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MyWikiBiz, Author Your Legacy — Thursday May 02, 2024
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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>&nbsp;''L'' = ''L''<sub>''SI''</sub> = {‹''s'',&nbsp;''i''› &isin; ''S''&nbsp;&times;&nbsp;''I'' : ‹''o'',&nbsp;''s'',&nbsp;''i''› &isin; ''L'' for some ''o'' &isin; ''O''}.
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: <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:
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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>&nbsp;''L'' = ''L''<sub>''OI''</sub> = {‹''o'',&nbsp;''i''› &isin; ''O''&nbsp;&times;&nbsp;''I'' : ‹''o'',&nbsp;''s'',&nbsp;''i''› &isin; ''L'' for some ''s'' &isin; ''S''}.
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: <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''&nbsp;</sub> and (''L''<sub>''B''</sub>)<sub>''OS''&nbsp;</sub> is merely echoed in (''L''<sub>''A''</sub>)<sub>''OI''&nbsp;</sub> and (''L''<sub>''B''</sub>)<sub>''OI''&nbsp;</sub>, respectively.
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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''&nbsp;</sub> = ''L''(''J'') associated with a given interpreter ''J'', it is convenient to use the following forms of abbreviation:
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'''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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:{| cellpadding=4
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