equation_database.inspirehep_Field_1989uq
Functions
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Applications of Perturbative QCD |
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Cross section for \(\gamma^* \to q \bar q\) |
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Differentiated cross section for \(e^+e^- \to q \bar q g\) |
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\(\gamma^* g \to q \bar q\) scattering averaged matrix element |
- equation_database.inspirehep_Field_1989uq.equation_2_1_30(sigma_0=sigma_0, alpha=alpha, e_q=e_q, Q=Q)[source]
Cross section for \(\gamma^* \to q \bar q\)
- Parameters:
sigma_0 – norm cross section
alpha – fine structure constant
e_q – electric charge of the quark
Q – mass of the virtual photon
- Returns:
\(\sigma_{0} = 3 Q \alpha e_{q}^{2}\),
\sigma_{0} = 3 Q \alpha e_{q}^{2}
<apply><eq/><ci><mml:msub><mml:mi>σ</mml:mi><mml:mi>0</mml:mi></mml:msub></ci><apply><times/><cn>3</cn><ci>Q</ci><ci>α</ci><apply><power/><ci><mml:msub><mml:mi>e</mml:mi><mml:mi>q</mml:mi></mml:msub></ci><cn>2</cn></apply></apply></apply>
Eq(sigma_0, 3*Q*alpha*e_q**2)
sigma_0 == 3*Q.*alpha.*e_q.^2
sigma_0 == 3*Q*alpha*e_q^2
(sigma_0 == 3*Q*alpha*e_q**2)
sigma_0 == 3*Q*alpha*pow(e_q, 2)
sigma_0 == 3*Q*alpha*std::pow(e_q, 2)
sigma_0 == 3*Q*alpha*e_q**2
sigma_0 == 3*Q*alpha*e_q.powi(2)
2 sigma_0 = 3*Q*alpha*e_q
2 σ₀ = 3⋅Q⋅α⋅e_q
- equation_database.inspirehep_Field_1989uq.equation_2_3_32(sigma=sigma, sigma_0=sigma_0, alpha_s=alpha_s, x_1=x_1, x_2=x_2)[source]
Differentiated cross section for \(e^+e^- \to q \bar q g\)
- Parameters:
sigma – cross section
sigma_0 – norm cross section
alpha_s – strong coupling constant
x_1 – quark momentum fraction
x_2 – antiquark momentum fraction
- Returns:
\(\frac{\frac{d^{2}}{d x_{2}d x_{1}} \sigma}{\sigma_{0}} = \frac{2 \alpha_{s} \left(x_{1}^{2} + x_{2}^{2}\right)}{3 \pi \left(1 - x_{1}\right) \left(1 - x_{2}\right)}\),
\frac{\frac{d^{2}}{d x_{2}d x_{1}} \sigma}{\sigma_{0}} = \frac{2 \alpha_{s} \left(x_{1}^{2} + x_{2}^{2}\right)}{3 \pi \left(1 - x_{1}\right) \left(1 - x_{2}\right)}
<apply><eq/><apply><divide/><apply><diff/><bvar><ci><mml:msub><mml:mi>x</mml:mi><mml:mi>2</mml:mi></mml:msub></ci><ci><mml:msub><mml:mi>x</mml:mi><mml:mi>1</mml:mi></mml:msub></ci></bvar><ci>σ</ci></apply><ci><mml:msub><mml:mi>σ</mml:mi><mml:mi>0</mml:mi></mml:msub></ci></apply><apply><divide/><apply><times/><cn>2</cn><ci><mml:msub><mml:mi>α</mml:mi><mml:mi>s</mml:mi></mml:msub></ci><apply><plus/><apply><power/><ci><mml:msub><mml:mi>x</mml:mi><mml:mi>1</mml:mi></mml:msub></ci><cn>2</cn></apply><apply><power/><ci><mml:msub><mml:mi>x</mml:mi><mml:mi>2</mml:mi></mml:msub></ci><cn>2</cn></apply></apply></apply><apply><times/><cn>3</cn><pi/><apply><minus/><cn>1</cn><ci><mml:msub><mml:mi>x</mml:mi><mml:mi>1</mml:mi></mml:msub></ci></apply><apply><minus/><cn>1</cn><ci><mml:msub><mml:mi>x</mml:mi><mml:mi>2</mml:mi></mml:msub></ci></apply></apply></apply></apply>
Eq(Derivative(sigma, x_1, x_2)/sigma_0, 2*alpha_s*(x_1**2 + x_2**2)/(3*pi*(1 - x_1)*(1 - x_2)))
Hold[D[sigma, x_1, x_2]]/sigma_0 == (2/3)*alpha_s*(x_1^2 + x_2^2)/(Pi*(1 - x_1)*(1 - x_2))
2 d ---------(sigma) / 2 2\ dx_2 dx_1 2*alpha_s*\x_1 + x_2 / ---------------- = ------------------------ sigma_0 3*pi*(1 - x_1)*(1 - x_2)
2 d ───────(σ) ⎛ 2 2⎞ dx₂ dx₁ 2⋅αₛ⋅⎝x₁ + x₂ ⎠ ────────── = ───────────────────── σ₀ 3⋅π⋅(1 - x₁)⋅(1 - x₂)
- equation_database.inspirehep_Field_1989uq.equation_4_3_20(e=e, e_q=e_q, g_s=g_s, Q=Q, u=u, t=t)[source]
\(\gamma^* g \to q \bar q\) scattering averaged matrix element
- Parameters:
e – electric charge
e_q – electric charge of the quark
g_s – strong coupling constant
Q – mass of the virtual photon
u – Mandelstam variable u
t – Mandelstam variable t
- Returns:
\(2 e^{2} e_{q}^{2} g_{s}^{2} \left(\frac{2 Q^{2} \left(Q^{2} + t + u\right)}{t u} + \frac{t}{u} + \frac{u}{t}\right)\),
2 e^{2} e_{q}^{2} g_{s}^{2} \left(\frac{2 Q^{2} \left(Q^{2} + t + u\right)}{t u} + \frac{t}{u} + \frac{u}{t}\right)
<apply><times/><cn>2</cn><apply><power/><ci>e</ci><cn>2</cn></apply><apply><power/><ci><mml:msub><mml:mi>e</mml:mi><mml:mi>q</mml:mi></mml:msub></ci><cn>2</cn></apply><apply><power/><ci><mml:msub><mml:mi>g</mml:mi><mml:mi>s</mml:mi></mml:msub></ci><cn>2</cn></apply><apply><plus/><apply><divide/><apply><times/><cn>2</cn><apply><power/><ci>Q</ci><cn>2</cn></apply><apply><plus/><apply><power/><ci>Q</ci><cn>2</cn></apply><ci>t</ci><ci>u</ci></apply></apply><apply><times/><ci>t</ci><ci>u</ci></apply></apply><apply><divide/><ci>t</ci><ci>u</ci></apply><apply><divide/><ci>u</ci><ci>t</ci></apply></apply></apply>
2*e**2*e_q**2*g_s**2*(2*Q**2*(Q**2 + t + u)/(t*u) + t/u + u/t)
2*e.^2.*e_q.^2.*g_s.^2.*(2*Q.^2.*(Q.^2 + t + u)./(t.*u) + t./u + u./t)
2*e^2*e_q^2*g_s^2*(2*Q^2*(Q^2 + t + u)/(t*u) + t/u + u/t)
2*e**2*e_q**2*g_s**2*(2*Q**2*(Q**2 + t + u)/(t*u) + t/u + u/t)
2*pow(e, 2)*pow(e_q, 2)*pow(g_s, 2)*(2*pow(Q, 2)*(pow(Q, 2) + t + u)/(t*u) + t/u + u/t)
2*std::pow(e, 2)*std::pow(e_q, 2)*std::pow(g_s, 2)*(2*std::pow(Q, 2)*(std::pow(Q, 2) + t + u)/(t*u) + t/u + u/t)
2*e**2*e_q**2*g_s**2*(2*Q**2*(Q**2 + t + u)/(t*u) + t/u + u/t)
2*e.powi(2)*e_q.powi(2)*g_s.powi(2)*(2*Q.powi(2)*(Q.powi(2) + t + u)/(t*u) + t/u + u/t)
/ 2 / 2 \ \ 2 2 2 |2*Q *\Q + t + u/ t u| 2*e *e_q *g_s *|----------------- + - + -| \ t*u u t/
⎛ 2 ⎛ 2 ⎞ ⎞ 2 2 2 ⎜2⋅Q ⋅⎝Q + t + u⎠ t u⎟ 2⋅e ⋅e_q ⋅gₛ ⋅⎜───────────────── + ─ + ─⎟ ⎝ t⋅u u t⎠