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Time Evolution of Coherent Excitation (STIRAP)
Time Evolution of Coherent Excitation (STIRAP)
How Camp
7 April, 2004
How Camp
7 April, 2004
What is Coherent Excitation?What is Coherent Excitation?
0.5
1.0
Ex
cite
d p
op
ula
tio
n
Incoherent
Coherent
ARP
0.0|1>
|2>
I
Rabi Period
Time
2-Level
0.5
1.0
0.0
|1>
|3>
3-Level
|2>
Pump
StokesRab
i F
req
uen
cy
Time
Stokes Pump
What is STIRAP?What is STIRAP?E
xcit
ed F
ract
ion
Time
0
1
|1>
|2>
|3>
ApplicationsApplications
• Control of Chemical Reactions
• Atom Optics
• Laser Cooling
• Measurement of Weak B-Fields
• Cavity QED
• BEC From Bergmann, et al. Annu. Rev. Phys. Chem. (2001)
Technique: What Others DoTechnique: What Others Do
5S1/2 F=3
Monitor 420 nm fluorescence from 6P-5S transition
5P3/2 F’=4
5D5/2 F’’=5
6P3/2
Stokes
Pump
Monitor 780 nm fluorescence from
MOT
780 nm
776 nm
85Rb
Problems:Problems:
5S1/2 F=3
Monitor 420 nm fluorescence from 6P-5S transition
5P3/2 F’=4
5D5/2 F’’=5
Stokes
Pump
Monitor 780 nm fluorescence from
MOT
780 nm
776 nm
• Inaccurate measure of 5S atoms
• Time resolution limited by lifetimes
• Inability to see all transitions
85Rb
6P3/2
Technique: What We Can DoTechnique: What We Can Do
5S1/2 F=2
5P3/2 F’=3
4D5/2 F’’=4
Stokes
Pump
780 nm
1529 nm • Accurate excited-state fractions
• Measure all 3 populations
• Monitor time-evolution of process (~2 ns resolution)
87Rb
What Theory PredictsWhat Theory Predicts
Stokes (L2)
Pump (L1)
4D
5P
5S
Delay = -30 ns
What Theory PredictsWhat Theory Predicts
Stokes (L2)
Pump (L1)
4D
5P
5S
Technique: How We Do ItTechnique: How We Do It
MOTRIMSMOTRIMS
Q-Value SpectraQ-Value Spectra
50 75 100 125 150
0
500
1000
1500
2000
2500
3000
3500
Co
un
ts
Q-Value (Channel)
5s-3p
4d-3d5s-3s
-5
-4
-3
-2
-1
0
4d 2D5/2
, 4d2D3/2
4f 2F7/2
, 4f2F5/2
4s 2S1/2
4p 2P1/2
, 4p 2P3/2
23Na
4s 2S1/2
3d 2D5/2
, 3d2D3/2
3p 2P
1/2, 3p
2P
3/2
3s 2S
1/2
12f
4d 2D3/2,5/2
5p 2P
3/2
5s 2S
1/2
87Rb
Pote
ntia
l Ene
rgy
(eV)
Hold That Thought!Hold That Thought!
Simplified Experimental SetupSimplified Experimental Setup
Ion Beam
Diameter: ~ 500 m
Pump Laser (L1)
Diameter: ~ 200 m
Stokes Laser (L2)
Diameter: ~ 350 m
MOT
Diameter: ~ 600 - 800 m
7 KeV Na+ Rb
STIRAP Laser TimingSTIRAP Laser Timing
Trapping Lasers ONStokes (L2) ON
~50 ns
Pump (L1) ON ~50 ns
Trapping Lasers ON
Trap Off Time: ~ 0.5 s
Total Period: 5 s
Correlating Q-Value & Laser TimingCorrelating Q-Value & Laser Timing
+ =
50 75 100 125 150
0
500
1000
1500
2000
2500
3000
3500
Cou
nts
Q-Value (Channel)
2D TAC Spectra
TAC SpectraTAC Spectra
Q-Value (Channel)
Tim
e (s
)
50 100 150
0.5
1.0
1.5
2.0
2.5
0.0
5s-3p 5p-3p 5s-3s
4d-3d4d-3s
5p-3p
Time Evolution of STIRAPTime Evolution of STIRAP
Future WorkFuture Work
• Explore Temporal Evolution of STIRAP:
• Pulse Delay
• Pulse Width
• Laser Intensity
• Laser Detuning
• See Rabi Flops ?!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
New MOTRIMS!New MOTRIMS!
How Do We Measure Q Value?How Do We Measure Q Value?
Q: energy defect
: Scattering angle (Lab frame)
Pr|| , Pr : parallel and perpendicular recoil momentum components
PP , PP’ : projectile momentum before and after the collision
Vp: projectile velocity
nc: number of transferred electrons
pp
pP’
pr
rp
rp
||
2|| 2
1PcrP VnPVQ
p
r
P
P
Chopping Our Lasers
-3 -2 -1 0 1 2 3-1000
0
1000
2000
3000
4000
5000-3 -2 -1 0 1 2 3
0
5000
10000
15000
5s-3p
5s-3sCo
un
ts
Q value (eV)
AOM Off
5p-3p5s-3s
5s-3p
5p-3d5p-4p
5p-4s
Co
un
ts
Tot
80 90 100 110 120 130 140 15030
40
50
60
70
80
90
100
110
120
130
140
150
Time of Flight difference (ns)
TA
C (
chan
nel)
1.000
1.433
2.053
2.941
4.214
6.037
8.649
12.39
17.75
25.44
36.44
52.21
74.81
107.2
153.6
220.0
100 200 300
0
60
120
180
Cou
nts
TAC (channel)
Capture from 5P Capture from 5S
Chopping Our Lasers