j theory in application to the spectral theory of
play

J-theory in application to the spectral theory of periodic GMP - PowerPoint PPT Presentation

J-theory in application to the spectral theory of periodic GMP matrices Benjamin Eichinger Institute of Analysis Johannes Kepler University Linz OTIND , 17st-20th December 1 / 19 Jacobi matrices Let d be a real compactly supported measure


  1. J-theory in application to the spectral theory of periodic GMP matrices Benjamin Eichinger Institute of Analysis Johannes Kepler University Linz OTIND , 17st-20th December 1 / 19

  2. Jacobi matrices Let d σ be a real compactly supported measure and P n = P n ( d σ ) the corresponding orthonormal polynomials. It is well known, that they satisfy a three-term recurrence relation. xP n ( x ) = a n P n − 1 ( x ) + b n P n ( x ) + a n + 1 P n + 1 , a n > 0 . That is, multiplication by x in the basis { P n } n ≥ 0 has the one-sided Jacobi matrix   0 b 0 a 1 a 1 b 1 a 2     J + = ... ... ... .   0    ... ...  2 / 19

  3. Jacobi matrices Let d σ be a real compactly supported measure and P n = P n ( d σ ) the corresponding orthonormal polynomials. It is well known, that they satisfy a three-term recurrence relation. xP n ( x ) = a n P n − 1 ( x ) + b n P n ( x ) + a n + 1 P n + 1 , a n > 0 . That is, multiplication by x in the basis { P n } n ≥ 0 has the one-sided Jacobi matrix   0 b 0 a 1 a 1 b 1 a 2     J + = ... ... ... .   0    ... ...  2 / 19

  4. Shift on Jacobi matrices Let us define the resolvent function r + ( z ) = � ( J + − z ) − 1 e 0 , e 0 � , � � e 0 = 1 0 0 . . . . Let r ( 1 ) be the resolvent function of J ( 1 ) + , + b 0 a 1 · · · 0 · · ·    . a 1 J + =  J ( 1 ) 0 + Then − 1 r + ( z ) = . 1 r ( 1 ) z − b 0 − a 2 + ( z ) That is, � 0 � � � r ( 1 ) � r + ( z ) � − 1 / a 1 + ( z ) ∼ , 1 a 1 ( z − b 0 ) / a 1 1 where � u � � x � � u � � x � ∼ ⇐ ⇒ ∃ c = c v y v y 3 / 19

  5. Shift on Jacobi matrices Let us define the resolvent function r + ( z ) = � ( J + − z ) − 1 e 0 , e 0 � , � � e 0 = 1 0 0 . . . . Let r ( 1 ) be the resolvent function of J ( 1 ) + , + b 0 a 1 · · · 0 · · ·    . a 1 J + =  J ( 1 ) 0 + Then − 1 r + ( z ) = . 1 r ( 1 ) z − b 0 − a 2 + ( z ) That is, � 0 � � � r ( 1 ) � r + ( z ) � − 1 / a 1 + ( z ) ∼ , 1 a 1 ( z − b 0 ) / a 1 1 where � u � � x � � u � � x � ∼ ⇐ ⇒ ∃ c = c v y v y 3 / 19

  6. Shift on Jacobi matrices Let us define the resolvent function r + ( z ) = � ( J + − z ) − 1 e 0 , e 0 � , � � e 0 = 1 0 0 . . . . Let r ( 1 ) be the resolvent function of J ( 1 ) + , + b 0 a 1 · · · 0 · · ·    . a 1 J + =  J ( 1 ) 0 + Then − 1 r + ( z ) = . 1 r ( 1 ) z − b 0 − a 2 + ( z ) That is, � 0 � � � r ( 1 ) � r + ( z ) � − 1 / a 1 + ( z ) ∼ , 1 a 1 ( z − b 0 ) / a 1 1 where � u � � x � � u � � x � ∼ ⇐ ⇒ ∃ c = c v y v y 3 / 19

  7. Shift on Jacobi matrices Let us define the resolvent function r + ( z ) = � ( J + − z ) − 1 e 0 , e 0 � , � � e 0 = 1 0 0 . . . . Let r ( 1 ) be the resolvent function of J ( 1 ) + , + b 0 a 1 · · · 0 · · ·    . a 1 J + =  J ( 1 ) 0 + Then − 1 r + ( z ) = . 1 r ( 1 ) z − b 0 − a 2 + ( z ) That is, � 0 � � � r ( 1 ) � r + ( z ) � − 1 / a 1 + ( z ) ∼ , 1 a 1 ( z − b 0 ) / a 1 1 where � u � � x � � u � � x � ∼ ⇐ ⇒ ∃ c = c v y v y 3 / 19

  8. periodic Jacobi matrices For periodic Jacobi matrices, i.e., ∃ p ∀ k a k + p = a k , b k + p = b k , it is convenient to extend the sequences periodically to Z and consider the two-sided Jacobi matrix ...     ... ...   0 a p − 1 J −         a p − 1 b p − 1 a 0 a 0     =     a 0 b 0 a 1 a 0         ... ... 0   J +   a 1     ... We define r − ( z ) = � ( J − − z ) − 1 e − 1 , e − 1 � . 4 / 19

  9. periodic Jacobi matrices For periodic Jacobi matrices, i.e., ∃ p ∀ k a k + p = a k , b k + p = b k , it is convenient to extend the sequences periodically to Z and consider the two-sided Jacobi matrix ...     ... ...   0 a p − 1 J −         a p − 1 b p − 1 a 0 a 0     =     a 0 b 0 a 1 a 0         ... ... 0   J +   a 1     ... We define r − ( z ) = � ( J − − z ) − 1 e − 1 , e − 1 � . 4 / 19

  10. We see that � 0 � 0 � � � r ( p ) � r + ( z ) � � − 1 / a 1 − 1 / a p + ( z ) ∼ ... 1 a 1 ( z − b 0 ) / a 1 a p ( z − b p − 1 ) / a p 1 � r + ( z ) � = T p ( z ) . 1 Theorem Let us define the polynomial of degree p, ∆( z ) = tr T p ( z ) . The spectrum of a periodic two-sided Jacobi matrix is purely absolutely continuous and it is given by E = ∆ − 1 ([ − 2 , 2 ]) . Moreover the resolvent functions are reflectionless on E , i.e., 1 r + ( x + i 0 ) = a 2 0 r − ( x + i 0 ) . Note that for this reason spectra of periodic Jacobi matrices are very special finite union of intervals. 5 / 19

  11. We see that � 0 � 0 � � � r ( p ) � r + ( z ) � � − 1 / a 1 − 1 / a p + ( z ) ∼ ... 1 a 1 ( z − b 0 ) / a 1 a p ( z − b p − 1 ) / a p 1 � r + ( z ) � = T p ( z ) . 1 Theorem Let us define the polynomial of degree p, ∆( z ) = tr T p ( z ) . The spectrum of a periodic two-sided Jacobi matrix is purely absolutely continuous and it is given by E = ∆ − 1 ([ − 2 , 2 ]) . Moreover the resolvent functions are reflectionless on E , i.e., 1 r + ( x + i 0 ) = a 2 0 r − ( x + i 0 ) . Note that for this reason spectra of periodic Jacobi matrices are very special finite union of intervals. 5 / 19

  12. We see that � 0 � 0 � � � r ( p ) � r + ( z ) � � − 1 / a 1 − 1 / a p + ( z ) ∼ ... 1 a 1 ( z − b 0 ) / a 1 a p ( z − b p − 1 ) / a p 1 � r + ( z ) � = T p ( z ) . 1 Theorem Let us define the polynomial of degree p, ∆( z ) = tr T p ( z ) . The spectrum of a periodic two-sided Jacobi matrix is purely absolutely continuous and it is given by E = ∆ − 1 ([ − 2 , 2 ]) . Moreover the resolvent functions are reflectionless on E , i.e., 1 r + ( x + i 0 ) = a 2 0 r − ( x + i 0 ) . Note that for this reason spectra of periodic Jacobi matrices are very special finite union of intervals. 5 / 19

  13. Functional model Let E be a finite union of intervals E = [ a 0 , b 0 ] \ � g j = 1 ( a j , b j ) and Ω = C \ E . Let g Ω ( z , z 0 ) denote the Green’s function of Ω and define the complex Green’s function by B z 0 ( z ) = e − g Ω ( z , z 0 ) − i � g Ω ( z , z 0 ) . Note that we have the properties: B z 0 ( z 0 ) = 0, | B z 0 | = 1 on E , γ j = e 2 π i ω Ω ( E j , z 0 ) B z 0 . | B z 0 | < 1 in Ω , B z 0 ◦ ˜ 6 / 19

  14. Functional model Let E be a finite union of intervals E = [ a 0 , b 0 ] \ � g j = 1 ( a j , b j ) and Ω = C \ E . Let g Ω ( z , z 0 ) denote the Green’s function of Ω and define the complex Green’s function by B z 0 ( z ) = e − g Ω ( z , z 0 ) − i � g Ω ( z , z 0 ) . Note that we have the properties: B z 0 ( z 0 ) = 0, | B z 0 | = 1 on E , γ j = e 2 π i ω Ω ( E j , z 0 ) B z 0 . | B z 0 | < 1 in Ω , B z 0 ◦ ˜ 6 / 19

  15. Functional model Let E be a finite union of intervals E = [ a 0 , b 0 ] \ � g j = 1 ( a j , b j ) and Ω = C \ E . Let g Ω ( z , z 0 ) denote the Green’s function of Ω and define the complex Green’s function by B z 0 ( z ) = e − g Ω ( z , z 0 ) − i � g Ω ( z , z 0 ) . Note that we have the properties: B z 0 ( z 0 ) = 0, | B z 0 | = 1 on E , γ j = e 2 π i ω Ω ( E j , z 0 ) B z 0 . | B z 0 | < 1 in Ω , B z 0 ◦ ˜ 6 / 19

  16. Functional model Let E be a finite union of intervals E = [ a 0 , b 0 ] \ � g j = 1 ( a j , b j ) and Ω = C \ E . Let g Ω ( z , z 0 ) denote the Green’s function of Ω and define the complex Green’s function by B z 0 ( z ) = e − g Ω ( z , z 0 ) − i � g Ω ( z , z 0 ) . Note that we have the properties: B z 0 ( z 0 ) = 0, | B z 0 | = 1 on E , γ j = e 2 π i ω Ω ( E j , z 0 ) B z 0 . | B z 0 | < 1 in Ω , B z 0 ◦ ˜ 6 / 19

  17. Functional model Let E be a finite union of intervals E = [ a 0 , b 0 ] \ � g j = 1 ( a j , b j ) and Ω = C \ E . Let g Ω ( z , z 0 ) denote the Green’s function of Ω and define the complex Green’s function by B z 0 ( z ) = e − g Ω ( z , z 0 ) − i � g Ω ( z , z 0 ) . Note that we have the properties: B z 0 ( z 0 ) = 0, | B z 0 | = 1 on E , γ j = e 2 π i ω Ω ( E j , z 0 ) B z 0 . | B z 0 | < 1 in Ω , B z 0 ◦ ˜ 6 / 19

  18. Functional model Let E be a finite union of intervals E = [ a 0 , b 0 ] \ � g j = 1 ( a j , b j ) and Ω = C \ E . Let g Ω ( z , z 0 ) denote the Green’s function of Ω and define the complex Green’s function by B z 0 ( z ) = e − g Ω ( z , z 0 ) − i � g Ω ( z , z 0 ) . Note that we have the properties: B z 0 ( z 0 ) = 0, | B z 0 | = 1 on E , γ j = e 2 π i ω Ω ( E j , z 0 ) B z 0 . | B z 0 | < 1 in Ω , B z 0 ◦ ˜ 6 / 19

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend