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Advances in Ab Initio Computations of Atomic Nuclei


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Ab initio computations based on effective field theories of quantum chromodynamics can now routinely predict and describe properties of medium-heavy nuclei, even reaching the heavy nucleus 208Pb. These computations leverage insights from nuclear structure physics and many-body methods to overcome the exponential complexity of the nuclear many-body problem.
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The content discusses the progress in ab initio computations of atomic nuclei, which are based on Hamiltonians derived from effective field theories of quantum chromodynamics (QCD). These computations have advanced from light nuclei to medium-mass and even heavy nuclei like 208Pb.

The key ideas and concepts behind these computations are presented:

  • The definition of "ab initio" in the context of nuclear physics, balancing resolution and predictive power
  • The construction of nuclear Hamiltonians from chiral effective field theory, including the role of spontaneous chiral symmetry breaking
  • The importance of the mean field in organizing and including correlations, and the advantages of breaking symmetries
  • The inclusion of short-range and long-range correlations using methods like coupled-cluster theory
  • The computation of excited states, including simple particle-hole excitations and collective rotational bands
  • Highlights of results, such as neutron skins, quenching of beta decays, and matrix elements for neutrinoless double-beta decay

The content emphasizes that these ab initio computations build on the insights and phenomenology gained from simpler nuclear models, rather than being a purely reductionist approach starting from QCD. The exponential complexity of the nuclear many-body problem is overcome by leveraging these insights and using systematically improvable approximations.

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"Computing nuclei from Hamiltonians is not exponentially hard, because the low-energy structure of many nuclei is simple enough that it can be computed sufficiently accurately and in a controlled fashion using methods that scale affordably." "The effort for the exact methods increases exponentially with increasing mass number and – meeting exponentially increasing computer power due to Moore's law – have approximately advanced linearly in mass number as time has progressed." "The approximate methods exhibit a cost that increases polynomially with increasing system size."
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"Computing nuclei from Hamiltonians is not exponentially hard, because the low-energy structure of many nuclei is simple enough that it can be computed sufficiently accurately and in a controlled fashion using methods that scale affordably." "Heuristics enter almost everywhere in heavy nuclei because the states one is interested in are – strictly speaking – metastable." "Spontaneous symmetry breaking has impactful consequences: Nambu-Goldstone bosons are the low-lying excitations in such systems."

Belangrijkste Inzichten Gedestilleerd Uit

by T. Papenbroc... om arxiv.org 10-02-2024

https://arxiv.org/pdf/2410.00843.pdf
Ab initio computations of atomic nuclei

Diepere vragen

How can the insights from nuclear structure phenomenology and collective models be further leveraged to improve the efficiency and accuracy of ab initio nuclear computations?

The insights from nuclear structure phenomenology and collective models can significantly enhance the efficiency and accuracy of ab initio nuclear computations in several ways. First, by integrating established phenomenological models, such as the shell model and collective models, researchers can identify effective degrees of freedom that simplify the many-body problem. For instance, the concept of nuclear deformation and the associated collective excitations can guide the selection of relevant single-particle states in the mean-field approximation, thereby reducing the computational complexity. Moreover, the use of effective interactions derived from phenomenological models can provide a more accurate starting point for ab initio calculations. By employing effective field theories that incorporate known nuclear phenomena, such as pairing correlations and collective motion, one can construct Hamiltonians that better reflect the underlying physics. This approach allows for a more systematic inclusion of correlations, which are crucial for accurately describing nuclear properties. Additionally, leveraging insights from collective models can inform the choice of basis states in ab initio computations. For example, using deformed bases that account for quadrupole and octupole deformations can lead to improved representations of nuclear states, particularly in heavier nuclei where such effects are pronounced. This can enhance the predictive power of calculations, especially for observables sensitive to nuclear shape and structure. Finally, the integration of machine learning techniques with phenomenological insights can further optimize the computational process. By training models on existing nuclear data, one can develop predictive algorithms that streamline the selection of parameters and interactions in ab initio computations, ultimately leading to faster and more accurate results.

What are the fundamental limitations of the ab initio approach, and how can they be overcome through new theoretical developments or computational advances?

The fundamental limitations of the ab initio approach primarily stem from the exponential growth of computational resources required as the mass number increases. As the complexity of the nuclear many-body problem escalates, exact methods become impractical for medium to heavy nuclei. This is compounded by the challenge of accurately modeling short-range correlations and the need for effective Hamiltonians that capture the nuances of nuclear interactions. To overcome these limitations, several theoretical developments and computational advances can be pursued. One promising avenue is the refinement of effective field theories, particularly chiral effective field theory, to include higher-order interactions and three-body forces more systematically. By improving the accuracy of the effective Hamiltonians, one can reduce the reliance on exact computations and enhance the predictive capabilities of approximate methods. Another approach involves the development of new computational techniques that exploit parallel processing and advanced algorithms. For instance, the use of tensor network methods and quantum computing could revolutionize the way ab initio calculations are performed, allowing for the efficient handling of large Hilbert spaces and complex interactions. These methods can potentially mitigate the exponential scaling of traditional approaches. Furthermore, the integration of renormalization group techniques can help in deriving softer interactions that are more amenable to many-body computations. By systematically reducing the cutoff in interactions, one can simplify the problem while retaining essential physical features, thus making ab initio calculations more tractable. Lastly, fostering interdisciplinary collaboration between nuclear physicists, computational scientists, and mathematicians can lead to innovative solutions that address the limitations of the ab initio approach. By combining expertise from various fields, new methodologies can emerge that enhance both the theoretical framework and computational efficiency of nuclear structure calculations.

Given the importance of the mean field in organizing correlations, how can the mean-field description be systematically improved beyond the Hartree-Fock level to capture more complex nuclear phenomena?

To systematically improve the mean-field description beyond the Hartree-Fock level, several strategies can be employed that focus on incorporating correlations and collective effects more effectively. One key approach is to extend the Hartree-Fock framework to include beyond-mean-field effects, such as pairing correlations and collective excitations. This can be achieved through methods like Hartree-Fock-Bogoliubov (HFB) theory, which incorporates pairing interactions explicitly, allowing for a more accurate description of nuclei, especially those near the drip lines where pairing effects are significant. Another avenue is the use of configuration interaction (CI) methods that build on the mean-field state by including excitations to higher single-particle states. By systematically including particle-hole excitations, one can capture the essential correlations that arise from the interactions between nucleons. This can be done through techniques such as the coupled-cluster method, which provides a powerful framework for including correlations in a controlled manner. Additionally, the implementation of symmetry restoration techniques can enhance the mean-field description. Since mean-field states often break symmetries, restoring these symmetries through projection methods can lead to a more accurate representation of the nuclear wave function. For instance, angular momentum projection can be applied to deformed mean-field states to account for rotational bands, thereby improving the description of excited states. Moreover, the use of advanced computational techniques, such as the no-core shell model or lattice effective field theory, can provide alternative frameworks for improving the mean-field description. These methods allow for a more flexible treatment of the nuclear many-body problem, enabling the exploration of different configurations and interactions that go beyond the traditional mean-field approach. Finally, integrating insights from nuclear structure phenomenology, such as collective motion and cluster formation, can inform the development of effective interactions that better capture the underlying physics. By incorporating these phenomenological insights into the mean-field framework, one can enhance the accuracy and predictive power of ab initio computations, ultimately leading to a more comprehensive understanding of complex nuclear phenomena.
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