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The Role of the Pauli Principle in Metastability Exchange Collisions M

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The Role of the Pauli Principle in Metastability Exchange Collisions M The role of the Pauli principle in metastability exchange collisions M. Pinard, F. Laloë To cite this version: M. Pinard, F. Laloë. The role of the Pauli principle in metastability exchange collisions. Journal de Physique, 1980, 41 (8), pp.799-818. 10.1051/jphys:01980004108079900. jpa-00209303 HAL Id: jpa-00209303 https://hal.archives-ouvertes.fr/jpa-00209303 Submitted on 1 Jan 1980 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. J. Physigue 41 (1980) 799-818 AOÛT 1980, 799 Classification Physics Abstracts 34.10 - 34.40 The role of the Pauli principle in metastability exchange collisions M. Pinard and F. Laloë Laboratoire de Spectroscopie Hertzienne de l’E.N.S. (*), 24, rue Lhomond, F 75231 Paris, France (Reçu le 20 novembre 1979, accepté le 14 avril 1980) Résumé. 2014 Dans les expériences de pompage optique, les collisions d’échange de métastabilité peuvent servir à transférer de l’orientation, alignement, etc... entre divers niveaux atomiques. Cet article est consacré à l’étude de telles collisions et de la façon dont elles agissent sur l’opérateur densité décrivant les variables internes des atomes. Le calcul présenté est valable pour des noyaux discernables ou identiques, ce qui rend possible une dis- cussion détaillée des effets d’indiscernabilité des noyaux (champ magnétique fictif, etc...). Deux cas sont étudiés : collisions sans dépolarisation (collisions He*-He), collisions avec dépolarisation partielle (Ne*-Ne par exemple). Les effets d’indiscernabilité nucléaire devraient être observables dans des expériences de pompage optique avec des gaz rares à basse température. Dans un appendice est discuté un autre effet d’indiscernabilité des particules qui peut être observé par des expé- riences de jets atomiques : au cours de la collision entre deux atomes 3He, tous deux dans le niveau fondamental, l’état de spin des atomes diffusés dans une direction particulière peut être changé par un effet d’indiscernabilité des noyaux. Abstract. 2014 In optical pumping experiments, metastability exchange collisions are used to transfer orientation, alignment, ... between different atomic levels. This article studies the effect of such collisions on the atom internal variables density operator by a method used in a previous publication for spin exchange collisions. The calculations are valid when the nuclei of the two atoms are distinguishable as well as when they are identical particles, which allows a detailed discussion of nuclear identity effects (apparent magnetic field, etc...). Two cases are successively studied : no depolarization of the electronic angular momentum (He*-He collisions) and partial depolarization (Ne*-Ne collisions for example). The nuclear identity effects should be observable in low temperature optical pumping experiments with noble gases. In an Appendix, another particle identity effect is studied, which can be observed in atomic beam experiments : during the collision of two 3He atoms, both in the ground state, the spin state of the atoms scattered in a particular direction can be changed by nuclear indistinguishability effects. 1. Introduction. - The role of the Pauli principle the hyperfine structure of the 2 1P state of ’He is too in spin exchange collisions has been discussed in a small to create a nuclear orientation during the previous article [1]. In order to emphasize the effects radiative lifetime). An indirect optical pumping arising from the particle indistinguishability, all method can nevertheless be used, as shown by particles were first supposed to be distinguishable, F. D. Colegrove, L. D. Schearer and G. K. Walters [3]. and the Pauli principle was only introduced in a The method consists in using the  = 1 .08 p line of second step. The same method will be used here, but helium (2 3S-2 3P transition) to create optically both for metastability exchange collisions. electronic and nuclear orientations of the 2 3S1 The importance of this type of collision in optical metastable state (which has a hyperfine structure of pumping experiments is well known [2]. In" helium approximately 6 GHz, much larger than its lifetime). experiments for example, direct nuclear polarization The nuclear polarization is then transferred to the of the ground state of 3 He cannot be achieved by using ground state of 3He by so called metastability exchange the optical resonance line for various reasons (this collisions between the 2 3S, and ground state atoms. line belongs to the vacuum U.V. part of the spectrum ; The corresponding evolution of the internal variable (I and J) density operator in both states has been studied by R. B. Partridge and G. W. Sefies [4]. These authors (*) Laboratoire Associé au Centre National de la Recherche evaluate coherence transfer effects in Scientifique. 3He optical pumping experiments, without including Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphys:01980004108079900 800 nuclear identity effects. One of the important physical metastability exchange calculations to the general ideas used is that the nuclear and electronic parts of case where the electronic internal variables can be newly formed metastable atoms are entirely uncor- affected by the collision. Since the fact that one of the related. When the two nuclei can be labelled, it is atoms is metastable does not enter explicitly in the indeed clear that, after exchange, the metastable atom calculation, it can be considered as a general study of contains the nucleus which was, before collision, the effects of nuclear identity on depolarizing col- associated with a ground state electronic cloud. lisions. In many experiments, these collisions occur On the other hand, when the two nuclei are identical with the same probability in all directions and the particles, it becomes impossible to tell which one rotational invariance introduces an important simpli- corresponds to a metastable or ground state atom, fication : the collision can be described in terms of so that a more careful examination seems to be electronic coefficients y(1) (orientation destruction necessary. One of the aims of the present article is to constant), y(2) (alignment destruction), even in the study precisely to what extent identical particle effects presence of a nuclear spin which is not affected by modify the equations obtained for the internal the collision [2, 11, 12, 13]. We shall see how this variable evolution. Actually, we shall find that in formalism must be adapted to take into account many practical situations (room temperature expe- energy transfer and nuclear identity effects. riments, low nuclear polarization), the decorrelation Another particle identity effect, which cannot be between electronic and nuclear spins, introduced in observed by optical pumping techniques, is briefly [4], is the only important effect of metastability discussed in an Appendix. This effect can be observed exchange. This justifies the use of equations of refe- in atomic beam experiments where a particular rence [4] as a starting point for subsequent calculations scattering direction is observed, and occurs during of the optical pumping process in 3He [5]. Neverthe- the interaction of two 3He atoms, which are both less, we shall also find that it is possible to design in the ground state. It is related to the subject of this experiments where nuclear identity effects (fictitious article as far as it is a modification of the atom internal magnetic fields) are not negligible, or maybe even variables arising from the Pauli principle. We shall dominant under appropriate conditions. see that the density operator, describing the internal There are in the literature other references concern- spin variables of the atoms scattered inside a given ing the effect of metastability exchange collisions in solid angle, is affected by particle identity effects. In interference effects occur in the forward helium optical pumping. A general paper on meta- particular, stable excitation transfer by H. J. Kolker and H. H. direction and change the spin state of the transmitted when the of the and incident beam Michels [6] includes a discussion of nuclear identity beam, spins target effects, but without introducing density operators are not parallel (or antiparallel). This effect is remi- for the internal atomic variables 1 and J. These authors niscent of the Faraday effect where the polarization of a beam is rotated in an medium. show why nuclear identity can rigorously be ignored light anisotropic At low collision we shall see that as far as only populations (longitudinal observables) energies, changes in the due to nuclear become the most are of importance in the experiment. This is an spin identity interesting result since, for example, it implies that significant. the maximum nuclear orientation obtained by optical pumping does not depend on nuclear identity effects. 2. Metastability exchange in hélium. - Let us first In section 2.2.2 of this we shall this article, discuss consider a specific case of metastability exchange colli- point in detail and show how these effects nevertheless sions between two helium atoms, one in the meta- do affect the evolution of the density matrix cohe- stable 2 3S1 state, the other in the ground state 1 iSo. rences is essential in resonance (which magnetic As mentioned in the introduction, one important Another related reference is a experiments). paper by feature of these collisions is that practically no depo- S. M. D. Rosner and F. Pipkin [7] which gives the larization occurs, due to the fact that all angular obtained in for uncorrelated part (the part [4] distin- momenta involved are spins, which are practically not of the and also guishable nuclei) density operator affected in a collision (Wigner rule).
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