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Quantum Information Science
QIS Quantum Computer
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The Quantum Century
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Y(1.9)K Y2K Shor Planck
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Three Great Ideas!
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(1) Quantum Computation Feynman ‘81 Deutsch ‘85 Shor ‘94
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A computer that operates on quantum states can perform tasks that are beyond the capability of any conceivable classical computer. Shor ‘94 Feynman ‘81 Deutsch ‘85
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? ? = ´ Finding Prime Factors
= ? ?
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= ´ Finding Prime Factors Shor ‘94
= Shor ‘94
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(2) Quantum Key Distribution Bennett Brassard ‘84
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Eavesdropping on quantum information can be detected; key distribution via quantum states is unconditionally secure. Bennett Brassard ‘84
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No tapping a quantum telephone!!
Alice Eve Bob No tapping a quantum telephone!!
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(3) Quantum Error Correction Shor ‘ Steane ‘95
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Shor ‘95 Steane ‘95 Quantum information can be protected,
and processed fault-tolerantly. Shor ‘ Steane ‘95
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Quantum Error Correction
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Quantum Error Correction
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Quantum Error Correction
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Quantum Error Correction
Redundancy protects against quantum errors!
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Challenges for 21st century science!
Three Great Ideas: 1) Quantum Computation 2) Quantum Key Distribution 3) Quantum Error Correction Where will they lead? Challenges for 21st century science!
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Quantum information and precision measurement
LIGO III: Beyond the standard quantum limit in 2008?! Thorne Kimble Caves
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physics lab, exploiting:
Quantum Information and Precision Measurement New strategies for the physics lab, exploiting: quantum entanglement quantum information processing quantum error correction etc.
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rin rout ? Unknown classical force = mystery Hamiltonian
(or master equation)
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Hamiltonian ? rout
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Hamiltonian ? Measure (Classical) Outcome Inference about H
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rin rout ? How should we “query” the box to
Hamiltonian ? rin rout How should we “query” the box to extract “optimal” information?
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Hamiltonian ? rin rout Drive the box: H = H? + HDrive Cf. Grover
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Entangled Strategies Gather More Information
Bloch sphere Which way does the spin point?
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Entangled Strategies Gather More Information
Which way does the spin point? parallel anti-parallel Compare: vs. Gisin, Popescu
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Ion Trap Quantum Computer
Zoller Ion Trap Quantum Computer I. Cirac, P. Zoller
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Ion Trap Quantum Computer
Zoller Ion Trap Quantum Computer I. Cirac, P. Zoller
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Ion Trap Quantum Computer
Zoller Ion Trap Quantum Computer I. Cirac, P. Zoller
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Ion Trap Quantum Computer
Zoller Ion Trap Quantum Computer I. Cirac, P. Zoller
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Ion Trap Quantum Computer
Zoller Ion Trap Quantum Computer I. Cirac, P. Zoller
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Experimental Challenges:
Read out single qubits. Controlled coherent multi-qubit interactions. Controlled fabrication. etc. From ions, photons, atoms to nuclei, electrons. What quantum states and operations are useful and/or important?
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Is there a sharp boundary?
Quantum vs. Classical Very Quantum Classical Is there a sharp boundary? Where is it?
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Octahedral Computation
Bloch Sphere
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Octahedral Computation
inscribed octahedron inscribed octahedron
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Controlled-NOT Gate a b a a b
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Octahedral Computation
Suffices for quantum error correction. Not universal quantum computation. Can be efficiently simulated on classical computer. Knill
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Octahedral Computation
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r The “boundary” is the octahedron.. Octahedral Computation
Conjecture (Kitaev): A reservoir of quantum states outside the octahedron Universal quantum computation The “boundary” is the octahedron..
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Is there a sharp boundary?
Quantum vs. Classical Very Quantum Classical Is there a sharp boundary? Where is it?
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Quantum vs. Classical Ensemble quantum computing at high temperature
(e.g., liquid state NMR). High T unentangled: A probability distribution of classical spins. But … entangling operations. Efficient classical simulations possible? A hierarchy of computational models? Knill, Laflamme, Caves, ...
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Multiparticle Entanglement
How to characterize it and quantify it, for pure states. Cf., two qubits: Y AB A B
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Y AB A B M copies
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Local Operations Y AB A B Local Operations M copies
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Local Operations Local Operations Classical M copies Communication
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N copies (N < M) EPR AB A B Bennett, et al....
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Y AB A B ( )M ( )N EPR AB A B Two party pure-state entanglement can be converted to a standard currency (EPR pairs) … and back again.
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But what about 3 (or more) part pure-state entanglement?
2 “cat” (GHZ) states A B C 3 EPR pairs A B C Unknown whether these are (asymptotically) interchangeable. Popescu, Bennett, ...
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Many particles ? m-cats (m-1)-cats (m-2)-cats 2-cats 1 2 3 4 m
Standard form: Quantum critical phenomena: how entangled is the ground state? Quantum dynamics: how hard to simulate (classically)?
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Fermilab Planckatron 103 GeV 1019 GeV !? 1016 in energy,
1032 in luminosity ..
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Q Feynmanlab
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Using quantum mechanics, a device can be built that can handle information in a way no classical machine will be able to reproduce, such as the determination of the prime factors of very large numbers in an amount of time not much more than what is needed to do multiplications and other basic arithmetic with these large numbers. If our theory is right, it should be possible to mimick such a device using a classical theory. This gives us a falsifiable prediction: ‘t Hooft It will never be possible to construct a `quantum computer’ that can factor a large number faster, and within a smaller region of space, than a classical machine would do, if the latter could be built out of parts at least as large and as slow as the Planckian dimensions.
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This theoretical failure to find a plausible alternative to quantum mechanics … suggests to me that quantum mechanics is the way it is because any small changes in quantum mechanics would lead to absurdities. Weinberg
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Concatenated Quantum Coding
Each box, when examined with higher resolution, is itself a block of five boxes.
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Unitarity Deviations from Unitarity (e.g, decoherence) fine resolution
coarser resolution still coarser resolution Unitarity
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Is Nature fault-tolerant? intrinsic Unitarity Deviations from
fine resolution Are the laws of physics attracted to quantum mechanics in the infrared? Deviations from Unitarity (e.g, intrinsic decoherence) coarser resolution Hawking ‘75 Is Nature fault-tolerant? still coarser resolution Unitarity
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The 1st Quantum Century:
What happened after 1926? We learned more about the Hamiltonian of the world: Standard model, M-theory (?) … We learned new tools for inferring its consequences: Renormalization group, broken symmetries .. and …. We began to appreciate the implications of the tensor product structure of Hilbert space: Quantum algorithms, Quantum error correction, ...
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Quantum Information Science
… is much more than a faster way to factor! An enduring place at the core of computer science: Cryptography Computational complexity Communication complexity Error correction, fault-tolerance Great Ideas destined for wider application: Precision measurement Quantum-classical boundary Many-particle entanglement A uniquely interdisciplinary community that should be nurtured.
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Quantum Information Science
QIS Quantum Computer
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