b) Time Resolved Laser Spectroscopy of Optical Transients
Ultrashort excitation of atoms and molecules allows time resolved observation of excited states
relaxation and measurement of coherent transients.
For observations on a picosecond time scale typical electronic detectors are not fast enough.
Therefore, methods of higher time resolution are applied, which take advantage of transforming
the time scale t to a length l via the velocity v with t = l/v.
Fast Beam Spectroscopy
Ions can be accelerated up to velocities of several % of the speed of light c. When these ions
pass a gas cell or a thin carbon foil, they are further ionized or also neutralized and at the same
time excited to higher atomic states.
Subsequent selective excitation with a conti-
nuously operating laser allows a well controlled
population change of the involved atomic states.
By measuring the fluorescence of the atoms or
ions with and without laser excitation as a func-
tion of the time of flight (distance after excita-
tion) makes possible cascade free lifetime mea-
surements of highly excited atomic or ionic
states on a picosecond time scale.
A sufficiently short excitation can also prepare coherent superpositions of sub-levels in the ex-
cited or lower state, when the inverse of the excitation time covers the splitting of adjacent sub-
levels. Then coherent transients are observed on the free induction decay. These transients are
oscillating with the respective sub-level splitting frequencies and are known as quantum beats.
They allow Doppler-free measurements of splitting frequencies.
Quantum Beats in Forward Scattering
An excitation and detection scheme using a transformation of time to length by the speed of
light c is known as pump-probe experiment. The time evolution of coherently excited states after
an excitation by an ultrashort pump pulse can
sensitively be detected by a time delayed
probe pulse, which passes an optical delay line
and crossed optical polarizers. Recording the
average transmitted intensity of the probe pul-
ses behind the polarizer as a function of the
delay then allows to sample the time evolution
of the coherently prepared sub-states in for-
ward scattering.
Since mode-locked lasers are typically generating pulses with repetition rates in the MHz up to
the GHz range, integration over millions of pulses for each delay time significantly improves the
signal-to-noise ratio.
A measurement with
85
Rb (72% abundance)
and
87
Rb (28%) demonstrates the high sensiti-
vity and time resolution of the set-up for the
observation of coherent transients in the time
domain, reflecting directly the respective level
splittings of the excited and ground states.
Quantum Beats at “Negative” Delay Times
The accuracy of measuring frequency splittings in the time domain is generally limited by the
finite delay time, and thus the observation time of typically several ten nanoseconds.
With a synchronously pumped mode-locked and cavity dumped dye-laser, however, long lived
coherent transients as they are expected in the ground state, can also be measured after delay
times of several µs, and this with ps time resolution.
Taking advantage of the well-known and extremely stable laser pulse separation time an atomic
coherence created by a pump pulse, can be sampled by a probe pulse derived from the next
pulse of the pulse train. At “negative” delay times then the time evolution of atoms is measured
after one pulse period reduced by the respective delay time.
This figure shows the beat pattern of the
85
Rb
ground state splitting with 3.04 GHz, on the left
side for negative delays displaying beats after
almost 2.4 µs, on the right side directly after
zero delay. From such measurement the beat
period can be interpolated over the full time
interval, and according to Fourier’s theorem the
ground state splitting can be determined within
100 kHz.
Observation of 500 GHz Quantum Beats
A coherent superposition of the 3p sodium fine-structure states with a wavelength splitting of
0.6 nm or a frequency difference of 517 GHz requires simultaneous excitation of the D
1
and D
2
resonance lines at 589 nm with subpicosecond pulses.
A synchronously pumped mode-locked dye-
laser with saturable absorber in the dye gene-
rates pulses of 400 femtoseconds duration at a
repetition rate of 84 MHz. Together with a pola-
rization selective detection scheme well resolv-
ed fine-structure quantum beats in forward
scattering with an oscillation period of 1.9 ps
can be measured, demonstrating the ultrahigh
time resolution of this experimental set-up.
Doctoral Theses
H. Harde
Cascade-Free Lifetime Measurements with Fast Ion Beams after Combined Gas-Laser-Excitation
- Development of a Set-Up and First Measurements with Ba+, Na, Ne und Li+
Physics Department, University of Kaiserslautern 1974
H. Burggraf
Hochauflösende Spektroskopie mit ultrakurzen Laserpulsen am Natrium
School of Electrical Engineering, Helmut-Schmidt-Uiversity, Hamburg 1985
H. Lehmitz
Kohärenzspektroskopie mit ultrakurzen Lichtimpulsen – Zeit- und frequenzaufgelöste Messungen am Beispiel von
Cäsium sowie Voruntersuchungen zu Messungen an gespeicherten Ytterbiumionen
School of Electrical Engineering, Helmut-Schmidt-Uiversity, Hamburg 1989
Refereed Publications in Journals and Conference Digests
H. Harde, G. Guthöhrlein
New Method for Cascade-Free Lifetime Measurements
Physical Review A 10, 1488 (1974)
H. Harde
Intracavity Dye-Laser Excitation of Fast Ions and Atoms
Summaries of the Sixth Conference of the ''European Group of Atomic Spectroscopy'', European Physical Society,
Berlin, p. 65 (1974)
H. Harde
Cascade-Free Lifetime Measurements by Laser Excitation of Foil- or Gas-Excited Beams
in ''Beam-Foil Spectroscopy 2'', ed. by J. A. Sellin and D. J. Pegg (Plenum Press, New York 1976), p. 859 (1976)
D. Schulze-Hagenest, H. Harde, W. Brand, W. Demtröder
Fast-Beam Spectroscopy by Combined Gas-Cell-Laser Excitation for Cascade-Free Lifetime Measurements of
Highly Excited States
Zeitschrift für Physik A 282, 149 (1977)
H. Harde, H. Burggraf, J. Mlynek, W. Lange
Time-Resolved Polarization Spectroscopy of Coherent Transients: Picosecond Studies with a Mode-Locked Dye
Laser
Technical Digest of Topical Meeting of Picosecond Phenomena (Optical Society of America, Washington DC,
1980), post-deadline paper, p. THB16 (1980)
H. Harde, H. Burggraf, J. Mlynek, W. Lange
Hyperfine Quantum Beats in Transmission: Subnanosecond Studies by Means of a Mode-Locked Dye Laser
Europhysics Conference Abstracts of 12th EGAS-Conference 4 E (European Physical Society, Pisa, 1980),
p. 71 (1980)
H. Harde, H. Burggraf, J. Mlynek, W. Lange
Quantum Beats in Forward Scattering: Subnanosecond Studies with a Mode-Locked Dye Laser
Optics Letters 6, 290 (1981)
H. Harde
Time-Resolved Coherence Spectroscopy in Rb Vapor
Conference Abstracts of Ninth International Conference on Atomic Physics, ed. by R. S. Van Dyck Jr. and
E. N. Fortson (University of Washington, Seattle, 1984), p. B 48 (1984)
H. Lehmitz, H. Harde
Polarization Selective Detection of Hyperfine Quantum Beats in Cs
in ''Methods of Laser Spectroscopy'', ed. by Y. Prior et al., Plenum Press, New York, p. 101 (1986)
H. Burggraf, M. Kuckartz, H. Harde
Observation of 517 GHz Fine Structure Quantum Beats in Na
in ''Methods of Laser Spectroscopy'', ed. by Y. Prior et al., Plenum Press, New York, p. 105 (1986)
H.Lehmitz, H. Harde
Measurement of First-Order Free-Induction-Decay in Cs
in ''Methods of Laser Spectroscopy'', ed. by Y. Prior et al., Plenum Press, New York, p. 109 (1986)
H. Burggraf, M. Kuckartz, H. Harde
Measurement of 1.9 ps Fine Structure Quantum Beats in Na
Technical Digest of International Quantum Electronics Conference (Optical Society of America, Washington, D.C.,
1986), p. 200 (1986)
Contributions on National Conferences and Meetings
H. Burggraf, H. Harde
Zeitaufgelöste Polarisationsspektroskopie mit Pikosekunden Laserimpulsen
Frühjahrstagung der Deutschen Physikalischen Gesellschaft, Sektion Quantenoptik, Münster, 12. März 1981,
Verhandl. DPG (VI) 16, 418 (1981)
H. Lehmitz, H. Hoidis, H. Harde
Quantunm Beats in Vorwärtsstreuung am Cs mit ps-Zeitauflösung
Frühjahrstagung der Deutschen Physikalischen Gesellschaft, Sektion Quantenoptik, Bayreuth, 27. März 1985,
Verhandl. DPG (VI) 20, 1054 (1985)
M. Kuckartz, H. Harde
Beobachtung von 517 GHz Quantum Beats in Na
Frühjahrstagung der Deutschen Physikalischen Gesellschaft, Sektion Quantenoptik, Heidelberg, 17. März 1986,
Verhandl. DPG (VI) 21, 728 (1986)
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