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Solve for m
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Solve for γ_μ
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i\gamma _{μ}∂^{\mu }\psi -m\psi =0
Use the distributive property to multiply i\gamma _{μ}∂^{\mu }-m by \psi .
-m\psi =-i\gamma _{μ}∂^{\mu }\psi
Subtract i\gamma _{μ}∂^{\mu }\psi from both sides. Anything subtracted from zero gives its negation.
\left(-\psi \right)m=-i\gamma _{μ}\psi ∂^{\mu }
The equation is in standard form.
\frac{\left(-\psi \right)m}{-\psi }=-\frac{i\gamma _{μ}\psi ∂^{\mu }}{-\psi }
Divide both sides by -\psi .
m=-\frac{i\gamma _{μ}\psi ∂^{\mu }}{-\psi }
Dividing by -\psi undoes the multiplication by -\psi .
m=i\gamma _{μ}∂^{\mu }
Divide -i\gamma _{μ}∂^{\mu }\psi by -\psi .
i\gamma _{μ}∂^{\mu }\psi -m\psi =0
Use the distributive property to multiply i\gamma _{μ}∂^{\mu }-m by \psi .
i\gamma _{μ}∂^{\mu }\psi =m\psi
Add m\psi to both sides. Anything plus zero gives itself.
i\psi ∂^{\mu }\gamma _{μ}=m\psi
The equation is in standard form.
\frac{i\psi ∂^{\mu }\gamma _{μ}}{i\psi ∂^{\mu }}=\frac{m\psi }{i\psi ∂^{\mu }}
Divide both sides by i∂^{\mu }\psi .
\gamma _{μ}=\frac{m\psi }{i\psi ∂^{\mu }}
Dividing by i∂^{\mu }\psi undoes the multiplication by i∂^{\mu }\psi .
\gamma _{μ}=-\frac{im}{∂^{\mu }}
Divide m\psi by i∂^{\mu }\psi .