Letter Optics Letters 1 Two-dimensional electronic spectroscopy of an ultracold gas

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Letter Optics Letters 1
Two-dimensional electronic spectroscopy of an
ultracold gas
FRIEDEMANN LANDMESSER1, TOBIAS SIXT1, KATRIN DULITZ1,2,*, LUKAS BRUDER1,*,AND FRANK
STIENKEMEIER1
1Institute of Physics, University of Freiburg, Hermann-Herder-Straße 3, 79104 Freiburg, Germany
2Institut für Ionenphysik und Angewandte Physik, Universität Innsbruck, 6020 Innsbruck, Austria
*Corresponding authors: katrin.erath-dulitz@uibk.ac.at, lukas.bruder@physik.uni-freiburg.de
Compiled January 13, 2023
Femtosecond coherent multidimensional spectroscopy is
demonstrated for an ultracold gas. For this, a setup
for phase modulation spectroscopy is used to probe the
32S1/222P1/2,3/2transition in an 800 µK-cold sample of
7Li atoms confined in a magneto-optical trap. The obser-
vation of a double quantum coherence response, a signa-
ture of interparticle interactions, paves the way for detailed
investigations of few- and many-body effects in ultracold
atomic and molecular gases using this technique. The ex-
periment combines a frequency resolution of 3 GHz with a
potential time resolution of 200 fs, which allows for high-
resolution studies of ultracold atoms and molecules both in
the frequency and in the time domain. ©
2023 Optica Publishing
Group
http://dx.doi.org/10.1364/ao.XX.XXXXXX
Ultracold atoms and molecules offer numerous exciting research
prospects in physics and chemistry, including the modelling of con-
densed matter systems [
1
], precision measurements of fundamental
physics [
2
], as well as the study of atomic and molecular interactions
and dynamics in a regime dominated by quantum effects [
3
,
4
]. The
presence of external fields may even be used to tune the interparticle
interaction strength [5].
The photoexcitation and photoionization of ultracold atoms pro-
vides access to research fields including ultracold Rydberg gases [
6
]
and ultracold plasmas [
7
]. Such experiments are rarely done using
femtosecond (fs) lasers, although they deliver coherent, intense laser
fields and provide access to the real-time dynamics of the excited sys-
tem. The direct observation of electronic dephasing in an ultracold
Rydberg gas, induced by an ultrashort laser pulse, provides a promi-
nent recent example for the capabilities of fs lasers in the study of
many-body effects [
8
]. Other recent work on the fs laser excitation
of a Bose-Einstein condensate to an ultracold microplasma has also
allowed for the monitoring of ultrafast electron cooling [9].
In general, these studies can strongly benefit from spectroscopic
techniques with both high frequency and time resolution as provided by
two-dimensional electronic spectroscopy (2DES) in the fs regime [
10
].
Here, the time evolution of electronic coherences is tracked interfero-
metrically with fs pulses. The Fourier spectrum of this signal directly
relates to the absorption/emission spectrum of the sample. Further,
2DES can be combined with the phase modulation (PM) technique [
11
]
enabling coherent pathway selectivity of incoherent observables. The
high sensitivity of this approach is beneficial for systems with low target
densities which has recently enabled 2DES studies of cold molecular
targets [
12
,
13
]. Moreover, most 2DES methods track the evolution
of single-quantum coherences (1QCs), that are electronic coherences
induced by one-photon transitions. The PM technique enables in addi-
tion the tracking of higher-order quantum coherences. Such
n
-quantum
coherence (nQC) signals provide information about multiphoton tran-
sitions and higher lying states, e.g. multi-excitonic states [
14
]. This
property has been used to gain access to interparticle interactions in
thermal atomic vapors, where cooperative effects are otherwise covered
by inhomogeneous broadenings [1519].
Since ultracold atomic and molecular ensembles with their well-
defined structural properties in the quantum regime are ideal testbeds
for few- and many-body effects, the combination of ultracold quan-
tum gases with coherent spectroscopy techniques, and their inherent
selectivity to weak interparticle couplings, opens up new prospects
for detailed studies of such phenomena. Here, we demonstrate the
application of 1QC and 2QC 2DES to an ensemble of ultracold atoms
in a magneto-optical trap (MOT). We choose
7
Li as a test system, since
the interaction of fs radiation with ultracold colliding pairs of Li atoms
in a MOT has already been studied in detail [
20
], so that the underlying
mechanisms are tangible.
In the experiment, the
7
Li atoms are cooled and trapped via the
22P3/222S1/2
transition (details below). The trapped atoms interact
with a sequence of four fs laser pulses resonantly driving the
32S1/2
22P3/2
transition. The interaction with the intense fs laser pulses leads
to a multitude of linear and nonlinear signals, of which a specific subset
(described in Fig. 1(A)) is selected and detected in the experiment.
Light-matter interactions with single-atom states and collective two-
atom states (excitonic states) are possible. For a more convenient
description, we assign the states as follows:
22S1/2
state as
|2Si
,
22P1/2,3/2
state as
|2Pi
and
32S1/2
state as
|3Si
. The two-atom states
denoted as
|0i−|2i
correspond to both atoms in the
|2Pi
state, one
atom promoted to the
|3Si
and both atoms promoted to the
|3Si
state,
respectively.
In the 1QC 2DES measurement (Fig. 1(A)), pulses 1 and 3 induce a
coherence between the
|2Pi
and
|3Si
state, while pulses 2 and 4 project
the coherence onto the excited/ground state manifold. Accordingly, the
time evolution of the electronic coherences is probed during the time
intervals
t21
and
t43
, while the system evolves on the excited/ground
arXiv:2210.03023v2 [physics.atom-ph] 12 Jan 2023
摘要:

LetterOpticsLetters1Two-dimensionalelectronicspectroscopyofanultracoldgasFRIEDEMANNLANDMESSER1,TOBIASSIXT1,KATRINDULITZ1,2,*,LUKASBRUDER1,*,ANDFRANKSTIENKEMEIER11InstituteofPhysics,UniversityofFreiburg,Hermann-Herder-Straße3,79104Freiburg,Germany2InstitutfürIonenphysikundAngewandtePhysik,Universität...

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