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Book
Physique quantique et statistique
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ISBN: 9782500008069 Year: 2017 Publisher: Bruxelles Presses universitaires de Bruxelles

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Mécanique quantique II
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Year: 2017 Publisher: Bruxelles Presses universitaires de Bruxelles

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Dissertation
Study of one-neutron halo through (d, p) transfer reactions

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In modern nuclear physics, a special group of nuclei located close to the drip line named halo nuclei has received tremendous attention due to their unique cluster structure. These nuclei exhibit large matter radii and are qualitatively described as a compact core surrounded by a diffuse halo which is formed by the loosely-bound valence nucleon(s). Their existence breaks down the consistent predictions by the classical shell model and challenges nuclear-structure calculations. To understand this exotic feature from first principles, lots of efforts have been undertaken by nuclear physicists during the past decades. One of the most successful probes to look into these questions is the (d,p) transfer which has been proved to be a very powerful tool to extract single-particle properties of nuclei and hence is ideal to study one-neutron halo nuclei.The main topic of this work is to improve the reliability of the nuclear-structure observables extracted from transfer reactions. In one of our works [Phys. Rev. C 98, 054602 (2018)], the experiment done by Schmitt et al. on the $^{10}$Be(d,p)$^{11}$Be transfer reaction at four beam energies [Phys. Rev. Lett. 108, 192701 (2012)] is reanalyzed. In order to probe only the halo of the nucleus which is represented by the asymptotic normalization coefficient (ANC), the beam energy and angular ranges at which such reaction is strictly peripheral have to be determined. These peripheral conditions are systematically identified by coupling a Halo effective field theory (EFT) description of the $^{11}$Be nucleus at leading order (LO) with the adiabatic distorted wave approximation (ADWA) to model the transfer. The results suggest that focussing on the transfer data collected with low beam energies and at forward scattering angles ensures the peripherality of the reaction and hence is the best way to reliably extract the ANC. The resulting values of ANC are (0.785 ± 0.030) fm$^{-1/2}$ for the ground state and (0.135 ± 0.005) fm$^{-1/2}$ for the first excited state. These values are in excellent agreement with the values predicted by ab initio calculations (0.786 fm$^{-1/2}$ for the ground state and 0.129 fm$^{-1/2}$ for the excited state) [Phys. Rev. Lett. 117, 242501 (2016)]. An alternative way to explore the sensitivity of transfer calculations to the short-range physics of the $^{10}$Be-n wave function using Halo EFT is offered by the supersymmetry (SuSy) method. With this method, the SuSy partner of the original wave function can be generated which shares the same asymptotic behavior but exhibits a very different internal part. Feeding those wave functions into the transfer calculations, the results confirm the above findings with respect to the peripherality of the $^{10}$Be(d,p) transfer.This method has then been extended to study another one-neutron halo nucleus: $^{15}$C which is important in nuclear astrophysics. Its ANC is extracted from the cross sections of the $^{14}$C(d,p) transfer measured by Mukhamedzhanov et al. [Phys. Rev. C, 84, 024616 (2011)]. The values obtained are (1.26 ± 0.02) fm$^{-1/2}$ and (0.056 ± 0.001) fm$^{-1/2}$ for the ground state and first excited state of $^{15}$C, respectively. Especially for the ground state case, again, a perfect agreement is reached between our result and the one predicted by Navrátil et al. (C$_{1/2+}$ = 1.282 fm$^{-1/2}$) in an ab initio calculation. Relying on the inferred ANC value, it enables us to fit an effective $^{14}$C-n interaction at NLO in Halo EFT, which has been used later in other reaction calculations, such as Coulomb breakup and radiative capture [Phys. Rev. C 100, 044615 (2019)].We have also looked at the extension of this idea to resonant states. After an analogous analysis using a bin description, it is figured out that the resonant width plays a key role in determining the magnitude of the cross sections for such transfers. Its effect on resonance can be comparable to that of the ANC on bound states. But the associated uncertainty is larger than that in the case of bound state.In collaboration with Prof. Obertelli, we have studied the potential use of sub-Coulomb (d,p) transfer to investigate the possible presence of a halo structure in the excitation spectrum of medium to heavy nuclei. Based on the hypothetical case of $^{95}$Sr, the dependencies of the transfer calculation on several crucial parameters including Q-value, nuclear spin and beam energy have been tested to understand better how the halo feature could be revealed by measuring transfer cross sections. The feasibility of this idea requires an accurate theoretical prediction and sensitive detection systems.On the experimental side, efforts have been made to progress in the data analysis of the IS561A experiment on $^{9}$Li(d,p) transfer performed at HIE-ISOLDE, CERN. Thanks to the preprocessing of the acquired data done by Jesper Halkjær Jensen (Aarhus), the necessary information on the elastic scattering channel ($^{9}$Li + d) has been successfully collected and matches well with our theoretical calculation. Due to some practical problems happening during the measurement which would propagate to the analysis and result in a low statistics, the extraction of the (d,p) channel will require further detailed analyses. To make up for this, the available data measured by Jeppesen et al. [Phys. Lett. B, 642(5): 449 - 454, 2006] and Cavallaro et al. [Phys. Rev. Lett. 118, 012701 (2017)] are taken into account to check in those cases the validity of the chosen model which has already been used to study the resonance of $^{11}$Be. The outcome suggests that the method we use is a fast and efficient option to simulate the resonance during the transfer. For the non-resonant part, choosing the prior form of the transition matrix instead of the post one is better suited.

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Dissertation
uantum scattering in a one-dimensional (a)periodic environment: Towards a microscopic quantum-detector model

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At the end of the nineteenth century, many physicists were convinced that all fundamental laws in nature were known. With Newton's laws one could exactly describe and predict the movements of everyday objects, as well as of celestial bodies. Using Maxwell's laws one could understand the once mysterious phenomena of electricity and magnetism. Finally, the laws of thermodynamics allowed a description of heat transfer and related processes. Nothing seemed further from the truth after a spectacular series of discoveries, demonstrating the need for radical new ideas to understand nature. There was Röntgen in 1895 and Becquerel in 1896 who both discovered new kinds of radiation. Another year later Thomson discovered the first sub-atomic particle: the electron. It took multiple years in order to be able to understand these phenomena with the aid of a novel theory, quantum mechanics. Ever since, this theory has been successful in clarifying countless new phenomena occurring at the smallest possible length scales. In spite of these impressive achievements, it seems that quantum mechanics lacks the ability to give a complete description of nature. This is because the theory makes a fundamental distinction between the interaction of small particle, say an atom, with another atom; and the interaction between an atom and a measurement apparatus. Since the measurement apparatus is made up of nothing but atoms, so its interaction with an atom must consist of nothing but interactions between atoms. It is a logical inconsistency to make a fundamental distinction between these two types of interactions. Concretely, particles are described as wave-functions in quantum mechanics. These wave-functions evolve by means of the Schrödinger equation, which is completely deterministic law. In other words, it is possible to predict exactly the wave function at any other time. When one performs a measurement, it is assumed that the wave-function undergoes a destructive evolution which cannot be described by the Schrödinger equation. The only basis for this assumption is that it predicts the correct behavior of measurement results. Scientists who are only concerned with results of measurements are satisfied with this description. There exists, however, another group of scientists who are not prepared to make this assumption blindly. Ever since the conception of quantum mechanics, around 1925, there has been research on the interaction of a simple system and a complex system, consisting of many atoms such as a measurement apparatus. In this work a description of this interaction is attempted in the case of a drastically simplified model of a measurement apparatus, with the aid of computer calculations. The influence of the atoms of the measurement apparatus on the measurement result is studied. A certain difference between periodic placement of the atoms and aperiodic placement is observed. In order to know if the observed difference is significant enough to have an influence in a realistic apparatus model, more sophisticated computer calculations are needed.

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