|
| 1 | +import numpy as np |
| 2 | +from scipy.constants import c, e, m_p |
| 3 | + |
| 4 | +from PyHEADTAIL.machines.synchrotron import Synchrotron |
| 5 | + |
| 6 | + |
| 7 | +class EmptyObject(object): |
| 8 | + pass |
| 9 | + |
| 10 | + |
| 11 | +class LHC(Synchrotron): |
| 12 | + |
| 13 | + def __init__(self, machine_configuration=None, optics_mode='smooth', **kwargs): |
| 14 | + |
| 15 | + |
| 16 | + pp = EmptyObject() |
| 17 | + pp.machine_configuration = machine_configuration |
| 18 | + pp.optics_mode = optics_mode |
| 19 | + |
| 20 | + pp.longitudinal_mode = 'non-linear' |
| 21 | + pp.alpha = 3.225e-04 |
| 22 | + pp.h_RF = 35640 |
| 23 | + pp.mass = m_p |
| 24 | + pp.charge = e |
| 25 | + pp.RF_at = 'middle' |
| 26 | + |
| 27 | + if pp.machine_configuration == 'Injection': |
| 28 | + pp.p0 = 450e9 * e / c |
| 29 | + pp.p_increment = 0. |
| 30 | + pp.accQ_x = 64.28 |
| 31 | + pp.accQ_y = 59.31 |
| 32 | + pp.V_RF = 6e6 |
| 33 | + pp.dphi_RF = 0. |
| 34 | + elif machine_configuration == '6.5_TeV_collision_tunes': |
| 35 | + pp.p0 = 6500e9 * e / c |
| 36 | + pp.p_increment = 0. |
| 37 | + pp.accQ_x = 64.31 |
| 38 | + pp.accQ_y = 59.32 |
| 39 | + pp.V_RF = 12e6 |
| 40 | + pp.dphi_RF = 0. |
| 41 | + else: |
| 42 | + raise ValueError('machine_configuration not recognized!') |
| 43 | + |
| 44 | + if pp.optics_mode == 'smooth': |
| 45 | + if 's' in list(kwargs.keys()): |
| 46 | + raise ValueError('s vector cannot be provided if optics_mode = "smooth"') |
| 47 | + |
| 48 | + pp.n_segments = kwargs['n_segments'] |
| 49 | + pp.circumference = 26658.8832 |
| 50 | + |
| 51 | + pp.name = None |
| 52 | + |
| 53 | + pp.beta_x = 92.7 |
| 54 | + pp.D_x = 0 |
| 55 | + pp.beta_y = 93.2 |
| 56 | + pp.D_y = 0 |
| 57 | + |
| 58 | + pp.alpha_x = None |
| 59 | + pp.alpha_y = None |
| 60 | + |
| 61 | + pp.s = None |
| 62 | + |
| 63 | + elif pp.optics_mode == 'non-smooth': |
| 64 | + if 'n_segments' in list(kwargs.keys()): |
| 65 | + raise ValueError('n_segments cannot be provided if optics_mode = "non-smooth"') |
| 66 | + pp.n_segments = None |
| 67 | + pp.circumference = None |
| 68 | + |
| 69 | + pp.name = kwargs['name'] |
| 70 | + |
| 71 | + pp.beta_x = kwargs['beta_x'] |
| 72 | + pp.beta_y = kwargs['beta_y'] |
| 73 | + |
| 74 | + try: |
| 75 | + pp.D_x = kwargs['D_x'] |
| 76 | + except KeyError: |
| 77 | + pp.D_x = 0 * np.array(kwargs['s']) |
| 78 | + try: |
| 79 | + pp.D_y = kwargs['D_y'] |
| 80 | + except KeyError: |
| 81 | + pp.D_y = 0 * np.array(kwargs['s']) |
| 82 | + |
| 83 | + pp.alpha_x = kwargs['alpha_x'] |
| 84 | + pp.alpha_y = kwargs['alpha_y'] |
| 85 | + |
| 86 | + pp.s = kwargs['s'] |
| 87 | + |
| 88 | + else: |
| 89 | + raise ValueError('optics_mode not recognized!') |
| 90 | + |
| 91 | + # detunings |
| 92 | + pp.Qp_x = 0 |
| 93 | + pp.Qp_y = 0 |
| 94 | + |
| 95 | + pp.app_x = 0 |
| 96 | + pp.app_y = 0 |
| 97 | + pp.app_xy = 0 |
| 98 | + |
| 99 | + pp.i_octupole_focusing = None |
| 100 | + pp.i_octupole_defocusing = None |
| 101 | + pp.octupole_knob = None |
| 102 | + |
| 103 | + for attr in list(kwargs.keys()): |
| 104 | + if kwargs[attr] is not None: |
| 105 | + if type(kwargs[attr]) is list or type(kwargs[attr]) is np.ndarray: |
| 106 | + str2print = '[%s ...]'%repr(kwargs[attr][0]) |
| 107 | + else: |
| 108 | + str2print = repr(kwargs[attr]) |
| 109 | + self.prints('Synchrotron init. From kwargs: %s = %s' |
| 110 | + % (attr, str2print)) |
| 111 | + if not hasattr(pp, attr): |
| 112 | + raise NameError("I don't understand %s"%attr) |
| 113 | + |
| 114 | + setattr(pp, attr, kwargs[attr]) |
| 115 | + |
| 116 | + |
| 117 | + |
| 118 | + if pp.i_octupole_focusing is not None or pp.i_octupole_defocusing is not None: |
| 119 | + if pp.octupole_knob is not None: |
| 120 | + raise ValueError('octupole_knobs and octupole currents cannot be used at the same time!') |
| 121 | + pp.app_x, pp.app_y, pp.app_xy = self._anharmonicities_from_octupole_current_settings( |
| 122 | + pp.i_octupole_focusing, pp.i_octupole_defocusing) |
| 123 | + self.i_octupole_focusing = pp.i_octupole_focusing |
| 124 | + self.i_octupole_defocusing = pp.i_octupole_defocusing |
| 125 | + |
| 126 | + if pp.octupole_knob is not None: |
| 127 | + if pp.i_octupole_focusing is not None or pp.i_octupole_defocusing is not None: |
| 128 | + raise ValueError('octupole_knobs and octupole currents cannot be used at the same time!') |
| 129 | + pp.i_octupole_focusing, pp.i_octupole_defocusing = self._octupole_currents_from_octupole_knobs(pp.octupole_knob, pp.p0) |
| 130 | + pp.app_x, pp.app_y, pp.app_xy = self._anharmonicities_from_octupole_current_settings( |
| 131 | + pp.i_octupole_focusing, pp.i_octupole_defocusing) |
| 132 | + self.i_octupole_focusing = pp.i_octupole_focusing |
| 133 | + self.i_octupole_defocusing = pp.i_octupole_defocusing |
| 134 | + |
| 135 | + |
| 136 | + super(LHC, self).__init__(optics_mode=pp.optics_mode, circumference=pp.circumference, n_segments=pp.n_segments, |
| 137 | + s=pp.s, name=pp.name, |
| 138 | + alpha_x=pp.alpha_x, beta_x=pp.beta_x, D_x=pp.D_x, alpha_y=pp.alpha_y, beta_y=pp.beta_y, D_y=pp.D_y, |
| 139 | + accQ_x=pp.accQ_x, accQ_y=pp.accQ_y, Qp_x=pp.Qp_x, Qp_y=pp.Qp_y, app_x=pp.app_x, app_y=pp.app_y, app_xy=pp.app_xy, |
| 140 | + alpha_mom_compaction=pp.alpha, longitudinal_mode=pp.longitudinal_mode, |
| 141 | + h_RF=np.atleast_1d(pp.h_RF), V_RF=np.atleast_1d(pp.V_RF), dphi_RF=np.atleast_1d(pp.dphi_RF), |
| 142 | + p0=pp.p0, p_increment=pp.p_increment, |
| 143 | + charge=pp.charge, mass=pp.mass, RF_at=pp.RF_at) |
| 144 | + |
| 145 | + |
| 146 | + def _anharmonicities_from_octupole_current_settings(self, i_octupole_focusing, i_octupole_defocusing): |
| 147 | + """Calculate the constants of proportionality app_x, app_y and |
| 148 | + app_xy (== app_yx) for the amplitude detuning introduced by the |
| 149 | + LHC octupole magnets (aka. LHC Landau octupoles) from the |
| 150 | + electric currents i_octupole_focusing [A] and i_octupole_defocusing [A] flowing |
| 151 | + through the magnets. The maximum current is given by |
| 152 | + i_max = +/- 550 [A]. The values app_x, app_y, app_xy obtained |
| 153 | + from the formulae are proportional to the strength of detuning |
| 154 | + for one complete turn around the accelerator, i.e. one-turn |
| 155 | + values. |
| 156 | + The calculation is based on formulae (3.6) taken from 'The LHC |
| 157 | + transverse coupled-bunch instability' by N. Mounet, EPFL PhD |
| 158 | + Thesis, 2012. Values (hard-coded numbers below) are valid for |
| 159 | + LHC Landau octupoles before LS1. Beta functions in x and y are |
| 160 | + correctly taken into account. Note that here, the values of |
| 161 | + app_x, app_y and app_xy are not normalized to the reference |
| 162 | + momentum p0. This is done only during the calculation of the |
| 163 | + detuning in the corresponding detune method of the |
| 164 | + AmplitudeDetuningSegment. |
| 165 | + More detailed explanations and references on how the formulae |
| 166 | + were obtained are given in the PhD thesis (pg. 85ff) cited |
| 167 | + above. |
| 168 | + """ |
| 169 | + i_max = 550. # [A] |
| 170 | + E_max = 7000. # [GeV] |
| 171 | + |
| 172 | + app_x = E_max * (267065. * i_octupole_focusing / i_max - |
| 173 | + 7856. * i_octupole_defocusing / i_max) |
| 174 | + app_y = E_max * (9789. * i_octupole_focusing / i_max - |
| 175 | + 277203. * i_octupole_defocusing / i_max) |
| 176 | + app_xy = E_max * (-102261. * i_octupole_focusing / i_max + |
| 177 | + 93331. * i_octupole_defocusing / i_max) |
| 178 | + |
| 179 | + # Convert to SI units. |
| 180 | + convert_to_SI = e / (1.e-9 * c) |
| 181 | + app_x *= convert_to_SI |
| 182 | + app_y *= convert_to_SI |
| 183 | + app_xy *= convert_to_SI |
| 184 | + |
| 185 | + return app_x, app_y, app_xy |
| 186 | + |
| 187 | + def _octupole_currents_from_octupole_knobs(self, octupole_knob, p0): |
| 188 | + i_octupole_focusing = 19.557 * octupole_knob / (-1.5) * p0 / 2.4049285931335872e-16 |
| 189 | + i_octupole_defocusing = - i_octupole_focusing |
| 190 | + return i_octupole_focusing, i_octupole_defocusing |
0 commit comments