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Vector Subspaces

If a subset W of a vector space V satisfies the definition of a vector space, with addition and scalar multiplication defined by the same operation as in V, then W is called a vector subspace or, more succinctly, a subspace of V. For example, the trivial subspace 0 is a subspace of any vector space. [Pg.45]

Exercise 3.23 Show that C ([—1, 1]) is a complex vector space. Show that the set of complex-valued polynomials in one variable is a vector subspace. Show that the bracket ( , ) (defined as in Section 3.2) is a complex scalar product on C ([—1, 1]). [Pg.108]

Note that HomG(T, IT) is a vector subspace of Hoin(V. IT). Also, its ele-... [Pg.169]

We know from numerous experiments that every quantum system has elementary states. An elementary state of a quantum system should be observer-independent. In other words, any observer should be able (in theory) to recognize that state experimentally, and the observations should all agree. Second, an elementary state should be indivisible. That is. one should not be able to think of the elementary state as a superposition of two or more more elementary states. If we accept the model that every recognizable state corresponds to a vector subspace of the state space of the system, then we can conclude that elementary states correspond to irreducible representations. The independence of the choice of observer compels the subspace to be invariant under the representahon. The indivisible nature of the subspace requires the subspace to be irreducible. So elementary states correspond to irreducible representations. More specifically, if a vector w represents an elementary state, then w should lie in an irreducible invariant subspace W, that is, a subspace whose only invariant subspaces are itself and 0. In fact, every vector in W represents a state indistinguishable from w, as a consequence of Exercise 6.6. [Pg.186]

Consider the grassmannian G G V) of N-dimenstonal vector subspaces of V. Let ST c V8tOe be the tautological locally free sheaf of rank N and... [Pg.81]

The following terminology is important The set ft = z,... xt of vectors x, 6 S is linearly dependent, iff there exists a set of scalars a,. ..at, not all zero, such that orixi + —h a = 0. If this is not possible, then the vectors are linearly independent. A vector x, for which a, 0 is one of the linearly dependent vectors. The set of vectors defines a vector subspace S, of S, called span(ft), which consists of all possible vectors z = aix, + —h atzt. This definition also provides a mapping from the array., a ) e Rk to the vector space span(ft). If ft is a linearly independent set, then the dimension of S, is k, and then the vectors constitutes a basis set in Si. If it is linearly dependent, then there is a subset fti 6 ft of size ki = card (ft,) which is linearly independent and spans the same space. Then ki is the dimension of S,. [Pg.4]

With T(GS> and T, one has the opportunity of removing from consideration any vector subspace containing near-null vectors, i.e., such vectors v that Sv w o. (There may be some difficulty in practice, if a library subroutine was used instead of handcoding, in the case of t(gs1). [Pg.24]

The general statements regarding the transversality of the intersections of submanifolds are stated in terms of the properties of the intersections of their associated tangent hyperplanes. These are vector subspaces, a plane or line spanned by a corresponding set of gradient vectors, not necessarily at the origin of the coordinate system. Such a vector subspace is called an affine subspace. [Pg.92]

Most techniques for solving large eigenvalue problems fall under the category of subspace iteration methods, which iteratively solve the eigenvalue problem in a linear vector subspace spanned by only a few vectors. Malmqvist173 provides a concise review of the subspace iteration methods most commonly found in quantum chemistry. Here we will outline some of these methods and note recent advances. [Pg.182]

A subspace of a vector space is a nonempty subset that is also a vector space. That is, vector subspaces also obey the laws of vector addition and scalar multiplication. If x and y are two vectors that lie in a vector subspace, then linear combinations of x and y will produce vectors that also lie in the subspace. For example, linear combinations of vectors [0, 0, 1] and [2, 0, 0] produce vectors that lie in a two-dimensional subspace (a plane) in R linear combinations of vector [5, 0.2, -3, 1, 8] lie in a one-dimensional subspace (a line) in R. ... [Pg.312]

B.2.1.7 Basis A basis for a vector space V is a collection of linearly independent vectors that span V. For example, the vectors [1,0, OF and [0,0, -1 are linearly independent and span a two-dimensional vector subspace space in R. (Linear combinations of the vectors generate other vectors that lie in a plane in R. ) Similarly, columns of the 5 X 5 identity matrix I are a basis for the vector space R. ... [Pg.312]

Linear combinations of the columns of A ([1, 2, 3] and [0,-1,4] ) produce vectors that span a two-dimensional vector subspace (a plane) in Similarly, linear combinations of the rows of A ([1,0], [2, -1] and [3,4] ) span the entire two-dimensional vector space in Note that vectors in the column space of A reside in R, whilst vectors in the row space of A reside in R, yet the dimensions of both the column and row space of A are both two. [Pg.313]

Remark 3.8. Clearly, Hn A] Z2) actually has a structure of a Z2-vector space, since it is a quotient of a vector space by a vector subspace. It is, however, customary to call it homology group. [Pg.40]

The null space KerB is a vector subspace of the whole space of Af-vectors. Let us have M-L linearly independent vectors (transposed row vectors) oej e KerB (A = 1, —, M-L), thus a basis of KerB . The basis can be completed by some L linearly independent vectors, say Bk (A = 1, —, L) to a basis of. Then the matrix... [Pg.179]

Let k be a vector space, a subset of V. We say is a (vector) subspace of V when V is a vector space for the summation and scalar multiplication restricted to elements of V. ... [Pg.521]

If U is an arbitrary subset of vector space U we say that I/ is stable for the two vector operations when the two conditions (B.3.2 and 3) are fulfilled this means that the sum of two vectors of k as well as an arbitrary scalar multiple of a vector of V are again in P . The condition is sufficient for to be a vector subspace of Thus... [Pg.521]

Let V be subset of vector space V. Then V is a vector subspace of P if and only if it is stable for the summation and scalar multiplication. [Pg.521]

The reader can check the assertions on returning to the above examples. Conversely, introducing the spaces ImL and KerL is a common way of introducing different vector subspaces. Our examples were restricted to straight lines and planes. In a general R, the subspaces do not have individual names they are quite abstract mathematical objects. [Pg.528]

But then, as y 0, the vector components of x - x where x, 9 would be restricted to the intersection of a vector subspace of dimension AM with. 9, which is absurd. Mote sophisticated arguments of the measure theory would show that there would be no Junction... [Pg.592]


See other pages where Vector Subspaces is mentioned: [Pg.73]    [Pg.106]    [Pg.158]    [Pg.232]    [Pg.237]    [Pg.263]    [Pg.11]    [Pg.12]    [Pg.16]    [Pg.156]    [Pg.121]    [Pg.185]    [Pg.185]    [Pg.180]    [Pg.28]    [Pg.521]    [Pg.521]    [Pg.522]    [Pg.528]    [Pg.528]    [Pg.528]    [Pg.531]    [Pg.532]    [Pg.536]    [Pg.536]    [Pg.541]    [Pg.556]    [Pg.557]    [Pg.558]    [Pg.89]   
See also in sourсe #XX -- [ Pg.45 ]

See also in sourсe #XX -- [ Pg.521 ]




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