Paper detail

A Short Remark on the Polaron in the Semi-relativistic Pauli-Fierz Model

We consider the polaron of the spinless semi-relativistic Pauli-Fierz model. The Hamiltonian of the model is defined by $H(\mathbf{P}) = \sqrt{(\mathbf{P}-dΓ(\mathbf{k}) + e\bA)^2 + M^2} + dΓ(ω_m)$, where $\mathbf{P}\in\mathbb{R}^3$ is the momentum of the polaron, $dΓ(\cdot)$ denotes the second quantization operator and $ω_m=|\mathbf{k}|+m$ denotes the dispersion relation of the photon with virtual mass $m\geq 0$. Let $E(\mathbf{P})$ be the lowest energy of $H(\mathbf{P})$. In this paper, we prove the inequality $E(\mathbf{P} - \mathbf{k}) - E(\mathbf{P}) + ω_m(\mathbf{k}) \geq m$, for all $\mathbf{P}, \mathbf{k}\in\mathbb{R}^3$.

preprint2013arXivOpen access

Signal facts

What is known right now

Open access1 author2 topics

Next steps

Decide what to do with this paper

Use like or dislike for the fast social read. The more specific scholarly feedback stays available below when needed.

Log in to curate

Reading frame

Keep the important context close to the paper

Keep the important signals around this paper in one place: votes, save state, collection context, reviews and the metadata you need before deciding what to do next.

Institutions

Add specific reaction

Move through the context

Research map

Open full explorer

Move through nearby people, institutions, topics and adjacent work without leaving the paper page.

Building this map preview

BZPEER is loading the nearby papers, people, topics and institutions for this page.

Structured reviews

0 review(s)

ContributeLeave structured feedbackUse the review template when you have a concrete strength, concern or method question.Open review form

No structured reviews yet. High-signal critique starts here.

Work discussion

0 comment(s)

DiscussAdd a high-signal commentKeep quick notes, caveats and replication pointers separate from formal reviews.Open comment form

No discussion yet. The first strong comment sets the tone.