Definite quadratic form - Wikipedia: "the quadratic form is called positive definite or negative definite."
'via Blog this'
Sunday, February 25, 2018
Riemannian manifold - Wikipedia
Riemannian manifold - Wikipedia: " real, smooth manifold M equipped with an inner product {\displaystyle g_{p}} on the tangent space {\displaystyle T_{p}M} at each point {\displaystyle p} that varies smoothly from point to point "
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Wednesday, February 14, 2018
Lie Groups (why do mirrors reverse left and right, but not up and down?)
Lie Groups: "Digression: the well-known puzzle, ``why do mirrors reverse left and right, but not up and down?'' is resolved mathematically by pointing out that a mirror perpendicular to the y-axis performs the reflection:
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Tuesday, February 13, 2018
Group action - Wikipedia
Group action - Wikipedia: "stabilizer subgroup of G with respect to x (also called the isotropy group "
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Saturday, February 10, 2018
Differential of a function - Wikipedia
Differential of a function - Wikipedia: "The differential dy is defined by
{\displaystyle dy=f'(x)\,dx,}
where {\displaystyle f'(x)} is the derivative of f with respect to x, and dx is an additional real variable (so that dy is a function of x and dx). "
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{\displaystyle dy=f'(x)\,dx,}
where {\displaystyle f'(x)} is the derivative of f with respect to x, and dx is an additional real variable (so that dy is a function of x and dx). "
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What first-order linearity really is
‘to first order everything is linear’. This is tautological, of course, but it really says
that most functions are differentiable and we can approximate by the first derivative.
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that most functions are differentiable and we can approximate by the first derivative.
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Differential (infinitesimal) - Wikipedia
Differential (infinitesimal) - Wikipedia: "the differential dy of y is related to dx by the formula
{\displaystyle \mathrm {d} y={\frac {\mathrm {d} y}{\mathrm {d} x}}\,\mathrm {d} x,}
where dy/dx denotes the derivative of y with respect to x."
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{\displaystyle \mathrm {d} y={\frac {\mathrm {d} y}{\mathrm {d} x}}\,\mathrm {d} x,}
where dy/dx denotes the derivative of y with respect to x."
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One-form - Wikipedia
One-form - Wikipedia: "Many real-world concepts can be described as one-forms:
Indexing into a vector"
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Indexing into a vector"
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Linear form - Wikipedia
Linear form - Wikipedia: "Any linear functional L is either trivial (equal to 0 everywhere) or surjective onto the scalar field."
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Linear form - Wikipedia
Linear form - Wikipedia: "A state of a quantum mechanical system can be identified with a linear functional."
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Quadrature (mathematics) - Wikipedia
Quadrature (mathematics) - Wikipedia: "In mathematics, quadrature is a historical term which means determining area."
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One-form - Wikipedia
One-form - Wikipedia: "The usage of one-form in this context usually distinguishes the one-forms from higher-degree multilinear functionals on the space"
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Function space - Wikipedia
Function space - Wikipedia: " if X is also vector space over F, the set of linear maps X → V form a vector space over F with pointwise operations (often denoted Hom(X,V)). One such space is the dual space of V: the set of linear functionals V → F with addition and scalar multiplication defined pointwise."
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Function space - Wikipedia
Function space - Wikipedia: "the set of functions from any set X into a vector space have a natural vector space structure given by pointwise addition and scalar multiplication."
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Pointwise - Wikipedia
Pointwise - Wikipedia: "By taking some algebraic structure {\displaystyle A} in the place of {\displaystyle R} , we can turn the set of all functions {\displaystyle X} to the carrier set of {\displaystyle A} into an algebraic structure of the same type in an analogous way."
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Thursday, February 08, 2018
Hamiltonian
It turns out that giving the position and momentum of a particle specifies a point
in a space called the ‘phase space’ or ‘state space’ of the particle. Mathematically this is often a
‘cotangent bundle’ — an important concept from the theory of manifolds. A cotangent bundle is
an example of a ‘symplectic manifold’, which in turn is an example of a more general thing called a
‘Poisson manifold’.
'via Blog this'
in a space called the ‘phase space’ or ‘state space’ of the particle. Mathematically this is often a
‘cotangent bundle’ — an important concept from the theory of manifolds. A cotangent bundle is
an example of a ‘symplectic manifold’, which in turn is an example of a more general thing called a
‘Poisson manifold’.
'via Blog this'
Monday, February 05, 2018
Classical mechanics observables a commutative and Lie algebra
In fact for all classical mechanics problems, the algebra of observables C∞(X) is always both a
commutative algebra and a Lie algebra, but even better, they fit together to form a Poisson algebra.
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commutative algebra and a Lie algebra, but even better, they fit together to form a Poisson algebra.
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Observables
In our example of a particle in R
n, we said an observable is a smooth function
F: R
n × R
n → R
by
(q, p) 7→ F(q, p)
from the phase space to R, sending each point of phase space (or state of our system) to the value
of the observables.
'via Blog this'
n, we said an observable is a smooth function
F: R
n × R
n → R
by
(q, p) 7→ F(q, p)
from the phase space to R, sending each point of phase space (or state of our system) to the value
of the observables.
'via Blog this'
configuration vs phase spaces
Hamiltonian mechanics focuses not on the configuration space but on the phase space or
state space, where a point specifies the position and momentum of the system
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state space, where a point specifies the position and momentum of the system
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Lorentz group
Schuller lecture 13 defines Lorentz group in a general way as a vector space equipped with a pseudo inner product (that is little bit less positive definite)
Configuration space (physics) - Wikipedia
Configuration space (physics) - Wikipedia: "In classical mechanics, the parameters that define the configuration of a system are called generalized coordinates, and the vector space defined by these coordinates is called the configuration space of the physical system. It is often the case that these parameters satisfy mathematical constraints, such that the set of actual configurations of the system is a manifold in the space of generalized coordinates. This manifold is called the configuration manifold of the system.
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Configuration space (mathematics) - Wikipedia
Configuration space (mathematics) - Wikipedia: "these are used to describe the state of a whole system as a single point in a high-dimensional space."
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Sunday, February 04, 2018
Picturing the Correspondences
Picturing the Correspondences: "Since the action preserves distances, one can also consider the action of the group just on the set of vectors of norm 1, i.e., on the sphere.)"
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Center (group theory) - Wikipedia
Center (group theory) - Wikipedia: "The center of an abelian group, G, is all of G.
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Symplectic group - Wikipedia
Symplectic group - Wikipedia: "Since all symplectic matrices have determinant 1, the symplectic group is a subgroup of the special linear group SL(2n, F).
Notational warning: What is here called Sp(2n, F) is often referred to as Sp(n, F).
More abstractly, the symplectic group can be defined as the set of linear transformations of a 2n-dimensional vector space over F that preserve a non-degenerate, skew-symmetric, bilinear form, see classical group for this definition. Such a vector space is called a symplectic vector space. The symplectic group of an abstract symplectic vector space V is also denoted Sp(V)."
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Notational warning: What is here called Sp(2n, F) is often referred to as Sp(n, F).
More abstractly, the symplectic group can be defined as the set of linear transformations of a 2n-dimensional vector space over F that preserve a non-degenerate, skew-symmetric, bilinear form, see classical group for this definition. Such a vector space is called a symplectic vector space. The symplectic group of an abstract symplectic vector space V is also denoted Sp(V)."
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Unitary group - Wikipedia
Unitary group - Wikipedia: "Hyperorthogonal group is an archaic name for the unitary group, especially over finite fields. For the group of unitary matrices with determinant 1, see Special unitary group.
In the simple case n = 1, the group U(1) corresponds to the circle group, consisting of all complex numbers with absolute value 1 under multiplication. All the unitary groups contain copies of this group."
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In the simple case n = 1, the group U(1) corresponds to the circle group, consisting of all complex numbers with absolute value 1 under multiplication. All the unitary groups contain copies of this group."
'via Blog this'
Lie Groups
Lie Groups: " and . These are, colloquially, the groups of rotations in 2-space and 3-space. O(n) is the group of reflections and rotations."
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'via Blog this'
Saturday, February 03, 2018
Homogeneous space - Wikipedia
Homogeneous space - Wikipedia: "homogeneous space can be thought of as a coset space without a choice of origin."
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Friday, February 02, 2018
Group action - Wikipedia
Group action - Wikipedia: "Free (or semiregular or fixed point free) if, given g, h in G, the existence of an x in X with g⋅x = h⋅x implies g = h. Equivalently: if g is a group element and there exists an x in X with g⋅x = x (that is, if g has at least one fixed point), then g is the identity. "
"fix point free" that is, the action transforms free of fixed points
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"fix point free" that is, the action transforms free of fixed points
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Group action - Encyclopedia of Mathematics
Group action - Encyclopedia of Mathematics: "If the homomorphism ρρ is injective the action is faithful: GG may be regarded as a subgroup of SXSX"
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Transitive Group Action -- from Wolfram MathWorld
Transitive Group Action -- from Wolfram MathWorld: "The space , which has a transitive group action, is called a homogeneous space when the group is a Lie group."
(w) Regular (or simply transitive or sharply transitive) if it is both transitive and free; this is equivalent to saying that for every two x, y in X there exists precisely one g in Gsuch that g⋅x = y. In this case, X is called a principal homogeneous space for G or a G-torsor.
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(w) Regular (or simply transitive or sharply transitive) if it is both transitive and free; this is equivalent to saying that for every two x, y in X there exists precisely one g in Gsuch that g⋅x = y. In this case, X is called a principal homogeneous space for G or a G-torsor.
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Group action - Wikipedia
Group action - Wikipedia: "The group action is transitive if and only if it has exactly one orbit, i.e., if there exists x in X with G⋅x = X. This is the case if and only if G⋅x = X for all x in X.
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Orthogonal Group -- from Wolfram MathWorld
Orthogonal Group -- from Wolfram MathWorld: "In fact, the orthogonal group is a smooth -dimensional submanifold"
Because the orthogonal group is a group and a manifold, it is a Lie group.
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Because the orthogonal group is a group and a manifold, it is a Lie group.
Group Orbit -- from Wolfram MathWorld
Group Orbit -- from Wolfram MathWorld: "For example, consider the action by the circle group on the sphere by rotations along its axis. Then the north pole is an orbit, as is the south pole. The equator is a one-dimensional orbit, as is a general orbit, corresponding to a line of latitude.
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torsors
torsors: " This combination of translations and dilations arises because R is not just a group, but a ring. "
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torsors
torsors: "You can always pretend a torsor is a group. But, it involves an arbitrary choice!"
:
Any group G is a G-torsor, and every other G-torsor is isomorphic to G - but not canonically!
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:
Any group G is a G-torsor, and every other G-torsor is isomorphic to G - but not canonically!
'via Blog this'
Thursday, February 01, 2018
Group representation - Wikipedia
Group representation - Wikipedia: "formally, a "representation" means a homomorphism from the group to the automorphism group of an object"
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