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Advanced Abstract Algebra - Maharshi Dayanand University, Rohtak

Advanced Abstract Algebra - Maharshi Dayanand University, Rohtak

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UNIT-III<br />

71<br />

1.<br />

J =<br />

only one linearly independent eigen vector belonging to<br />

Lλ<br />

NM<br />

1 0 0 0<br />

0 λ 1 0 0<br />

0 0 λ 1 0<br />

0 0 0 λ 1<br />

0 0 0 0<br />

λ<br />

O<br />

QP<br />

∃<br />

λλ<br />

J =<br />

L<br />

λ<br />

0<br />

NM<br />

1<br />

λ 1<br />

0 λ<br />

λ 1 0<br />

This Jordan canonical form consists of only one Jordan block with eigen value λ on the diagonal<br />

2. two linearly independent eigen vectors belonging to .<br />

Then the Jordan canonical form of A is either one of the forms<br />

0 λ<br />

1<br />

0 0<br />

λ<br />

O<br />

QP<br />

J =<br />

, or<br />

Lλ<br />

NM<br />

λ<br />

1 0 0<br />

0 λ 1 0<br />

0 0 λ 1<br />

0 0 0<br />

λ<br />

O<br />

QP<br />

Each of which consists of two Jordan blocks with eigen value λ on the diagonal.<br />

3. ∃ three linearly independent eigen vectors belonging to<br />

Then the Jordan Canonical form of A is either one of the forms<br />

J =<br />

, or<br />

Lλ<br />

NM<br />

λ<br />

λ 1 0<br />

0 λ 1<br />

0 0 λ<br />

O<br />

QP<br />

4.<br />

Each of which consists of three Jordan blocks with eigen value λ on the diagonal.<br />

four linearly independent eigen vectors belonging to .<br />

Then the Jordan canonical form of A is of the form<br />

5.<br />

This consists of four Jordan blocks with eigen value λ on the diagonal.<br />

five linearly independent eigen vectors belonging to .<br />

Then the Jordan canonical form of A is of the form.

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