1 | <head> |
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2 | <title>BEAM</title> |
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3 | <!-- Changed by: Hans Grote, 30-Sep-2002 --> |
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4 | </head> |
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5 | |
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6 | <body bgcolor="#ffffff"> |
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7 | |
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8 | <center> |
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9 | EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH |
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10 | <IMG SRC="http://cern.ch/madx/icons/mx7_25.gif" align=right> |
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11 | <h2>BEAM: Set Beam Parameters</h2> |
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12 | </center> |
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13 | |
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14 | Many commands in MAD-X require the setting of various quantities related |
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15 | to the beam in the machine. Therefore, MAD-X will stop with a fatal error |
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16 | if an attempt is made to expand (USE) a sequence for which no BEAM |
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17 | command has been issued before. |
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18 | <p> |
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19 | The quantities are entered by a BEAM command: |
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20 | <pre> |
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21 | BEAM, PARTICLE=name,MASS=real,CHARGE=real, |
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22 | ENERGY=real,PC=real,GAMMA=real, |
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23 | EX=real,EXN=real,EY=real,EYN=real, |
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24 | ET=real,SIGT=real,SIGE=real, |
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25 | KBUNCH=integer,NPART=real,BCURRENT=real, |
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26 | BUNCHED=logical,RADIATE=logical,BV=integer,SEQUENCE=name; |
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27 | </pre> |
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28 | Warning: BEAM updates, i. e. it replaces attributes explicitely |
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29 | mentioned, but does not return to default values for others! |
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30 | To reset to <a href="resbeam.html#defaults">beam value defaults</a>, |
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31 | use <a href="resbeam.html">RESBEAM</a>. |
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32 | The particle restmass and <a name=charge>charge</a> are defined by: |
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33 | <ul> |
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34 | <li><a name=particle>PARTICLE</a>: |
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35 | The name of particles in the machine. |
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36 | MAD knows the restmass and the charge for the following particles: |
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37 | <ul><li>POSITRON: |
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38 | The particles are positrons (MASS=<i>m<sub>e</sub></i>, CHARGE=1), |
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39 | <li>ELECTRON: |
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40 | The particles are electrons (MASS=<i>m<sub>e</sub></i>, CHARGE=-1), |
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41 | <li>PROTON: |
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42 | The particles are protons (MASS=<i>m<sub>p</sub></i>, CHARGE=1), |
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43 | <li>ANTIPROTON: |
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44 | The particles are anti-protons (MASS=<i>m<sub>p</sub></i>, CHARGE=-1). |
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45 | <li>POSMUON: |
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46 | The particles are positive muons (MASS=<i>m<sub>mu</sub></i>, CHARGE=1), |
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47 | <li>NEGMUON: |
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48 | The particles are negative muons (MASS=<i>m<sub>mu</sub></i>, CHARGE=-1). |
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49 | </ul> |
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50 | </ul> |
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51 | Therefore neither restmass nor charge can be modified for these predefined |
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52 | particles. On the other hand, for ions and all other user defined |
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53 | particles the name, restmass, and charge can be entered independently. |
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54 | <p> |
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55 | By default the total particle energy is 1 GeV. |
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56 | A different value can be defined by one of the following: |
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57 | <ul> |
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58 | <li><a name=energy>ENERGY</a>: |
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59 | The total energy per particle in GeV. |
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60 | If given, it must be greater then the particle restmass. |
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61 | <li><a name=pc>PC</a>: |
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62 | The momentum per particle in GeV/c. |
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63 | If given, it must be greater than zero. |
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64 | <li><a name=gamma>GAMMA</a>: |
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65 | The ratio between total energy and rest energy of the particles: |
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66 | GAMMA = <i>E / m<sub>0</sub></i>. |
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67 | If given, it must be greater than one. |
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68 | If the restmass is changed a new value for the energy should be entered. |
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69 | Otherwise the energy remains unchanged, |
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70 | and the momentum PC and the quantity GAMMA are recalculated. |
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71 | </ul> |
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72 | |
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73 | The emittances are defined by: |
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74 | <ul> |
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75 | <li><a name=ex>EX</a>: |
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76 | The horizontal emittance <i>E<sub>x</sub></i> (default: 1 m). |
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77 | <li><a name=ey>EY</a>: |
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78 | The vertical emittance <i>E<sub>y</sub></i> (default: 1 m). |
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79 | <li><a name=et>ET</a>: |
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80 | The longitudinal emittance <i>E<sub>t</sub></i> (default: 1 m). |
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81 | </ul> |
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82 | |
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83 | The emittances can be replaced |
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84 | by the normalised emittances and the energy spread: |
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85 | <ul> |
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86 | <li><a name=exn>EXN</a>: |
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87 | The normalised horizontal emittance [m]: |
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88 | <i>E<sub>xn</sub></i> = |
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89 | 4 (GAMMA<sup>2</sup> - 1)<sup>1/2</sup> <i>E<sub>x</sub></i> |
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90 | (ignored if <i>E<sub>x</sub></i> is given). |
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91 | <li><a name=eyn>EYN</a>: |
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92 | The normalised vertical emittance [m]: |
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93 | <i>E<sub>yn</sub></i> = |
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94 | 4 (GAMMA<sup>2</sup> - 1)<sup>1/2</sup> <i>E<sub>y</sub></i> |
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95 | (ignored if <i>E<sub>x</sub></i> is given). |
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96 | <li><a name=sigt>SIGT</a>: |
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97 | The bunch length <i>c</i> sigma(<i>t</i>) in [m]. |
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98 | <li><a name=sige>SIGE</a>: |
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99 | The <em>relative</em> energy spread sigma(<i>E</i>)/<i>E</i> in [1]. |
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100 | </ul> |
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101 | Certain commands compute the synchrotron tune <i>Q<sub>s</sub></i> |
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102 | from the RF cavities. |
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103 | If <i>Q<sub>s</sub></i> is non-zero, |
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104 | the relative energy spread and the bunch length are |
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105 | <p> |
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106 | sigma(<i>E</i>) / <i>p<sub>0</sub> c = |
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107 | (2 pi Q<sub>s</sub> E<sub>t</sub> / ETA C)<sup>1/2</sup></i>, |
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108 | <p> |
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109 | <i>c</i> sigma(<i>t</i>) = |
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110 | </i>(ETA C E<sub>t</sub> / 2 pi Q<sub>s</sub>)<sup>1/2</sup></i>. |
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111 | <p> |
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112 | <i>C</i> is the machine circumference, and |
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113 | <p> |
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114 | <i>ETA</i> = GAMMA<sup>-2</sup> - GAMMA(transition)<sup>-2</sup>. |
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115 | <p> |
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116 | The order of precedence in the parameter evaluation is given below: |
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117 | <pre> |
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118 | particle->(mass+charge) |
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119 | energy->pc->gamma->beta |
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120 | ex->exn |
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121 | ey->eyn |
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122 | current->npart |
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123 | et->sigt->sige |
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124 | </pre> |
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125 | where any item to the left takes precendence over the others. |
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126 | <p> |
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127 | Finally, the BEAM command accepts |
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128 | <ul> |
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129 | <li><a name=kbunch>KBUNCH</a>: |
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130 | The number of particle bunches in the machine (default: 1). |
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131 | <li><a name=npart>NPART</a>: |
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132 | The number of particles per bunch (default: 0). |
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133 | <li><a name=bcurrent>BCURRENT</a>: |
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134 | The bunch current (default: 0 A). |
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135 | <li><a name=bunched>BUNCHED</a>: |
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136 | A logical flag. |
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137 | If set, the beam is treated as bunched whenever this makes sense. |
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138 | <li><a name=radiate>RADIATE</a>: |
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139 | A logical flag. |
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140 | If set, synchrotron radiation is considered in all bipolar magnets. |
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141 | <li><a name=bv>BV</a>: an integer specifying the direction of the |
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142 | particle movement in a beam line; either +1 (default), or -1. For |
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143 | a detailed explanation see under <a href=bv_flag.html>bv flag</a>. |
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144 | <li><a name=sequence>SEQUENCE</a>: this attaches the beam command to a |
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145 | specific sequence; if the name is omitted, the BEAM command refers to |
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146 | the default beam always present. Sequences without attached beam use this |
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147 | default beam. When updating a beam, the corresponding sequence name, |
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148 | if any, must always be mentioned. |
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149 | </ul> |
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150 | The BEAM command changes only the parameters entered. |
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151 | The command |
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152 | <a href=resbeam.html>RESBEAM</a> |
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153 | resets all beam data to their |
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154 | <a href = "resbeam.html#defaults">beam value defaults</a>. |
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155 | <p> |
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156 | Examples: |
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157 | <pre> |
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158 | BEAM, PARTICLE=ELECTRON,ENERGY=50,EX=1.E-6,EY=1.E-8,SIGE=1.E-3; |
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159 | ... |
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160 | BEAM, RADIATE; |
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161 | ... |
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162 | RESBEAM; |
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163 | BEAM, EX=2.E-5,EY=3.E-7,SIGE=4.E-3; |
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164 | </pre> |
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165 | The first command selects electrons, and sets energy and emittances. |
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166 | The second one turns on synchrotron radiation. |
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167 | The last two select positrons (by default), |
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168 | set the energy to 1 GeV (default), |
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169 | clear the synchrotron radiation flag, |
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170 | and set the emittances to the values entered. |
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171 | <p> |
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172 | Some program modules of MAD-X may also store data into a beam data block. |
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173 | Expressions may refer to data in this beam data block |
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174 | using the notation |
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175 | <pre>BEAM->attribute-name</pre> or <pre>BEAM%sequence->attribute-name.</pre> |
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176 | This notation refers to the value of attribute-name |
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177 | found in the default BEAM resp. the beam belonging to the sequence |
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178 | given. |
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179 | This can be used for receiving or using values, e.g. |
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180 | <pre> |
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181 | value,beam%lhcb2->bv; |
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182 | </pre> |
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183 | or for storing values in the beam (this does NOT trigger an update |
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184 | of dependent variables !), e.g. |
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185 | <pre> |
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186 | beam->charge=-1; |
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187 | </pre> |
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188 | The current values in the BEAM bank can be obtained by the command |
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189 | <pre>show,beam;</pre> resp. <pre>show,beam%sequence;</pre> |
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190 | <p> |
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191 | <address> |
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192 | <a href="http://www.cern.ch/Hans.Grote/hansg_sign.html">hansg</a> |
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193 | 11.9.2000 |
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194 | </address> |
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195 | |
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196 | </body> |
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