Susanne Fechner’s research while affiliated with University of Wuerzburg and other places

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Publications (9)


Molecular quantum control landscapes in von Neumann time-frequency phase space
  • Article

October 2010

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20 Reads

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19 Citations

Stefan Ruetzel

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Susanne Fechner

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[...]

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David J Tannor

Recently we introduced the von Neumann representation as a joint time-frequency description for femtosecond laser pulses and suggested its use as a basis for pulse shaping experiments. Here we use the von Neumann basis to represent multidimensional molecular control landscapes, providing insight into the molecular dynamics. We present three kinds of time-frequency phase space scanning procedures based on the von Neumann formalism: variation of intensity, time-frequency phase space position, and/or the relative phase of single subpulses. The shaped pulses produced are characterized via Fourier-transform spectral interferometry. Quantum control is demonstrated on the laser dye IR140 elucidating a time-frequency pump-dump mechanism.


Accurate and efficient implementation of the von Neumann representation for laser pulses with discrete and finite spectra
  • Article
  • Publisher preview available

October 2009

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9 Reads

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19 Citations

We recently introduced the von Neumann picture, a joint time–frequency representation, for describing ultrashort laser pulses. The method exploits a discrete phase-space lattice of nonorthogonal Gaussians to represent the pulses; an arbitrary pulse shape can be represented on this lattice in a one-to-one manner. Although the representation was originally defined for signals with an infinite continuous spectrum, it can be adapted to signals with discrete and finite spectrum with great computational savings, provided that discretization and truncation effects are handled with care. In this paper, we present three methods that avoid loss of accuracy due to these effects. The approach has immediate application to the representation and manipulation of femtosecond laser pulses produced by a liquid-crystal mask with a discrete and finite number of pixels.

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Polarization-shaped femtosecond laser pulses in the ultraviolet

August 2009

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24 Reads

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25 Citations

Journal of Optics A Pure and Applied Optics

We present an experimental concept for the generation and characterization of polarization-shaped femtosecond laser pulses in the ultraviolet. Polarization-shaped laser pulses are frequency-doubled in an interferometrically stable setup comprising two perpendicularly oriented nonlinear crystals. Dual-channel spectral interferometry is employed to fully characterize the electric field of the polarization-shaped ultraviolet pulses. The method is experimentally demonstrated for a central wavelength of 400 nm. Advantages and prospective applications, as well as limitations and possible alternatives, are discussed.


Experimental implementation of ultrashort laser pulses in the von Neumann picture

December 2008

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3 Reads

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7 Citations

Applied Physics B

The characterization and interpretation of ultrashort laser pulses is most intuitive in the joint time–frequency domain, where structures like multiple pulses become immediately apparent. For practical reasons, ultrafast femtosecond laser pulse shaping, however, is commonly carried out in the frequency domain. Here we implement pulse shaping of optical fields defined in the von Neumann representation, which is a joint time–frequency distribution with complex-valued Gaussian basis functions. We discuss the feasibility as well as the principal limitations of this technique, show illustrative examples, and propose possible applications in coherent control.


Quantenkontrolle im Zeit-Frequenz-Phasenraum

August 2008

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54 Reads

Die in der vorliegenden Arbeit eingeführte von Neumann-Darstellung beschreibt jeden Laserpuls auf eineindeutige Weise als Summe von an verschiedenen Punkten des Zeit-Frequenz-Phasenraumes zentrierten, bandbreitebegrenzten Gaußimpulsen. Diese Laserpulse bilden sozusagen die „elementaren“ Bausteine, aus denen jeder beliebige Lichtimpuls konstruiert werden kann. Die von Neumann-Darstellung vereint eine Reihe von Eigenschaften, die sie für eine Anwendung auf dem Gebiet der Quantenkontrolle besonders geeignet erscheinen lässt. So ist sie eine bijektive Abbildung zwischen den Freiheitsgraden des verwendeten Impulsformers und der Phasenraumdarstellung der resultierenden, geformten Laserpulse. Jeder denkbaren Wahl von Impulsformerparametern entspricht genau eine von Neumann-Darstellung und umgekehrt. Trotzdem ermöglicht sie, ebenso wie die Husimi- oder die Wigner-Darstellung, eine intuitive Interpretation der dargestellten Lichtimpulse, da deren zeitliche und spektrale Struktur sofort zu erkennen ist. The von Neumann-representation introduced in this thesis describes each laser pulse in a one-to-one manner as a sum of bandwidth-limited, Gaussian laser pulses centered around different points in phase space. These pulses can be regarded as elementary building blocks from which every single laser pulse can be constructed. The von Neumann-representation combines different useful properties for applications in quantum control. First, it is a one-to-one map between the degrees of freedom of the pulse shaper and the phase-space representation of the corresponding shaped laser pulse. In other words: Every possible choice of pulse shaper parameters corresponds to exactly one von Neumann-representation and vice versa. Moreover, since temporal and spectral structures become immediately seizable, the von Neumann-representation, as well as the Husimi- or the Wigner-representations, allows for an intuitive interpretation of the represented laser pulse.


(a) Setup for the generation and characterization of polarization-shaped UV pulses. The polarization-shaped NIR pulse is frequency doubled in two BBO crystals and combined with the frequency-doubled reference pulse. The beam is then decomposed into two orthogonal polarization components that are separately analyzed with a spectrometer. The reference pulse passes over a delay stage to adjust the temporal delay between shaped pulse and reference pulse. The reference pulse is characterized in FROG and XFROG measurements. (b) Sketch illustrating frequency doubling of polarization-shaped NIR pulses (propagating along the k direction): one component of the fundamental is doubled in the first, the other component in the second crystal (optical axis indicated by arrow a).
Polarization-shaped UV double pulse: (a) spectral and (b) temporal intensity, (c) quasi-3D plot.
Polarization-shaped UV pulse train: (a) spectral and (b) temporal intensity, (c) quasi-3D plot.
Generation of polarization-shaped ultraviolet femtosecond pulses

April 2008

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29 Reads

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40 Citations

We experimentally demonstrate the generation and characterization of polarization-shaped femtosecond laser pulses in the ultraviolet at a central wavelength of 400 nm . Near-infrared laser pulses are first polarization shaped and then frequency doubled in an interferometrically stable setup that employs two perpendicularly oriented nonlinear crystals. A new pulse shaper design involving volume phase holographic gratings reduces losses and hence leads to an increase in pulse energy.


Definition of the von Neumann parameters. A discrete signal in the frequency or in the time domain can be mapped one-to-one on the von Neumann joint time-frequency grid. This grid covers the complete spectral and temporal ranges, Ω and T, defined by the Fourier relation, but the spectral and temporal resolutions (δt and δω in time and frequency domain and Δt and Δω on the von Neumann grid) are different such that the total number of sample points, N, remains the same in all three cases. The FWHM of the Gaussian basis function of the von Neumann representation σ t and σ ω are illustrated with respect to the grid spacing by the circle.
Two examples of the von Neumann transformation. The first example is a chirped laser pulse with a quadratic spectral phase. Its spectral intensity (a) and phase (b) is sampled at 121 frequency points and shown as black lines. The second example is an ultrashort laser pulse with the first half of the spectrum shifted forward and the second half backward in time. The corresponding spectral intensity (d) and phase (e) are again plotted in black. These electric fields were transformed onto a von Neumann grid of 11 × 11 points and subsequently transformed back to the frequency domain. The von Neumann intensity of the chirped pulse (c) shows a characteristic shape and the von Neumann intensity of the double pulse (f) displays two subpulses of different central frequency. The reconstructed spectral intensity and phase is added in (a), (b), (c) and (d) as red circles. Apart from small discrepancies, the reconstruction quality is very good and the original signal is recovered.
Example for the reconstruction of von Neumann representations. A von Neumann representation was defined on a 11 × 11 von Neumann grid. It is shown on the left side in intensity (a) and phase (b). In order to test the quality of the von Neumann transformation it was transformed both to the frequency (c) and the time domain (d) representation using 121 sample points with red lines indicating the intensity and black dashed lines the corresponding phases. The von Neumann picture after transforming back from the spectral domain to the von Neumann grid is displayed as intensity (e) and phase (f). Since the phase for positions with negligible intensity has no meaning, we used “phase blanking” for simplification of the plot, i.e. setting all those von Neumann phase values to zero for which the corresponding intensities are less than 5% of the maximal intensity. The agreement between the original and the reconstructed von Neumann representation is excellent.
The relation between the von Neumann phase and the phase of the electric field. A double pulse in the von Neumann plane is shown in intensity (a) and phase (b). The two parts of the double pulse have the same von Neumann intensity, which leads to equally intense pulses in the frequency and time domains. The von Neumann phase at these points is set to 0.75 π rad at ω 1 = 2.33 fs⁻¹and to -0.25 π rad at ω 2 =2.38 fs⁻¹. The corresponding signal in frequency domain (c) is represented as intensity (red line) and phase (black dashed line). The arrows connecting (b) and (c) show that the signal phase is identical with the von Neumann phase at positions ω 1 and ω 2.
Shaped ultrashort laser pulse in different representations. This example is based on a Gaussian spectrum and piecewise linear spectral phase, creating “colored double pulses” with temporally shifted “red” and “blue” components. (a) Electric field (Fourier) representation in the frequency domain (upper panel) and in the time domain (lower panel) with intensity (red) and phase (dashed black). The two representations are equivalent and connected via Fourier transformation. (b) Real-valued and oscillating temporal electric field. (c) Wigner representation with positive and negative valued interference structures in the middle. (d) Non-negative Husimi representation obtained by smoothing the Wigner representation with a Gaussian. For these two jtf representations a resolution of 121 × 121 was applied in order to obtain time and frequency marginals with the same resolution as the electric field representations of 121 sample points. The von Neumann representation on a 11 × 11 grid with intensity (e) and phase (f) contains equal information as the other representations.
The von Neumann picture: a new representation for ultrashort laser pulses

November 2007

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36 Reads

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34 Citations

In recent years, the use of joint time-frequency representations to characterize and interpret shaped femtosecond laser pulses has proven to be very useful. However, the number of points in a joint time-frequency representation is daunting as compared with those in either the frequency or time representation. In this article we introduce the use of the von Neumann representation, in which a femtosecond pulse is represented on a discrete lattice of evenly spaced time-frequency points using a non-orthogonal Gaussian basis. We show that the information content in the von Neumann representation using a lattice of N points in time and √N points in frequency is exactly the same as in a frequency (or time) array of N points. Explicit formulas are given for the forward and reverse transformation between an N-point frequency signal and the von Neumann representation. We provide numerical examples of the forward and reverse transformation between the two representations for a variety of different pulse shapes; in all cases the original pulse is reconstructed with excellent precision. The von Neumann representation has the interpretational advantages of the Husimi representation but requires a bare minimum number of points and is stably and conveniently inverted; moreover, it avoids the periodic boundary conditions of the Fourier representation.


Generation of shaped ultraviolet pulses at the third harmonic of titanium-sapphire femtosecond laser radiation

July 2007

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46 Reads

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43 Citations

Applied Physics B

We experimentally demonstrate a method to generate shaped femtosecond laser pulses in the ultraviolet at a central wavelength of 267nm, the third harmonic of conventional titanium-sapphire femtosecond laser systems. Employing a 128-pixel liquid-crystal spatial light modulator, we impose variable spectral phase modulations upon the near-infrared laser pulses. By this, complex laser pulses can be shaped whose overall spectrum is still conserved. Our experiments show that it is possible to easily transfer these pulses into the ultraviolet at 267nm via sum-frequency mixing in nonlinear crystals and to predictably generate multistructured ultraviolet femtosecond laser pulses. We analyze the temporal and spectral composition of these pulses after frequency conversion into the ultraviolet using difference-frequency cross-correlation and XFROG (cross-correlation frequency-resolved optical gating) techniques with an unmodulated fundamental laser pulse. The method can be employed to facilitate adaptive quantum control experiments in the ultraviolet wavelength regime, where the major absorption bands of many organic molecular systems are located.


Generation of femtosecond pulse sequences in the ultraviolet by spectral phase modulation

April 2006

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16 Reads

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4 Citations

Proceedings of SPIE - The International Society for Optical Engineering

We employ a 128-pixel liquid-crystal spatial light modulator to generate variable pulse sequences from a titanium-sapphire femtosecond laser amplifier system centered at 800 nm. By applying phase modulations based on triangular-shaped spectral phase patterns, pulse sequences can be generated whose overall spectrum is still conserved but whose subpulses differ in their spectral composition. We further use nonlinear crystals to analyze the shape of these pulses after frequency conversion. Our experiments show that it is possible to transfer these pulse sequences into the ultraviolet at central wavelengths of 400 nm and 267 nm without losing the ability to spectrally distinguish between the femtosecond subpulses. This is affirmed by measurements using cross-correlation and XFROG (cross-correlation frequency resolved optical gating) techniques with an unmodulated laser pulse. Simulations of the experiments are performed for comparison. We also discuss promising applications in spectroscopy or information encoding.

Citations (7)


... The vN representation is employed in quantum chemistry for the calculation of wavefunctions [237], energy levels [238], and quantum dynamics [231,[239][240][241][242][243]. Furthermore, it was shown to lead to a compact representation of ultrashort laser pulses [244][245][246] including their polarization state [247] and a reduced parameter space for quantum-control experiments [248,249]. A recent paradigm shift [231,239] makes the vN basis a promising transform domain for signal compression [250] and thus for application in compressed-sensing reconstruction algorithms. ...

Reference:

Coherent Multidimensional Spectroscopy in Molecular Beams and Liquids Using Incoherent Observables
Accurate and efficient implementation of the von Neumann representation for laser pulses with discrete and finite spectra

... Ultraviolet laser pulses can be shaped using acousto-optic modulators [52]. Shaped pulses in the near-infrared can also be converted to the ultraviolet using frequency doubling or other frequency conversion methods [53,54]. However, special care must be taken because the conversion efficiency will be strongly affected by the spectral phase. ...

Polarization-shaped femtosecond laser pulses in the ultraviolet
  • Citing Article
  • August 2009

Journal of Optics A Pure and Applied Optics

... Thanks to the developments in laser and optics technology, especially in higher harmonic generation techniques, [13][14][15] frequency-tripled ultrashort pulsed laser systems are available to emit femtosecond pulses in the ultraviolet (UV) spectral region with a high pulse energy and average power, while exhibiting high beam quality. De Michele et al. 16 compared the waveguide inscriptions on silica glass generated by 1030 and 343 nm femtosecond lasers. ...

Generation of shaped ultraviolet pulses at the third harmonic of titanium-sapphire femtosecond laser radiation
  • Citing Article
  • July 2007

Applied Physics B

... The vN representation is employed in quantum chemistry for the calculation of wavefunctions [237], energy levels [238], and quantum dynamics [231,[239][240][241][242][243]. Furthermore, it was shown to lead to a compact representation of ultrashort laser pulses [244][245][246] including their polarization state [247] and a reduced parameter space for quantum-control experiments [248,249]. A recent paradigm shift [231,239] makes the vN basis a promising transform domain for signal compression [250] and thus for application in compressed-sensing reconstruction algorithms. ...

Experimental implementation of ultrashort laser pulses in the von Neumann picture
  • Citing Article
  • December 2008

Applied Physics B

... Quantum control landscapes have found a variety of applications in physics and chemistry. They were exploited to manipulate the intensity of the Autler-Townes components in the photoelectron spectrum [6], making an experimental implementation for retinal photoisomerization in bacteriorhodopsin [7], manipulating molecular systems [8], inducing multiphoton excitations in atoms and vibrational population transfer in molecules [9], discovering the failure of greedy algorithms to generate fast quantum gates [10], experimentally observing saddle points [11] and analyzing quantum state preparation and entanglement creation [12] in two-spin quantum systems, dressing chopped-random-basis optimization [13], discovering a discontinuous phase transition with broken symmetry in a two-qubit quantum system [14], etc. ...

Molecular quantum control landscapes in von Neumann time-frequency phase space
  • Citing Article
  • October 2010

... Essentially, the Husimi Q representation is a continuous version of the "pixelated" von Neumann representation [18,53], which we have previously used in similar studies [25]. Here, the width parameter α is set to 1/2, resulting in the same widths in x and p. ...

The von Neumann picture: a new representation for ultrashort laser pulses

... The tutorial does not discuss the generation and manipulation of nonstationary waves, apart from a superficial level. Additionally, many topics were excluded, such as the connection between coherence and polarization [117][118][119][120][121][122][123], time dependent polarization modulation [124][125][126][127], geometric phase [127][128][129][130][131][132], correlation induced effects [42,[133][134][135][136][137][138][139], and interaction between nonstationary fields and matter [140][141][142][143][144], just to name a few. ...

Generation of polarization-shaped ultraviolet femtosecond pulses