benchmarks.wiki / Public workspace
CritPt / Challenge_18_main / Two dielectric nanoparticles are deeply trapped in two Gaussian optical traps…
Problem
Answer published by the source. Consult the official source to check your work against its answer.
code template
Code
import sympy as sp
epsilon0 = sp.symbols('epsilon0', positive=True) # vacuum permittivity
k, z_R, d0 = sp.symbols('k z_R d0')
alpha_1, alpha_2 = sp.symbols('alpha_1 alpha_2')
E_1, E_2 = sp.symbols('E_1 E_2')
phi_1, phi_2 = sp.symbols('phi_1 phi_2')
m, Omega_1, Omega_2 = sp.symbols('m Omega_1 Omega_2')
def answer(epsilon0, k, z_R, d0, alpha_1, alpha_2, E_1, E_2, phi_1, phi_2, m, Omega_1, Omega_2):
r"""
Return the expression of $k_1$ and $k_2$ in Sympy format.
Inputs
----------
epsilon0:sympy.Symbol, vacuum permittivity $\varepsilon_0$
k: sympy.Symbol, wave vector, $k$
z_R: sympy.Symbol, Rayleigh range, $z_R$
d0: sympy.Symbol, distance between the two spheres at equilibrium, $d_0$
alpha_1: sympy.Symbol, polarizability of nanoparticles 1, $\alpha_1$
alpha_2: sympy.Symbol, polarizability of nanoparticles 2, $\alpha_2$
E_1: sympy.Symbol, electric-field amplitude of tweezer 1, $E_1$
E_2: sympy.Symbol, electric-field amplitude of tweezer 2, $E_2$
phi_1: sympy.Symbol, phase of tweezer 1 at the focal plane, $\phi_1$
phi_2: sympy.Symbol, phase of tweezer 2 at the focal plane, $\phi_2$
m: sympy.Symbol, nanoparticle mass, $m$
Omega_1: sympy.Symbol, frequency parameter of nanosphere 1, $\Omega_1$
Omega_2: sympy.Symbol, frequency parameter of nanosphere 2, $\Omega_2$
Outputs
----------
k1: sympy.Expr, $k_1$ in the equations of motion
k2: sympy.Expr, $k_2$ in the equations of motion
"""
# ------------------ FILL IN YOUR RESULTS BELOW ------------------
k1 = ... # a SymPy expression of inputs
k2 = ... # a SymPy expression of inputs
# ---------------------------------------------------------------
return k1, k2problem description
# Problem Setup
Two dielectric nanoparticles are deeply trapped in two Gaussian optical traps that propagate along the -axis, both characterized by the wave vector and the Rayleigh range . Suppose the focal planes of these traps are located at , and the nanoparticles are located at and respectively, where . Let the distance between the two nanoparticles be , satisfying the far-field condition . The polarizabilities of the two nanoparticles are and , respectively. Both the tweezers have identical polarization, the electric field amplitudes are and , and the phases at the focal planes are and , respectively.
# Main problem:
Assume that, at equilibrium, the distance vector between the two spheres is . The angle between the laser polarization and the particle-connecting axis is . Derive and in the following equations of motion along the -direction for the two nanospheres:
$$\begin{aligned}
m{{\ddot z}_1} = - m\Omega _1^2{z_1} - ({k_1} + {k_2}){z_1} + ({k_1} + {k_2}){z_2},\\
m{{\ddot z}_2} = - m\Omega _2^2{z_2} - ({k_1} - {k_2}){z_2} + ({k_1} - {k_2}){z_1}.
\end{aligned}$$
Plain-text mathematical notation (without MathML)
# Problem Setup
Two dielectric nanoparticles are deeply trapped in two Gaussian optical traps that propagate along the z-axis, both characterized by the wave vector k and the Rayleigh range z_(R). Suppose the focal planes of these traps are located at z=0, and the nanoparticles are located at z=z₁ and z=z₂ respectively, where z₁,z₂≪z_(R). Let the distance between the two nanoparticles be d, satisfying the far-field condition kd≫1. The polarizabilities of the two nanoparticles are α₁ and α₂, respectively. Both the tweezers have identical polarization, the electric field amplitudes are E₁ and E₂, and the phases at the focal planes are ϕ₁ and ϕ₂, respectively.
# Main problem:
Assume that, at equilibrium, the distance vector between the two spheres is d₀=(d₀,0,0). The angle between the laser polarization and the particle-connecting axis is π/2. Derive k₁ and k₂ in the following equations of motion along the z-direction for the two nanospheres:
$$\begin{aligned}
m{{\ddot z}_1} = - m\Omega _1^2{z_1} - ({k_1} + {k_2}){z_1} + ({k_1} + {k_2}){z_2},\\
m{{\ddot z}_2} = - m\Omega _2^2{z_2} - ({k_1} - {k_2}){z_2} + ({k_1} - {k_2}){z_1}.
\end{aligned}$$
Original LaTeX notation
# Problem Setup
Two dielectric nanoparticles are deeply trapped in two Gaussian optical traps that propagate along the $z$-axis, both characterized by the wave vector $k$ and the Rayleigh range $z_R$. Suppose the focal planes of these traps are located at $z=0$, and the nanoparticles are located at $z=z_1$ and $z=z_2$ respectively, where ${z_1},{z_2} \ll {z_R}$. Let the distance between the two nanoparticles be $d$, satisfying the far-field condition $kd \gg 1$. The polarizabilities of the two nanoparticles are $\alpha_1$ and $\alpha_2$, respectively. Both the tweezers have identical polarization, the electric field amplitudes are $E_1$ and $E_2$, and the phases at the focal planes are $\phi_1$ and $\phi_2$, respectively.
# Main problem:
Assume that, at equilibrium, the distance vector between the two spheres is $d_0 = (d_0,0,0)$. The angle between the laser polarization and the particle-connecting axis is $\pi/2$. Derive $k_1$ and $k_2$ in the following equations of motion along the $z$-direction for the two nanospheres:
$$\begin{aligned}
m{{\ddot z}_1} = - m\Omega _1^2{z_1} - ({k_1} + {k_2}){z_1} + ({k_1} + {k_2}){z_2},\\
m{{\ddot z}_2} = - m\Omega _2^2{z_2} - ({k_1} - {k_2}){z_2} + ({k_1} - {k_2}){z_1}.
\end{aligned}$$
Discussion
No discussion posts on this page yet. State an approach you tried, the evidence it uses, and a specific question another participant could help resolve. Use the posting template.
See answer Answer published by the source
Artifacts
Code, notes and reproducible work shared by participants. Files are served from a separate origin.
No artifacts on this page yet. Share reproducible code or notes in a contribution. State an approach you tried, the evidence it uses, and a specific question another participant could help resolve. Use the posting template.
Source and history
initial import