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| The connotative component of a sign relation ''L'' can be formalized as its dyadic projection on the plane generated by the sign domain and the interpretant domain, defined as follows: | | The connotative component of a sign relation ''L'' can be formalized as its dyadic projection on the plane generated by the sign domain and the interpretant domain, defined as follows: |
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− | : ''Con''(''L'') = ''Proj''<sub>''SI''</sub> ''L'' = ''L''<sub>''SI''</sub> = {‹''s'', ''i''› ∈ ''S'' × ''I'' : ‹''o'', ''s'', ''i''› ∈ ''L'' for some ''o'' ∈ ''O''}. | + | : <math>\operatorname{Con}(L) = \operatorname{proj}_{SI} L = L_{SI} = \{ (s, i) \in S \times I : (o, s, i) \in L ~\text{for some}~ o \in O \}</math>. |
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− | The intentional component of semantics for a sign relation ''L'', or its ''second moment of denotation'', is adequately captured by its dyadic projection on the plane generated by the object domain and interpretant domain, defined as follows: | + | The intentional component of semantics for a sign relation <math>L</math>, or its ''second moment of denotation'', is adequately captured by its dyadic projection on the plane generated by the object domain and interpretant domain, defined as follows: |
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− | : ''Int''(''L'') = ''Proj''<sub>''OI''</sub> ''L'' = ''L''<sub>''OI''</sub> = {‹''o'', ''i''› ∈ ''O'' × ''I'' : ‹''o'', ''s'', ''i''› ∈ ''L'' for some ''s'' ∈ ''S''}. | + | : <math>\operatorname{Int}(L) = \operatorname{proj}_{OI} L = L_{OI} = \{ (o, i) \in O \times I : (o, s, i) \in L ~\text{for some}~ s \in S \}</math>. |
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− | As it happens, the sign relations ''L''<sub>''A''</sub> and ''L''<sub>''B''</sub> in the present example are fully symmetric with respect to exchanging signs and interpretants, so all of the structure of (''L''<sub>''A''</sub>)<sub>''OS'' </sub> and (''L''<sub>''B''</sub>)<sub>''OS'' </sub> is merely echoed in (''L''<sub>''A''</sub>)<sub>''OI'' </sub> and (''L''<sub>''B''</sub>)<sub>''OI'' </sub>, respectively. | + | As it happens, the sign relations <math>L_\text{A}</math> and <math>L_\text{B}</math> in the present example are fully symmetric with respect to exchanging signs and interpretants, so all of the structure of <math>(L_\text{A})_{OS}</math> and <math>(L_\text{B})_{OS}</math> is merely echoed in <math>(L_\text{A})_{OI}</math> and <math>(L_\text{B})_{OI}</math>, respectively. |
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− | '''Note on notation.''' When there is only one sign relation ''L''<sub>''J'' </sub> = ''L''(''J'') associated with a given interpreter ''J'', it is convenient to use the following forms of abbreviation: | + | '''Note on notation.''' When there is only one sign relation <math>L_J = L(J)</math> associated with a given interpreter <math>J</math>, it is convenient to use the following forms of abbreviation: |
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