Helium Trimer in the Framework of Helium Trimer in the Framework of Faddeev Approach Faddeev Approach Elena Kolganova Elena Kolganova BLTP JINR, Dubna, BLTP JINR, Dubna, Russia Russia In collaboration with A.K.Motovilov (JINR Dubna) W.Sandhas (PI Bonn) 1 Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)
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Helium Trimer in the Framework of Faddeev Approach
Helium Trimer in the Framework of Faddeev Approach. Elena Kolganova BLTP JINR, Dubna , Russia. In collaboration with A.K.Motovilov (JINR Dubna) W.Sandhas (PI Bonn). Two-body and three-body, experiment. 4 He - 4 He. - PowerPoint PPT Presentation
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Helium Trimer in the Framework Helium Trimer in the Framework of Faddeev Approachof Faddeev Approach
Elena KolganovaElena KolganovaBLTP JINR, Dubna, BLTP JINR, Dubna,
RussiaRussia
In collaboration with
A.K.Motovilov (JINR Dubna)
W.Sandhas (PI Bonn)
1Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)
Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)2
First observation by Luo et al. (1993) and Schöllkopf, Toennies (1994)
First measurement of the bond length by Grisenti et al.(2000)
Estimation of the binding energy and scattering length
When the total angular momentum L of the system is fixed, the three-body dynamics is constrained onto three-dimensional internal space [5], which can be parametrized by coordinates
For zero angular momentum the Faddeev equations in internal space are given by the set of three coupled three-dimensional equations
0( ) ( , , ) ( , , )H V E V
or in hyperspherical coordinates 2 2 ˆ ˆ, tan / , ( , )x y y x x y
1/ 20
exp( )( , , ) ( ) exp( ) ( ; ) ( , ; )d
i Ex y x ipy a E A E
7Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)
E.Kolganova (Dubna)E.Kolganova (Dubna) 88
For computational purposes, one can reduce the dimension by expanding the Faddeev components into an auxiliary basis, at the expense of dealing with an infinite number of partial equations. Expanding the function F in a series of bispherical harmonics
2 2
0 2 2 2 2
( 1) ( 1)l lH
x y x y
( )
,
( , )( , , ) | 0l
l
x yF x y l
xy
One can obtain the partial equation
' '
1( ) ( ) ( )
0 ' '' ' 1
( ) ( , ) ( , , ) ( , )l ll l
l
H V E x y V d h x y x y
2 2 2 2
2 2 2 2
2
2
x c x s y c s x y
y s x c y c s x y
The asymptotic boundary conditions for the partial-wave Faddeev components of the 2’2,3 scattering wave function for and/or reads ’ and/or y’ reads
( ) ( )' ' ' ' ' ' ' ' ' '
exp( )( , ) ( ) ( ) ( ) ( ) ( ) ( , )l ll l l l l
i Ex y x j py x h py a p A p
Where p is the relative moment conjugate to Jacoby variable y, E is the scattering energy,
stand for the spherical Bessel and Hankel functions2
and' ',E p j h
8Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)
Bogolyubov Conference, August 24, 2009 Elena Kolganova (JINR, Dubna)9
Three-body, theorybound states and scattering4He3 and 3He 4He2
9Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)
Bogolyubov Conference, August 24, 2009 Elena Kolganova (JINR, Dubna)10
Three-body, theory bound states
4He3
V. Kolontsov
10Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)
• My collaborators - Prof. A.K.Motovilov and Prof. W.Sandhas
•Diploma student – V.Kolontsov
•Alexander von Humboldt foundation
•Heisenberg-Landau Program
Few-Body Conference, August 31, 2009 Elena Kolganova (JINR, Dubna)11
to see the influence of applying 3D eq. to their values and positionsKolganova E.A. and Motovilov A.K. Mechanism of the Emergence of Efimov States in the 4He Trimer Yad. Fiz. 1999. V. 62. P. 1253–1267 [Phys. At. Nucl. 62, 1179 (1999)].