91影视

In quantum physics, eigen spinors are considered basis vectors that represent a particle's general spin state. They are not vectors in the strictest sense, but rather spinors.

The probability formula states that the ratio of the number of favorable outcomes to the total number of alternatives equals the likelihood of an event occurring.

Use equations. 4.151 and 4.163 that are mentioned as follows,

$$\begin{gathered} {蠂}_{+}^{\left(x\right)}=\left(\begin{array}{c}\frac{1}{\sqrt{2}}\\ \frac{1}{\sqrt{2}}\end{array}\right),\left(eigenvalue+\frac{鈩�}{2}\right) \\ {蠂}_{+}^{\left(x\right)}\left(\begin{array}{c}\frac{1}{\sqrt{2}}\\ \frac{1}{\sqrt{2}}\end{array}\right),\left(eigenvalue-\frac{鈩�}{2}\right) \end{gathered}$$

The generic spinor x (Equation 4.139) can be written as a linear combination since the eigenvectors of a hermitian matrix, they span the space.

$x=\left(\frac{a+b}{\sqrt{2}}\right)x_{+}^{\left(x\right)}+\left(\frac{a-b}{\sqrt{2}}\right)x_{-}^{\left(x\right)}$

Determine the value of $\overline{)x)}$.

$\overline{)x)=\left(\begin{array}{cc}\cos \frac{伪}{2}& e^{i纬B_0\frac{1}{2}}\\ \sin \frac{伪}{2}& e^{-i纬B_0\frac{1}{2}}\end{array}\right)}$

Find the value of probability,$P_{+}^x$.

localid="1659017003900" $$\begin{gathered} P_{+}^x={\left|\left(x_{+}^x|x\right)\right|}^2 \\ =\frac{1}{2}\left|\left(11\right)\left(\begin{array}{cc}\cos \frac{伪}{2}& e^{iy{B}_0\frac{1}{2}}\\ \sin \frac{伪}{2}& e^{-i7y{B}_0\frac{f}{2}}\end{array}\right)\right| \\ =\frac{1}{2}\left[\cos \frac{伪}{2}{e}^{iy{B}_0\frac{t}{2}}+\sin \frac{伪}{2}{e}^{iy{B}_0\frac{t}{2}}\right]脳\left[\cos \frac{伪}{2}{e}^{iy{B}_0\frac{t}{2}}+\sin \frac{伪}{2}{e}^{-iy{B}_0\frac{t}{2}}\right] \\ =\frac{1}{2}\left[{\cos }^2\frac{伪}{2}+\sin \frac{伪}{2}+\cos \frac{伪}{2}\sin \frac{伪}{2}\left(e^{iy{B}_0}+e^{-iy{B}_0}\right)\right] \end{gathered}$$

Evaluate the above expression further.

$$\begin{gathered} P_{+}^x=\frac{1}{2}\left[1+2\sin \frac{伪}{2}\cos \frac{伪}{2}\cos \left(纬B_{0}t\right)\right] \\ {P}_{+}^x\left(t\right)=\frac{1}{2}\left[1+\sin 伪\cos \left(纬B_{0}t\right)\right] \end{gathered}$$

Thus, the probability along -direction is $\frac{1}{2}\left[1+\sin 伪\cos \left(纬B_{0}t\right)\right]$.

From part a ofProblem 4.32,

$x_{+}^{\left(y\right)}=\frac{1}{\sqrt{2}}\left(\begin{array}{c}1\\ i\end{array}\right)$

Substitute the above value in $c_{+}^{\left(y\right)}=x_{+}^{\left(y\right)鈹�}x$.

$$\begin{gathered} c_{+}^{\left(y\right)}=x_{+}^{\left(y\right)鈹�}x \\ =\frac{1}{\sqrt{2}}\left(1-i\right)\left(\begin{array}{c}\cos \frac{伪}{2}{e}^{iy{B}_{0}t/2}\\ \sin \frac{伪}{2}{e}^{-iy{B}_{0}t/2}\end{array}\right) \\ =\frac{1}{\sqrt{2}}\left[\cos \frac{伪}{2}{e}^{iy{B}_{0}t/2}-i\sin \frac{伪}{2}{e}^{-iy{B}_{0}t/2}\right] \end{gathered}$$

Determine the value of the probability, $P_{+}^y$.

$$\begin{gathered} P_{+}^x={\left|\left(x_{+}^x\right|x)\right|}^2 \\ =\frac{1}{2}\left|\left(1-i\right)\left(\begin{array}{c}\cos \frac{伪}{2}{e}^{i-B_0\frac{1}{2}}\\ \sin \frac{伪}{2}{e}^{-17}{B}_0\frac{1}{2}\end{array}\right)\right| \\ =\frac{1}{2}\left[{\cos }^2\frac{伪}{2}+{\sin }^2\frac{伪}{2}+i\sin \frac{伪}{2}\cos \frac{伪}{2}\left(e^{iy-B_{0}t}-e^{-i-y{B}_{0}t}\right)\right] \\ =\frac{1}{2}\left[1-2\sin \frac{伪}{2}\cos \frac{伪}{2}\sin \left(纬B_{0}t\right)\right] \\ {P}_{+}^y\left(t\right)=\frac{1}{2}\left[1-\sin 伪\sin \left(纬B_{0}t\right)\right] \end{gathered}$$

Thus, the probability along -direction is $\frac{1}{2}\left[1-\sin 伪\sin \left(纬B_{0}t\right)\right]$.

The normalized eigen spinors for is as follows,

$$\begin{gathered} x_{+}^{\left(z\right)}=\left(\begin{array}{c}1\\ 0\end{array}\right) \\ {c}_{+}^{\left(z\right)}=\left(\begin{array}{cc}1& 0\end{array}\right)\left(\begin{array}{c}\cos \frac{伪}{2}{e}^{iy{B}_{0}t/2}\\ \sin \frac{伪}{2}{e}^{-iy{B}_{0}t/2}\end{array}\right) \\ =\cos \frac{伪}{2}{e}^{-iy{B}_{0}t/2} \end{gathered}$$

Determine the value of the probability,$P_{+}^{\left(z\right)}$.

$$\begin{gathered} P_{+}^{\left(z\right)}\left(t\right)={\left|c_{+}^{\left(z\right)}\right|}^2 \\ ={\cos }^2\frac{伪}{2} \end{gathered}$$

Hence, the probability along z-direction is ${\cos }^2\frac{伪}{2}$.