Daniel M. Reich’s research while affiliated with Freie Universität Berlin and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (59)


FIG. 1. Isosurfaces with values −0.22 (blue) and 0.22 (orange) for chiral potentials according to Eq. (2) with optimized coefficients c lm for angular expansions up to L = 2-5 and g = 0.747. The value of the chirality measure according to Eq. (3) is indicated below each potential.
Tracking chirality in photoelectron circular dichroism
  • Article
  • Full-text available

February 2025

·

21 Reads

·

2 Citations

Physical Review Research

Marec W. Heger

·

Daniel M. Reich

In photoelectron circular dichroism (PECD) it is generally difficult to trace how and when the chirality of the molecule is imprinted onto the photoelectron. We present simulations of PECD in a simple model and employ chirality measures to establish a quantitative connection between the chirality of the potential, the electronic wave function's chirality, and the anisotropy of the photoelectron distribution. We show that these measures are suitable indicators for chirality, paving the way for tracking the chiral evolution from the nuclear scaffold to the final observable. Published by the American Physical Society 2025

Download

Anisotropy Factor Spectra for Weakly Allowed Electronic Transitions in Chiral Ketones

February 2025

·

23 Reads

·

·

Tom Ring

·

[...]

·

Daniel M. Reich

Quantum chemical calculations of one‐photon absorption, electronic circular dichroism and anisotropy factor spectra for the A‐band transition of fenchone, camphor and 3‐methylcyclopentanone (3MCP) are reported. While the only weakly allowed nature of the transition leads to comparatively large anisotropies, a proper theoretical description of the absorption for such a transition requires to account for non‐Condon effects. We present experimental data for the anisotropy of 3MCP in the liquid phase and show that corresponding Herzberg–Teller corrections are critical to reproduce the main experimental features. The results obtained with our comprehensive theoretical model highlight the importance of the vibrational degree of freedom, paving the way for a deeper understanding of the dynamics in electronic circular dichroism.


(a) Excitation diagram for 2 + 1 REMPI featuring a two-photon ionization (photon energy 0.58 eV) from the molecular ground state of camphor to an intermediate state. Population in the intermediate state is ionized by a third photon into the continuum. (b) Illustration of photoelectron circular dichroism for camphor. The interaction of chiral molecules with circularly polarized light results in a forward–backwards asymmetry in the photoelectron angular distribution indicated by the blue shaded area.
Relative quadrature error of PECD calculated with Eq. (8) as resulting from the 2 + 1 REMPI process shown in Fig. 1(a) applied to randomly oriented molecules. We calculate PADs at 0.58 eV photoelectron energy, averaged over the Euler angles β and γ for α = 0. The error is shown for the maximum PECD signal, corresponding to the forward direction (θk = 0). Methods are Lebedev–Laikov quadrature (L), spherical designs from Ref. 72 (D), equidistant step methods with the same sampling density for β and γ (T × T), and near-uniform spherical coverings by Fibonacci spheres (F). The arrows indicate the degree L for which the error of the Lebedev–Laikov method and the spherical designs reaches machine precision.
(a) Exciting and probing a chiral vibrational wavepacket in planar COFCl. A Raman excitation (magenta arrows) creates a superposition of the two lowest out-of-plane vibrational states of the central C-atom via an electronically excited state with vibrational level |v⟩, followed by one-photon ionization (blue) populating a vibrational level |v′⟩ in the parent ion’s ground state. (b) Visualization of the field configuration. Electric field coils generate the static field, orienting the molecules. Pump (magenta) and probe (blue) pulses are circularly polarized in a plane perpendicular to this field. (c) Rank profile of the Euler angle distribution P(ω) from Eq. (12) for different temperatures obtained with the Lebedev–Laikov method of degree L = 131 . The horizontal gray line indicates the value 10⁻⁶ used to determine the maximum rank of P(ω). (d) Relative quadrature error of PECD calculated with Eq. (8) for the process shown in (a) and (b) at 6 eV photoelectron energy. The orientation average is weighted with the Euler angle distribution from Eq. (12) at rotational temperature 5 K. The vertical gray lines indicate the number of sampling points needed to achieve degree L = 41 for a method with efficiency E = 1 and E = 2 / 3 . The inset displays a zoom of the same data, with the horizontal gray line highlighting a relative error of 1%. Methods are Lebedev–Laikov quadrature (L), the spherical designs from Ref. 72 (D), Gauss–Legendre product grids (GL × T), equidistant step methods with the same sampling density for β and γ (T × T), and near-uniform spherical coverings by Fibonacci spheres (F).
(a) Visualization of the fenchone molecule. The orange arrow indicates the electric dipole transition moment (scaled × 400), and the blue arrow indicates the magnetic dipole transition moment (scaled × 4). (b) Illustration of circular dichroism in fenchone. The system is treated via an effective two-level model corresponding to the electronic A band transition n → π*. The interaction of the chiral molecule with circular polarized (represented by helical arrows) light results in a difference in absorption. (c) Relative quadrature error of the anisotropy factor g calculated with Eq. (8). The inset displays a zoom for the region of relative quadrature errors around 0.1%. Methods are the composite trapezoid rule (T), Lebedev–Laikov quadrature (L), Gauss–Legendre quadrature (GL), and near-uniform SO(3) coverings (C) from Ref. 50, with a cross indicating product methods. The equidistant step method (T × T × T) uses the same number of points for all Euler angles.
Numerical evaluation of orientation averages and its application to molecular physics

October 2024

·

37 Reads

In molecular physics, it is often necessary to average over the orientation of molecules when calculating observables, in particular when modeling experiments in the liquid or gas phase. Evaluated in terms of Euler angles, this is closely related to integration over two- or three-dimensional unit spheres, a common problem discussed in numerical analysis. The computational cost of the integration depends significantly on the quadrature method, making the selection of an appropriate method crucial for the feasibility of simulations. After reviewing several classes of spherical quadrature methods in terms of their efficiency and error distribution, we derive guidelines for choosing the best quadrature method for orientation averages and illustrate these with three examples from chiral molecule physics. While Gauss quadratures allow for achieving numerically exact integration for a wide range of applications, other methods offer advantages in specific circumstances. Our guidelines can also be applied to higher-dimensional spherical domains and other geometries. We also present a Python package providing a flexible interface to a variety of quadrature methods.


Feshbach resonances in cold collisions as a benchmark for state of the art ab initio theory

August 2024

·

13 Reads

Quantum resonances in collisions and reactions are a sensitive probe of the intermolecular forces. They may dominate the final quantum state distribution, as recently observed for Feshbach resonances in a cold collision experiment (Science 380, 77 (2023)). This raises the question whether the sensitivity of such measurements is sufficient to assess the quality of theoretical models for the interaction. We here compare measured collision cross sections to those obtained with exact quantum coupled-channels scattering calculations for three different ab initio potential energy surfaces. We find that the ability to test the correct prediction of energy redistribution over molecular degrees of freedom is within reach, requiring only a modest improvement in energy resolution of current experiments. Such improvement will enable the separation of individual resonances and allow for an unambiguous experimental test of different theory approaches.


FIG. 1. (a) Excitation diagram for 2+1 REMPI featuring a two-photon ionization (photon energy 0.58 eV) from the molecular ground state of camphor to an intermediate state. Population in the intermediate state is ionized by a third photon into the continuum. (b) Illustration of photoelectron circular dichroism for camphor. The interaction of chiral molecules with circularly polarized light results in a forward-backwards asymmetry in the photoelectron angular distribution indicated by the blue shaded area.
FIG. 2. Relative quadrature error of PECD calculated with Eq. (8) as resulting from the 2+1 REMPI process shown in Fig. 1(a) applied to randomly oriented molecules. We calculate PADs at 0.58 eV photoelectron energy, averaged over the Euler angles β and γ for α = 0. The error is shown for the maximum PECD signal, corresponding to the forward direction (θ k = 0). Methods are Lebedev-Laikov quadrature (L), spherical designs from Ref. 69 (D), equidistant step methods with the same sampling density for β and γ (T×T) and near-uniform spherical coverings by Fibonacci spheres (F). The arrows indicate the degree L for which the error of the Lebedev-Laikov method and the spherical designs reaches machine precision.
FIG. 3. (a) Exciting and probing a chiral vibrational wavepacket in planar COFCl. A Raman excitation (magenta arrows) creates a superposition of the two lowest out-of-plane vibrational states of the central C-atom via an electronically excited state with vibrational level |v⟩, followed by one-photon ionization (blue) populating a vibrational level |v ′ ⟩ in the parent ion's ground state. (b) Visualization of the field configuration. Electric field coils generate the static field orienting the molecules. Pump (magenta) and probe (blue) pulses are circularly polarized in a plane perpendicular to this field. (c) Rank profile of the Euler angle distribution P (ω) from Eq. (12) for different temperatures obtained with the Lebedev-Laikov method of degree L = 131. The horizontal gray line indicates the value 10 −6 used to determine the maximum rank of P (ω). (d) Relative quadrature error of PECD calculated with Eq. (8) for the process shown in (a) and (b) at 6 eV photoelectron energy. The orientation average is weighted with the Euler angle distribution from Eq. (12) at rotational temperature 5 K. The vertical gray lines indicate the number of sampling points needed to achieve degree L = 41 for a method with efficiency E = 1 and E = 2/3. The inset displays a zoom of the same data, with the horizontal gray line highlighting a relative error of 1 %. Methods are Lebedev-Laikov quadrature (L), the spherical designs from Ref. 69 (D), Gauss-Legendre product grids (GL×T), equidistant step methods with the same sampling density for β and γ (T×T) and near-uniform spherical coverings by Fibonacci spheres (F).
FIG. 4. (a) Visualization of the fenchone molecule. The orange arrow indicates the electric dipole transition moment (scaled ×400) and the blue arrow indicates the magnetic dipole transition moment (scaled ×4). (b) Illustration of circular dichroism in fenchone. The system is treated via an effective two-level model corresponding to the electronic A band transition n → π * . The interaction of the chiral molecule with circular polarized (represented by helical arrows) light results in a difference in absorption. (c) Relative quadrature error of the anisotropy factor g calculated with Eq. (8). The inset displays a zoom for the region of relative quadrature errors around 0.1%. Methods are the composite trapezoid rule (T), Lebedev-Laikov quadrature (L), Gauss-Legendre quadrature (GL), and near-uniform SO(3) coverings (C) from Ref. 47, with a cross indicating product methods. The equidistant step method (T×T×T) uses the same number of points for all Euler angles.
Numerical evaluation of orientation averages and its application to molecular physics

July 2024

·

77 Reads

In molecular physics, it is often necessary to average over the orientation of molecules when calculating observables, in particular when modelling experiments in the liquid or gas phase. Evaluated in terms of Euler angles, this is closely related to integration over two- or three-dimensional unit spheres, a common problem discussed in numerical analysis. The computational cost of the integration depends significantly on the quadrature method, making the selection of an appropriate method crucial for the feasibility of simulations. After reviewing several classes of spherical quadrature methods in terms of their efficiency and error distribution, we derive guidelines for choosing the best quadrature method for orientation averages and illustrate these with three examples from chiral molecule physics. While Gauss quadratures allow for achieving numerically exact integration for a wide range of applications, other methods offer advantages in specific circumstances. Our guidelines can also by applied to higher-dimensional spherical domains and other geometries. We also present a Python package providing a flexible interface to a variety of quadrature methods.


FIG. 1. Isosurfaces with values -0.3 (blue) and 0.3 (orange) for chiral potentials according to Eq. (2) with optimized coefficients c lm for angular expansions up to L = 2 − 5 and g = 1. The value of the chirality measure according to Eq. (3) is indicated below each potential.
Tracking Chirality in Photoelectron Circular Dichroism

May 2024

·

62 Reads

Photoelectron circular dichroism (PECD) originates from the interplay between a molecule's chiral nuclear scaffold and a circularly polarized ionizing laser field. It is one of the most sensitive characterization techniques for the chirality of molecules in the gas phase. However, due to the complexity of the observable, it is generally difficult to predict and track how and when the chirality of the molecule is imprinted onto the photoelectron. Here, we present simulations of PECD for single-photon ionization in a hydrogenic single-electron model with an artificial chiral potential. This framework allows us to systematically tune the system's chirality and characterize the emergence of PECD. To this end, we propose chirality measures for potentials and wave functions to establish a quantitative connection with the resulting anisotropy in the photelectron distribution. We show that these chirality measures are suitable indicators for chirality in our model, paving the way for tracking the evolution of chirality from the nuclear scaffold to the final observable.


Anisotropy factor spectra for weakly allowed electronic transitions in chiral ketones

May 2024

·

19 Reads

Quantum chemical calculations of one-photon absorption, electronic circular dichroism and anisotropy factor spectra for the A-band transition of fenchone, camphor and 3-methylcyclopentanone (3MCP) are reported. While the only weakly allowed nature of the transition leads to comparatively large anisotropies, a proper theoretical description of the absorption for such a transition requires to account for non-Condon effects. We present experimental data for the anisotropy of 3MCP in the liquid phase and show that corresponding Herzberg-Teller corrections are critical to reproduce the main experimental features. The results obtained with our comprehensive theoretical model highlight the importance of the vibrational degree of freedom, paving the way for a deeper understanding of the dynamics in electronic circular dichroism.


Figure 2: Flowchart for the pure-state controllability algorithm. The yellow rhomboids show the initial inputs necessary to define the circuit C P SC ( ⃗ ϑ).
Determining the ability for universal quantum computing: Testing controllability via dimensional expressivity

December 2023

·

28 Reads

·

1 Citation

Quantum

Operator controllability refers to the ability to implement an arbitrary unitary in SU(N) and is a prerequisite for universal quantum computing. Controllability tests can be used in the design of quantum devices to reduce the number of external controls. Their practical use is hampered, however, by the exponential scaling of their numerical effort with the number of qubits. Here, we devise a hybrid quantum-classical algorithm based on a parametrized quantum circuit. We show that controllability is linked to the number of independent parameters, which can be obtained by dimensional expressivity analysis. We exemplify the application of the algorithm to qubit arrays with nearest-neighbour couplings and local controls. Our work provides a systematic approach to the resource-efficient design of quantum chips.


FIG. 2. Spectra of the optimized pulses for optimization towards maximally entangled cat states with |α tgt | = 1 (top) and |α tgt | = 2 (bottom). The dashed lines indicate the transition frequencies between the eigenstates |n, ±± of the drift Hamiltonian, defined in Eq. (39).
FIG. 3. Detailed analysis of the optimized pulse towards |α tgt | = 2.0, showing the pulse in time domain (c), in frequency domain (a), and a time-frequency distribution (b) calculated via the Gabor transform. All quantities are expressed in units of the coupling strength g.
FIG. 4. The final value of |α| plotted against the pulse duration T for different optimizations. The different marker styles indicate optimizations performed with different target values |α tgt |. The dashed auxiliary lines on the right, colored with the same color as the marker styles, are added to guide the eye.
FIG. 8. Visualization of the strategy change, storing excitation in the qubit instead of the harmonic oscillator, when optimizing with strong dissipation. (a) The same plot as in Fig. 7(b). (b), (c) The dynamics of the qubit in Bloch sphere representation. For the sake of clarity, we only show the final part of the dynamics in (b) and (c), as indicated by the gray dashed lines in (a).
Optimizing for an arbitrary Schrödinger cat state

October 2023

·

36 Reads

·

5 Citations

Physical Review Research

We derive a set of functionals for optimization towards an arbitrary cat state and demonstrate their application by optimizing the dynamics of a Kerr-nonlinear Hamiltonian with two-photon driving. The versatility of our framework allows us to adapt our functional towards optimization of maximally entangled cat states, applying it to a Jaynes-Cummings model. We identify the strategy of the obtained control fields and determine the quantum speed limit as a function of the cat state's excitation. Finally, we extend our optimization functionals to open quantum system dynamics and apply it to the Jaynes-Cummings model with decay on the oscillator. For strong dissipation and large cat radii, we find a change in the control strategy compared to the case without dissipation. Our results highlight the power of optimal control with functionals specifically crafted for complex physical tasks and the versatility of the quantum optimal control toolbox for practical applications in the quantum technologies.


Fig. 1 Results for the optimisation of circular dichroism of a rotational ensemble for the A-band transition of fenchone. (a) Evolution of the excited-state population as a function of time for the R (green) and S (purple) enantiomer of fenchone, as well as the corresponding value of the anisotropy parameter g (yellow, in the right y axis). The dashed line corresponds to the circularly polarised guess pulse, while the solid line corresponds to the optimised control fields. The oscillations of g at short times are a numerical artifact due to the near 0 absorption of the excited states during the first femtoseconds. (b) Optimised pulses in time domain. (c) Optimised pulses in frequency domain.
Correction: Increasing ion yield circular dichroism in femtosecond photoionisation using optimal control theory

August 2023

·

28 Reads

·

2 Citations

Physical Chemistry Chemical Physics

Correction for 'Increasing ion yield circular dichroism in femtosecond photoionisation using optimal control theory' by Manel Mondelo-Martell et al., Phys. Chem. Chem. Phys., 2022, 24, 9286-9297, https://doi.org/10.1039/D1CP05239J.


Citations (35)


... For instance, several works suggest quantification of a degree of intrinsic chirality based only on geometrical properties, [31][32][33][34][35] or on properties of a molecular potential and density matrix. 36 The latter approach proposes a route to systematically tune an artificial chiral potential to maximize the respective PECD for randomly oriented molecules. ...

Reference:

Characterization of the photoelectron circular dichroism of fixed-in-space molecules through an asymmetry of the ionic potential
Tracking chirality in photoelectron circular dichroism

Physical Review Research

... A lot of effort was therefore put in the development of algorithms, in particular focusing on error mitigation, [3], [4], and expressivity analysis of quantum circuits, [5], [4], which recently led also to use the expressivity algorithm developed by us to a theoretical analysis of the controllability of quantum devices [6]. In addition, noise models, [7], [8], the role of noise in equivariant quantum neural networks, [9] and methods such as the Bayesian approach, [10], or classical splitting of quantum circuits, [11], were investigated for their use in practical quantum computing applications. ...

Determining the ability for universal quantum computing: Testing controllability via dimensional expressivity

Quantum

... Achieving high-fidelity quantum state preparation (QSP) under effective control is crucial for quantum computing and simulation [1,2]. This process often requires iterative solutions of a set of nonlinear equations [3,4], which is complex and time-consuming. Consequently, the quest for efficient methods to prepare arbitrary quantum states has become a prominent issue in quantum control. ...

Optimizing for an arbitrary Schrödinger cat state

Physical Review Research

... Anisotropy was enhanced via optimal control, leading to optimized driving fields with elliptical polarization and a DC component. 115 Since neither the molecule nor the pulse has symmetries, the CD depends on all three Euler angles. In contrast to the previous case studies, the light-molecule interaction is non-perturbative due to the high intensity of the light. ...

Correction: Increasing ion yield circular dichroism in femtosecond photoionisation using optimal control theory

Physical Chemistry Chemical Physics

... 19 The validity of the FCI level of theory for the He-H + 2 channel 20 was independently and successfully established from quantum wavepacket calculations to interpret Feshbach resonance measurements and final adjustment to experimental data through PES-morphing. [21][22][23] The present work uses and evaluates an accurate mixed kernel/neural network (NN) representation of a fully reactive PES for the [HHHe] + system 24 The initial state-selected T −dependent rate coefficients k v=0,j∈ [0,5] (T ) up to 1000 K are characterized from classical and quantum nuclear dynamics simulations using this KerNN PES and a recently corrected PES (cR-PES) 19 of the RFCI8 PES. 18 First, the potential energy surfaces are presented and validated, followed by the results on thermal rates and final state distributions. ...

Tomography of Feshbach resonance states
  • Citing Article
  • April 2023

Science

... Shaped laser pulses are also used in trapped ions and Rydberg atoms [6,7]. Many numerical methods have been proposed to design control pulses, such as Gradient Ascent Pulse Engineering (GRAPE), the Krotov method, the Chopped Random Basis (CRAB) method, etc [8][9][10][11]. These methods can leverage the system model to directly generate control pulses. ...

Krotov: A Python implementation of Krotov's method for quantum optimal control

SciPost Physics

... Recently, fenchone has become established as the prototypical molecule for the introduction and study of laser driven PECD phenomena, in particular those using resonance enhanced multiphoton ionization (REMPI-PECD). [13][14][15][16][17][18][19][20][21][22][23][24] Just as in single photon PECD phenomena, photoelectron angular distributions that are forward/backward asymmetric with respect to the propagation direction of a circularly polarized laser beam are observed. These arise from pure electric dipole interaction of the ionizing photon with the molecular target, resulting in very strong chiral asymmetry factors that may range up to several tens per cent. ...

Pulse length dependence of photoelectron circular dichroism

Physical Chemistry Chemical Physics

... [58,59] Moreover, the improved modeling of the vibronic transitions will be an important asset to lift studies on optimal control of circular dichroism from few-level systems closer to physical reality. [60] Finally, to understand the difference in anisotropy between absorption and ion yield we expect that further theoretical investigations in the role of higher-lying electronic excited states are required which will be subject to future work. Theoretical CD (upper plots) and ABS (lower plots) spectra of fenchone and camphor at room temperature comparing the results for FC and FCHT calculations with experimental spectra. ...

Increasing ion yield circular dichroism in femtosecond photoionisation using optimal control theory

Physical Chemistry Chemical Physics

... The interplay between the chirp and the vibrational structure can be an important resource for coherent control as has been evidenced for example in the photoassociation of Mg 2 dimers. [58,59] Moreover, the improved modeling of the vibronic transitions will be an important asset to lift studies on optimal control of circular dichroism from few-level systems closer to physical reality. [60] Finally, to understand the difference in anisotropy between absorption and ion yield we expect that further theoretical investigations in the role of higher-lying electronic excited states are required which will be subject to future work. ...

Coherent Control of Ultrafast Bond Making and Subsequent Molecular Dynamics: Demonstration of Final-State Branching Ratio Control

... Theory of optimal control of various quantum systems such as atoms, molecules, etc. forms an important research direction at the intersection of mathematics, physics, chemistry, and computer science. It exploits diverse mathematics tools [1][2][3][4][5][6][7][8][9] and has applications to controlled generation of quantum gates for closed [10,11] and open quantum systems [12,13], controlled transfer along a spin chain [14], nuclear magnetic resonance [2,15,16], etc. Quantum systems in applications are typically open, i.e. interacting with their environment (reservoir). ...

Corrigendum: Optimal control theory for a unitary operation under dissipative evolution (2014 New J. Phys. 16 055012)