Vector subspace

Orthogonal complement

Given an inner product space (𝑉,𝕂,βŸ¨β‹…|β‹…βŸ©), the orthogonal complement π΄βŸ‚ of a subset 𝐴 βŠ†π‘‰ is the vector subspace of vectors orthogonal to those 𝐴 #m/def/linalg

π΄βŸ‚={π‘£βˆˆπ‘‰:(βˆ€π‘Žβˆˆπ΄)[βŸ¨π‘Ž|π‘£βŸ©=0]}
Proof of subspace

Clearly\Spanβƒ—πŸŽ βˆˆπ΄βŸ‚. If 𝑣1,𝑣2 βˆˆπ΄βŸ‚ and 𝛼,𝛽 βˆˆπ•‚ then βŸ¨π‘Ž|𝛼𝑣1+𝛽𝑣2⟩ =π›ΌβŸ¨π‘Ž|𝑣1⟩ +π›½βŸ¨π‘Ž|𝑣2⟩ =0 for all π‘Ž ∈𝐴, and thus 𝛼𝑣1 +𝛽𝑣2 βˆˆπ΄βŸ‚. Therefore π΄βŸ‚ is a subspace.

A slightly more general concept is Dual annihilator.

Properties

Let 𝐴 βŠ†π‘‰ be an arbitrary subset. Then

  1. π΄βŸ‚ is topologically closed
  2. 𝐴 βˆ©π΄βŸ‚ ={0}
  3. 𝐡 βŠ†π΄ ⟹ π΄βŸ‚ βŠ†π΅βŸ‚
  4. 𝐴 βŠ†(π΄βŸ‚)βŸ‚
  5. If Bπœ–(𝑣) βŠ†π΄ for some 𝑣 βˆˆπ‘‰, then π΄βŸ‚ ={0}
  6. π΄βŸ‚ =(span⁑𝐴)βŸ‚
Proof of 1–6

Note that the orthogonal complement of a singleton {𝑣} can be expressed as a preΓ―mage

{𝑣}βŸ‚=(βŸ¨π‘£|)βˆ’1{0}

Since {0} is closed in 𝕂, and the inner product is continuous, it follows {𝑣}βŸ‚ is closed. Now for an arbitrary set 𝐴,

π΄βŸ‚=β‹‚π‘Žβˆˆπ΄{π‘Ž}βŸ‚

which is an intersection of closed sets and is therefore closed, proving ^S1.

Note if 𝑣 ∈𝐴 βˆ©π΄βŸ‚ then βŸ¨π‘£|π‘£βŸ© =0, implying 𝑣 =0 by ^IP3, proving ^S2.

Let 𝐡 βŠ†π΄ βŠ†π‘‰ and 𝑣 βˆˆπ΄βŸ‚. Then βŸ¨π‘£|π‘βŸ© =0 for any 𝑏 ∈𝐡 βŠ†π΄, so 𝑣 βˆˆπ΅βŸ‚, proving ^S3.

Let π‘Ž ∈𝐴. Then by definition βŸ¨π‘Ž|π‘£βŸ© =0 for any 𝑣 βˆˆπ΄βŸ‚, so π‘Ž ∈(π΄βŸ‚)βŸ‚, proving ^S4.

Without loss of generality 𝑣 =0, for βŸ¨π΅πœ–(𝑣)|π‘ŽβŸ© =0 iff ⟨Bπœ–(𝑣)βˆ’π‘£|π‘ŽβŸ© =⟨Bπœ–(0)|π‘ŽβŸ© =0. Now

Bπœ–(0)={π‘£βˆˆπ‘‰:βŸ¨π‘£|π‘£βŸ©<πœ–}

and

⟨Bπœ–(0)|π‘¦βŸ©=0⟺⟨Bπœ–(0)|πœ–π‘¦2β€–π‘¦β€–βŸ©=0

but since πœ–π‘¦2‖𝑦‖ ∈Bπœ–(0), it follows from ^IP3 that 𝑦 =0, proving ^S5.

Let π‘₯ βˆˆπ΄βŸ‚ and 𝑦 ∈span⁑𝐴, so 𝑦 =βˆ‘π‘›π‘–=1πœ†π‘–π‘Žπ‘– for some {π‘Žπ‘–}𝑛𝑖=1 βŠ†π΄. Then

⟨π‘₯|π‘¦βŸ©=⟨π‘₯|π‘›βˆ‘π‘–=1πœ†π‘–|π‘Žπ‘–βŸ©=0

proving ^S6.

Let π‘Š ≀𝑉 be a vector subspace. Then

  1. 𝑉 =π‘Š βŠ•π‘ŠβŸ‚ (Internal direct sum).
  2. π‘Š =(π‘ŠβŸ‚)βŸ‚.
Proof of 1–2

^V1 follows directly from ^S2, and ^V2 follows directly from ^S4.

Other properties include

See also


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