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Optical Feshbach resonances in ultra-cold ytterbium
M. Borkowski, A. A. Buchachenko, R. Ciuryło,
P. S. Julienne, Y. Takasu, Y. Takahashi
The project „Precise Optical Control and Metrology of Quantum Systems” is supported
by the Foundation for Polish Science program TEAM cofinanced by the European
Regional Development Fund. This research is a part of the scientific program
of the National Laboratory FAMO in Toruń, Poland.
Support
Bound states of Yb2
(11)
(13)
(38)
(18)
(21)
(74)
(26)
(19)
(40)
(50)
(23)
(26)
Borkowski al, Phys. Rev. A 80, 012715 (2009).
Model potential
Exp. Theo.1 Theo.2
C6 [Eh a06] 1.932(30) x103 2.07(20) x103 1.929(39) x103
C8 [Eh a08] 1.9(5) x105 2.02(20)x105
1Zhang and Dalgarno, Mol. Phys. 106, 1525 (2008).2Safronova et al, Phys. Rev. Lett. 109, 230802 (2012)
Scattering resonances
,10 ,6 ,2
,12 ,8 ,4
g
g
l
aa
l
a
Gao, Phys. Rev. A 62, 050702(R) (2000); 64, 010701(R) (2001).
Kr 100
Spectra
172Yb 176Yb
Borkowski et al, Phys. Rev. A 80, 012715 (2009).
174Yb
T=25 K
Tojo et al, Phys. Rev. Lett. 96, 153201 (2006).
Two channels model
)1)(2(1212
1
12
)1(
12
)1()1(
12
1
12
1
1
1001
0110
JJBVJ
JV
J
JVV
J
JJ
VVJ
JJJBJV
J
JV
J
J
Jl
Jl
2
2
2 rB
1)1(2)(
)12(441)(
2
1
1)1(2)(
)12(441)(
2
1
2
01
22
01
01101
2
01
22
01
01100
JJBVV
JB
VV
BVVVV
JJBVV
JB
VV
BVVVV
)12(
)12()1( )1(
)12()1(
)12( 2)1(
11
00
-
JJ
JJJBJV
JJ
JJJJBV
01for VVB
Model potential
Wang and Dolg, Theor. Chem. Acc. 100, 124 (1998).
Shape of ab initio potential is very different
Experiment and theory
174Yb ∆e(0u) [MHz]
Je=1 Je=3
Exp. Theor. Exp. Theor.
-4.4(1.0) -4.2 -3.0
-9.5(1.0) -9.7 -7.5
-19.7(1.0) -20.1 -16.1(2.0) -16.7
-37.4(1.0) -38.5 -32.5(2.0) -33.3
-68.6(1.0) -69.1 -61.7
-119.1(2.0) -117.8 -107.5
-191.3(1.0) -192.3 -179.0(2.0) -178.2
-302.3(1.0) -302.5 -284.5(2.0) -283.9
-461.1(1.0) -461.3 -437.4
-684.6(1.0) -684.9 -654.7(2.0) -654.6
-993.7(1.0) -993.7 -955.9
-1412.8(1.0) -1413.0 -1366.7(2.0) -1366.4
-1973.5(1.0) -1973.9 -1918.1(2.0) -1917.3
176Yb ∆e(0u) [MHz]
Je=1 Je=3
Exp. Theor. Exp. Theor.
-3.1 -2.1
-7.9(2.0) -7.5 -5.9(2.0) -5.7
-16.5(2.0) -16.0 -13.9(2.0) -13.1
-32.0(2.0) -31.2 -27.4(2.0) -26.8
-56.2(2.0) -57.0 -50.0(2.0) -50.5
-98.5 -89.4
-162.6 -150.1
-258.2(2.0) -258.3 -242.8(2.0) -241.7
-398.1(2.0) -397.1 -376.4(2.0) -375.5
-594.4(2.0) -593.8 -567.3(2.0) -566.3
-867.6(2.0) -866.7 -832.7(2.0) -832.2
-1240.1(2.0) -1238.9 -1196.2
-1738.5 -1686.5
Borkowski et al, Phys. Rev. A 80, 012715 (2009).
Optical length
22opt
22optbg
21
1)(
2
1),(
21)(),(
IlIb
IlaIa
E pegee
Reduced detuning
Fedichev et al, Phys. Rev. Lett. 77, 2913 (1996).
Bohn, and Julienne, Phys. Rev. A 60, 414 (1999).
Ciuryło et al, Phys. Rev. A 71, 030701 (2005).
Blatt et al, Phys. Rev. Lett. 107, 073202 (2011).
Optical length 174Yb, Je=1
∆e(0u)
[MHz]
lopt/I
[a0/(W cm-2)]
-4.2 1.6×105
-9.7 5.5×104
-20.1 2.0×104
-38.5 7.9×103
-69.1 3.1×103
-117.8 1.2×103
-192.3 466
-302.5 150
-461.3 33
-684.9 1
-993.7 4
-1413.0 17
-1973.9 27.5
I= 1 W
Yamazaki et al, Phys. Rev. Lett. 105, 05045 (2010).
Experiment with 174Yb
ascat=+104 a0
ascat=-594 a0
ascat=-24 a0
ascat=+250 a0
ascat=+63 a0
Optical tuning of scatering length
Experiment with 172YbEnomoto et al, Phys. Rev. Lett. 101, 203201 (2008).
Fatemi et al, Phys. Rev. Lett. 85, 4462 (2000).
Heteronuclear bosonic system
rotA HHH int 2
12121 egge
AAAA
eg
ge
E
E
egge
AA
AA
A
A
AAAA
21
21
2
1
2121
0
0
1
1
2
1
2
12
1
2
1
1 1
2121
2121
EEEE
EEEE
AAAA
AAAA
1
1
0
0
11
u
g
V
V
AH
intH
AH
Heteronuclear bosonic system
222121 )1(
2
1
ugug
EEEEAAAA VVVV
ug
EEAA
VV21for
VEEAA 21
2
1
EE
EEAA
AA ugug
21
21
2)1(
22
)1(1
2
)1(12
VVVV
EEAA
ug
21for VV
EE
C
AA 21
2
3res
6
)(1 C
EEE
p
AA
I21
)1(
C3 [Eh a03]
0u -0.1949(11)
0g +0.1949
1g -0.0974
1u +0.0974
Heteronuclear bosonic system
C3 [Eh a03]
0u -0.1949(11)
0g +0.1949
1g -0.0974
1u +0.0974
EEE
p
AA
I21
)1(
ug
u g
Borkowski et al, Phys. Rev. A 84, 030702(R) (2011).
gerade-gerade transitions
ggug
Meath, J. Chem. Phys. 48, 227 (1968).
Machholm, Phys. Rev. A 64, 033425 (2001).
Ab initio potential
Buchanchenko et al, Eur. Phys. J. D 45, 147 (2007).
174Yb2 N=72
Experiment with kHz accuracy.
Ab initio potential leads to small reduction of
residuals on average from about 83 kHz to 64 kHz
Zhang and Dalgarno, Mol. Phys. 106, 1525 (2008).
Testing models
Tang and Toennies, J. Chem. Phys. 80, 3726 (1984).
Zhang and Dalgarno, Mol. Phys. 106, 1525 (2008).
12
1
22 )(i
ii EuE
6
66
8
88 )()()(
r
Crf
r
CrfrV
2
6888
2
4666
)(
)(
rWCCrf
rWCCrf
FS
FS
rCrf
rCrf
FS
FS
8
218
6
2
16
16
)0()0(531)(
4
)0(23)(
small r
large r
long range
Summary
• Bosonic and fermionic isotopes of Yb offer large variety of the scattering lengths.
• The simple mass scaling approach works well in case of cold collision of Yb atoms in ground and excited state.
• Results obtained for homo-nuclear systems can be extended for hetero-nuclear.
• Gerade-gerade transitions can be well described and results are consistent with dose for gerade-ungerade transitions