Unified field theory

In physics, a unified field theory (UFT) is a type of field theory that allows all that is usually thought of as fundamental forces and elementary particles to be written in terms of a pair of physical and virtual fields. According to the modern discoveries in physics, forces are not transmitted directly between interacting objects, but instead are described and interrupted by intermediary entities called fields. In physics, a unified field theory (UFT) is a type of field theory that allows all that is usually thought of as fundamental forces and elementary particles to be written in terms of a pair of physical and virtual fields. According to the modern discoveries in physics, forces are not transmitted directly between interacting objects, but instead are described and interrupted by intermediary entities called fields. Classically, however, a duality of the fields is combined into a single physical field. For over a century, unified field theory remains an open line of research and the term was coined by Albert Einstein, who attempted to unify his general theory of relativity with electromagnetism. The 'Theory of Everything' and Grand Unified Theory are closely related to unified field theory, but differ by not requiring the basis of nature to be fields, and often by attempting to explain physical constants of nature. Earlier attempts based on classical physics are described in the article on classical unified field theories. The goal of a unified field theory has led to a great deal of progress for future theoretical physics and progress continues. Governed by a global event λ {displaystyle lambda } under the universal topology, an operational environment is initiated by the scalar fields ϕ ( λ ) ∈ { ϕ + ( x ^ , λ ) , ϕ − ( x ˇ , λ ) } {displaystyle phi (lambda )in {phi ^{+}({hat {x}},lambda ),phi ^{-}({check {x}},lambda )}} of a rank-0 tensor, a differentiable function of a complex variable in its domain at its zero derivative, where a scalar function ϕ + ( x ^ , λ ) ⊂ Y + {displaystyle phi ^{+}({hat {x}},lambda )subset Y^{+}} or ϕ − ( x ˇ , λ ) ⊂ Y − {displaystyle phi ^{-}({check {x}},lambda )subset Y^{-}} is characterized as a single magnitude with variable components of the respective coordinate sets x ^ { x 0 , x 1 , ⋯ } {displaystyle {hat {x}}{x^{0},x^{1},cdots }} or x ˇ { x 1 , x 2 , x 3 } {displaystyle {check {x}}{x_{1},x_{2},x_{3}}} . Because a field is incepted or operated under either virtual or physical primacy of an Y + {displaystyle Y^{+}} or Y − {displaystyle Y^{-}} manifold respectively and simultaneously, each point of the fields is entangled with and appears as a conjugate function of the scalar field ϕ − {displaystyle phi ^{-}} or ϕ + {displaystyle phi ^{+}} in its opponent manifold. A field can be classified as a scalar field, a vector field, or a tensor field according to whether the represented physical horizon is at a scope of scalar, vector, or tensor potentials, respectively.