Dirac and Majorana spinors for neutrinos

bubble
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Dirac description
If I well understood a Dirac description for fermions is :
##\Psi_{D}=\Psi_{L}+\Psi_{R}## where ##\Psi_{L}## is the left-chiral spinor and ##\Psi_{R}## the right-chiral spinor.
Each spinor, ##\Psi_{L} ## and ##\Psi_{R}## has 2 components cotrresponding to the particle and antiparticle :
Q1 : Can we write ##\Psi_{L}=(\nu_{L},\bar{\nu}_{R}) ##? and ##\Psi_{R}=(\nu_{R},\bar{\nu}_{L})## ?

Majorana description
The Majorana condition is ##\Psi_{L}=\Psi_{L}^{c}## and ##\Psi_{R}=\Psi_{R}^{c}##.
Q2: is it right ?
If yes, ##\Psi_{M}=\Psi_{L}+\Psi_{R}## can be written as ##\Psi_{M}=\Psi_{L}+\Psi_{R}^{c}=\Psi_{L}+(\Psi_{L})^{c}##
with ##\Psi_{L}=(\nu_{L},\bar{\nu}_{R}) ## and ##(\Psi_{L})^{c}=((\nu_{L})^{c},(\bar{\nu}_{R})^{c}) =(\nu_{R}^{c},\bar{\nu}_{L}^{c})=(\nu_{R},\bar{\nu}_{L})##
So the Majorana field describes the 4 states of the neutrino (##\nu_{L},\bar{\nu}_{R},\nu_{R},\bar{\nu}_{L}##)
Q3: In such notation what is the difference between ##\nu_{L}^{c}## and ##\bar{\nu}_{L} ## ? Majorana condition ##\nu_{L}^{c} = \nu_{L}## can be also written as : ##\bar{\nu}_{L} = \nu_{L}## ?

I realize I am lost between antiparticle notation ##\bar{\nu}## and charge conjugate ##\nu^{c}##
Can you help me ?
 
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Your questions cannot be answered without careful explanation of the notation. Are you using a particular text?

I recommend Srednicki's text (draft version available free from his web page) for a detailed explanation of Weyl, Dirac, and Majorana fields.
 
Thank you, this text is very useful.
But I am still not sure to understand the difference between the fields component and the particle.
For example for the Dirac field where ##\Psi_{D}=\Psi_{L}+\Psi_{R}##, the four components of the field ##\Psi_{D}## are ##\nu_{L},\bar{\nu}_{R},\nu_{R},\bar{\nu}_{L}## or is it something completely different ?
Thank you...
 
bubble said:
Dirac description
If I well understood a Dirac description for fermions is :
##\Psi_{D}=\Psi_{L}+\Psi_{R}## where ##\Psi_{L}## is the left-chiral spinor and ##\Psi_{R}## the right-chiral spinor.
Each spinor, ##\Psi_{L} ## and ##\Psi_{R}## has 2 components
No, \Psi_{L} and \Psi_{R} are 4-component spinors just like \Psi_{D}. Why don’t you work it out yourself? In Dirac representation, you have \gamma_{5} = \left( \begin{array}{cc} 0_{2 \times 2} & I_{2 \times 2} \\ I_{2 \times 2} & 0_{2 \times 2} \end{array} \right) . So, if you write \Psi_{D} = \left( \chi , \phi \right)^{T}, with \chi = \left( \psi_{1} , \psi_{2} \right)^{T} and \phi = \left( \psi_{3} , \psi_{4} \right)^{T}, you find \Psi_{L} = \frac{1}{2} \left( \begin{array}{c} \chi - \phi \\ \phi - \chi \end{array} \right) , \ \ \ \Psi_{R} = \frac{1}{2} \left( \begin{array}{c} \chi + \phi \\ \phi + \chi \end{array} \right) .
corresponding to the particle and antiparticle
Wrong again, Dirac equation has 4 independent solutions, each (massive) solution is given by 4-component spinor. Two of these solutions (spin up: u^{(1)} (p) & spin down: u^{(2)} (p)) represent a (massive) fermion and the other two solutions ( v^{( 1 , 2 )} (p) ) describe the corresponding anti-fermion. The same is true for massless fermions except that the Dirac equation splits into two decoupled equations for the 2-component spinors \chi and \phi : E \chi = - ( \sigma \cdot p ) \chi , E \phi = ( \sigma \cdot p ) \phi . Each one of these equations has 2 independent solutions: one (2-spinor) for E = | p | ( \nu_{L}, if you like), and the other 2-spinor solution is for E = - | p | ( i.e., \bar{\nu}_{R} ) . So, when we say that \chi describes \nu_{L} and \bar{\nu}_{R}, this DOSE NOT mean that \nu_{L} is the first component of \chi and \bar{\nu}_{R} is the second component. No, \nu_{L} and \bar{\nu}_{R} are 2 independent solutions of the SAME equation and each (massless particle) is described by 2-component spinor. Indeed, in the Weyl (chiral) representation, you find \Psi_{L} = ( \chi , 0 )^{T} and \Psi_{R} = ( 0 , \phi )^{T}.
Q1 : Can we write ##\Psi_{L}=(\nu_{L},\bar{\nu}_{R}) ##? and ##\Psi_{R}=(\nu_{R},\bar{\nu}_{L})## ?
What does it mean to pair together 2 independent solutions of the same equation? Is \Psi_{D} ( p ) = \left( u ( p ) , v ( p ) \right)? Does the object ( e^{-} , e^{+} ) make any mathematical sense? No, \Psi_{D} = u^{(1)} , u^{(2)} , v^{(1)} , v^{(2)}, these are four independent 4-component spinors solutions of the Dirac equation.

Sam
 
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