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An '''MOS''' (can be pronounced "moss") or '''Moment Of Symmetry''' is a scale in which every interval except for the period comes in two sizes.
| ro = G2S
}}{{Beginner|Mathematics of MOS}}
A '''moment of symmetry''' ('''MOS''' or '''mos'''<ref group="note">The acronym "MOS" is generally pronounced ''em-oh-ess'', while the {{w|anacronym}} "mos", more common in informal and experimental settings, is generally pronounced ''moss''. Sometimes "MOSS" or "moss", standing for "moment of symmetry scale", are used instead, although there is no significant difference in meaning.</ref>) '''scale''' is a [[periodic scale]] where every 2nd (that is, every interval formed by ascending a step) is either small or large with no in-between, and the same goes for 3rds, 4ths, etc. Multiples of the period (which is usually the octave or a fraction thereof), however, come in only one size.


== History and terminology ==
MOS scales are often referred to as MOSes, thus MOS can be used as either an adjective or a noun.
The term ''MOS'', and the method of scale construction it entails, were invented by [[Erv Wilson]] in 1975. His original paper is archived on Anaphoria.com here: [http://anaphoria.com/mos.PDF Moments of Symmetry]. There is also an introduction by Kraig Grady here: [http://anaphoria.com/wilsonintroMOS.html Introduction to Erv Wilson's Moments of Symmetry].
 
Sometimes, scales are defined with respect to a period and an additional "equivalence interval," considered to be the interval at which pitch classes repeat. MOS's in which the equivalence interval is a multiple of the period, and in which there is more than one period per equivalence interval, are sometimes called '''Multi-MOS's'''. MOS's in which the equivalence interval is equal to the period are sometimes called '''Strict MOS's'''. MOS's in which the equivalence interval and period are simply disjunct, with no rational relationship between them, are simply MOS and have no additional distinguishing label.
 
With a few notable exceptions, Wilson generally focused his attention on MOS with period equal to the equivalence interval. Hence, some people prefer to use the term [[Distributional Evenness|distributionally even scale]], with acronym DE, for the more general class of scales which are MOS with respect to other intervals. MOS/DE scales are also sometimes known as ''well-formed scales'', the term used in the 1989 paper by Norman Carey and David Clampitt. A great deal of interesting work has been done on scales in academic circles extending these ideas. The idea of MOS also includes secondary or bi-level MOS scales which are actually the inspiration of Wilson's concept. They are in a sense the MOS of MOS patterns. This is used to explain the pentatonics used in traditional Japanese music, where the 5 tone cycles are derived from a 7 tone MOS, which are not found in the concept of DE.


As for using MOS scales in practice for making music, the period and equivalence interval are often taken to be the octave, but an additional parameter is required for defining a scale: the ''step ratio'', which is the ratio of the small step (usually denoted ''s'') to the large step (usually denoted ''L''). This is usually written as ''L''/''s'', however, using ''s''/''L'' has the advantage of avoiding division by zero in the trivial case where ''s'' = 0. Different step ratios can produce very varied sounding scales (and very varied corresponding potential temperament interpretations) for a given MOS pattern and period, so it's useful to consider a spectrum of simple step ratios for tunings. On this basis, a system has been proposed by a few users, detailed in a later section.
== Examples ==
The most widely used MOS scale is the [[5L 2s|diatonic scale]]. It has 7 steps: 5 large ones (major 2nds) and 2 small ones (minor 2nds), and thus is named 5L&nbsp;2s. The major mode is LLsLLLs. The other modes are rotations of this pattern (e.g. LsLLsLL is the minor mode).


== Patterns ==
The following is a standardized, nearly finalized set of temperament-agnostic names for octave-equivalent MOS scales of sizes between 6 and 10. Some of these come from temperament-agnostic MOS names coined by [[Igliashon Jones]] and others. Some are directly taken from temperament-based names for scales, often because the regular temperament is the only "good" or simple temperament in the range. 1L ns names are intentionally unspecific because the generator can be anywhere from the octave to to 1\(n+1)) and can better be viewed as subsets of larger MOSes, for example [[1L 6s]] as a subset of [[7L 1s]].
See [[MOS naming]] for another naming scheme. See the [[Catalog of MOS]] for a listing of MOS in the more usual Ls scheme. See also the [[pergen]]s page.
=== 6-note MOSes ===
* [[1L 5s]]: antimachinoid
* [[2L 4s]]: rice (range splits into echinoid[6] and antiechinoid[6])
* [[3L 3s]]: trisymmetric (range splits into Tcherepnin[6] and trifoiceish[6])
* [[4L 2s]]: bicycle (range splits into antilemboid[6] and lemboid[6])
* [[5L 1s]]: machinoid
=== 7-note MOSes ===
* [[1L 6s]]: antiarcheotonic
* [[2L 5s]]: antidiatonic (range splits into mavila[7] and joanatonic[7])
* [[3L 4s]]: mosh (range splits into dicoid[7] and sephiroid[7])
* [[4L 3s]]: smitonic
* [[5L 2s]]: diatonic
* [[6L 1s]]: archeotonic
=== 8-note MOSes ===
* [[1L 7s]]: antiporcupoid
* [[2L 6s]]: antiechinoid (range splits into pajaroid[8] and octodecoid[8])
* [[3L 5s]]: sensoid
* [[4L 4s]]: diminished, tetrasymmetric
* [[5L 3s]]: oneirotonic
* [[6L 2s]]: echinoid
* [[7L 1s]]: porcupoid
=== 9-note MOSes ===
* [[1L 8s]]: antibleuish
* [[2L 7s]]: joanatonic
* [[3L 6s]]: Tcherepnin
* [[4L 5s]]: orwelloid
* [[5L 4s]]: semiquartal
* [[6L 3s]]: triforceish
* [[7L 2s]]: mavila, superdiatonic
* [[8L 1s]]: bleuish
=== 10-note MOSes ===
* [[1L 9s]]: antisinatonic
* [[2L 8s]]: pajaroid
* [[3L 7s]]: sephiroid
* [[4L 6s]]: antilemboid
* [[5L 5s]]: blackwood, pentasymmetric
* [[6L 4s]]: lemboid
* [[7L 3s]]: dicoid
* [[8L 2s]]: octodecoid
* [[9L 1s]]: sinatonic
== Step ratio spectrum ==
=== Motivation and name system ===
The melodic sound of a MOS is not just affected by the tuning of its intervals, but by the sizes of its steps. MOSes with L more similar to s sound smoother and more mellow. MOSes with L much larger than s sound jagged and dramatic. The ''step ratio'', the ratio between the sizes of L and s, is thus important to the sound of the scale. We in the discord have named nine specific simple L:s ratios.
{| class="wikitable"
{| class="wikitable"
|+Step ratio names
|+ style="font-size: 105%;" | Interval classes in the 5L&nbsp;2s MOS scale
!Name
!Ratio
!Diatonic example
|-
|-
|Equalized
! rowspan="2" | Interval class
|L:s = 1:1
! colspan="2" | Small version
|7edo
! colspan="2" | Large version
|-
|-
|Supersoft
! Quality
|L:s = 4:3
! Size
|26edo
! Quality
! Size
|-
|-
|Soft
! 2nds (1 step)
|L:s = 3:2
| minor
|19edo
| s
| major
| L
|-
|-
|Semisoft
! 3rds (2 steps)
|L:s = 5:3
| minor
|31edo
| {{nowrap|1L + 1s}}
| major
| 2L
|-
|-
|Basic (or quintessential)
! 4ths (3 steps)
|L:s = 2:1
| perfect
|12edo
| {{nowrap|2L + 1s}}
| augmented
| 3L
|-
|-
|Semihard
! 5ths (4 steps)
|L:s = 5:2
| diminished
|29edo
| {{nowrap|2L + 2s}}
| perfect
| {{nowrap|3L + 1s}}
|-
|-
|Hard
! 6ths (5 steps)
|L:s = 3:1
| minor
|17edo
| {{nowrap|3L + 2s}}
| major
| {{nowrap|4L + 1s}}
|-
|-
|Superhard
! 7ths (6 steps)
|L:s = 4:1
| minor
|22edo
| {{nowrap|4L + 2s}}
| major
| {{nowrap|5L + 1s}}
|-
|-
|Paucitonic
! 8ves (7 steps)
|L:s = 1:0
| perfect
|5edo
| {{nowrap|5L + 2s}}
| colspan="2" | (only one version)
|}
|}
For example, the 5L2s (diatonic) scale of 19edo has a step ratio of 3:2, which is "soft". We call the 19edo diatonic scale "soft diatonic". Tunings of a MOS with L:s larger are "harder", and tunings with L:s smaller are "softer".


The two extremes, equalized and paucitonic, are degenerate cases. An equalized MOS has L equal to s, so the MOS pattern is no longer apparent. A paucitonic MOS has s = 0, merging adjacent tones s apart into a single tone. In both cases, the MOS structure is no longer valid.
Note that the melodic minor scale (LsLLLLs) has only two step sizes, but it is not MOS since it has three different sizes of fifths: perfect, diminished, and augmented.
 
Other MOS scales include [[2L&nbsp;3s]], where among its 5 modes are the major pentatonic scale (ssLsL) and the minor pentatonic scale (LssLs), and less commonly [[4L&nbsp;4s]], also known as the octatonic scale in 12edo, which alternates between large and small steps and comes in two modes (LsLsLsLs and sLsLsLsL).
 
See the [[catalog of MOS]] for other MOS scales.
 
== Periods and generators ==
Every MOS scale can be ''generated'' by stacking a certain interval called the [[generator]] and octave-reducing (or more generally, [[period]]-reducing). For example, the diatonic scale is generated by stacking 6 fifths (or equivalently, 6 fourths) and octave-reducing to get a 7 note scale. Another example, 2L&nbsp;3s is generated by stacking 4 fifths to get 5 notes. However, stacking 5 fifths to get a hexatonic scale such as {{nowrap| C D E F G A C }} does not produces a MOS, because there are more than 2 sizes of each interval class.
 
The amount of stacking that produces a MOS scale depends only on the size of the generator relative to the size to the period. For a just fifth and a just octave, the valid scale sizes are 2, 3, 5, 7, 12, 17, 29, 41, 53, …. However for a quarter-comma meantone fifth, the valid sizes are 2, 3, 5, 7, 12, 19, 31, 50, ….
 
== Step ratio spectrum ==
The [[step ratio]] is the ratio of the larger step size to the smaller step size. MOSes with smaller step ratios sound smooth and soft. MOSes with larger step ratios sound jagged and hard. Different step ratios produce different corresponding potential temperament interpretations. The [[TAMNAMS #Step ratio spectrum|TAMNAMS]] system has names for specific ratios and also ranges of ratios.


In between the nine specific ratios there are eight ranges of ratios. Each range has a name. These names are useful for classifying MOS tunings which don't match any of the nine simple step ratios. ''Hypohard'' could be used for tunings that are harder than basic but not as hard as the 3:1 tuning; similarly, ''hyposoft'' can be used for the range between soft and basic.
When the step ratio is a rational number, the MOS is tuned to an edo. A counter-example is 5L&nbsp;2s tuned to quarter-comma meantone, which has a step ratio of about 1.649.


By default, all ranges include their endpoints. For example, a hard tuning is considered a quasihard tuning. To exclude endpoints, the modifier "strict" can be used, for example "strict hyposoft".
{| class="wikitable"
{| class="wikitable"
|+Intermediate ranges
|+ style="font-size: 105%;" | 5L&nbsp;2s step ratios in various edos
!Name
!Range
|-
|-
|Ultrasoft
! Example edo
|1:1 ≤ L:s ≤ 4:3
! Step ratio
! TAMNAMS name
! Likely temperament<br />interpretations
|-
|-
|Parasoft
! 12
|4:3 ≤ L:s ≤ 3:2
| 2:1
| basic
| [[Meantone]] or [[Schismatic]]
|-
|-
|Quasisoft
! 19
|3:2 ≤ L:s ≤ 5:3
| 3:2
| soft
| [[Meantone]]
|-
|-
|Minisoft
! 22
|5:3 ≤ L:s ≤ 2:1
| 4:1
|-
| superhard
|Minihard
| [[Archy]] or [[Superpyth]]
|2:1 ≤ L:s ≤ 5:2
|-
|Quasihard
|5:2 ≤ L:s ≤ 3:1
|-
|Parahard
|3:1 ≤ L:s ≤ 4:1
|-
|Ultrahard
|4:1 ≤ L:s ≤ 1:0
|}
|}


=== Derivation ===
== Naming ==
The idea is to start with the simplest ratios (L/s = 1/0 and L/s = 1/1) and derive more complex ratios through repeated application of the [[mediant]] (aka Farey addition) to adjacent fractions. Applying the mediant to the starting intervals 1/0 and 1/1 gives (1+1)/(1+0) = 2/1, and as this is the simplest possible ratio where the large and small step are distinguished and nonzero, it is called the "quintessential" ("quintess." or "essential" for short) or "basic" tuning. (Note that if applying the mediant to 1/0 seems confusing, think of it as equivalent to applying the mediant to 0/1 and 1/1 and the ratios as flipped, thus representing s/L rather than L/s when written this way.) As L/s = 1/1 represents L and s being equal in size, it is called "equalized". As L/s = 1/0 represents s = 0, it is called "paucitonic", meaning "few tones", as the resulting scale is also equalized but with fewer tones per period than expected. The mediant of 1/1 and 2/1 is 3/2, thus making the scale sound mellower/softer, and as this is the simplest (in the sense of lowest [[Odd limit#Relationship_to_other_limits|integer limit]]) ratio to represent such a property, it is simply called the "soft" tuning, and analogously, the mediant of 2/1 and 1/0, 3/1, is called the "hard" tuning. Thus you can say that a step ratio tuning is "hard of" or "soft of" another step ratio tuning. To get something between soft and basic we take the mediant again and get 5/3 for "semisoft", and analogously 5/2 for "semihard". To get something more extreme we take the mediant of 1/0 with 3/1 for a harder-than-hard tuning, giving us 4/1 for "superhard" and analogously 4/3 for "supersoft". Something softer than supersoft is "ultrasoft". Something harder than superhard is "ultrahard". Something between soft and supersoft is "parasoft", as "para-" means both "beyond" and "next to". Something between hard and superhard is "parahard". The reasoning for the "para- super- ultra-" progression (note that "super-" is the odd one out as it refers to an exact ratio) is it mirrors naming for shades of musical intervals and because "parapythagorean" is between "pythagorean" and "superpythagorean". Something between soft and basic is "hyposoft" as it is less soft than soft. Something between hard and basic is "hypohard" for the same reason. Between semisoft and quintessential is "minisoft" and between semihard and quintessential is "minihard". Finally, between soft and semisoft is "quasisoft" as such scales may potentially be mistaken for soft or semisoft while not being either - hence the use of the prefix "quasi-", and between hard and semihard is "quasihard" for the same reason. This results in the "central spectrum" below - an elegant system which names all exact L/s ratios in the 5-integer-limit excepting only 5/1 and 5/4 which are disincluded intentionally for a variety of reasons: to keep the maximum corresponding notes per period in an [[EPD|equal pitch division]] low, because it keeps the 'tree' of mediants complete to a certain number of layers, and because their disinclusion gives a roughly-equally-spaced set of ratios, with the regions between 4/3 and 1/1 and between 4/1 and 1/0 being the only exceptions - corresponding to extreme tunings. Note that filling in those extreme regions is the purpose of the extended spectrum, detailed after.
Every MOS can be uniquely specified by giving its [[signature]], i.e. the number of large and small steps, which is typically notated e.g. "5L&nbsp;2s,". Every possible signature corresponds to a valid MOS scale. Sometimes, if one simply wants to talk about step sizes without specifying which is large and small, the notation "5a&nbsp;2b" is used (which could refer to either diatonic or {{nowrap| [[2L 5s|anti-diatonic]] {{=}} 2L 5s }}).


=== Central spectrum ===
By default, the [[equave]] of a MOS is assumed to be [[2/1]]. To specify a non-octave equave, "{{angbr|equave}}" is placed after the signature, e.g. {{mos scalesig|4L 5s<3/1>|link=1}}. Using angle brackets (<code>&#x26;#x27E8;</code> and <code>&#x26;#x27E9;</code>) is recommended; using greater-than and less-than signs ("&#x3C;equave&#x3E;") can also be done, but this can conflict with HTML and other uses of these symbols.
'''Equalized''': L/s = 1/1 (trivial/pathological)


::: ('''Ultrasoft''' range here, may also be called "pseudoequalized" if especially close to equalized.)
Several naming systems have been proposed for MOSes, which can be seen at [[MOS naming]].


:: '''Supersoft''': L/s = 4/3
== History and terminology ==
The term ''MOS'', and the method of scale construction it entails, were invented by [[Erv Wilson]] in 1975. His original paper is archived on Anaphoria.com here: [https://anaphoria.com/mos.pdf ''Moments of Symmetry'']. There is also an introduction by [[Kraig Grady]] here: [https://anaphoria.com/wilsonintroMOS.html ''Introduction to Erv Wilson's Moments of Symmetry''].


::: ('''Parasoft''' range here.)
Sometimes, scales are defined with respect to a period and an additional [[equivalence interval]], the interval at which pitch classes repeat. MOSes in which the equivalence interval is a multiple of the period, and in which there is more than one period per equivalence interval, are sometimes called '''Multi-MOSes'''. For example, a MOS with a half-octave period is called a '''2mos''', with a 1/3-octave period a '''3mos''', and so on. MOSes in which the equivalence interval is equal to the period are sometimes called '''Strict MOSes'''. MOSes in which the equivalence interval and period are simply disjunct, with no rational relationship between them, are simply MOS and have no additional distinguishing label.


: '''Soft''': L/s = 3/2
With a few notable exceptions, Wilson generally focused his attention on MOS with period equal to the equivalence interval. Hence, some people prefer to use the term [[Distributional evenness|distributionally even scale]], with acronym DE, for the more general class of scales which are MOS with respect to other intervals. MOS/DE scales are also sometimes known as ''well-formed scales'', the term used in the 1989 paper by Norman Carey and David Clampitt<ref>Norman Carey and David Clampitt. "Aspects of Well-Formed Scales", ''Music Theory Spectrum'', Vol. 11, No. 2 (Autumn, 1989), pp. 187-206.</ref>. A great deal of work has been done in academic circles extending these ideas. The idea of MOS also includes secondary or bi-level MOS scales which are actually the inspiration of Wilson's concept. They are in a sense the MOS of MOS patterns. This is used to explain the [[pentatonic]]s used in traditional [[Japanese music]] (e.g. {{nowrap| A B C E F A }}), where the 5-tone cycles are derived from a 7-tone MOS, which are not found in the concept of DE.


::: (Beginning of '''hyposoft''' range here.)
== Equivalent definitions and generalizations ==
A scale is a MOS if and only if it satisfies one of the following equivalent criteria:
# [[Maximum variety]] 2: Ascending by a certain number of steps is equivalent to ascending by one of at most two intervals, and the maximum of two is achieved (i. e. it is not true that ascending by a certain number of steps is always equivalent to ascending by one interval.)  
# [[Binary]] and has a [[generator]]: The scale step comes in exactly two sizes, and the scale is formable from stacking some interval called a generator and octave-reducing.
# Mode of a Christoffel word: The scale can be formed by creating a 2D lattice where the period is on the lattice, then taking pitches by travelling vertically and horizontally from the origin, maintaining as close to the line from the origin to the octave as possible without going above it.


::: ('''Quasisoft''' range here.)
Each definition generalizes to scales with three or more step sizes, but these generalizations are not equivalent. The concepts of [[balanced word|balance]] and [[distributional evenness]] provide still different generalizations, although defining MOS through these terms is less helpful. For more information, see [[Mathematics of MOS]].


:: '''Semisoft''': L/s = 5/3
== Properties ==
=== Basic properties ===
* For every MOS scale with an [[octave]] period (which is usually the [[octave]]), if ''x''-[[edo]] is the [[collapsed]] tuning (where the small step vanishes) and ''y''-[[edo]] is the [[equalized]] tuning (where the large (''L'') step and small (''s'') step are the same size), then by definition it is an {{nowrap| ''x''L (''y'' − ''x'')s }} MOS scale, and the [[basic]] tuning where {{nowrap| ''L'' {{=}} 2''s'' }} is thus {{nowrap|(''x'' + ''y'')}}-[[edo]]. This is also true if the period is 1\''p'', that is, 1 step of ''p''-[[edo]], which implies that ''x'' and ''y'' are divisible by ''p'', though note that in that case (if {{nowrap| ''p'' > 1 }}) you are considering a "multiperiod" MOS scale.
* More generally, whenever ''px''-[[edo]] and ''py''-[[edo]] are used to define two [[val]]s (usually but not necessarily through taking the [[Patent val|patent vals]]) while simultaneously also being used to define the {{nowrap|''px''L (''py'' − ''px'')s}} MOS scale (where ''p'' is the number of periods per octave), then the ''px'' & ''py'' temperament corresponds to that MOS scale, and adding ''x'' and/or ''y'' corresponds to tuning closer to ''x''-[[edo]] and/or ''y''-[[edo]] respectively. (Optionally, see the below more precise statement for the mathematically-inclined.)
* For the mathematically-inclined, we can say that whenever we consider a MOS with ''X''/''p'' notes per period in the [[collapsed]] tuning and ''Y''/''p'' notes per period in the [[equalized]] tuning and ''p'' periods per [[Octave stretching|tempered octave]] (or more generally tempered [[equave]]), and whenever we want to associate that MOS with the {{nowrap| ''X'' & ''Y'' }} rank 2 temperament'''*''', we can say that any {{w|natural number|natural}}-coefficient {{w|linear combination}} of vals {{val| ''X'' … }} and {{val| ''Y'' … }} (where {{nowrap| ''X'' < ''Y'' }}) corresponds uniquely to a tuning of the {{nowrap| ''X'' & ''Y'' }} rank 2 temperament between ''X''-[[ET]] and ''Y''-[[ET]] (inclusive) iff {{nowrap| gcd(''a'', ''b'') {{=}} 1 }}, because if {{nowrap| ''k'' {{=}} gcd(''a'', ''b'') > 1 }} then the val {{nowrap| ''a''{{val| ''X'' … }} + ''b''{{val| ''Y'' … }} }} has a common factor ''k'' in all of its terms, meaning it is guaranteed to be [[contorted]]. The tuning corresponding to the {{w|Rational number|rational}} ''a''/''b'' is technically only unique up to (discarding of) [[octave stretching]] (or more generally [[equave]]-tempering).


::: ('''Minisoft''' range here.)
: The period of this temperament is {{nowrap|1\gcd(''X'', ''Y'')}}, and the rational ''a''/''b'' is very closely related to the [[step ratio]] of the corresponding MOS scale, because {{nowrap| 1{{val| ''X'' … }} + 0{{val| ''Y'' … }} }} is the {{nowrap|''L'' {{=}} 1|''s'' {{=}} 0}} tuning while {{nowrap| 0{{val| ''X'' … }} + 1{{val| ''Y'' … }} }} is the {{nowrap|''L'' {{=}} 1|''s'' {{=}} 1}} tuning and {{nowrap| 1{{val| ''X'' … ;}} + 1{{val| ''Y'' … }} }} is the {{nowrap|''L'' {{=}} 2|''s'' {{=}} 1}} tuning, so that {{nowrap|''L'' {{=}} ''a'' + ''b''}} and {{nowrap|''s'' {{=}} ''b''}} and therefore:


::: (End of '''hyposoft''' range here.)
: {{nowrap|1/([[step ratio]]) {{=}} ''s''/''L''}} {{nowrap|{{=}} ''b''/(''a'' + ''b'')}} implying [[step ratio]] {{nowrap| ''r'' {{=}} (''a'' + ''b'')/''b'' ≥ 1 }} for {{w|Natural number|natural}} ''a'' and ''b'', where if {{nowrap| ''b'' {{=}} 0 }} then the step ratio is infinite, corresponding to the [[collapsed]] tuning.<ref group="note">It is ''important to note'' that the correspondence to the {{nowrap| ''X'' & ''Y'' }} rank-2 temperament only works in all cases if we allow the temperament to be [[contorted]] on its [[subgroup]]; alternatively, it works if we exclude cases where {{nowrap| ''X'' & ''Y'' }} describe a contorted temperament on the subgroup given. An example is the {{nowrap| 5 & 19 }} temperament is contorted in the [[5-limit]] (having a generator of a semifourth, corresponding to [[5L&nbsp;14s]]), so we either need to consider the temperament itself to be contorted (generated by something lacking an interpretation in the subgroup given, two of which yielding a meantone-tempered [[~]][[4/3]]) or we exclude it because of its contortion.</ref>


'''Quintesssential''': L/s = 2/1
* Every MOS scale has two ''child MOS'' scales. The two children of the MOS scale ''a''L&nbsp;''b''s are {{nowrap| (''a'' + ''b'')L ''a''s }} (generated by generators of soft-of-basic ''a''L ''b''s) and {{nowrap| ''a''L (''a'' + ''b'')s }} (generated by generators of hard-of-basic ''a''L''&nbsp;b''s).
* Every MOS scale (with a specified [[equave]] ''Ɛ''), excluding {{nowrap|''a''L ''a''s{{angbr|''Ɛ''|-)}} }}, has a ''parent MOS''. If {{nowrap| ''a'' > ''b'' }}, the parent of ''a''L&nbsp;''b''s is {{nowrap| ''b''L (''a'' − ''b'')s }}; if {{nowrap| ''a'' < ''b'' }}, the parent of ''a''L&nbsp;''b''s is {{nowrap| ''a''L (''b'' − ''a'')s }}.


::: (Beginning of '''hypohard''' range here.)
=== Advanced discussion ===
See:
* [[Mathematics of MOS]], a more formal definition and a discussion of the mathematical properties.
** [[Recursive structure of MOS scales]], a description of how MOS scales are recursive and how one scale can be converted into a related scale.
** [[MOS scale family tree]], a tree initially described by Erv Wilson that organizes scales by parent-and-child relationship, which also helps illustrate mos recursion.
* [[Generator ranges of MOS]], organized by number of scale steps and quantity of L/s steps.
* [[MOS diagrams]], visualizations of the MOS process.
* [http://x31eq.com/temper/method.html How to Find Linear Temperaments], by [[Graham Breed]]


::: ('''Minihard''' range here.)
== Individual pages for MOS scales ==
=== L ≤ 12, s ≤ 12 ===
{| class="wikitable center-all"
|+ style="font-size: 105%; white-space: nowrap;" | Pages for MOS scales ({{nowrap|L ≤ 12|s ≤ 12}})
|-
| [[1L&nbsp;1s]]
| [[1L&nbsp;2s]]
| [[1L&nbsp;3s]]
| [[1L&nbsp;4s]]
| [[1L&nbsp;5s]]
| [[1L&nbsp;6s]]
| [[1L&nbsp;7s]]
| [[1L&nbsp;8s]]
| [[1L&nbsp;9s]]
| [[1L&nbsp;10s]]
| [[1L&nbsp;11s]]
| [[1L&nbsp;12s]]
|-
| [[2L&nbsp;1s]]
| [[2L&nbsp;2s]]
| [[2L&nbsp;3s]]
| [[2L&nbsp;4s]]
| [[2L&nbsp;5s]]
| [[2L&nbsp;6s]]
| [[2L&nbsp;7s]]
| [[2L&nbsp;8s]]
| [[2L&nbsp;9s]]
| [[2L&nbsp;10s]]
| [[2L&nbsp;11s]]
| [[2L&nbsp;12s]]
|-
| [[3L&nbsp;1s]]
| [[3L&nbsp;2s]]
| [[3L&nbsp;3s]]
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|}


:: '''Semihard''': L/s = 5/2
=== L ≤ 12, 13 ≤ s ≤ 24 ===
{| class="wikitable mw-collapsible mw-collapsed center-all"
|+ style="font-size: 105%; white-space: nowrap;" | Pages for MOS scales ({{nowrap|L ≤ 12|13 ≤ s ≤ 24}})
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| [[1L&nbsp;13s]]
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::: ('''Quasihard''' range here.)
=== 13 ≤ L ≤ 24, s ≤ 12 ===
{| class="wikitable mw-collapsible mw-collapsed center-all"
|+ style="font-size: 105%; white-space: nowrap;" | Pages for MOS scales ({{nowrap|13 ≤ L ≤ 24|s ≤ 12}})
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| [[13L&nbsp;1s]]
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|}


::: (End of '''hypohard''' range here.)
=== Larger MOS scales ===
[[7L&nbsp;34s]], [[9L&nbsp;29s]], [[12L&nbsp;29s]], [[12L&nbsp;41s]], [[13L&nbsp;14s]], [[14L&nbsp;13s]], [[17L&nbsp;14s]], [[25L&nbsp;6s]], [[41L&nbsp;12s]]


: '''Hard''': L/s = 3/1
== Variations ==
 
* [[MODMOS scales]] are derived from chromatic alterations of one or more tones of an MOS scale, typically by the interval of {{nowrap| L s }}, the "chroma".
::: ('''Parahard''' range here.)
* [[Muddle]]s are subsets of MOS parent scales with the general shape of a smaller (and possibly unrelated) MOS scale.
 
* [[MOS cradle]] is a technique of embedding MOS-like structures inside MOS scales and may or may not produce subsets of MOS scales.
:: '''Superhard''': L/s = 4/1
* [[Operations on MOSes]]
 
::: ('''Ultrahard''' range here, may also be called "pseudopaucitonic" if especially close to paucitonic.)
 
'''Paucitonic''': L/s = 1/0 = infinity (trivial/pathological)
 
=== Extending the spectrum's edges ===
Extending the spectrum builds on the central spectrum and relies on a few key observations. Firstly, as periods and MOSSes come in wildly different shapes and sizes, and as we want to represent a somewhat representative variety of "simple" tunings for the step ratio for a given MOS pattern and period, the notion of "simple" used will correspond to the number of equally-spaced tones per period required. This is expressed as [number of large steps in pattern]*L + [number of small steps in pattern]*s, where L and s are from the step ratio itself, L/s, and are assumed to be coprime. Then, in order to not introduce bias to MOS patterns with more L's or more s's, we should assume that both are equally likely and thus weight both equally, which means that the resulting minimum number of tones per period for a ratio L/s is L+s. The next observation is that the large values of L/s can be a lot more consequential than the ones close to 1/1 due to the fact that small steps are guaranteed to be smaller than large steps and that we don't know how many small steps there are compared to large steps, and therefore the "hard" end of the spectrum is more vast, and analogously, L/s values close to 1/1 will tend to be inconsequential and for very close values likely impractical to distinguish - in the extremes only serving small tuning adjustments rather than melodic properties. This leads to another observation: MOS patterns with periods tuned to step ratios, while related to temperaments, ''are not'' temperaments - instead forming a sort of amalgamative superset of temperaments if you want to force a temperament interpretation, and thus their main function is in melodic structure, with temperaments informing potential harmonies and microtunings. Thus, the spectrum should be kept minimal and simple so that it is both generally hearable and not too specific.
 
The most obvious adjustment to the edges is to draw a distinction between "ultrasoft" and "pseudoequalized" by adding a step ratio corresponding to "semiequalized", and between "ultrahard" and "pseudopaucitonic" by adding a step ratio corresponding to "semipaucitonic". Thus:
 
'''Ultrasoft''' is between '''supersoft''' and '''semiequalized''' and '''pseudoequalized''' is between '''semiequalized''' and '''equalized'''.
 
'''Ultrahard''' is between '''superhard''' and '''semipaucitonic''', and '''pseudopaucitonic''' is between '''semipaucitonic''' and '''paucitonic'''.
 
Then all that's left is to decide what the step ratios for semipaucitonic and semiequalized should be. In order to keep the spacing (of the s/L ratios when graphed, or to a lesser extent the L/s ratios if you see the roughly gradual increase in spacing in that form) roughly consistent with all the other ratios, '''semiequalized''' should be L/s = 6/5 rather than L/s = 5/4. Then note the complexity of L/s = 6/5 is 6+5=11, so to find the corresponding complexity for '''semipaucitonic''' we use L/s = 10/1 as 10+1=11 too. Then finally, to preserve some of the symmetry, we include L/s = 6/1 as '''extrahard'''. Although L/s = 10/1 for '''semipaucitonic''' may seem a little extreme of a boundary, L/s = 12/1 would actually be what is the most "equally spaced" continuing on from 6/1 for the same reason that L/s = 6/5 is the most "equally spaced". Note that while the range from '''superhard''' to '''semipaucitonic''' is '''ultrahard''', the region may be split into two sub-ranges:
 
'''superhard''' (L/s=4/1) to '''extrahard''' (L/s=6/1) is '''hyperhard''' (4 < L/s < 6).
 
'''extrahard''' (L/s=6/1) to '''semipaucitonic''' (L/s=10/1) is '''clustered''' (6 < L/s < 10).
 
With the inclusion of these 3 new L/s rations nearer the edges of the spectrum and names for the range divisions they create, we get the extended spectrum, summarised and detailed below, just for the regions affected to avoid repetition.
 
=== Extended spectrum ===
'''Equalized''': L/s = 1/1 (trivial/pathological)
 
::: ('''Pseudoequalized''' range here.)
 
:: '''Semiequalized''': L/s = 6/5
 
::: ('''Ultrasoft''' range here.)
 
:: '''Supersoft''': L/s = 4/3
 
(4/3 < L/s < 4/1 range here, called the '''nonextreme''' range, detailed by central spectrum.)
 
:: '''Superhard''': L/s = 4/1
 
::: (Beginning of '''ultrahard''' range here.)
 
::: ('''Hyperhard''' range here.)
 
:: '''Extrahard''': L/s = 6/1
 
::: ('''Clustered''' range here.)
 
::: (End of '''ultrahard''' range here.)
 
:: '''Semipaucitonic''': L/s = 10/1
 
::: ('''Pseudopaucitonic''' range here.)


'''Paucitonic''': L/s = 1/0 = infinity (trivial/pathological)
== Listen ==
This is an algorithmically generated recording of every MOS scale that has 14 or fewer notes for a total of 91 scales being showcased here. Each MOS scale played has its simplest step ratio (large step is 2 small step is 1) and therefore is inside the smallest EDO that can support it. Each MOS scale is also in its brightest mode. And rhythmically, each scale is being played with its respective MOS rhythm. Note that changing the mode or step ratio of any of these MOSes may dramatically alter the sound and therefore this recording is not thoroughly representative of each MOS but rather a small taste.


=== Terminology and final notes ===
[[File:Every-MOS-Scale-With-14-Or-Fewer-Notes.mp3|left|800x800px]] {{clear}}
A ratio of L/s = k/1 can be called ''k-hard'' and a ratio of L/s = k/(k-1) can analogously be called ''k-soft'', so the simplest ultrasoft tuning is 5-soft or "pentasoft", the simplest hyperhard tuning is 5-hard or "pentahard", the simplest clustered tuning is 7-hard or "heptahard", 8-hard is "octahard", 9-hard is "nonahard", and finally, the characteristic simple ultrahard tuning is 6-hard or "extrahard", as previously discussed, which can be seen to be similar to "hexahard" - hopefully helping with memorisation.


A perhaps useful (or otherwise mildly amusing) mnemonic is "2-soft is too soft to be hard and 2-hard is too hard to be soft", representing that 2-soft = 2-hard = 2/1 = '''basic'''.
== See also ==
 
* Pailiaq's [https://lkorr.github.io/mos-explorer/ MOS explorer], an interactive tool for visualizing MOSses and the MOS spectrum.
Note that often the central spectrum will be sufficient for exploring a MOS pattern-period combination, and the extended spectrum is intended more for (literally) edge cases where it may be useful. Often if a temperament interpretation doesn't seem to show up for a MOS  pattern-period combination, it just means the temperament needs a more complex MOS pattern to narrow down the generator range. An example of this phenomena is the highly complex MOS pattern of [[12L 17s]] represents near-Pythagorean tunings well due to having a generator of a fourth or a fifth bounded between those of [[12edo]] and those of [[29edo]], which are roughly equally off but in opposite directions, and many important near-Pythagorean systems show up in just the ratios of the central spectrum alone.
* [[Diamond-mos notation]], a microtonal [[notation]] system focused on MOS scales
 
* [[Metallic MOS]], an article focusing on MOS scales based on metallic means, such as [[phi]]
== Mathematics ==
* [[MOS rhythm]]
See:
* [[:Category:MOS scales|Category:MOS scales]], the category including all MOS-related articles on this wiki
* [[Mathematics of MOS]], a more formal definition and a discussion of the mathematical properties.
* [[Gallery of MOS patterns]]
* [[Generator ranges of MOS]], organized by number of scale steps and quantity of L/s steps.
* [[MOS Diagrams]], visualizations of the MOS process.
* [http://x31eq.com/temper/method.html How to Find Linear Temperaments], by [[Graham Breed]]
 
== Variations ==
* [[MODMOS Scales]] are derived from chromatic alterations of one or more tones of an MOS scale, typically by the interval of L-s, the "chroma".
* [[Muddle]]s are subsets of MOS parent scales with the general shape of a smaller (and possibly unrelated) MOS scale.
* [[MOS Cradle]] is a technique of embedding MOS-like structures inside MOS scales and may or may not produce subsets of MOS scales.
* [[Operations on MOSes]]


== As applied to rhythms ==
== Notes ==
David Canright was the first to suggest Fibonacci Rhythms in 1/1. This led to Kraig Grady to be the first to apply MOS patterns to rhythms. Two papers on the subject can be found here:
<references group="note" />
* [http://anaphoria.com/hora.pdf A Rhythmic Application of the Horagrams] from Xenharmonikon 16
* [http://anaphoria.com/horo2.pdf More on Horogram Rhythms].


MOS structures and thinking can be applied to the design of rhythms as well. See [[MOS Rhythm Tutorial]].
== References ==
<references />


[[Category:Math]]
[[Category:Math]]
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[[Category:Overview]]
[[Category:Scale]]
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