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Daniel Chernowitz

Publications and source records attributed to Daniel Chernowitz.

3 recordsLinked to original sources

Leveraged Learning: entropy destroyed per bit received

A learner holds a prior belief over boolean maps that answer a finite set of $Q$ questions, and receives answers one by one. Each answer costs surprisal and destroys uncertainty, not only about the question asked but every question still unasked. We call the ratio the leverage: table entropy destroyed per bit of surprisal received. It is unit for a uniform prior, but with an intelligent prior can be higher (not lower). Averaged over the truth prior and over the question order, the leverage is found exactly, and is generated by one sequence: the mean entropy $G_\ell$ of the answers to $\ell$ questions. Sending the number of input bits to infinity at fixed asked fraction $t = \ell/Q$, the increments of that sequence become a profile $\gamma(t)$, and initial question entropy $\eta_0$. The leverage closes to a thermodynamic limit. $L(t) = [\eta_0 - (1-t)\gamma(t)]/\int_0^t \gamma$. Exchangeable priors, by de Finetti, all give a flat $\gamma(t)$ and hence a hyperbolic $L(t)$, their deduction confined to a boundary layer at $t = 0$. We construct a simplicity prior that escapes this, grading Boolean maps by the degree of their polynomial over $\mathbb{F}_2$ and budgeting weight across degree shells by a CDF $F$. Reed-Muller capacity then gives $\gamma(t) = 1 - F(t)$ exactly, so any nonincreasing profile, and any leverage curve it generates, is realizable at macroscopic times.

cond-mat.stat-mech

On the Dynamics of Free-Fermionic Tau-Functions at Finite Temperature

In this work we explore an instance of the $\tau$-function of vertex type operators, specified in terms of a constant phase shift in a free-fermionic basis. From the physical point of view this $\tau$-function has multiple interpretations: as a correlator of Jordan-Wigner strings, a Loschmidt Echo in the Aharonov-Bohm effect, or the generating function of the local densities in the Tonks-Girardeau gas. We present the $\tau$-function as a form-factors series and tackle it from four vantage points: (i) we perform an exact summation and express it in terms of a Fredholm determinant in the thermodynamic limit, (ii) we use bosonization techniques to perform partial summations of soft modes around the Fermi surface to acquire the scaling at zero temperature, (iii) we derive large space and time asymptotic behavior for the thermal Fredholm determinant by relating it to effective form-factors with an asymptotically similar kernel, and (iv) we identify and sum the important basis elements directly through a tailor-made numerical algorithm for finite-entropy states in a free-fermionic Hilbert space. All methods confirm each other. We find that, in addition to the exponential decay in the finite-temperature case the dynamic correlation functions exhibit an extra power law in time, universal over any distribution and time scale.

cond-mat.stat-mech

Entanglement Dynamics of Random GUE Hamiltonians

In this work, we consider a model of a subsystem interacting with a reservoir and study dynamics of entanglement assuming that the overall time-evolution is governed by non-integrable Hamiltonians. We also compare to an ensemble of Integrable Hamiltonians. To do this, we make use of unitary invariant ensembles of random matrices with either Wigner-Dyson or Poissonian distributions of energy. Using the theory of Weingarten functions, we derive universal average time evolution of the reduced density matrix and the purity and compare these results with several physical Hamiltonians: randomized versions of the transverse field Ising and XXZ models, Spin Glass and, Central Spin and SYK model. The theory excels at describing the latter two. Along the way, we find general expressions for exponential $n$-point correlation functions in the gas of GUE eigenvalues.

quant-ph