9869:
7521:
7053:
6477:-dimensions. In other words, the discrete Laplacian filter of any size can be generated conveniently as the sampled Laplacian of Gaussian with spatial size befitting the needs of a particular application as controlled by its variance. Monomials which are non-linear operators can also be implemented using a similar reconstruction and approximation approach provided that the signal is sufficiently over-sampled. Thereby, such non-linear operators e.g.
32:
8465:
4135:
7516:{\displaystyle {\begin{aligned}{\frac {d\phi _{i}}{dt}}&=-k\sum _{j}A_{ij}\left(\phi _{i}-\phi _{j}\right)\\&=-k\left(\phi _{i}\sum _{j}A_{ij}-\sum _{j}A_{ij}\phi _{j}\right)\\&=-k\left(\phi _{i}\ \deg(v_{i})-\sum _{j}A_{ij}\phi _{j}\right)\\&=-k\sum _{j}\left(\delta _{ij}\ \deg(v_{i})-A_{ij}\right)\phi _{j}\\&=-k\sum _{j}\left(L_{ij}\right)\phi _{j}.\end{aligned}}}
5078:
7963:
1767:
3866:
5465:
4326:
3675:
9251:
9859:
converges to the same value at each of the vertices of the graph, which is the average of the initial values at all of the vertices. Since this is the solution to the heat diffusion equation, this makes perfect sense intuitively. We expect that neighboring elements in the graph will exchange energy
4140:
for γ ∈ is compatible with discrete scale-space properties, where specifically the value γ = 1/3 gives the best approximation of rotational symmetry. Regarding three-dimensional signals, it is shown that the
Laplacian operator can be approximated by the two-parameter family of difference operators
6327:
2414:
In this approach, the domain is discretized into smaller elements, often triangles or tetrahedra, but other elements such as rectangles or cuboids are possible. The solution space is then approximated using so called form-functions of a pre-defined degree. The differential equation containing the
9872:
This GIF shows the progression of diffusion, as solved by the graph laplacian technique. A graph is constructed over a grid, where each pixel in the graph is connected to its 8 bordering pixels. Values in the image then diffuse smoothly to their neighbors over time via these connections. This
2427:
and calculated as sum of differences over the nearest neighbours of the central pixel. Since derivative filters are often sensitive to noise in an image, the
Laplace operator is often preceded by a smoothing filter (such as a Gaussian filter) in order to remove the noise before calculating the
9901:
The complete Matlab source code that was used to generate this animation is provided below. It shows the process of specifying initial conditions, projecting these initial conditions onto the eigenvalues of the
Laplacian Matrix, and simulating the exponential decay of these projected initial
9897:
diffusing over time through a graph. The graph in this example is constructed on a 2D discrete grid, with points on the grid connected to their eight neighbors. Three initial points are specified to have a positive value, while the rest of the values in the grid are zero. Over time, the
4597:
8460:{\displaystyle {\begin{aligned}0={}&{\frac {d\left(\sum _{i}c_{i}(t)\mathbf {v} _{i}\right)}{dt}}+kL\left(\sum _{i}c_{i}(t)\mathbf {v} _{i}\right)\\{}={}&\sum _{i}\left\\{}={}&\sum _{i}\left\\\Rightarrow 0={}&{\frac {dc_{i}(t)}{dt}}+k\lambda _{i}c_{i}(t),\\\end{aligned}}}
5601:. In particular any discrete image, with reasonable presumptions on the discretization process, e.g. assuming band limited functions, or wavelets expandable functions, etc. can be reconstructed by means of well-behaving interpolation functions underlying the reconstruction formulation,
1560:
2785:
4130:{\displaystyle \nabla _{\gamma }^{2}=(1-\gamma )\nabla _{5}^{2}+\gamma \nabla _{\times }^{2}=(1-\gamma ){\begin{bmatrix}0&1&0\\1&-4&1\\0&1&0\end{bmatrix}}+\gamma {\begin{bmatrix}1/2&0&1/2\\0&-2&0\\1/2&0&1/2\end{bmatrix}}}
4591:
11233:
1200:
6799:
11542:
are on the extended (affine) ADE Dynkin diagrams, of which there are 2 infinite families (A and D) and 3 exceptions (E). The resulting numbering is unique up to scale, and if the smallest value is set at 1, the other numbers are integers, ranging up to 6.
6448:
domain but also an effective range in the frequency domain (alternatively
Gaussian scale space) which can be controlled explicitly via the variance of the Gaussian in a principled manner. The resulting filtering can be implemented by separable filters and
3852:
2627:
5084:
9578:
3273:
3363:
3180:
7628:
4147:
2176:
3522:
2998:
3078:
2915:
2415:
Laplace operator is then transformed into a variational formulation, and a system of equations is constructed (linear or eigenvalue problems). The resulting matrices are usually very sparse and can be solved with iterative methods.
9113:
9833:
2673:) finite-difference formula seen previously. It is stable for very smoothly varying fields, but for equations with rapidly varying solutions a more stable and isotropic form of the Laplacian operator is required, such as the
807:
2518:
3740:
D version, which is based on the graph generalization of the
Laplacian, assumes all neighbors to be at an equal distance, and hence leads to the following 2D filter with diagonals included, rather than the version above:
8884:
5073:{\displaystyle (\nabla _{+^{3}}^{2}f)_{0,0,0}={\frac {1}{4}}(f_{-1,-1,0}+f_{-1,+1,0}+f_{+1,-1,0}+f_{+1,+1,0}+f_{-1,0,-1}+f_{-1,0,+1}+f_{+1,0,-1}+f_{+1,0,+1}+f_{0,-1,-1}+f_{0,-1,+1}+f_{0,+1,-1}+f_{0,+1,+1}-12f_{0,0,0}),}
991:
1762:{\displaystyle C_{ij}={\begin{cases}{\frac {1}{2}}(\cot \alpha _{ij}+\cot \beta _{ij})&ij{\text{ is an edge, that is }}j\in N(i),\\-\sum \limits _{k\in N(i)}C_{ik}&i=j,\\0&{\text{otherwise}}\end{cases}}}
5697:
5911:
6131:
6616:). This may also be seen by applying the Fourier transform. Note that the discrete Laplacian on an infinite grid has purely absolutely continuous spectrum, and therefore, no eigenvalues or eigenfunctions.
3516:
11472:
7844:
2684:
498:
2331:
7920:
9655:
8558:
6352:. An advantage of using Gaussians as interpolation functions is that they yield linear operators, including Laplacians, that are free from rotational artifacts of the coordinate frame in which
1001:
In addition to considering the connectivity of nodes and edges in a graph, mesh
Laplace operators take into account the geometry of a surface (e.g. the angles at the nodes). For a two-dimensional
6042:
7968:
7537:
7058:
9072:
1484:
7689:
6628:, then this definition of the Laplacian can be shown to correspond to the continuous Laplacian in the limit of an infinitely fine grid. Thus, for example, on a one-dimensional grid we have
4337:
2423:
Discrete
Laplace operator is often used in image processing e.g. in edge detection and motion estimation applications. The discrete Laplacian is defined as the sum of the second derivatives
11138:
3440:
11319:
1055:
11035:
8988:
6634:
5460:{\displaystyle (\nabla _{\times ^{3}}^{2}f)_{0,0,0}={\frac {1}{4}}(f_{-1,-1,-1}+f_{-1,-1,+1}+f_{-1,+1,-1}+f_{-1,+1,+1}+f_{+1,-1,-1}+f_{+1,-1,+1}+f_{+1,+1,-1}+f_{+1,+1,+1}-8f_{0,0,0}).}
3748:
8594:
are non-negative, showing that the solution to the diffusion equation approaches an equilibrium, because it only exponentially decays or remains constant. This also shows that given
2526:
10937:
2828:
11590:
2667:
9486:
668:
11529:
5553:
9873:
particular image starts off with three strong point values which spill over to their neighbors slowly. The whole system eventually settles out to the same value at equilibrium.
331:
3185:
1529:
629:
6985:
3278:
3095:
9327:
9356:
8805:
7955:
7783:
6124:
5511:
4321:{\displaystyle \nabla _{\gamma _{1},\gamma _{2}}^{2}=(1-\gamma _{1}-\gamma _{2})\,\nabla _{7}^{2}+\gamma _{1}\,\nabla _{+^{3}}^{2}+\gamma _{2}\,\nabla _{\times ^{3}}^{2}),}
7532:
1273:
840:
591:
11263:
11070:
9105:
6527:
1303:
6446:
5733:
8619:
8588:
1992:
1950:
11384:
9428:
eigenvectors of ones and zeros, where each connected component corresponds to an eigenvector with ones at the elements in the connected component and zeros elsewhere.
7727:
5800:
9426:
3670:{\displaystyle a_{x_{1},x_{2},\dots ,x_{n}}=\left\{{\begin{array}{ll}-2n&{\text{if }}s=n,\\1&{\text{if }}s=n-1,\\0&{\text{otherwise,}}\end{array}}\right.}
869:
359:
259:
11364:
9685:
6881:
5579:
536:
10965:
8776:
8747:
8698:
8655:
6397:
1911:
1353:
568:
379:
6062:
5931:
1798:
2360:) on the boundary of the lattice grid, thus this is the case of no source at the boundary, that is, a no-flux boundary condition (aka, insulation, or homogeneous
9895:
9857:
9705:
9246:{\displaystyle \lim _{t\to \infty }e^{-k\lambda _{i}t}={\begin{cases}0,&{\text{if}}&\lambda _{i}>0\\1,&{\text{if}}&\lambda _{i}=0\end{cases}}}
7754:
6850:
1326:
9458:
6547:
6475:
6417:
6370:
6350:
6086:
5955:
5820:
5773:
5753:
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1841:
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1397:
1377:
1243:
1223:
1047:
1027:
299:
279:
6614:
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8937:
is simply an orthogonal coordinate transformation of the initial condition to a set of coordinates which decay exponentially and independently of each other.
9725:
9478:
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9376:
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676:
148:. For the case of a finite-dimensional graph (having a finite number of edges and vertices), the discrete Laplace operator is more commonly called the
212:, differing by sign and scale factor (sometimes one averages over the neighboring vertices, other times one just sums; this makes no difference for a
2447:
3860:
It can be shown that the following discrete approximation of the two-dimensional
Laplacian operator as a convex combination of difference operators
11698:
Reuter, M.; Biasotti, S.; Giorgi, D.; Patane, G.; Spagnuolo, M. (2009). "Discrete
Laplace-Beltrami operators for shape analysis and segmentation".
8813:
884:
6322:{\displaystyle \nabla ^{2}f({\bar {r}}_{k})=\sum _{k'\in K}f_{k'}(\nabla ^{2}\mu ({\bar {r}}-{\bar {r}}_{k'}))|_{{\bar {r}}={\bar {r}}_{k}}}
5607:
5825:
96:
49:
68:
12189:
2780:{\displaystyle \mathbf {D} _{xy}^{2}={\begin{bmatrix}0.25&0.5&0.25\\0.5&-3&0.5\\0.25&0.5&0.25\end{bmatrix}}}
12156:
3445:
11396:
5822:. On a uniform grid, such as images, and for bandlimited functions, interpolation functions are shift invariant amounting to
387:
75:
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2199:
12137:
12104:
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11819:
9589:
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82:
6485:
which are used in pattern recognition for their total least-square optimality in orientation estimation, can be realized.
5960:
4586:{\displaystyle (\nabla _{7}^{2}f)_{0,0,0}=f_{-1,0,0}+f_{+1,0,0}+f_{0,-1,0}+f_{0,+1,0}+f_{0,0,-1}+f_{0,0,+1}-6f_{0,0,0},}
11984:
9379:
1428:
11644:
8993:
2391:
64:
11883:
11228:{\displaystyle G(v,w;\lambda )=\left\langle \delta _{v}\left|{\frac {1}{H-\lambda }}\right|\delta _{w}\right\rangle }
7639:
115:
11896:
Patra, Michael; Karttunen, Mikko (2006). "Stencils with isotropic discretization error for differential operators".
1195:{\displaystyle (\Delta u)_{i}\equiv {\frac {1}{2A_{i}}}\sum _{j}(\cot \alpha _{ij}+\cot \beta _{ij})(u_{j}-u_{i}),}
6794:{\displaystyle {\frac {\partial ^{2}F}{\partial x^{2}}}=\lim _{\epsilon \rightarrow 0}{\frac {-}{\epsilon ^{2}}}.}
3379:
11859:
11272:
6088:-dimensions. Accordingly, the discrete Laplacian becomes a discrete version of the Laplacian of the continuous
3847:{\displaystyle \mathbf {D} _{xy}^{2}={\begin{bmatrix}1&1&1\\1&-8&1\\1&1&1\end{bmatrix}}.}
2622:{\displaystyle \mathbf {D} _{xy}^{2}={\begin{bmatrix}0&1&0\\1&-4&1\\0&1&0\end{bmatrix}}}
10972:
6450:
53:
8948:
11798:
9573:{\displaystyle \lim _{t\to \infty }\phi (t)=\left\langle c(0),\mathbf {v^{1}} \right\rangle \mathbf {v^{1}} }
12132:. Proceedings of Symposia in Pure Mathematics. Vol. 77. American Mathematical Society. pp. 51–86.
10910:
6332:
which in turn is a convolution with the
Laplacian of the interpolation function on the uniform (image) grid
2793:
12204:
11560:
7733:
6853:
6482:
6419:-dimensions, and are frequency aware by definition. A linear operator has not only a limited range in the
5475:
A discrete signal, comprising images, can be viewed as a discrete representation of a continuous function
2635:
2377:
209:
141:
3268:{\displaystyle {\frac {1}{26}}{\begin{bmatrix}3&6&3\\6&-88&6\\3&6&3\end{bmatrix}}}
2424:
641:
12194:
11502:
11107:
5516:
11546:
The ordinary ADE graphs are the only graphs that admit a positive labeling with the following property:
9860:
until that energy is spread out evenly throughout all of the elements that are connected to each other.
3358:{\displaystyle {\frac {1}{26}}{\begin{bmatrix}2&3&2\\3&6&3\\2&3&2\end{bmatrix}}}
3175:{\displaystyle {\frac {1}{26}}{\begin{bmatrix}2&3&2\\3&6&3\\2&3&2\end{bmatrix}}}
304:
6904:
6454:
2361:
1489:
1416:
596:
89:
7732:
To find a solution to this differential equation, apply standard techniques for solving a first-order
546:. For a graph with a finite number of edges and vertices, this definition is identical to that of the
12043:"Discrete Green's functions and spectral graph theory for computationally efficient thermal modeling"
7623:{\displaystyle {\begin{aligned}{\frac {d\phi }{dt}}&=-k(D-A)\phi \\&=-kL\phi ,\end{aligned}}}
6950:
1400:
1006:
11083:
If the number of edges meeting at a vertex is uniformly bounded, and the potential is bounded, then
9167:
1585:
12179:
11836:
11749:
11712:
9898:
exponential decay acts to distribute the values at these points evenly throughout the entire grid.
9286:
6091:
5478:
1983:
1968:
188:
11595:
The resulting numbering is unique (scale is specified by the "2"), and consists of integers; for E
9332:
8781:
7931:
7759:
7027:
are connected (if they are not connected, no heat is transferred). Then, for thermal conductivity
2171:{\displaystyle \Delta f(x,y)\approx {\frac {f(x-h,y)+f(x+h,y)+f(x,y-h)+f(x,y+h)-4f(x,y)}{h^{2}}},}
1248:
815:
573:
12199:
11608:
11241:
11095:
11043:
9257:
6500:
1278:
539:
42:
11125:
11077:
9077:
6422:
5705:
11744:
11707:
1916:
334:
11369:
8890:
This approach has been applied to quantitative heat transfer modelling on unstructured grids.
8597:
8566:
5778:
12184:
12067:
12042:
11114:
7705:
6494:
6493:
The spectrum of the discrete Laplacian on an infinite grid is of key interest; since it is a
2428:
derivative. The smoothing filter and Laplace filter are often combined into a single filter.
1972:
1408:
845:
344:
226:
12094:
11860:
Lindeberg, T., "Scale-space for discrete signals", PAMI(12), No. 3, March 1990, pp. 234–254.
11343:
9405:
5558:
506:
12054:
12013:
11488:
Certain equations involving the discrete Laplacian only have solutions on the simply-laced
10950:
9663:
6859:
6375:
1889:
1412:
1331:
553:
364:
164:
8752:
8723:
8667:
8624:
6047:
5916:
2993:{\displaystyle {\begin{bmatrix}0&1&0\\1&-6&1\\0&1&0\end{bmatrix}}}
1774:
1407:. The above cotangent formula can be derived using many different methods among which are
8:
11773:
11129:
11121:
3073:{\displaystyle {\begin{bmatrix}0&0&0\\0&1&0\\0&0&0\end{bmatrix}}}
2910:{\displaystyle {\begin{bmatrix}0&0&0\\0&1&0\\0&0&0\end{bmatrix}}}
1420:
12160:
12058:
12017:
1308:
12072:
12026:
12001:
11921:
11613:
11493:
11483:
9880:
9842:
9690:
7739:
6835:
6805:
6532:
6460:
6402:
6355:
6335:
6071:
5940:
5805:
5758:
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2674:
2670:
1980:
1869:
1849:
1826:
1803:
1534:
1382:
1362:
1228:
1208:
1032:
1012:
338:
284:
264:
172:
11876:
Lindeberg, T., Scale-Space Theory in Computer Vision, Kluwer Academic Publishers, 1994
9828:{\displaystyle \lim _{t\to \infty }\phi _{j}(t)={\frac {1}{N}}\sum _{i=1}^{N}c_{i}(0)}
9434:
6584:
6552:
216:). The traditional definition of the graph Laplacian, given below, corresponds to the
12133:
12100:
12076:
11980:
11952:
11925:
11913:
11879:
11815:
11623:
6065:
2436:
For one-, two- and three-dimensional signals, the discrete Laplacian can be given as
542:
between vertices w and v. Thus, this sum is over the nearest neighbors of the vertex
9868:
9256:
In other words, the equilibrium state of the system is determined completely by the
5581:. Derivation operation is therefore directly applicable to the continuous function,
12119:
12090:
12062:
12021:
12002:"Computational heat transfer with spectral graph theory: Quantitative verification"
11944:
11905:
11807:
11754:
11717:
11680:
9710:
9463:
9385:
9361:
9263:
8920:
8917:, its eigenvectors are all orthogonal. So the projection onto the eigenvectors of
8914:
8896:
8703:
7030:
7010:
6990:
6930:
6910:
6886:
6809:
6478:
1404:
547:
184:
176:
168:
149:
137:
2384:
11837:"A Family of Large-Stencil Discrete Laplacian Approximations in Three Dimensions"
11554:
In terms of the Laplacian, the positive solutions to the inhomogeneous equation:
11266:
802:{\displaystyle (\Delta _{\gamma }\phi )(v)=\sum _{w:\,d(w,v)=1}\gamma _{wv}\left}
145:
11489:
11113:
On regular lattices, the operator typically has both traveling-wave as well as
10279:% BELOW IS THE KEY CODE THAT COMPUTES THE SOLUTION TO THE DIFFERENTIAL EQUATION
6821:
6813:
6625:
2513:{\displaystyle {\vec {D}}_{x}^{2}={\begin{bmatrix}1&-2&1\end{bmatrix}}}
2345:
180:
175:
as a stand-in for the continuous Laplace operator. Common applications include
11758:
11721:
3583:
2380:), is rarely used for graph Laplacians, but is common in other applications.
1979:. For example, the Laplacian in two dimensions can be approximated using the
12173:
12123:
11917:
11672:
8879:{\displaystyle c_{i}(0)=\left\langle \phi (0),\mathbf {v} _{i}\right\rangle }
7695:
5934:
213:
11684:
10636:% Transform from eigenvector coordinate system to original coordinate system
10333:% Compute the laplacian matrix in terms of the degree and adjacency matrices
986:{\displaystyle (M\phi )(v)={\frac {1}{\deg v}}\sum _{w:\,d(w,v)=1}\phi (w).}
11088:
2403:
2387:
11811:
11972:
11496:. Specifically, the only positive solutions to the homogeneous equation:
11099:
6817:
2437:
160:
129:
20:
11875:
11806:. Weinheim, Germany: Wiley-VCH Verlag GmbH & Co. KGaA. p. 219.
11550:
Twice any label minus two is the sum of the labels on adjacent vertices.
9382:
in the graph, then this vector of all ones can be split into the sum of
10947:
can be considered to be a multiplicative operator acting diagonally on
2399:
1379:; that is, e.g. one third of the summed areas of triangles incident to
12127:
11909:
11386:
a complex number, the Green's function considered to be a function of
12099:, Elements of Mathematics, translated by Pressley, Andrew, Springer,
11117:
solutions, depending on whether the potential is periodic or random.
10940:
5692:{\displaystyle f({\bar {r}})=\sum _{k\in K}f_{k}\mu _{k}({\bar {r}})}
1964:
11948:
11599:
they range from 58 to 270, and have been observed as early as 1968.
5906:{\displaystyle \mu _{k}({\bar {r}})=\mu ({\bar {r}}-{\bar {r}}_{k})}
3857:
These kernels are deduced by using discrete differential quotients.
593:
is the product of the column vector and the Laplacian matrix, while
31:
1002:
12040:
10372:% Initial condition (place a few large positive values around and
156:
11538:"Twice any label is the sum of the labels on adjacent vertices,"
1425:
To facilitate computation, the Laplacian is encoded in a matrix
11999:
5470:
2185:
in both dimensions, so that the five-point stencil of a point (
638:
If the graph has weighted edges, that is, a weighting function
9431:
The consequence of this is that for a given initial condition
2348:. There are no constraints here on the values of the function
11673:"Digital geometry processing with discrete exterior calculus"
11103:
2431:
10549:% Transform the initial condition into the coordinate system
3511:{\displaystyle \mathbf {D} _{x_{1},x_{2},\dots ,x_{n}}^{2},}
11670:
11467:{\displaystyle (H-\lambda )G(v,w;\lambda )=\delta _{w}(v).}
9239:
7839:{\textstyle L\mathbf {v} _{i}=\lambda _{i}\mathbf {v} _{i}}
3664:
1755:
493:{\displaystyle (\Delta \phi )(v)=\sum _{w:\,d(w,v)=1}\left}
11844:
International Journal for Numerical Methods in Engineering
11697:
11671:
Crane, K.; de Goes, F.; Desbrun, M.; Schröder, P. (2013).
2364:). The control of the state variable at the boundary, as
2326:{\displaystyle \{(x-h,y),(x,y),(x+h,y),(x,y-h),(x,y+h)\}.}
19:
For the discrete equivalent of the Laplace transform, see
10351:% Compute the eigenvalues/vectors of the laplacian matrix
11800:
Phase-Field Methods in Materials Science and Engineering
7915:{\textstyle \phi (t)=\sum _{i}c_{i}(t)\mathbf {v} _{i}.}
6812:. In image processing, it is considered to be a type of
6457:
representations for further computational efficiency in
1399:. It is important to note that the sign of the discrete
11734:
9650:{\displaystyle \mathbf {v^{1}} ={\frac {1}{\sqrt {N}}}}
1955:
A more general overview of mesh operators is given in.
220:
continuous Laplacian on a domain with a free boundary.
11492:(all edges multiplicity 1), and are an example of the
9883:
9845:
9713:
9693:
9666:
9466:
9437:
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2929:
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2716:
2558:
2483:
11735:
Forsyth, D. A.; Ponce, J. (2003). "Computer Vision".
11563:
11505:
11399:
11372:
11346:
11275:
11244:
11141:
11046:
10975:
10953:
10913:
10579:% Loop through times and decay each initial component
9919:% The number of pixels along a dimension of the image
9736:
9592:
9489:
9116:
8893:
In the case of undirected graphs, this works because
8816:
8553:{\displaystyle c_{i}(t)=c_{i}(0)e^{-k\lambda _{i}t}.}
8479:
7966:
7694:
Notice that this equation takes the same form as the
7642:
7535:
7056:
6804:
This definition of the Laplacian is commonly used in
6637:
6587:
6555:
6535:
6503:
6463:
6425:
6405:
6378:
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6338:
6134:
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3525:
3448:
3382:
3281:
3188:
3098:
3006:
2923:
2843:
2796:
2687:
2638:
2529:
2450:
2202:
1995:
1919:
1892:
1872:
1852:
1829:
1806:
1777:
1563:
1537:
1492:
1431:
1385:
1365:
1334:
1311:
1281:
1251:
1231:
1211:
1058:
1035:
1015:
887:
848:
818:
679:
644:
599:
576:
556:
509:
390:
367:
347:
307:
287:
267:
229:
11898:
Numerical Methods for Partial Differential Equations
9863:
6037:{\displaystyle {\bar {r}}=(x_{1},x_{2}...x_{n})^{T}}
1403:
is conventionally opposite the sign of the ordinary
670:
is given, then the definition can be generalized to
9988:% Use 8 neighbors, and fill in the adjacency matrix
56:. Unsourced material may be challenged and removed.
11889:
11584:
11523:
11466:
11378:
11358:
11313:
11257:
11227:
11064:
11029:
10959:
10931:
9889:
9851:
9827:
9719:
9699:
9679:
9649:
9572:
9472:
9452:
9420:
9394:
9370:
9350:
9321:
9272:
9245:
9099:
9066:
8982:
8929:
8905:
8878:
8799:
8770:
8741:
8712:
8692:
8649:
8613:
8582:
8552:
8459:
7949:
7928:is a symmetric matrix, its unit-norm eigenvectors
7914:
7838:
7777:
7748:
7721:
7683:
7622:
7515:
7039:
7019:
6999:
6979:
6939:
6919:
6895:
6875:
6844:
6793:
6608:
6581:(as the averaging operator has spectral values in
6573:
6541:
6521:
6469:
6440:
6411:
6391:
6364:
6344:
6321:
6118:
6080:
6056:
6036:
5949:
5925:
5905:
5814:
5794:
5767:
5747:
5727:
5691:
5593:
5573:
5547:
5505:
5459:
5072:
4585:
4320:
4129:
3846:
3669:
3510:
3434:
3357:
3267:
3174:
3072:
2992:
2909:
2822:
2779:
2661:
2621:
2512:
2325:
2170:
1944:
1905:
1878:
1858:
1835:
1812:
1792:
1761:
1543:
1523:
1478:
1391:
1371:
1347:
1320:
1297:
1267:
1237:
1217:
1194:
1041:
1021:
985:
863:
834:
801:
662:
623:
585:
562:
530:
492:
373:
353:
325:
293:
273:
253:
9067:{\textstyle c_{i}(t)=c_{i}(0)e^{-k\lambda _{i}t}}
5802:are interpolation functions specific to the grid
1479:{\displaystyle L\in \mathbb {R} ^{|V|\times |V|}}
874:Closely related to the discrete Laplacian is the
12171:
11834:
11790:
10902:
9738:
9491:
9118:
8953:
6676:
1886:-th entry along the diagonal is the vertex area
12047:International Journal of Heat and Mass Transfer
11102:; this is a consequence of the duality between
7924:Plugging into the original expression (because
7684:{\displaystyle {\frac {d\phi }{dt}}+kL\phi =0.}
1952:is the sought discretization of the Laplacian.
12041:Cole, K. D.; Riensche, A.; Rao, P. K. (2022).
11895:
9839:In other words, at steady state, the value of
6852:describes a temperature distribution across a
2344:discrete Laplacian on the graph, which is the
11796:
11679:. SIGGRAPH '13. Vol. 7. pp. 1–126.
6497:, it has a real spectrum. For the convention
2390:have very special properties, e.g., they are
12000:Yavari, R.; Cole, K. D.; Rao, P. K. (2020).
11797:Provatas, Nikolas; Elder, Ken (2010-10-13).
9877:This section shows an example of a function
6064:on uniform grids, are appropriately dilated
5471:Implementation via continuous reconstruction
3435:{\displaystyle a_{x_{1},x_{2},\dots ,x_{n}}}
2394:of one-dimensional discrete Laplacians, see
2317:
2203:
1205:where the sum is over all adjacent vertices
11314:{\displaystyle \delta _{w}(v)=\delta _{wv}}
10669:% Display the results and write to GIF file
9358:of all ones is in the kernel. If there are
11993:
11828:
10943:function defined on the graph. Note that
8720:in terms of the overall initial condition
2432:Implementation via operator discretization
2376:) given on the boundary of the grid (aka,
570:can be written as a column vector; and so
12066:
12025:
12006:International Journal of Thermal Sciences
11938:
11932:
11748:
11711:
11642:
11030:{\displaystyle (P\phi )(v)=P(v)\phi (v).}
8983:{\textstyle \lim _{t\to \infty }\phi (t)}
6827:
4289:
4253:
4224:
1440:
941:
722:
426:
116:Learn how and when to remove this message
16:Analog of the continuous Laplace operator
12154:
12096:Groupes et algebres de Lie: Chapters 4–6
12089:
12083:
12068:10.1016/j.ijheatmasstransfer.2021.122112
12034:
11728:
11098:of this Hamiltonian can be studied with
9867:
7756:as a linear combination of eigenvectors
2409:
2383:Multidimensional discrete Laplacians on
1305:are the two angles opposite of the edge
155:The discrete Laplace operator occurs in
12129:Analysis on Graphs and Its Applications
11871:
11869:
11867:
11855:
11853:
11835:O'Reilly, H.; Beck, Jeffrey M. (2006).
11771:
11691:
8940:
2425:Laplace operator#Coordinate expressions
12172:
12118:
11971:
11664:
10932:{\displaystyle P\colon V\rightarrow R}
10615:% Exponential decay for each component
3704:) of the element in the kernel in the
2823:{\displaystyle \mathbf {D} _{xyz}^{2}}
167:, as well as in the study of discrete
140:, defined so that it has meaning on a
11585:{\displaystyle \Delta \phi =\phi -2.}
11477:
9727:in the graph, it can be rewritten as
2662:{\displaystyle \mathbf {D} _{xy}^{2}}
1958:
204:There are various definitions of the
11864:
11850:
11619:Kronecker sum of discrete Laplacians
7846:) with time-dependent coefficients,
7702:is replacing the Laplacian operator
2396:Kronecker sum of discrete Laplacians
663:{\displaystyle \gamma \colon E\to R}
54:adding citations to reliable sources
25:
11524:{\displaystyle \Delta \phi =\phi ,}
5548:{\displaystyle {\bar {r}}\in R^{n}}
2418:
1687:
337:of the vertices taking values in a
199:
13:
12027:10.1016/j.ijthermalsci.2020.106383
11564:
11506:
11053:
9748:
9501:
9128:
8963:
7710:
6656:
6642:
6504:
6216:
6136:
5092:
4605:
4345:
4291:
4255:
4226:
4152:
3925:
3904:
3871:
1996:
1505:
1062:
996:
684:
603:
577:
394:
348:
326:{\displaystyle \phi \colon V\to R}
14:
12216:
12148:
11643:Leventhal, Daniel (Autumn 2011).
9864:Example of the operator on a grid
8563:As shown before, the eigenvalues
6907:, the heat transferred from node
1524:{\displaystyle Lu=(\Delta u)_{i}}
624:{\displaystyle (\Delta \phi )(v)}
12190:Numerical differential equations
9599:
9595:
9564:
9560:
9547:
9543:
9338:
8861:
8787:
8778:onto the unit-norm eigenvectors
8347:
8300:
8217:
8177:
8094:
8023:
7937:
7899:
7826:
7801:
7765:
7729:; hence, the "graph Laplacian".
6980:{\textstyle \phi _{i}-\phi _{j}}
5735:are discrete representations of
3754:
3451:
2799:
2690:
2677:, which includes the diagonals:
2641:
2532:
1409:piecewise linear finite elements
842:is the weight value on the edge
635:th entry of the product vector.
30:
11965:
5933:being an appropriately dilated
1655: is an edge, that is
341:. Then, the discrete Laplacian
136:is an analog of the continuous
41:needs additional citations for
11765:
11636:
11458:
11452:
11436:
11418:
11412:
11400:
11292:
11286:
11163:
11145:
11076:, an analog of the continuous
11021:
11015:
11009:
11003:
10994:
10988:
10985:
10976:
10923:
9822:
9816:
9769:
9763:
9745:
9644:
9620:
9535:
9529:
9515:
9509:
9498:
9447:
9441:
9322:{\textstyle \sum _{j}L_{ij}=0}
9125:
9035:
9029:
9013:
9007:
8977:
8971:
8960:
8853:
8847:
8833:
8827:
8765:
8759:
8736:
8730:
8687:
8681:
8644:
8638:
8518:
8512:
8496:
8490:
8447:
8441:
8401:
8395:
8366:
8332:
8326:
8284:
8278:
8209:
8203:
8161:
8155:
8089:
8083:
8018:
8012:
7894:
7888:
7862:
7856:
7585:
7573:
7415:
7402:
7305:
7292:
6772:
6769:
6757:
6748:
6742:
6736:
6730:
6727:
6721:
6712:
6700:
6694:
6683:
6603:
6588:
6568:
6556:
6451:decimation (signal processing)
6432:
6305:
6289:
6278:
6273:
6270:
6253:
6237:
6228:
6212:
6170:
6158:
6148:
6113:
6107:
6098:
6025:
5979:
5970:
5900:
5888:
5872:
5863:
5854:
5848:
5839:
5686:
5680:
5671:
5629:
5623:
5614:
5526:
5513:, where the coordinate vector
5500:
5494:
5485:
5451:
5151:
5117:
5088:
5064:
4664:
4630:
4601:
4363:
4341:
4312:
4221:
4189:
3954:
3942:
3900:
3888:
2458:
2406:can be explicitly calculated.
2314:
2296:
2290:
2272:
2266:
2248:
2242:
2230:
2224:
2206:
2149:
2137:
2125:
2107:
2098:
2080:
2071:
2053:
2044:
2026:
2014:
2002:
1787:
1781:
1706:
1700:
1673:
1667:
1642:
1598:
1512:
1502:
1470:
1462:
1454:
1446:
1186:
1160:
1157:
1113:
1069:
1059:
977:
971:
957:
945:
906:
900:
897:
888:
791:
785:
776:
770:
738:
726:
705:
699:
696:
680:
654:
618:
612:
609:
600:
525:
513:
482:
476:
467:
461:
442:
430:
409:
403:
400:
391:
317:
248:
236:
194:
183:, and in machine learning for
1:
12124:"Discrete geometric analysis"
11772:Matthys, Don (Feb 14, 2001).
11629:
11074:discrete Schrödinger operator
10903:Discrete Schrödinger operator
9351:{\textstyle \mathbf {v} ^{1}}
8800:{\textstyle \mathbf {v} _{i}}
7950:{\textstyle \mathbf {v} _{i}}
7778:{\textstyle \mathbf {v} _{i}}
6883:is the temperature at vertex
6119:{\displaystyle f({\bar {r}})}
5555:and the value domain is real
5506:{\displaystyle f({\bar {r}})}
10375:% make everything else zero)
9074:that remain are those where
7734:matrix differential equation
6624:If the graph is an infinite
6483:Generalized Structure Tensor
3714:is the number of directions
2440:with the following kernels:
2378:Dirichlet boundary condition
1800:denotes the neighborhood of
1268:{\displaystyle \alpha _{ij}}
835:{\displaystyle \gamma _{wv}}
586:{\displaystyle \Delta \phi }
7:
11979:. Oxford University Press.
11602:
11258:{\displaystyle \delta _{w}}
11065:{\displaystyle H=\Delta +P}
10702:'Diffusion t = %3f'
10312:% Compute the degree matrix
9100:{\textstyle \lambda _{i}=0}
8657:, the solution at any time
7526:In matrix-vector notation,
6619:
6549:, the spectrum lies within
6522:{\displaystyle \Delta =I-M}
6488:
1298:{\displaystyle \beta _{ij}}
179:, where it is known as the
65:"Discrete Laplace operator"
10:
12221:
11481:
11390:is the unique solution to
8621:and the initial condition
6455:pyramid (image processing)
6441:{\displaystyle {\bar {r}}}
6044:. Other approximations of
5728:{\displaystyle f_{k}\in R}
2362:Neumann boundary condition
1417:discrete exterior calculus
18:
12157:"Spectral gap of a graph"
11977:Networks: An Introduction
11759:10.1016/j.cag.2009.03.005
11722:10.1016/j.cag.2009.03.005
11677:ACM SIGGRAPH 2013 Courses
8913:is symmetric, and by the
8614:{\textstyle \lambda _{i}}
8583:{\textstyle \lambda _{i}}
1945:{\displaystyle L=M^{-1}C}
1401:Laplace-Beltrami operator
1007:Laplace-Beltrami operator
261:be a graph with vertices
134:discrete Laplace operator
11737:Computers & Graphics
11700:Computers & Graphics
11652:University of Washington
11379:{\displaystyle \lambda }
11265:is understood to be the
9904:
7722:{\textstyle \nabla ^{2}}
5795:{\displaystyle \mu _{k}}
3692:is the position (either
2398:, in which case all its
1984:finite-difference method
1969:finite-difference method
191:on neighborhood graphs.
189:semi-supervised learning
12155:Ollivier, Yann (2004).
11685:10.1145/2504435.2504442
11609:Spectral shape analysis
11269:function on the graph:
9707:, i.e. for each vertex
9421:{\textstyle \lambda =0}
6905:Newton's law of cooling
6816:, more specifically an
2340:= 1, the result is the
2181:where the grid size is
1049:can be approximated as
864:{\displaystyle wv\in E}
354:{\displaystyle \Delta }
254:{\displaystyle G=(V,E)}
11586:
11525:
11468:
11380:
11360:
11359:{\displaystyle w\in V}
11315:
11259:
11229:
11066:
11031:
10961:
10933:
9985:% The adjacency matrix
9891:
9874:
9853:
9829:
9805:
9721:
9701:
9681:
9680:{\textstyle \phi _{j}}
9651:
9574:
9474:
9454:
9422:
9396:
9372:
9352:
9323:
9274:
9247:
9101:
9068:
8984:
8931:
8907:
8880:
8801:
8772:
8743:
8714:
8694:
8651:
8615:
8584:
8554:
8461:
7951:
7916:
7840:
7779:
7750:
7723:
7685:
7624:
7517:
7041:
7021:
7001:
6981:
6941:
6921:
6897:
6877:
6876:{\textstyle \phi _{i}}
6846:
6828:Discrete heat equation
6795:
6610:
6575:
6543:
6523:
6471:
6442:
6413:
6393:
6366:
6346:
6323:
6120:
6082:
6058:
6038:
5951:
5927:
5907:
5816:
5796:
5769:
5749:
5729:
5693:
5595:
5575:
5574:{\displaystyle f\in R}
5549:
5507:
5461:
5074:
4587:
4322:
4131:
3848:
3671:
3512:
3436:
3359:
3269:
3176:
3074:
2994:
2911:
2824:
2781:
2663:
2623:
2514:
2327:
2172:
1963:Approximations of the
1946:
1907:
1880:
1860:
1837:
1814:
1794:
1763:
1545:
1525:
1480:
1393:
1373:
1349:
1322:
1299:
1269:
1239:
1219:
1196:
1043:
1023:
987:
865:
836:
803:
664:
625:
587:
564:
532:
531:{\displaystyle d(w,v)}
494:
375:
355:
327:
295:
275:
255:
11941:Vision with Direction
11812:10.1002/9783527631520
11587:
11526:
11482:Further information:
11469:
11381:
11361:
11321:; that is, it equals
11316:
11260:
11230:
11115:Anderson localization
11067:
11032:
10962:
10960:{\displaystyle \phi }
10934:
10552:% of the eigenvectors
9892:
9871:
9854:
9830:
9785:
9722:
9702:
9682:
9652:
9575:
9475:
9455:
9423:
9397:
9373:
9353:
9324:
9283:Since by definition,
9275:
9248:
9102:
9069:
8985:
8932:
8908:
8881:
8802:
8773:
8771:{\textstyle \phi (0)}
8744:
8742:{\textstyle \phi (0)}
8715:
8695:
8693:{\textstyle c_{i}(0)}
8652:
8650:{\textstyle c_{i}(0)}
8616:
8585:
8555:
8462:
7952:
7917:
7841:
7780:
7751:
7724:
7686:
7625:
7518:
7042:
7022:
7002:
6982:
6942:
6922:
6898:
6878:
6847:
6796:
6611:
6576:
6544:
6524:
6495:self-adjoint operator
6472:
6443:
6414:
6394:
6392:{\displaystyle f_{k}}
6367:
6347:
6324:
6121:
6083:
6059:
6039:
5952:
5928:
5908:
5817:
5797:
5770:
5750:
5730:
5694:
5596:
5576:
5550:
5508:
5462:
5075:
4588:
4323:
4132:
3849:
3672:
3513:
3437:
3360:
3270:
3177:
3075:
2995:
2912:
2825:
2782:
2664:
2624:
2515:
2410:Finite-element method
2328:
2173:
1975:, can also be called
1973:finite-element method
1947:
1908:
1906:{\displaystyle A_{i}}
1881:
1861:
1838:
1815:
1795:
1764:
1546:
1526:
1481:
1394:
1374:
1350:
1348:{\displaystyle A_{i}}
1323:
1300:
1270:
1240:
1220:
1197:
1044:
1024:
1009:of a scalar function
988:
866:
837:
804:
665:
626:
588:
565:
563:{\displaystyle \phi }
533:
495:
376:
374:{\displaystyle \phi }
356:
328:
296:
276:
256:
171:. It is also used in
159:problems such as the
11778:Marquette University
11561:
11503:
11397:
11370:
11344:
11273:
11242:
11139:
11126:Schrödinger operator
11078:Schrödinger operator
11044:
10973:
10951:
10911:
9881:
9843:
9734:
9711:
9691:
9664:
9590:
9487:
9464:
9435:
9406:
9386:
9380:connected components
9362:
9333:
9287:
9264:
9114:
9078:
8994:
8949:
8941:Equilibrium behavior
8921:
8897:
8814:
8782:
8753:
8724:
8704:
8668:
8625:
8598:
8567:
8477:
7964:
7932:
7850:
7793:
7760:
7740:
7706:
7698:, where the matrix −
7640:
7533:
7054:
7031:
7011:
6991:
6951:
6931:
6911:
6887:
6860:
6836:
6635:
6585:
6553:
6533:
6501:
6461:
6423:
6403:
6376:
6356:
6336:
6132:
6092:
6072:
6057:{\displaystyle \mu }
6048:
5961:
5941:
5926:{\displaystyle \mu }
5917:
5826:
5806:
5779:
5759:
5739:
5706:
5608:
5585:
5559:
5517:
5479:
5085:
4598:
4338:
4148:
3867:
3749:
3523:
3446:
3380:
3279:
3186:
3096:
3004:
2921:
2841:
2794:
2685:
2669:corresponds to the (
2636:
2527:
2448:
2200:
1993:
1917:
1890:
1870:
1850:
1827:
1804:
1793:{\displaystyle N(i)}
1775:
1561:
1535:
1490:
1429:
1383:
1363:
1332:
1309:
1279:
1249:
1229:
1209:
1056:
1033:
1013:
885:
846:
816:
677:
642:
597:
574:
554:
507:
388:
365:
345:
305:
285:
265:
227:
165:loop quantum gravity
50:improve this article
12205:Geometry processing
12059:2022IJHMT.18322112C
12018:2020IJTS..15306383C
11130:resolvent formalism
11096:spectral properties
10882:'DelayTime'
10870:'WriteMode'
10825:'DelayTime'
10813:'Loopcount'
6947:is proportional to
6626:square lattice grid
6372:is represented via
5112:
4625:
4358:
4311:
4275:
4239:
4185:
3938:
3917:
3884:
3771:
3708:-th direction, and
3504:
2832:seven-point stencil
2819:
2707:
2658:
2549:
2474:
2346:square lattice grid
1977:discrete Laplacians
1005:triangle mesh, the
12195:Finite differences
11939:Bigun, J. (2006).
11645:"Image processing"
11614:Electrical network
11582:
11521:
11494:ADE classification
11484:ADE classification
11478:ADE classification
11464:
11376:
11356:
11311:
11255:
11225:
11062:
11027:
10957:
10929:
9890:{\textstyle \phi }
9887:
9875:
9852:{\textstyle \phi }
9849:
9825:
9752:
9717:
9700:{\textstyle \phi }
9697:
9677:
9647:
9570:
9505:
9470:
9450:
9418:
9392:
9368:
9348:
9319:
9299:
9270:
9243:
9238:
9132:
9097:
9064:
8980:
8967:
8927:
8903:
8876:
8797:
8768:
8739:
8710:
8690:
8647:
8611:
8580:
8550:
8470:whose solution is
8457:
8455:
8256:
8133:
8072:
8001:
7947:
7912:
7877:
7836:
7775:
7749:{\textstyle \phi }
7746:
7736:. That is, write
7719:
7681:
7620:
7618:
7513:
7511:
7474:
7374:
7320:
7223:
7197:
7110:
7037:
7017:
6997:
6977:
6937:
6917:
6893:
6873:
6845:{\textstyle \phi }
6842:
6806:numerical analysis
6791:
6690:
6606:
6571:
6539:
6519:
6467:
6438:
6409:
6389:
6362:
6342:
6319:
6196:
6116:
6078:
6066:Gaussian functions
6054:
6034:
5947:
5923:
5903:
5812:
5792:
5765:
5745:
5725:
5689:
5650:
5591:
5571:
5545:
5503:
5457:
5091:
5070:
4604:
4583:
4344:
4318:
4290:
4254:
4225:
4151:
4127:
4121:
4017:
3924:
3903:
3870:
3844:
3835:
3752:
3667:
3662:
3508:
3449:
3432:
3376:: For the element
3355:
3349:
3265:
3259:
3172:
3166:
3070:
3064:
2990:
2984:
2907:
2901:
2820:
2797:
2777:
2771:
2688:
2675:nine-point stencil
2671:Five-point stencil
2659:
2639:
2619:
2613:
2530:
2510:
2504:
2451:
2385:rectangular cuboid
2323:
2168:
1981:five-point stencil
1967:, obtained by the
1959:Finite differences
1942:
1903:
1876:
1856:
1833:
1810:
1790:
1759:
1754:
1710:
1541:
1521:
1476:
1389:
1369:
1345:
1321:{\displaystyle ij}
1318:
1295:
1265:
1235:
1215:
1192:
1112:
1039:
1019:
983:
967:
876:averaging operator
861:
832:
799:
748:
660:
621:
583:
560:
528:
490:
452:
371:
351:
323:
291:
271:
251:
206:discrete Laplacian
173:numerical analysis
12139:978-0-8218-9384-5
12106:978-3-540-69171-6
12091:Bourbaki, Nicolas
11958:978-3-540-27322-6
11910:10.1002/num.20129
11821:978-3-527-63152-0
11624:Discrete calculus
11204:
10858:'out.gif'
10801:'out.gif'
9783:
9737:
9660:For each element
9618:
9617:
9490:
9460:for a graph with
9453:{\textstyle c(0)}
9290:
9216:
9181:
9117:
8990:, the only terms
8952:
8749:, simply project
8413:
8296:
8247:
8173:
8124:
8063:
8047:
7992:
7957:are orthogonal):
7868:
7661:
7558:
7465:
7395:
7365:
7311:
7285:
7214:
7188:
7101:
7086:
6786:
6675:
6670:
6542:{\displaystyle Z}
6470:{\displaystyle n}
6435:
6412:{\displaystyle n}
6365:{\displaystyle f}
6345:{\displaystyle K}
6308:
6292:
6256:
6240:
6176:
6161:
6110:
6081:{\displaystyle n}
5973:
5957:-dimensions i.e.
5950:{\displaystyle n}
5891:
5875:
5851:
5815:{\displaystyle K}
5768:{\displaystyle K}
5748:{\displaystyle f}
5683:
5635:
5626:
5594:{\displaystyle f}
5529:
5497:
5149:
4662:
3658:
3626:
3600:
3290:
3197:
3182:; second plane =
3107:
2917:; second plane =
2461:
2336:If the grid size
2193:) in the grid is
2163:
1879:{\displaystyle i}
1859:{\displaystyle M}
1836:{\displaystyle M}
1813:{\displaystyle i}
1750:
1686:
1656:
1596:
1544:{\displaystyle C}
1392:{\displaystyle i}
1372:{\displaystyle i}
1238:{\displaystyle i}
1218:{\displaystyle j}
1103:
1101:
1042:{\displaystyle i}
1022:{\displaystyle u}
930:
928:
711:
415:
294:{\displaystyle E}
274:{\displaystyle V}
169:dynamical systems
126:
125:
118:
100:
12212:
12164:
12159:. Archived from
12143:
12110:
12109:
12087:
12081:
12080:
12070:
12038:
12032:
12031:
12029:
11997:
11991:
11990:
11969:
11963:
11962:
11936:
11930:
11929:
11893:
11887:
11873:
11862:
11857:
11848:
11847:
11841:
11832:
11826:
11825:
11805:
11794:
11788:
11787:
11785:
11784:
11769:
11763:
11762:
11752:
11732:
11726:
11725:
11715:
11706:(3): 381–390df.
11695:
11689:
11688:
11668:
11662:
11661:
11659:
11658:
11649:
11640:
11591:
11589:
11588:
11583:
11530:
11528:
11527:
11522:
11473:
11471:
11470:
11465:
11451:
11450:
11385:
11383:
11382:
11377:
11365:
11363:
11362:
11357:
11320:
11318:
11317:
11312:
11310:
11309:
11285:
11284:
11264:
11262:
11261:
11256:
11254:
11253:
11234:
11232:
11231:
11226:
11224:
11220:
11219:
11218:
11209:
11205:
11203:
11189:
11183:
11182:
11128:is given in the
11124:of the discrete
11122:Green's function
11108:Boolean algebras
11071:
11069:
11068:
11063:
11036:
11034:
11033:
11028:
10966:
10964:
10963:
10958:
10938:
10936:
10935:
10930:
10898:
10895:
10892:
10889:
10886:
10883:
10880:
10877:
10876:'append'
10874:
10871:
10868:
10865:
10862:
10859:
10856:
10853:
10850:
10847:
10844:
10841:
10838:
10835:
10832:
10829:
10826:
10823:
10820:
10817:
10814:
10811:
10808:
10805:
10802:
10799:
10796:
10793:
10790:
10787:
10784:
10781:
10778:
10775:
10772:
10769:
10766:
10763:
10760:
10757:
10754:
10751:
10748:
10745:
10742:
10739:
10736:
10733:
10730:
10727:
10724:
10721:
10718:
10715:
10712:
10709:
10706:
10703:
10700:
10697:
10694:
10691:
10688:
10685:
10682:
10679:
10676:
10673:
10670:
10667:
10664:
10661:
10658:
10655:
10652:
10649:
10646:
10643:
10640:
10637:
10634:
10631:
10628:
10625:
10622:
10619:
10616:
10613:
10610:
10607:
10604:
10601:
10598:
10595:
10592:
10589:
10586:
10583:
10580:
10577:
10574:
10571:
10568:
10565:
10562:
10559:
10556:
10553:
10550:
10547:
10544:
10541:
10538:
10535:
10532:
10529:
10526:
10523:
10520:
10517:
10514:
10511:
10508:
10505:
10502:
10499:
10496:
10493:
10490:
10487:
10484:
10481:
10478:
10475:
10472:
10469:
10466:
10463:
10460:
10457:
10454:
10451:
10448:
10445:
10442:
10439:
10436:
10433:
10430:
10427:
10424:
10421:
10418:
10415:
10412:
10409:
10406:
10403:
10400:
10397:
10394:
10391:
10388:
10385:
10382:
10379:
10376:
10373:
10370:
10367:
10364:
10361:
10358:
10355:
10352:
10349:
10346:
10343:
10340:
10337:
10334:
10331:
10328:
10325:
10322:
10319:
10316:
10313:
10310:
10307:
10304:
10301:
10298:
10295:
10292:
10289:
10286:
10283:
10280:
10277:
10274:
10271:
10268:
10265:
10262:
10259:
10256:
10253:
10250:
10247:
10244:
10241:
10238:
10235:
10232:
10229:
10226:
10223:
10220:
10217:
10214:
10211:
10208:
10205:
10202:
10199:
10196:
10193:
10190:
10187:
10184:
10181:
10178:
10175:
10172:
10169:
10166:
10163:
10160:
10157:
10154:
10151:
10148:
10145:
10142:
10139:
10136:
10133:
10130:
10127:
10124:
10121:
10118:
10115:
10112:
10109:
10106:
10103:
10100:
10097:
10094:
10091:
10088:
10085:
10082:
10079:
10076:
10073:
10070:
10067:
10064:
10061:
10058:
10055:
10052:
10049:
10046:
10043:
10040:
10037:
10034:
10031:
10028:
10025:
10022:
10019:
10016:
10013:
10010:
10007:
10004:
10001:
9998:
9995:
9992:
9989:
9986:
9983:
9980:
9977:
9974:
9971:
9968:
9965:
9962:
9959:
9956:
9953:
9950:
9947:
9944:
9941:
9938:
9935:
9932:
9929:
9926:
9923:
9920:
9917:
9914:
9911:
9908:
9896:
9894:
9893:
9888:
9858:
9856:
9855:
9850:
9834:
9832:
9831:
9826:
9815:
9814:
9804:
9799:
9784:
9776:
9762:
9761:
9751:
9726:
9724:
9723:
9718:
9706:
9704:
9703:
9698:
9686:
9684:
9683:
9678:
9676:
9675:
9656:
9654:
9653:
9648:
9619:
9613:
9609:
9604:
9603:
9602:
9579:
9577:
9576:
9571:
9569:
9568:
9567:
9557:
9553:
9552:
9551:
9550:
9504:
9479:
9477:
9476:
9471:
9459:
9457:
9456:
9451:
9427:
9425:
9424:
9419:
9401:
9399:
9398:
9393:
9377:
9375:
9374:
9369:
9357:
9355:
9354:
9349:
9347:
9346:
9341:
9328:
9326:
9325:
9320:
9312:
9311:
9298:
9279:
9277:
9276:
9271:
9252:
9250:
9249:
9244:
9242:
9241:
9229:
9228:
9217:
9214:
9194:
9193:
9182:
9179:
9158:
9157:
9153:
9152:
9131:
9106:
9104:
9103:
9098:
9090:
9089:
9073:
9071:
9070:
9065:
9063:
9062:
9058:
9057:
9028:
9027:
9006:
9005:
8989:
8987:
8986:
8981:
8966:
8936:
8934:
8933:
8928:
8915:spectral theorem
8912:
8910:
8909:
8904:
8885:
8883:
8882:
8877:
8875:
8871:
8870:
8869:
8864:
8826:
8825:
8806:
8804:
8803:
8798:
8796:
8795:
8790:
8777:
8775:
8774:
8769:
8748:
8746:
8745:
8740:
8719:
8717:
8716:
8711:
8699:
8697:
8696:
8691:
8680:
8679:
8656:
8654:
8653:
8648:
8637:
8636:
8620:
8618:
8617:
8612:
8610:
8609:
8589:
8587:
8586:
8581:
8579:
8578:
8559:
8557:
8556:
8551:
8546:
8545:
8541:
8540:
8511:
8510:
8489:
8488:
8466:
8464:
8463:
8458:
8456:
8440:
8439:
8430:
8429:
8414:
8412:
8404:
8394:
8393:
8380:
8376:
8361:
8357:
8356:
8355:
8350:
8344:
8343:
8325:
8324:
8309:
8308:
8303:
8297:
8295:
8287:
8277:
8276:
8263:
8255:
8242:
8237:
8231:
8227:
8226:
8225:
8220:
8202:
8201:
8186:
8185:
8180:
8174:
8172:
8164:
8154:
8153:
8140:
8132:
8119:
8114:
8108:
8104:
8103:
8102:
8097:
8082:
8081:
8071:
8048:
8046:
8038:
8037:
8033:
8032:
8031:
8026:
8011:
8010:
8000:
7982:
7978:
7956:
7954:
7953:
7948:
7946:
7945:
7940:
7921:
7919:
7918:
7913:
7908:
7907:
7902:
7887:
7886:
7876:
7845:
7843:
7842:
7837:
7835:
7834:
7829:
7823:
7822:
7810:
7809:
7804:
7784:
7782:
7781:
7776:
7774:
7773:
7768:
7755:
7753:
7752:
7747:
7728:
7726:
7725:
7720:
7718:
7717:
7690:
7688:
7687:
7682:
7662:
7660:
7652:
7644:
7629:
7627:
7626:
7621:
7619:
7594:
7559:
7557:
7549:
7541:
7522:
7520:
7519:
7514:
7512:
7505:
7504:
7495:
7491:
7490:
7473:
7452:
7448:
7447:
7438:
7434:
7433:
7432:
7414:
7413:
7393:
7392:
7391:
7373:
7352:
7348:
7344:
7343:
7342:
7333:
7332:
7319:
7304:
7303:
7283:
7282:
7281:
7255:
7251:
7247:
7246:
7245:
7236:
7235:
7222:
7210:
7209:
7196:
7187:
7186:
7160:
7156:
7152:
7151:
7150:
7138:
7137:
7123:
7122:
7109:
7087:
7085:
7077:
7076:
7075:
7062:
7046:
7044:
7043:
7038:
7026:
7024:
7023:
7018:
7006:
7004:
7003:
6998:
6986:
6984:
6983:
6978:
6976:
6975:
6963:
6962:
6946:
6944:
6943:
6938:
6926:
6924:
6923:
6918:
6902:
6900:
6899:
6894:
6882:
6880:
6879:
6874:
6872:
6871:
6851:
6849:
6848:
6843:
6810:image processing
6800:
6798:
6797:
6792:
6787:
6785:
6784:
6775:
6692:
6689:
6671:
6669:
6668:
6667:
6654:
6650:
6649:
6639:
6615:
6613:
6612:
6609:{\displaystyle }
6607:
6580:
6578:
6577:
6574:{\displaystyle }
6572:
6548:
6546:
6545:
6540:
6528:
6526:
6525:
6520:
6479:Structure Tensor
6476:
6474:
6473:
6468:
6447:
6445:
6444:
6439:
6437:
6436:
6428:
6418:
6416:
6415:
6410:
6398:
6396:
6395:
6390:
6388:
6387:
6371:
6369:
6368:
6363:
6351:
6349:
6348:
6343:
6328:
6326:
6325:
6320:
6318:
6317:
6316:
6315:
6310:
6309:
6301:
6294:
6293:
6285:
6281:
6269:
6268:
6267:
6258:
6257:
6249:
6242:
6241:
6233:
6224:
6223:
6211:
6210:
6209:
6195:
6188:
6169:
6168:
6163:
6162:
6154:
6144:
6143:
6125:
6123:
6122:
6117:
6112:
6111:
6103:
6087:
6085:
6084:
6079:
6063:
6061:
6060:
6055:
6043:
6041:
6040:
6035:
6033:
6032:
6023:
6022:
6004:
6003:
5991:
5990:
5975:
5974:
5966:
5956:
5954:
5953:
5948:
5932:
5930:
5929:
5924:
5912:
5910:
5909:
5904:
5899:
5898:
5893:
5892:
5884:
5877:
5876:
5868:
5853:
5852:
5844:
5838:
5837:
5821:
5819:
5818:
5813:
5801:
5799:
5798:
5793:
5791:
5790:
5774:
5772:
5771:
5766:
5754:
5752:
5751:
5746:
5734:
5732:
5731:
5726:
5718:
5717:
5698:
5696:
5695:
5690:
5685:
5684:
5676:
5670:
5669:
5660:
5659:
5649:
5628:
5627:
5619:
5600:
5598:
5597:
5592:
5580:
5578:
5577:
5572:
5554:
5552:
5551:
5546:
5544:
5543:
5531:
5530:
5522:
5512:
5510:
5509:
5504:
5499:
5498:
5490:
5466:
5464:
5463:
5458:
5450:
5449:
5422:
5421:
5388:
5387:
5354:
5353:
5320:
5319:
5286:
5285:
5252:
5251:
5218:
5217:
5184:
5183:
5150:
5142:
5137:
5136:
5111:
5106:
5105:
5104:
5079:
5077:
5076:
5071:
5063:
5062:
5035:
5034:
5004:
5003:
4973:
4972:
4942:
4941:
4911:
4910:
4880:
4879:
4849:
4848:
4818:
4817:
4787:
4786:
4756:
4755:
4725:
4724:
4694:
4693:
4663:
4655:
4650:
4649:
4624:
4619:
4618:
4617:
4592:
4590:
4589:
4584:
4579:
4578:
4551:
4550:
4523:
4522:
4495:
4494:
4467:
4466:
4439:
4438:
4411:
4410:
4383:
4382:
4357:
4352:
4327:
4325:
4324:
4319:
4310:
4305:
4304:
4303:
4288:
4287:
4274:
4269:
4268:
4267:
4252:
4251:
4238:
4233:
4220:
4219:
4207:
4206:
4184:
4179:
4178:
4177:
4165:
4164:
4136:
4134:
4133:
4128:
4126:
4125:
4115:
4097:
4062:
4044:
4022:
4021:
3937:
3932:
3916:
3911:
3883:
3878:
3853:
3851:
3850:
3845:
3840:
3839:
3770:
3765:
3757:
3731:
3719:
3713:
3703:
3699:
3695:
3691:
3676:
3674:
3673:
3668:
3666:
3663:
3659:
3656:
3627:
3624:
3601:
3598:
3574:
3573:
3572:
3571:
3553:
3552:
3540:
3539:
3517:
3515:
3514:
3509:
3503:
3498:
3497:
3496:
3478:
3477:
3465:
3464:
3454:
3441:
3439:
3438:
3433:
3431:
3430:
3429:
3428:
3410:
3409:
3397:
3396:
3364:
3362:
3361:
3356:
3354:
3353:
3291:
3283:
3275:; third plane =
3274:
3272:
3271:
3266:
3264:
3263:
3198:
3190:
3181:
3179:
3178:
3173:
3171:
3170:
3108:
3100:
3087:27-point stencil
3079:
3077:
3076:
3071:
3069:
3068:
3000:; third plane =
2999:
2997:
2996:
2991:
2989:
2988:
2916:
2914:
2913:
2908:
2906:
2905:
2829:
2827:
2826:
2821:
2818:
2813:
2802:
2786:
2784:
2783:
2778:
2776:
2775:
2706:
2701:
2693:
2668:
2666:
2665:
2660:
2657:
2652:
2644:
2628:
2626:
2625:
2620:
2618:
2617:
2548:
2543:
2535:
2519:
2517:
2516:
2511:
2509:
2508:
2473:
2468:
2463:
2462:
2454:
2419:Image processing
2332:
2330:
2329:
2324:
2177:
2175:
2174:
2169:
2164:
2162:
2161:
2152:
2021:
1951:
1949:
1948:
1943:
1938:
1937:
1912:
1910:
1909:
1904:
1902:
1901:
1885:
1883:
1882:
1877:
1865:
1863:
1862:
1857:
1843:be the diagonal
1842:
1840:
1839:
1834:
1819:
1817:
1816:
1811:
1799:
1797:
1796:
1791:
1768:
1766:
1765:
1760:
1758:
1757:
1751:
1748:
1723:
1722:
1709:
1657:
1654:
1641:
1640:
1619:
1618:
1597:
1589:
1576:
1575:
1553:cotangent matrix
1551:be the (sparse)
1550:
1548:
1547:
1542:
1530:
1528:
1527:
1522:
1520:
1519:
1485:
1483:
1482:
1477:
1475:
1474:
1473:
1465:
1457:
1449:
1443:
1405:Laplace operator
1398:
1396:
1395:
1390:
1378:
1376:
1375:
1370:
1354:
1352:
1351:
1346:
1344:
1343:
1327:
1325:
1324:
1319:
1304:
1302:
1301:
1296:
1294:
1293:
1274:
1272:
1271:
1266:
1264:
1263:
1244:
1242:
1241:
1236:
1224:
1222:
1221:
1216:
1201:
1199:
1198:
1193:
1185:
1184:
1172:
1171:
1156:
1155:
1134:
1133:
1111:
1102:
1100:
1099:
1098:
1082:
1077:
1076:
1048:
1046:
1045:
1040:
1028:
1026:
1025:
1020:
992:
990:
989:
984:
966:
929:
927:
913:
870:
868:
867:
862:
841:
839:
838:
833:
831:
830:
808:
806:
805:
800:
798:
794:
761:
760:
747:
692:
691:
669:
667:
666:
661:
630:
628:
627:
622:
592:
590:
589:
584:
569:
567:
566:
561:
548:Laplacian matrix
537:
535:
534:
529:
499:
497:
496:
491:
489:
485:
451:
380:
378:
377:
372:
360:
358:
357:
352:
332:
330:
329:
324:
300:
298:
297:
292:
280:
278:
277:
272:
260:
258:
257:
252:
200:Graph Laplacians
177:image processing
150:Laplacian matrix
138:Laplace operator
121:
114:
110:
107:
101:
99:
58:
34:
26:
12220:
12219:
12215:
12214:
12213:
12211:
12210:
12209:
12180:Operator theory
12170:
12169:
12151:
12146:
12140:
12114:
12113:
12107:
12088:
12084:
12039:
12035:
11998:
11994:
11987:
11970:
11966:
11959:
11949:10.1007/b138918
11937:
11933:
11894:
11890:
11874:
11865:
11858:
11851:
11839:
11833:
11829:
11822:
11803:
11795:
11791:
11782:
11780:
11770:
11766:
11733:
11729:
11696:
11692:
11669:
11665:
11656:
11654:
11647:
11641:
11637:
11632:
11605:
11598:
11562:
11559:
11558:
11504:
11501:
11500:
11490:Dynkin diagrams
11486:
11480:
11446:
11442:
11398:
11395:
11394:
11371:
11368:
11367:
11345:
11342:
11341:
11302:
11298:
11280:
11276:
11274:
11271:
11270:
11267:Kronecker delta
11249:
11245:
11243:
11240:
11239:
11214:
11210:
11193:
11188:
11184:
11178:
11174:
11173:
11169:
11140:
11137:
11136:
11100:Stone's theorem
11087:is bounded and
11045:
11042:
11041:
10974:
10971:
10970:
10952:
10949:
10948:
10912:
10909:
10908:
10905:
10900:
10899:
10896:
10893:
10890:
10887:
10884:
10881:
10878:
10875:
10872:
10869:
10866:
10863:
10860:
10857:
10854:
10851:
10848:
10845:
10842:
10839:
10836:
10833:
10830:
10827:
10824:
10821:
10818:
10815:
10812:
10809:
10806:
10803:
10800:
10797:
10794:
10791:
10788:
10785:
10782:
10779:
10776:
10773:
10770:
10767:
10764:
10761:
10758:
10755:
10752:
10749:
10746:
10743:
10740:
10737:
10734:
10731:
10728:
10725:
10722:
10719:
10716:
10713:
10710:
10707:
10704:
10701:
10698:
10695:
10692:
10689:
10686:
10683:
10680:
10677:
10674:
10671:
10668:
10665:
10662:
10659:
10656:
10653:
10650:
10647:
10644:
10641:
10638:
10635:
10632:
10629:
10626:
10623:
10620:
10617:
10614:
10611:
10608:
10605:
10602:
10599:
10596:
10593:
10590:
10587:
10584:
10581:
10578:
10575:
10572:
10569:
10566:
10563:
10560:
10557:
10554:
10551:
10548:
10545:
10542:
10539:
10536:
10533:
10530:
10527:
10524:
10521:
10518:
10515:
10512:
10509:
10506:
10503:
10500:
10497:
10494:
10491:
10488:
10485:
10482:
10479:
10476:
10473:
10470:
10467:
10464:
10461:
10458:
10455:
10452:
10449:
10446:
10443:
10440:
10437:
10434:
10431:
10428:
10425:
10422:
10419:
10416:
10413:
10410:
10407:
10404:
10401:
10398:
10395:
10392:
10389:
10386:
10383:
10380:
10377:
10374:
10371:
10368:
10365:
10362:
10359:
10356:
10353:
10350:
10347:
10344:
10341:
10338:
10335:
10332:
10329:
10326:
10323:
10320:
10317:
10314:
10311:
10308:
10305:
10302:
10299:
10296:
10293:
10290:
10287:
10284:
10281:
10278:
10275:
10272:
10269:
10266:
10263:
10260:
10257:
10254:
10251:
10248:
10245:
10242:
10239:
10236:
10233:
10230:
10227:
10224:
10221:
10218:
10215:
10212:
10209:
10206:
10203:
10200:
10197:
10194:
10191:
10188:
10185:
10182:
10179:
10176:
10173:
10170:
10167:
10164:
10161:
10158:
10155:
10152:
10149:
10146:
10143:
10140:
10137:
10134:
10131:
10128:
10125:
10122:
10119:
10116:
10113:
10110:
10107:
10104:
10101:
10098:
10095:
10092:
10089:
10086:
10083:
10080:
10077:
10074:
10071:
10068:
10065:
10062:
10059:
10056:
10053:
10050:
10047:
10044:
10041:
10038:
10035:
10032:
10029:
10026:
10023:
10020:
10017:
10014:
10011:
10008:
10005:
10002:
9999:
9996:
9993:
9990:
9987:
9984:
9981:
9978:
9975:
9972:
9969:
9966:
9963:
9960:
9957:
9954:
9951:
9948:
9945:
9942:
9939:
9936:
9933:
9930:
9927:
9924:
9921:
9918:
9915:
9912:
9909:
9906:
9882:
9879:
9878:
9866:
9844:
9841:
9840:
9810:
9806:
9800:
9789:
9775:
9757:
9753:
9741:
9735:
9732:
9731:
9712:
9709:
9708:
9692:
9689:
9688:
9671:
9667:
9665:
9662:
9661:
9608:
9598:
9594:
9593:
9591:
9588:
9587:
9563:
9559:
9558:
9546:
9542:
9541:
9525:
9521:
9494:
9488:
9485:
9484:
9465:
9462:
9461:
9436:
9433:
9432:
9407:
9404:
9403:
9387:
9384:
9383:
9363:
9360:
9359:
9342:
9337:
9336:
9334:
9331:
9330:
9304:
9300:
9294:
9288:
9285:
9284:
9265:
9262:
9261:
9237:
9236:
9224:
9220:
9218:
9213:
9211:
9202:
9201:
9189:
9185:
9183:
9178:
9176:
9163:
9162:
9148:
9144:
9137:
9133:
9121:
9115:
9112:
9111:
9085:
9081:
9079:
9076:
9075:
9053:
9049:
9042:
9038:
9023:
9019:
9001:
8997:
8995:
8992:
8991:
8956:
8950:
8947:
8946:
8943:
8922:
8919:
8918:
8898:
8895:
8894:
8865:
8860:
8859:
8843:
8839:
8821:
8817:
8815:
8812:
8811:
8791:
8786:
8785:
8783:
8780:
8779:
8754:
8751:
8750:
8725:
8722:
8721:
8705:
8702:
8701:
8675:
8671:
8669:
8666:
8665:
8632:
8628:
8626:
8623:
8622:
8605:
8601:
8599:
8596:
8595:
8574:
8570:
8568:
8565:
8564:
8536:
8532:
8525:
8521:
8506:
8502:
8484:
8480:
8478:
8475:
8474:
8454:
8453:
8435:
8431:
8425:
8421:
8405:
8389:
8385:
8381:
8379:
8377:
8375:
8363:
8362:
8351:
8346:
8345:
8339:
8335:
8320:
8316:
8304:
8299:
8298:
8288:
8272:
8268:
8264:
8262:
8261:
8257:
8251:
8243:
8241:
8236:
8233:
8232:
8221:
8216:
8215:
8197:
8193:
8181:
8176:
8175:
8165:
8149:
8145:
8141:
8139:
8138:
8134:
8128:
8120:
8118:
8113:
8110:
8109:
8098:
8093:
8092:
8077:
8073:
8067:
8062:
8058:
8039:
8027:
8022:
8021:
8006:
8002:
7996:
7991:
7987:
7983:
7981:
7979:
7977:
7967:
7965:
7962:
7961:
7941:
7936:
7935:
7933:
7930:
7929:
7903:
7898:
7897:
7882:
7878:
7872:
7851:
7848:
7847:
7830:
7825:
7824:
7818:
7814:
7805:
7800:
7799:
7794:
7791:
7790:
7769:
7764:
7763:
7761:
7758:
7757:
7741:
7738:
7737:
7713:
7709:
7707:
7704:
7703:
7653:
7645:
7643:
7641:
7638:
7637:
7617:
7616:
7592:
7591:
7560:
7550:
7542:
7540:
7536:
7534:
7531:
7530:
7510:
7509:
7500:
7496:
7483:
7479:
7475:
7469:
7450:
7449:
7443:
7439:
7425:
7421:
7409:
7405:
7384:
7380:
7379:
7375:
7369:
7350:
7349:
7338:
7334:
7325:
7321:
7315:
7299:
7295:
7277:
7273:
7272:
7268:
7253:
7252:
7241:
7237:
7228:
7224:
7218:
7202:
7198:
7192:
7182:
7178:
7177:
7173:
7158:
7157:
7146:
7142:
7133:
7129:
7128:
7124:
7115:
7111:
7105:
7088:
7078:
7071:
7067:
7063:
7061:
7057:
7055:
7052:
7051:
7032:
7029:
7028:
7012:
7009:
7008:
6992:
6989:
6988:
6971:
6967:
6958:
6954:
6952:
6949:
6948:
6932:
6929:
6928:
6912:
6909:
6908:
6903:. According to
6888:
6885:
6884:
6867:
6863:
6861:
6858:
6857:
6837:
6834:
6833:
6830:
6780:
6776:
6693:
6691:
6679:
6663:
6659:
6655:
6645:
6641:
6640:
6638:
6636:
6633:
6632:
6622:
6586:
6583:
6582:
6554:
6551:
6550:
6534:
6531:
6530:
6502:
6499:
6498:
6491:
6462:
6459:
6458:
6427:
6426:
6424:
6421:
6420:
6404:
6401:
6400:
6383:
6379:
6377:
6374:
6373:
6357:
6354:
6353:
6337:
6334:
6333:
6311:
6300:
6299:
6298:
6284:
6283:
6282:
6277:
6276:
6260:
6259:
6248:
6247:
6246:
6232:
6231:
6219:
6215:
6202:
6201:
6197:
6181:
6180:
6164:
6153:
6152:
6151:
6139:
6135:
6133:
6130:
6129:
6102:
6101:
6093:
6090:
6089:
6073:
6070:
6069:
6049:
6046:
6045:
6028:
6024:
6018:
6014:
5999:
5995:
5986:
5982:
5965:
5964:
5962:
5959:
5958:
5942:
5939:
5938:
5918:
5915:
5914:
5894:
5883:
5882:
5881:
5867:
5866:
5843:
5842:
5833:
5829:
5827:
5824:
5823:
5807:
5804:
5803:
5786:
5782:
5780:
5777:
5776:
5760:
5757:
5756:
5740:
5737:
5736:
5713:
5709:
5707:
5704:
5703:
5675:
5674:
5665:
5661:
5655:
5651:
5639:
5618:
5617:
5609:
5606:
5605:
5586:
5583:
5582:
5560:
5557:
5556:
5539:
5535:
5521:
5520:
5518:
5515:
5514:
5489:
5488:
5480:
5477:
5476:
5473:
5433:
5429:
5396:
5392:
5362:
5358:
5328:
5324:
5294:
5290:
5260:
5256:
5226:
5222:
5192:
5188:
5158:
5154:
5141:
5120:
5116:
5107:
5100:
5096:
5095:
5086:
5083:
5082:
5046:
5042:
5012:
5008:
4981:
4977:
4950:
4946:
4919:
4915:
4888:
4884:
4857:
4853:
4826:
4822:
4795:
4791:
4764:
4760:
4733:
4729:
4702:
4698:
4671:
4667:
4654:
4633:
4629:
4620:
4613:
4609:
4608:
4599:
4596:
4595:
4562:
4558:
4531:
4527:
4503:
4499:
4475:
4471:
4447:
4443:
4419:
4415:
4391:
4387:
4366:
4362:
4353:
4348:
4339:
4336:
4335:
4306:
4299:
4295:
4294:
4283:
4279:
4270:
4263:
4259:
4258:
4247:
4243:
4234:
4229:
4215:
4211:
4202:
4198:
4180:
4173:
4169:
4160:
4156:
4155:
4149:
4146:
4145:
4120:
4119:
4111:
4106:
4101:
4093:
4087:
4086:
4081:
4073:
4067:
4066:
4058:
4053:
4048:
4040:
4030:
4029:
4016:
4015:
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1994:
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1986:, resulting in
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1419:(PDF download:
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997:Mesh Laplacians
934:
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886:
883:
882:
847:
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823:
819:
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813:
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306:
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111:
105:
102:
59:
57:
47:
35:
24:
17:
12:
11:
5:
12218:
12208:
12207:
12202:
12200:Edge detection
12197:
12192:
12187:
12182:
12168:
12167:
12165:
12163:on 2007-05-23.
12150:
12149:External links
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12105:
12082:
12033:
11992:
11986:978-0199206650
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11931:
11904:(4): 936–953.
11888:
11863:
11849:
11827:
11820:
11789:
11764:
11750:10.1.1.157.757
11743:(3): 381–390.
11727:
11713:10.1.1.157.757
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9750:
9747:
9744:
9740:
9720:{\textstyle j}
9716:
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9500:
9497:
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9473:{\textstyle N}
9469:
9449:
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9395:{\textstyle k}
9391:
9371:{\textstyle k}
9367:
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9273:{\textstyle L}
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8945:To understand
8942:
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8930:{\textstyle L}
8926:
8906:{\textstyle L}
8902:
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8713:{\textstyle i}
8709:
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8661:can be found.
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7040:{\textstyle k}
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7020:{\textstyle j}
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6940:{\textstyle j}
6936:
6920:{\textstyle i}
6916:
6896:{\textstyle i}
6892:
6870:
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6826:
6822:Laplace filter
6814:digital filter
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4723:
4720:
4717:
4714:
4711:
4708:
4705:
4701:
4697:
4692:
4689:
4686:
4683:
4680:
4677:
4674:
4670:
4666:
4661:
4658:
4653:
4648:
4645:
4642:
4639:
4636:
4632:
4628:
4623:
4616:
4612:
4607:
4603:
4593:
4582:
4577:
4574:
4571:
4568:
4565:
4561:
4557:
4554:
4549:
4546:
4543:
4540:
4537:
4534:
4530:
4526:
4521:
4518:
4515:
4512:
4509:
4506:
4502:
4498:
4493:
4490:
4487:
4484:
4481:
4478:
4474:
4470:
4465:
4462:
4459:
4456:
4453:
4450:
4446:
4442:
4437:
4434:
4431:
4428:
4425:
4422:
4418:
4414:
4409:
4406:
4403:
4400:
4397:
4394:
4390:
4386:
4381:
4378:
4375:
4372:
4369:
4365:
4361:
4356:
4351:
4347:
4343:
4329:
4328:
4317:
4314:
4309:
4302:
4298:
4293:
4286:
4282:
4278:
4273:
4266:
4262:
4257:
4250:
4246:
4242:
4237:
4232:
4228:
4223:
4218:
4214:
4210:
4205:
4201:
4197:
4194:
4191:
4188:
4183:
4176:
4172:
4168:
4163:
4159:
4154:
4138:
4137:
4124:
4118:
4114:
4110:
4107:
4105:
4102:
4100:
4096:
4092:
4089:
4088:
4085:
4082:
4080:
4077:
4074:
4072:
4069:
4068:
4065:
4061:
4057:
4054:
4052:
4049:
4047:
4043:
4039:
4036:
4035:
4033:
4028:
4025:
4020:
4014:
4011:
4009:
4006:
4004:
4001:
4000:
3997:
3994:
3992:
3989:
3986:
3984:
3981:
3980:
3977:
3974:
3972:
3969:
3967:
3964:
3963:
3961:
3956:
3953:
3950:
3947:
3944:
3941:
3936:
3931:
3927:
3923:
3920:
3915:
3910:
3906:
3902:
3899:
3896:
3893:
3890:
3887:
3882:
3877:
3873:
3855:
3854:
3843:
3838:
3832:
3829:
3827:
3824:
3822:
3819:
3818:
3815:
3812:
3810:
3807:
3804:
3802:
3799:
3798:
3795:
3792:
3790:
3787:
3785:
3782:
3781:
3779:
3774:
3769:
3764:
3761:
3756:
3736:Note that the
3734:
3733:
3726:
3725:
3722:
3716:
3710:
3705:
3687:
3686:
3683:
3679:
3678:
3677:
3665:
3654:
3652:
3649:
3648:
3645:
3642:
3639:
3636:
3633:
3630:
3622:
3620:
3617:
3616:
3613:
3610:
3607:
3604:
3596:
3594:
3591:
3588:
3585:
3584:
3581:
3577:
3570:
3566:
3562:
3559:
3556:
3551:
3547:
3543:
3538:
3534:
3529:
3507:
3502:
3495:
3491:
3487:
3484:
3481:
3476:
3472:
3468:
3463:
3459:
3453:
3442:of the kernel
3427:
3423:
3419:
3416:
3413:
3408:
3404:
3400:
3395:
3391:
3386:
3371:
3368:
3367:
3366:
3352:
3346:
3343:
3341:
3338:
3336:
3333:
3332:
3329:
3326:
3324:
3321:
3319:
3316:
3315:
3312:
3309:
3307:
3304:
3302:
3299:
3298:
3296:
3289:
3286:
3262:
3256:
3253:
3251:
3248:
3246:
3243:
3242:
3239:
3236:
3234:
3231:
3228:
3226:
3223:
3222:
3219:
3216:
3214:
3211:
3209:
3206:
3205:
3203:
3196:
3193:
3169:
3163:
3160:
3158:
3155:
3153:
3150:
3149:
3146:
3143:
3141:
3138:
3136:
3133:
3132:
3129:
3126:
3124:
3121:
3119:
3116:
3115:
3113:
3106:
3103:
3092:first plane =
3083:
3082:
3081:
3067:
3061:
3058:
3056:
3053:
3051:
3048:
3047:
3044:
3041:
3039:
3036:
3034:
3031:
3030:
3027:
3024:
3022:
3019:
3017:
3014:
3013:
3011:
2987:
2981:
2978:
2976:
2973:
2971:
2968:
2967:
2964:
2961:
2959:
2956:
2953:
2951:
2948:
2947:
2944:
2941:
2939:
2936:
2934:
2931:
2930:
2928:
2904:
2898:
2895:
2893:
2890:
2888:
2885:
2884:
2881:
2878:
2876:
2873:
2871:
2868:
2867:
2864:
2861:
2859:
2856:
2854:
2851:
2850:
2848:
2837:first plane =
2817:
2812:
2809:
2806:
2801:
2788:
2774:
2768:
2765:
2763:
2760:
2758:
2755:
2754:
2751:
2748:
2746:
2743:
2740:
2738:
2735:
2734:
2731:
2728:
2726:
2723:
2721:
2718:
2717:
2715:
2710:
2705:
2700:
2697:
2692:
2656:
2651:
2648:
2643:
2631:
2630:
2616:
2610:
2607:
2605:
2602:
2600:
2597:
2596:
2593:
2590:
2588:
2585:
2582:
2580:
2577:
2576:
2573:
2570:
2568:
2565:
2563:
2560:
2559:
2557:
2552:
2547:
2542:
2539:
2534:
2521:
2507:
2501:
2498:
2496:
2493:
2490:
2488:
2485:
2484:
2482:
2477:
2472:
2467:
2460:
2457:
2433:
2430:
2420:
2417:
2411:
2408:
2392:Kronecker sums
2334:
2333:
2322:
2319:
2316:
2313:
2310:
2307:
2304:
2301:
2298:
2295:
2292:
2289:
2286:
2283:
2280:
2277:
2274:
2271:
2268:
2265:
2262:
2259:
2256:
2253:
2250:
2247:
2244:
2241:
2238:
2235:
2232:
2229:
2226:
2223:
2220:
2217:
2214:
2211:
2208:
2205:
2179:
2178:
2167:
2160:
2156:
2151:
2148:
2145:
2142:
2139:
2136:
2133:
2130:
2127:
2124:
2121:
2118:
2115:
2112:
2109:
2106:
2103:
2100:
2097:
2094:
2091:
2088:
2085:
2082:
2079:
2076:
2073:
2070:
2067:
2064:
2061:
2058:
2055:
2052:
2049:
2046:
2043:
2040:
2037:
2034:
2031:
2028:
2025:
2019:
2016:
2013:
2010:
2007:
2004:
2001:
1998:
1960:
1957:
1941:
1936:
1933:
1929:
1925:
1922:
1900:
1896:
1875:
1855:
1832:
1809:
1789:
1786:
1783:
1780:
1756:
1746:
1744:
1741:
1740:
1737:
1734:
1731:
1728:
1725:
1721:
1718:
1714:
1708:
1705:
1702:
1699:
1696:
1693:
1689:
1685:
1682:
1681:
1678:
1675:
1672:
1669:
1666:
1663:
1660:
1652:
1649:
1646:
1644:
1639:
1636:
1632:
1628:
1625:
1622:
1617:
1614:
1610:
1606:
1603:
1600:
1595:
1592:
1587:
1586:
1584:
1579:
1574:
1571:
1567:
1540:
1518:
1514:
1510:
1507:
1504:
1501:
1498:
1495:
1472:
1468:
1464:
1460:
1456:
1452:
1448:
1442:
1437:
1434:
1413:finite volumes
1388:
1368:
1342:
1338:
1317:
1314:
1292:
1289:
1285:
1262:
1259:
1255:
1234:
1214:
1203:
1202:
1191:
1188:
1183:
1179:
1175:
1170:
1166:
1162:
1159:
1154:
1151:
1147:
1143:
1140:
1137:
1132:
1129:
1125:
1121:
1118:
1115:
1110:
1106:
1097:
1093:
1089:
1085:
1080:
1075:
1071:
1067:
1064:
1061:
1038:
1018:
998:
995:
994:
993:
982:
979:
976:
973:
970:
965:
962:
959:
956:
953:
950:
947:
944:
940:
937:
933:
926:
923:
920:
916:
911:
908:
905:
902:
899:
896:
893:
890:
860:
857:
854:
851:
829:
826:
822:
810:
809:
797:
793:
790:
787:
784:
781:
778:
775:
772:
769:
765:
759:
756:
752:
746:
743:
740:
737:
734:
731:
728:
725:
721:
718:
714:
710:
707:
704:
701:
698:
695:
690:
686:
682:
659:
656:
653:
650:
647:
620:
617:
614:
611:
608:
605:
602:
582:
579:
559:
540:graph distance
527:
524:
521:
518:
515:
512:
501:
500:
488:
484:
481:
478:
475:
472:
469:
466:
463:
460:
456:
450:
447:
444:
441:
438:
435:
432:
429:
425:
422:
418:
414:
411:
408:
405:
402:
399:
396:
393:
381:is defined by
370:
350:
322:
319:
316:
313:
310:
290:
270:
250:
247:
244:
241:
238:
235:
232:
201:
198:
196:
193:
181:Laplace filter
124:
123:
38:
36:
29:
15:
9:
6:
4:
3:
2:
12217:
12206:
12203:
12201:
12198:
12196:
12193:
12191:
12188:
12186:
12183:
12181:
12178:
12177:
12175:
12166:
12162:
12158:
12153:
12152:
12141:
12135:
12131:
12130:
12125:
12121:
12117:
12116:
12108:
12102:
12098:
12097:
12092:
12086:
12078:
12074:
12069:
12064:
12060:
12056:
12052:
12048:
12044:
12037:
12028:
12023:
12019:
12015:
12011:
12007:
12003:
11996:
11988:
11982:
11978:
11974:
11968:
11960:
11954:
11950:
11946:
11942:
11935:
11927:
11923:
11919:
11915:
11911:
11907:
11903:
11899:
11892:
11885:
11884:0-7923-9418-6
11881:
11877:
11872:
11870:
11868:
11861:
11856:
11854:
11845:
11838:
11831:
11823:
11817:
11813:
11809:
11802:
11801:
11793:
11779:
11775:
11768:
11760:
11756:
11751:
11746:
11742:
11738:
11731:
11723:
11719:
11714:
11709:
11705:
11701:
11694:
11686:
11682:
11678:
11674:
11667:
11653:
11646:
11639:
11635:
11625:
11622:
11620:
11617:
11615:
11612:
11610:
11607:
11606:
11600:
11579:
11576:
11573:
11570:
11567:
11557:
11556:
11555:
11549:
11548:
11547:
11544:
11537:
11536:
11535:
11518:
11515:
11512:
11509:
11499:
11498:
11497:
11495:
11491:
11485:
11461:
11455:
11447:
11443:
11439:
11433:
11430:
11427:
11424:
11421:
11415:
11409:
11406:
11403:
11393:
11392:
11391:
11389:
11373:
11353:
11350:
11347:
11338:
11336:
11332:
11328:
11324:
11306:
11303:
11299:
11295:
11289:
11281:
11277:
11268:
11250:
11246:
11221:
11215:
11211:
11206:
11200:
11197:
11194:
11190:
11185:
11179:
11175:
11170:
11166:
11160:
11157:
11154:
11151:
11148:
11142:
11135:
11134:
11133:
11131:
11127:
11123:
11118:
11116:
11111:
11109:
11105:
11101:
11097:
11092:
11090:
11086:
11081:
11079:
11075:
11059:
11056:
11050:
11047:
11024:
11018:
11012:
11006:
11000:
10997:
10991:
10982:
10979:
10969:
10968:
10967:
10954:
10946:
10942:
10926:
10920:
10917:
10914:
10864:'gif'
10807:'gif'
9903:
9899:
9884:
9870:
9861:
9846:
9819:
9811:
9807:
9801:
9796:
9793:
9790:
9786:
9780:
9777:
9772:
9766:
9758:
9754:
9742:
9730:
9729:
9728:
9714:
9694:
9672:
9668:
9641:
9638:
9635:
9632:
9629:
9626:
9623:
9614:
9610:
9605:
9586:
9585:
9584:
9554:
9538:
9532:
9526:
9522:
9518:
9512:
9506:
9495:
9483:
9482:
9481:
9467:
9444:
9438:
9429:
9415:
9412:
9409:
9389:
9381:
9365:
9343:
9329:, the vector
9316:
9313:
9308:
9305:
9301:
9295:
9291:
9281:
9267:
9259:
9233:
9230:
9225:
9221:
9208:
9205:
9198:
9195:
9190:
9186:
9173:
9170:
9164:
9159:
9154:
9149:
9145:
9141:
9138:
9134:
9122:
9110:
9109:
9108:
9094:
9091:
9086:
9082:
9059:
9054:
9050:
9046:
9043:
9039:
9032:
9024:
9020:
9016:
9010:
9002:
8998:
8974:
8968:
8957:
8938:
8924:
8916:
8900:
8891:
8872:
8866:
8856:
8850:
8844:
8840:
8836:
8830:
8822:
8818:
8810:
8809:
8808:
8792:
8762:
8756:
8733:
8727:
8707:
8684:
8676:
8672:
8662:
8660:
8641:
8633:
8629:
8606:
8602:
8593:
8575:
8571:
8547:
8542:
8537:
8533:
8529:
8526:
8522:
8515:
8507:
8503:
8499:
8493:
8485:
8481:
8473:
8472:
8471:
8450:
8444:
8436:
8432:
8426:
8422:
8418:
8415:
8409:
8406:
8398:
8390:
8386:
8382:
8372:
8369:
8358:
8352:
8340:
8336:
8329:
8321:
8317:
8313:
8310:
8305:
8292:
8289:
8281:
8273:
8269:
8265:
8258:
8252:
8248:
8245:
8238:
8228:
8222:
8212:
8206:
8198:
8194:
8190:
8187:
8182:
8169:
8166:
8158:
8150:
8146:
8142:
8135:
8129:
8125:
8122:
8115:
8105:
8099:
8086:
8078:
8074:
8068:
8064:
8059:
8055:
8052:
8049:
8043:
8040:
8034:
8028:
8015:
8007:
8003:
7997:
7993:
7988:
7984:
7974:
7971:
7960:
7959:
7958:
7942:
7927:
7922:
7909:
7904:
7891:
7883:
7879:
7873:
7869:
7865:
7859:
7853:
7831:
7819:
7815:
7811:
7806:
7796:
7788:
7770:
7743:
7735:
7730:
7714:
7701:
7697:
7696:heat equation
7678:
7675:
7672:
7669:
7666:
7663:
7657:
7654:
7649:
7646:
7636:
7635:
7634:
7613:
7610:
7607:
7604:
7601:
7598:
7596:
7588:
7582:
7579:
7576:
7570:
7567:
7564:
7562:
7554:
7551:
7546:
7543:
7529:
7528:
7527:
7506:
7501:
7497:
7492:
7487:
7484:
7480:
7476:
7470:
7466:
7462:
7459:
7456:
7454:
7444:
7440:
7435:
7429:
7426:
7422:
7418:
7410:
7406:
7399:
7396:
7388:
7385:
7381:
7376:
7370:
7366:
7362:
7359:
7356:
7354:
7345:
7339:
7335:
7329:
7326:
7322:
7316:
7312:
7308:
7300:
7296:
7289:
7286:
7278:
7274:
7269:
7265:
7262:
7259:
7257:
7248:
7242:
7238:
7232:
7229:
7225:
7219:
7215:
7211:
7206:
7203:
7199:
7193:
7189:
7183:
7179:
7174:
7170:
7167:
7164:
7162:
7153:
7147:
7143:
7139:
7134:
7130:
7125:
7119:
7116:
7112:
7106:
7102:
7098:
7095:
7092:
7090:
7082:
7079:
7072:
7068:
7064:
7050:
7049:
7048:
7034:
7014:
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5935:sinc function
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2835:
2834:is given by:
2833:
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2397:
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2388:regular grids
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2165:
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2128:
2122:
2119:
2116:
2113:
2110:
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2101:
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2086:
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2074:
2068:
2065:
2062:
2059:
2056:
2050:
2047:
2041:
2038:
2035:
2032:
2029:
2023:
2017:
2011:
2008:
2005:
1999:
1989:
1988:
1987:
1985:
1982:
1978:
1974:
1970:
1966:
1956:
1953:
1939:
1934:
1931:
1927:
1923:
1920:
1898:
1894:
1873:
1853:
1846:
1830:
1821:
1807:
1784:
1778:
1769:
1742:
1735:
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1726:
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1703:
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1676:
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1612:
1608:
1604:
1601:
1593:
1590:
1582:
1577:
1572:
1569:
1565:
1556:
1555:with entries
1554:
1538:
1516:
1508:
1499:
1496:
1493:
1466:
1458:
1450:
1435:
1432:
1423:
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1418:
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1406:
1402:
1386:
1366:
1358:
1340:
1336:
1315:
1312:
1290:
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1260:
1257:
1253:
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1212:
1189:
1181:
1177:
1173:
1168:
1164:
1152:
1149:
1145:
1141:
1138:
1135:
1130:
1127:
1123:
1119:
1116:
1108:
1104:
1095:
1091:
1087:
1083:
1078:
1073:
1065:
1052:
1051:
1050:
1036:
1016:
1008:
1004:
980:
974:
968:
963:
960:
954:
951:
948:
942:
938:
935:
931:
924:
921:
918:
914:
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903:
894:
891:
881:
880:
879:
877:
872:
858:
855:
852:
849:
827:
824:
820:
795:
788:
782:
779:
773:
767:
763:
757:
754:
750:
744:
741:
735:
732:
729:
723:
719:
716:
712:
708:
702:
693:
688:
673:
672:
671:
657:
651:
648:
645:
636:
634:
615:
606:
580:
557:
549:
545:
541:
522:
519:
516:
510:
486:
479:
473:
470:
464:
458:
454:
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445:
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427:
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416:
412:
406:
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384:
383:
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368:
340:
336:
320:
314:
311:
308:
288:
268:
245:
242:
239:
233:
230:
221:
219:
215:
214:regular graph
211:
207:
192:
190:
186:
182:
178:
174:
170:
166:
162:
158:
153:
151:
147:
146:discrete grid
143:
139:
135:
131:
120:
117:
109:
106:December 2007
98:
95:
91:
88:
84:
81:
77:
74:
70:
67: –
66:
62:
61:Find sources:
55:
51:
45:
44:
39:This article
37:
33:
28:
27:
22:
12185:Graph theory
12161:the original
12128:
12095:
12085:
12050:
12046:
12036:
12009:
12005:
11995:
11976:
11973:Newman, Mark
11967:
11943:. Springer.
11940:
11934:
11901:
11897:
11891:
11843:
11830:
11799:
11792:
11781:. Retrieved
11777:
11774:"LoG Filter"
11767:
11740:
11736:
11730:
11703:
11699:
11693:
11676:
11666:
11655:. Retrieved
11651:
11638:
11594:
11553:
11545:
11541:
11533:
11487:
11387:
11339:
11334:
11330:
11326:
11322:
11237:
11119:
11112:
11093:
11089:self-adjoint
11084:
11082:
11073:
11039:
10944:
10906:
9902:conditions.
9900:
9876:
9838:
9659:
9582:
9430:
9402:independent
9282:
9255:
8944:
8892:
8889:
8663:
8658:
8591:
8562:
8469:
7925:
7923:
7786:
7731:
7699:
7693:
7633:which gives
7632:
7525:
6831:
6803:
6623:
6492:
6331:
5701:
5474:
4330:
4139:
3859:
3856:
3737:
3735:
3370:
2632:
2435:
2422:
2413:
2404:eigenvectors
2382:
2373:
2369:
2365:
2357:
2353:
2349:
2341:
2337:
2335:
2190:
2186:
2182:
2180:
1976:
1962:
1954:
1844:
1822:
1770:
1557:
1552:
1424:
1356:
1204:
1029:at a vertex
1000:
875:
873:
811:
637:
632:
631:is just the
543:
502:
222:
217:
205:
203:
154:
133:
127:
112:
103:
93:
86:
79:
72:
60:
48:Please help
43:verification
40:
11337:otherwise.
9946:% The image
6818:edge filter
5937:defined in
3745:2D filter:
2790:3D filter:
2681:2D filter:
2523:2D filter:
2444:1D filter:
2438:convolution
2400:eigenvalues
1845:mass matrix
1357:vertex area
550:. That is,
195:Definitions
161:Ising model
130:mathematics
21:Z-transform
12174:Categories
12120:Sunada, T.
12053:: 122112.
12012:: 106383.
11783:2019-12-01
11657:2019-12-01
11630:References
11534:in words,
11340:For fixed
10192:&&
10180:&&
10168:&&
3720:for which
3657:otherwise,
3085:and using
1971:or by the
1486:such that
361:acting on
281:and edges
185:clustering
76:newspapers
12093:(2002) ,
12077:244652819
11926:123145969
11918:0749-159X
11745:CiteSeerX
11708:CiteSeerX
11577:−
11574:ϕ
11568:ϕ
11565:Δ
11516:ϕ
11510:ϕ
11507:Δ
11444:δ
11434:λ
11410:λ
11407:−
11374:λ
11351:∈
11300:δ
11278:δ
11247:δ
11212:δ
11201:λ
11198:−
11176:δ
11161:λ
11054:Δ
11013:ϕ
10983:ϕ
10955:ϕ
10941:potential
10924:→
10918::
9885:ϕ
9847:ϕ
9787:∑
9755:ϕ
9749:∞
9746:→
9695:ϕ
9669:ϕ
9636:…
9507:ϕ
9502:∞
9499:→
9480:vertices
9410:λ
9378:disjoint
9292:∑
9222:λ
9187:λ
9146:λ
9139:−
9129:∞
9126:→
9083:λ
9051:λ
9044:−
8969:ϕ
8964:∞
8961:→
8845:ϕ
8757:ϕ
8728:ϕ
8700:for each
8603:λ
8572:λ
8534:λ
8527:−
8423:λ
8367:⇒
8337:λ
8249:∑
8126:∑
8065:∑
7994:∑
7870:∑
7854:ϕ
7816:λ
7789:(so that
7744:ϕ
7711:∇
7673:ϕ
7650:ϕ
7611:ϕ
7602:−
7589:ϕ
7580:−
7568:−
7547:ϕ
7498:ϕ
7467:∑
7460:−
7441:ϕ
7419:−
7400:
7382:δ
7367:∑
7360:−
7336:ϕ
7313:∑
7309:−
7290:
7275:ϕ
7263:−
7239:ϕ
7216:∑
7212:−
7190:∑
7180:ϕ
7168:−
7144:ϕ
7140:−
7131:ϕ
7103:∑
7096:−
7069:ϕ
6987:if nodes
6969:ϕ
6965:−
6956:ϕ
6865:ϕ
6840:ϕ
6778:ϵ
6767:ϵ
6764:−
6752:−
6734:−
6716:−
6710:ϵ
6684:→
6681:ϵ
6657:∂
6643:∂
6592:−
6514:−
6505:Δ
6433:¯
6306:¯
6290:¯
6254:¯
6244:−
6238:¯
6226:μ
6217:∇
6190:∈
6178:∑
6159:¯
6137:∇
6108:¯
6052:μ
5971:¯
5921:μ
5889:¯
5879:−
5873:¯
5861:μ
5849:¯
5831:μ
5784:μ
5720:∈
5681:¯
5663:μ
5644:∈
5637:∑
5624:¯
5566:∈
5533:∈
5527:¯
5495:¯
5424:−
5382:−
5339:−
5314:−
5305:−
5262:−
5246:−
5228:−
5203:−
5194:−
5178:−
5169:−
5160:−
5098:×
5093:∇
5037:−
4998:−
4958:−
4936:−
4927:−
4874:−
4828:−
4812:−
4797:−
4744:−
4704:−
4682:−
4673:−
4606:∇
4553:−
4517:−
4455:−
4393:−
4346:∇
4297:×
4292:∇
4281:γ
4256:∇
4245:γ
4227:∇
4213:γ
4209:−
4200:γ
4196:−
4171:γ
4158:γ
4153:∇
4076:−
4027:γ
3988:−
3952:γ
3949:−
3930:×
3926:∇
3922:γ
3905:∇
3898:γ
3895:−
3876:γ
3872:∇
3806:−
3638:−
3587:−
3558:…
3483:…
3415:…
3230:−
2955:−
2742:−
2584:−
2492:−
2459:→
2285:−
2213:−
2129:−
2093:−
2033:−
2018:≈
1997:Δ
1965:Laplacian
1932:−
1749:otherwise
1695:∈
1688:∑
1684:−
1662:∈
1631:β
1627:
1609:α
1605:
1506:Δ
1459:×
1436:∈
1284:β
1254:α
1174:−
1146:β
1142:
1124:α
1120:
1105:∑
1079:≡
1063:Δ
969:ϕ
932:∑
922:
895:ϕ
856:∈
821:γ
783:ϕ
780:−
768:ϕ
751:γ
713:∑
694:ϕ
689:γ
685:Δ
655:→
649::
646:γ
607:ϕ
604:Δ
581:ϕ
578:Δ
558:ϕ
474:ϕ
471:−
459:ϕ
417:∑
398:ϕ
395:Δ
369:ϕ
349:Δ
318:→
312::
309:ϕ
12122:(2008).
11975:(2010).
11603:See also
11222:⟩
11171:⟨
10738:frame2im
10720:getframe
9555:⟩
9523:⟨
9107:, since
8873:⟩
8841:⟨
8664:To find
6927:to node
6856:, where
6832:Suppose
6620:Theorems
6489:Spectrum
6265:′
6207:′
6186:′
5755:on grid
3625:if
3599:if
3374:D filter
2342:negative
1823:And let
1003:manifold
335:function
218:negative
12055:Bibcode
12014:Bibcode
11846:: 1–16.
11072:is the
10840:imwrite
10783:imwrite
10753:rgb2ind
10696:sprintf
10672:imagesc
10645:reshape
6808:and in
2189:,
1913:. Then
1355:is the
538:is the
157:physics
90:scholar
12136:
12103:
12075:
11983:
11955:
11924:
11916:
11882:
11818:
11747:
11710:
11238:where
11104:posets
10540:'*
10252:index2
10204:index2
10096:length
9583:where
9258:kernel
7394:
7284:
6481:, and
5702:where
4331:where
3681:where
2830:using
1866:whose
1771:Where
1531:. Let
1415:, and
1328:, and
812:where
503:where
301:. Let
210:graphs
132:, the
92:
85:
78:
71:
63:
12073:S2CID
11922:S2CID
11840:(PDF)
11804:(PDF)
11648:(PDF)
11040:Then
10939:be a
10846:imind
10789:imind
10744:frame
10714:frame
10690:title
10684:caxis
10384:zeros
10246:index
10198:<=
10174:<=
10045:index
9955:zeros
9928:zeros
6854:graph
6399:, in
5913:with
333:be a
144:or a
142:graph
97:JSTOR
83:books
12134:ISBN
12101:ISBN
11981:ISBN
11953:ISBN
11914:ISSN
11880:ISBN
11816:ISBN
11366:and
11333:and
11132:by
11120:The
11106:and
11094:The
10907:Let
10837:else
10570:0.05
10528:(:);
10360:diag
10288:diag
10234:newy
10213:newx
10195:newy
10186:>
10183:newy
10171:newx
10162:>
10159:newx
10132:newy
10108:newx
9196:>
7007:and
5775:and
3089:by:
2767:0.25
2757:0.25
2730:0.25
2720:0.25
2402:and
1275:and
339:ring
223:Let
208:for
187:and
163:and
69:news
12063:doi
12051:183
12022:doi
12010:153
11945:doi
11906:doi
11808:doi
11755:doi
11718:doi
11681:doi
11325:if
10897:end
10894:end
10888:0.1
10831:0.1
10819:inf
10765:256
10711:));
10687:();
10678:Phi
10651:Phi
10639:Phi
10630:Phi
10618:Phi
10594:exp
10588:C0V
10582:Phi
10555:for
10531:C0V
10339:eig
10327:Adj
10321:Deg
10309:));
10300:Adj
10294:sum
10282:Deg
10276:end
10273:end
10270:end
10267:end
10240:Adj
10081:for
10027:for
10009:for
9949:Adj
9739:lim
9687:of
9492:lim
9260:of
9119:lim
8954:lim
8590:of
7785:of
7397:deg
7287:deg
6677:lim
6529:on
6068:in
3730:= 0
3700:or
2762:0.5
2750:0.5
2737:0.5
2725:0.5
1624:cot
1602:cot
1422:).
1359:of
1225:of
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1117:cot
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128:In
52:by
12176::
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11920:.
11912:.
11902:22
11900:.
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11866:^
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11814:.
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11739:.
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11650:.
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11110:.
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11080:.
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10852:cm
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10591:.*
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9280:.
9215:if
9180:if
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7047:,
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10977:(
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10816:,
10810:,
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10741:(
10735:=
10726:1
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10699:(
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10675:(
10663:N
10660:,
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10633:;
10627:*
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10414:5
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10390:N
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10315:L
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10243:(
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10228:N
10225:*
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10219:1
10216:-
10210:(
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10123:(
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10114:x
10111:=
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10078:;
10075:y
10072:+
10069:N
10066:*
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10051:(
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10042:N
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10030:y
10024:N
10021::
10018:1
10015:=
10012:x
10006:;
10003:=
9997:;
9994:=
9979:N
9976:*
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9967:N
9964:*
9961:N
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9952:=
9940:N
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9934:N
9931:(
9925:=
9922:A
9916:;
9910:=
9907:N
9835:.
9823:)
9820:0
9817:(
9812:i
9808:c
9802:N
9797:1
9794:=
9791:i
9781:N
9778:1
9773:=
9770:)
9767:t
9764:(
9759:j
9743:t
9715:j
9673:j
9645:]
9642:1
9639:,
9633:,
9630:1
9627:,
9624:1
9621:[
9615:N
9611:1
9606:=
9600:1
9596:v
9565:1
9561:v
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9544:v
9539:,
9536:)
9533:0
9530:(
9527:c
9519:=
9516:)
9513:t
9510:(
9496:t
9468:N
9448:)
9445:0
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9439:c
9416:0
9413:=
9390:k
9366:k
9344:1
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9317:0
9314:=
9309:j
9306:i
9302:L
9296:j
9268:L
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9231:=
9226:i
9209:,
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9174:,
9171:0
9165:{
9160:=
9155:t
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9142:k
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9095:0
9092:=
9087:i
9060:t
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9040:e
9036:)
9033:0
9030:(
9025:i
9021:c
9017:=
9014:)
9011:t
9008:(
9003:i
8999:c
8978:)
8975:t
8972:(
8958:t
8925:L
8901:L
8886:.
8867:i
8862:v
8857:,
8854:)
8851:0
8848:(
8837:=
8834:)
8831:0
8828:(
8823:i
8819:c
8793:i
8788:v
8766:)
8763:0
8760:(
8737:)
8734:0
8731:(
8708:i
8688:)
8685:0
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8659:t
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8639:(
8634:i
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8516:0
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8314:k
8311:+
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8282:t
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8259:[
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8239:=
8229:]
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8218:v
8213:L
8210:)
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8116:=
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8100:i
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8087:t
8084:(
8079:i
8075:c
8069:i
8060:(
8056:L
8053:k
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8029:i
8024:v
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8016:t
8013:(
8008:i
8004:c
7998:i
7989:(
7985:d
7975:=
7972:0
7943:i
7938:v
7926:L
7910:.
7905:i
7900:v
7895:)
7892:t
7889:(
7884:i
7880:c
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7866:=
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7860:t
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7820:i
7812:=
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7797:L
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7700:L
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7670:L
7667:k
7664:+
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7614:,
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7599:=
7586:)
7583:A
7577:D
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7565:=
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7544:d
7507:.
7502:j
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6789:.
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6731:]
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6569:]
6566:2
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6560:0
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6537:Z
6517:M
6511:I
6508:=
6465:n
6453:/
6430:r
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6381:f
6360:f
6340:K
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5977:=
5968:r
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5840:(
5835:k
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5419:1
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4657:1
4652:=
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925:v
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910:=
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796:]
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771:(
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742:=
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720::
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709:=
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703:v
700:(
697:)
681:(
658:R
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619:)
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613:(
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601:(
544:v
526:)
523:v
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514:(
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487:]
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477:(
468:)
465:v
462:(
455:[
449:1
446:=
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440:v
437:,
434:w
431:(
428:d
424::
421:w
413:=
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407:v
404:(
401:)
392:(
321:R
315:V
289:E
269:V
249:)
246:E
243:,
240:V
237:(
234:=
231:G
119:)
113:(
108:)
104:(
94:·
87:·
80:·
73:·
46:.
23:.
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