Bose 2.2 User Manual Page 91

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the images, taken after the expansion from the lattice, we observe the interference pattern
of the condensate and, in addition, a thermal cloud in the background (see Fig. 5.8(a)).
To extract the atom number in the condensate, we first integrate the recorded 2D
0 2 4 6 8 10
0
10
20
30
40
50
y
z
absorption image integrated along z
optical density
y (in pixels)
(a) (b)
Fig. 5.8, Data acquisition and evaluation:
(a) 2D density distribution of the atomic
cloud after time-of-flight, recorded by absorption imaging (lattice depth
U
lat
=
10
E
R
, final scattering length
a
= 20
a
0
). The field of view is (50
×
50)
pixels
2
=
(307
×
307)
m
2
. Red (blue) colors indicate high (low) density. (b) Density
profile in the
y
-direction (black crosses) obtained by integrating the 2D density
distribution along
z
. We extract the BEC atom number from a bi-modal fit
(red line). Before performing the full fit, we fit the thermal cloud (blue line)
to the wings of the density profile, i.e. we disregard the region between the
magenta horizontal bars.
density distribution along the
z
-direction. Then, we perform a one-dimensional bi-modal
fit, accounting for the presence of the condensate and the thermal cloud as shown in
Fig. 5.8(b). The 1D fitting function for the BEC is obtained by integrating the 3D density
of a single condensate (see Eq. (2.22)) over the x- and y-direction with the result [197]
n
BEC,1D
(y, t) =
15 N
BEC
16 R
y
(t)
max
"
1
y
2
R
2
y
(t)
, 0
#
2
. (5.5)
where
N
BEC
is the atom number in the condensate and
R
y
(
t
) is the radius of the BEC
after an expansion of time t. The thermal cloud has the following Gaussian shape,
n
th,1D
(y, t) =
N
th
2π l
y
(t, T )
exp
"
y
2
2l
2
y
(t, T )
#
, (5.6)
with
N
th
the number of thermal atoms and
l
y
(
t, T
) the width of the thermal cloud,
determined by the expansion time
t
and the temperature
T
of the sample. We briefly
explain the fitting procedure in Fig. 5.8 while more technical details are given in Ref. [122,
Ch. A.2.]. By using the 1D fitting method, we obtain a reliable evaluation of the BEC
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