f3d2 energetics and interaction with v,v´=8 & f3d1 energetics and interaction with v,v´=9

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f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9 Shifts of levels and peaks(?) agust,www,....january09/PPT-030309ak.ppt

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f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9 Shifts of levels and peaks(?) agust,www,....january09/PPT-030309ak.ppt. f3D2, f / P,R state; i.e. D - (see 241208;2). J´(higher). J´(higher). - PowerPoint PPT Presentation

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Page 1: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

f3D2 energetics and interaction with V,v´=8&f3D1 energetics and interaction with V,v´=9

Shifts of levels and peaks(?)

agust,www,....january09/PPT-030309ak.ppt

Page 2: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

agust,heima,...january09/Term values for triplet paper-030309kmak.xls

f3D2, f / P,R state; i.e. - (see 241208;2)

J´(higher) J´(higher)

Page 3: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

E(e)

f32, e / O,Q,S state; i.e. + (see 241208;2)

E(e))

E(e))

Page 4: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

f3D2,v´=0 DE(f3D2)av. terms

82079,982145,15 65,2492982231,26 86,1114682338,08 106,824382465,63 127,548982613,74 148,1048

J´234567

agust, heima, ...january09/Term values for triplet paper-190209kmak.xls

E

J´,J´-

1

J´(higher)

DE(DE)

20,8621720,7128420,7246220,55592

Page 5: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

5 5

4

3 4 5 6 7

3 4 5 6 7

V1S+,v´=8+

+

+

+

-

-

-

parities

-+

+

f3D2 (e) (f +)(see 241208;2)

To be expected:

Page 6: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

Hence observations are not according to expectations

IF anything it seems to be the opposite effect, i.e. the gap between J´= 4 & 5 decreases instead of increses

Large fluctuations in DE(DE) are observed suggesting that uncertainty is too large andThat insignificant shifts of levels are endeed observed

Let´s now see what shifts the W12 values obtained for f3D2 <-> V,v´=8 interaction will correspond to

Page 7: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

agust,heima,...january09/Term values for triplet paper-030309kmak.xls

f3D1, f / P,R state; i.e. - (see 241208;2)

J´(higher)

J´(higher)

Page 8: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

agust,heima,...january09/Term values for triplet paper-030309kmak.xls

f3D1, e / O,Q,S state; i.e. + (see 241208;2)

J´(higher) J´(higher)

E(e)

E(e))

E(e))

Page 9: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

f3D1,v´=1 DE(f3D1)av. Terms:

82544,0482585,48 41,4426782647,29 61,8073382729,84 82,5498182832,47 102,633582957,29 124,817283100,74 143,4541

J´1234567

agust, heima, ...january09/Term values for triplet paper-190209kmak.xls

E

J´,J´-

1

J´(higher)

DE(DE)

20,3646620,7424820,0836922,18366

18,6369

Page 10: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

5

5

4

3 4 5 6 7

3 4 5 6 7

f3D1 (e) (f+)(see 241208;2) V1S+,v´=9

66

E(e)

E(e))

To be expected:

+

+

+

-

-

-

-

-

+

parities

Page 11: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

Hence observations are not according to expectations

IF anything it seems to be the opposite effect, i.e. the gap between J´= 5 & 6 increases (see slide 8) instead of decreases

Large fluctuations in DE(DE) are observed suggesting that uncertainty is too large andThat insignificant shifts of levels are endeed observed

NB: according to agust,heima,.... january09/Term values for triplet paper-030309kmak.xlsThe same seems to hold for the “New State”, i.e. IF anything it seems to be the opposite effect, i.e. the gap between J´= 5 & 6 increases (see slide 12) instead of decreases

g3S+(1) <-> V,v´=9

See next pages:

agust, heima, ...january09/Term values for triplet paper-190209kmak.xls

Page 12: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

agust, heima, ...january09/Term values for triplet paper-190209kmak.xls

Page 13: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

5

5

4

3 4 5 6 7

3 4 5 6 7

g3S+(1) (e) V1S+,v´=9

66

E(e)

E(e))

To be expected:

+

+

+

-

-

-

-

-

+

parities

Page 14: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

i.e. from D(DE) should be about 3.86 ~ 4

From above it looks as is the absolut maximum deviations of DE´s (i.e. D(DE)´s) are Something like: D(DE)f3D2: 0.5 f3D1 1g3S+(1) 2

If i try using D(DE) = 0.5 I obtain:Now I go back to and calculate corresponding W12´:

W12(5) 5,48DE 17,48DE0 13,61722DE-DE0 3,862776(DE-DE0)/2 1,931388

agust,heima,...january09/Term values for triplet paper-030309kmak.xls

Let´s now see what shifts the W12 values obtained for f3D2 <-> V,v´=8 interaction will correspond to

(DE-DE0)max 0,5W12 2,075452W12 ca 2

agust,heima,...january09/Term values for triplet paper-030309kmak.xls

av. Terms

DE(f3D2-V f3D2,v´=0 abs(DE(f3D2-Vv´=8)) from KM W12=

C12=0.5+sqrt(DE**2 - 4*W12**2)/(2*DE)

82225,8 v´=8) av. terms W12max 0.37*(J´(J´+1))1/282232,1282244,75 -164,856 82079,9 164,8555 82,42775 164,9 0,9063112 0,9999782263,67 -118,526 82145,15 118,5261 59,26303 118,7 1,2817176 0,99988382289,14 -57,8775 82231,26 57,87753 28,93876 57,7 1,6546903 0,99918282320,61 17,47426 82338,08 17,47426 8,737129 17,1 2,02657346 0,98636482358,43 107,1982 82465,63 107,1982 53,59912 107,4939 2,39787406 0,999499

alfa = 4,232beta= 1W12´= 0,37n 0,5shift, de 0f 1abs(35) 0,011763242

agust,heima,...january09/f3D2&Vv8-020309ak:

Page 15: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

Exp.

Calc.

I(35Cl

+ )/I(H

35Cl

+ )

Now let´s make a model including the Gateway mechanism.

Page 16: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

Ry0Ry1

V

t3S

Page 17: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

EWE

cc

cHClIClI

tocloseprobablyifcc

HClIClI

ccandccandfor

cccc

HClIClI

ccHClI

smallprobablyccHClI

ccClI

smallbuttsignificanccClI

24

21;

1))1((

)()(

(?)1;1;11

))1(()()(

11

)()(

)(

(?);;)(

)(

;)(

212

2

222

2

22

22

22

22

21

22

22

21

1

2

222

211

21

222

222

211

2222

21

21

222

21

22

Page 18: f3D2 energetics and interaction with V,v´=8 & f3D1 energetics and interaction with V,v´=9

#;

´)(2)1´´(4´)(

211

)1(´)(2

)1´´(4´)(21

)()(

2´12

2

2´12

2

JEJJWJE

JEJJWJE

HClIClI

#;

´)(2)1´´(4´)(

211

´)(2)1´´(4´)(

21

)()(

2´12

2

2´12

2

JEJJWJE

JEJJWJE

HClIClI

Compaired to

before