Geri Dön

n-Örgü grubunun burav temsiline benzer temsilleri

Brau-like representation of the n-braid group

  1. Tez No: 46398
  2. Yazar: ŞEYDA CANAN TEKİN
  3. Danışmanlar: PROF.DR. METİN ARIK
  4. Tez Türü: Doktora
  5. Konular: Matematik, Mathematics
  6. Anahtar Kelimeler: Gruplar, Groups
  7. Yıl: 1995
  8. Dil: Türkçe
  9. Üniversite: İstanbul Teknik Üniversitesi
  10. Enstitü: Fen Bilimleri Enstitüsü
  11. Ana Bilim Dalı: Belirtilmemiş.
  12. Bilim Dalı: Belirtilmemiş.
  13. Sayfa Sayısı: Belirtilmemiş.

Özet

/>>=/> +i >(9) e|n+->=e>+->(10) g'\n+l>=g'n+l\n + ±>(11) &'|n>=6'|n + l>(12) 1n *^> s g\n+±>=gn+l\n + l>(13) d\n>=dn\n>(14) where |n > and |n + | > belong to linear spaces V and W such that dimV - dimW and a,b,b',d:V->V f,g:W^V f',g':V-+W e:W^W. These definitions should satisfy the 17 equations arising from the relation (4). If öne applies (6-14) for 17 equations the relations among the elements of B are found as (l-O(l-O = (l-«M,)(l-<+1) = 3,(15) *n+en+dn^=2-q,(16) /n/: = (i-O(i-O,(17) gn+lg'n+l = (i - ^+1)(ı - O,(ıs) M'n = (l-<*n+1)(l-O,(19) f'nbngn+l = fnb'ng'n+l = («" - l)(en - 1)«+1 - 1).(20) Now, we try to find a representation in the case where B is unitary, i.e. BB^ = B^B = I where B^ is hennitean conjugate of B. Then (15-20) show that the Hecke algebra relation B2 = (l - q)B + q are satisfied. For unitary B, this relation linearizes as B = (l - q) + qB^. Using this we show that there is no ünite dimensional unitary representation. However for the pseudo unitary case where pl Gj3i = G finite dimensional representations exits and we construct such a representation with a diagonal G with Gz = I. Example. For a real T = TO, let an > l be chosen. Then ali en 's will be viü

Özet (Çeviri)

/>>=/> + i > (9) e|n+->=e>+-> (10) g'\n+l>=g'n+l\n + ±> (11) b'\n>=b'n\n + l> (12) <7|n+->=gn+1|n + l> (13) d\n >= dn \n > (14) where \n > and \n + | > belong to linear spaces V and W such that dimV = dimW and a,b,b',d:V->V f,g:W-+V f',g':V-+W These definitions should satisfy the 17 equations arising from the relation (4). If one applies (6-14) for 17 equations the relations among the elements of B axe found as (i-0(i-0 = (i-«.+x)(i-<U) = 3, (15) an+^+dn+1=2-q, (16) /“/I = (l-0(l-en), (17) gn+lg'n+l = (i - <*n+1)(i - O, (is) M>(i-<*.+i)(i-0, (19) = («. ”l)(e. - 1)«+1 - 1). (20) Now, we try to find a representation in the case where B is unitary, i.e. BB^ = B^B = I where B^ is hermitean conjugate of B. Then (15-20) show that the Hecke algebra relation B2 = (1 - q)B + q are satisfied. For unitary B, this relation linearizes as B - (1 - q) + qB^. Using this we show that there is no finite dimensional unitary representation. However for the pseudo unitary case where PjGfii = G finite dimensional representations exits and we construct such a representation with a diagonal G with G2 = I. Example. For a real r = r0, let an > 1 be chosen. Then all en 's will be viii/>>=/> +i >(9) e|n+->=e>+->(10) g'\n+l>=g'n+l\n + ±>(11) &'|n>=6'|n + l>(12) 1n *^> s g\n+±>=gn+l\n + l>(13) d\n>=dn\n>(14) where |n > and |n + | > belong to linear spaces V and W such that dimV - dimW and a,b,b',d:V->V f,g:W^V f',g':V-+W e:W^W. These definitions should satisfy the 17 equations arising from the relation (4). If öne applies (6-14) for 17 equations the relations among the elements of B are found as (l-O(l-O = (l-«M,)(l-<+1) = 3,(15) *n+en+dn^=2-q,(16) /n/: = (i-O(i-O,(17) gn+lg'n+l = (i - ^+1)(ı - O,(ıs) M'n = (l-<*n+1)(l-O,(19) f'nbngn+l = fnb'ng'n+l = («“ - l)(en - 1)«+1 - 1).(20) Now, we try to find a representation in the case where B is unitary, i.e. BB^ = B^B = I where B^ is hennitean conjugate of B. Then (15-20) show that the Hecke algebra relation B2 = (l - q)B + q are satisfied. For unitary B, this relation linearizes as B = (l - q) + qB^. Using this we show that there is no ünite dimensional unitary representation. However for the pseudo unitary case where pl Gj3i = G finite dimensional representations exits and we construct such a representation with a diagonal G with Gz = I. Example. For a real T = TO, let an > l be chosen. Then ali en 's will be viü/>>=/> + i > (9) e|n+->=e>+-> (10) g'\n+l>=g'n+l\n + ±> (11) b'\n>=b'n\n + l> (12) <7|n+->=gn+1|n + l> (13) d\n >= dn \n > (14) where \n > and \n + | > belong to linear spaces V and W such that dimV = dimW and a,b,b',d:V->V f,g:W-+V f',g':V-+W These definitions should satisfy the 17 equations arising from the relation (4). If one applies (6-14) for 17 equations the relations among the elements of B axe found as (i-0(i-0 = (i-«.+x)(i-<U) = 3, (15) an+^+dn+1=2-q, (16) /”/I = (l-0(l-en), (17) gn+lg'n+l = (i - <*n+1)(i - O, (is) M>(i-<*.+i)(i-0, (19) = («.“ l)(e. - 1)«+1 - 1). (20) Now, we try to find a representation in the case where B is unitary, i.e. BB^ = B^B = I where B^ is hermitean conjugate of B. Then (15-20) show that the Hecke algebra relation B2 = (1 - q)B + q are satisfied. For unitary B, this relation linearizes as B - (1 - q) + qB^. Using this we show that there is no finite dimensional unitary representation. However for the pseudo unitary case where PjGfii = G finite dimensional representations exits and we construct such a representation with a diagonal G with G2 = I. Example. For a real r = r0, let an > 1 be chosen. Then all en 's will be viii/>>=/> +i >(9) e|n+->=e>+->(10) g'\n+l>=g'n+l\n + ±>(11) &'|n>=6'|n + l>(12) 1n *^> s g\n+±>=gn+l\n + l>(13) d\n>=dn\n>(14) where |n > and |n + | > belong to linear spaces V and W such that dimV - dimW and a,b,b',d:V->V f,g:W^V f',g':V-+W e:W^W. These definitions should satisfy the 17 equations arising from the relation (4). If öne applies (6-14) for 17 equations the relations among the elements of B are found as (l-O(l-O = (l-«M,)(l-<+1) = 3,(15) *n+en+dn^=2-q,(16) /n/: = (i-O(i-O,(17) gn+lg'n+l = (i - ^+1)(ı - O,(ıs) M'n = (l-<*n+1)(l-O,(19) f'nbngn+l = fnb'ng'n+l = («”- l)(en - 1)«+1 - 1).(20) Now, we try to find a representation in the case where B is unitary, i.e. BB^ = B^B = I where B^ is hennitean conjugate of B. Then (15-20) show that the Hecke algebra relation B2 = (l - q)B + q are satisfied. For unitary B, this relation linearizes as B = (l - q) + qB^. Using this we show that there is no ünite dimensional unitary representation. However for the pseudo unitary case where pl Gj3i = G finite dimensional representations exits and we construct such a representation with a diagonal G with Gz = I. Example. For a real T = TO, let an > l be chosen. Then ali en 's will be viü/>>=/> + i > (9) e|n+->=e>+-> (10) g'\n+l>=g'n+l\n + ±> (11) b'\n>=b'n\n + l> (12) <7|n+->=gn+1|n + l> (13) d\n >= dn \n > (14) where \n > and \n + | > belong to linear spaces V and W such that dimV = dimW and a,b,b',d:V->V f,g:W-+V f',g':V-+W These definitions should satisfy the 17 equations arising from the relation (4). If one applies (6-14) for 17 equations the relations among the elements of B axe found as (i-0(i-0 = (i-«.+x)(i-<U) = 3, (15) an+^+dn+1=2-q, (16) /“/I = (l-0(l-en), (17) gn+lg'n+l = (i - <*n+1)(i - O, (is) M>(i-<*.+i)(i-0, (19) = («. ”l)(e. - 1)«+1 - 1). (20) Now, we try to find a representation in the case where B is unitary, i.e. BB^ = B^B = I where B^ is hermitean conjugate of B. Then (15-20) show that the Hecke algebra relation B2 = (1 - q)B + q are satisfied. For unitary B, this relation linearizes as B - (1 - q) + qB^. Using this we show that there is no finite dimensional unitary representation. However for the pseudo unitary case where PjGfii = G finite dimensional representations exits and we construct such a representation with a diagonal G with G2 = I. Example. For a real r = r0, let an > 1 be chosen. Then all en 's will be viii

Benzer Tezler

  1. Örgü grubu ile ilgili cebirsel yapılar ve bunların temsilleri

    Başlık çevirisi yok

    FÜGEN AYDIN (TORUNBALCI)

    Doktora

    Türkçe

    Türkçe

    1993

    MatematikYıldız Teknik Üniversitesi

    Matematik Ana Bilim Dalı

    YRD. DOÇ. DR. ALEMDAR DEMİREL

  2. Gauge theories based on quantum groups, representations of the braid group

    Başlık çevirisi yok

    ALİ YILDIZ

    Yüksek Lisans

    İngilizce

    İngilizce

    1993

    Fizik ve Fizik MühendisliğiBoğaziçi Üniversitesi

    Fizik Ana Bilim Dalı

    PROF. DR. METİN ARIK

  3. Klasik düğüm teorisine modern bir yaklaşım (düğüm kristalleri)

    Classical knot theory in modern guise (the knot crystals)

    DAVUT YILDIRIM

    Yüksek Lisans

    Türkçe

    Türkçe

    2000

    MatematikNiğde Üniversitesi

    Matematik Ana Bilim Dalı

    Y.DOÇ.DR. İSMET ALTINTAŞ

  4. Yeni evli çiftlerin ebeveynlerinden aldıkları sosyal ve ekonomik yardımların ev yönetimine etkileri

    Başlık çevirisi yok

    SELMA SALMAN (ENER)

    Yüksek Lisans

    Türkçe

    Türkçe

    1990

    Ev EkonomisiHacettepe Üniversitesi

    Ev İdaresi ve Aile Ekonomisi Ana Bilim Dalı

    PROF. DR. R. GÜNSEL TERZİOĞLU