Entanglement entropy production in deep inelastic scattering
- URL: http://arxiv.org/abs/2110.04881v2
- Date: Tue, 4 Jan 2022 22:00:23 GMT
- Title: Entanglement entropy production in deep inelastic scattering
- Authors: Kun Zhang, Kun Hao, Dmitri Kharzeev, Vladimir Korepin
- Abstract summary: Deep inelastic scattering (DIS) samples a part of the wave function of a hadron in the vicinity of the light cone.
We show that the resulting entanglement entropy depends on time logarithmically, $mathcal S(t)=1/3 ln(t/tau)$ with $tau = 1/m$ for $1/m le tle (mx)-1$, where $m$ is the proton mass and $x$ is Bjorken $x$.
- Score: 6.359294579761927
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Deep inelastic scattering (DIS) samples a part of the wave function of a
hadron in the vicinity of the light cone. Lipatov constructed a spin chain
which describes the amplitude of DIS in leading logarithmic approximation.
Kharzeev and Levin proposed the entanglement entropy as an observable in DIS
[Phys. Rev. D 95, 114008 (2017)], and suggested a relation between the
entanglement entropy and parton distributions. Here we represent the DIS
process as a local quench in the Lipatov's spin chain, and study the time
evolution of the produced entanglement entropy. We show that the resulting
entanglement entropy depends on time logarithmically, $\mathcal S(t)=1/3
\ln{(t/\tau)}$ with $\tau = 1/m$ for $1/m \le t\le (mx)^{-1}$, where $m$ is the
proton mass and $x$ is the Bjorken $x$. The central charge $c$ of Lipatov's
spin chain is determined here to be $c=1$; using the proposed relation between
the entanglement entropy and parton distributions, this corresponds to the
gluon structure function growing at small $x$ as $xG(x) \sim 1/x^{1/3}$.
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