Show that an expected value of a vacuum state is equal to 1

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The discussion centers on proving that the expected value of a vacuum state equals 1, involving various operators and the vacuum state \(\ket{\phi_0}\). Participants question the validity of the problem, noting that if \(\hat{c}_{-k \downarrow} \ket{\phi_0} = 0\), the expected value would vanish. Clarifications are sought regarding the definitions of the annihilation operators and the vacuum state. Ultimately, it is revealed that the professor made an error in the homework statement, as the last operator should be conjugated for the expected value to equal one. The conclusion confirms that the original formulation would yield a value of zero.
mcas
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Homework Statement
Using the following anticommutator relations of fermionic one-particle operators:
[itex]\{\hat{c}_{k\alpha},\hat{c}_{k'\beta} \}= \{ \hat{c}^\dagger_{k\alpha}, \hat{c}^\dagger_{k'\beta} \} = 0[/itex]
[itex]\{\hat{c}_{k\alpha},\hat{c}^\dagger_{k'\beta} \}=\delta_{kk'}\delta_{\alpha\beta}[/itex]

Show that the expected value for a vacuum state [itex]|\phi_0>[/itex] is:

[itex] <\phi_0| \hat{c}_{-k \downarrow} \hat{c}_{k \uparrow}\hat{c}^\dagger_{k \uparrow}\hat{c}_{-k \downarrow}|\phi_0>=1
[/itex]
Relevant Equations
Given in the homework statement
<br /> \langle \phi_0| \hat{c}_{-k \downarrow} \hat{c}_{k \uparrow}\hat{c}^\dagger_{k \uparrow}\hat{c}_{-k \downarrow}|\phi_0\rangle = \\ \langle \phi_0| - \hat{c}_{k \uparrow} \hat{c}_{-k \downarrow} \hat{c}^\dagger_{k \uparrow}\hat{c}_{-k \downarrow}|\phi_0\rangle = \\ \langle \phi_0| \hat{c}_{k \uparrow} \hat{c}^\dagger_{k \uparrow} \hat{c}_{-k \downarrow}\hat{c}_{-k \downarrow}|\phi_0\rangle = \\ \langle \phi_0|(1- \hat{c}^\dagger_{k \uparrow} \hat{c}_{k \uparrow} ) \hat{c}_{-k \downarrow}\hat{c}_{-k \downarrow}|\phi_0\rangle = \\ \langle \phi_0|\hat{c}_{-k \downarrow}\hat{c}_{-k \downarrow}|\phi_0\rangle - \langle \phi_0|\hat{c}^\dagger_{k \uparrow} \hat{c}_{k \uparrow} \hat{c}_{-k \downarrow}\hat{c}_{-k \downarrow}|\phi_0\rangle<br />

Then I changed \hat{c}^\dagger_{k \uparrow} \hat{c}_{k \uparrow} in the second term to (1- \hat{c}^\dagger_{k \uparrow} \hat{c}_{k \uparrow} ) and the result was \langle \phi_0| \hat{c}_{-k \downarrow} \hat{c}_{k \uparrow}\hat{c}^\dagger_{k \uparrow}\hat{c}_{-k \downarrow}|\phi_0\rangle which is exactly what I sarted from.

I don't know where to go from this so I would really appreciate any help!
 
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Where did you get this problem from?

Are the ##\hat{c}_{k\alpha}## usual annihilation operators?
How is the ##\ket{\phi_0}## state defined?

If ##\ket{\phi_0}## is the usual vacuum defined from the ##\hat{c}## operators then, if I'm not wrong, by definition ##\hat{c}_{-k \downarrow} \ket{\phi_0}=0## and the whole expectation value vanishes. So, either I'm confused by something, or the problem is wrong, or you have extra information that is crucial for solving the problem.
 
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Gaussian97 said:
Where did you get this problem from?

Are the ##\hat{c}_{k\alpha}## usual annihilation operators?
How is the ##\ket{\phi_0}## state defined?

If ##\ket{\phi_0}## is the usual vacuum defined from the ##\hat{c}## operators then, if I'm not wrong, by definition ##\hat{c}_{-k \downarrow} \ket{\phi_0}=0## and the whole expectation value vanishes. So, either I'm confused by something, or the problem is wrong, or you have extra information that is crucial for solving the problem.
It's a problem formulated by my professor.
After you post I contacted him and indeed, he made a mistake in the homework statement, as the last operator \hat{c}_{-k \downarrow} should be conjugated for the expected value to be one. In the original statement, the value will be 0.
Thank you!
 
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