Simultaneous control over both excitational and motional degrees of freedom of quantum objects facilitates measurement accuracies at a level that enables the measurement of subtle relativistic effects, tests of the Standard Model and even the search for expected effects of physics beyond it. Theoretical calculations predict enhanced sensitivities of forbidden optical transitions in highly charged ions (HCIs) to possible variations of fundamental constants, such as the fine structure constant. Within this thesis, a versatile preparation technique of cold and strongly localized HCIs has been developed and demonstrated, adding a multitude of laser accessible systems to the quantum toolbox, that have enhanced sensitivity to fundamental physics. HCIs are extracted from an electron beam ion trap (EBIT), where they are produced in the MK temperature range. Subsequently they are cooled down to the mK regime, needed for high precision laser spectroscopy, in a cryogenic linear Paul trap. Deceleration, precooling and multi-pass stopping approaches enable HCI implantation within a prestored, continuously laser-cooled Be+-Coulomb crystal. Here the HCIs are co-crystallized in mixed-species ensembles (specifically Ar13+ highly charged and Be+ coolant ions) - ranging from large 3-dimensional crystals over ion strings down to a single Ar13+ ion cooled by a single Be+ ion. The precooling, retrapping and sympathetic stopping process, as well as various Coulomb crystal configurations are characterized and compared to simulations and theoretical models. The developed experimental concept and its modular implementation enable, for the first time, the localization of HCIs in a microscopic region of a Paul trap, today's standard method for singly-charged ion frequency metrology. This is a necessary prerequisite for the development of novel ultra-precise optical clocks based on quantum logic spectroscopy on forbidden transitions in HCIs and subsequent low-energy searches for physics beyond the Standard Model.
Simultaneous control over both excitational and motional degrees of freedom of quantum objects facilitates measurement accuracies at a level that enables the measurement of subtle relativistic effects, tests of the Standard Model and even the search for expected effects of physics beyond it. Theoretical calculations predict enhanced sensitivities of forbidden optical transitions in highly charged ions (HCIs) to possible variations of fundamental constants, such as the fine structure constant. Within this thesis, a versatile preparation technique of cold and strongly localized HCIs has been developed and demonstrated, adding a multitude of laser accessible systems to the quantum toolbox, that have enhanced sensitivity to fundamental physics. HCIs are extracted from an electron beam ion trap (EBIT), where they are produced in the MK temperature range. Subsequently they are cooled down to the mK regime, needed for high precision laser spectroscopy, in a cryogenic linear Paul trap. Deceleration, precooling and multi-pass stopping approaches enable HCI implantation within a prestored, continuously laser-cooled Be+-Coulomb crystal. Here the HCIs are co-crystallized in mixed-species ensembles (specifically Ar13+ highly charged and Be+ coolant ions) - ranging from large 3-dimensional crystals over ion strings down to a single Ar13+ ion cooled by a single Be+ ion. The precooling, retrapping and sympathetic stopping process, as well as various Coulomb crystal configurations are characterized and compared to simulations and theoretical models. The developed experimental concept and its modular implementation enable, for the first time, the localization of HCIs in a microscopic region of a Paul trap, today's standard method for singly-charged ion frequency metrology. This is a necessary prerequisite for the development of novel ultra-precise optical clocks based on quantum logic spectroscopy on forbidden transitions in HCIs and subsequent low-energy searches for physics beyond the Standard Model.
Control over the motional degrees of freedom of atoms, ions, and molecules in a field-free environment enables unrivalled measurement accuracies but has yet to be applied to highly charged ions (HCIs), which are of particular interest to future atomic clock designs and searches for physics beyond the Standard Model. Here, we report on the Coulomb crystallization of HCIs (specifically (40)Ar(13+)) produced in an electron beam ion trap and retrapped in a cryogenic linear radiofrequency trap by means of sympathetic motional cooling through Coulomb interaction with a directly laser-cooled ensemble of Be(+) ions. We also demonstrate cooling of a single Ar(13+) ion by a single Be(+) ion-the prerequisite for quantum logic spectroscopy with a potential 10(-19) accuracy level. Achieving a seven-orders-of-magnitude decrease in HCI temperature starting at megakelvin down to the millikelvin range removes the major obstacle for HCI investigation with high-precision laser spectroscopy.
We report on the sympathetic cooling and Coulomb crystallization of xenon highly charged ions (HCIs) with laser-cooled Ca+ ions. The HCIs are produced in a compact electron beam ion trap, then charge selected, decelerated, and finally injected into a cryogenic linear Paul trap. There, they are captured into 40Ca+ Coulomb crystals, and co-crystallized within them, causing dark voids in their fluorescence images. Fine control over the number of trapped ions and HCIs allows us to realize mixed-species crystals with arbitrary ordering patterns. By investigating Xeq+--Ca+ strings, we confirm the HCI charge states, measure their lifetime and characterize the mixed-species motional modes. Our system effectively combines the established quantum control toolbox for Ca+ with the rich set of atomic properties of Xe highly charged ions, providing a resourceful platform for optical frequency metrology, searches for signatures of new physics, and quantum information science.
Fundamental interactions and symmetries define the structure and properties of all matter, in particular of its small and diverse visible constituents—the atoms. The study of their distinctive spectra through precision spectroscopy is therefore a vital tool to advance our understanding of nature. Highly charged ions (HCIs) constitute the largest fraction of all atoms since every atom has as many charge states as electrons it can bind. Although most of the matter on Earth is neutral, HCIs are ubiquitous in the universe and their systematic study is essential not only for atomic physics but eminently for astrophysics, nuclear physics, and fusion research, among others. Recently, HCIs have been identified as ideal candidates for sensitive tests of physics beyond the Standard Model of particle physics and for use in future high-accuracy optical atomic clocks. However, the realization of such proposals has been hindered by the hitherto constrained laboratory control and limited spectroscopic accuracy of about parts-per-million fractional uncertainty levels. This thesis reports the first coherent laser spectroscopy of HCIs, boosting the achievable spectroscopic precision by eight orders of magnitude compared to traditional spectroscopy methods. The 2P1/2–2P3/2 fine-structure ground-state transition in highly charged 40Ar13+ at an optical wavelength of 441 nm was chosen as a proof-of-principle case. A single ion of this species was isolated from a megakelvin-hot plasma cloud and co-trapped together with a laser-cooled singly charged 9Be+ ion in a two-ion crystal, confined in the harmonic potential of a cryogenic linear Paul trap. This coupled quantum-mechanical system was then cooled to its ground state of axial motion, corresponding to the lowest temperature of a HCI ever achieved. The spectroscopy was realized by implementing quantum logic techniques which allow preparation of the quantum state of the HCI and to map its electronic state after spectroscopy onto the 9Be+ logic ion in order to detect it there with high efficiency through electron shelving. In addition to the increase of spectroscopic precision, the excited-state lifetime and g-factor were measured—the latter one to unprecedented accuracy, resolving effects from special relativity, interelectronic interactions, and quantum electrodynamics. Moreover, it settled a discrepancy between theoretical predictions. The demonstrated techniques are not limited to the specific 40Ar13+ species but universally applicable to other HCIs. Thereby, this work unlocks the potential of HCIs for unrivaled tests of fundamental physics, the search for new physics—such as a 5th force, variations of fundamental constants and dark matter candidates—as well as the use of HCIs in novel optical atomic clocks.
We report the sympathetic cooling and Coulomb crystallization of xenon highly charged ions (HCIs) with laser-cooled Ca+ ions. The HCIs are produced in a compact electron beam ion trap, then charge selected, decelerated, and finally injected into a cryogenic linear Paul trap. There, they are captured into 40 Ca+ Coulomb crystals, and cocrystallized within them, causing dark voids in their fluorescence images. Fine control over the number of trapped ions and HCIs allows us to realize mixed-species crystals with arbitrary ordering patterns. By investigating Xeq+ − Ca+ strings, we confirm the HCI charge states, measure their lifetime, and characterize the mixed-species motional modes. Our system effectively combines the established quantum control toolbox for Ca+ with the rich set of atomic properties of Xe highly charged ions, providing a resourceful platform for optical frequency metrology, searches for signatures of new physics, and quantum information science.
Electron beam ion traps used for spectroscopy of highly charged ions (HCI) produce a deep trapping potential leading to high temperatures of the stored ions, and thus limiting the achievable spectral resolution. A novel device at the Max-Planck-Institut für Kernphysik, the Cryogenic linear Paul Trap Experiment (CryPTEx), attached to an electron beam ion trap, provides a new experimental platform to overcome these limitations. The trap assembly operates at a temperature of 4 K and offers optical access for quantum manipulation and imaging of the trapped ions. Since forbidden optical transitions in HCI do not support direct laser cooling, sympathetic cooling with Coulomb crystals of singly charged ions such as Be+ or Mg+ will be applied in order to reach the natural linewidth of optical forbidden transitions in HCI of interest. With the added advantage of long ion trapping times resulting from residual gas pressures of H2 at 4 K below 10−15 mbar, CryPTEx has been commissioned in collaboration with the Ion Trap Group in Århus using rovibrationally cooled MgH+ ions. Strong suppression of the black body radiation at the trap center, ion storage times of about 28 hours, and largely enhanced population of the rovibrational ground state were achieved.
Abstract Precision spectroscopy of atomic systems1 is an invaluable tool for the study of fundamental interactions and symmetries2. Recently, highly charged ions have been proposed to enable sensitive tests of physics beyond the standard model2–5 and the realization of high-accuracy atomic clocks3, 5, owing to their high sensitivity to fundamental physics and insensitivity to external perturbations, which result from the high binding energies of their outer electrons. However, the implementation of these ideas has been hindered by the low spectroscopic accuracies (of the order of parts per million) achieved so far6–8. Here we cool trapped, highly charged argon ions to the lowest temperature reported so far, and study them using coherent laser spectroscopy, achieving an increase in precision of eight orders of magnitude. We use quantum logic spectroscopy9, 10 to probe the forbidden optical transition in 40Ar13+ at a wavelength of 441 nanometres and measure its excited-state lifetime and g-factor. Our work unlocks the potential of highly charged ions as ubiquitous atomic systems for use in quantum information processing, as frequency standards and in highly sensitive tests of fundamental physics, such as searches for dark-matter candidates11 or violations of fundamental symmetries2.