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![Page 1: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/1.jpg)
Refractive Index Enhancement in Atomic Vapors
Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes
Department of Physics, University of Wisconsin Madison, WI
![Page 2: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/2.jpg)
Key Question
How much can we increase the refractive index, n, of an atomic medium while maintaining vanishing absorption?
When an electromagnetic wave is in a medium with refractive index n, the wavelength of the wave is /n. As a result the resolution is increased.
![Page 3: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/3.jpg)
Two-level scheme
g
e
Ep
e2
max0
1
2 e
N
A laser beam tuned close to a two level resonance can experience a large refractive index.
In a gas with a pressure of 1 torr, can get values as large as 100. However, thiseffect is not useful since, is just as large.
![Page 4: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/4.jpg)
Two two-level scheme
g
1
pE
g
2
+
g
e
1
pE1cE+
g
e
2
pE 2cEpE
The interference between an absorptive resonance and an amplifying resonancecan result in a large refractive index with vanishing absorption.
M. Fleischhauer et. al. Phys. Rev. A 46, 1468 (1992).
![Page 5: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/5.jpg)
Numerical calculation in Rbsu
scep
tibili
ty
10-2
p (MHz) p (MHz)
10-2 10-2
p (MHz)
-4
-2
0
2
4
-1 0 1 2 3 4-4
-2
0
2
4
-1 0 1 2 3-4
-2
0
2
4
-1 0 1 2
1F
2F
pE1cE
2F 3F
pE 2cE87Rb 85Rb
N=1015 /cm3
Ic1 Ic2 100 W/cm2
Detuning=30 GHz
![Page 6: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/6.jpg)
Maximum susceptibility
1 10 102 103 104
10-2
10-1
1
10
Ic1, Ic2 (W/cm2)
real
par
t of
susc
eptib
ility
10-3
How much can one increase the real part of the susceptibility while maintainingvanishing imaginary part?
2
max0
1
2 e
N
D. D. Yavuz, Phys. Rev. Lett. 95, 223601 (2005)
![Page 7: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/7.jpg)
First experiments
F=0, 1, 2, 3
Ep Ec
optical pumpinglaser
F=1
F=287Rb vapor cell
Ep
Ecoptical pumpinglaser
85 GHz
beam detectionand diagnostics
87Rb energy level diagram
B. E. Unks, N. A. Proite, and D. D. Yavuz, Rev. Sci. Inst. 78, 083108 (2007).
N=1.71013 /cm3
![Page 8: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/8.jpg)
Raman self-focusing and self-defocusing
/ 2π (MHz)
norm
aliz
ed tr
ansm
issi
on
0.8
1
1.2
1.4
-8 -4 0 4 8
The refractive index increases and decreases on either side of the resonance causesself-focusing and self-defocusing.
>0, self-focusing
<0, self-defocusing
![Page 9: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/9.jpg)
Self-focused and defocused profilesIn
tens
ity
x (mm)
0
0.5
1
1.5
2
-1 -0.5 0 0.5 10
0.5
1
1.5
2
-1 -0.5 0 0.5 1
x (mm)
>0, self-focusing <0, self-defocusing
Inte
nsity
![Page 10: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/10.jpg)
Future work
Cold atomic clouds offer key advantages over vapor cells:
Narrow Raman linewidths
Tighter focusing
Orthogonal geometries
Spatial Raman Solitons
Combine an absorptive resonance with an amplifying resonance
![Page 11: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/11.jpg)
All-optical devices
Ep
atomic cloud
Ec1 Ec2
Intensity pattern
refractive index pattern
I(x)
n(x)
Since the refractive index enhancement is proportional to the intensity of the control lasers, an intensity pattern is transferred to a refractive index pattern.
![Page 12: Refractive Index Enhancement in Atomic Vapors Deniz Yavuz, Nick Proite, Brett Unks, Tyler Green, Dan Sikes Department of Physics, University of Wisconsin.](https://reader035.fdocuments.in/reader035/viewer/2022062805/5697bffb1a28abf838cc0d85/html5/thumbnails/12.jpg)
Conclusions
Far-off resonant Raman systems offer a new approach for achieving largerefractive index with vanishing absorption.
As a first step, we have observed Raman self-focusing and self-defocusing in an alkali vapor cell.
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Adiabatic vs non-adiabatic evolution
before the cell after the cell
0 2 4 6
inte
nsit
y (a
. u.)
inte
nsit
y (a
. u.)
time (s) time (s)0 2 4 6
time (s)
inte
nsit
y (a
. u.)
0 4 8 0 4 8time (s)
inte
nsit
y (a
. u.)
adiabatic evolution
non-adiabatic evolution