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HBr , V(m+i), i = 4-8,10 https://notendur.hi.is/~ agust/rannsoknir/Crete/PPT-131202x

HBr , V(m+i), i = 4-8,10 https://notendur.hi.is/~ agust/rannsoknir/Crete/PPT-131202.pptx https://notendur.hi.is/~ agust/rannsoknir/Crete/PXP-131203.pxp https://notendur.hi.is/~agust/rannsoknir/Crete/XLS-131203.xlsx. HBr , V(m+i)´s. H + + Br (1/2). H + + Br (3/2) Normalized.

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HBr , V(m+i), i = 4-8,10 https://notendur.hi.is/~ agust/rannsoknir/Crete/PPT-131202x

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  1. HBr, V(m+i), i = 4-8,10 https://notendur.hi.is/~agust/rannsoknir/Crete/PPT-131202.pptx https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp https://notendur.hi.is/~agust/rannsoknir/Crete/XLS-131203.xlsx

  2. HBr, V(m+i)´s H+ + Br(1/2) H+ + Br(3/2) Normalized H+ <- HBr+(v´) V(m+10) V(m+8) V(m+7) V(m+6) V(m+5) V(m+4) KER/eV Agust,labtop,C:/…/PXP-131127a.pxp ; Gr0, Lay0

  3. HBr; 3/2 <-3/2 transitions V(m+10) V(m+8) V(m+7) V(m+6) V(m+5) V(m+4) KER/eV Agust,labtop,C:/…/PXP-131127a.pxp ; Gr0, Lay0 <= XLS-131127.xls („KER,I,II“)

  4. HBr; 3/2 <-3/2 Transitions KER spectranormalized tothe H+ + Br(3/2) channel v+= 8 10 12 13 V(m+6) V(m+5) V(m+4) v+= 8 10 12 13 v+= 8 10 12 13 KER/eV Agust,heima & labtop,C:/…/PXP-131129.pxp ; Gr1, Lay1 <= XLS-131127.xls („KER,I,II“)

  5. HBr; 3/2 <-3/2 Transitions KER spectranormalized tothe H+ + Br(3/2) channel v+= 8 10 12 13 15 V(m+10) V(m+8) V(m+7) v+= 8 10 1213 v+= 8 10 12 13 KER/eV Agust heima&,labtop,C:/…/PXP-131129.pxp ; Gr2, Lay2 <= XLS-131127.xls („KER,I,II“)

  6. HBr; 1/2 <-1/2 transitions ? KER/eV agust heima/…/PXP-131202.pxp ; Gr0, Lay0 <= XLS-131202.xls („KER,III,IV“)

  7. HBr; 3/2 <-3/2 (boldsticks) &1/2 <-1/2 (thinsticks) v+= 8 10 12 13 8 9 10 11 V(m+6) V(m+5) V(m+4) v+= 8 10 12 13 8 9 10 v+= 8 10 11 12 8 9 10 KER/eV agust heima/…/PXP-131202.pxp ; Gr1 Lay1

  8. HBr; 3/2 <-3/2 (boldsticks) &1/2 <-1/2 (thinsticks) v+= 8 10 12 13 15 9 10 11 V(m+10) V(m+8) V(m+7) v+= 8 10 1213 8 9 10 11 v+= 8 10 12 13 8 9 10 KER/eV agust heima/…/PXP-131202.pxp ; Gr1 Lay1

  9. HBr; 1/2 <-3/2 (boldsticks) &3/2 <-1/2 (thinsticks) v+= 10 12 13 6 7 8 9 V(m+6) V(m+5) V(m+4) v+= 10 12 13 6 7 8 9 v+= 10 12 13 6 7 8 9 KER/eV agust heima/…/PXP-131203.pxp ; Gr1 Lay1

  10. HBr; 1/2 <-3/2 (boldsticks) &3/2 <-1/2 (thinsticks) v+= 10 12 13 15 6 7 8 9 V(m+10) V(m+8) V(m+7) v+= 10 1213 6 7 8 v+= 10 12 13 6 7 8 KER/eV agust heima/…/PXP-131203.pxp ; Gr2 Lay2

  11. HBr; 3/2 <-3/2 (boldsticks) &1/2 <-1/2 (thinsticks) v+= 8 10 11 12 13 9 10 E(0), J´=1 KER/eV https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131208.pxp

  12. Thevibrationalstructure in the „H+ + Br/Br* viaHBr+(v+) ionizationchannel“ is dueto a combination of H+ + Br(3/2) <- HBr+(v+)(3/2) (i.e. 3/2 <-3/2) and H++ Br(1/2) <- HBr+(v+)(1/2) (i.e. 1/2 <-1/2) transitions

  13. V(m+10) v+ (1/2) 14 13 12 11 10 9 8 v+(3/2) 16 15 14 13 12 11 10 https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp

  14. V(m+8) v+ (1/2) 14 13 12 11 10 9 8 v+(3/2) 16 15 14 13 12 11 10 https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp

  15. V(m+7) v+ (1/2) 14 13 12 11 10 9 8 v+(3/2) 16 15 14 13 12 11 10 https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp

  16. V(m+6) v+ (1/2) 14 13 12 11 10 9 8 v+(3/2) 16 15 14 13 12 11 10 https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp

  17. V(m+5) v+ (1/2) 14 13 12 11 10 9 8 v+(3/2) 16 15 14 13 12 11 10 https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp

  18. V(m+4) v+ (1/2) 14 13 12 11 10 9 8 v+(3/2) 16 15 14 13 12 11 10 https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp

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  22. [(3)2P] ..superexcitedstate H++Br+e HBr+*(A) [B2S+] ..superexcitedstate H+Br+ + e v+=14 v+=12 H+ + Br- H*(n=2)+Br HBr+*(X) [4P,5s] Rydb. H + Br**(5s) HBr+(X) H V F E 2hnto V(m+7) https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131203.pxp

  23. HBr, V(m+i)´s H+ + Br(1/2) H+ + Br(3/2) Normalized H+ <- HBr+(v´) V(m+10) V(m+9) V(m+8) V(m+7) V(m+6) V(m+5) V(m+4) KER/eV https://notendur.hi.is/~agust/rannsoknir/Crete/PXP-131209a.pxp ; Gr0 Lay0

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