Graduate Question on Zeno time derivation

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The discussion centers on difficulties in understanding the derivation of Zeno time from two academic papers. The original poster struggles with the algebraic steps in both sources, particularly in connecting equations (4) and (5) to equation (6) in the first paper, and understanding equation (1.3) in the second paper. They express confusion over the presence of an epsilon squared term and the overall algebraic manipulation. A helpful response clarifies the relationships between projectors and provides insight into the calculations, ultimately aiding in the understanding of the Zeno time derivation. The exchange highlights the complexities of quantum mechanics and the importance of clear mathematical reasoning in theoretical physics.
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Hi,

I'm trying to follow the derivation of the Zeno time from two sources and am struggling. I think I'm missing some sort of algebraic trick and any tips would be appreciated. A bit more detail below.

In the attached paper \citep{Facchi_2008}, the Zeno time (equation (6)) is derived from equation (4) and equation (5), but I don't see how.

1705786258003.png


In the second attached paper \citep{PhysRevA.89.042116}, the Zeno time is derived in equation (1.6) though I cannot even see how how equation (1.3) is derived (let alone the Zeno time).

1705786470408.png
REFERENCES

@article{Facchi_2008,
doi = {10.1088/1751-8113/41/49/493001},
url = {https://dx.doi.org/10.1088/1751-8113/41/49/493001},
year = {2008},
month = {oct},
publisher = {},
volume = {41},
number = {49},
pages = {493001},
author = {P Facchi and S Pascazio},
title = {Quantum Zeno dynamics: mathematical and physical aspects},
journal = {Journal of Physics A: Mathematical and Theoretical},
}

@article{PhysRevA.89.042116,
title = {Classical limit of the quantum Zeno effect by environmental decoherence},
author = {Bedingham, D. and Halliwell, J. J.},
journal = {Phys. Rev. A},
volume = {89},
issue = {4},
pages = {042116},
numpages = {17},
year = {2014},
month = {Apr},
publisher = {American Physical Society},
doi = {10.1103/PhysRevA.89.042116},
url = {https://link.aps.org/doi/10.1103/PhysRevA.89.042116}
}
 

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Hint: ##P## and ##Q## are projectors, i.e. ##P^2=P##, ##Q^2=Q##, ##PQ=QP=0##.
 
Demystifier said:
Hint: ##P## and ##Q## are projectors, i.e. ##P^2=P##, ##Q^2=Q##, ##PQ=QP=0##.

Thank you very much for your reply. I did try using those relationships (and I understand why they are true), however, I still could not get the algebra to work.

Furthermore, in equation (1.3) of the below extract frrom \citep{PhysRevA.89.042116}, I cannot even see how the ##\epsilon^2## term on the RHS of the equation (1.3) is possible. The reason for this is that I believe any ##\epsilon^2## term on the LHS would be of the form ##\frac{\epsilon^2}{\hbar^2}##.

This, together with my inability to get the algebra to match, led me to believe I am missing something else fundamental.
1705827783054.png
 
Mainframes said:
Thank you very much for your reply. I did try using those relationships (and I understand why they are true), however, I still could not get the algebra to work.
First observe that from ##P=|\psi_0\rangle\langle\psi_0|## we have
$$P|\psi_0\rangle = |\psi_0\rangle , \;\;\; Q|\psi_0\rangle = 0.$$
The goal is to compute
$$\tau_Z^{-2} = \langle\psi_0|H^2| \psi_0\rangle - \langle\psi_0|H| \psi_0\rangle^2.$$
The second term is proportional to
$$\langle\psi_0|H| \psi_0\rangle^2=
\langle\psi_0|H| \psi_0\rangle \langle\psi_0|H| \psi_0\rangle
= \langle\psi_0|HPH| \psi_0\rangle ,$$
while the first term is
$$\langle\psi_0|H^2| \psi_0\rangle = \langle\psi_0| PH(Q+P)HP | \psi_0\rangle$$
$$=\langle\psi_0| PHQHP | \psi_0\rangle + \langle\psi_0| PHPHP | \psi_0\rangle$$
$$=\langle\psi_0| PHQQHP | \psi_0\rangle + \langle\psi_0| HPH | \psi_0\rangle$$
$$=\langle\psi_0| H_{int}^2 | \psi_0\rangle + \langle\psi_0| H | \psi_0\rangle^2 .$$
Combining all this we get
$$\tau_Z^{-2} = \langle\psi_0| H_{int}^2 | \psi_0\rangle$$
which is Eq. (6).
 
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Demystifier said:
First observe that from ##P=|\psi_0\rangle\langle\psi_0|## we have
$$P|\psi_0\rangle = |\psi_0\rangle , \;\;\; Q|\psi_0\rangle = 0.$$
The goal is to compute
$$\tau_Z^{-2} = \langle\psi_0|H^2| \psi_0\rangle - \langle\psi_0|H| \psi_0\rangle^2.$$
The second term is proportional to
$$\langle\psi_0|H| \psi_0\rangle^2=
\langle\psi_0|H| \psi_0\rangle \langle\psi_0|H| \psi_0\rangle
= \langle\psi_0|HPH| \psi_0\rangle ,$$
while the first terms is
$$\langle\psi_0|H^2| \psi_0\rangle = \langle\psi_0| PH(Q+P)HP | \psi_0\rangle$$
$$=\langle\psi_0| PHQHP | \psi_0\rangle + \langle\psi_0| PHPHP | \psi_0\rangle$$
$$=\langle\psi_0| PHQQHP | \psi_0\rangle + \langle\psi_0| HPH | \psi_0\rangle$$
$$=\langle\psi_0| H_{int}^2 | \psi_0\rangle + \langle\psi_0| H | \psi_0\rangle^2 .$$
Combining all this we get
$$\tau_Z^{-2} = \langle\psi_0| H_{int}^2 | \psi_0\rangle$$
which is Eq. (6).
This is brilliant. Thank you so much for this (it has certainly Demystified the result to me)
 
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