Source code for ampform.helicity

"""Generate an amplitude model with the helicity formalism."""

import logging
import operator
from collections import defaultdict
from difflib import get_close_matches
from functools import reduce
from typing import (
    Any,
    DefaultDict,
    Dict,
    Iterable,
    List,
    Optional,
    Tuple,
    Type,
    Union,
)

import attr
import sympy as sp
from attr.validators import instance_of
from qrules.combinatorics import (
    perform_external_edge_identical_particle_combinatorics,
)
from qrules.particle import ParticleCollection
from qrules.transition import ReactionInfo, StateTransition
from sympy.physics.quantum.cg import CG
from sympy.physics.quantum.spin import Rotation as Wigner
from sympy.printing.latex import LatexPrinter

from ampform.dynamics.builder import (
    ResonanceDynamicsBuilder,
    TwoBodyKinematicVariableSet,
)
from ampform.kinematics import (
    HelicityAdapter,
    get_helicity_angle_label,
    get_invariant_mass_label,
)

from .decay import TwoBodyDecay
from .naming import (
    CanonicalAmplitudeNameGenerator,
    HelicityAmplitudeNameGenerator,
    generate_transition_label,
)

ParameterValue = Union[float, complex, int]


[docs]@attr.s(frozen=True) class HelicityModel: _expression: sp.Expr = attr.ib( validator=attr.validators.instance_of(sp.Expr) ) _parameter_defaults: Dict[sp.Symbol, ParameterValue] = attr.ib( validator=attr.validators.instance_of(dict) ) _components: Dict[str, sp.Expr] = attr.ib( validator=attr.validators.instance_of(dict) ) _adapter: HelicityAdapter = attr.ib( validator=attr.validators.instance_of(HelicityAdapter) ) particles: ParticleCollection = attr.ib( validator=instance_of(ParticleCollection) ) @property def expression(self) -> sp.Expr: return self._expression @property def components(self) -> Dict[str, sp.Expr]: return self._components @property def parameter_defaults(self) -> Dict[sp.Symbol, ParameterValue]: return self._parameter_defaults @property def adapter(self) -> HelicityAdapter: return self._adapter
[docs] def sum_components( # noqa: R701 self, components: Iterable[str] ) -> sp.Expr: """Coherently or incoherently add components of a helicity model.""" components = list(components) # copy for component in components: if component not in self.components: first_letter = component[0] candidates = get_close_matches( component, filter( lambda c: c.startswith( first_letter # pylint: disable=cell-var-from-loop ), self.components, ), ) raise KeyError( f'Component "{component}" not in model components. ' f"Did you mean any of these?", candidates, ) if any(map(lambda c: c.startswith("I"), components)) and any( map(lambda c: c.startswith("A"), components) ): intensity_sum = self.sum_components( components=filter(lambda c: c.startswith("I"), components), ) amplitude_sum = self.sum_components( components=filter(lambda c: c.startswith("A"), components), ) return intensity_sum + amplitude_sum if all(map(lambda c: c.startswith("I"), components)): return sum(self.components[c] for c in components) if all(map(lambda c: c.startswith("A"), components)): return abs(sum(self.components[c] for c in components)) ** 2 raise ValueError( 'Not all component names started with either "A" or "I"' )
[docs]class HelicityAmplitudeBuilder: """Amplitude model generator for the helicity formalism.""" def __init__(self, reaction: ReactionInfo) -> None: self._name_generator = HelicityAmplitudeNameGenerator() self.__reaction = reaction self.__parameter_defaults: Dict[sp.Symbol, ParameterValue] = {} self.__components: Dict[str, sp.Expr] = {} self.__dynamics_choices: Dict[ TwoBodyDecay, ResonanceDynamicsBuilder ] = {} if len(reaction.transitions) < 1: raise ValueError( f"At least one {StateTransition.__name__} required to" " genenerate an amplitude model!" ) self.__adapter = HelicityAdapter(reaction) for grouping in reaction.transition_groups: self.__adapter.register_topology(grouping.topology) self.__particles = extract_particle_collection(reaction.transitions)
[docs] def set_dynamics( self, particle_name: str, dynamics_builder: ResonanceDynamicsBuilder ) -> None: for transition in self.__reaction.transitions: for node_id in transition.topology.nodes: decay = TwoBodyDecay.from_transition(transition, node_id) decaying_particle = decay.parent.particle if decaying_particle.name == particle_name: self.__dynamics_choices[decay] = dynamics_builder
[docs] def formulate(self) -> HelicityModel: self.__components = {} self.__parameter_defaults = {} return HelicityModel( expression=self.__formulate_top_expression(), components=self.__components, parameter_defaults=self.__parameter_defaults, adapter=self.__adapter, particles=self.__particles, )
def __formulate_top_expression(self) -> sp.Expr: transition_groups = group_transitions(self.__reaction.transitions) self.__register_parameter_couplings(transition_groups) coherent_intensities = [ self.__formulate_coherent_intensity(group) for group in transition_groups ] return sum(coherent_intensities) def __register_parameter_couplings( self, transition_groups: List[List[StateTransition]] ) -> None: for graph_group in transition_groups: for transition in graph_group: self._name_generator.register_amplitude_coefficient_name( transition ) def __formulate_coherent_intensity( self, transition_group: List[StateTransition] ) -> sp.Expr: graph_group_label = generate_transition_label(transition_group[0]) sequential_expressions: List[sp.Expr] = [] for transition in transition_group: sequential_graphs = ( perform_external_edge_identical_particle_combinatorics( transition.to_graph() ) ) for graph in sequential_graphs: transition = StateTransition.from_graph(graph) expression = self.__formulate_sequential_decay(transition) sequential_expressions.append(expression) amplitude_sum = sum(sequential_expressions) coherent_intensity = abs(amplitude_sum) ** 2 self.__components[fR"I_{{{graph_group_label}}}"] = coherent_intensity return coherent_intensity def __formulate_sequential_decay( self, transition: StateTransition ) -> sp.Expr: partial_decays: List[sp.Symbol] = [ self._formulate_partial_decay(transition, node_id) for node_id in transition.topology.nodes ] sequential_amplitudes = reduce(operator.mul, partial_decays) coefficient = self.__generate_amplitude_coefficient(transition) prefactor = self.__generate_amplitude_prefactor(transition) expression = coefficient * sequential_amplitudes if prefactor is not None: expression = prefactor * expression self.__components[ f"A_{{{self._name_generator.generate_amplitude_name(transition)}}}" ] = expression return expression def _formulate_partial_decay( self, transition: StateTransition, node_id: int ) -> sp.Expr: wigner_d = formulate_wigner_d(transition, node_id) dynamics = self.__formulate_dynamics(transition, node_id) return wigner_d * dynamics def __formulate_dynamics( self, transition: StateTransition, node_id: int ) -> sp.Expr: decay = TwoBodyDecay.from_transition(transition, node_id) if decay not in self.__dynamics_choices: return 1 builder = self.__dynamics_choices[decay] variable_set = _generate_kinematic_variable_set(transition, node_id) expression, parameters = builder(decay.parent.particle, variable_set) for par, value in parameters.items(): if par in self.__parameter_defaults: previous_value = self.__parameter_defaults[par] if value != previous_value: logging.warning( f'New default value {value} for parameter "{par.name}"' f" is inconsistent with existing value {previous_value}" ) self.__parameter_defaults[par] = value return expression def __generate_amplitude_coefficient( self, transition: StateTransition ) -> sp.Symbol: """Generate coefficient parameter for a sequential amplitude. Generally, each partial amplitude of a sequential amplitude transition should check itself if it or a parity partner is already defined. If so a coupled coefficient is introduced. """ suffix = self._name_generator.generate_sequential_amplitude_suffix( transition ) coefficient_symbol = sp.Symbol(f"C_{{{suffix}}}") self.__parameter_defaults[coefficient_symbol] = complex(1, 0) return coefficient_symbol def __generate_amplitude_prefactor( self, transition: StateTransition ) -> Optional[float]: prefactor = get_prefactor(transition) if prefactor != 1.0: for node_id in transition.topology.nodes: raw_suffix = self._name_generator.generate_coefficient_name( transition, node_id ) if ( raw_suffix in self._name_generator.parity_partner_coefficient_mapping ): coefficient_suffix = self._name_generator.parity_partner_coefficient_mapping[ raw_suffix ] if coefficient_suffix != raw_suffix: return prefactor return None
[docs]class CanonicalAmplitudeBuilder(HelicityAmplitudeBuilder): r"""Amplitude model generator for the canonical helicity formalism. This class defines a full amplitude in the canonical formalism, using the helicity formalism as a foundation. The key here is that we take the full helicity intensity as a template, and just exchange the helicity amplitudes :math:`F` as a sum of canonical amplitudes :math:`A`: .. math:: F^J_{\lambda_1,\lambda_2} = \sum_{LS} \mathrm{norm}(A^J_{LS})C^2. Here, :math:`C` stands for `Clebsch-Gordan factor <https://en.wikipedia.org/wiki/Clebsch%E2%80%93Gordan_coefficients>`_. """ def __init__(self, reaction_result: ReactionInfo) -> None: super().__init__(reaction_result) self._name_generator = CanonicalAmplitudeNameGenerator() def _formulate_partial_decay( self, transition: StateTransition, node_id: int ) -> sp.Expr: amplitude = super()._formulate_partial_decay(transition, node_id) cg_coefficients = formulate_clebsch_gordan_coefficients( transition, node_id ) return cg_coefficients * amplitude
[docs]def extract_particle_collection( transitions: Iterable[StateTransition], ) -> ParticleCollection: """Collect all particles from a collection of state transitions.""" particles = ParticleCollection() for transition in transitions: for state in transition.states.values(): if state.particle not in particles: particles.add(state.particle) return particles
[docs]def formulate_clebsch_gordan_coefficients( transition: StateTransition, node_id: int ) -> sp.Expr: r"""Compute the two Clebsch-Gordan coefficients for a state transition node. In the **canonical basis** (also called **partial wave basis**), :doc:`Clebsch-Gordan coefficients <sympy:modules/physics/quantum/cg>` ensure that the projection of angular momentum is conserved (:cite:`kutschkeAngularDistributionCookbook1996`, p. 4). When calling :func:`~qrules.generate_transitions` with :code:`formalism="canonical-helicity"`, AmpForm formulates the amplitude in the canonical basis from amplitudes in the helicity basis using the transformation in :cite:`chungSpinFormalismsUpdated2014`, Eq. (4.32). See also :cite:`kutschkeAngularDistributionCookbook1996`, Eq. (28). This function produces the two Clebsch-Gordan coefficients in :cite:`chungSpinFormalismsUpdated2014`, Eq. (4.32). For a two-body decay :math:`1 \to 2, 3`, we get: .. math:: C^{s_1,\lambda}_{L,0,S,\lambda} C^{S,\lambda}_{s_2,\lambda_2,s_3,-\lambda_3} :label: formulate_clebsch_gordan_coefficients with: - :math:`s_i` the intrinsic `Spin.magnitude <qrules.particle.Spin.magnitude>` of each state :math:`i`, - :math:`\lambda_{2}, \lambda_{3}` the helicities of the decay products (can be taken to be their `~qrules.transition.State.spin_projection` when following a constistent boosting procedure), - :math:`\lambda=\lambda_{2}-\lambda_{3}`, - :math:`L` the *total* angular momentum of the final state pair (`~qrules.quantum_numbers.InteractionProperties.l_magnitude`), - :math:`S` the coupled spin magnitude of the final state pair (`~qrules.quantum_numbers.InteractionProperties.s_magnitude`), - and :math:`C^{j_3,m_3}_{j_1,m_1,j_2,m_2} = \langle j1,m1;j2,m2|j3,m3\rangle`, as in :doc:`sympy:modules/physics/quantum/cg`. Example ------- >>> import qrules >>> reaction = qrules.generate_transitions( ... initial_state=[("J/psi(1S)", [+1])], ... final_state=[("gamma", [-1]), "f(0)(980)"], ... ) >>> transition = reaction.transitions[1] # angular momentum 2 >>> formulate_clebsch_gordan_coefficients(transition, node_id=0) CG(1, -1, 0, 0, 1, -1)*CG(2, 0, 1, -1, 1, -1) .. math:: C^{s_1,\lambda}_{L,0,S,\lambda} C^{S,\lambda}_{s_2,\lambda_2,s_3,-\lambda_3} = C^{1,(-1-0)}_{2,0,1,(-1-0)} C^{1,(-1-0)}_{1,-1,0,0} = C^{1,-1}_{2,0,1,-1} C^{1,-1}_{1,-1,0,0} """ decay = TwoBodyDecay.from_transition(transition, node_id) angular_momentum = decay.interaction.l_magnitude coupled_spin = decay.interaction.s_magnitude parent = decay.parent child1 = decay.children[0] child2 = decay.children[1] decay_particle_lambda = child1.spin_projection - child2.spin_projection cg_ls = CG( j1=sp.Rational(angular_momentum), m1=0, j2=sp.Rational(coupled_spin), m2=sp.Rational(decay_particle_lambda), j3=sp.Rational(parent.particle.spin), m3=sp.Rational(decay_particle_lambda), ) cg_ss = CG( j1=sp.Rational(child1.particle.spin), m1=sp.Rational(child1.spin_projection), j2=sp.Rational(child2.particle.spin), m2=sp.Rational(-child2.spin_projection), j3=sp.Rational(coupled_spin), m3=sp.Rational(decay_particle_lambda), ) return sp.Mul(cg_ls, cg_ss, evaluate=False)
[docs]def formulate_wigner_d(transition: StateTransition, node_id: int) -> sp.Expr: r"""Compute `~sympy.physics.quantum.spin.WignerD` for a transition node. Following :cite:`kutschkeAngularDistributionCookbook1996`, Eq. (10). For a two-body decay :math:`1 \to 2, 3`, we get .. math:: D^{s_1}_{m_1,\lambda_2-\lambda_3}(-\phi,\theta,0) :label: formulate_wigner_d with: - :math:`s_1` the `Spin.magnitude <qrules.particle.Spin.magnitude>` of the decaying state, - :math:`m_1` the `~qrules.transition.State.spin_projection` of the decaying state, - :math:`\lambda_{2}, \lambda_{3}` the helicities of the decay products in in the restframe of :math:`1` (can be taken to be their intrinsic `~qrules.transition.State.spin_projection` when following a constistent boosting procedure), - and :math:`\phi` and :math:`\theta` the helicity angles (see also :func:`.get_helicity_angle_label`). Note that :math:`\lambda_2, \lambda_3` are ordered by their number of children, then by their state ID (see :class:`.TwoBodyDecay`). See :cite:`kutschkeAngularDistributionCookbook1996`, Eq. (30) for an example of Wigner-:math:`D` functions in a *sequential* two-body decay. Example ------- >>> import qrules >>> reaction = qrules.generate_transitions( ... initial_state=[("J/psi(1S)", [+1])], ... final_state=[("gamma", [-1]), "f(0)(980)"], ... ) >>> transition = reaction.transitions[0] >>> formulate_wigner_d(transition, node_id=0) WignerD(1, 1, -1, -phi_0, theta_0, 0) .. math:: D^{s_1}_{m_1,\lambda_2-\lambda_3}\left(-\phi,\theta,0\right) = D^{1}_{+1,(-1-0)}\left(-\phi_0,\theta_0,0\right) = D^{1}_{1,-1}\left(-\phi_0,\theta_0,0\right) """ decay = TwoBodyDecay.from_transition(transition, node_id) _, phi, theta = _generate_kinematic_variables(transition, node_id) return Wigner.D( j=sp.Rational(decay.parent.particle.spin), m=sp.Rational(decay.parent.spin_projection), mp=sp.Rational( decay.children[0].spin_projection - decay.children[1].spin_projection ), alpha=-phi, beta=theta, gamma=0, )
[docs]def get_prefactor(transition: StateTransition) -> float: """Calculate the product of all prefactors defined in this transition. .. seealso:: `qrules.quantum_numbers.InteractionProperties.parity_prefactor` """ prefactor = 1.0 for node_id in transition.topology.nodes: interaction = transition.interactions[node_id] if interaction and interaction.parity_prefactor is not None: prefactor *= interaction.parity_prefactor return prefactor
[docs]def group_transitions( transitions: Iterable[StateTransition], ) -> List[List[StateTransition]]: """Match final and initial states in groups. Each `~qrules.transition.StateTransition` corresponds to a specific state transition amplitude. This function groups together transitions, which have the same initial and final state (including spin). This is needed to determine the coherency of the individual amplitude parts. """ transition_groups: DefaultDict[ Tuple[ Tuple[Tuple[str, float], ...], Tuple[Tuple[str, float], ...], ], List[StateTransition], ] = defaultdict(list) for transition in transitions: initial_state = sorted( ( transition.states[i].particle.name, transition.states[i].spin_projection, ) for i in transition.topology.incoming_edge_ids ) final_state = sorted( ( transition.states[i].particle.name, transition.states[i].spin_projection, ) for i in transition.topology.outgoing_edge_ids ) group_key = (tuple(initial_state), tuple(final_state)) transition_groups[group_key].append(transition) return list(transition_groups.values())
def _generate_kinematic_variable_set( transition: StateTransition, node_id: int ) -> TwoBodyKinematicVariableSet: decay = TwoBodyDecay.from_transition(transition, node_id) inv_mass, phi, theta = _generate_kinematic_variables(transition, node_id) child1_mass = sp.Symbol( get_invariant_mass_label(transition.topology, decay.children[0].id), real=True, ) child2_mass = sp.Symbol( get_invariant_mass_label(transition.topology, decay.children[1].id), real=True, ) return TwoBodyKinematicVariableSet( incoming_state_mass=inv_mass, outgoing_state_mass1=child1_mass, outgoing_state_mass2=child2_mass, helicity_theta=theta, helicity_phi=phi, angular_momentum=decay.extract_angular_momentum(), ) def _generate_kinematic_variables( transition: StateTransition, node_id: int ) -> Tuple[sp.Symbol, sp.Symbol, sp.Symbol]: """Generate symbol for invariant mass, phi angle, and theta angle.""" decay = TwoBodyDecay.from_transition(transition, node_id) phi_label, theta_label = get_helicity_angle_label( transition.topology, decay.children[0].id ) inv_mass_label = get_invariant_mass_label( transition.topology, decay.parent.id ) return ( sp.Symbol(inv_mass_label, real=True), sp.Symbol(phi_label, real=True), sp.Symbol(theta_label, real=True), ) # https://github.com/sympy/sympy/issues/21001 # pylint: disable=protected-access, unused-argument def _latex_fix(self: Type[CG], printer: LatexPrinter, *args: Any) -> str: j3, m3, j1, m1, j2, m2 = map( printer._print, (self.j3, self.m3, self.j1, self.m1, self.j2, self.m2), ) return f"{{C^{{{j3},{m3}}}_{{{j1},{m1},{j2},{m2}}}}}" CG._latex = _latex_fix