1 | <head> |
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2 | <title>MULTIPOLE</title> |
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3 | <!-- Changed by: Chris ISELIN, 27-Jan-1997 --> |
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4 | <!-- Changed by: Hans Grote, 17-Jun-2002 --> |
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5 | <!-- Changed by: Frank Schmidt, 28-Aug-2003 --> |
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6 | </head> |
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7 | |
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8 | <body bgcolor="#ffffff"> |
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9 | |
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10 | <h2>MULTIPOLE: General Thin Multipole</h2> |
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11 | |
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12 | <pre> |
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13 | label: MULTIPOLE,LRAD=real,TILT=real, |
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14 | KNL:={..,..,..}, KSL:={..,..,..}; |
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15 | </pre> |
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16 | A MULTIPOLE is a thin-lens magnet of arbitrary order, including a dipole: |
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17 | <ul> |
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18 | <li>LRAD: |
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19 | A fictitious length, which was originally just used to compute synchrotron |
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20 | radiation effects.<br> A non-zero <b><font color="#ff0000"> LRAD </b></font> in conjunction |
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21 | with the <a href="../control/general.html#option">OPTION</a> |
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22 | <b><font color="#ff0000"> thin_foc </b></font> set to a <b><font color="#ff0000"> true </b></font> logical |
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23 | value takes into account of the weak focussing of bending magnets. |
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24 | <LI>TILT: |
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25 | The roll angle about the longitudinal axis (default: 0 rad). |
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26 | A positive angle represents a clockwise rotation of the multipole |
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27 | element. |
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28 | <p><b><font color="#ff0000"> |
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29 | Please note that contrary to MAD8 one has to specify the desired TILT |
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30 | angle, otherwise it is taken as 0 rad. We believe that the MAD8 |
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31 | concept of having individual TILT values for each component and on top |
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32 | with default values led to considerable confusion and allowed for |
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33 | excessive and unphysical freedom. Instead, in MAD-X the KNL/KSL |
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34 | components can be considered as the normal or skew multipole |
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35 | components of the magnet on the bench, while the TILT attribute can be |
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36 | considered as an tilt alignment error in the machine. |
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37 | </b></font> |
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38 | <li>KNL: |
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39 | The normal multipole coefficients from order zero to the maximum; |
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40 | the parameters are positional, therefore zeros must be filled in |
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41 | for components that do not exist. Example of a thin-lens sextupole: |
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42 | <pre> |
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43 | ms:multipole, knl:={0, 0, k2l}; |
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44 | </pre> |
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45 | <li>KSL: |
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46 | The skew multipole coefficients from order zero to the maximum; |
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47 | the parameters are positional, therefore zeros must be filled in |
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48 | for components that do not exist. Example of a thin-lens skew octupole: |
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49 | <pre> |
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50 | ms:multipole, ksl:={0, 0, 0, k3sl}; |
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51 | </pre> |
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52 | </ul> |
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53 | Both KNL and KSL may be specified for the same multipole. |
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54 | <p> |
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55 | A multipole with no dipole component has no effect on the reference |
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56 | orbit, |
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57 | i.e. the reference system at its exit is the same as at its entrance. |
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58 | If it includes a dipole component, |
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59 | it has the same effect on the reference orbit as a dipole |
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60 | with zero length and deflection angle K0L, being the first component |
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61 | of KNL above. |
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62 | <p> |
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63 | <address> |
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64 | <a href="http://www.cern.ch/Hans.Grote/hansg_sign.html">hansg</a>, |
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65 | <a href="http://www.cern.ch/Frank.Schmidt/frs_sign.html">Frank.Schmidt</a>, |
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66 | August 28, 2003 |
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67 | </address> |
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68 | |
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69 | </body> |
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