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Problem
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code template
Code
import sympy as sp
chi, kappa, sigma, k = sp.symbols('chi kappa sigma k', real=True)
def answer(chi, kappa, sigma, k):
r"""
Return the expression of hydrodynamic mode spectrum $\omega(k)$ in Sympy format.
Inputs
----------
chi: sympy.Symbol, charge susceptibility, $\chi$
kappa: sympy.Symbol, quadrupole superfluid stiffness, $\kappa$
sigma: sympy.Symbol, coefficient of the leading order dissipative term, $\sigma$
k: sympy.Symbol, momentum, $k$
Outputs
----------
omega: set[sympy.Expr], a set of hydrodynamic mode dispersion relation(s), $\omega(k)$
"""
# ------------------ FILL IN YOUR RESULTS BELOW ------------------
omega = ... # a set of SymPy expression of inputs
# ---------------------------------------------------------------
return omegaproblem description
# Problem setup:
Effective field theory is a powerful tool used to construct phenomenological models via symmetries. The method has recently been extended to dissipative systems via the Schwinger-Keldysh formalism. In this problem we will study the dissipative effective field theory associated to spontaneous symmetry breaking of multipolar symmetries.
Consider a system with a conserved density , conserved dipole moments , and a conserved quadrupole moment . Assume that these are the only conserved quantities in the system.
Suppose that the quadrupole generator is spontaneously broken, and the charge and dipole generators are unbroken.
# Main problem:
Compute the spectrum of hydrodynamic modes .
Let be the charge susceptibility, be the quadrupole superfluid stiffness, and be the coefficient of the leading order dissipative term. You may assume all other EFT coefficients are zero. Express your answer in terms of , , and .
Plain-text mathematical notation (without MathML)
# Problem setup: Effective field theory is a powerful tool used to construct phenomenological models via symmetries. The method has recently been extended to dissipative systems via the Schwinger-Keldysh formalism. In this problem we will study the dissipative effective field theory associated to spontaneous symmetry breaking of multipolar U(1) symmetries. Consider a 1d system with a conserved density N=∫ρ, conserved dipole moments D=∫xρ, and a conserved quadrupole moment Q=∫x²ρ. Assume that these are the only conserved quantities in the system. Suppose that the quadrupole Q generator is spontaneously broken, and the charge N and dipole D generators are unbroken. # Main problem: Compute the spectrum of hydrodynamic modes ω(k). Let χ be the charge susceptibility, κ be the quadrupole superfluid stiffness, and σ be the coefficient of the leading order dissipative term. You may assume all other EFT coefficients are zero. Express your answer in terms of χ, κ, and σ.
Original LaTeX notation
# Problem setup: Effective field theory is a powerful tool used to construct phenomenological models via symmetries. The method has recently been extended to dissipative systems via the Schwinger-Keldysh formalism. In this problem we will study the dissipative effective field theory associated to spontaneous symmetry breaking of multipolar $U(1)$ symmetries. Consider a $1d$ system with a conserved density $N = \int \rho$, conserved dipole moments $D = \int x \rho$, and a conserved quadrupole moment $Q = \int x^2 \rho$. Assume that these are the only conserved quantities in the system. Suppose that the quadrupole $Q$ generator is spontaneously broken, and the charge $N$ and dipole $D$ generators are unbroken. # Main problem: Compute the spectrum of hydrodynamic modes $\omega(k)$. Let $\chi$ be the charge susceptibility, $\kappa$ be the quadrupole superfluid stiffness, and $\sigma$ be the coefficient of the leading order dissipative term. You may assume all other EFT coefficients are zero. Express your answer in terms of $\chi$, $\kappa$, and $\sigma$.
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