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32 | 32 | "charged particle beam simulation. It was created by Andrei Terebilo in\n",
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33 | 33 | "the late 1990’s. The original papers[^at1][^at2] still serve as a good introduction to AT. The AT described in those papers is AT1.3, the latest version produced by Terebilo. The next version of AT is considered AT2.0[^nash]. Here we provide examples showing some of the changes from AT1.3, but also serving as an introduction for someone just starting AT.\n",
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34 | 34 | "\n",
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35 |
| - "### Coordinates\n", |
| 35 | + "### AT Coordinate system\n", |
36 | 36 | "\n",
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37 |
| - "The 6-d phase space coordinates used in AT are as follows:\n", |
| 37 | + "The AT coordinate system is based on a design trajectory along which the magnetic elements are aligned,\n", |
| 38 | + "and a reference particle:\n", |
| 39 | + "\n", |
| 40 | + "```{image} /images/coord_system.*\n", |
| 41 | + ":alt: coordinate system\n", |
| 42 | + ":align: center\n", |
| 43 | + "```\n", |
| 44 | + "\n", |
| 45 | + "By convention, the reference particle travels along the design trajectory at constant nominal energy and defines the phase origin of the RF voltage.\n", |
| 46 | + "\n", |
| 47 | + "The 6-d coordinate vector $\\vec Z$ is:\n", |
38 | 48 | "\n",
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39 | 49 | "$$\n",
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40 |
| - "\\vec Z = \\begin{pmatrix} x \\\\ \\frac{p_x}{p_0} \\simeq x'(1+\\delta) \\\\ y \\\\ \\frac{p_y}{p_0} \\simeq y'(1+\\delta) \\\\ \\delta=\\frac{\\left(p-p_0\\right)}{p_0} \\\\ \\beta c \\tau\\end{pmatrix}\n", |
| 50 | + "\\vec Z = \\begin{pmatrix} x \\\\ \\dfrac{p_x}{p_0} \\approx x'(1+\\delta) \\\\ y \\\\ \\dfrac{p_y}{p_0} \\approx y'(1+\\delta) \\\\ \\delta=\\dfrac{p-p_0}{p_0} \\\\ \\beta c \\tau\\end{pmatrix}\n", |
41 | 51 | "$$\n",
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42 | 52 | "\n",
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43 |
| - "$p_0$ is the reference momentum. $\\tau$ is the\n", |
44 |
| - "time lag relative to the ideal particle." |
| 53 | + "$p_0$ is the reference momentum.\n", |
| 54 | + "\n", |
| 55 | + "AT works with relative path lengths: the 6{sup}`th` coordinate $\\beta c\\tau$ represents\n", |
| 56 | + "the path lengthening with respect to the reference particle. $\\tau$ is the delay with\n", |
| 57 | + "respect to the reference particle: the particle is late for $\\tau > 0$.\n" |
45 | 58 | ]
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46 | 59 | },
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47 | 60 | {
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1760 | 1773 | "name": "python",
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1761 | 1774 | "nbconvert_exporter": "python",
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1762 | 1775 | "pygments_lexer": "ipython3",
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1763 |
| - "version": "3.11.10" |
| 1776 | + "version": "3.9.21" |
1764 | 1777 | },
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1765 | 1778 | "toc-autonumbering": false,
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1766 | 1779 | "toc-showcode": false,
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