Why Use Different Components for E>0 and E<0 in Dirac Equation?

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    Dirac Dirac equation
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SUMMARY

The discussion focuses on the use of different components in the Dirac equation for energy states E>0 and E<0. For E>0, the bispinor components are represented as $$\phi_p = \begin{pmatrix} 1 \\ 0 \end{pmatrix}$$ or $$\begin{pmatrix} 0 \\ 1 \end{pmatrix}$$, while for E<0, the components are denoted as $$\chi_p = \begin{pmatrix} 1 \\ 0 \end{pmatrix}$$ or $$\begin{pmatrix} 0 \\ 1 \end{pmatrix}$$. The distinction arises from the properties of the $$\beta$$ matrix, which influences the eigenvalues corresponding to positive and negative energy states. Additionally, the conversion of $$\phi_p = \frac{c \sigma \cdot p}{E_p - mc^2} x_p$$ to $$\frac{-c \sigma \cdot p}{|E_p| + mc^2} x_p$$ involves recognizing that $$|E_p|$$ denotes the absolute value of the energy.

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TimeRip496
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I just started learning this so I am a bit lost. This is where I am lost http://www.nyu.edu/classes/tuckerman/quant.mech/lectures/lecture_7/node1.html .

Why when E>0, we use $$\phi_p=
\begin{pmatrix}
1 \\
0 \\
\end{pmatrix}
$$ or $$
\begin{pmatrix}
0 \\
1 \\
\end{pmatrix}
$$

while when E<0, we use this instead
$$x_p=
\begin{pmatrix}
1 \\
0 \\
\end{pmatrix}
$$ or $$
\begin{pmatrix}
0 \\
1 \\
\end{pmatrix}
$$
where ∅p is the upper component while xp is the lower component of the bispinor in Dirac equation.
Can we do it the other way round or
$$\phi_p=
\begin{pmatrix}
1 \\
0 \\
0 \\
0 \\
\end{pmatrix}
...$$ instead?Secondly, how did the author convert $$\phi_p = \frac{c \sigma .p}{E_p -mc^2}x_p=?=\frac{-c \sigma .p}{|E_p| +mc^2}x_p$$? Does the mod sign means anything?

Can someone help me or point me in the right direction cause this is my first time learning this. Thanks a lot!
 
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TimeRip496 said:
Why when E>0, we use

$$\phi_p= \begin{pmatrix}

1 \\

0 \\

\end{pmatrix}
or
\begin{pmatrix}

0 \\

1 \\

\end{pmatrix}
$$
while when E<0, we use this instead
$$\chi_p=\begin{pmatrix}

1 \\

0 \\

\end{pmatrix}
or
\begin{pmatrix}

0 \\

1 \\

\end{pmatrix}
$$

where ∅p is the upper component while xp is the lower component of the bispinor in Dirac equation.

Can we do it the other way round ... ?

It's because of the ##\beta## matrix (as it's called in the notation you're using, from Dirac; see lesson 6). The top two rows are +1 (on the diagonal), the bottom two -1. The corresponding eigenvalues are pos and neg, obviously, when setting the momentum to zero, as shown in lesson 7. If you wrote the ##\beta## matrix "the other way round" then the E>0 and E<0 cases would also be switched, that is, ##\phi_p## and ##\chi_p## would play opposite roles. There are many other valid ways to write ##\beta## and ##\alpha## matrix (called "representations") all physically equivalent. BTW that second component is "chi" not "x".

TimeRip496 said:
or $$\phi_p=\begin{pmatrix}

1 \\

0 \\

0 \\

0 \\

\end{pmatrix}
...$$ instead?

In my answer above I assumed you meant, can we switch the roles of ##\phi_p## (E>0) and ##\chi_p## (E<0), and ignored this. For one thing ##\phi_p## is a 2-vector not 4 but even if you meant ##u_p## it still doesn't make sense, AFAIK.

TimeRip496 said:
Secondly, how did the author convert $$\phi_p = \frac{c \sigma .p}{E_p -mc^2}x_p=?=\frac{-c \sigma .p}{|E_p| +mc^2}x_p$$? Does the mod sign means anything?

The term ##|E_p|## is not a mod but an absolute value, since ##E_p## is just a real number. So you get the RHS simply by multiplying LHS numerator and denominator each by -1, remembering that ##E_p## is negative in this case.
 
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