Analysis
1. Limit
1.1. Limit Superior and Limit Inferior
,- Supremum Limit, Limit Supremum, Limsup, Superior Limit, Upper Limit, Outer Limit.
,- Infimum Limit, Limit Infimum, Liminf, Inferior Limit, Lower Limit, Inner Limit
1.1.1. Definition
2. Cauchy Sequnce
2.1. In Metric Space
- A sequence
in a metric space is called Cauchy sequence if:
3. Convergence
3.1. Fixed-Point Iteration
Useful in finding a root of a function.
Convert the problem
The iteration is gueranteed to converge around the fixed-point if the slope is confined within -1 and 1. To be more precise, the graph of the function should not poke through the tops and bottoms of any square centered at the origin. Although there are possiblities that the point outside the square can converge.
The slope
4. Continuity
4.1. Definitions
4.1.1. Via Limits of Functions
- is equal to itself.
- Otherwise, occurs.
4.1.2. Via Neighborhoods
- For any
, there is a neighborhood such that .
4.1.3. Via Limits of Sequences
- For any sequence
that converges to , the sequence converges to .
4.1.4. Weierstrass and Jordan Definitions
- Epsilon-Delta Definition of Continuous Functions
, .
4.1.5. Via Control of the Remainder
4.1.6. Via Oscillation
4.1.7. Via Hyperreals
4.1.8. Topological Definition
- Therefore, it preserves the topology.1
- This definition might vary from the standard definition depending
on the context.
- Wait, this is continuous?? - YouTube
- The floor funtion
is continuous under the lower limit topology.
4.2. Properties
- Monotone surjective function is continuous, and admits an inverse function.
- Given a sequence of functions
that converges pointwise, that is:- the function
that is referred to as the pointwise limit of the sequence, need not be continuous, even if all functions are continuous.
- the function
- https://en.wikipedia.org/wiki/Continuous_function
4.3. Intermediate Value Theorem
IVT
4.3.1. Statement
For a continuous function
4.3.2. Proof
Consider the subset
4.4. Extreme Value Theorem
EVT
4.4.1. Statement
- If
is continuous on the interval , then has maxima and minima on .
4.5. Generalizations
4.5.1. Uniform Continuity
- See
4.5.2. Absolute Continuity
4.5.3. Lipschitz Continuity
- See
4.5.4. Directional Continuity
- The ((66926f42-20ef-4364-ba6e-be96b34f547c)) is equal to the function value.
4.5.4.1. Right-Continuous
4.5.4.2. Left-Continuous
4.5.5. Hölder Continuity
4.5.6. Semicontinuity
- See
5. Coordinate System
The coordinate system assigns numbers to each point, which is essential in doing analysis.
5.1. Orthogonal Coordinate System
5.1.1. Cartesian Coordinate System
5.1.2. Cylindrical Coordinate System
5.1.3. Elliptic Coordinate System
5.1.4. Hyperbolic Coordinates
5.2. Barycentric Coordinate System
5.3. Coordinate Systems for the Hyperbolic Plane
6. Implicit Function Theorem
6.1. Jacobian Matrix
6.2. Statement
- For a continuously differentiable function
, and a point with , - If the right-hand panel of the Jacobian
is invertible, then:- there exists an open set
containing - such that there exists a unique continuously differentiable function
- such that
, and for all . - And the Jacobian matrix of partial derivatives of
in is:
- there exists an open set
7. Triple Product Rule
- Cyclic Chain Rule, Cyclic Relation, Cyclical Rule, Euler's Chain Rule
7.1. Statement
- For three interdependent variables
:
7.2. Derivation
- The interdependence implies the existence of a implicit function
. - By the implicit function theorem :
- The same thing can be said for the others, yielding the formula.
8. Inverse Function Theorem
- Sufficient condition for a function to be invertible in a
neighborhood of a point.
- The derivative is continuous and non-zero at the point.
- Differentiability of
is hard to prove.- The partial derivative in the other direction might not exists, if the function is not invertible.
8.1. Statement
8.1.1. Single Variable
- For a continuously differentiable function
with nonzero derivative at the point , the is continuous differentiable near and the derivative is:
8.1.2. Multivariable
For a continuously differentiable function
There exist neighbourhoods
Furthermore, the inverse function
- Using the Jacobian:
8.2. Holomorphic Inverse Function Theorem
8.3. Inverse Function Rule
- The result of the inverse function theorem for the derivative of an inverse.
9. Differentiation
9.1. Differentiability
9.1.1. Weierstrass Function
The canonical example of function that is continuous everywhere but differentiable nowhere.
9.2. Faá di Bruno's Formula
- Generalized Chain Rule
9.2.1. Formula
where the sum is over all -tuple of nonnegative integers satisfying:- Equivalently:
where is the set of all partitions of the set .
9.3. Generalized Leibniz Rule
- Generalized Product Rule
9.3.1. Formula
9.4. Generalizations
9.4.1. Logarithmic Derivative
- The rate of relative change.
9.4.1.1. Definition
- Logarithmic derivative is defined as
- Still, the rules of logarithm are valid.
9.4.1.2. Properties
- It is invariant under scalar multiplication(dilation).
- By Faá di Bruno's formula,
- Note the case when
and .
- Note the case when
9.4.1.3. Operator Theory
Integrating factor of first order linear inhomogeneous differential eqaution is
found by integrating:
9.4.2. Partial Derivative
if the function is continuous. See Schwarz's theorem.- Continuous partial derivatives in every axis implies differentiability.
- Partial derivative is sensitive on the dependencies of variables, by the nature of multivariable function.
9.4.2.1. Totality
We can have arbitrary dependency of variables. Therefore proper restriction of the variable is necessary2:
- Functional Approach: Explicitly state the dependency within a
function.
- For a mathematicians things are all functions, and for a physicists things are all variables, from which the confusion arises.
- Equational Approach: additional notation for the restricted
variables.
Math Cnv. | Physics Cnv. | |
Total Ordinary | ||
Total Partial | ||
Inbetween | j |
|
Explicit Partial |
- Mathematicians assume total partial derivatives, and physicists
assume explicit partial derivatives.3
- Physicist also use the
for the total partial derivatives. For example, . - And mathematician needs use additional notation for explicit partials.
- Physicist also use the
- It might be disambiguating to use different symbol for total partial and explicit partial
9.4.2.2. Differentiability
- Partial Differentiable
- Locally Flat
where and converges to 0 at .
Partial differentiability does not guarantee the continuity, while (ordinary) differentiablility does implies continuity.
9.4.2.3. Schwarz's Theorem
- Clairaut's Theorem, Young's Theorem, Clairaut's Theorem on Equality of Mixed Partials
If a function
9.4.2.4. Total Differential
More commonly known as total derivative.
Best linear approximation of a function
See formalisms of dx.
9.4.3. Material Derivative
See material derivative.
9.4.4. Directional Derivative
9.4.6. Tensor Derivative
9.4.6.1. Derivatives
9.4.6.2. Gradient
In Cartesian coordinates,
This increases the order of tensor by one.
9.4.6.3. Divergence
In Cartesian coordinates, the divergence of second-order tensor
is typically taken to be,
9.4.6.4. Curl
In Cartesian coordinates, the curl of second-order tensor is,
9.4.7. Exterior Derivative
Derivative of the differential forms. See exterior derivative.
9.4.8. Covariant Derivative
Derivative on a manifold. See covariant derivative
9.4.9. Functional Derivative
9.4.9.1. Variational Derivative
9.4.9.1.1. Definition
Given a functional
The functional derivative
9.4.9.1.2. Interpretation
The infinite partial derivatives for each point
Intuitively, the Gateaux derivative can be thought of
as the total differential in infinitely many variables:
9.4.9.2. Pointwise Derivative
The function is now a set of infinitely many independent variables
parametrized by the argument.
It follows that
9.4.10. Gateaux Derivative
- / gatɔʊ /
- Generalization of the directional derivative
9.4.10.1. Definition
- For locally convex topological vector spaces
and , and , the Gateaux differential at in the direction is: - If the limit exists for all
, then is Gateaux differentiable at .
9.4.10.2. Properties
- It is homogeneous in the second variable:
- It can be defined, even though the function is not continuous.
- It formalizes the functional derivative used in the calculus of variations
9.4.11. Fréchet Derivative
- Generalization of the derivative
9.4.11.1. Defintion
- For normed vector space
and , a function is Fréchet differentiable at if there exists a bounded linear operator such that:
9.4.11.2. Properties
- If a function is Fréchet differentiable at
, it is Gateaux differentiable at . .
9.4.12. Hadamard Derivative
- Suited for stochastic programming and symptotic statistics.
9.4.12.1. Definition
- For Banach space
and , a map is Hadamrd-directionally differentiable at in the direction , if there exists a map such that: for all sequences and .
9.4.12.2. Properties
- If Hadamard directional derivative eixsts, then the Gateaux derivative also exists and the two derivatives coincide.
9.4.13. Lie Derivative
9.4.13.1. Definition
- Derivative of a tensor field along a vector field on a manifold.
9.4.13.1.1. Algebraic Definition
- Axiom 1.
- For a order-0 tensor field
:
- For a order-0 tensor field
- Axiom 2.
- Leibniz's Rule with respect to Tensor Product:
- For any tensor
over a manifold ,
- Axiom 3.
- Leibniz's Rule with respect to tensor contraction:
- Axiom 4.
- Commute with Exterior Derivative on Order-0 Tensor Field:
- Commute with Exterior Derivative on Order-0 Tensor Field:
9.4.13.2. Properties
- Set of vector fields form a Lie algebra with Lie derivative as the Lie bracket.
- For a vector field it is equivalent to
- where
is the covariant derivative
9.4.14. Arithmetic Derivative
9.4.15. Weak Derivative
- The integration by parts holds.
9.4.15.1. Definition
- For a function
in the Lebesgue space , in is called the weak derivative of if: for all infinitely differentiable functions with .
9.4.15.2. Examples
- The absolute value function
has a weak derivative, the sign function:
9.4.16. Schwarzian Derivative
9.4.16.1. Definition
9.4.16.2. Properties
- The Schwarzian derivative of a is zero.
- It is invariant under projective transformations.
10. Method of Lagrange Multipliers
- If a function
has local extremum at point under the constraint of then and the is called the Lagrange multiplier. - The local maximum of a function
under the constraint , when the Lagrangian has differential of zero .
11. Taylor Expansion
11.1. Derivation
11.1.1. By Fundamental Theorem of Calculus
For a smooth function
11.2. Taylor's Theorem
11.3. Lagrange Inversion Theorem
Also known as the Lagrange-Bürmann Formula. The formula for Taylor series expansion of the inverse function.
For a analytic function
12. Analytic Function
- The Subtle Reason Taylor Series Work | Smooth vs. Analytic Functions - YouTube
- Analyticity is the rare property.
- This is due to Taylor's theorem and the remainder is bounded for analytic function.
12.1. Definition
A function
12.2. Counterintuitive Examples
- Smooth but not analytic.
- Fabius function
- Another example
13. Holomorphic Function
13.1. Properties
- A holomorphic function is analytic.
- At all non-zero point, the tranfromation given by the function is conformal.
14. Integration
14.1. Definition (Riemann)
14.2. Formalisms of dx
Many definitions of the integral does not define what
14.2.1. Tangent Line
and is the tangential rise in the graph of the function.
14.2.2. Differential Form
14.2.3. Nonstandard Analysis
14.3. Generalizations
14.3.1. Darboux Integral
- Darboux Integral is frequently used instead of the Riemann integral, since Riemann's definition is not practical.
14.3.1.1. Definition
14.3.1.1.1. Darboux Sum
- Upper Darboux Sum
- Lower Darboux Sum
14.3.1.1.2. Darboux Integral
- Upper Darboux Integral
- Lower Darboux Integral
- If the upper and lower Darboux integral is the same, it is Darboux
integrable and the value is the Darboux integral.
14.3.1.2. Darboux Integrable
- The upper and lower integral are equal.
- It is equivalent to the Riemann integrability.
- Equivalently:
14.3.2. Riemann-Stieltjes Integral
- Stieltjes Integral
- Generalization of the Riemann integral.
- First published in 1894 by Stieltjes.
14.3.2.1. Definition
- An integral expression with respect to a function.
is the integrad and is the integrator.
14.3.2.2. Properties
- If
is differentiable, then the differential is equivalent to , thence yielding the ordinary integral.
14.3.2.3. Example
14.3.3. Lebesgue Integral
14.3.4. Bochner Integral
Extension of the multidimensional Lebesgue integral to functions that take values in a Banach space.
14.3.5. Iterated Integral
14.3.6. Multiple Integral
14.3.7. Cauchy Principal Value
The value for divergent integrals.
14.3.8. Hadamard Regularization
The value for divergent integrals.
15. Special Integrals
15.1. Elliptic Integral
15.2. Euler Integral
15.3. Gaussian Integral
15.4. Dirichlet Integral
15.5. Fresnel Integral
16. Cauchy Principal Value
16.1. Definition
Method for assigning values to certain improper integrals.
17. Legendre Transformation
17.1. Definition
For a differentiable function
This can be done on subset of variables. The variables participating in the transformation are called active variables, and the variables that are not are called passive variables.
17.2. Interpretation
The negative y-intercept in terms of the slope is the Legendre transformation.
18. Convolution
18.1. Definition
- For integrable function
and : - Note that this is also the case for the complex functions.
18.2. Properties
- Commutativity
- Associativity
- Distributivity
- It is multiplication within L1 space
, since: forming the algebra over .
18.3. Image Processing
- The kernel
is convolved with the image to produce the filtered image : - The kernel and the image are often represented with matrices.
19. Möbius Transformation
19.1. Definition
- For a complex number
the Möbius transformation is:- with a invertible matrix
- with a invertible matrix
19.2. Properties
- is one of the ingredients.
- Any Möbius map can be mapped to a rigid motion of the .
- It is the projective transformations of the complex projective line.
\[
\sim\]
- and forms the projective linear group
.
- The subgroup projective special linear group
is isomorphic to the ((66ade534-e14a-4d82-b5b9-e5a712e29779)) .
20. Interchange of Operations
20.1. Limits
20.2. Differentiations
20.3. Integrations
20.4. Integration with Limits or Infinite Series
20.5. Integration with Differentiation
21. Differential Operator
21.1. Total Symbol
- Replace the partials
by variables in the differential operator.
21.2. Principal Symbol
- The linear operator
on a smooth section of the vector bundles and of a manifold , is a differential operator of order if, in local coordinates of :- where
is a bundle map symmetric on the multi-indices .
- The
th order coefficients of transforms as a symmetric tensor:- where
is the th ((66e0ee31-071d-416a-a891-060ff6efd962)) of the cotangent bundle of .
- This symmetric tensor
is known as the principal symbol of . - The principal symbol is obtained by replacing the partials
by variables which is the covectors:
22. Hölder's Inequality
22.1. Statement
23. References
- dx, dy とは結局何なのか? - YouTube
- Cauchy sequence - Wikipedia
- Intermediate value theorem - Wikipedia
- Elliptic coordinate system - Wikipedia
- Hyperbolic coordinates - Wikipedia
- Coordinate systems for the hyperbolic plane - Wikipedia
- Symmetry of second derivatives - Wikipedia
- Determining the Speed of a Fixed-Point Iteration - YouTube
- Implicit function theorem - Wikipedia
- Triple product rule - Wikipedia
- Inverse function theorem - Wikipedia
- Faà di Bruno's formula - Wikipedia
- General Leibniz rule - Wikipedia
- Logarithmic differentiation - Wikipedia
- Logarithmic derivative - Wikipedia
- Total derivative - Wikipedia
- Directional derivative - Wikipedia
- Tensor derivative (continuum mechanics) - Wikipedia
- Gateaux derivative - Wikipedia
- Fréchet derivative - Wikipedia
- Hadamard derivative - Wikipedia
- what is the Gateaux derivative? - YouTube
- Lie derivative - Wikipedia
- Weak derivative - Wikipedia
- Schwarzian derivative - Wikipedia
- Lagrange multiplier - Wikipedia
- {짱박사 경제학} 라그랑지 접근법-최적화 문제 풀이 간편방법 - YouTube
- A better way to think about Taylor series #SoMEpi - YouTube
- Darboux integral - Wikipedia
- Why We Never Actually Learn Riemann's Original Definition of Integrals | Riem…
- Riemann–Stieltjes integral - Wikipedia
- Integral - Wikipedia
- Are These All of the Types of Integrals? - YouTube
- Cauchy principal value - Wikipedia
- Convolution - Wikipedia
- Kernel (image processing) - Wikipedia
- What if we define 1/0 = ∞? | Möbius transformations visualized - YouTube
- Möbius transformation - Wikipedia
- Differential operator - Wikipedia
- Hölder's inequality - Wikipedia