Math Problem Statement

For JUST state |ψ3⟩, find the probability that the spin component will be 'up' along the Y-direction. Use bra-ket notation in your calculations.

Solution

The problem asks us to find the probability that the spin component will be "up" along the Y-direction for the given quantum state ψ3|\psi_3\rangle.

Step-by-Step Solution

1. Quantum State of ψ3|\psi_3\rangle

We are given the state ψ3|\psi_3\rangle as:

ψ3=+2eiπ4|\psi_3\rangle = |+\rangle - 2 e^{-i\frac{\pi}{4}} |-\rangle

This is a superposition of the eigenstates +|+\rangle and |-\rangle, which are typically associated with the spin component along the Z-direction.

2. Transformation to Y-basis

To find the probability for the spin component to be "up" along the Y-direction, we need to express ψ3|\psi_3\rangle in terms of the spin-up and spin-down states along the Y-axis, denoted +y|+\rangle_y and y|-\rangle_y.

The Y-basis states can be written in terms of the Z-basis states +|+\rangle and |-\rangle as:

+y=12(++i)|+\rangle_y = \frac{1}{\sqrt{2}} (|+\rangle + i |-\rangle) y=12(+i)|-\rangle_y = \frac{1}{\sqrt{2}} (|+\rangle - i |-\rangle)

3. Expanding ψ3|\psi_3\rangle in Terms of +y|+\rangle_y and y|-\rangle_y

Now, let's express ψ3|\psi_3\rangle in the Y-basis.

ψ3=+2eiπ4|\psi_3\rangle = |+\rangle - 2 e^{-i\frac{\pi}{4}} |-\rangle

Substitute the Z-basis states in terms of the Y-basis states:

[ |\psi_3\rangle = \left[ \frac{1}{\sqrt{2}} (|+\rangle_y + |-\rangle_y) \right] - 2 e^{-i\frac{\pi}{4}} \left[ \frac{1}{\sqrt{2}} (|+\rangle_y - i |-\rangle_y) \right] ]

Simplify the expression by distributing and combining like terms:

ψ3=12+y+12y2eiπ42+y+2ieiπ42y|\psi_3\rangle = \frac{1}{\sqrt{2}} |+\rangle_y + \frac{1}{\sqrt{2}} |-\rangle_y - \frac{2 e^{-i\frac{\pi}{4}}}{\sqrt{2}} |+\rangle_y + \frac{2 i e^{-i\frac{\pi}{4}}}{\sqrt{2}} |-\rangle_y

Now combine the terms with +y|+\rangle_y and y|-\rangle_y:

ψ3=12eiπ42+y+1+2ieiπ42y|\psi_3\rangle = \frac{1 - 2 e^{-i\frac{\pi}{4}}}{\sqrt{2}} |+\rangle_y + \frac{1 + 2 i e^{-i\frac{\pi}{4}}}{\sqrt{2}} |-\rangle_y

4. Probability for Spin "Up" Along Y-axis

The probability for the spin to be "up" along the Y-axis is the square of the amplitude of the +y|+\rangle_y term. The amplitude of +y|+\rangle_y is:

12eiπ42\frac{1 - 2 e^{-i\frac{\pi}{4}}}{\sqrt{2}}

Now, compute the probability:

Pup,y=12eiπ422P_{\text{up}, y} = \left| \frac{1 - 2 e^{-i\frac{\pi}{4}}}{\sqrt{2}} \right|^2

First, calculate 12eiπ41 - 2 e^{-i\frac{\pi}{4}}:

eiπ4=12i12e^{-i\frac{\pi}{4}} = \frac{1}{\sqrt{2}} - i \frac{1}{\sqrt{2}}

12(12i12)=12+i21 - 2 \left( \frac{1}{\sqrt{2}} - i \frac{1}{\sqrt{2}} \right) = 1 - \sqrt{2} + i \sqrt{2}

Now, calculate the magnitude squared of this expression:

12+i22=(12)2+(2)2\left| 1 - \sqrt{2} + i \sqrt{2} \right|^2 = (1 - \sqrt{2})^2 + (\sqrt{2})^2

=(12)2+2=(122+2)+2=522= (1 - \sqrt{2})^2 + 2 = (1 - 2\sqrt{2} + 2) + 2 = 5 - 2\sqrt{2}

Finally, the probability is:

Pup,y=5222P_{\text{up}, y} = \frac{5 - 2\sqrt{2}}{2}

Thus, the probability for the spin component to be "up" along the Y-direction is:

Pup,y=5222P_{\text{up}, y} = \frac{5 - 2\sqrt{2}}{2}

Do you need further details or clarifications?

Relative Questions:

  1. What is the significance of the Y-axis in quantum spin measurements?
  2. How can one interpret complex coefficients in quantum superposition?
  3. Why are basis transformations important in quantum mechanics?
  4. What role do Z-basis states play when measuring along different axes?
  5. How do probabilities arise from amplitudes in quantum mechanics?

Tip:

In quantum mechanics, always check that the total probability sums to 1 when calculating probabilities in a given basis.

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Math Problem Analysis

Mathematical Concepts

Quantum Mechanics
Bra-Ket Notation
Quantum Superposition
Complex Numbers

Formulas

|ψ3⟩ = |+⟩ - 2e^(-iπ/4)|-⟩
|+⟩_y = 1/√2 (|+⟩ + i|-⟩)
|-⟩_y = 1/√2 (|+⟩ - i|-⟩)
Probability P_up_y = |Amplitude of |+⟩_y|²
e^(-iπ/4) = cos(π/4) - i sin(π/4)

Theorems

Quantum State Transformation
Probability Amplitude Calculation in Quantum Mechanics

Suitable Grade Level

Undergraduate - Advanced Quantum Mechanics