Zitterbewegung

Zitterbewegung ("trembling motion" in German) is a hypothetical rapid motion of elementary particles, in particular electrons, that obey the Dirac equation. The existence of such motion was first proposed by Erwin Schrödinger in 1930 as a result of his analysis of the wave packet solutions of the Dirac equation for relativistic electrons in free space, in which an interference between positive and negative energy states produces what appears to be a fluctuation (at the speed of light) of the position of an electron around the median, with a frequency of $2 mc 2 / ℏ$ , or approximately 7021160000000000000♠1.6×10²¹ radians per second. A reexamination of Dirac theory, however, shows that interference between positive and negative energy states may not be a necessary criterion for observing zitterbewegung.^[1]

For the hydrogen atom, the zitterbewegung produces the Darwin term which plays the role in the fine structure as a small correction of the energy level of the s-orbitals.

Theory for a free electron

The time-dependent Dirac equation is written as

H\psi (\mathbf {x} ,t)=i\hbar {\frac {\partial \psi }{\partial t}}(\mathbf {x} ,t)

,

where $\hbar$ is the (reduced) Planck constant, $\psi (\mathbf {x} ,t)$ is the wave function (bispinor) of the electron, and $H$ is the Dirac Hamiltonian of a free particle:

H=\beta mc^{2}+\sum _{j=1}^{3}\alpha _{j}p_{j}c

,

where ${\textstyle m}$ is the mass of the electron, ${\textstyle c}$ is the speed of light, ${\textstyle p_{j}}$ is the momentum operator, and $\beta$ and $\alpha _{j}$ are matrices related to the Gamma matrices ${\textstyle \gamma _{\mu }}$ , as ${\textstyle \beta =\gamma _{0}}$ and ${\textstyle \alpha _{j}=\gamma _{0}\gamma _{j}}$ .

In the Heisenberg picture implies that any operator $Q$ obeys the equation

-i\hbar {\frac {\partial Q}{\partial t}}=\left[H,Q\right].

In particular, the time-dependence of the position operator is given by

\hbar {\frac {\partial x_{k}(t)}{\partial t}}=i\left[H,x_{k}\right]=\hbar c\alpha _{k}

.

where $x k (t)$ is the position operator at time $t$ .

The above equation shows that the operator $α k$ can be interpreted as the $k$ -th component of a "velocity operator". To add time-dependence to $α k$ , one implements the Heisenberg picture, which says

\alpha _{k}(t)=e^{\frac {iHt}{\hbar }}\alpha _{k}e^{-{\frac {iHt}{\hbar }}}

.

The time-dependence of the velocity operator is given by

\hbar {\frac {\partial \alpha _{k}(t)}{\partial t}}=i\left[H,\alpha _{k}\right]=2\left(i\gamma _{k}m-\sigma _{kl}p^{l}\right)=2i\left(p_{k}-\alpha _{k}H\right)

,

where

\sigma _{kl}\equiv {\frac {i}{2}}\left[\gamma _{k},\gamma _{l}\right].

Now, because both $p k$ and $H$ are time-independent, the above equation can easily be integrated twice to find the explicit time-dependence of the position operator.

First:

\alpha _{k}(t)=\left(\alpha _{k}(0)-cp_{k}H^{-1}\right)e^{-{\frac {2iHt}{\hbar }}}+cp_{k}H^{-1}

,

and finally

x_{k}(t)=x_{k}(0)+c^{2}p_{k}H^{-1}t+{\tfrac {1}{2}}i\hbar cH^{-1}\left(\alpha _{k}(0)-cp_{k}H^{-1}\right)\left(e^{-{\frac {2iHt}{\hbar }}}-1\right)

.

The resulting expression consists of an initial position, a motion proportional to time, and an unexpected oscillation term with an amplitude equal to the Compton wavelength. That oscillation term is the so-called zitterbewegung.

The zitterbewegung term vanishes on taking expectation values for wave-packets that are made up entirely of positive- (or entirely of negative-) energy waves. This can be achieved by taking a Foldy–Wouthuysen transformation. Thus, we arrive at the interpretation of the zitterbewegung as being caused by interference between positive- and negative-energy wave components.

Experimental simulation

Zitterbewegung of a free relativistic particle has never been observed. However, it has been simulated twice. First, with a trapped ion, by putting it in an environment such that the non-relativistic Schrödinger equation for the ion has the same mathematical form as the Dirac equation (although the physical situation is different).^[2]^[3] Then, in 2013, it was simulated in a setup with Bose–Einstein condensates.^[4]

References and notes

↑ David Hestenes (1990). "The zitterbewegung interpretation of quantum mechanics". Foundations of Physics. 20 (10): 1213–1232. Bibcode:1990FoPh...20.1213H. doi:10.1007/BF01889466.
↑ "Quantum physics: Trapped ion set to quiver". Nature News and Views. 463 (7277).
↑ Gerritsma; Kirchmair; Zähringer; Solano; Blatt; Roos (2010). "Quantum simulation of the Dirac equation". Nature. 463 (7277): 68–71. arXiv:0909.0674. Bibcode:2010Natur.463...68G. doi:10.1038/nature08688.
↑ Leblanc; Beeler; Jimenez-Garcia; Perry; Sugawa; Williams; Spielman (2013). "Direct observation of zitterbewegung in a Bose–Einstein condensate". New Journal of Physics. 15 (7): 073011. doi:10.1088/1367-2630/15/7/073011.

External links

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[1] David Hestenes (1990). "The zitterbewegung interpretation of quantum mechanics". Foundations of Physics. 20 (10): 1213–1232. Bibcode:1990FoPh...20.1213H. doi:10.1007/BF01889466.

[2] "Quantum physics: Trapped ion set to quiver". Nature News and Views. 463 (7277).

[3] Gerritsma; Kirchmair; Zähringer; Solano; Blatt; Roos (2010). "Quantum simulation of the Dirac equation". Nature. 463 (7277): 68–71. arXiv:0909.0674. Bibcode:2010Natur.463...68G. doi:10.1038/nature08688.

[4] Leblanc; Beeler; Jimenez-Garcia; Perry; Sugawa; Williams; Spielman (2013). "Direct observation of zitterbewegung in a Bose–Einstein condensate". New Journal of Physics. 15 (7): 073011. doi:10.1088/1367-2630/15/7/073011.

Zitterbewegung

Theory for a free electron

Experimental simulation

See also

References and notes

Further reading

External links