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Billions of molecules are used, each one a separate quantum computer. Most advanced experimental demonstrations to date, but poor scalability as molecule design gets difficult and SNR falls. Qubits are stored in nuclear spin of flourine atoms and controlled by different frequencies of magnetic pulses.

Used to factor 15 experimentally.

Vandersypen, 2000

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Qubits are stored in the spin of the nucleus of phosphorus atoms embedded in a zero-spin silicon substrate. Standard VLSI gates on top control electric field, allowing electrons to read nuclear state and transfer that state to another P atom.

Kane, Nature, 393(133), 1998

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High electron mobility transistor (HEMT)

http://www.fqd.fujitsu.com/

Quantum dot structure

N < 30

# of electrons

(5)

Coulomb blockade region, (the number of electrons is an integer,

N) orbital degree of freedom

&

spin degree of freedom

double quantum dot

bonding & anti-bonding orbitals (charge qubit)

(spin qubit)

Single-electron tunneling (SET)

S. Tarucha et al., Phys. Rev. Lett. 77, 3613 (1996).

1s 2p 3d

|ψ(r)| 2 500 nm

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coherency of the system

dissipation (T 1 ), decoherence (T 2 ) & manipulation

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A double quantum dot fabricated in AlGaAs/GaAs

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Approximate number of electrons: 10 ~ 30 Charging energy of each dot: ~ 1 meV Typical energy spacing in each dot: ~100 ueV Electrostatic coupling energy:~200 ueV Lattice temp. ~ 20 mK (2 ueV)

Electron temp. ~ 100 mK (9 ueV) <

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(Y. Nakamura ’99)

(6)

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Double quantum dot AlGaAs/GaAs 2DEG EB litho., fine gates,

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filtering

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Two-qubit device

Pashkin et al., Nature, 421(823), 2003

One-qubit device can control the number of Cooper pairs of electrons in the box, create superposition of states.

Superconducting device, operates at low temperatures (30 mK).

Nakamura et al., Nature, 398(786), 1999

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J. Martinis, NIST

Qubit representation is phase of current oscillation.

Device is physically large enough to see!

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the loop.

(7)

„ ‡ ˆ

NIST, Oxford, Australia, MIT, others Ions (charged atoms) are

suspended in space in an oscillating electric field.

Each atom is controlled by a laser.

‹ Ž 

NIST, Oxford, Australia, MIT, others Number of atoms that can

be controlled is limited, and each requires its own laser. Probably <100 ions max.

T‘ ’“ ”• – —• ’ ’“ ”˜ ™š ’œ› ž Ÿ

Deutsch, UNM

Neutral atoms are held in place by standing waves from several lasers.

Atoms can be brought together to execute gates by changing the waves slightly.

Also used to make high-precision atomic clocks.

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All-optical CNOT gate composed from

beam splitters and wave plates. O'Brien et al., Nature 426(264), 2003

(8)

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Apples-to-apples comparison is difficult, and coherence times are rising experimentally.

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Our entire discussion so far has been on “perfect”

quantum gates, but of course they are not perfect.

Various “threshold theorems” have suggested that

we need 10^4 to 10^6 gates in less than the

decoherence time in order to apply quantum error

correction (QEC). QEC is a big enough topic to

warrant several lectures on its own.

(9)

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