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The Graphical Bepresentation of The Relations Between The Multipole Mixing Ratios And The Angular Correlation Coeffıcients.

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Çok - Kutuplu Karışım Oranları ve Açısal

Korelasyon Katsayıları Arasındaki Bağıntıların

Grafikle Gösterilmesi.

The Graphıcal Bepresentatıon of The Relatıons

Between The Multıpole Mıxıng Ratios And

The Angular Correlatıon Coeffıcıents.

İhsan ULUEK *> Yılmaz GÜNEY**'

*) S.D.M.M. Akademisi Ph. D.

**) S.D.M.M. Akademisi Dipl. Eng.

ÖZET

Çok-kutuplu (8-Multipol) karışım oranları deneysel olarak kore­

lasyon katsayılarından elde edilmektedir. Bu çalışmada 2(1,2)2

, 6>ü ;

2( 1,2)2 , 8 <0 ; 3(1,2)2,8>0 ; 3( 1,2)2, 8<0 ; 3( 1,2)3 ,8>0 ; 3( 1,2)3 ,

8<0 ; 2( 1,2)3 , 8>0 ; 2( 1,2)3 , 8<0 korelasyon katsayıları ve karışım

oranlan arasındaki bağıntıları grafiksel olarak gösterilmiş ve yapılan

deneysel çalışmalara hesaplama kolaylığı getirmesi sağlanmıştır.

SÜMMARY

Multipole miaing ratios (8) are determined from the experimental

correlatıon coefficienis. İn this work the relation between 2(1,2)2,8>0 ;

2(1,2)2 , 8<0 ; 3(1,2)2,8>0 ; 3(1,2)2 , 8<0 ; 3(1,2)3,8>0 ; 3(1,2)3 ,

8<0 ; 2( 1,2)3,8>0 ; 2(1,2)3 , 8<0 correlatıon coefficients and mixing

ratios are represented graphically and a practical way is shoum for the

czperimental calculations.

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The Graphical Representation of Tht Relations Betvveen The Multipole... 69

INTRODUCTION

The importance of angular correlations and the multipole mixing ratios has been shown previously (1-3); the experimental application of these vvere also discussed in (1,4-6). In order to prepare the results of these experimental vvork practically and check the data at önce it is very ııseful to have the graphical relation betvveen the angular correla- tion coefficicnts and themultipole mixing ratios.

THE RELATİON BETVVEEN THE CGRRELATION COEFFICIENTS AND THE MULTİPOLE MINING RATİOS

Forthe yi—y.(0) correlations (1) :

W(0)=

Akk Gtk Ukk Qkk Pkk

(cos0) k-even

In thiseguation Akk = Ak(Yı)Ak(y2) and A

*

(8 1)=[F*(LıL 1J(Jin/)—281FA(L1L1'(7IJın()+6I2FA(LI,L1'Ji</.n<)](l + 612)-1 (0 At(Y2)

= [Fk(L2L2JfJ,nl)

+ 282Fi(L2L2V/J/n/) +

k{L2 L2 JfJ

+ 8ı2)-’ <«>

Here 5 is the multipole mixing ratio, and it is defined as the intensity ratio of L' multipole to the L multipole ; and are given by :

8]— <

Jını

IItc

L

j II •//.-•/

ini

II it II

J >

82 =

<Jinl || tt’Li

II

Jf>KJinl

II t.L2 II

Jf>

SOME SPECIAL CASES AND THE1R GRAPHS

For 8<0 and 8>0, in the J(L, L')J' notation 2(1,2)2 , 2(1,2)3 , 3 (1,2)2 and 3 (1,2) 3 States are of interest. Because in practice these are the most freauent ones and experimentaly it is very much appreciated to knovv these at önce (4-6). The graphical representation of these ca- ses have been determined from (i) and (ii) and are shovvn belovv.

When the coefficients are obtained experimentaly for W(0) the re­ sults are divided by GkkUkkQkk and Akk vvill be found. The relation bet­ vveen Ak(Yı) , Ak(y2) and Akk is :

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2->2 transitions and 5 = y(Z>' 2)/y(Z>=l) ; 5> 0] as a function of 6-

Flg. 2) The Angular Correlation coefficients A.ı and for the 2-»2 transitions and 5=y (L' = 2)/y(Zj=l) ; 5>0] as a function of g.

(4)

The Graphıeal Representation of The Relations Betweem The Mııltipole... 71

(5)

72 thsan ULUEİR — Yılmaz. GÜNEY

(6)

The Graphıcal Representatlon of The Relations Between The Multipole... 73

Fig. 7) The Angular Correlation coefıicients A„(y2> and A [for the 2_>3 transitions and 5 = y(Zz 2)/y(L = l) ; 5> OJ as a fıınctlon of 5-

Fig. 8) The Angular Correlation coefficients A.(y> and At(y.) Ifor the 2—>3 transitions and 5 = r<^' =2)/y(L = l) ; 5<0] as a function of g.

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74 İhsan ULUER — Yılmaz GÜNEY

Au = Ak(Yı) Ak(y2)

and therefore, if Ad-^) or Al (yj are found expereimentaly or theoreti- caly then the multipole mixing ratio can be found easily from the graphs below.

If the experiment is an electron y(8) correlation then the coefficients are also divided by bk partide paremeters and the püre Ak coefficients are obtained, and thus the results of 5 are read from the graphs.

Our thanks are due to the S.D.M.M. Academy Mathematics division staff during the boring calculations which lasted for a long time.

R E F E R E N C E S

1) î. Uluer and M. N. Khan, S.D.M.M.A. Bullettn, SEA - 1, (1976), 46 - 61.

2) R. M. Steffen and K. Alder, «Electromagnetic Interaction in Nuclear Spectros- copy», Ed. W. D. Hamilton, Nord Holland, (1975), 505 - 582.

3) J. K. Tuli. Nuclear Data Sheets 12. (1975), 477.

4) 1. Uluer et. al. Journal of Physics, G - 4, (1975), 476.

5) î. Uluer, Technlcal Journal AEK. Vol. 2, No. 3, (1975), 105.

6) I. Uluer, S.D.M.M.A. Dergisi, MMA - 1, (1976), 41 - 57.

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