A Quantum Model of Spin Noise ✛ ✎

Original: "Quantum Model Of Spin Noise"
· R. Annabestani, D. G. Cory, J. Emerson
arXiv:1407.7620 · 2014-07-29 · arXiv non-exclusive · independent analysis · 3 min
Spin noise is described in the language of open quantum systems, unifying strong and weak measurements.

Context

Spin noise, arising from quantum fluctuations of a particle ensemble, has been observed experimentally since Bloch's prediction in 1946. This phenomenon becomes significant in samples with a small number of spins or with very long relaxation times, where fluctuations can exceed thermal polarization. The work sits at the intersection of quantum information and magnetic resonance: in the archive, studies of quantum noise and its robustness surround it, but this article stands out for its systematic approach via the open quantum systems formalism, rather than introducing fluctuating fields.

Methods

The model is built on representing the evolution of a spin ensemble as a sequence of quantum operations: measurement and evolution. The interaction with the bath is described by a CPTP map (completely positive trace-preserving map), and the interaction with the detector is described through measurement operators. For strong measurements, projectors onto subspaces with fixed magnetization are used; for weak measurements, POVM elements (positive operator-valued measure) with a Gaussian profile are used. The cases of a collective depolarizing map and arbitrary CPTP maps on non-interacting spins are considered.

Results

Analytical expressions are obtained for the probability distributions of measurement outcomes and correlation functions. For a fully mixed initial state and depolarizing evolution, the correlation function decays exponentially with a characteristic relaxation time: R(k) = (N/4) exp(-$t_k$/T). The noise amplitude grows as the square root of the number of spins. It is shown that the statistics of the second measurement correlate with the first, with the correlation vanishing at large time intervals or for weak measurements. For arbitrary initial states, except for the first measurement, the statistics coincide with the mixed-state case.

Implications

The work demonstrates that spin noise can be fully described within the standard formalism of open quantum systems, without invoking phenomenological fluctuating fields as in earlier models. This differs from neighboring works that focus on specific experimental implementations or on robustness to noise, whereas here a universal theoretical framework is proposed. Such an approach simplifies analysis and opens the way to a unified description of noise in various quantum technologies.

Future development

The model can be extended to interacting spins, inhomogeneous fields, and more realistic detection models. It may be applied to spin qubits in quantum computers, where noise limits coherence time. Also promising is the investigation of the connection between weak measurements and back-action on the system.

Impact

The results are useful for interpreting spin noise experiments in NMR, magnetometry, and quantum sensing. The model can serve as a basis for designing error correction schemes in spin-based quantum processors.

Next steps

Test the model's predictions against experimental data, especially for small spin ensembles. Generalize to the case of interacting spins and non-ideal measurements.

Key open problems

The work touches on the fundamental problem of quantum measurement: how obtaining information about a system affects its state. The connection between strong and weak measurements and their role in the emergence of noise remains an open question in quantum theory.

The knowledge machine's view

This section is addressed to the author of the paper and their colleagues. Neighbouring works were found by meaning-based search across our archive, not by word overlap. We do not review: we show the field around the work.

What the work does

This work builds a theoretical model of spin noise in ensembles of quantum particles based on the formalism of open quantum systems. The authors consider sequences of measurements and evolution, and derive analytical expressions for the noise statistics and correlation functions, applicable to strong and weak measurements, arbitrary initial states, and CPTP maps.

Where its strength is

A systematic description of spin noise via quantum operations without phenomenological fluctuating fields, yielding explicit analytical results for correlations and statistics.

Where it could go next

Worth trying

  • Test whether known experimental spin noise spectra are reproduced in the limit of weak continuous measurements.
  • Use the model to compute higher-order correlations in small ensembles where thermal polarization is small.
  • Consider non-stationary CPTP maps and their influence on noise statistics.

Why this may matter

A unified theoretical framework for spin noise could simplify the analysis of quantum measurements and aid in the development of quantum technologies sensitive to ensemble fluctuations.

In 1946, Felix Bloch predicted that even without an external magnetic field, a spin ensemble exhibits a fluctuating magnetic moment proportional to the square root of the number of particles. This effect was experimentally confirmed only decades later.

R(k) = \frac{N}{4} e^{-t_k/T}
The correlation between measurements decays exponentially with time
\sigma[M; t_1] = \frac{1}{2}\sqrt{N}
The noise grows as the square root of the number of spins

Key numbers

  • Noise amplitude: √N/2 (in units of ħ/2)
  • Characteristic correlation time: T (relaxation time)
  • Number of spins in the example: 100
  • Width of weak measurement: w=5
Scientists
Niels BohrPascual JordanWerner HeisenbergEnrico FermiPaul DiracWolfgang Pauli
Concepts
statistical noise spin foam quantum number spin–statistics theorem jitter random fluctuation stochastic fluctuations spin axis fluctuation oscillation instability wave function uncertainty stochastic neutrino oscillations virtual particle Neural Network Oscillations spin probability theory vibration