Bulk Spin Resonance Quantum Computation

At the current rate of progress, in about two decades the scaling of VLSI is going to simultaneously hit many physical limits: a transistor will be one atom wide, a memory cell will have just one electron per bit (and the cost of the fab plant will be the GNP of the planet). If computers are to work any faster, progress is going to have to come from a radically different direction.

Quantum computation is an exciting prospect, because a quantum computer (if it could be built) would be exponentially faster than a classical computer on some problems. For example, a quantum computer could find prime factors in polynomial time instead of the exponential time required by a classical computer, thereby breaking conventional cryptographic codes.

The problem with building a quantum computer is that the quantum bits (called qubits) simultaneously need to be protected from the environment so that they retain their quantum phase, but they need to be coupled to the environment so that initial conditions can be loaded, the calculation applied, and the results read out. Because of these apparently contradictory constraints, it's taken a heroic experimental effort to make just a 2 bit quantum computer. This has been done in systems such as trapped ions, or cavity quantum electrodynamics, that carefully isolate the qubits and cool them to their ground state.

Neil Gershenfeld and Isaac Chuang have developed an entirely new approach to quantum computation that promises to solve many of these problems. Instead of carefully isolating a small number of qubits, we use a large thermal ensemble (such as a cup of coffee). Such a system has ~10^23 degrees of freedom; by applying RF pulses that excite nuclear magnetic resonances, we can create a tiny deviation from equilibrium that acts just like a much smaller number of pure qubits.

The nuclear spin is beautifully isolated from the environment; its spin coherence can last for thousands of seconds. By representing the effective computational qubits in such an ensemble, we get these very long coherence times permitting thousands of logical operations before coherence is lost. Further, because the bits are represented in an ensemble, it is possible to continuously read out the quantum state (somthing that is of course impossible for individual quantum degrees of freedom). Best of all, the most important part of the experimental apparatus is built by nature in the form of ordinary molecules.

Implementing such a quantum computer requires the mature techniques of multiple pulse spin resonance. Using existing NMR spectrometers it will be straightforward to reach about 10 qubits, enough to demonstrate for the first time quantum superfast algorithms and quantum error correction, and to prepare a range of unusual quantum states that have never been realized before (such as the Greenberger-Horne-Zeilinger states that maximally violate Bell's Theorem). The required instrumentation even promises to scale down to the desktop, so that everyone could have a quantum co-processor.


Here is the first paper on bulk spin resonance quantum computation (N. Gershenfeld and I. Chuang, Science, 275, pp. 350-356, 1997). More recent experimental and theoretical papers are available at the Physics and Media Group's publications page,

here is one of the first news articles (The Economist, pp. 91-92, February 22, 1997),

and here is a talk about it.

Go to Chuang's archive on quantum computation

Useful NMRQC resources