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CritPt / Challenge_57_main / Consider a vector field A^(μ) coupled to the standard model B−L current…
Problem
Answer published by the source. Consult the official source to check your work against its answer.
code template
Code
def answer():
r"""
Return the values of the smallest $\epsilon_{B-L}$ for three scenarios.
Inputs
----------
None
Outputs
----------
eps_B_L_min: list[float],
smallest $\epsilon_{B-L}$ it can probe at $250\,\text{Hz}$ with an observation time of $13$ years and SNR of $1$
for scenarios where $\delta q=\{0.074, 6\times 10^{-3}, 5\times 10^{-4}\}$.
"""
# ------------------ FILL IN YOUR RESULTS BELOW ------------------
eps_B_L_min = ...
# ---------------------------------------------------------------
return eps_B_L_minproblem description
# Problem setup:
Consider a vector field coupled to the standard model current through . If the vector field makes up all the dark matter, the local dark matter density indicates that the field could exert a measurable force on mirrors in laser interferometers, with sufficiently large coupling. Consider LIGO, with a strain sensitivity of at frequency .
# Main problem:
Take the dark charge to mass radio to be for the inner mirrors, where is the mass of a neutron. We introduce a doped outer mirror, resulting in a differential forced between the inner and outer mirror. We assume the outer mirror gains an additiona , where is the mass of a neutron. With an observation time of years and SNR of , what is the smallest it can probe at ? Provide answers for scenarios where .
Plain-text mathematical notation (without MathML)
# Problem setup:
Consider a vector field A^(μ) coupled to the standard model B−L current J_(B−L)^(μ) through L⊃−ϵ_(B−L)eJ_(B−L)^(μ)A_(μ). If the vector field makes up all the dark matter, the local dark matter density indicates that the field could exert a measurable force on mirrors in laser interferometers, with sufficiently large coupling. Consider LIGO, with a strain sensitivity of 3×10^(−24) Hz^(−1/2) at frequency 250 Hz.
# Main problem:
Take the dark charge Q_(D) to mass M radio to be (Q_(D))/(M)∼(0.5)/(m_(n)) for the inner mirrors, where m_(n) is the mass of a neutron. We introduce a doped outer mirror, resulting in a differential forced between the inner and outer mirror. We assume the outer mirror gains an additiona δ((Q_(D))/(M))∼(δq)/(m_(n)), where m_(n) is the mass of a neutron. With an observation time of 13 years and SNR of 1, what is the smallest ϵ_(B−L) it can probe at 250 Hz? Provide answers for scenarios where δq={0.074,6×10^(−3),5×10^(−4)}.Original LaTeX notation
# Problem setup:
Consider a vector field $A^\mu$ coupled to the standard model $B-L$ current $J^\mu_{B-L}$ through $\mathcal{L}\supset -\epsilon_{B-L}eJ^\mu_{B-L} A_\mu$. If the vector field makes up all the dark matter, the local dark matter density indicates that the field could exert a measurable force on mirrors in laser interferometers, with sufficiently large coupling. Consider LIGO, with a strain sensitivity of $3\times 10^{-24}\, \text{Hz}^{-1/2}$ at frequency $250\,\text{Hz}$.
# Main problem:
Take the dark charge $Q_D$ to mass $M$ radio to be $\frac{Q_D}{M}\sim \frac{0.5}{m_n}$ for the inner mirrors, where $m_n$ is the mass of a neutron. We introduce a doped outer mirror, resulting in a differential forced between the inner and outer mirror. We assume the outer mirror gains an additiona $\delta \left(\frac{Q_D}{M}\right)\sim \frac{\delta q}{m_n}$, where $m_n$ is the mass of a neutron. With an observation time of $13$ years and SNR of $1$, what is the smallest $\epsilon_{B-L}$ it can probe at $250\,\text{Hz}$? Provide answers for scenarios where $\delta q=\{0.074, 6\times 10^{-3}, 5\times 10^{-4}\}$.Discussion
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