Functional-theoretic Algebra
   HOME

TheInfoList



OR:

Any vector space can be made into a unital
associative algebra In mathematics, an associative algebra ''A'' over a commutative ring (often a field) ''K'' is a ring ''A'' together with a ring homomorphism from ''K'' into the center of ''A''. This is thus an algebraic structure with an addition, a mult ...
, called functional-theoretic algebra, by defining products in terms of two linear functionals. In general, it is a
non-commutative algebra In mathematics, a noncommutative ring is a ring whose multiplication is not commutative; that is, there exist ''a'' and ''b'' in the ring such that ''ab'' and ''ba'' are different. Equivalently, a ''noncommutative ring'' is a ring that is not a ...
. It becomes commutative when the two functionals are the same.


Definition

Let ''AF'' be a
vector space In mathematics and physics, a vector space (also called a linear space) is a set (mathematics), set whose elements, often called vector (mathematics and physics), ''vectors'', can be added together and multiplied ("scaled") by numbers called sc ...
over a
field Field may refer to: Expanses of open ground * Field (agriculture), an area of land used for agricultural purposes * Airfield, an aerodrome that lacks the infrastructure of an airport * Battlefield * Lawn, an area of mowed grass * Meadow, a grass ...
''F'', and let ''L''1 and ''L''2 be two
linear functional In mathematics, a linear form (also known as a linear functional, a one-form, or a covector) is a linear mapIn some texts the roles are reversed and vectors are defined as linear maps from covectors to scalars from a vector space to its field of ...
s on AF with the property ''L''1(''e'') = ''L''2(''e'') = 1''F'' for some ''e'' in ''AF''. We define multiplication of two elements ''x'', ''y'' in ''AF'' by : x \cdot y = L_1(x)y + L_2(y)x - L_1(x) L_2(y) e. It can be verified that the above multiplication is associative and that ''e'' is the identity of this multiplication. So, AF forms an associative algebra with unit ''e'' and is called a ''functional theoretic algebra''(FTA). Suppose the two linear functionals ''L''1 and ''L''2 are the same, say ''L.'' Then ''AF'' becomes a commutative algebra with multiplication defined by : x \cdot y = L(x)y + L(y)x - L(x)L(y)e.


Example

''X'' is a nonempty set and ''F'' a field. ''F''''X'' is the set of functions from ''X'' to ''F''. If ''f, g'' are in ''F''''X'', ''x'' in ''X'' and ''α'' in ''F'', then define : (f+g)(x) = f(x) + g(x)\, and : (\alpha f)(x)=\alpha f(x).\, With addition and scalar multiplication defined as this, ''F''''X'' is a vector space over ''F.'' Now, fix two elements ''a, b'' in ''X'' and define a function ''e'' from ''X'' to ''F'' by ''e''(''x'') = 1''F'' for all ''x'' in ''X''. Define ''L''1 and ''L2'' from ''F''''X'' to ''F'' by ''L''1(''f'') = ''f''(''a'') and ''L''2(''f'') = ''f''(''b''). Then ''L''1 and ''L''2 are two linear functionals on ''F''''X'' such that ''L''1(''e'')= ''L''2(''e'')= 1''F'' For ''f, g'' in ''F''''X'' define : f \cdot g = L_1(f)g + L_2(g)f - L_1(f) L_2(g) e = f(a)g + g(b)f - f(a)g(b)e. Then ''F''''X'' becomes a non-commutative function algebra with the function ''e'' as the identity of multiplication. Note that : (f \cdot g)(a) = f(a)g(a)\mbox (f \cdot g)(b) = f(b)g(b).


FTA of Curves in the Complex Plane

Let C denote the
field Field may refer to: Expanses of open ground * Field (agriculture), an area of land used for agricultural purposes * Airfield, an aerodrome that lacks the infrastructure of an airport * Battlefield * Lawn, an area of mowed grass * Meadow, a grass ...
of Complex numbers. A continuous function ''γ'' from the closed interval [0, 1] of real numbers to the field C is called a curve. The complex numbers ''γ''(0) and ''γ''(1) are, respectively, the initial and terminal points of the curve. If they coincide, the curve is called a ''loop''. The set ''V''[0, 1] of all the curves is a vector space over C. We can make this vector space of curves into an algebra by defining multiplication as above. Choosing e(t) = 1, \forall \in [0, 1] we have for ''α,β'' in ''C''[0, 1], : \cdot = (0) + (1) - (0)(1)e Then, ''V''[0, 1] is a non-commutative algebra with ''e'' as the unity. We illustrate this with an example.


Example of f-Product of Curves

Let us take (1) the line segment joining the points (1, 0) and (0, 1) and (2) the unit circle with center at the origin. As curves in ''V''[0, 1], their equations can be obtained as : f(t)=1 - t + it \mbox g(t)= \cos(2\pi t)+ i\sin(2\pi t) Since g(0)=g(1)=1 the circle ''g'' is a loop. The line segment ''f'' starts from : f(0)=1 and ends at f(1)= i Now, we get two ''f''-products f \cdot g \mbox g \cdot f given by :(f\cdot g)(t)=[-t+\cos (2\pi t)]+i[t+\sin(2\pi t)] and :(g\cdot f)(t)=[1-t - \sin (2\pi t)] +i[t-1+\cos(2\pi t)] See the Figure. Observe that f\cdot g \neq g\cdot f showing that multiplication is non-commutative. Also both the products starts from f(0)g(0)=1 \mbox f(1)g(1)= i.


See also

* N-curve


References

* Sebastian Vattamattam and R. Sivaramakrishnan, ''A Note on Convolution Algebras'', in ''Recent Trends in Mathematical Analysis'', Allied Publishers, 2003. * Sebastian Vattamattam and R. Sivaramakrishnan, ''Associative Algebras via Linear Functionals'', Proceedings of the Annual Conference of K.M.A., Jan. 17 - 19, 2000, pp. 81-89 * Sebastian Vattamattam, ''Non-Commutative Function Algebras'', in ''Bulletin of Kerala Mathematical Association'', Vol. 4, No. 2, December 2007 * Sebastian Vattamattam, ''Transforming Curves by n-Curving'', in ''Bulletin of Kerala Mathematics Association'', Vol. 5, No. 1, December 2008 * Sebastian Vattamattam, ''Book of Beautiful Curves'', January 201
Book of Beautiful Curves
* R. Sivaramakrishnan, ''Certain Number Theoretic Episodes in Algebra'', Chapman and Hall/CR
Certain Number Theoretic Episodes in Algebra
{{refend Algebras