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Paula - Linear Quantum-Spin Systems

 
 

Govinda Clos, Matthias Wittemer, Jan-Philipp Schröder, Frederick Hakelberg, Philip Kiefer, Ulrich Warring, and Tobias Schaetz

introduction

quantum simulation with trapped ions

    Richard Feynman originally proposed to use a well-controlled quantum system to efficiently tackle problems that are too complex to be addressed with classical computers, such as quantum dynamics of many body systems; he called his hypothetical device a quantum computer (QC). Today, we classify it as an analog quantum simulator (AQS) to distinguish it from a QC, in which the dynamics of a system are implemented via algorithms of gate operations on subsets of qubits. In an AQS the strategy is to adiabatically evolve a quantum system from an experimentally well-prepared (initial) state to a new state by changing its Hamiltonian in a controlled manner, to reveal, for example, highly non-trivial dynamics, such as quantum phase transitions. Either device, QC and AQS, may help to develop insights into underlying physics. In addition, well-controlled quantum systems may enable to simulate processes in quantum chemistry and (quantum) biology, such as photosynthesis, where it is under debate whether the laws of quantum mechanics could also influence biological and other macroscopic objects. In any cases, we may gain a deeper understanding of the essential ingredients by directly observing a controlled model quantum system.

ion_crystalLabor_dunkel

laser cooled trapped ions form complex 3D (cp. KINKS) and more simple linear Coulomb crystals

    Currently there are efforts to implement QC/AQS in many different physical systems; we purse an approach with trapped ions: In the past, spectacular progress has been achieved in controlling the dynamics of such isolated quantum systems, as highlighted with the award of the 2012 Physics Nobel Prize to S. Haroch and D. J. Wineland: ”for ground-breaking experimental methods that enable measuring and manipulation of individual quantum systems” [Nobel prize website]. Nonetheless such controlled quantum systems (cp. tools below) have been limited to only a few constituents to permit mitigating residual decoherence effects. Methods for implementing large-scale devices/systems are still in the developmental phase. One of our goals is to contribute to a substantially more robust implementation of such systems to enable and to drive progress toward larger quantum systems (cp. BERMUDA project). While another mission of the PAULA apparatus is to study couplings of isolated quantum systems to well-controlled environments (open-quantum systems).
 
  paula_assembly_3.jpgdye_laserBBO

impressions from a quantum simulator: ion trap, dye-laser system, and second-harmonic-generation stage

    In the past, PAULA has been used to demonstrate the first optical trap for ions (now a dedicated spin-off project: OPIAT) and proof-of-principle quantum simulation experiments, e.g.: simulation of a quantum phase transition [Nature Physics 4, 757 - 761 (2008)] and quantum walk [Phys. Rev. Lett. 103, 090504 (2009)].

our tools in the lab

 

further reading

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