dorsal/arxiv
View SchemaNew Use of Dimensional Continuation Illustrated by dE/dx in a Plasma and the Lamb Shift
| Authors | Lowell S. Brown |
|---|---|
| Categories | |
| ArXiv ID | physics/9911056 |
| URL | https://arxiv.org/abs/physics/9911056 |
| DOI | 10.1103/PhysRevD.62.045026 |
| Journal | Phys.Rev. D62 (2000) 045026 |
Abstract
Physical processes ranging from the Lamb shift to the energy loss dE/dx of a charged particle traversing a plasma entail processes that occur over a wide range of energy or length scales. Different physical mechanisms dominate at one or the other end of this range. For example, in the energy loss problem, soft collisions that are screened by collective effects are important at large distances, while at short distances hard collisions are important where the exact details of the single-particle interactions must be taken into account. We introduce a novel application of dimensional continuation. The soft processes dominate at all scales when the spatial dimension \nu is less than 3, and we use them to compute the result to leading order for \nu < 3. On the other hand, the hard processes dominate at all scales for \nu > 3, and we use them to compute the result to leading order for these spatial dimensions. We then explain why the sum of the analytic continuation of these disparate mechanisms yields the correct leading-order result for the physical limit at \nu = 3 dimensions. After applying this new method to the energy loss problem in some detail, we then show how it also provides a very short and easy way to compute the Lamb shift.
{
"annotation_id": "d9357223-ab76-494e-ba46-e63c792378f5",
"date_created": "2026-03-02T18:01:25.410000Z",
"date_modified": "2026-03-02T18:01:25.410000Z",
"file_hash": "78f800084b3b3d071509ef0ed184b95abfd0941e691b46a4d26a027173554c7c",
"private": false,
"record": {
"abstract": "Physical processes ranging from the Lamb shift to the energy loss dE/dx of a\ncharged particle traversing a plasma entail processes that occur over a wide\nrange of energy or length scales. Different physical mechanisms dominate at one\nor the other end of this range. For example, in the energy loss problem, soft\ncollisions that are screened by collective effects are important at large\ndistances, while at short distances hard collisions are important where the\nexact details of the single-particle interactions must be taken into account.\nWe introduce a novel application of dimensional continuation. The soft\nprocesses dominate at all scales when the spatial dimension \\nu is less than 3,\nand we use them to compute the result to leading order for \\nu \u003c 3. On the\nother hand, the hard processes dominate at all scales for \\nu \u003e 3, and we use\nthem to compute the result to leading order for these spatial dimensions. We\nthen explain why the sum of the analytic continuation of these disparate\nmechanisms yields the correct leading-order result for the physical limit at\n\\nu = 3 dimensions. After applying this new method to the energy loss problem\nin some detail, we then show how it also provides a very short and easy way to\ncompute the Lamb shift.",
"arxiv_id": "physics/9911056",
"authors": [
"Lowell S. Brown"
],
"categories": [
"physics.plasm-ph",
"cond-mat.stat-mech",
"hep-ph"
],
"doi": "10.1103/PhysRevD.62.045026",
"journal_ref": "Phys.Rev. D62 (2000) 045026",
"title": "New Use of Dimensional Continuation Illustrated by dE/dx in a Plasma and the Lamb Shift",
"url": "https://arxiv.org/abs/physics/9911056"
},
"schema_id": "dorsal/arxiv",
"source": {
"execution_id": "3a461bf6-6084-49f0-ace0-1cf921320189",
"id": "arXiv Dataset IDs",
"type": "Model",
"variant": "snapshot-2026-03-01",
"version": "0.1.0"
},
"user_id": 1000002
}