Description.
The Java String intern() method is used to retrieve the canonical representation for the current string object. In short, the intern() method is used to make an exact copy of a String in heap memory and store it in the String constant pool. A pool is a special storage space in Java heap memory where the string literals can be stored.
A canonical representation indicates that values of a specific type of resource can be described or represented in multiple ways, with one of those ways are chosen as the preferred canonical form.
Note − The equality of two objects can easily be tested by testing the equality of their canonical forms.
Following is the syntax of the Java String intern() method −
It does not accept any parameter.
This method returns a canonical representation for the string object.
If the given string is not null , the intern() method creates the same copy of the current string object in the heap memory.
In the following program, we are instantiating the string class with the value "TutorialsPoint" . Using the intern() method, we are trying to create an exact copy of the current string in the heap memory.
On executing the above program, it will produce the following result −
If the given string has a null value , the intern() method throws the NullPointerException .
In the following example, we are creating a string literal with the null value . Using the intern() method, we are trying to retrieve the canonical representation of the current string object.
Following is the output of the above program −
Using the intern() method we can check the equality of the string objects based on their conical forms.
In this program, we are creating an object of the string class with the value "Hello" . Then, using the intern() method, we are trying to retrieve the canonical representation of the string object, and compare them using the equals() method.
The above program, produces the following output −
To Continue Learning Please Login
www.springer.com The European Mathematical Society
2020 Mathematics Subject Classification: Primary: 60E07 Secondary: 60G51 [ MSN ][ ZBL ]
A formula for the logarithm $ \mathop{\rm ln} \phi ( \lambda ) $ of the characteristic function of an infinitely-divisible distribution :
$$ \mathop{\rm ln} \phi ( \lambda ) = i \gamma \lambda - \frac{\sigma ^ {2} \lambda ^ {2} }{2} + \int\limits _ {- \infty } ^ { 0 } \left ( e ^ {i \lambda x } - 1 - \frac{i \lambda x }{1 + x ^ {2} } \right ) \ d M ( x) + $$
$$ + \int\limits _ { 0 } ^ \infty \left ( e ^ {i \lambda x } - 1 - \frac{i \lambda x }{1 + x ^ {2} } \right ) d N ( x) , $$
where the characteristics of the Lévy canonical representation, $ \gamma $, $ \sigma ^ {2} $, $ M $, and $ N $, satisfy the following conditions: $ - \infty < \gamma < \infty $, $ \sigma ^ {2} \geq 0 $, and $ M ( x) $ and $ N ( x) $ are non-decreasing left-continuous functions on $ ( - \infty , 0 ) $ and $ ( 0 , \infty ) $, respectively, such that
$$ \lim\limits _ {x \rightarrow \infty } \ N ( x) = \lim\limits _ {x \rightarrow - \infty } \ M ( x) = 0 $$
$$ \int\limits _ { - 1} ^ { 0 } x ^ {2} d M ( x) < \infty ,\ \ \int\limits _ { 0 } ^ { 1 } x ^ {2} d N ( x) < \infty . $$
To every infinitely-divisible distribution there corresponds a unique system of characteristics $ \gamma $, $ \sigma ^ {2} $, $ M $, $ N $ in the Lévy canonical representation, and conversely, under the above conditions on $ \gamma $, $ \sigma ^ {2} $, $ M $, and $ N $ the Lévy canonical representation with respect to such a system determines the logarithm of the characteristic function of some infinitely-divisible distribution.
Thus, for the normal distribution with mean $ a $ and variance $ \sigma ^ {2} $:
$$ \gamma = a ,\ \sigma ^ {2} = \sigma ^ {2} ,\ \ N ( x) \equiv 0 ,\ M ( x) \equiv 0 . $$
For the Poisson distribution with parameter $ \lambda $:
$$ \gamma = \frac \lambda {2} ,\ \ \sigma ^ {2} = 0 ,\ \ M ( x) \equiv 0 ,\ \ N ( x) = \left \{ \begin{array}{rl} - \lambda & \textrm{ for } x \leq 1 , \\ 0 & \textrm{ for } x > 1 . \\ \end{array} \right .$$
To the stable distribution with exponent $ \alpha $, $ 0 < \alpha < 2 $, corresponds the Lévy representation with
$$ \sigma ^ {2} = 0 ,\ \ \textrm{ any } \ \gamma ,\ M ( x) = \frac{c _ {1} }{| x | ^ \alpha } ,\ \ N ( x) = - \frac{c _ {2} }{x ^ \alpha } , $$
where $ c _ {i} \geq 0 $, $ i = 1 , 2 $, are constants $ ( c _ {1} + c _ {2} > 0 ) $. The Lévy canonical representation of an infinitely-divisible distribution was proposed by P. Lévy in 1934. It is a generalization of a formula found by A.N. Kolmogorov in 1932 for the case when the infinitely-divisible distribution has finite variance. For $ \mathop{\rm ln} \phi ( \lambda ) $ there is a formula equivalent to the Lévy canonical representation, proposed in 1937 by A.Ya. Khinchin and called the Lévy–Khinchin canonical representation . The probabilistic meaning of the functions $ N $ and $ M $ and the range of applicability of the Lévy canonical representation are defined as follows: To every infinitely-divisible distribution function $ F $ corresponds a stochastically-continuous process with stationary independent increments
$$ X = \{ {X ( t) } : {0 \leq t < \infty } \} ,\ X ( 0) = 0 , $$
$$ F ( X) = {\mathsf P} \{ X ( 1) < x \} . $$
In turn, a separable process $ X $ of the type mentioned has with probability 1 sample trajectories without discontinuities of the second kind; hence for $ b > a > 0 $ the random variable $ Y ( [ a , b ) ) $ equal to the number of elements in the set
$$ \left \{ {t } : {a \leq \lim\limits _ {\tau \downarrow 0 } \ X ( t + \tau ) - \lim\limits _ {\tau \downarrow 0 } \ X ( t - \tau ) < b , 0 \leq t \leq 1 } \right \} , $$
i.e. to the number of jumps with heights in $ [ a , b ) $ on the interval $ [ 0 , 1 ] $, exists. In this notation, one has for the function $ N $ corresponding to $ F $,
$$ {\mathsf E} \{ Y ( [ a , b ) ) \} = N ( b) - N ( a) . $$
A similar relation holds for the function $ M $.
Many properties of the behaviour of the sample trajectories of a separable process $ X $ can be expressed in terms of the characteristics of the Lévy canonical representation of the distribution function $ {\mathsf P} \{ X ( 1) < x \} $. In particular, if $ \sigma ^ {2} = 0 $,
$$ \lim\limits _ {x \rightarrow 0 } N ( x) > - \infty ,\ \ \lim\limits _ {x \rightarrow 0 } M ( x) < \infty , $$
$$ \gamma = \int\limits _ {- \infty } ^ { 0 } \frac{x}{1 + x ^ {2} } d M ( x) + \int\limits _ { 0 } ^ \infty \frac{x}{1 + x ^ {2} } d N ( x) , $$
then almost-all the sample functions of $ X $ are with probability 1 step functions with finitely many jumps on any finite interval. If $ \sigma ^ {2} = 0 $ and if
$$ \int\limits _ { - 1} ^ { 0 } | x | d M ( x) + \int\limits _ { 0 } ^ { 1 } x d N ( x) < \infty , $$
then with probability 1 the sample trajectories of $ X $ have bounded variation on any finite interval. Directly in terms of the characteristics of the Lévy canonical representation one can calculated the infinitesimal operator corresponding to the process $ X $, regarded as a Markov random function. Many analytical properties of an infinitely-divisible distribution function can be expressed directly in terms of the characteristics of its Lévy canonical representation.
There are analogues of the Lévy canonical representation for infinitely-divisible distributions given on a wide class of algebraic structures.
[GK] | B.V. Gnedenko, A.N. Kolmogorov, "Limit distributions for sums of independent random variables" , Addison-Wesley (1954) (Translated from Russian) |
[Pe] | V.V. Petrov, "Sums of independent random variables" , Springer (1975) (Translated from Russian) |
[PR] | Yu.V. [Yu.V. Prokhorov] Prohorov, Yu.A. Rozanov, "Probability theory, basic concepts. Limit theorems, random processes" , Springer (1969) (Translated from Russian) |
[GS] | I.I. [I.I. Gikhman] Gihman, A.V. [A.V. Skorokhod] Skorohod, "The theory of stochastic processes" , , Springer (1975) (Translated from Russian) |
[I] | K. Itô, "Stochastic processes" , Aarhus Univ. (1969) |
[Lo] | M. Loève, "Probability theory" , , Springer (1977) |
[B] | L.P. Breiman, "Probability" , Addison-Wesley (1968) |
[Lu] | E. Lukacs, "Characteristic functions" , Griffin (1970) |
[H] | H. Heyer, "Probability measures on locally compact groups" , Springer (1977) |
[Pa] | K.R. Parthasarathy, "Probability measures on metric spaces" , Acad. Press (1967) |
[GK2] | B.V. Gnedenko, A.N. Kolmogorov, "Introduction to the theory of random processes" , Saunders (1969) (Translated from Russian) |
Stack Exchange network consists of 183 Q&A communities including Stack Overflow , the largest, most trusted online community for developers to learn, share their knowledge, and build their careers.
Q&A for work
Connect and share knowledge within a single location that is structured and easy to search.
We had our Digital Systems class today, and our professor kept throwing around the word 'canonical' around a whole lot, but I'm very confused as to what this is.
What I understood is that it's the way of representing an expression uniquely (i.e., two non-equivalent functions cannot have the same canonical form) Is my interpretation correct.
So would Sum of Minterms be canonical or not? If we simplify the SoM form, would it still be canonical?
Canonical form basically holds every variable in its group.
So if you have three variables named A, B and C, your SoM could be A~BC+~ABC+AB~C = Y .
Now you can simplify this to reduce the number of variables in the equation. This simplification is easy for us to solve manually. But for a computer, it needs to know the A, B and C values as a group ( 101+011+110 from the example above). Because of this, canonical form holds significance.
If you simplify, it just becomes a normal Boolean expression and not a canonical form
So would Sum of Minterms be canonical or not?
When Sum of Products is in its canonical form, it is called 'Sum of Minterms'. Similarly, Product of Sums in its canonical form is called 'Product of Max terms'.
So yes, SoM is canonical.
For a Boolean equation to be in canonical form means that all the terms in it contain all the variables, irrespective of whether a variable in a term is inverted or not.
For example, you have 3 variables (p, q, r) and a function f = p’qr + pq’r + pqr’ + pqr
Here the equation is in canonical form and its simplified form (standard form), after carrying out simplification is, f = pq + qr + pr
Sign up or log in, post as a guest.
Required, but never shown
By clicking “Post Your Answer”, you agree to our terms of service and acknowledge you have read our privacy policy .
Hot network questions.
Each type in a 5800 system has a canonical representation as a string value. The canonical string representation of each type is shown in Table 4–1 .
Data Type | Canonical String Representation |
---|---|
| The string itself. |
| The string itself. |
| Hexadecimal dump of the value with two hex digits per byte. |
| Result of . For example, or . |
| Result of . For example, or or or . |
| . For example, |
| . For example, . |
| (time relative to UTC). For example, . |
| 60-digit hexadecimal dump of the |
This canonical string encoding is used in the following places:
When exposing the field as a directory component or a filename component in a virtual view
When converting a typed value to a string as the result of the getAsString operation on a NameValueRecord or a QueryResultSet operation
When parsing a literal value as described in Literals for 5800 System Data Types to create a typed query value from a string representation of that value.
The inverse of the canonical string encoding is used in the following places:
It is always allowed to store a string value into any metadata field, no matter what the type of the field is. The actual data stored is the result of applying the canonical string decode operation to the incoming string value.
On a virtual view lookup operation, the canonical string decode operation is used on the supplied filename to derive the actual metadata values to look up, given their string representations in the filename.
The decode operation is allowed to accept incoming string values that would never be a legal output for an encode operation. Some examples of this include:
decodeBinary of an odd number of hex digits. The convention is to left-justify the supplied digits in the binary value. For example, the string "b0a" corresponds to the binary literal [b0a0] .
decodeDate of a non-standard date format.
A double value encoded with a non-canonical number of digits. For example, .00145E20 instead of 1.45E17 .
If you take a value V and encode it into a string S , and then perform the canonical decode operation on S to get a new value V’ . Does V always equal V’ ? The answer is yes in most cases, but not always.
What is actually guaranteed is the weaker statement that if encode(V) = S and if decode(S)=V’ , then encode(V’) is also equal to S .
Part of the book series: Lecture Notes in Control and Information Sciences ((LNCIS,volume 152))
1876 Accesses
This is a preview of subscription content, log in via an institution to check access.
Institutional subscriptions
Unable to display preview. Download preview PDF.
Rights and permissions.
Reprints and permissions
© 1991 Springer-Verlag
(1991). Canonical representations. In: Aplevich, J.D. (eds) Implicit Linear Systems. Lecture Notes in Control and Information Sciences, vol 152. Springer, Berlin, Heidelberg. https://doi.org/10.1007/BFb0044368
DOI : https://doi.org/10.1007/BFb0044368
Published : 20 January 2006
Publisher Name : Springer, Berlin, Heidelberg
Print ISBN : 978-3-540-53537-9
Online ISBN : 978-3-540-46759-5
eBook Packages : Springer Book Archive
Anyone you share the following link with will be able to read this content:
Sorry, a shareable link is not currently available for this article.
Provided by the Springer Nature SharedIt content-sharing initiative
Policies and ethics
Stack Exchange network consists of 183 Q&A communities including Stack Overflow , the largest, most trusted online community for developers to learn, share their knowledge, and build their careers.
Q&A for work
Connect and share knowledge within a single location that is structured and easy to search.
Let $p$ be an arbitrary point on the unit sphere $$ S = \{(x,y,z) \mid x^2+y^2+z^2 = 1 \},$$ other than the north or south poles $(0,0,\pm 1)$.
There is a one-dimensional family of rotations which take $n = (0,0,1)$ to $p$, but one rotation is canonical: the one that keeps $n$, $p$, and $0$ in a plane. In other words the cross product $u = n \times p$ should be an axis of rotation.
Is there a nice way to write down the matrix $M \in SO(3)$ for this canonical rotation?
I observe that we have three equations: (1) $M^T M = I$, (2) $M n = p$, and (3) $M u = u $.
Since I want $M \in SO(3)$ rather than simply $M \in O(3)$ we also have $\det M = 1$.
This should be enough to determine $M$, but I still don't see an obvious way to write down a formula.
Let the point $p$ be given in cartesian coordinates by $(\sin\theta\cos\phi, \sin\theta\sin\phi, \cos\phi)$, so that $\theta$ and $\phi$ are the usual spherical coordinates on $S^2$. Then the matrix that rotates $n=(1,0,0)$ to $p$, and also preserves the plane passing through both of them and the origin, is given by
$M=\left(\begin{array}{ccc}\sin^2\phi + \cos\theta\cos^2\phi & (-1+\cos\theta)\sin\phi\cos\phi & \sin\theta\cos\phi\\ (-1+\cos\theta)\sin\phi\cos\phi & \cos^2\phi+\cos\theta\sin^2\phi & \sin\theta\sin\phi\\ -\sin\theta\cos\phi & -\sin\theta\sin\phi & \cos\theta \end{array}\right).$
It's straightforward but tedious to check that this is indeed an orthogonal matrix with determinant $1$ that sends $n$ to $p$ and fixes $u=n\times p=(-\sin\theta\sin\phi,\sin\theta\cos\phi,0)$, and hence the desired transformation.
I produced this matrix by considering that, for each fixed $\phi$, what you desire is a one-parameter subgroup of $SO(3)$: the group of rotations that fix $u$. It therefore is the family of exponentials of an infinitesimal transformation, i.e. an element of the Lie algebra $\frak{so}\mathrm{(3)}$. For example, a tiny rotation tilting the $z$-axis toward the $x$-axis differs from the identity by $\left(\begin{array}{ccc} & & \epsilon\\ & & \\ -\epsilon & & \end{array}\right)$, and $\exp\left(\begin{array}{ccc} & & \theta\\ & & \\ -\theta & & \end{array}\right) = \left(\begin{array}{ccc} \cos\theta & & \sin\theta\\ & 1 & \\ -\sin\theta & & \cos\theta \end{array}\right).$
Similarly, the Lie algebra element corresponding to an infinitesimal rotation of the $z$-axis in the direction of the $y$-axis is given by $\left(\begin{array}{ccc} & & \\ & & \epsilon\\ & -\epsilon& \end{array}\right)$, and $\exp\left(\begin{array}{ccc} & & \\ & & \theta\\ & -\theta & \end{array}\right) = \left(\begin{array}{ccc} 1 & & \\ & \cos\theta & \sin\theta\\ & -\sin\theta & \cos\theta \end{array}\right).$
We want the Lie algebra element which has components $\cos\phi$ toward the $x$-axis and $\sin\phi$ toward the $y$-axis; thus we desire the exponential $M=\exp\left(\begin{array}{ccc} & & \theta\cos\phi\\ & & \theta\sin\phi\\ -\theta\cos\phi & -\theta\sin\phi & \end{array}\right)=\exp(A).$
This matrix $A$ is diagonalizable, so its exponential $M$ can be computed by hand, which is how I arrived at my answer above.
Not the answer you're looking for browse other questions tagged linear-algebra rotations ., hot network questions.
Help | Advanced Search
Title: canonicalizing zeta generators: genus zero and genus one.
Abstract: Zeta generators are derivations associated with odd Riemann zeta values that act freely on the Lie algebra of the fundamental group of Riemann surfaces with marked points. The genus-zero incarnation of zeta generators are Ihara derivations of certain Lie polynomials in two generators that can be obtained from the Drinfeld associator. We characterize a canonical choice of these polynomials, together with their non-Lie counterparts at even degrees $w\geq 2$, through the action of the dual space of formal and motivic multizeta values. Based on these canonical polynomials, we propose a canonical isomorphism that maps motivic multizeta values into the $f$-alphabet. The canonical Lie polynomials from the genus-zero setup determine canonical zeta generators in genus one that act on the two generators of Enriquez' elliptic associators. Up to a single contribution at fixed degree, the zeta generators in genus one are systematically expanded in terms of Tsunogai's geometric derivations dual to holomorphic Eisenstein series, leading to a wealth of explicit high-order computations. Earlier ambiguities in defining the non-geometric part of genus-one zeta generators are resolved by imposing a new representation-theoretic condition. The tight interplay between zeta generators in genus zero and genus one unravelled in this work connects the construction of single-valued multiple polylogarithms on the sphere with iterated-Eisenstein-integral representations of modular graph forms.
Comments: | 92 pages. Submission includes ancillary data files |
Subjects: | Quantum Algebra (math.QA); High Energy Physics - Phenomenology (hep-ph); High Energy Physics - Theory (hep-th); Algebraic Geometry (math.AG); Number Theory (math.NT) |
Report number: | UUITP-16/24 |
Cite as: | [math.QA] |
(or [math.QA] for this version) |
Access paper:.
Code, data and media associated with this article, recommenders and search tools.
arXivLabs is a framework that allows collaborators to develop and share new arXiv features directly on our website.
Both individuals and organizations that work with arXivLabs have embraced and accepted our values of openness, community, excellence, and user data privacy. arXiv is committed to these values and only works with partners that adhere to them.
Have an idea for a project that will add value for arXiv's community? Learn more about arXivLabs .
Data-driven three-dimensional (3D) mineral prospectivity modeling (MPM) employs diverse 3D exploration indicators to express geological architecture and associated characteristics in ore systems. The integration of 3D geological models with 3D computational simulation data enhances the effectiveness of 3D MPM in representing the geological architecture and its coupled geodynamic processes that govern mineralization. Despite variations in modality (i.e., data source, representation, and information abstraction levels) between geological models and simulation data, the cross-modal gap between these two types of data remains underexplored in 3D MPM. This paper presents a novel 3D MPM approach that robustly fuses multimodal information from geological models and simulation data. Acknowledging the coupled and correlated nature of geological architectures and geodynamic processes, a joint fusion strategy is employed, aligning information from both modalities by enforcing their correlation. A joint fusion neural network is devised to extract maximally correlated features from geological models and simulation data, fusing them in a cross-modality feature space. Specifically, correlation analysis (CCA) regularization is utilized to maximize the correlation between features of the two modalities, guiding the network to learn coordinated and joint fused features associated with mineralization. This results in a more effective 3D mineral prospectivity model that harnesses the strengths from both modalities for mineral exploration targeting. The proposed method is evaluated in a case study of the world-class Jiaojia gold deposit, NE China. Extensive experiments were carried out to compare the proposed method with state-of-the-art methods, methods using unimodal data, and variants without CCA regularization. Results demonstrate the superior performance of the proposed method in terms of prediction accuracy and targeting efficacy, highlighting the importance of CCA regularization in enhancing predictive power in 3D MPM.
IMAGES
VIDEO
COMMENTS
A canonical form means that values of a particular type of resource can be described or represented in multiple ways, and one of those ways is chosen as the favored canonical form. (That form is canonized, like books that made it into the bible, and the other forms are not.) A classic example of a canonical form is paths in a hierarchical file ...
The canonical form of a positive integer in decimal representation is a finite sequence of digits that does not begin with zero. More generally, for a class of objects on which an equivalence relation is defined, a canonical form consists in the choice of a specific object in each class. For example:
A representation r: p 1(C f x 1,. . ., xn)) !GLr(C) is canonical if there is a finite index subgroup of p 1(Mg,n) preserving the conjugacy class of r. Remark 4.2. Observe that any finite image representation is canonical be-cause the finitely many generators can only map to finitely many elements
My textbook (Saurabh's Introduction to VLSI Design Flow) mentions while discussing formal verification that a representation of a Boolean function is said to be canonical if the following holds:. If a representation is canonical, then the two functionally equivalent functions are represented identically. Conversely, if a representation is canonical and if two functions have the same ...
So the distribution determines the value of the variables ( γ γ and G G in the example) appearing in the expression of what the canonical representation should look like. A better known example of the same use of 'canonical' is the Jordan Canonical Form of a linear transformation. Yes, for every linear transformation there are many equivalent ...
1. The canonical or diagonal form of A is a diagonal matrix D with the eigenvalues of A on the main diagonal. If the columns of E contain the eigenvectors of A, D is the matrix that satisfies that: AE = ED A E = E D. Share. Cite. Follow. edited Apr 1, 2023 at 10:05. answered Apr 1, 2023 at 9:58.
The Basic Idea. This post is intended to be a hopefully-not-too-intimidating summary of the rational canonical form (RCF) of a linear transformation. Of course, anything which involves the word "canonical" is probably intimidating no matter what. But even so, I've attempted to write a distilled version of the material found in (the first half ...
There is a formula for finding the sum of divisors of a given number. If n = p 1k1 xp 2k2 x …x p mkm is the canonical representation of a number n then the sum of positive divisors of n is given by. Example: 2000 = 2 4 x 5 3. Sum of positive divisors of 2000 = [2 5 -1/2-1] [5 4 -1/5-1] = [31/1] x [624/4] = 31 x 156 = 4836.
Tour Start here for a quick overview of the site Help Center Detailed answers to any questions you might have Meta Discuss the workings and policies of this site
Advantages of Canonical Form: Uniqueness: The canonical form of a boolean function is unique, which means that there is only one possible canonical form for a given function. Clarity: The canonical form of a boolean function provides a clear and unambiguous representation of the function.
a canonical representation for idioms that amounts to a full structural description for the literal reading of the sentence. Then the Stage 1 procedure, which rewrites the parser output into logical assertions, uses an idiom dictionary to produce separate sets of assertions for the idiomatic and literal read- ...
uniqueness of the scale as determined by a canonical representation. Much more important and much more difficult is the question as to which properties a function must have in order that it can be transformed into a canonical function. The conditions depend, of course, on the type of the function H used for the canonical representation.
The canonical representation' states that any causal wavelet w can be represented as the convolution of its minimum-phase counterpart and a causal all-pass wavelet p; that is, ( 58) Because the inverse of a minimum-phase wavelet is minimum phase, it follows that is minimum phase and hence is causal. From the canonical representation, we see ...
Description. The Java String intern() method is used to retrieve the canonical representation for the current string object. In short, the intern() method is used to make an exact copy of a String in heap memory and store it in the String constant pool. A pool is a special storage space in Java heap memory where the string literals can be stored. A canonical representation indicates that ...
The Lévy canonical representation of an infinitely-divisible distribution was proposed by P. Lévy in 1934. It is a generalization of a formula found by A.N. Kolmogorov in 1932 for the case when the infinitely-divisible distribution has finite variance. For $ \mathop {\rm ln} \phi ( \lambda ) $ there is a formula equivalent to the Lévy ...
Canonical form basically holds every variable in its group. So if you have three variables named A, B and C, your SoM could be A~BC+~ABC+AB~C = Y. Now you can simplify this to reduce the number of variables in the equation. This simplification is easy for us to solve manually. But for a computer, it needs to know the A, B and C values as a ...
The actual data stored is the result of applying the canonical string decode operation to the incoming string value. On a virtual view lookup operation, the canonical string decode operation is used on the supplied filename to derive the actual metadata values to look up, given their string representations in the filename.
Canonical Form; Canonical Representation; Canonical System; Canonical Parameter; Echelon Form; These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.
We might even allow equivalence classes to have more than one canonical representative. Solving the problem for all canonical representatives nevertheless still amounts to solving the problem for all objects. As another example, consider Latin squares. The Latin square $$\begin{bmatrix} A & B & C \\ C & A & B \\ B & C & A \\ \end{bmatrix}$$ and ...
exp( θ − θ) = (1 cosθ sinθ − sinθ cosθ). We want the Lie algebra element which has components cosϕ toward the x -axis and sinϕ toward the y -axis; thus we desire the exponential. M = exp( θcosϕ θsinϕ − θcosϕ − θsinϕ) = exp(A). This matrix A is diagonalizable, so its exponential M can be computed by hand, which is how I ...
The canonical Lie polynomials from the genus-zero setup determine canonical zeta generators in genus one that act on the two generators of Enriquez' elliptic associators. Up to a single contribution at fixed degree, the zeta generators in genus one are systematically expanded in terms of Tsunogai's geometric derivations dual to holomorphic ...
Canonical form is a term commonly used among computer scientists and statisticians to represent any mathematical object that has been reduced down as far as possible into a mathematical expression. The distinction between "canonical" and "normal" forms varies from subfield to subfield, however in most representations the canonical ...
Data-driven three-dimensional (3D) mineral prospectivity modeling (MPM) employs diverse 3D exploration indicators to express geological architecture and associated characteristics in ore systems. The integration of 3D geological models with 3D computational simulation data enhances the effectiveness of 3D MPM in representing the geological architecture and its coupled geodynamic processes that ...