What Atomic Physics has to offer for Quantum Computing Tony Hyun Kim 6.UAT Proposal Talk Spring 2008.

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Presentation transcript:

What Atomic Physics has to offer for Quantum Computing Tony Hyun Kim 6.UAT Proposal Talk Spring 2008

Quantum Computing: (Brief) Inspiration Modern computing devices are based on classical mechanics (CM). But CM is a special limit of quantum mechanics. – Conclusion: Quantum devices can only have greater computational power than classical ones.

Quantum Computing: (Brief) Inspiration By a standard “complexity measure”… TaskQuantum computational gains Functional Iteration f(f(…f(x)…))) Not sped up at all! Locating an entry in a database of N entries O(N)  O(N 0.5 ) Prime factorizationApparently, sped up exponentially!

Outline 1.Requirements for a quantum computer 2.Why atomic physics? 1.Dilute gases in optical lattices 2.Atom cooling 3.The next challenge. 4.Plan of action for our group.

Basic Requirements for a Quantum Computer 1.Scalable physical system with well-characterized qubits 2.The ability to initialize the state of the qubits 3.Long decoherence times 4.Universal set of quantum gates 5.A qubit-specific measurement capacity 6.Ability to transport qubits Source: DiVincenzo, David P. “The Physical Implementation of Quantum Computation.” Fortschritte der Physik.

1) “Scalable physical system with well- characterized qubits” Qubit: A two-level physical system. – e.g. ground and excited states of an atom. Use two-level system to encode binary information.

2) “Ability to initialize the state of the qubits” Clearly necessary for information processing. For example, suppose we want to reset all qubits. – Physically, we need a way to manipulate many qubits en masse.

3) “A qubit-specific measurement capacity” Need a reliable way to access information. Must allow for specific addressing of the physical element. “Address”

Summary of the Problem Quantum computing demands: – A scalable physical system with two states – Ability to initialize the macroscopic system – Qubit-specific measurement capacity Proposal: – Dilute gases found in atomic physics labs are an ideal system meeting the above requirements.

Outline 1.Requirements for a quantum computer 2.Why atomic physics? 1.Dilute gases in optical lattices 2.Atom cooling 3.The next challenge. 4.Plan of action for our group.

Why atomic physics? Precision. An optical “tweezer”

Atomic physics: an illustrious recent history Development of precise, atomic physics techniques have led to several recent Nobel prizes. – 1997 – Chu, Cohen-Tannoudji, Phillips: “For development of methods to cool and trap atoms with laser light.” – 2001 – Cornell, Ketterle, Wieman: “For the achievement of Bose-Einstein condensation in dilute gases of alkali atoms…” – 2005 – Hall, Haensch: “For their contributions to the development of laser-based precision spectroscopy, including the optical frequency comb technique.”

Dilute gases in an optical lattice Chu, C-T, Phillips (1997) – Begin by setting up a standing wave

Dilute gases in an optical lattice Neutral atoms are attracted to regions of high oscillating electric field (“ac Stark effect”).

Dilute gases in an optical lattice: Typical numbers We routinely produce: ~1 million atoms per run. Our optical lattice is based on infrared laser: λ = 1000 nm The overlap volume of the lattice beams is: ~(1mm) 3 So, one atom per site is a realistic scenario! Number of sites: N = 1,000,000 Approximately one atom per site!

A Scalable QM System Atomic physics quantum computer: – Excited atomic/molecular states in optical lattice – As of now, we can create such experimental setups routinely. We possess dual-species oven: sodium and lithium

Resetting all qubits: atom cooling Decades of experience in cooling atoms – Remove thermal energy  Favor the ground state.

Summary of Previous Work The current state of atomic physics gives: – A readily scalable platform for qubits. (Requirement 1) – Easy to initialize to the “reset state.” (Requirement 2)

Outline 1.Requirements for a quantum computer 2.Why atomic physics? 1.Dilute gases in optical lattices 2.Atom cooling 3.The next challenge. 4.Plan of action for our group.

A qubit-specific measurement capacity We now have qubits in a known geometry. How to manipulate individual qubits? Proposal: – Use light-induced transitions.

Light induced transitions in an optical lattice Consider the 1D array of qubits: – With a fixed wavelength laser source, tuned to atomic transition Fixed frequency laser source

Light induced transitions in an optical lattice Laser frequency is fixed. – Instead, tune the atoms  Modify the atomic energy spacing. Fixed frequency laser source Capacitor with controlled voltage

What needs to be done E-Field modification of energy levels depends on electric dipole of the qubit. Our task: – Produce a molecule with a permanent dipole moment. – For our group, that means: – Production of sodium-lithium molecule.

Outline 1.Requirements for a quantum computer 2.Why atomic physics? 1.Dilute gases in optical lattices 2.Atom cooling 3.The next challenge. 4.Plan of action for our group.

Calendar Early summer 2008: – Installation of the optical lattice chamber. Summer 2008: – Settle the lab’s temperature problem. – Reinstallation of the optics/electronic equipment.

Calendar (continued) Fall 2008: – Association of lithium and sodium atoms. Sometime further on: – Attain deeply bound lithium and sodium atoms.