The essential spectrum

The essential spectrum
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基本频谱

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发表时间:
2009
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通讯作者:
N. Feldman
N. Feldman
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作者:
A. Aleman;W. Ross;N. Feldman

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设B(H)是Hilbert空间(H)上的有界线性算子代数,K是(H)上的紧算子理想,则形成Calkin代数B(H)/K和自然映射π:B(H)→ B(H)/K.回想一下,如果π(A)在B(H)/K中可逆,则A∈B(H)是Fredholm。一个著名的定理[19,p.356]说,A是Fredholm精确地当Rng A是封闭的,并且ker A和H/RangA都是有限维的。算子A是半Fredholm的,如果π(A)在B(H)/K中右可逆或左可逆. Equivalent. A是semi-Fredholm当且仅当RngA是闭的且ker(A)或H/RngA是有限维的。我们还使用符号 $$ sigma(A):= { lambda in mathbb{C}:lambda I-A is not invertible}(A的谱),$$ $$ sigma(A):= { lambda in mathbb{C}:lambda I-A is not Fredholm}(A的本质谱)。$$ 注意,σ e(A)<$σ(A)。对于半Fredholm算子A,令 $$ ind(A):= dim ker A - dim(H/Rng A)$$ 是A的索引。当集合{±∞|被赋予离散拓扑,映射A→ ind(A)(从半Fredholm算子集到半Fredholm {±∞|是连续的[19,p.361]。
If B(H) is the algebra of bounded linear operators on a Hilbert space (H) and K is the ideal of compact operators on (H), one forms the Calkin algebra B(H)/K and the natural map π: B(H) → B(H)/K. Recall that A∈B(H) is Fredholm if π(A) is invertible in B(H)/K. A well-known theorem [19, p. 356] says that A is Fredholm precisely when Rng A is closed and both ker A and H/RangA are finite dimensional. An operator A is semi-Fredholm if π(A) is either right or left invertible in B(H)/K. Equivalently. A is semi-Fredholm if and only if RngA is closed and either ker(A) or H/RngA is finite dimensional. We also use the notation $$ sigma (A): = { lambda in mathbb{C}:lambda I - A is not invertible} (spectrum of A),$$ $$ sigma (A): = { lambda in mathbb{C}:lambda I - A is not Fredholm} (essential spectrum of A).$$ Note that σ e (A) ⊂ σ(A). For a semi-Fredholm operator A let $$ ind(A): = dim ker A - dim (H/Rng A)$$ be the index of A. When the set ℤ∪{±∞| is endowed with the discrete topology, the map A→ ind(A) (from the set of semi-Fredholm operators to ℤ∪{±∞| is continuous [19, p. 361].