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・ Diffusion current
・ Diffusion curve
・ Diffusion damping
・ Diffusion equation
・ Diffusion filter
・ Differential mobility detector
・ Differential nonlinearity
・ Differential norming
・ Differential object marking
・ Differential of a function
・ Differential of the first kind
・ Differential operator
・ Differential optical absorption spectroscopy
・ Differential outcomes effect
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Differential poset
・ Differential privacy
・ Differential psychology
・ Differential pulley
・ Differential pulse voltammetry
・ Differential pulse-code modulation
・ Differential refractometer
・ Differential rotation
・ Differential scanning calorimetry
・ Differential screw
・ Differential signaling
・ Differential space–time code
・ Differential staining
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Differential poset : ウィキペディア英語版
Differential poset
In mathematics, a differential poset is a partially ordered set (or ''poset'' for short) satisfying certain local properties. (The formal definition is given below.) This family of posets was introduced by as a generalization of Young's lattice (the poset of integer partitions ordered by inclusion), many of whose combinatorial properties are shared by all differential posets. In addition to Young's lattice, the other most significant example of a differential poset is the Young–Fibonacci lattice.
==Definitions==

A poset ''P'' is said to be a differential poset, and in particular to be ''r''-differential (where ''r'' is a positive integer), if it satisfies the following conditions:
* ''P'' is graded and locally finite with a unique minimal element;
* for every two distinct elements ''x'', ''y'' of ''P'', the number of elements covering both ''x'' and ''y'' is the same as the number of elements covered by both ''x'' and ''y''; and
* for every element ''x'' of ''P'', the number of elements covering ''x'' is exactly ''r'' more than the number of elements covered by ''x''.
These basic properties may be restated in various ways. For example, Stanley shows that the number of elements covering two distinct elements ''x'' and ''y'' of a differential poset is always either 0 or 1, so the second defining property could be altered accordingly.
The defining properties may also be restated in the following linear algebraic setting: taking the elements of the poset ''P'' to be formal basis vectors of an (infinite dimensional) vector space, let ''D'' and ''U'' be the operators defined so that ''D'' ''x'' is equal to the sum of the elements covered by ''x'', and ''U'' ''x'' is equal to the sum of the elements covering ''x''. (The operators ''D'' and ''U'' are called the ''down'' and ''up operator'', for obvious reasons.) Then the second and third conditions may be replaced by the statement that ''DU'' – ''UD'' = ''rI'' (where ''I'' is the identity).
This latter reformulation makes a differential poset into a combinatorial realization of a Weyl algebra, and in particular explains the name ''differential'': the operators "''d''/''dx''" and "multiplication by ''x''" on the vector space of polynomials obey the same commutation relation as ''U'' and ''D''/''r''.

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