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}}=\left|{\begin{matrix}\kappa &\lambda &\mu \\\xi &o&\rho \\\zeta &\eta &\theta \end{matrix}}\right|;\qquad {\bar {\beta }}=\left|{\begin{matrix}\lambda &\mu &\iota...

alpha α iota ι rho ρ beta β kappa κ sigma σ gamma γ lambda λ tau τ delta δ mu μ upsilon υ epsilon ϵ nu ν phi ϕ zeta ζ xi ξ chi χ eta η omicron o psi ψ...

ι kappa κ lambda λ mu μ nu ν xi ξ pi π piv ϖ rho ρ sigma σ sigmaf ς tau τ upsilon υ phi φ chi χ psi ψ omega ω Gamma Γ Delta Δ Theta Θ Lambda Λ Xi Ξ Pi...

t 2 ) ( 1 − κ 2 t 2 ) . {\displaystyle u=\int _{0}^{\xi }{\frac {dt}{\sqrt {(1-t^{2})(1-\kappa ^{2}t^{2})}}}.} The following rational approximation problem...

{\displaystyle \kappa \in \mathbb {R} ^{d}} . Since μ ( κ ) = 0 {\displaystyle \mu (\kappa )=0} would mean that ‖ ξ − x l ‖ → 0 , l → ∞ {\displaystyle \|\xi -x_{l}\|\to...

Digamma 6) Ζζ Zeta 7 Ηη Eta 8 Θθ Theta 9 Ιι Iota 10 Κκ Kappa 20 Λλ Lambda 30 Μμ Mu 40 Νν Nu 50 Ξξ Xi 60 Οο Omicron 70 Ππ Pi 80 (Ϟϟ Qoppa 90) Ρρ Rho 100 Σσς...

\cos(\lambda )-\xi \sin(\lambda )={\frac {x'\eta -y'\xi }{\sqrt {x'^{2}+y'^{2}}}}} ; and w T 2 + w N 2 = ξ 2 + η 2 {\displaystyle w_{T}^{2}+w_{N}^{2}=\xi ^{2}+\eta...

{\begin{matrix}{\tilde {\kappa }}&=&\kappa \left(l,m\right)-\lambda (El_{2}+2Flm+Nm^{2}),&\Downarrow {\frac {\partial {\tilde {\kappa }}}{\partial l}}={\frac...

q 1 … ( x − λ ℓ ) q ℓ {\displaystyle \left|T_{1}-xI\right|=(x-\lambda _{1})^{q_{1}}\dots (x-\lambda _{\ell })^{q_{\ell }}} and | T 2 − x I | = ( x − λ...

{\displaystyle \kappa \in \mathbb {R} ^{d}} . Since μ ( κ ) = 0 {\displaystyle \mu (\kappa )=0} would mean that ‖ ξ − x l ‖ → 0 , l → ∞ {\displaystyle \|\xi -x_{l}\|\to...

epsilon= EPS zeta = ZET eta = ETA theta= TET iota = IOT kappa = KAP lambda= LAM mu = MU nu = NU xi = XI omicron= OMI pi = PI rho = RHO sigma= SIG tau = TAU...

{\displaystyle Q^{\kappa }:=(q_{1}^{k_{1}},\ldots ,q_{r}^{k_{r}})} . Let n = ( P κ ) 1 = p 1 k 1 ⋯ p r k r {\displaystyle n=(P^{\kappa })^{1}=p_{1}^{k_{1}}\cdots...

and Beta are just "A" and "B", respectively). Lowercase epsilon, theta, kappa, phi, pi, rho, and sigma are provided in two different versions. The alternate...

{\displaystyle c={\sqrt {{\kappa \cdot p} \over \rho }}} which using the ideal gas law is identical to: c = κ ⋅ R ⋅ T {\displaystyle c={\sqrt {\kappa \cdot R\cdot T}}}...

} κ {\displaystyle \kappa } kappa Spring constant Dielectric constant Λ {\displaystyle \Lambda } λ {\displaystyle \lambda } lambda Wavelength Thermal conductivity...

{\begin{aligned}h\in \ker \Phi &\Leftrightarrow h=\kappa \iota ,\kappa \in K,\iota \in I\\&\Leftrightarrow h=\kappa \iota ,\kappa \in K,\iota \in H\cap I\\&\Leftrightarrow...

ι kappa κ lambda λ mu μ nu ν xi ξ pi π piv ϖ rho ρ sigma σ sigmaf ς tau τ upsilon υ phi φ chi χ psi ψ omega ω Gamma Γ Delta Δ Theta Θ Lambda Λ Xi Ξ Pi...

} κ {\displaystyle \kappa } kappa Spring constant Dielectric constant Λ {\displaystyle \Lambda } λ {\displaystyle \lambda } lambda Wavelength Thermal conductivity...

\iota } Iota K , κ {\displaystyle \mathrm {K} ,\kappa } Kappa Λ , λ {\displaystyle \Lambda ,\lambda } Lambda M , μ {\displaystyle \mathrm {M} ,\mu } Mu N...

I {\displaystyle I} Kappa κ {\displaystyle \kappa } K {\displaystyle K} Lambda λ {\displaystyle \lambda } Λ {\displaystyle \Lambda } Mu μ {\displaystyle...