Editing Moiré pattern

{{short description|Interference pattern}}
{{redirect2|Moiré|Moire||Moire (disambiguation)}}
{{multiple image
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| image1 = Moiré pattern.svg
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| caption1 = A moiré pattern formed by two units of parallel lines, one unit rotated 5° clockwise relative to the other
| image2 = Divers - Illustrated London News Feb 6 1873-2.PNG
| alt2 = 
| caption2 = The fine lines that make up the sky in this image create moiré patterns when shown at some resolutions for the same reason that photographs of televisions exhibit moiré patterns: the lines are not absolutely level.
| footer = 
}}
[[File:Moire-bridge-picket-fence.jpg|thumb|Difference in distance of the front and rear picket fence on a bridge create moiré patterns.]]
[[File:Moiré pattern.png|thumb|Moiré pattern appearing on scaled camera captures of LCD screen]]
[[File:ShadingNetMoiree.webm|thumb|Moiré pattern of double layered shading net]]

In mathematics, physics, and art, '''moiré patterns''' ({{IPAc-en|UK|'|m|w|ɑː|r|eɪ}} {{respell|MWAH|ray}}, {{IPAc-en|US|m|w|ɑː|ˈ|r|eɪ}} {{respell|mwah|RAY}},<ref>{{cite encyclopedia |last=Wells|first=John |author-link=John C. Wells |title=Longman Pronunciation Dictionary |publisher=Pearson [[Longman]] |edition=3rd |date=3 April 2008 |isbn=978-1-4058-8118-0}}</ref> {{IPA|fr|mwaʁe|lang|LL-Q150 (fra)-Lyokoï-moiré.wav}}) or '''moiré fringes'''<ref name="SIMicroscopy">{{cite journal | last=Gustafsson|first=M. G. L. |title=Surpassing the lateral resolution limit by a factor of two using structured illumination microscopy |journal=[[Journal of Microscopy]] |doi=10.1046/j.1365-2818.2000.00710.x |pmid=10810003 |volume=198 |issue=2 |year=2000 |pages=82–87 |s2cid=9257781 |doi-access=free}}</ref> are large-scale [[wave interference|interference patterns]] that can be produced when a partially opaque [[grating|ruled pattern]] with transparent gaps is overlaid on another similar pattern. For the moiré interference pattern to appear, the two patterns must not be completely identical, but rather displaced, rotated, or have slightly different pitch.

Moiré patterns appear in many situations. In printing, the printed pattern of dots can interfere with the image. In television and digital photography, a pattern on an object being photographed can interfere with the shape of the light sensors to generate unwanted artifacts. They are also sometimes created deliberately; in [[micrometer (device)|micrometers]], they are used to amplify the effects of very small movements.

In physics, its manifestation is [[wave interference]] like that seen in the [[double-slit experiment]] and the [[Beat (acoustics)|beat phenomenon]] in [[acoustics]].

== Etymology ==
The term originates from ''[[Moire (fabric)|moire]]'' (''moiré'' in its French adjectival form), a type of [[textile]], traditionally made of [[silk]] but now also made of [[cotton]] or [[synthetic fiber]], with a rippled or "watered" appearance. Moire, or "watered textile", is made by pressing two layers of the textile when wet. The similar but imperfect spacing of the threads creates a characteristic pattern which remains after the fabric dries.

In French, the noun ''moire'' is in use from the 17th century, for "watered silk". It was a loan of the English ''[[mohair]]'' (attested 1610). In French usage, the noun gave rise to the verb  ''moirer'', "to produce a watered textile by weaving or pressing", by the 18th century. The adjective ''moiré'' formed from this verb is in use from at least 1823.

== Pattern formation ==
[[File:070309-moire-a5-a5-upward-movement.gif|thumb|Line moiré with slow movement of the revealing layer upward]]
[[File:070320-a6-shape-moire-pr-gt-pb.gif|thumb|Shape moiré]]
[[File:Moire.gif|thumb|Moiré pattern created by overlapping two sets of concentric circles]]

Moiré patterns are often an [[Artifact (observational)|artifact]] of [[Digital image|images]] produced by various [[digital imaging]] and [[computer graphics]] techniques, for example when [[Image scanner|scanning]] a [[halftone]] picture or [[Ray tracing (graphics)|ray tracing]] a checkered plane (the latter being a special case of [[aliasing]], due to [[undersampling]] a fine regular pattern).<ref>{{cite web|title=Scanning Images in Books/Magazines/Newspapers (Moire patterns)|url=http://www.scantips.com/basics06.html|website=www.scantips.com|access-date=2020-02-27}}</ref>  This can be overcome in texture mapping through the use of [[mipmapping]] and [[anisotropic filtering]].

The drawing on the upper right shows a moiré pattern.  The lines could represent fibers in moiré silk, or lines drawn on paper or on a computer screen. The [[Nonlinear optics|nonlinear]] interaction of the optical patterns of lines creates a real and visible pattern of roughly parallel dark and light bands, the moiré pattern, superimposed on the lines.<ref>{{cite book
| title = Energy Minimization Methods in Computer Vision and Pattern Recognition
| editor1-first = Anil K.
| editor1-last = Jain
| first1 = Mário 
| last1 = Figueiredo
| first2 = Josiane
| last2 = Zerubia
| publisher = Springer
| year = 2001
| url = https://books.google.com/books?id=yb8otde21fcC&q=%22moire+pattern%22+nonlinear&pg=RA1-PA198| isbn = 9783540425236
}}</ref>

The moiré effect also occurs between overlapping transparent objects.<ref>{{Cite journal|last1=Miao|first1=Houxun|last2=Panna|first2=Alireza|last3=Gomella|first3=Andrew A.|last4=Bennett|first4=Eric E.|last5=Znati|first5=Sami|last6=Chen|first6=Lei|last7=Wen|first7=Han|title=A universal moiré effect and application in X-ray phase-contrast imaging|journal=Nature Physics|volume=12|issue=9|pages=830–834|doi=10.1038/nphys3734|year=2016|bibcode=2016NatPh..12..830M|pmc=5063246|pmid=27746823}}</ref> For example, an invisible phase mask is made of a transparent polymer with a wavy thickness profile. As light shines through two overlaid masks of similar phase patterns, a broad moiré pattern occurs on a screen some distance away. This phase moiré effect and the classical moiré effect from opaque lines are two ends of a continuous spectrum in optics, which is called the universal moiré effect. The phase moiré effect is the basis for a type of broadband interferometer in x-ray and particle wave applications. It also provides a way to reveal hidden patterns in invisible layers.

===Line moiré===
{{main|Line moiré}}

Line moiré is one type of moiré pattern; a pattern that appears when superposing two transparent layers containing correlated opaque patterns. Line moiré is the case when the superposed patterns comprise straight or curved lines. When moving the layer patterns, the moiré patterns transform or move at a faster speed. This effect is called optical moiré speedup.

More complex [[line moiré]] patterns are created if the lines are curved or not exactly parallel.

===Shape moiré===
{{main|Shape moiré}}

Shape moiré is one type of moiré pattern demonstrating the phenomenon of moiré magnification.<ref>{{cite conference
| title = Optical Inspection of Arrays and Periodic Structures Using Moire Magnification
| first1 = M.C. | last1 = Hutley
| first2 = R.F. | last2 = Stevens
| conference = IEE Colloquium, Microengineering in Optics and Optoelectronics
| date = 1999-11-16
| url = http://scitation.aip.org/getabs/servlet/GetabsServlet?prog=normal&id=IEESEM001999000187000008000001&idtype=cvips&gifs=yes
}}</ref><ref>{{cite journal
 |title      = Properties of Moiré Magnifiers
 |first1     = Hala
 |last1      = Kamal
 |first2     = Reinhard
 |last2      = Völkel
 |first3     = Javier
 |last3      = Alda
 |journal    = Optical Engineering
 |volume     = 37
 |issue      = 11
 |pages      = 3007–3014
 |date       = November 1998
 |url        = https://www.suss-microoptics.com/suss-microoptics/technical-publications/Moire_Magnifiers.pdf
 |archive-url = https://web.archive.org/web/20201108012304/https://www.suss-microoptics.com/suss-microoptics/technical-publications/Moire_Magnifiers.pdf
 |url-status = usurped
 |archive-date = November 8, 2020
 |access-date = 2021-03-30
 |doi        = 10.1117/1.601889
 |bibcode    = 1998OptEn..37.3007K
}}</ref> 1D shape moiré is the particular simplified case of 2D shape moiré. [[Dimension|One-dimensional]] patterns may appear when superimposing an [[Opacity (optics)|opaque]] layer containing tiny horizontal [[Transparency and translucency|transparent]] lines on top of a layer containing a complex shape which is periodically repeating along the [[Cartesian coordinate system|vertical axis]].

Moiré patterns revealing complex shapes, or sequences of symbols embedded in one of the layers (in form of periodically repeated compressed shapes) are created with shape moiré, otherwise called ''band moiré'' patterns. One of the most important properties of shape moiré is its ability to magnify tiny shapes along either one or both axes, that is, stretching. A common 2D example of moiré magnification occurs when viewing a [[chain-link fence]] through a second chain-link fence of identical design.  The fine structure of the design is visible even at great distances.

== Calculations ==
{{unreferenced section|date=April 2018}}

=== Moiré of parallel patterns ===

==== Geometrical approach ====
{{multiple image
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| image1 = Moire parallel.svg
| alt1 = 
| caption1 = The patterns are superimposed in the mid-width of the figure.
| image2 = Moire ecart angulaire.png
| alt2 = 
| caption2 = Moiré obtained by the superimposition of two similar patterns rotated by an angle {{mvar|α}}
| footer = 
}}

Consider two patterns made of parallel and equidistant lines, e.g., vertical lines. The step of the first pattern is {{mvar|p}}, the step of the second is {{math|''p'' + ''δp''}}, with {{math|0 < ''δp'' < ''p''}}.

If the lines of the patterns are superimposed at the left of the figure, the shift between the lines increases when going to the right. After a given number of lines, the patterns are opposed: the lines of the second pattern are between the lines of the first pattern. If we look from a far distance, we have the feeling of pale zones when the lines are superimposed (there is white between the lines), and of dark zones when the lines are "opposed".

The middle of the first dark zone is when the shift is equal to {{math|{{sfrac|''p''|2}}}}. The {{mvar|n}}th line of the second pattern is shifted by {{math|''n δp''}} compared to the {{mvar|n}}th line of the first network. The middle of the first dark zone thus corresponds to
<math display="block">n \cdot \delta p = \frac{p}{2}</math>
that is
<math display="block">n = \frac{p}{2 \delta p}.</math>
The distance {{mvar|d}} between the middle of a pale zone and a dark zone is
<math display="block">d = n \cdot (p+\delta p) = \frac{p^2}{2 \delta p}+\frac{p}{2}</math>
the distance between the middle of two dark zones, which is also the distance between two pale zones, is
<math display="block">2d = \frac{p^2}{\delta p}+p</math>
From this formula, we can see that:
* the bigger the step, the bigger the distance between the pale and dark zones;
* the bigger the discrepancy {{mvar|δp}}, the closer the dark and pale zones; a great spacing between dark and pale zones mean that the patterns have very close steps.

The principle of the moiré is similar to the [[Vernier scale]].

==== Mathematical function approach ====
[[File:Moiré grid.svg|thumb|upright|Moiré pattern (bottom) created by superimposing two grids (top and middle)]]

The essence of the moiré effect is the (mainly visual) perception of a distinctly different third pattern which is caused by inexact superimposition of two similar patterns. The mathematical representation of these patterns is not trivially obtained and can seem somewhat arbitrary. In this section we shall give a mathematical example of two parallel patterns whose superimposition forms a moiré pattern, and show one way (of many possible ways) these patterns and the moiré effect can be rendered mathematically.

The visibility of these patterns is dependent on the medium or substrate in which they appear, and these may be opaque (as for example on paper) or transparent (as for example in plastic film). For purposes of discussion we shall assume the two primary patterns are each printed in greyscale ink on a white sheet, where the opacity (e.g., shade of grey) of the "printed" part is given by a value between 0 (white) and 1 (black) inclusive, with {{sfrac|1|2}} representing neutral grey. Any value less than 0 or greater than 1 using this grey scale is essentially "unprintable".

We shall also choose to represent the opacity of the pattern resulting from printing one pattern atop the other at a given point on the paper as the average (i.e. the arithmetic mean) of each pattern's opacity at that position, which is half their sum, and, as calculated, does not exceed 1. (This choice is not unique. Any other method to combine the functions that satisfies keeping the resultant function value within the bounds [0,1] will also serve; arithmetic averaging has the virtue of simplicity—with hopefully minimal damage to one's concepts of the printmaking process.)

We now consider the "printing" superimposition of two almost similar, sinusoidally varying, grey-scale patterns to show how they produce a moiré effect in first printing one pattern on the paper, and then printing the other pattern over the first, keeping their coordinate axes in register. We represent the grey intensity in each pattern by a positive opacity function of distance along a fixed direction (say, the x-coordinate) in the paper plane, in the form

<math display="block">f = \frac{1 + \sin(k x)}{2}</math>

where the presence of 1 keeps the function positive definite, and the division by 2 prevents function values greater than 1.

The quantity {{mvar|k}} represents the periodic variation (i.e., spatial frequency) of the pattern's grey intensity, measured as the number of intensity cycles per unit distance. Since the sine function is cyclic over argument changes of {{math|2π}}, the distance increment {{math|Δ''x''}} per intensity cycle (the wavelength) obtains when {{math|''k'' Δ''x'' {{=}} 2π}}, or {{math|Δ''x'' {{=}} {{sfrac|2π|''k''}}}}.

Consider now two such patterns, where one has a slightly different periodic variation from the other:

<math display="block">\begin{align}
 f_1 &= \frac{1 + \sin(k_1 x)}{2} \\[4pt]
 f_2 &= \frac{1 + \sin(k_2 x)}{2}
\end{align}</math>

such that {{math|''k''<sub>1</sub> ≈ ''k''<sub>2</sub>}}.

The average of these two functions, representing the superimposed printed image, evaluates as follows (see reverse identities here :[[Prosthaphaeresis]] ):

<math display="block">\begin{align} f_3 &= \frac{f_1 + f_2}{2} \\[5pt] &= \frac12 + \frac{\sin(k_1 x) + \sin(k_2 x)}{4} \\[5pt] &= \frac{1 + \sin(A x) \cos(B x)}{2} \end{align}</math>

where it is easily shown that

<math display="block">A = \frac{k_1 + k_2}{2}</math>

and

<math display="block">B = \frac{k_1 - k_2}{2}.</math>

This function average, {{math|''f''<sub>3</sub>}}, clearly lies in the range [0,1]. Since the periodic variation {{mvar|A}} is the average of and therefore close to {{math|''k''<sub>1</sub>}} and {{math|''k''<sub>2</sub>}}, the moiré effect is distinctively demonstrated by the sinusoidal envelope "beat" function {{math|cos(''Bx'')}}, whose periodic variation is half the difference of the periodic variations {{math|''k''<sub>1</sub>}} and {{math|''k''<sub>2</sub>}} (and evidently much lower in frequency).

Other one-dimensional moiré effects include the classic [[beat (acoustics)|beat]] frequency tone which is heard when two pure notes of almost identical pitch are sounded simultaneously. This is an acoustic version of the moiré effect in the one dimension of time: the original two notes are still present—but the listener's ''perception'' is of two pitches that are the average of and half the difference of the frequencies of the two notes. Aliasing in sampling of time-varying signals also belongs to this moiré paradigm.

=== Rotated patterns ===
Consider two patterns with the same step {{mvar|p}}, but the second pattern is rotated by an angle {{mvar|α}}. Seen from afar, we can also see darker and paler lines: the pale lines correspond to the lines of [[Node (physics)|nodes]], that is, lines passing through the intersections of the two patterns.

If we consider a cell of the lattice formed, we can see that it is a [[rhombus]] with the four sides equal to {{math|''d'' {{=}} {{sfrac|''p''|sin ''α''}}}}; (we have a right [[triangle]] whose hypotenuse is {{mvar|d}} and the side opposite to the angle {{mvar|α}} is {{mvar|p}}).

{{multiple image
| direction = vertical
| total_width = 160
| align = right
| image1 = Moire calcul angle.png
| alt1 = 
| caption1 = Unit cell of the "net"; "''ligne claire''" means "pale line".
| image2 = Moire02.gif
| alt2 = 
| caption2 = Effect of changing angle
| footer = 
}}

The pale lines correspond to the small [[diagonal]] of the rhombus. As the diagonals are the [[Bisection|bisectors]] of the neighbouring sides, we can see that the pale line makes an angle equal to {{math|{{sfrac|''α''|2}}}} with the perpendicular of each pattern's line.

Additionally, the spacing between two pale lines is {{mvar|D}}, half of the long diagonal. The long diagonal {{math|2''D''}} is the hypotenuse of a right triangle and the sides of the right angle are {{math|''d''(1 + cos ''α'')}} and {{mvar|p}}. The [[Pythagorean theorem]] gives:
<math display="block">(2 D)^2 = d^2 (1 + \cos \alpha)^2 + p^2</math>
that is:
<math display="block">\begin{align} (2D)^2 &= \frac{p^2}{\sin^2 \alpha}(1+ \cos \alpha)^2 + p^2 \\[5pt]
&= p^2 \cdot \left ( \frac{(1 + \cos \alpha)^2}{\sin^2 \alpha} + 1\right) \end{align}</math>
thus
<math display="block">\begin{align} (2D)^2 &= 2 p^2 \cdot \frac{1+\cos \alpha}{\sin^2 \alpha} \\[5pt] D &= \frac{\frac{p}{2}}{\sin\frac{\alpha}{2}}. \end{align}</math>

{{multiple image
| total_width = 320
| align = right
| image1 = Moire Circles.svg
| alt1 = 
| caption1 = 
| image2 = Moire Lines.svg
| alt2 = 
| caption2 = 
| image3 = Moire Lines and Circles.svg
| alt3 = 
| caption3 = 
| footer = Effect on curved lines
}}

When {{mvar|α}} is very small ({{math|''α'' < {{sfrac|π|6}}}}) the following [[small-angle approximation]]s can be made:
<math display="block">\begin{align} \sin \alpha &\approx \alpha \\ \cos \alpha &\approx 1 \end{align}</math>
thus
<math display="block">D \approx \frac{p}{\alpha}.</math>

We can see that the smaller {{mvar|α}} is, the farther apart the pale lines; when both patterns are parallel ({{math|''α'' {{=}} 0}}), the spacing between the pale lines is infinite (there is no pale line).

There are thus two ways to determine {{mvar|α}}: by the orientation of the pale lines and by their spacing
<math display="block">\alpha \approx \frac{p}{D}</math>
If we choose to measure the angle, the final error is proportional to the measurement error. If we choose to measure the spacing, the final error is proportional to the inverse of the spacing. Thus, for the small angles, it is best to measure the spacing.

== Implications and applications ==

=== Printing full-color images ===
[[File:BeatTrackMoirePattern.ogg|thumb|upright=1.5|
'''Warning: audiogenic [[epileptic seizure]] hazard.''' The product of two "beat tracks" of slightly different speeds overlaid, producing an audible moiré pattern; if the beats of one track correspond to where in space a black dot or line exists and the beats of the other track correspond to the points in space where a camera is sampling light, because the frequencies are not exactly the same and aligned perfectly together, beats (or samples) will align closely at some moments in time and far apart at other times. The closer together beats are, the darker it is at that spot; the farther apart, the lighter. The result is periodic in the same way as a graphic moiré pattern. See: [[phasing (music)|phasing]].]]
In [[graphic arts]] and [[prepress]], the usual technology for printing full-color images involves the superimposition of [[halftone]] screens. These are regular rectangular dot patterns—often four of them, printed in cyan, yellow, magenta, and black. Some kind of moiré pattern is inevitable, but in favorable circumstances the pattern is "tight"; that is, the spatial frequency of the moiré is so high that it is not noticeable. In the graphic arts, the term ''moiré'' means an ''excessively visible'' moiré pattern. Part of the prepress art consists of selecting screen angles and halftone frequencies which minimize moiré. The visibility of moiré is not entirely predictable. The same set of screens may produce good results with some images, but visible moiré with others.

=== Television screens and photographs ===
{{multiple image
| total_width = 320
| align = right
| image1 = Moire on parrot feathers.jpg
| alt1 = 
| caption1 = Strong moiré visible in this photo of a parrot's feathers (more pronounced in the full-size image)
| image2 = Moiré fringes IMG 3712.jpg
| alt2 = 
| caption2 = Moiré pattern seen over a cage in the San Francisco Zoo
| footer = 
}}
Moiré patterns are commonly seen on television screens when a person is wearing a shirt or jacket of a particular weave or pattern, such as a [[houndstooth]] jacket. This is due to interlaced scanning in televisions and non-film cameras, referred to as [[interline twitter]]. As the person moves about, the moiré pattern is quite noticeable. Because of this, newscasters and other professionals who regularly appear on TV are instructed to avoid clothing which could cause the effect.

Photographs of a [[television|TV]] screen taken with a [[digital camera]] often exhibit moiré patterns. Since both the TV screen and the digital camera use a scanning technique to produce or to capture pictures with horizontal scan lines, the conflicting sets of lines cause the moiré patterns. To avoid the effect, the digital camera can be aimed at an angle of 30 degrees to the TV screen.

=== {{Anchor|Inogon light|Inogon leading mark}} Marine navigation ===
The moiré effect is used in shoreside beacons called "Inogon leading marks" or "Inogon lights", manufactured by Inogon Licens AB, Sweden, to designate the safest path of travel for ships heading to locks, marinas, ports, etc., or to indicate underwater hazards (such as pipelines or cables). The moiré effect creates arrows that point towards an imaginary line marking the hazard or line of safe passage; as navigators pass over the line, the arrows on the beacon appear to become vertical bands before changing back to arrows pointing in the reverse direction.<ref>{{cite web|title=US Patent 4,629,325|url=https://patents.google.com/patent/US4629325|website=Google Patents|access-date=5 March 2018}}</ref><ref>{{cite web|author=Alexander Trabas |url=http://www.listoflights.org/leuchtfeuer/detail?id=487 |title=Prohibited anchorage |publisher=Light of Lights |access-date=9 December 2016}}</ref><ref>{{cite book |title=Hydrographic Dictionary |date=2003 |publisher=[[International Hydrographic Organization]] |location=Monaco |page=113 |edition=5 |chapter=inogen light {{sic}}}}</ref> An example can be found in the UK on the eastern shore of [[Southampton Water]], opposite [[Fawley Refinery|Fawley oil refinery]] ({{coord|50|51|21.63|N|1|19|44.77|W|type:landmark_region:GB|display=inline}}).<ref>{{Citation|first=Tom|last=Scott|author-link=Tom Scott (presenter)|title=The Moiré Effect Lights That Guide Ships Home|date=5 March 2018|url=https://www.youtube.com/watch?v=d99_h30swtM|access-date=5 March 2018}}</ref> Similar moiré effect beacons can be used to guide mariners to the centre point of an oncoming bridge; when the vessel is aligned with the centreline, vertical lines are visible.
Inogon lights are deployed at airports to help pilots on the ground keep to the centreline while docking on stand.<ref>{{cite book |last1=Kazda |first1=Antonín |last2=Caves |first2=Robert |title=Airport design and operation |date=2015 |publisher=Emerald |location=Bingley, England |isbn=9781784418700 |pages=204–205 |edition=3}}</ref>

=== Strain measurement ===
{{See also|Theory of elasticity|Strain tensor|Holographic interferometry}}
[[File:Moire extensometrie.png|thumb|Use of the moiré effect in strain measurement: case of uniaxial traction (top) and of pure shear (bottom); the lines of the patterns are initially horizontal in both cases]]

In [[manufacturing]] industries, these patterns are used for studying microscopic [[Strain (materials science)|strain]] in materials: by deforming a grid with respect to a reference grid and measuring the moiré pattern, the stress levels and patterns can be deduced. This technique is attractive because the scale of the moiré pattern is much larger than the deflection that causes it, making measurement easier.

The moiré effect can be used in [[Strain (materials science)|strain]] measurement: the operator just has to draw a pattern on the object, and superimpose the reference pattern to the [[Deformation (engineering)|deformed]] pattern on the deformed object.

A similar effect can be obtained by the superposition of a [[Hologram|holographic]] image of the object to the object itself: the hologram is the reference step, and the difference with the object are the deformations, which appear as pale and dark lines.

=== Image processing ===
Some [[image scanner]] [[computer program]]s provide an optional [[Filter (software)|filter]], called a "descreen" filter, to remove moiré pattern artifacts which would otherwise be produced when scanning printed [[halftone]] images to produce digital images.<ref>{{cite web|url=http://www.scantips.com/basics6c.html|title=Scanning Images in Magazines/Books/Newspapers|website=ScanTips.com|access-date=22 April 2010}}</ref>

=== Banknotes ===
Many [[banknote]]s exploit the tendency of digital scanners to produce moiré patterns by including fine circular or wavy designs that are likely to exhibit a moiré pattern when scanned and printed.<ref>{{cite book |editor1-last=Sincerbox |editor1-first=Glenn T. |title=Counterfeit deterrent features for the next-generation currency design |date=1991 |publisher=National Materials Advisory Board |location=Washington DC |isbn=9780309050289 |page=61}}</ref>

=== Microscopy ===
In [[super-resolution microscopy]], the moiré pattern can be used to obtain images with a resolution higher than the [[diffraction limit]], using a technique known as [[super resolution microscopy#Structured illumination microscopy (SIM)|structured illumination microscopy]].<ref name="SIMicroscopy" />

In [[Scanning tunneling microscope|scanning tunneling microscopy]], moiré fringes appear if surface atomic layers have a different [[crystal structure]] than the bulk crystal. This can for example be due to [[surface reconstruction]] of the crystal, or when a thin layer of a second crystal is on the surface, e.g. single-layer,<ref name=":2">{{Cite journal|last=Kobayashi|first=Katsuyoshi|date=1996-01-01|title=Moiré pattern in scanning tunneling microscopy: Mechanism in observation of subsurface nanostructures|journal=Physical Review B|volume=53|issue=16|pages=11091–11099|doi=10.1103/PhysRevB.53.11091|pmid=9982681|bibcode=1996PhRvB..5311091K}}</ref><ref name=":3">{{Cite journal|last=N’Diaye|first=Alpha T.|date=2006-01-01|title=Two-Dimensional Ir Cluster Lattice on a Graphene Moiré on Ir(111)|journal=Physical Review Letters|volume=97|issue=21|pages=215501|doi=10.1103/PhysRevLett.97.215501|pmid=17155746|arxiv=cond-mat/0609286|bibcode=2006PhRvL..97u5501N|s2cid=19791195}}</ref> double-layer [[graphene]],<ref>{{Cite journal|last=K. Schouteden|first=N. Galvanetto|date=2015|title=Scanning probe microscopy study of chemical vapor deposition grown graphene transferred to Au(111)|journal=Carbon|volume=95|pages=318–322|doi=10.1016/j.carbon.2015.08.033}}</ref> or [[Van der Waals force|Van der Waals]] heterostructure of graphene and hBN,<ref>{{cite journal |last1=Tang |first1=Shujie |last2=Wang |first2=Haomin |last3=Zhang |first3=Yu |last4=Li |first4=Ang |last5=Xie |first5=Hong |last6=Liu |first6=Xiaoyu |last7=Liu |first7=Lianqing |last8=Li |first8=Tianxin |last9=Huang |first9=Fuqiang |last10=Xie |first10=Xiaoming |last11=Jiang |first11=Mianheng |title=Precisely aligned graphene grown on hexagonal boron nitride by catalyst free chemical vapor deposition |journal=Scientific Reports |date=16 September 2013 |volume=3 |issue=1 |pages=2666 |doi=10.1038/srep02666 |pmid=24036628 |pmc=3773621 |bibcode=2013NatSR...3E2666T |arxiv=1309.0172 }}</ref><ref name=":4">{{cite journal |title=Silane-catalysed fast growth of large single-crystalline graphene on hexagonal boron nitride |journal=Nature Communications  |volume=6  |year=2015|page=6499|doi=10.1038/ncomms7499 |pmid=25757864  |pmc=4382696  |last1=Tang |first1=Shujie |last2=Wang |first2=Haomin|last3=Wang |first3=Huishan |arxiv=1503.02806|bibcode=2015NatCo...6.6499T}}</ref> or [[bismuth]] and [[antimony]] nanostructures.<ref name=":5">{{cite journal |title=Moiré patterns in van der Waals heterostructures|journal=Physical Review B  |volume=99  |year=2019|issue=7|page=075422|doi=10.1103/PhysRevB.99.075422 |last1=Le Ster |first1=Maxime |last2=Maerkl |first2=Tobias|last3=Kowalczyk |first3=Pawel J.|last4=Brown|first4=Simon A.|hdl=10092/16978 |bibcode=2019PhRvB..99g5422L |s2cid=128326155 |hdl-access=free}}</ref>

In [[transmission electron microscopy]] (TEM), translational moiré fringes can be seen as parallel contrast lines formed in [[Phase-contrast imaging|phase-contrast TEM]] imaging by the interference of diffracting crystal lattice planes that are overlapping, and which might have different spacing and/or orientation.<ref name=":0">{{Cite book|title=Transmission electron microscopy : a textbook for materials science |url=https://archive.org/details/transmissionelec00dbwi |url-access=limited |last1=Williams|first1=David B.| last2=Carter|first2=C. Barry| date=2009-01-01| publisher= Springer|isbn=9780387765013| pages=[https://archive.org/details/transmissionelec00dbwi/page/n408 393]–397| oclc=876600051}}</ref> Most of the moiré contrast observations reported in the literature are obtained using high-resolution phase contrast imaging in TEM. However, if probe aberration-corrected [[Annular dark-field imaging|high-angle annular dark field]] [[scanning transmission electron microscopy]] (HAADF-STEM) imaging is used, more direct interpretation of the crystal structure in terms of atom types and positions is obtained.<ref name=":0" /><ref name=":1">{{Cite journal| last1=Heczko|first1=M.| last2=Esser|first2=B.D.| last3=Smith|first3=T.M.| last4=Beran| first4=P.| last5=Mazánová| first5=V.| last6=McComb| first6=D.W.| last7=Kruml| first7=T.| last8=Polák| first8=J.| last9=Mills| first9=M.J.| date=14 March 2018| title=Atomic resolution characterization of strengthening nanoparticles in a new high-temperature-capable 43Fe-25Ni-22.5Cr austenitic stainless steel|journal=Materials Science and Engineering: A| volume=719| pages=49–60| doi=10.1016/j.msea.2018.02.004| issn=0921-5093| doi-access=free}}</ref>

===Materials science and condensed matter physics===
{{multiple image
| total_width       = 440
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| image1            = Graphene moire on Ir(111) - schematic.svg
| alt1              = 
| caption1          = When graphene is grown on the (111) surface of iridium, its long-wavelength height modulation can be thought of as a moiré pattern arising from the superposition of the two mismatched hexagonal lattices.
| image2            = Moire of twisted bilayer graphene.svg
| alt2              = 
| caption2          = Moiré pattern arising from the superposition of two graphene lattices twisted by 4°
| footer            = 
| direction         = 
}}

In condensed matter physics, the moiré phenomenon is commonly discussed for [[two-dimensional materials]]. The effect occurs when there is mismatch between the lattice parameter or angle of the 2D layer and that of the underlying substrate,<ref name=":2" /><ref name=":3" /> or another 2D layer, such as in 2D material heterostructures.<ref name=":4" /><ref name=":5" /> The phenomenon is exploited as a means of engineering the electronic structure or optical properties of materials,<ref name="LiuWeiss2016">{{cite journal|last1=Liu|first1=Yuan|last2=Weiss|first2=Nathan O.|last3=Duan|first3=Xidong|last4=Cheng|first4=Hung-Chieh|last5=Huang|first5=Yu|last6=Duan|first6=Xiangfeng|title=Van der Waals heterostructures and devices|journal=Nature Reviews Materials|volume=1|issue=9|pages=16042|year=2016|issn=2058-8437|doi=10.1038/natrevmats.2016.42|bibcode=2016NatRM...116042L}}</ref> which some call moiré materials. The often significant changes in electronic properties when twisting two atomic layers and the prospect of electronic applications has led to the name [[twistronics]] of this field. A prominent example is in twisted bi-layer [[graphene]], which forms a moiré pattern and at a particular ''magic angle'' exhibits superconductivity and other important electronic properties.<ref>[https://physics.aps.org/articles/v12/12 APS Physics - Trend: Bilayer Graphene's Wicked, Twisted Road]</ref>

In [[materials science]], known examples exhibiting moiré contrast are [[thin film]]s<ref>{{cite journal|last1=Yin|first1=Xi|last2=Liu|first2=Xinhong|last3=Pan|first3=Yung-Tin|last4=Walsh|first4=Kathleen A.|last5=Yang|first5=Hong|date=10 December 2014|title=Hanoi Tower-like Multilayered Ultrathin Palladium Nanosheets|journal=Nano Letters|volume=14|issue=12|pages=7188–7194|bibcode=2014NanoL..14.7188Y|doi=10.1021/nl503879a|pmid=25369350}}</ref> or [[nanoparticle]]s of MX-type (M = Ti, Nb; X = C, N) overlapping with austenitic matrix. Both phases, MX and the matrix, have face-centered cubic crystal structure and cube-on-cube orientation relationship. However, they have significant lattice misfit of about 20 to 24% (based on the chemical composition of alloy), which produces a moiré effect.<ref name=":1" />{{Clear}}

== See also ==
* [[Aliasing]]
* [[Angle-sensitive pixel]]
* [[Barrier grid animation and stereography]] (kinegram)
* [[Beat (acoustics)]]
* [[Euclid's orchard]]
* [[Guardian (sculpture)|''Guardian'' (sculpture)]]
* [[Kell factor]]
* [[Lenticular printing]]
* [[Moiré Phase Tracking]]
* [[Multidimensional sampling]]

== Footnotes ==
{{Reflist}}

== External links ==
{{commons}}
* [https://web.archive.org/web/20150315155426/http://www.pip-dickens.com/moire.html A series of oil paintings based on moiré principles by British artist, Pip Dickens]
* [http://www.mathematik.com/Moire/ A live demonstration of the moiré effect that stems from interferences between circles]
* [http://www.kirl.nl/moireGen.swf An interactive example of various moiré patterns] {{Webarchive|url=https://web.archive.org/web/20110724154923/http://www.kirl.nl/moireGen.swf |date=2011-07-24 }} Use arrow keys and mouse to manipulate layers.
* [https://doi.org/10.1038/nphys3734 A universal moiré effect and application in X-ray phase-contrast imaging]
* [https://www.youtube.com/watch?v=d99_h30swtM "The Moiré Effect Lights That Guide Ships Home"], an article on [[YouTube]] by [[Tom Scott (entertainer)|Tom Scott]] about the Moiré Inogon light in Southampton
* [https://www.sqrt.ch/museum "The Moiré Museum"], interactive vector graphics with links to the physics and mathematics of the Moiré effect and artistic contributions

{{DEFAULTSORT:Moire pattern}}
[[Category:Geometry]]
[[Category:Interference]]
[[Category:Patterns]]
[[Category:Printing]]