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Application of the Coulomb spheroidal basis for diatomic molecular - - PowerPoint PPT Presentation

Application of the Coulomb spheroidal basis for diatomic molecular calculations T . Kereselidze and G. Chkadua Department of Exact and Natural Sciences, Tbilisi State University, 0179 Tbilisi, Georgia Content: 1. Introduction 2. The Coulomb


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SLIDE 1

Application of the Coulomb spheroidal basis for diatomic molecular calculations

T . Kereselidze and G. Chkadua

Department of Exact and Natural Sciences, Tbilisi State University, 0179 Tbilisi, Georgia

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SLIDE 2

i

E

Content:

  • 1. Introduction
  • 2. The Coulomb spheroidal wave functions
  • 3. Basic equations
  • 4. Obtained results and comparison with the characteristics
  • f the hydrogen molecular ion H2

+

  • 5. Conclusion
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SLIDE 3

S ym m e t rical d iat

  • m ic

m ol e cu l e S฀

2 2 2 2 2

, , , , H H C N O

+ 2 2 2 2 2

, , , , H H C N O

+ ( )

Heitler and London LCAO

Hund and Mulliken

slide-4
SLIDE 4

a

r 

b

r 

Hydrogen molecular ion H 2

+

ZA=1 ZB=1

E

R

slide-5
SLIDE 5

Prolate spheroidal coordinate system

, , ( / )

a b a b

r r r r arctg y x R R ξ η ϕ + − = = =

1 , 1 1 2 ξ η ϕ π ≤ < ∞ − ≤ ≤ ≤ <

slide-6
SLIDE 6

Schrödinger equation for hydrogen molecular ion

( ) ( ) ( )

1 1 1 ( ) 2

a b

R r r ε

± ± ±

  − ∆ − − Ψ = Ψ    

( ) ( )

( , ) ( , ) 2

im n m n n m n m

e X R Y R

ξ ξ η η

ϕ

ξ η π

− ± ±

Ψ =

( ) ( )

( ) 2 2 2 2 2 ( ) ( ) 2 2 2 2 ( ) 2

1 2 ( , ) 2 1 1 ( , ) 2 1 d dX R m R X R d d d dY R m Y R d d ε ξ λ ξ ξ ξ ξ ξ ξ ε η λ η η η η η

± ± ± ±

  − + + + − =   −     − + − − − =   −  

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SLIDE 7

Electornic energies of H 2

+

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SLIDE 8

HE GR OUND AND FIR STEXCIT ED T ER M S OF

2

H +

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SLIDE 9

฀ i st OF P UBL

ICATION: 1 T฀ K e re Se l

id ze ฀

Z ฀ S ฀ M A CHA VA R IA NI A ND G ฀ c h Kad u a฀ E UR

P HYS฀ J ฀ D 6 3 8 1 ฀ 2 0 1 1 ฀ 2 ฀ J ฀ M ฀ P e e K฀ T฀ K e re Se l

id ze ฀

I฀ N oSe l

id ze A ND J ฀

K ie l

KoP f฀

J ฀ P HYS฀ B ฀ A T฀ m ol

  • P t

P HYS฀ 4 0 ฀ 5 6 5 ฀ 2 0 0 7 ฀

3฀ a ฀ d e vd ariaN i฀ t฀ m ฀ K e re Se l id ze ฀ i฀ l ฀ N oSe l id ze ฀ e ฀ d al im ie r฀ P ฀ S au vaN ฀ P ฀ a N ge l

aN d r ฀ S cot t ฀

P h yS฀

r e v฀ v฀ a 71฀ P ฀ 022512 ฀ 2005฀ 4฀ t฀ m ฀ K e re Se l id ze ฀ i฀ l ฀ N oSe l id ze aN d m ฀ i฀ c h ib iSov฀ J ฀ P h yS฀ b ฀ a t ฀ m ol ฀

  • P t

฀ P h yS฀ 36 853 ฀ 2003฀ 5฀ a ฀ z ฀ d e vd ariaN i฀ t฀ m ฀ K e re Se l id ze aN d i฀ l ฀ N oSe l id ze ฀ K h im ich e SKaia P h ySica v฀ 22 P ฀ 3 ฀ 2003฀ 6฀ t฀ m ฀ K e re Se l id ze ฀ z ฀ S ฀ m ach avariaN i aN d i฀ l ฀ N oSe l id ze ฀ J ฀ P h yS฀ b ฀ a t ฀ m ol ฀

  • P t

฀ P h yS฀ 31฀ 15 ฀ 1998฀ 7฀ t฀ m ฀ K e re Se l id ze ฀ z ฀ S ฀ m ach avariaN i aN d i฀ l ฀ N oSe l id ze ฀ J ฀ P h yS฀ b ฀ a t ฀ m ol ฀

  • P t

฀ P h yS฀ 29฀ 257 ฀ 1996฀

8฀

t฀ m ฀ K e re Se l id ze ฀ h ฀ a ฀ m ou rad aN d m ฀ f ฀ t zu l u Kid ze ฀ J ฀ P h yS ฀ b ฀ a t ฀ m ol ฀

  • P t

฀ P h yS฀ 25฀ 2957 ฀ 1992฀ 9฀ t฀ m ฀ K e re Se l id ze ฀ S ov฀ P h yS฀ J e t f 100฀ 95 ฀ 1991฀ 10฀ m ฀ i฀ c h ib iSov aN d t฀ m ฀ K e re Se l id ze ฀ P re P riN t ia e ฀ 5410฀ 6฀ m oScow ฀ P ฀ 1฀ 43 ฀ 1991฀ 11฀ t฀ m ฀ K e re Se l id ze P roce e d iN g

  • f

g e orgiaN a cad e m y

  • f

S cie N ce S ฀ v฀ 139฀ P ฀ 481 ฀ 1990฀ 12฀ a ฀ z ฀ d e vd ariaN i฀ t฀ m ฀ K e re Se l id ze aN d a ฀ l ฀ z agre b iN ฀ J ฀ P h yS฀ b ฀ a t ฀ m ol ฀

  • P t

฀ P h yS฀ 23฀ 2457 ฀ 1990฀ 13T.฀. ฀ er esel i dze, J. ฀ hys. ฀ : ฀ t . ฀o l . ฀ hys. 20, 1891 (1987) 14฀ t฀ m ฀ K e re Se l id ze aN d b ฀ i฀ K iKiaN i฀ S ov฀ P h yS฀ J e t f 87฀ 741 ฀ 1984฀ 15฀ t฀ m ฀ K e re Se l id ze ฀ S ov฀ P h yS฀ J e t f 69฀ 67 ฀ 1975฀ 16฀ t฀ m ฀ K e re Se l id ze aN d

b ฀ f irSov฀ S ov฀ P h yS฀ J e t f 65฀ 98 ฀ 1973฀

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SLIDE 10

Schrödinger equation for hydrogen-like ion

, , , , ,

1 ( ) 2

a b a b a b a b a b

Z R r ε   − ∆ − Ψ = Ψ      

, ,

( , ) ( , ) 2

im a b a b n n m n m n m

e X R Y R

ξ η ξ η

ϕ

ξ η π

Ψ =

( ) ( )

2 2 2 2 2 , 2 2 2 2 , 2

1 ( , ) 2 1 1 ( , ) 2 1

a b a b

d dX R m ZR X R d d d dY R m ZR Y R d d ε ξ λ ξ ξ ξ ξ ξ ξ ε η λ η η η η η η   − + + + − =   −     − + − − − =   −   

1 n n n m

ξ η

= + + +

slide-11
SLIDE 11

/ 2 , / 2

( ) ( )

ZR n m a b ZR n m

X e W Y e W

ξ η

ξ η

= =

1,2 / 2 ,1 1,2 , / 2 1 ,0

( ) ( )

ZR n m m a b ZR n m m

nh X e W ZR nh Y e W ZR

ξ η

ξ ξ η η

  = −       =    

The Coulomb spheroidal wave functions

1, n m = +

0; n n

ξ η

+ =

1 ฀

2, n m = +

1,2; n n

ξ η

+ =

2 ฀

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SLIDE 12

2 1,2,3 1,2,3 / 2 2 ,1 ,2 1,2,3 2 2 2 1,2,3 1,2,3 , / 2 2 2 ,1 ,0 1,2,3 2 2

( 2 4) 1 ( ) 2 ( 2 4) 1 ( ) 2

ZR n m m m a b ZR n m m m

nh n h X e h m W ZR Z R nh n h Y e h m W ZR Z R

ξ η

ξ ξ ξ η η η

  = − + − − −         = + − − −      

3, n m = +

1,2,3; n n

ξ η

+ =

3 ฀

2 / 2

( ) ( 1)m W ξ ξ = −

2 / 2

( ) (1 )m W η η = −

1 n n n m

ξ η

= + + +

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SLIDE 13

The basic equations

{ }

( , ) ( , )

a im nn m nn m

X R Y R e

ξ η

ϕ

ξ η

( )

( , ) ( , )

a b nn m nn m nn m

Y Y R Y R

η η η

η η

±

= ±

{ }

( , ) ( , )

a im nn m nn m

X R Y R e

ξ η

ϕ

ξ η

1 ( ) ( ) ( ) 1

( ) ( , ) ( , )

n m nn m nn m nn m n n

C R X R Y R

η ξ η η

ξ η

∞ − − ± ± ± = =

Φ = ∑ ∑

( ) ( )

( , , , ) ( , , )

im

R R e

ϕ

ξ η ϕ ξ η

± ±

Ψ = Φ

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SLIDE 14

The basic equations

( )

฀฀ ฀฀

1 ( ) ( ) ( ) ( ) , , 1 n m n nn n n nn n n nn n n

E U V C

η η η η η η

ε

∞ − − ± ± ± ± = =

  − + =    

∑ ∑

฀฀ ฀฀ ฀฀ ฀฀ ฀฀ ฀฀ ฀฀ ฀฀ ฀฀ ฀฀

( ) 2 ( ) ( ) ( ) 2 ( ) , ( ) ( ) ( ) , ( ) ( ) ( )

2 (2 )

nn nn nn nn n n n n n n n n n n n n nn nn n n n n n n n n nn nn nn n n n n

U X X X X V Z X X R Z X X d

ξ η ξ η η η ξ η ξ η ξ η η η ξ η ξ η η ξ η

ξ η ξ η

± ± ± ± ± ± ± ± ± ±

= 〈 〉〈ϒ ϒ 〉 − 〈 〉 〈ϒ ϒ 〉  = − 〈 〉〈ϒ ϒ 〉    + 〈 〉 〈ϒ ϒ 〉  

 2 2

/ 2

n

E Z n = −

( )

฀฀ ฀฀

( ) ( ) ( ) , , n n n nn n n nn

E U V

η η η η

ε ±

± ±

− + =

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SLIDE 15

฀ xac t VAL

UES

0.25

  • 1.4754
  • 1.8980
  • 1.8981
  • 1.8986

0.5

  • 1.4213
  • 1.7318
  • 1.7319
  • 1.7350

0.75

  • 1.3560
  • 1.5753
  • 1.5757
  • 1.5824

1.0

  • 1.2884
  • 1.4410
  • 1.4418
  • 1.4518

1.25

  • 1.2230
  • 1.3283
  • 1.3295
  • 1.3418

1.50

  • 1.1617
  • 1.2338
  • 1.2353
  • 1.2490

1.75

  • 1.1053
  • 1.1541
  • 1.1559
  • 1.1701

2.0

  • 1.0538
  • 1.0865
  • 1.0885
  • 1.1026

2.25

  • 1.0071
  • 1.0286
  • 1.0307
  • 1.0444

2.5

  • 0.9648
  • 0.9788
  • 0.9808
  • 0.9938

2.75

  • 0.9267
  • 0.9355
  • 0.9376
  • 0.9497

3.0

  • 0.8924
  • 0.8978
  • 0.8998
  • 0.9109

3.5

  • 0.8339
  • 0.8357
  • 0.8375
  • 0.8466

4.0

  • 0.7869
  • 0.7873
  • 0.7898
  • 0.7961

4.5

  • 0.7493
  • 0.7493
  • 0.7506
  • 0.7562

5.0

  • 0.7192
  • 0.7192
  • 0.7202
  • 0.7244

6.0

  • 0.6757
  • 0.6757
  • 0.6763
  • 0.6786

7.0

  • 0.6469
  • 0.6469
  • 0.6472
  • 0.6485

8.0

  • 0.6267
  • 0.6267
  • 0.6269
  • 0.6276

9.0

  • 0.6118
  • 0.6118
  • 0.6119
  • 0.6123

10.0

  • 0.6003
  • 0.6003
  • 0.6004
  • 0.6006

12.0

  • 0.5834
  • 0.5834
  • 0.5834
  • 0.5835

16.0

  • 0.5625
  • 0.5625
  • 0.5625
  • 0.5625

20.0

  • 0.5500
  • 0.5500
  • 0.5500
  • 0.5500

R au 1 Z = 1 ≠ Z 1 ≠ Z

e l e ct roN ic e N e rgie S for St at e

1sσ

( ) 1

( )

s

R au

σ

ε +

slide-16
SLIDE 16

e l e ct roN ic e N e rgie S for St at e

2pπ

฀ xac t VAL

UES

0.25

  • 0.3746
  • 0.4880
  • 0.4980
  • 0.4980

0.5

  • 0.3735
  • 0.4923
  • 0.4923
  • 0.4923

0.75

  • 0.3716
  • 0.4839
  • 0.4839
  • 0.4841

1.0

  • 0.3692
  • 0.4736
  • 0.4737
  • 0.4741

1.25

  • 0.3662
  • 0.4622
  • 0.4623
  • 0.4631

1.50

  • 0.3627
  • 0.4503
  • 0.4504
  • 0.4517

1.75

  • 0.3589
  • 0.4380
  • 0.4382
  • 0.4402

2.0

  • 0.3548
  • 0.4259
  • 0.4261
  • 0.4288

2.25

  • 0.3504
  • 0.4140
  • 0.4143
  • 0.4176

2.5

  • 0.3458
  • 0.4025
  • 0.4029
  • 0.4068

2.75

  • 0.3411
  • 0.3914
  • 0.3919
  • 0.3964

3.0

  • 0.3363
  • 0.3808
  • 0.3814
  • 0.3864

3.5

  • 0.3266
  • 0.3610
  • 0.3619
  • 0.3678

4.0

  • 0.3169
  • 0.3432
  • 0.3443
  • 0.3508

4.5

  • 0.3073
  • 0.3272
  • 0.3285
  • 0.3354

5.0

  • 0.2979
  • 0.3129
  • 0.3143
  • 0.3214

6.0

  • 0.2803
  • 0.2884
  • 0.2899
  • 0.2970

7.0

  • 0.2642
  • 0.2684
  • 0.2699
  • 0.2766

8.0

  • 0.2499
  • 0.2519
  • 0.2534
  • 0.2595

9.0

  • 0.2374
  • 0.2383
  • 0.2397
  • 0.2450

10.0

  • 0.2265
  • 0.2269
  • 0.2282
  • 0.2327

12.0

  • 0.2092
  • 0.2092
  • 0.2102
  • 0.2133

16.0

  • 0.1871
  • 0.1871
  • 0.1876
  • 0.1888

20.0

  • 0.1745
  • 0.1745
  • 0.1747
  • 0.1751

( ) 2

( )

p

R au

π

ε +

R au 1 Z = 1 ≠ Z 1 ≠ Z

slide-17
SLIDE 17

v ariat ioN al P riN ciP l e

( )(

, )

i

d Z R dZ ε ± =

( ) ( ) ( ) ( ) ( )

฀ ( , , ) ( , , ) ( , ) ( , , ) ( , , )

i i i i i

R H R Z R R R ξ η ξ η ε ξ η ξ η

± ± ± ± ±

〈Φ Φ 〉 = 〈Φ Φ 〉

slide-18
SLIDE 18

t h e e ffe ct ive ch arge aS a fu N ct ioN

  • f

r

slide-19
SLIDE 19
slide-20
SLIDE 20

m ol e cu l ar

  • rb it

al corre l at ioN

R UL E 2

u u

n n n l n m

η η

= + = +

1 2 1

u u

n n n l n m

η η

= + + = + + 2 2 1

u u

l m n l m n

η η

− = − = +

1

r u u

n n l nξ ≡ − − =

  • r

sym m et r i c st at es ฀

  • r

ant i sym m et r i c st at es

slide-21
SLIDE 21

Thank you for attention!