue to the near-IR region (Fig. 6C(i)–(iii)).98
Electrical stimuli have been explored to trigger color changes in reflectin-based thin-film devices. By leveraging reflectin's exceptional ability to conduct protons, Ordinario et al. reported a two-terminal protochromic device that consisted of a RfA1 film sandwiched between a palladium hydride (PdHx) electrode and a gold (Au) electrode.99 PdHx served as a proton reservoir, while Au served as an ion-blocking electrode. Upon application of a positive (negative) voltage, protons are injected (withdrawn) from PdHx into (from) the RfA1 layer, resulting in an increase (decrease) in its thickness and thus an ∼20-nm red (blue) shift in its peak reflection wavelength (Fig. 6D).99 In another study, voltage-dependent electrochemical reduction was shown to reversibly change the size of RfA1 assemblies through a charge-neutralization process that closely resembles the phosphorylation-driven condensation observed in biological iridophore lamellas.100,101 This mechanism was experimentally validated on a platinum (Pt) electrode using electrochemical correlative ellipsometry, where applying a small voltage (up to −0.8 V) reduced the RfA1 film thickness and increased its refractive index from 1.36 to 1.40 at a wavelength of 632.8 nm (Fig. 6E).101 These concurrent changes in film geometry and optical properties show promise for the continued development of iridophore-like, color-changing devices.
Light-responsive reflectin-based devices with tunable optical properties have been developed. One approach is to integrate reflectins with photosensitive molecules, where the light-driven changes are mainly contributed by the photosensitive molecules rather than reflectins. For example, Wolde-Michael et al. reported a bilayer device composed of reflectin and phytochrome-1 protein (from Agrobacterium fabrum).102 Due to a photo-induced conformational change in phytochrome between the open and closed states, the phytochrome layer exhibited a color change with its reflectance peak shifting from ∼750 nm to ∼710 nm upon exposure to different wavelengths of light, thereby adjusting the overall appearance of the reflectin-phytochrome bilayer device. Another approach is to leverage dynamic inter-/intra-molecular interactions between reflectins and photosensitive molecules upon light exposure. Tobin et al. designed a multivalent azobenzene photoswitch (azoEDTA) molecule with anionic end groups to form complex assemblies with RfA1.103 Photoisomerization of azoEDTA between the trans and cis states altered its electrostatic crosslinking dynamics with the cationic blocks in RfA1, which enabled repeated modulation of the size and secondary structure of the reflectin-azoEDTA assemblies (Fig. 6F). The average diameter of the assemblies cycled between 74 ± 52 nm and 39 ± 25 nm upon repeated exposure to 365-nm and 470-nm light, resulting in reversible control of solution absorbance and turbidity.
Recently, reflectins have been explored for integration into engineered living cells for stimuli-responsive optical modulation. Chatterjee et al. reported the direct expression of a histidine-tagged RfA1 within human embryonic kidney (HEK) 293 cells through transfection with a target vector encoding.104 Due to the formation of reflectin nano-aggerates, the initially transparent HEK cells became less transparent after transfection, exhibiting an increased level of scattering (i.e., diffuse transmission and reflection). In analogy to the ACh-regulated, transparency-modulating leucophores in Doryteuthis opalescens, the RfA1-containing HEK cells were able to modulate their optical transparency in response to chemical stimuli such as sodium chloride (NaCl).104 An increase in the NaCl concentration from 117 mM to 217 mM resulted in an ∼2-fold increase in the solution's diffuse transmittance and reflectance (Fig. 6G). This enhanced scattering was attributed to changes in the size, geometry, and arrangement of reflectin nano-aggerates under varied ionic strength, which significantly altered the visible opacity of the host cells.104 Similar optical tunability were observed in both transiently and stably transfected RfA1-expressing cells.105
Xa-Based Optical Materials | Material Production Approach | Device Format | Device Fabrication | Device Substrate | External Stimuli | Optical Functionality | Refs |
---|---|---|---|---|---|---|---|
Xa | Chemical synthesis | Thin films | Electrodeposition | PEDOT:PSS-modified ITO | Electrical bias | Change in color (from yellow to red) | 115 |
Xa | Chemical synthesis | Thin films | Inkjet printing | PET sheet | Electrical bias | Change in color (from yellow to red) | 116 |
Xa | Chemical synthesis | Thin films | Casting | Chromatography paper | Ultraviolet light | Change in color (from yellow to red) | 118 |
Xa–SiO2 composite | Chemical synthesis (silification) | Nanoparticle coatings | Drop-casting | Glass & Spandex fabrics | Chemical (ascorbic acid) | Change in color (from yellow to red) | 113 |
Xa–TiO2 composite | Chemical synthesis & Composite mixing | Paint films | Spray-coating | Polyurethane | Ultraviolet light | Change in color (from yellow to red) | 114 |
Xa–polystyrene (PS) composite | Chemical synthesis (carboxylation) | Powder-pressed films | Mechanical press | Glass | Nanoparticle size & loading | Change in reflectance (various colors) | 111 |
Xa–PS–Triblock copolymer (TBC) composite | Chemical synthesis | Colloidal suspension | Suspension injection | ITO glass | Electrical bias | Change in color (from blue to beige) | 117 |
Xa–PS microcapsules | Chemical synthesis | Water-oil–water double emulsion capsules | Capillary-based microfluidic injection | — | Chemical (osmotic pressure change due to NaCl concentration) | Color switching between green (structural) and brown (pigmentary) | 112 |
Pristine Xa is known as a color-changing biochrome depending on its redox states. Kumar et al. developed a Xa-based electrochromic device, where Xa was coated onto an indium-doped tin oxide (ITO)-based substrate that was pre-modified with poly(3,4-ethylene dioxythiophene):poly(styrene sulfonate) (PEDOT:PSS) (Fig. 7A(i)).115 The device was able to switch from yellow under an oxidizing potential (+1.5 V) to red under a reducing potential (−1.5 V), with a red shift in the absorption peak by ∼70 nm (Fig. 7A(ii) and (iii)).115 By varying the ratio of Xa and (blue-tinted) PEDOT:PSS, different color combinations were achieved (Fig. 7A(iv)), although they were limited to the yellow-red regions.115 To improve device scalability, Sullivan et al. introduced inkjet printing to prepare Xa-based electrochromic pixels and enabled multilayer printing, array fabrication, and pixel miniaturization with enhanced precision (Fig. 7B(i)).116 Each pixel could be precisely patterned, with color switchable between yellow and red depending on the redox states of Xa (Fig. 7B(ii)).116 In addition to electrochemical processes, Xa exhibits a photoreduction-induced color change from yellow to red under solar radiation. Using this mechanism, Wilson et al. developed a wearable Xa-based light sensor capable of monitoring light exposure from UV to near-IR via chromaticity shifts (Fig. 7C).118 To enhance the device's light-sensing performance, cystine solution was added to Xa, which enabled radiation-triggered formation of cysteine–a reducing agent that facilitates color change in Xa.118
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Fig. 7 Xanthommatin (Xa) Pigment Derived from Cephalopod Skin as Dynamic Optical Materials. (A) (i) Schematic of a Xa-based electrochromic device with a multilayered structure.115 (ii) Proposed chemical structures of Xa in its oxidized (left) and reduced (right) states.115 (iii) Absorption spectra of oxidized and reduced Xa films on a PEDOT:PSS-modified ITO substrate. (iv) Optical images showing the colors of four independent Xa-based electrochromic devices in oxidized (top) and reduced (bottom) states.115 (B) (i) Schematic of an inkjet-printed Xa-based electrochromic pixel.116 (ii) Optical images of miniaturized pixels with similar color-changing performance, showing switchable colors in both outer and inner electrodes depending on the redox state.116 (C) (i) Schematic of a wearable Xa-based light sensor with patterned microfluidic channels.118 (ii) Radiation exposure detection by measuring the chromaticity shift in Xa light sensors under varying intensity of erythemally weighted ultraviolet radiation (UVEry).118 (iii) Distinct color change in a cystine-activated Xa light sensor from yellow to red upon exposure to 1 J cm−2 UVB light.118 (D) (i) Synthesis scheme of Xa-encapsulated silica nanoparticles (XaNPs).113 (ii)–(v) Optical images of a Spandex fabric coated with only silica nanoparticles (SiNPs) or XaNPs at different states (i.e., original, acid-reduced, and re-oxidized).113 (E) (i) Schematic of photo-induced color change in Xa when incorporated with photo-electronic TiO2 nanoparticles of different sizes.114 (ii) Change in the hue angle of Xa–TiO2 films upon exposure to various wavelength bands in the UV, visible, and IR regions.114 (iii) Optical images of Xa–TiO2 films blended with a photo-insensitive pigment of ultramarine in two different formulations, showing expanded color space and similar photochromic performance.114 Panel size: ∼500 mm2. (F) (i) Synthesis of Xa-functionalized PS nanoparticles via surface carboxylic acid groups.111 (ii) SEM image of amorphous photonic structures formed by mixing both pristine and Xa-functionalized PS nanoparticles.111 (iii) Optical images showing the achievable color palette by varying the PS nanoparticle size (vertical axis) and the amount of Xa-functionalized PS (horizontal axis) (scale bar: 6 mm).111 (G) (i) Schematic of an electrophoretic display made from triblock copolymer-stabilized Xa–PS (Xa/TBC-PS) nanospheres. The display color is tunable through reversible particle distribution driven by electrostatic interactions.117 (ii) SEM image of self-assembled Xa/TBC-PS nanospheres prepared by solution dropcasting on a glass substrate.117 (iii) An 8-pixel electrophoretic display made from Xa/TBC-PS before (left) and after (right) activation. The electrically activated pixels appeared in blue, and the non-activated pixels appeared light beige.117 (iv) Reflectance intensity at 555 nm for a representative pixel over 22 repeated cycles.117 (H) (i) Schematic of the fabrication of chromatophore-like capsules using a capillary-based microfluidic device.112 (ii) Transmission (top) and reflection-mode (bottom) optical microscope images of chromatophore-like capsules reversibly switching between expanded and compressed states upon increased salt concentration, displaying bright green or dark brown colors dictated by pigmentary or structural coloration.112 Part A was reproduced with permission from the American Chemical Society (Copyright©2018). Part B was reproduced with permission from John Wiley and Sons (Copyright©2023). Part C was reproduced with permission from the American Chemical Society (Copyright©2022). Part D was reproduced with permission from the American Chemical Society (Copyright©2021). Part E was reproduced with permission from John Wiley and Sons (Copyright©2023). Part F was reproduced with permission from John Wiley and Sons (Copyright©2021). Part G was reproduced with permission from the American Chemical Society (Copyright©2025). Part H was reproduced with permission from the Royal Society of Chemistry (Copyright©2024). |
Various inorganic particles (e.g., SiO2, TiO2) have been incorporated with the Xa pigment to expand the resulting devices’ optical functionality. Using a diatom-inspired biosilification process, Martin et al. fabricated Xa-silica nanoparticles (XaNPs) by encapsulating Xa onto silica nanoparticles in the presence of amine-terminated polyamidoamine (PAMAM) dendrimers and monosilicic acid via electrostatic interactions (Fig. 7D(i)).113 A range of neutral colors with varying hues were obtained by adjusting the Xa loading concentration. The resulting XaNPs could be easily processed and casted onto flexible Spandex fabrics, exhibiting homogeneous particle distribution on the individual fibers. Benefiting from XaNPs’ mesoporous structures, the color of the XaNP-coated fabrics was tunable by changing the local pH, such as through exposure to ascorbic acid, through a plausible proton-coupled reduction mechanism (Fig. 7D(ii)–(v)).113 In another study, Martin et al. developed a color-changing paint formulation by leveraging the redox-dependent absorption of Xa and the photoelectronic properties of titanium dioxide (TiO2).114 As a common photocatalyst and whitening agent, TiO2 is known to generate excited electrons from the valence to the conduction band when exposed to light with wavelengths below 400 nm.119 These excited electrons can readily convert Xa from oxidized (yellow) to reduced (red) states (Fig. 7E(i)). The resulting Xa-TiO2 exhibited a significant color change under UVA light (wavelength from 315 nm to 400 nm), while negligible change was noticed under visible-NIR light (wavelength above 400 nm) (Fig. 7E(ii)).114 Furthermore, the devices’ color space were expanded into blue-green regions by blending other photo-insensitive natural pigments (e.g., ultramarine) (Fig. 7E(iii)).114
Synthetic organic particles have been engineered to produce short-wavelength structural coloration, which can be coupled with the intrinsic long-wavelength pigmentary coloration of Xa pigments to significantly expand the achievable color space. Polystyrene (PS) nanospheres are well-known building blocks for forming photonic crystals with tunable structural colors by adjusting the size and packing of spheres.120 By tethering Xa onto carboxylic acid-functionalized PS nanospheres, Lin et al. fabricated amorphous photonic assemblies with tunable color and contrast by changing the nanosphere size and loading concentration (Fig. 7F(i)).111 The incorporation of Xa into PS preserved the short-range structural order but disrupted the long-range order in the assemblies, resulting in angle-independent colors (Fig. 7E(ii) and (iii)).111 In another study, Lee et al. functionalized Xa-impregnated PS nanospheres with a triblock copolymer (TBC) made of polyethylene glycol–polypropylene glycol–polyethylene glycol through a swelling–deswelling process (Fig. 7G(i) and (ii)).117 An electrophoretic display was fabricated by sandwiching the Xa–PS–TBC suspension between two ITO glass electrodes. Upon application of a direct-current (DC) electrical field, negatively charged Xa–PS–TBC particles are attracted to and organized at the positively charged electrode, displaying a blue structural color (Fig. 7E(iii)). Once the electrical field is withdrawn, the particles are redispersed, displaying a light beige color. The incorporation of TBC effectively enhanced the colloidal stability and cyclic reversibility under electrophoretic control (Fig. 7E(iv)).117 Furthermore, Kim et al. fabricated stimuli-responsive double emulsion microcapsules from Xa-functionalized PS particles that can dynamically switch between pigmentary and structural coloration.112 The microcapsules were produced using a capillary-based microfluidic device to form stabilized water-in-oil-in-water assemblies, with aqueous suspended Xa–PS particles in the core (Fig. 7H(i)).112 Upon an increase in osmotic pressure (e.g., adding NaCl), the microcapsules underwent shrinkage with densely packed PS particles in the core, revealing bright green color from structural coloration (Fig. 7H(ii)). Once the osmotic pressure was removed, the microcapsules slowly returned to an expanded state, and the PS particles became loosely packed with a dominant pigmentary-based brown color.112
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Fig. 8 Cephalopod skin-inspired systems with tunable optical properties in the visible. (A) (i) Illustration of a cephalopod skin-like, multiplexed flexible monochromatic display with distributed sensing and actuating capabilities.121 (ii) Each individual unit within the array features a five-layer device structure consisting of an artificial chromatophore (ac), an artificial leucophore (al), artificial muscle (am), a PDMS substrate, and an artificial opsin unit (ao). Optical images of a multiplexed display with 256 active pixel units, displaying (iii) spatial patterns (e.g., dots) and (iv) letters of ‘U o I’ even when bent.121 (B) (i) Squid skin-inspired camouflage display for aquatic environments, featuring tunable body transparency in response to environmental lighting.122 The display consists of an array of six electrochromic display pixels integrated with a wireless control system. (ii) Demonstration of the operation of the wireless adaptive camouflage display in response to gradually dimming underwater lighting conditions through a voltage-controlled electrochromic process.122 (C) (i) Schematics of a cephalopod color-changing skin that mimics the interplay between size-changing pigmentary chromatophores and structurally colored iridophores.124 (ii) and (iii) Various colors produced by overlaying green or blue iridophores with thermally responsive chromatophores that undergo volume shrinkage at elevated temperatures.124 (D) Schematics of the working mechanism of a light-responsive artificial chromatophore (LAC), featuring dynamic actuation of a stretchable sac and photo-active muscles under light.125 (ii) Light-induced actuation of a LAC unit over time, showing expansion in the white area (i.e., stretchable sac).125 (iii) Quantitative characterization of the light-induced strain and white area ratio in a representative LAC as a function of light irradiation time.125 Part A was reproduced with permission from the National Academy of Sciences (Copyright©2014). Part B was reproduced with permission from Springer Nature (Copyright©2024). Part C was reproduced with permission from John Wiley and Sons (Copyright©2025). Part D was reproduced with permission from the American Chemical Society (Copyright©2021). |
Moving down to the organ/cellular scale, the structures and working principles of individual cephalopod skin components (e.g., chromatophores and iridophores) have attracted extensive attention for bioinspired adaptive optical systems that control visible light. Zhou et al. introduced a color-changing skin by mimicking the intricate interplay between chromatophores and iridophores (Fig. 8C(i)).124 To mimic chromatophores, a temperature-responsive poly(N-isopropyl acrylamide) (PNIPAAm)-based hydrogel film was fabricated by dispersing pigments including natural cuttlefish ink (brown), FeCl3 solution (yellow), and Ponceau S (pink) to render different pigmentary colors. The hydrogel film could shrink upon heating above its volume-phase transition temperature and thus reversibly change its size and color concentration when exposed to an IR laser. To mimic iridophores, structurally colored layers exhibiting green and blue hues were fabricated using PS nanoparticles. By overlaying the artificial chromatophore and iridophore layers, multiple color combinations were obtained and could dynamically respond to environmental thermal stimuli (Fig. 8C(ii) and (iii)).124 In another study, Han et al. reported a light-responsive artificial chromatophore (LAC) capable of appearance modulation via light-driven actuation.125 A single LAC consisted of two active components: a photoactive muscle and a stretchable, color-changing sac (Fig. 8D(i)). The photoactive muscle was made of a PNIPAAm hydrogel embedded with photothermal polydopamine (PDA) nanoparticles, which generated heat upon light exposure, causing the hydrogel matrix to shrink. The elastic sac was made of an acrylic acid hydrogel with ionic crosslinking (Fe3+) that could be stretched over 200%. Through multi-material projection micro-stereolithography, these two components were printed to form an LAC unit that could reversibly change its visual appearance (i.e., black-to-white ratio) in response to both temperature and light stimuli (Fig. 8D(ii) and (iii)).125
Besides tunable optical properties, cephalopod skin has also inspired numerous luminescence-based technologies involving the control of light emission in response to external stimuli such as light, electricity, heat, strain, and chemical reactions.126–130 Morin et al. developed pneumatically actuated soft camouflage crawling robots by embedding a network of microfluidic channels into a deformable silicone rubber (Fig. 9A(i)).126 Injection of different liquids into the microfluidic channels allowed dynamic modulation of the pigmentary, fluorescent, and chemiluminescent appearances of the soft robots (Fig. 9A(ii) and (iv)).126 In addition, Wang et al. developed a chromatophore-like, electro-mechano-chemical responsive system using a spiropyran-blended mechanochromic elastomer for active fluorescent modulation (Fig. 9B).127 Upon mechanical stretching, the elastomer switched from light yellow to blue, accompanied by an increase in fluorescence emission intensity due to a ring-opening reaction of spiropyran to form merocyanine. By sandwiching the mechanochromic elastomer between two transparent electrodes, crater-like patterns were formed under high voltage due to electrostatic attraction-induced wrinkling instability, thereby revealing bright red fluorescent patterns at the strained crater edges, with intensity tunable by adjusting the electric field strength.127 Inspired by the regenerative ability of cephalopod skin, self-healing functionality was further incorporated into mechanoluminescent skins via dynamic supramolecular interactions involving boroxine and hydrogen bonds.128 The mechanoluminescence performance was able to fully recover even after severe mechanical damage.128 In another study, Larson et al. developed a cephalopod-inspired electroluminescent skin, featuring a five-layer architecture composed of a zinc sulfide (ZnS) phosphor-based light-emitting layer sandwiched between two ionic hydrogel electrodes and encapsulated by a pair of silicone shells (Fig. 9C(i)).129 The electroluminescent layer could emit light in different colors depending on the type of metal dopant in the ZnS. Multipixel soft skins were shown to maintain consistent light-emitting performance under various deformation modes, including stretching, rolling, folding, and wrapping (Fig. 9C(ii)).129
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Fig. 9 Cephalopod skin-inspired systems with light-emitting functions in the visible. (A) (i) Top view (top) and cross-sectional view (bottom) of the body design of a cephalopod-inspired soft camouflage crawling robot, featuring microfluidic channels embedded in a silicone matrix.126 Optical images of the cephalopod-inspired soft robot showing various camouflage displays, including (ii) pigmentary, (iii) fluorescent, and (iv) chemiluminescent patterns.126 (B) (i) Cross-sectional schematics of a chromatophore-like, electro-mechano-chemical responsive (EMCR) device before (left) and after (right) electrical actuation, featuring an electrically induced deformation of the EMCR elastomer. (ii) Optical microscopy images of an EMCR device before (left) and after (right) electrical actuation, featuring dynamic surface structures. (iii) Fluorescent microscope images of the same EMCR device before (left) and after (right) electrical actuation, featuring dynamic fluorescent patterning.127 (C) (i) Schematic of a cephalopod-inspired electroluminescence skin with a five-layer device structure.129 (ii) (Top) Digital camera images of a multiplexed electroluminescent skin (with blue-light emission) under various deformation modes, including stretching, rolling, folding, and wrapping. (Bottom) Digital camera images of another electroluminescent skin (with orange-light emission) displaying various patterns.129 Part A was reproduced with permission from The American Association for the Advancement of Science (Copyright©2012). Part B was reproduced with permission from Springer Nature (Copyright©2014). Part C was reproduced with permission from The American Association for the Advancement of Science (Copyright©2016). |
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Fig. 10 Cephalopod skin-inspired dynamic optical systems in the infrared (IR). (A) (i) Top-view schematics of a dielectric elastomer-based adaptive IR-reflecting camouflage system with a size-variable IR-reflecting active area upon actuation, resembling chromatophores.131 (ii) Cross-sectional schematics of the same IR-reflecting camouflage system, showing iridophore-inspired tunable surface morphology of the IR-reflecting coatings upon actuation.131 (iii) SEM images of the morphology of a 20 nm aluminum (Al)-coated IR-reflecting system before (left) and after (right) mechanical actuation, featuring a drastic transition from highly wrinkled to flat, smooth surfaces.131 (iv) Broadband IR reflectance modulation of the Al-coated IR-reflecting system before (left) and after (right) mechanical actuation, showing strain-tunable total, diffuse, and specular reflectance.131 (B) (i) Side-view schematics of a chromatophore-inspired, liquid metal-dispersed elastomer with variable size and surface morphology under equiaxial stretch.133 (ii) 3D-reconstructed micro-CT images of the composite with 30 vol% of liquid metal doping under 0% (left) and 200% (right) equiaxial strain.133 (C) (i) Schematics of a chromatophore-inspired dynamic thermoregulatory composite featuring tunable IR transparency via microcrack engineering.134 (ii) Optical images of a representative composite before (left) and after (right) the application of 50% uniaxial strain. Insets: SEM morphology images (top) and elemental maps (bottom) at 0% and 50% strain.134 (iii) Plot of estimated environmental setpoint temperatures at which an individual would remain comfortable. Quantitative comparisons were made between the cephalopod-inspired composite and other commonly available fabric materials, showing a large tunable thermo-comfort window of the composite upon strain.134 (D) (i) Cross-sectional schematics of a Japetella heathi squid-inspired system for dynamic multispectral transparency modulation across the visible and IR regions, showing active control of the total, diffuse, and specular transmittance through actuation-induced geometrical and morphological changes.136 (ii) Optical images of a multispectral transparency-modulating device functioning in the visible region upon electromechanical actuation.136 (iii) IR camera images of the same multispectral transparency-modulating device functioning in the thermal IR region upon electromechanical actuation by reversibly revealing and hiding the modified Starry Night.136 Part A was reproduced with permission from The American Association for the Advancement of Science (Copyright©2018). Part B was reproduced with permission from Elsevier Ltd. (Copyright©2023). Part C was reproduced with permission from Springer Nature (Copyright©2019). Part D was reproduced with permission from John Wiley and Sons (Copyright©2020). |
In several follow-up studies, various IR-reflecting photonic components have been developed for integration onto or into similar stretchable elastomer-based platforms, with their surface morphologies and IR properties tunable upon mechanical or electromechanical stimuli. As an example, Liu et al., embedded copper (Cu) nanostructures into a thermoplastic elastomer made of styrene–ethylene–butylene–styrene (SEBS).132 The presence of mechanical mismatch between the Cu and the soft SEBS matrix led to the formation of distinct nano- or micro-structures on the SEBS surface upon applied tensile or compressive strains, which in turn resulted in different thermal appearances for dynamic IR signature management.132 Similarly, liquid metal (LM) microdroplets were dispersed into silicone elastomers.133 Upon equiaxial strain, the LM microdroplets underwent shape transformation due to their malleable form factor, transitioning from contracted dots with wrinkled surfaces to expanded plate-like discs with flat surfaces, thereby enabling dynamic modulation of IR reflection and emissivity (Fig. 10B).133
Besides reflection, other IR radiative properties (e.g., transmission, absorption, and emissivity) have been explored using cephalopod-inspired designs. By mimicking the opening and closure of chromatophores, Leung et al. developed a dynamic IR composite with tunable IR transparency through microcrack engineering (Fig. 10C(i)).134 In their design, a nanostructured Cu film was deposited through glancing angle deposition, with extended Cu pillars anchored into a SEBS elastomer. Upon uniaxial strain, microcracks were formed in the elastomer-bound Cu due to mechanical mismatch, allowing more IR radiation to transmit through the microcracks (Fig. 10C(ii)). By increasing the applied strain from 0% to 50%, the average total IR transmittance increased from ∼1% to ∼24%, corresponding to an increase in the transmitted heat flux from ∼248 W m−2 to ∼307 W m−2. This substantial change in radiative heat transfer readily enabled the use of this composite in a wearable thermoregulatory sleeve, theoretically allowing the wearer to maintain thermal comfort across an environmental setpoint temperature window of ∼8.2 °C (Fig. 10C(iii)).134 Later, Badshah et al. demonstrated scalable manufacturing of similar composites with a low estimated material cost of ∼0.1 US$ per m2, with comparable dynamic heat-regulating performance validated in beverage packaging scenarios.135 In another work, Xu et al. draw inspiration from the Japetella heathi squid and designed a single device to achieve unprecedented dynamic modulation of multispectral light transmission across the visible and far-wavelength IR regions (wavelengths between 400 nm and 16.6 μm) (Fig. 10D(i)).136 A tri-layer device architecture was constructed with a pair of IR-transparent block copolymers (PBCs) sandwiching an IR-absorbing acrylate elastomer. Upon mechanical actuation, the device's broadband specular-to-diffuse transmission ratios were modulated by >3000-fold in the visible, due to the strain-dependent reorganization of surface microstructures in the IR-transparent PBCs, and by >4-fold in the IR, due to the strain-dependent thickness in the IR-absorbing acrylate elastomer. This exceptional IR transparency-modulating performance was maintained under electromechanical actuation, featuring a rapid response time of ∼570 ms and excellent cycling stability of over 2000 cycles for unprecedented multispectral camouflage (Fig. 10D(ii) and (iii)).136 This device platform was further modified by incorporating a stimuli-responsive acene-based dye that allowed tuning of its absorption peak and enabled dynamic near-IR appearance modulation.137
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Fig. 11 Cephalopod skin-inspired visual shape-morphing systems. (A) (i) A Macroctopus maorum octopus sitting on the ocean floor, showing actuated papillae in the skin.138,139 (ii)–(iv) One of the octopus's skin papillae was rapidly actuated and displaced within 0.22 s. (B) (i) Schematic of a pneumatically actuated artificial papilla made from a circumferentially constrained and radially stretched elastomer.138 (ii) Incorporation of suspended mesh supports enables high-fidelity deformation.138 (iii) Demonstrations of the shape-morphing capability of the papillae-inspired surfaces, mimicking rocks (top) and a Graptoveria amethorum succulent plant (bottom).138 (C) (i) Schematic (left) and temperature map (right) of a papillae-inspired, spirally twisted, thermally responsive fiber coil before Joule heating, feature a flat profile.139 (ii) Schematic (left) and temperature map (right) of the same fiber coil after Joule heating, exhibiting clear vertical extension due to thermally induced uncoiling.139 (iii) Integration of an actuatable fiber coil in an octopus replica.139 Insets: Papillae-like skin displacement are shown upon heating. Part A was reproduced with permission from The American Association for the Advancement of Science (Copyright©2017) and John Wiley and Sons (Copyright©2021). Part B was reproduced with permission from The American Association for the Advancement of Science (Copyright©2017). Part C was reproduced with permission from John Wiley and Sons (Copyright© 2021). |
Moving forward, vast challenges and opportunities exist to further our understanding of the biological materials (e.g., reflectins) behind cephalopod's camouflage feats and development of bioinspired optical materials and technologies. Despite the important role of reflectins in cephalopods’ optical functionalities, important knowledge gaps remain regarding the molecular structure–function relationships of these intrinsically disordered proteins, as well as their self-assembly into various forms under physiological conditions. The conformational changes within reflectins upon different environmental stimuli (e.g., ionic concentration, pH) are not well understood at the molecular level. In addition, although reflectins have been studied in a few isoforms from select cephalopod species, the specific sequence motifs responsible for their hierarchical assembly remain underexplored, with limited information linking molecular features to macroscopic optical functionality. This knowledge gap is further complicated by the diversity of wild-type isoforms across cephalopod species. Although not discussed in the scope of this review, reflectins are among the best naturally occurring protein-based proton conductors;21,91,92 however, it remains unclear whether this remarkable bioelectrical property contributes to rapid optical switching via signal transduction, particularly given our limited understanding of reflectin–membrane interactions in color-changing cells. While substantial interdisplinary effort is needed to address these gaps, elucidating these mechanisms would inform a multiscale approach to effectively utilize or engineer reflectin-based biomolecules and guide the rational design of synthetic or biohybrid materials with cephalopod-like functionalities, for example, building LEGO-like block copolymers with building blocks inspired by reflectins’ functional motifs.
Although the cellular-level understanding of the bio-optical components within cephalopod skin is largely established, no existing artificial device has yet been developed that fully replicates these dynamic structures with comparable sophistication, performance, and efficiency. In essence, nature evolves based on a “just-enough” principle by balancing functionality with limited available materials, where often non-ideal structures are grown via a bottom-up approach. While traditional silicon-based electronics and emerging soft electronics offer ultrahigh manufacturing precision (not to mention access to a vast library of exotic materials), existing cephalopod-inspired optical devices are still fabricated via a top-down approach and remain largely in the proof-of-concept stage. One promising route forward is the bottom-up growth of hybridized living optics, where biological components (e.g., cells, organs) are utilized to produce dynamic optical materials and structures.140 To achieve this, inspiration can be drawn from recent success in organic electronics, such as genetically targeted chemical assembly, in which organic semiconductors are synthesized in situ to form self-assembled structures directly at cellular interfaces.141
In addition, nearly all prior work has attempted to mimic only single (or very few) aspects of cephalopod skin under restricted operating conditions. An emerging direction is to design standalone soft machines that integrate multiple optical and mechanical modalities, such as color change, texture modulation, luminescence, and locomotion, to better emulate natural camouflage. While cephalopod-inspired multimodal camouflage has been shown in some exploratory devices, their pattern resolution is often limited with relatively low spatiotemporal fidelity, in comparison to the (at least) thousands of color-changing cells and/or organs found in living cephalopod skin. Moreover, the scalability of these man-made systems is still low due to the requirement of exotic materials and often complex manufacturing processes. Additional consideration should be given to enhancing device reliability and robustness under extreme or varying environments (e.g., temperature, humidity, background lighting), which remain largely underexplored. Furthermore, we note that the same principles underpinning cephalopods’ dynamic color-changing behavior can be further extended to engineer stimuli-responsive systems with spectral responsiveness beyond the already-demonstrated visible and IR regions, into other technologically valuable domains such as the ultraviolet and terahertz. This can be potentially achieved through the incorporation of novel materials and photonic structures (e.g., metasurfaces).
So far, very few works have demonstrated cephalopod-like distributed neural control mechanisms enabled by their highly sophisticated peripheral nervous systems (given that nearly two-thirds of cephalopod neurons are distributed across their skin). Indeed, open-loop control with limited feedback has been implemented in most reported cephalopod-inspired optical systems. Moving forward, improved real-time environmental awareness can be achieved by constructing closed-loop control systems through the integration of multimodal, distributed sensory networks capable of detecting various signals (e.g., light, temperature, force, chemicals). Meanwhile, it is important to maintain low power consumption in these artificial systems, given that cephalopods perform all their visual stunts with remarkably low energy expenditure. When coupled with cephalopod-like distributed sensing, power management, edge computing, and artificial intelligence for data processing and decision-making, autonomous system operation can be realized in unstructured environments with significantly improved adaptability.
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