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P. Vukusic, J. R. Sambles, C. R. Lawrence, and R. J. Wootton, " Quantified interference and diffraction in single Morpho butterfly scales.," Proc. R. Soc. London, Ser. B 0962-8452 266, 1403-1411 (1999). 10.1098/rspb.1999.0794 (Pubitemid 29366479)
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Optical classification of microstructure in butterfly wing-scales
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Photophysics of structural color in the Morpho butterflies
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Wavelength-selective and anisotropic light-diffusing scale on the wing of the Morpho butterfly
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S. Yoshioka and S. Kinoshita, " Wavelength-selective and anisotropic light-diffusing scale on the wing of the Morpho butterfly.," Proc. R. Soc. London, Ser. B 0962-8452 271, 581-587 (2004). 10.1098/rspb.2003.2618 (Pubitemid 38365846)
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17
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70350019362
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2 =-1.
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2 =-1.
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19
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0004158491
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Pigmentary color is caused by the absorption of certain wavelengths in the visible spectrum. Absorption occurs because a photon of the incident light has the right energy to excite an electron from a lower state to a higher state in a region of a molecule known as a "chromophore." A bleaching agent, such as hydrogen peroxide (a strong oxidizer), alters the chromophore and either destroys the mechanism for absorption or moves it to wavelengths outside the visible spectrum., 2nd ed. (Wiley-Interscience, New York); Also see 〈〉 and 〈 en.wikipedia.org/wiki/Bleach 〉.
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Pigmentary color is caused by the absorption of certain wavelengths in the visible spectrum. Absorption occurs because a photon of the incident light has the right energy to excite an electron from a lower state to a higher state in a region of a molecule known as a "chromophore." A bleaching agent, such as hydrogen peroxide (a strong oxidizer), alters the chromophore and either destroys the mechanism for absorption or moves it to wavelengths outside the visible spectrum. K. Nassau, The Physics and Chemistry of Color: The Fifteen Causes of Color, 2nd ed. (Wiley-Interscience, New York, 2001); Also see 〈 en.wikipedia.org/wiki/Chromophore 〉 and 〈 en.wikipedia.org/wiki/Bleach 〉.
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Nassau, K.1
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20
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Plattner, L.1
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21
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70350037100
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Some of the authors provided results for incident light with two orthogonal states of linear polarization (TE and TM). In such cases, these states have been combined to obtain results for unpolarized light.
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Some of the authors provided results for incident light with two orthogonal states of linear polarization (TE and TM). In such cases, these states have been combined to obtain results for unpolarized light.
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22
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0000812231
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Structural colors in insects. II
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0022-3654,. 10.1021/j150273a001
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C. W. Mason, " Structural colors in insects. II.," J. Phys. Chem. 0022-3654 31, 321-354 (1927). 10.1021/j150273a001
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Mason, C.W.1
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23
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0037829580
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Morpho butterflies wings color modeled with lamellar grating theory
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1094-4087.
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B. Gralak, G. Tayeb, and S. Enoch, " Morpho butterflies wings color modeled with lamellar grating theory.," Opt. Express 1094-4087 9, 567-578 (2001).
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Gralak, B.1
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24
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68149158246
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A detailed electromagnetic simulation for the structural color of butterfly wings
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0003-6935.
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R. T. Lee and G. S. Smith, " A detailed electromagnetic simulation for the structural color of butterfly wings.," Appl. Opt. 0003-6935 48, 4177-4190 (2009).
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25
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41049107581
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Mechanisms of structural colour in the Morpho butterfly: Cooperation of regularity and irregularity in an iridescent scale
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DOI 10.1098/rspb.2002.2019
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S. Kinoshita, S. Yoshioka, and K. Kawagoe, " Mechanisms of structural colour in the Morpho butterfly: Cooperation of regularity and irregularity in an iridescent scale.," Proc. R. Soc. London, Ser. B 0962-8452 269, 1417-1421 (2002). 10.1098/rspb.2002.2019 (Pubitemid 34810655)
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Kinoshita, S.1
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Kawagoe, K.3
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26
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70350003144
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Notice, in the model (shown in dark gray), a small section of the lowest lamella has been included that is outside the unit cell to make all of the sections of lamellae in the model the same size, which greatly simplifies the calculations.
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Notice, in the model (shown in dark gray), a small section of the lowest lamella has been included that is outside the unit cell to make all of the sections of lamellae in the model the same size, which greatly simplifies the calculations.
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27
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70350024592
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The notation TE (TM) indicates that the electric (magnetic) field of the incident plane wave is transverse to the plane of symmetry of the ridge (x-y plane), which is also the plane of incidence: the plane containing the vector wave number for the incident wave and the normal to the surface of the lamellae. Sometimes, the TE case is indicated by E, ⊥, s, or σ (electric field perpendicular to the plane of incidence) and the TM case by H, , p, or π (electric field parallel to the plane of incidence).
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The notation TE (TM) indicates that the electric (magnetic) field of the incident plane wave is transverse to the plane of symmetry of the ridge (x-y plane), which is also the plane of incidence: the plane containing the vector wave number for the incident wave and the normal to the surface of the lamellae. Sometimes, the TE case is indicated by E, ⊥, s, or σ (electric field perpendicular to the plane of incidence) and the TM case by H, p, or π (electric field parallel to the plane of incidence).
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28
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70350038926
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ωt].
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ωt].
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29
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70350017380
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This relation for the equivalent current may be more familiar in the time domain: J b = P /t.
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This relation for the equivalent current may be more familiar in the time domain: J b = P /t.
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31
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70350038928
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The superscript sr is used to indicate that this is the "scattered radiated" field: The part of the scattered field that behaves as 1/r, where r is the radial distance from the ridge.
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The superscript sr is used to indicate that this is the "scattered radiated" field: The part of the scattered field that behaves as 1/r, where r is the radial distance from the ridge.
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32
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70350017378
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This topic is covered in many introductory textbooks on electromagnetism and optics, for example, (Cambridge U. P., Cambridge), p;, 4th ed. (Addison-Wesley, San Francisco, CA, 2002), 111-122. Here the convention used is one in which the TE (TM) reflection and transmission coefficients apply to the w component of the electric field (magnetic field), and the angles are measured with respect to the normal to the interface.
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This topic is covered in many introductory textbooks on electromagnetism and optics, for example, P. C. Clemmow, An Introduction to Electromagnetic Theory (Cambridge U. P., Cambridge, 1973), pp. 201-203; E. Hecht, Optics, 4th ed. (Addison-Wesley, San Francisco, CA, 2002), pp. 111-122. Here the convention used is one in which the TE (TM) reflection and transmission coefficients apply to the w component of the electric field (magnetic field), and the angles are measured with respect to the normal to the interface.
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(1973)
An Introduction to Electromagnetic Theory, Optics
, pp. 201-203
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Clemmow, P.C.1
Hecht, E.2
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33
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70350027722
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Because of the many approximations made in estimating the electric field within the lamellae, the analysis is accurate only for obtaining the relative amount of scattering for different wavelengths. Therefore, all plots are presented in the normalized form.
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Because of the many approximations made in estimating the electric field within the lamellae, the analysis is accurate only for obtaining the relative amount of scattering for different wavelengths. Therefore, all plots are presented in the normalized form.
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34
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70350006242
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A factor of 1/N has been added before the sum; this factor does not affect the proportionality.
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A factor of 1/N has been added before the sum; this factor does not affect the proportionality.
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35
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70350011288
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For visible wavelengths (400 nmλ700 nm), we have 0.09h/λ0.16, and the value of the first sinc function is within the range of 0.73-0.90.
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For visible wavelengths (400 nmλ700 nm), we have 0.09h/λ0.16, and the value of the first sinc function is within the range of 0.73-0.90.
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36
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70350039593
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n cos φ/cos γ.
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n cos φ/cos γ.
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37
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70350019755
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Reference
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Reference, pp. 493-506.
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38
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70350035054
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0, Eq. becomes comparable to the results for the two-dimensional structure described in Ref..
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0, Eq. becomes comparable to the results for the two-dimensional structure described in Ref..
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39
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70350039596
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The small gaps in the curves for A 2 at angles near φ=0° occur because there are no real solutions to the equations in this region.
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The small gaps in the curves for A 2 at angles near φ=0° occur because there are no real solutions to the equations in this region.
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40
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17444392888
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Brilliant blue observation from a Morpho-butterfly-scale quasi-structure
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DOI 10.1143/JJAP.44.L48
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, vol.44
, Issue.1-7
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Watanabe, K.1
Hoshino, T.2
Kanda, K.3
Haruyama, Y.4
Matsui, S.5
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41
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42449124648
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Optimization of reproduced Morpho-blue coloration
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DOI 10.1117/12.733954, Photonic Crystals and Photonic Crystal Fibers for Sensing Applications III
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A. Saito, Y. Ishikawa, Y. Miyamura, M. Akai-Kasaya, and Y. Kuwahara, " Optimization of reproduced Morpho-blue coloration.," Proc. SPIE 0277-786X 6767, 676706-1-8 (2007). 10.1117/12.733954 (Pubitemid 351563203)
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Saito, A.1
Ishikawa, Y.2
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Kuwahara, Y.5
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