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2 votes

Correlation functions zero for repeated creation or annihilation operators

Okey, the zero has to come from computing the trace $$ {\rm Tr}(R_0 b_j^\dagger b_k^\dagger)=0, $$ but I don't see easily why this is the case. Here $R_0$ is the density matrix of the bath composed ...
hft's user avatar
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1 vote

Translation operators and positive-semidefinite condition

Your working looks correct, but there is a much simpler approach. It is easy to see that your operator is unitary. This implies that it has a complete set of eigenstates. Furthermore all its ...
By Symmetry's user avatar
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1 vote

Coordinate-free calculations in bra-ket notation

I'm interested if bra-ket notation can be used without having to introduce a basis or coordinates in calculations and proofs. If you are asking if it can be used without a basis, yes, it can. There ...
hft's user avatar
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4 votes

Question about the identity operator and the bosonic ladder operators

The answer is no. Below I give a proof for the $n=1$ case that the only operators obeying these constraints are of the form $$B=b P_1+ b^{-1} P_2 \quad , \tag 1$$ where $P_1=\sum\limits_{n=0}^\infty |...
Tobias Fünke's user avatar
3 votes

Question about the identity operator and the bosonic ladder operators

I am a bit confused by your condition that $B$ should be self-adjoint, which would mean $B^{\dagger}=B$. I suspect you meant that $B$ was to be unitary, $B^{\dagger}=B^{-1}$. However, it seems to ...
Buzz's user avatar
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1 vote

Where does the complex conjugate term generally come from in a Hamiltonian?

This type of Hamiltonian is a second quantisation one. The most important part is defining your operators $a$ and $a^\dagger$. For example, if you have two interacting dipoles the interaction energy ...
Olivier Masset's user avatar
4 votes
Accepted

Where does the complex conjugate term generally come from in a Hamiltonian?

The simplest justification is probably that the Hamiltonian has to be Hermitian. After all, its eigenvalues are interpreted as the possible energies of the system, and hence they need to be real. This ...
Níckolas Alves's user avatar
9 votes
Accepted

Determining Bound States from Møller Operator

If $H=H_0+V$, where $V$ is a so-called Kato potential, then the point spectrum of $H$ corresponds to the bound states, while the scattering states correspond to the continuous spectrum (Ruelle's ...
Tobias Fünke's user avatar
1 vote

Why does the Pauli objection not disqualify the existence of the position operator?

According to the Pauli objection (see for example here or the answer to this question) there can be no time operator $\hat{T}$ canonically conjugate to the Hamiltonian $\hat{H}$ of a physical system ...
hft's user avatar
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2 votes
Accepted

Equivalent definitions of Wick ordering

For what it's worth, given a family $(\hat{A}_i)_{i\in I}$ of operators $\hat{A}_i\in{\cal A}$ in a (super) operator algebra ${\cal A}$ there seems to be an implicit/tacit assumption that the $n$th ...
Qmechanic's user avatar
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3 votes

What are single-, double- and multi-trace operators in AdS/CFT?

Briefly speaking, on the CFT boundary side of the holographic principle/AdS-CFT correspondence, there is a (super) YM theory with an $SU(N)$ color group. A boundary observable ${\cal O}(x)$ [build ...
Qmechanic's user avatar
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2 votes

Pauli matrix exponentials

am I correct that it follows that $e^{-i\frac{\theta}{2}\hat{X}}|+\rangle = e^{-i\frac{\theta}{2}}|+\rangle$ and $e^{-i\frac{\theta}{2}\hat{X}}|-\rangle = e^{i\frac{\theta}{2}}|-\rangle$ since $\hat{X}...
hft's user avatar
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0 votes

Choice of spacetime foliation while quantising a conformal field theory

A Hilbert space is assigned to a foliation of the manifold. More precisely, we assign a Hilbert space to every slice in the foliation. The Hilbert spaces on two different slices in the same foliation ...
Prahar's user avatar
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2 votes

Exercise on self-adjointness of Hamiltonian

Thanks to @ZeroTheHero who brought me onto the right track, I was able to find the solution to the problem myself. The Hamiltonian with respect to the basis $\{ | \psi \rangle, |\phi \rangle, |\Gamma\...
Octavius's user avatar
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2 votes

How do we know at the operator-level that the tadpole $\langle\Omega|\phi(x)|\Omega\rangle=0$ vanishes in scalar $\phi^4$ theory?

I think you are basically there: Let $\hat{U}$ be the unitary operation you defined, $\hat{U} \hat{\phi}(x) \hat{U}^\dagger \equiv -\hat{\phi}(x)$. This is a definition. We then assume (or check) that ...
Lucas Baldo's user avatar
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-1 votes

Extracting the dimension of an operator from algebra

Can we extract the dimension of $P$ and $K$ from the commutation relations? The answer is no as, dimensionally, $P$ and $K$ cancel out of those equations.
lcv's user avatar
  • 1,965
2 votes

Extracting the dimension of an operator from algebra

Yes, the dila(ta)tion operator $D/i=x^{\mu} \partial_{\mu}$ is a Euler vector field that literally counts the length dimension for operators made from only $x^{\nu}$ and $\partial_{\lambda}$.
Qmechanic's user avatar
  • 202k
0 votes

Generator of two-qubit quantum gate

I'm not sure I fully understood your question, but the thing you exponentiate to get a controlled $Y$ gate, $$ \mathsf{CY} = \frac{1}{2} \left( \mathbb{1} \otimes \mathbb{1} + Z \otimes \mathbb{1} + \...
just a phase's user avatar
0 votes

Dictionary between interpretations of field operators

Perhaps there is a simple confusion. As you may notice yourself your points 1. and 2. are not compatible with each other. What you can say is that the quantization of a real scalar field is given by ...
lcv's user avatar
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2 votes
Accepted

Dictionary between interpretations of field operators

Assuming that you are interested in the physical interpretation of the hermitean field operator of a free relativistic scalar theory in the Heisenberg picture, its Fourier decomposition (omitting the ...
Hyperon's user avatar
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0 votes

Total momentum operator of the Klein-Gordon field (before limit to the continuum)

When you related the quadrature operator $q$ to the ladder operators $a$'s in the "solution," there is an implied commutation relation for the ladder operators that you can derive from the ...
flippiefanus's user avatar
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3 votes
Accepted

Ladder operators and creation & annihilation operators - different between $a$, $b$ and $c$

When we talk about the quantum harmonic oscillator, $a$ and $a^{\dagger}$ are usually used.($a$ may stands for "annihilation".) Note that we have not discuss second quantization here, so $a$ ...
Gordon Liu's user avatar
2 votes

Ladder operators and creation & annihilation operators - different between $a$, $b$ and $c$

Someone can tell me the different between the notation $a$ or $b$ or $c$? The name of these operators doesn't matter. The important thing are the commutation relations between these two operators (...
Thomas Fritsch's user avatar
3 votes

Where does the "arbitrary constant" in the $L_{0}$ Virasoro operator come from?

Starting from the classical Poisson algebra of $L_m$ quantities (which form a Witt algebra), we would like to quantize it, i.e. define operators $\hat{L}_m$. Due to the operator ordering ambiguity, ...
Qmechanic's user avatar
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1 vote

How to find the expectation value of momentum operator?

I am going to rewrite your formulas because the placement of some of your quantities is personally confusing. $$\left \langle \hat{p} \right \rangle = \int_{-\infty}^{\infty}dx \ \psi^{*}(x)\left(-i\...
Silly Goose's user avatar
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1 vote

Why do QM books point out that $S^2$ commutes with $S_x$, $S_y$, and $S_z$?

$\newcommand\ket[1]{|{#1}\rangle}\newcommand\up{\uparrow}\newcommand\down{\downarrow}$To expound on one of the comments: $S^2$ is not always so simple, as a matrix. For a system with a fixed spin, yes,...
HTNW's user avatar
  • 4,113
4 votes

What can we say about the eigendecomposition of quantum channels?

As you observe correctly, $\mathbb N$ is a linear map. Thus, the same holds as for any eigendecomposition of linear maps. In particular, there need not be a complete basis of eigenvectors (there can ...
Norbert Schuch's user avatar
2 votes

Why do QM books point out that $S^2$ commutes with $S_x$, $S_y$, and $S_z$?

The 2 x 2 spin matrices are for the (fundamental) spinor representation: two component spinors. All two component spinors have a spin quantum number $s=\frac 1 2$, and a fixed angular momentum: $$ S = ...
JEB's user avatar
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2 votes

Why do QM books point out that $S^2$ commutes with $S_x$, $S_y$, and $S_z$?

Your QM book stresses these facts because it means that this operator is something called the "Casimir invariant", which must be proportional to the identity operator and commute with all ...
just a phase's user avatar
4 votes
Accepted

What can we say about the eigendecomposition of quantum channels?

Generally speaking, no. Here is a quantum channel which provides a counter example. Let $|i\rangle$, $i = 1, \dots, n$ be an orthonormal basis on an $n$ dimensional Hilbert space, and define $$A_i = |...
pseudo-goldstone's user avatar

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