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25.09.2006 10:51

Match making in an egg carton

Dr. Olivia Meyer-Streng Presse- und Öffentlichkeitsarbeit
Max-Planck-Institut für Quantenoptik

    Molecules are possible candidates for quantum bits, the memory and processor units of a future quantum computer. Thereby, it is important that the molecules can store and exchange quantum information. In order for this to work, the molecules need to be arranged and kept in a regular array. Physicists at the Max Planck Institute of Quantum Optics in Garching have now succeeded in creating such a state using an optical lattice. The optical lattice is formed by superimposing several laser beams, the resulting shape of which resembles a stack of egg cartons. Exactly two atoms were placed into each well of this 'egg carton'. By applying a magnetic field, these atom pairs are associated to molecules (Nature Physics, 24th of September).

    In principle, atoms and molecules are equally well suited as memory units for quantum information processing. However, polar molecules, i.e. molecules with a positive and negative charge pole, can interact via electric forces - very much the way two magnets repel or attract each other depending on their relative orientation. Such an electric interaction is a convenient way for the molecules to communicate with each other and exchange information. This makes them highly interesting candidates for quantum information processing.

    Molecules however, are made up of several atoms, making them complicated objects. While atoms can be cooled down and brought to a standstill using laser light and other tricks, this is not as easily accomplished for molecules due to their complicated internal structure. Their atoms can vibrate against each other and at the same time the whole molecule can also rotate. One prerequisite for using molecules as quantum bits, however, is that their temperature is close to absolute zero, i.e. the molecules should more or less be at rest. The physicists also solved this challenge. As Prof. Dr. Gerhard Rempe, director at the Max-Planck Institute for Quantum Optics explains: "We circumvent this problem by producing the molecules right at the sites of the optical lattice."

    To this end, the researchers transferred a very cold gas of rubidium atoms, a so-called Bose-Einstein condensate, into the optical lattice. The optical lattice is created by intersecting several laser beams in the right fashion. The shape of the resulting light field resembles a stack of egg cartons, where the wells, or lattice sites, correspond to energetically favourable locations. As a consequence, the rubidium atoms prefer to sit at these sites. The depth of the lattice sites depends on laser intensity. At low laser intensities, the atoms can move almost freely in the optical lattice and move from site to site. With increasing laser intensities, the wells become deeper and deeper and at some point the atoms can not escape from the well in which they find themselves - they are trapped and localized. The resulting highly ordered state is called a Mott insulator state. Changing the overall atom number in the lattice, the physicists were able to create a situation with exactly two atoms per site in the centre of the lattice. Only at the edges of the optical lattice, atoms were trapped on singly-occupied sites. (Fig. 1)

    In the following step, the scientists applied a magnetic field and slowly changed its strength, thus exploiting a phenomenon called Feshbach resonance: Once the magnetic field has reached a certain strength, it becomes more favourable for the atoms in doubly-occupied sites to bind themselves to their partner than to stay single. Those atoms doomed to stay single because they have no partner to associate with are expelled from the optical lattice. They are of no great use any more, as Gerhard Rempe elucidates: "We have 'blasted away' the atoms on singly-occupied sites by using other laser light. As a result we got a state with exactly one molecule per lattice site."

    Once the magnetic field is returned to its original value, the molecular bond breaks up again and the atoms return to their initial state. This fact is important for verifying whether or not the experiment has been successfully realized, as only the atoms are visible in the experiment. The molecules are invisible in the detection. Thomas Volz, who carried out the experiment with his colleagues, explains that "since we broke the bond and could again observe the state with two atoms per lattice site, we made sure that the molecules stayed on their sites and did not escape from the lattice." (Fig. 2)

    The production of a state with exactly one molecule per lattice site is an important pre-requisite for the realization of quantum information processing with molecules. The Garching experiment is therefore an important step in this direction. [T.V.]

    Further information:
    Prof. Dr. Gerhard Rempe
    Professor at TU Munich
    Director at Max Planck Institute of Quantum Optics
    Hans-Kopfermann-Straße 1
    85748 Garching
    Telefon: +49 - 89 / 32905 701 / 711
    Fax: +49 - 89 / 32905 336
    E-Mail: gerhard.rempe@mpq.mpg.de

    Dr. Thomas Volz
    Max Planck Institute of Quantum Optics
    Hans-Kopfermann-Straße 1
    85748 Garching
    Telefon: +49 - 89 / 32905 241
    E-mail: thomas.volz@mpq.mpg.de

    Dr. Olivia Meyer-Streng
    Press & Public Relations Office
    Max Planck Institute of Quantum Optics
    Hans-Kopfermann-Straße 1
    85748 Garching
    Telefon: +49 - 89 / 32905 213
    Fax: +49 - 89 / 32905 200
    E-mail: olivia.meyer-streng@mpq.mpg.de


    Bilder

    Fig.1: Schematic illustration of the state with one molecule per lattice site. The lattice sites in the centre of the lattice are occupied by molecules (red colour). They were associated from two (identical) atoms using a magnetic field. At the edge of the lattice there are singly-occupied sites with atoms that have no partner to bind with (orange colour). In the experiment, the number of (occupied) sites is much larger.
    Fig.1: Schematic illustration of the state with one molecule per lattice site. The lattice sites in ...
    MPQ
    None

    Fig.2: Interference pictures with atoms and molecules. After switching off the lattice light, the atoms fly apart, which can be observed using a CCD camera. An interference pattern with the typical satellite peaks thereby develops. The three pictures were taken before binding the atoms to the molecules, after binding and after breaking up the bond again. The fact that the first and last of the three pictures are so similar proves that the experiment was successful. The picture in the middle only shows atoms from singly-occupied lattice sites. The molecules are invisible in the detection
    Fig.2: Interference pictures with atoms and molecules. After switching off the lattice light, the at ...
    MPQ
    None


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    Fig.1: Schematic illustration of the state with one molecule per lattice site. The lattice sites in the centre of the lattice are occupied by molecules (red colour). They were associated from two (identical) atoms using a magnetic field. At the edge of the lattice there are singly-occupied sites with atoms that have no partner to bind with (orange colour). In the experiment, the number of (occupied) sites is much larger.


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    Fig.2: Interference pictures with atoms and molecules. After switching off the lattice light, the atoms fly apart, which can be observed using a CCD camera. An interference pattern with the typical satellite peaks thereby develops. The three pictures were taken before binding the atoms to the molecules, after binding and after breaking up the bond again. The fact that the first and last of the three pictures are so similar proves that the experiment was successful. The picture in the middle only shows atoms from singly-occupied lattice sites. The molecules are invisible in the detection


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