{"title":"希尔伯特空间算子的谱理论","authors":"S. Chavan, G. Misra","doi":"10.1017/9781009023306.003","DOIUrl":null,"url":null,"abstract":"Index Let B be a unital Banach algebra and let G denote the group of invertible elements in B. Let G0 be the connected component of G containing the identity of G. Note that any connected component of G is open because all connected neighborhoods of its element are contained in it. It follows immediately that any connected component of G is closed in G, as well. In particular, G0 is open as well as closed subset of G. Example 1.3.9 Let X be a compact Hausdorff space. Consider the Banach algebra C(X) of continuous functions from X into C. Note that the group G of invertible elements in C(X) is given by G = { f ∈C(X) : f is nowhere vanishing on X}. Moreover, 1 is the identity for C(X). Let f ∈ C(X) belong to the connected component G0 of G containing 1. Since G0 is locally path-connected (G0 is open and C(X) is a vector space, therefore locally path-connected), there exists a collection { fλ}λ∈[0,1] of continuous functions in C(X) such that f0 = 1 and f1 = f . Define Γ : X × [0,1]→G by Γ(x,λ) = fλ(x), and note that Γ(x,0) = 1 and Γ(x,1) = f (x) for every x ∈ X. In other words, G0 consists of precisely those elements in G that are homotopic to 1. Recall that Fn(H) is the set of Fredholm operators in L(H) of index n. Lemma 1.3.4 Let G (H) be the group of invertible elements in Q(H). If G0(H) denotes the connected component of G (H) containing the identity element in G(H), then G (H) = {π(T ) : T ∈ F (H)} and G0(H) = {π(T ) : T ∈ F0(H)}, where π :L(H)→Q(H) is the Calkin map. Proof Since Fn(H) is a connected component of F (H) (see Corollary 1.3.3) and since π is an open map, G (H) is the union of clopen sets {π(T ) : T ∈ F0(H)} and {π(T ) : T ∈ F (H)\\F0(H)}. Moreover, this union is disjoint. Indeed, if S n ∈ Fn(H) and S m ∈ Fm(H), then π(S n) = π(S m) implies S n − S m is a compact operator. Since the Fredholm index is invariant under compact perturbations (Theorem 1.3.1), we have m = n in this case. Let B be a unital Banach algebra and let G denote the group of invertible elements in B. Let G0 be the connected component of G containing the identity of G. For f ,g ∈G0, we record the following observations: • Since Lg : G0→ gG0 given by Lg( f ) = g f is surjective and continuous, every coset of G0 is connected. • Since f g and f belongs to the connected subset fG0 of B, fG0 ∪G0 is connected and non-empty. In particular, fG0∪G0 ⊆G0, and hence, G0 is a subgroup. • For any h ∈G, hG0h−1 is a connected subset containing identity, and hence, hG0h−1 = G0. That is, G0 is normal. i i “BDFT ̇Book” — 2021/5/18 — 12:14 — page 31 — #43 i i i i i i Spectral Theory for Hilbert Space Operators 31 • The cosets of G0 are connected components of G. Since G0 is a clopen subset of G, the quotient G/G0 is a discrete group. The previous discussion forms the basis of the following definition. Definition 1.3.10 Let B be a unital Banach algebra. Let G denote the group of invertible elements in B and let G0 denote the connected component of G containing the identity of G. The abstract index group for B is the quotient group G/G0. In what follows, we will be particularly interested in the abstract index group for the Banach algebra C(X). Example 1.3.11 (Example 1.3.9 continued) Recall that the group G of invertible elements in C(X) is the set of nowhere vanishing continuous functions in C(X). It turns out that the connected component G0 of C(X) containing the identity element 1 in C(X) is the group exp(C(X)) of functions of the form e f for some f ∈ C(X). To see this, note that if f lies in an open unit ball in C(X) around 1, then f = eg, where g ∈ B is given by","PeriodicalId":150570,"journal":{"name":"Notes on the Brown-Douglas-Fillmore Theorem","volume":"26 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2021-07-31","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Spectral Theory for Hilbert Space Operators\",\"authors\":\"S. Chavan, G. Misra\",\"doi\":\"10.1017/9781009023306.003\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Index Let B be a unital Banach algebra and let G denote the group of invertible elements in B. Let G0 be the connected component of G containing the identity of G. Note that any connected component of G is open because all connected neighborhoods of its element are contained in it. It follows immediately that any connected component of G is closed in G, as well. In particular, G0 is open as well as closed subset of G. Example 1.3.9 Let X be a compact Hausdorff space. Consider the Banach algebra C(X) of continuous functions from X into C. Note that the group G of invertible elements in C(X) is given by G = { f ∈C(X) : f is nowhere vanishing on X}. Moreover, 1 is the identity for C(X). Let f ∈ C(X) belong to the connected component G0 of G containing 1. Since G0 is locally path-connected (G0 is open and C(X) is a vector space, therefore locally path-connected), there exists a collection { fλ}λ∈[0,1] of continuous functions in C(X) such that f0 = 1 and f1 = f . Define Γ : X × [0,1]→G by Γ(x,λ) = fλ(x), and note that Γ(x,0) = 1 and Γ(x,1) = f (x) for every x ∈ X. In other words, G0 consists of precisely those elements in G that are homotopic to 1. Recall that Fn(H) is the set of Fredholm operators in L(H) of index n. Lemma 1.3.4 Let G (H) be the group of invertible elements in Q(H). If G0(H) denotes the connected component of G (H) containing the identity element in G(H), then G (H) = {π(T ) : T ∈ F (H)} and G0(H) = {π(T ) : T ∈ F0(H)}, where π :L(H)→Q(H) is the Calkin map. Proof Since Fn(H) is a connected component of F (H) (see Corollary 1.3.3) and since π is an open map, G (H) is the union of clopen sets {π(T ) : T ∈ F0(H)} and {π(T ) : T ∈ F (H)\\\\F0(H)}. Moreover, this union is disjoint. Indeed, if S n ∈ Fn(H) and S m ∈ Fm(H), then π(S n) = π(S m) implies S n − S m is a compact operator. Since the Fredholm index is invariant under compact perturbations (Theorem 1.3.1), we have m = n in this case. Let B be a unital Banach algebra and let G denote the group of invertible elements in B. Let G0 be the connected component of G containing the identity of G. For f ,g ∈G0, we record the following observations: • Since Lg : G0→ gG0 given by Lg( f ) = g f is surjective and continuous, every coset of G0 is connected. • Since f g and f belongs to the connected subset fG0 of B, fG0 ∪G0 is connected and non-empty. In particular, fG0∪G0 ⊆G0, and hence, G0 is a subgroup. • For any h ∈G, hG0h−1 is a connected subset containing identity, and hence, hG0h−1 = G0. That is, G0 is normal. i i “BDFT ̇Book” — 2021/5/18 — 12:14 — page 31 — #43 i i i i i i Spectral Theory for Hilbert Space Operators 31 • The cosets of G0 are connected components of G. Since G0 is a clopen subset of G, the quotient G/G0 is a discrete group. The previous discussion forms the basis of the following definition. Definition 1.3.10 Let B be a unital Banach algebra. Let G denote the group of invertible elements in B and let G0 denote the connected component of G containing the identity of G. The abstract index group for B is the quotient group G/G0. In what follows, we will be particularly interested in the abstract index group for the Banach algebra C(X). Example 1.3.11 (Example 1.3.9 continued) Recall that the group G of invertible elements in C(X) is the set of nowhere vanishing continuous functions in C(X). It turns out that the connected component G0 of C(X) containing the identity element 1 in C(X) is the group exp(C(X)) of functions of the form e f for some f ∈ C(X). To see this, note that if f lies in an open unit ball in C(X) around 1, then f = eg, where g ∈ B is given by\",\"PeriodicalId\":150570,\"journal\":{\"name\":\"Notes on the Brown-Douglas-Fillmore Theorem\",\"volume\":\"26 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2021-07-31\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Notes on the Brown-Douglas-Fillmore Theorem\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1017/9781009023306.003\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Notes on the Brown-Douglas-Fillmore Theorem","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1017/9781009023306.003","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
设B是一个一元巴拿赫代数,设G表示B中可逆元素的群。设G0是G中含有G单位元的连通分量。注意G的任何连通分量都是开的,因为它的元素的所有连通邻域都包含在其中。因此,G的连通分量在G中也是封闭的。特别地,G0是g的开子集和闭子集。例1.3.9设X为紧Hausdorff空间。考虑从X到C的连续函数的Banach代数C(X),注意C(X)中可逆元素的群G由G = {f∈C(X): f在X上无处消失}给出。而且,1是C(X)的恒等式。设f∈C(X)属于包含1的G的连通分量G0。由于G0是局部路径连通的(G0是开的,C(X)是向量空间,因此是局部路径连通的),因此在C(X)中存在一个连续函数的集合{fλ}λ∈[0,1],使得f0 = 1, f1 = f。定义Γ: X X[0,1]→G = Γ(X,λ) = fλ(X),并注意对于每个X∈X, Γ(X,0) = 1和Γ(X,1) = f (X)。换句话说,G0恰好由G中与1同伦的元素组成。回想Fn(H)是L(H)中指标n的Fredholm算子的集合。引理1.3.4设G (H)为Q(H)中可逆元素的群。若G0(H)表示含有G(H)中单位元的G(H)连通分量,则G(H) = {π(T): T∈F (H)}, G0(H) = {π(T): T∈F0(H)},其中π:L(H)→Q(H)是Calkin映射。证明由于Fn(H)是F (H)的连通分量(见推论1.3.3),并且由于π是开映射,所以G (H)是闭集{π(T): T∈F0(H)}和{π(T): T∈F (H)\F0(H)}的并集。此外,这个联盟是不团结的。的确,如果sn∈Fn(H),且S m∈Fm(H),则π(sn) = π(S m)暗示S n−S m是紧算子。由于Fredholm指数在紧摄动下是不变的(定理1.3.1),在这种情况下我们有m = n。设B是一个一元Banach代数,设G表示B中的可逆元素群,设G0是G中包含G单位元的连通分量。对于f, G∈G0,我们记录如下观察结果:•由于Lg(f) = gf给出的Lg: G0→gG0是满射连续的,所以G0的每一个余集都是连通的。•由于fg和f属于B的连通子集fG0,所以fG0∪G0是连通的非空子集。其中,fG0∪G0≥G0,因此,G0是一个子群。•对于任意h∈G, hG0h−1是包含单位元的连通子集,因此,hG0h−1 = G0。也就是说,G0是正常的。i i i i i i i i i i i i Hilbert空间算子的谱理论31•G0的余集是G的连通分量,因为G0是G的闭子集,所以商G/G0是离散群。前面的讨论构成了以下定义的基础。1.3.10设B为一元巴拿赫代数。设G表示B中可逆元素的群,设G0表示G中包含G的单位元的连通分量,B的抽象指标群为商群G/G0。在接下来的内容中,我们将对Banach代数C(X)的抽象索引群特别感兴趣。例1.3.11(续例1.3.9)回想C(X)中可逆元素的群G是C(X)中无处消失的连续函数的集合。结果表明,C(X)的连通分量G0包含C(X)中的单位元1是对于某些f∈C(X)的e (f)形式的函数的群exp(C(X))。要了解这一点,请注意,如果f在C(X)中位于1附近的开放单位球中,则f = eg,其中g∈B由
Index Let B be a unital Banach algebra and let G denote the group of invertible elements in B. Let G0 be the connected component of G containing the identity of G. Note that any connected component of G is open because all connected neighborhoods of its element are contained in it. It follows immediately that any connected component of G is closed in G, as well. In particular, G0 is open as well as closed subset of G. Example 1.3.9 Let X be a compact Hausdorff space. Consider the Banach algebra C(X) of continuous functions from X into C. Note that the group G of invertible elements in C(X) is given by G = { f ∈C(X) : f is nowhere vanishing on X}. Moreover, 1 is the identity for C(X). Let f ∈ C(X) belong to the connected component G0 of G containing 1. Since G0 is locally path-connected (G0 is open and C(X) is a vector space, therefore locally path-connected), there exists a collection { fλ}λ∈[0,1] of continuous functions in C(X) such that f0 = 1 and f1 = f . Define Γ : X × [0,1]→G by Γ(x,λ) = fλ(x), and note that Γ(x,0) = 1 and Γ(x,1) = f (x) for every x ∈ X. In other words, G0 consists of precisely those elements in G that are homotopic to 1. Recall that Fn(H) is the set of Fredholm operators in L(H) of index n. Lemma 1.3.4 Let G (H) be the group of invertible elements in Q(H). If G0(H) denotes the connected component of G (H) containing the identity element in G(H), then G (H) = {π(T ) : T ∈ F (H)} and G0(H) = {π(T ) : T ∈ F0(H)}, where π :L(H)→Q(H) is the Calkin map. Proof Since Fn(H) is a connected component of F (H) (see Corollary 1.3.3) and since π is an open map, G (H) is the union of clopen sets {π(T ) : T ∈ F0(H)} and {π(T ) : T ∈ F (H)\F0(H)}. Moreover, this union is disjoint. Indeed, if S n ∈ Fn(H) and S m ∈ Fm(H), then π(S n) = π(S m) implies S n − S m is a compact operator. Since the Fredholm index is invariant under compact perturbations (Theorem 1.3.1), we have m = n in this case. Let B be a unital Banach algebra and let G denote the group of invertible elements in B. Let G0 be the connected component of G containing the identity of G. For f ,g ∈G0, we record the following observations: • Since Lg : G0→ gG0 given by Lg( f ) = g f is surjective and continuous, every coset of G0 is connected. • Since f g and f belongs to the connected subset fG0 of B, fG0 ∪G0 is connected and non-empty. In particular, fG0∪G0 ⊆G0, and hence, G0 is a subgroup. • For any h ∈G, hG0h−1 is a connected subset containing identity, and hence, hG0h−1 = G0. That is, G0 is normal. i i “BDFT ̇Book” — 2021/5/18 — 12:14 — page 31 — #43 i i i i i i Spectral Theory for Hilbert Space Operators 31 • The cosets of G0 are connected components of G. Since G0 is a clopen subset of G, the quotient G/G0 is a discrete group. The previous discussion forms the basis of the following definition. Definition 1.3.10 Let B be a unital Banach algebra. Let G denote the group of invertible elements in B and let G0 denote the connected component of G containing the identity of G. The abstract index group for B is the quotient group G/G0. In what follows, we will be particularly interested in the abstract index group for the Banach algebra C(X). Example 1.3.11 (Example 1.3.9 continued) Recall that the group G of invertible elements in C(X) is the set of nowhere vanishing continuous functions in C(X). It turns out that the connected component G0 of C(X) containing the identity element 1 in C(X) is the group exp(C(X)) of functions of the form e f for some f ∈ C(X). To see this, note that if f lies in an open unit ball in C(X) around 1, then f = eg, where g ∈ B is given by