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・ Amplitude damping channel
・ Amplitude death
・ Amplitude distortion
・ Amplitude domain reflectometry
・ Amplitude gate
・ Amplitude modulation
・ Amplitude modulation signalling system
・ Amplitude of accommodation
・ Amplitude of low frequency fluctuations
・ Amplitude panning
・ Amplitude Studios
・ Amplitude versus offset
・ Amplitude-companded single-sideband modulation
・ Amplitude-Comparison Monopulse
・ Amplitude-shift keying
Amplituhedron
・ AmpLive
・ Amplypterus
・ Amplypterus celebensis
・ Amplypterus mansoni
・ Amplypterus mindanaoensis
・ Amplypterus panopus
・ Amplypterus sumbawanensis
・ Ampm
・ Ampney
・ Ampney Crucis
・ Ampney St Mary
・ Ampney St Peter
・ Ampo snack
・ Ampohibe


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Amplituhedron : ウィキペディア英語版
Amplituhedron
An amplituhedron is a geometric structure that enables simplified calculation of particle interactions in some quantum field theories. In planar ''N'' = 4 supersymmetric Yang–Mills theory, also equivalent to the peturbative topological B model string theory in twistor space, an amplituhedron is defined as a mathematical space known as the positive Grassmannian.
Amplituhedron theory challenges the notion that space-time locality and unitarity are necessary components of a model of particle interactions. Instead, they are treated as properties that emerge from an underlying phenomenon.
The connection between the amplituhedron and scattering amplitudes is at present a conjecture that has passed many non-trivial checks, including an understanding of how locality and unitarity arise as consequences of positivity.
Research has been led by Nima Arkani-Hamed. Edward Witten described the work as “very unexpected" and said that "it is difficult to guess what will happen or what the lessons will turn out to be."
== Description ==
In the approach, the on-shell scattering process "tree" is described by a positive Grassmannian, a structure in algebraic geometry analogous to a convex polytope, that generalizes the idea of a simplex in projective space. A polytope is the ''n''-dimensional analogue of 3-dimensional polyhedrons, and the values being calculated in this case are scattering amplitudes, and so the object is called an ''amplituhedron''.
Using twistor theory, BCFW recursion relations involved in the scattering process may be represented as a small number of twistor diagrams. These diagrams effectively provide the recipe for constructing the positive Grassmannian, i.e. the amplituhedron, which may be captured in a single equation. The scattering amplitude can thus be thought of as the volume of a certain polytope, the positive Grassmannian, in momentum twistor space.
When the volume of the amplituhedron is calculated in the planar limit of ''N'' = 4 ''D'' = 4 supersymmetric Yang–Mills theory, it describes the scattering amplitudes of subatomic particles.〔 The amplituhedron thus provides a more intuitive geometric model for calculations whose underlying principles were until then highly abstract.
The twistor-based representation provides a recipe for constructing specific cells in the Grassmannian which assemble to form a positive Grassmannian, i.e. the representation describes a specific cell decomposition of the positive Grassmannian.
The recursion relations can be resolved in many different ways, each giving rise to a different representation, with the final amplitude expressed as a sum of on-shell processes in different ways as well. Therefore any given on-shell representation of scattering amplitudes is not unique, but all such representations of a given interaction yield the same amplituhedron.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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