Concept

Bloch sphere — where it appears

A sphere whose points represent every pure state of a two-level quantum system, with the poles the two basis states and the equator their equal superpositions. Rotations of the sphere are pulses of the driving field, and a measurement projects the state onto the vertical axis.

Named by 2 essays across one field — each of them below, with the objects they name alongside it.

Also named here as quantum projection noise — the same set of essays touches all of them, so they are one junction rather than several.

$Ramsey fringes: two short pulses and a long wait. The fraction of atoms found in the upper state against the detuning of the drive from the atoms' frequency, in cycles per pulse length, for two π/2 pulses of length τ separated by a free time T = 10τ (solid), computed from the exact two-level evolution. Fringes of period 1/T ride under an envelope set by the short pulses (dotted, the response to one pulse of length 2τ). The central fringe is 0.0444 cycles per τ wide at half height, close to 1/2T. A single long pulse covering the same total time, 12τ (dashed), gives a peak 0.0666 wide: 1.50 times wider, and with no way of telling a large detuning from a small one by its side fringes alone.$

The wait that sets the precision

To measure an atom's frequency, the obvious method is to drive it and look for the response, and the sharpness of the answer is set by how long the drive lasts. Norman Ramsey found in 1949 that most of the drive is wasted. Two short pulses with a long wait between them do better than one long pulse, because during the wait the atom keeps its own time undisturbed, and any difference from the drive's time piles up as an angle the second pulse can read. Every primary clock in the world runs on that idea, and its precision is set by two numbers: how long the atoms can be left alone, and how many of them there are.

quantum · Measurement

A round uncertainty sheared into a thin one. The uncertainty in the direction of 100 atoms' combined spin, seen along the spin, drawn out to one standard deviation in each direction. Left: the atoms each in an independent superposition — a disk of variance N/4 = 25 in every transverse direction, so a rotation shows only once it moves the spin by √N/2 = 5.0 units. Right: after one-axis twisting, which turns the spin about the vertical axis at a rate proportional to its height, so that the upper half of the disk is pushed one way and the lower half the other (arrows). The disk becomes an ellipse with variances 1.22 and 535, its long axis tilted 12.2° from the horizontal. Its narrow direction, turned to lie along the rotation to be measured, is 12.0 dB quieter than the disk, allowing for the 11.8% the twisting costs in the length of the spin.

The atoms that measure better together

A clock read with a hundred independent atoms locates its phase no better than the scatter of a hundred coin tosses allows, because each atom answers the final question by itself. Let the atoms interact for a moment before they are read and that scatter can be shaped: the round uncertainty of their combined spin is sheared into a thin ellipse, and a phase error invisible against the coin-toss noise becomes four standard deviations wide. The gain grows with the number of atoms, and it is real only if the detector can count atoms nearly one by one.

quantum · Measurement

Named alongside it

The objects these essays reach for when they reach for this one.

Atomic clock Quantum projection noise Binomial distribution Entanglement Interference Linewidth Measurement Spin squeezing Standard quantum limit Superposition Two-level system Uncertainty principle

All concepts