smash::Nucleus Class Reference

#include <nucleus.h>

A nucleus is a collection of particles that are initialized, before the beginning of the simulation and all have the same velocity.

Definition at line 27 of file nucleus.h.

Inheritance diagram for smash::Nucleus:

Collaboration diagram for smash::Nucleus:

Classes
struct	TestparticleConfusion

Public Member Functions
	Nucleus ()=default
	default constructor More...
	Nucleus (Configuration &config, int nTest)
	Constructor for Nucleus, that needs the configuration parameters from the inputfile and the number of testparticles. More...
	Nucleus (const std::map< PdgCode, int > &particle_list, int nTest)
virtual	~Nucleus ()=default
double	mass () const
virtual ThreeVector	distribute_nucleon ()
	The distribution of return values from this function is according to a spherically symmetric Woods-Saxon distribution suitable for this nucleus. More...
double	woods_saxon (double x)
	Woods-Saxon distribution. More...
void	arrange_nucleons ()
	Sets the positions of the nucleons inside a nucleus. More...
virtual void	set_parameters_automatic ()
	Sets the deformation parameters of the Woods-Saxon distribution according to the current mass number. More...
virtual void	set_parameters_from_config (Configuration &config)
	Sets the parameters of the Woods-Saxon according to manually added values in the configuration file. More...
virtual void	generate_fermi_momenta ()
	Generates momenta according to Fermi motion for the nucleons. More...
void	boost (double beta_scalar)
	Boosts the nuclei into the computational frame, such that the nucleons have the appropriate momentum and the nuclei are lorentz-contracted. More...
void	fill_from_list (const std::map< PdgCode, int > &particle_list, int testparticles)
	Adds particles from a map PDG code => Number_of_particles_with_that_PDG_code to the nucleus. More...
void	shift (double z_offset, double x_offset, double simulation_time)
	Shifts the nucleus to correct impact parameter and z displacement. More...
virtual void	rotate ()
	Rotates the nucleus. More...
void	copy_particles (Particles *particles)
	Copies the particles from this nucleus into the particle list. More...
size_t	size () const
	Number of numerical (=test-)particles in the nucleus: More...
size_t	number_of_particles () const
	Number of physical particles in the nucleus: More...
FourVector	center () const
	Calculate geometrical center of the nucleus. More...
void	align_center ()
	Shifts the nucleus so that its center is at (0,0,0) More...
std::vector< ParticleData >::iterator	begin ()
	For iterators over the particle list: More...
std::vector< ParticleData >::iterator	end ()
	For iterators over the particle list: More...
std::vector< ParticleData >::const_iterator	cbegin () const
	For const iterators over the particle list: More...
std::vector< ParticleData >::const_iterator	cend () const
	For const iterators over the particle list: More...
void	set_diffusiveness (double diffuse)
	Sets the diffusiveness of the nucleus. More...
double	get_diffusiveness () const
void	set_saturation_density (double density)
	Sets the saturation density of the nucleus. More...
double	get_saturation_density () const
double	default_nuclear_radius ()
void	set_nuclear_radius (double rad)
	Sets the nuclear radius. More...
double	get_nuclear_radius () const

Protected Attributes
std::vector< ParticleData >	particles_
	Particles associated with this nucleus. More...

Private Attributes
double	diffusiveness_
	Diffusiveness of Woods-Saxon distribution of this nucleus in fm (for diffusiveness_ == 0, we obtain a hard sphere). More...
double	saturation_density_ = nuclear_density
	Saturation density of this nucleus. More...
double	nuclear_radius_
	Nuclear radius of this nucleus. More...
double	proton_radius_ = 1.2
	Single proton radius in fm. More...
size_t	testparticles_ = 1
	Number of testparticles per physical particle. More...

Friends
std::ostream &	operator<< (std::ostream &, const Nucleus &)
	Writes the state of the Nucleus object to the output stream. More...

Constructor & Destructor Documentation

smash::Nucleus::Nucleus ( )

default

default constructor

smash::Nucleus::Nucleus	(	Configuration &	config,
		int	nTest
	)

Constructor for Nucleus, that needs the configuration parameters from the inputfile and the number of testparticles.

Parameters

[in]	config	contains the parameters from the inputfile on the numbers of particles with a certain PDG code
[in]	nTest	number of testparticles

Definition at line 33 of file nucleus.cc.

                                                 {
  // Fill nuclei with particles.
  std::map<PdgCode, int> part = config.take({"Particles"});
  fill_from_list(part, nTest);
  // Look for user-defined values or take the default parameters.
  if (config.has_value({"Diffusiveness"}) && config.has_value({"Radius"}) &&
      config.has_value({"Saturation_Density"})) {
    set_parameters_from_config(config);
  } else if (!config.has_value({"Diffusiveness"}) &&
             !config.has_value({"Radius"}) &&
             !config.has_value({"Saturation_Density"})) {
    set_parameters_automatic();
  } else {
    throw std::invalid_argument(
        "Diffussiveness, Radius and Saturation_Density "
        "required to manually configure the Woods-Saxon"
        " distribution. Only one/two were provided. \n"
        "Providing none of the above mentioned "
        "parameters automatically configures the "
        "distribution based on the atomic number.");
  }
}

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smash::Nucleus::Nucleus	(	const std::map< PdgCode, int > &	particle_list,
		int	nTest
	)

Definition at line 28 of file nucleus.cc.

                                                                     {
  fill_from_list(particle_list, nTest);
  set_parameters_automatic();
}

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virtual smash::Nucleus::~Nucleus ( )

virtualdefault

Member Function Documentation

double smash::Nucleus::mass

(

)

const

Returns

Mass of the nucleus [GeV]. It needs to be double to allow for calculations at LHC energies.

Definition at line 56 of file nucleus.cc.

                           {
  double total_mass = 0.;
  for (auto i = cbegin(); i != cend(); i++) {
    total_mass += i->momentum().abs();
  }
  return total_mass / (testparticles_ + 0.0);
}

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ThreeVector smash::Nucleus::distribute_nucleon ( )

virtual

The distribution of return values from this function is according to a spherically symmetric Woods-Saxon distribution suitable for this nucleus.

Woods-Saxon-distribution

\(\frac{dN}{dr} = \frac{r^2}{\exp\left(\frac{r-r_0}{d}\right) + 1}\) where \(d\) is the diffusiveness_ parameter and \(r_0\) is nuclear_radius_.

Returns

Woods-Saxon distributed position.

The distribution

Nucleons in nuclei are distributed according to a Woods-Saxon-distribution (see Woods:1954zz)

\[\frac{dN}{d^3r} = \frac{\rho_0}{\exp\left(\frac{r-r_0}{d}\right) +1},\]

where \(d\) is the diffusiveness of the nucleus. For \(d=0\), the nucleus is a hard sphere. \(\rho_0\) and \(r_0\) are, in this limit, the nuclear ground state density and nuclear radius, respectively. For small \(d\), this is still approximately true.

This distribution is obviously spherically symmetric, hence we can rewrite \(d^3r = 4\pi r^2 dr\) and obtain

\[\frac{dN}{4\pi\rho_0dr} = \frac{r^2}{\exp\left(\frac{r-r_0}{d}\right) + 1}.\]

Let us rewrite that in units of \(d\) (that's the diffusiveness) and drop any constraints on normalization (since in the end we only care about relative probabilities: we create as many nucleons as we need). Now, \(p(B)\) is the un-normalized probability to obtain a point at \(r = Bd\) (with \(R = r_0/d\)):

\[p(B) = \frac{B^2}{\exp(B-R) + 1}.\]

Splitting it up in two regimes

We shift the distribution so that \(B-R\) is 0 at \(t = 0\): \(t = B-R\):

\[p^{(1)}(t)= \frac{(t+R)^2}{\exp(t)+1}\]

and observe

\[\frac{1}{\exp(x)+1} = \frac{e^{-x}}{e^{-x}e^{x}+e^{-x}} = \frac{e^{-x}}{e^{-x}+1}.\]

The distribution function can now be split into two cases. For negative t (first case), \(-|t| = t\), and for positive t (second case), \(-|t| = -t\):

\[p^{(1)}(t) = \frac{1}{e^{-|t|}+1} \cdot (t+R)^2 \cdot \begin{cases} 1 & -R \le t < 0 \\ e^{-t} & t \ge 0 \end{cases}.\]

Apart from the first term, all that remains here can easily and exactly be generated from unrejected uniform random numbers (see below). The first term itself - \((1+e^{-|t|})^{-1}\) - is a number between 1/2 and 1.

If we now have a variable \(t\) distributed according to the remainder, \(p^{(2)}(t)\), and reject \(t\) with a probability \(p^{(rej)}(t) = 1 - p^{(survive)}(t) = 1 - (1+e^{-|t|})^{-1}\), the resulting distribution is \(p^{(combined)}(t) = p^{(2)}(t) \cdot p^{(survive)}(t)\). Hence, we need to generate \(p^{(2)}(t)\), which we can normalize to

\[\tilde{p}^{(2)}(t) = \frac{1}{1+3/R+6/R^2+6/R^3} \cdot \begin{cases} \frac{3}{R^3} (t+R)^2 & -R \le t < 0 \\ e^{-t} \left( \frac{3}{R}+\frac{6}{R^2}t+\frac{6}{R^3}\frac{1}{2}t^2 \right) & t \ge 0 \end{cases}.\]

(the tilde \(\tilde{p}\) means that this is normalized).

Four parts inside the rejection

Let \(c_1 = 1+3/R+6/R^2+6/R^3\). The above means:

\[\mbox{Choose: } \begin{cases} \tilde p^{({\rm I})} = \frac{3}{R^3}(t+R)^2 \Theta(-t) \Theta(t+R) \\ \tilde p^{({\rm II})}= e^{-t}\Theta(t) \\ \tilde p^{({\rm III})}=e^{-t}\Theta(t) t \\ \tilde p^{({\rm IV})} =e^{-t}\Theta(t) \frac{1}{2} t^2 \end{cases} \mbox{ with a probability of }\begin{cases} \frac{1}{c_1} \cdot 1 \\ \frac{1}{c_1} \cdot \frac{3}{R} \\ \frac{1}{c_1} \cdot \frac{6}{R^2} \\ \frac{1}{c_1} \cdot \frac{6}{R^3} \end{cases}.\]

Let us see how those are generated. \(\chi_i\) are uniformly distributed numbers between 0 and 1.

\[p(\chi_i) = \Theta(\chi_i)\Theta(1-\chi_i)\]

For simple distributions (only one \(\chi\) involved), we invert \(t(\chi)\), derive it w.r.t. \(t\) and normalize.

Case I: \(p^{({\rm I})}\)

Simply from one random number:

\[t = R\left( \sqrt[ 3 ]{\chi} - 1 \right)\]

\[\tilde p^{({\rm I})} = \frac{3}{R^3}(t+R)^2 \mbox{ for } -R \le t \le 0\]

Case II: \(p^{({\rm II})}\)

Again, from one only:

\[t = -\log(\chi)\]

\[p(t) = \frac{d\chi}{dt}\]

\[p^{({\rm II})} = e^{-t} \mbox{ for } t > 0\]

Case III: \(p^{({\rm III})}\)

Here, we need two variables:

\[t = -\log{\chi_1} -\log{\chi_2}\]

\(p^{({\rm III})}\) is now the folding of \(p^{({\rm II})}\) with itself[1]:

\[p^{({\rm III})} = \int_{-\infty}^{\infty} d\tau e^{-\tau} e^{-(t-\tau)} \Theta(\tau) \Theta(t-\tau) = t e^{-t} \mbox{ for } t > 0\]

Case IV: \(p^{({\rm IV})}\)

Three variables needed:

\[t = -\log{\chi_1} -\log{\chi_2} -\log{\chi_3}\]

\(p^{({\rm IV})}\) is now the folding of \(p^{({\rm II})}\) with \(p^{({\rm III})}\):

\[p^{({\rm IV})} = \int_{ - \infty}^{\infty} d\tau e^{- \tau} \left( t - \tau \right) e^{ - (t - \tau)} \Theta(\tau) \Theta(t - \tau) = \frac{1}{2} t^2 e^{ -t} \mbox{ for } t > 0\]

[1]: This is [the probability to find a \(\tau\)] times [the probability to find the value \(\tau_2 = t-\tau\) that added to \(\tau\) yields \(t\)], integrated over all possible combinations that have that property.

From the beginning

So, the algorithm needs to do all this from the end:

• Decide which branch \(\tilde p^{({\rm I - IV})}\) to go into

• Generate \(t\) from the distribution in the respective branches
• Reject that number with a probability \(1-(1+\exp(-|t|))^{-1}\) (the efficiency of this should be \(\gg \frac{1}{2}\))

• Shift and rescale \(t\) to \(r = d\cdot t + r_0\)

Reimplemented in smash::CustomNucleus, and smash::DeformedNucleus.

Definition at line 216 of file nucleus.cc.

                                        {
  // Get the solid angle of the nucleon.
  Angles dir;
  dir.distribute_isotropically();
  // diffusiveness_ zero or negative? Use hard sphere.
  if (almost_equal(diffusiveness_, 0.)) {
    return dir.threevec() * nuclear_radius_ * std::cbrt(random::canonical());
  }
  if (almost_equal(nuclear_radius_, 0.)) {
    return smash::ThreeVector();
  }
  double radius_scaled = nuclear_radius_ / diffusiveness_;
  double prob_range1 = 1.0;
  double prob_range2 = 3. / radius_scaled;
  double prob_range3 = 2. * prob_range2 / radius_scaled;
  double prob_range4 = 1. * prob_range3 / radius_scaled;
  double ranges234 = prob_range2 + prob_range3 + prob_range4;
  double t;
  do {
    double which_range = random::uniform(-prob_range1, ranges234);
    if (which_range < 0.0) {
      t = radius_scaled * (std::cbrt(random::canonical()) - 1.);
    } else {
      t = -std::log(random::canonical());
      if (which_range >= prob_range2) {
        t -= std::log(random::canonical());
        if (which_range >= prob_range2 + prob_range3) {
          t -= std::log(random::canonical());
        }
      }
    }
  } while (random::canonical() > 1. / (1. + std::exp(-std::abs(t))));
  double position_scaled = t + radius_scaled;
  double position = position_scaled * diffusiveness_;
  return dir.threevec() * position;
}

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double smash::Nucleus::woods_saxon

(

double

x

)

Woods-Saxon distribution.

Parameters

[in]

x

the position at which to evaluate the function

Returns

un-normalized Woods-saxon probability

Definition at line 262 of file nucleus.cc.

                                    {
  return r * r / (std::exp((r - nuclear_radius_) / diffusiveness_) + 1);
}

void smash::Nucleus::arrange_nucleons

(

)

Sets the positions of the nucleons inside a nucleus.

Definition at line 266 of file nucleus.cc.

                               {
  for (auto i = begin(); i != end(); i++) {
    // Initialize momentum
    i->set_4momentum(i->pole_mass(), 0.0, 0.0, 0.0);
    /* Sampling the Woods-Saxon, get the radial
     * position and solid angle for the nucleon. */
    ThreeVector pos = distribute_nucleon();

    // Set the position of the nucleon.
    i->set_4position(FourVector(0.0, pos));
  }

  // Recenter and rotate
  align_center();
  rotate();
}

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void smash::Nucleus::set_parameters_automatic ( )

virtual

Sets the deformation parameters of the Woods-Saxon distribution according to the current mass number.

The values are taken from DeJager:1987qc. They are in agreement with MC-Glauber models such as GLISSANDO (see Rybczynski:2013yba) and TGlauber MC (see Loizides:2017ack)

Definition at line 283 of file nucleus.cc.

                                       {
  int A = Nucleus::number_of_particles();
  switch (A) {
    case 1:  // single particle
      /* In case of testparticles, an infinite reaction loop will be
       * avoided by a small finite spread according to a single particles
       * 'nucleus'. The proper solution will be to introduce parallel
       * ensembles. */
      set_nuclear_radius(testparticles_ == 1
                             ? 0.
                             : 1. - std::exp(-(testparticles_ - 1.) * 0.1));
      set_diffusiveness(testparticles_ == 1 ? -1. : 0.02);
      break;
    case 238:  // Uranium
      // Default values.
      set_diffusiveness(0.556);
      set_nuclear_radius(6.86);
      set_saturation_density(0.166);
      break;
    case 208:  // Lead
      // Default values.
      set_diffusiveness(0.54);
      set_nuclear_radius(6.67);
      set_saturation_density(0.161);
      break;
    case 197:  // Gold
      // Default values.
      set_diffusiveness(0.535);
      set_nuclear_radius(6.38);
      set_saturation_density(0.1695);
      break;
    case 63:  // Copper
      // Default values.
      set_diffusiveness(0.5977);
      set_nuclear_radius(4.20641);
      set_saturation_density(0.1686);
      break;
    default:
      if (A <= 16) {
        // radius: rough guess for all nuclei not listed explicitly with A <= 16
        // saturation density already has reasonable default
        set_nuclear_radius(1.2 * std::cbrt(A));
        set_diffusiveness(0.545);
      } else {
        // radius and diffusiveness taken from \iref{Rybczynski:2013yba}
        set_diffusiveness(0.54);
        set_nuclear_radius(1.12 * std::pow(A, 1.0 / 3.0) -
                           0.86 * std::pow(A, -1.0 / 3.0));
      }
  }
}

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void smash::Nucleus::set_parameters_from_config ( Configuration &  config )

virtual

Sets the parameters of the Woods-Saxon according to manually added values in the configuration file.

Parameters

config

The configuration for this nucleus (projectile or target).

Definition at line 335 of file nucleus.cc.

                                                              {
  set_diffusiveness(static_cast<double>(config.take({"Diffusiveness"})));
  set_nuclear_radius(static_cast<double>(config.take({"Radius"})));
  // Saturation density (normalization for accept/reject sampling)
  set_saturation_density(
      static_cast<double>(config.take({"Saturation_Density"})));
}

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void smash::Nucleus::generate_fermi_momenta ( )

virtual

Generates momenta according to Fermi motion for the nucleons.

For neutrons and protons Fermi momenta are calculated as \( p_{F} = (3 \pi^2 \rho)^{1/3}\), where \( rho \) is neutron density for neutrons and proton density for protons. The actual momenta \(p_x\), \(p_y\), \(p_z\) are uniformly distributed in the sphere with radius \(p_F\).

Reimplemented in smash::DeformedNucleus.

Definition at line 343 of file nucleus.cc.

                                     {
  const int N_n = std::count_if(begin(), end(), [](const ParticleData i) {
    return i.pdgcode() == pdg::n;
  });
  const int N_p = std::count_if(begin(), end(), [](const ParticleData i) {
    return i.pdgcode() == pdg::p;
  });
  const FourVector nucleus_center = center();
  const int A = N_n + N_p;
  constexpr double pi2_3 = 3.0 * M_PI * M_PI;
  const auto &log = logger<LogArea::Nucleus>();

  log.debug() << N_n << " neutrons, " << N_p << " protons.";

  ThreeVector ptot = ThreeVector(0.0, 0.0, 0.0);
  for (auto i = begin(); i != end(); i++) {
    // Only protons and neutrons get Fermi momenta
    if (i->pdgcode() != pdg::p && i->pdgcode() != pdg::n) {
      if (i->is_baryon()) {
        log.warn() << "No rule to calculate Fermi momentum "
                   << "for particle " << i->pdgcode();
      }
      continue;
    }
    const double r = (i->position() - nucleus_center).abs3();
    double rho = nuclear_density /
                 (std::exp((r - nuclear_radius_) / diffusiveness_) + 1.);
    if (i->pdgcode() == pdg::p) {
      rho = rho * N_p / A;
    }
    if (i->pdgcode() == pdg::n) {
      rho = rho * N_n / A;
    }
    const double p =
        hbarc * std::pow(pi2_3 * rho * random::uniform(0.0, 1.0), 1.0 / 3.0);
    Angles phitheta;
    phitheta.distribute_isotropically();
    const ThreeVector ith_3momentum = phitheta.threevec() * p;
    ptot += ith_3momentum;
    i->set_3momentum(ith_3momentum);
    log.debug() << "Particle: " << *i
                << ", pF[GeV]: " << hbarc * std::pow(pi2_3 * rho, 1.0 / 3.0)
                << " r[fm]: " << r
                << " Nuclear radius[fm]: " << nuclear_radius_;
  }
  if (A == 0) {
    // No Fermi momenta should be assigned
    assert(ptot.x1() == 0.0 && ptot.x2() == 0.0 && ptot.x3() == 0.0);
  } else {
    /* Ensure zero total momentum of nucleus - redistribute ptot equally
     * among protons and neutrons */
    const ThreeVector centralizer = ptot / A;
    for (auto i = begin(); i != end(); i++) {
      if (i->pdgcode() == pdg::p || i->pdgcode() == pdg::n) {
        i->set_4momentum(i->pole_mass(),
                         i->momentum().threevec() - centralizer);
      }
    }
  }
}

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void smash::Nucleus::boost

(

double

beta_scalar

)

Boosts the nuclei into the computational frame, such that the nucleons have the appropriate momentum and the nuclei are lorentz-contracted.

Note that the usual boost cannot be applied for nuclei, since the particles would end up with different times and the binding energy needs to be taken into account.

Parameters

[in]

beta_scalar

velocity in z-direction used for boost.

Definition at line 404 of file nucleus.cc.

                                      {
  double beta_squared = beta_scalar * beta_scalar;
  double one_over_gamma = std::sqrt(1.0 - beta_squared);
  double gamma = 1.0 / one_over_gamma;
  /* We are talking about a /passive/ lorentz transformation here, as
   * far as I can see, so we need to boost in the direction opposite to
   * where we want to go
   *     ( The vector we transform - p - stays unchanged, but we go into
   *       a system that moves with -beta. Now in this frame, it seems
   *       like p has been accelerated with +beta.
   *     ) */
  for (auto i = begin(); i != end(); i++) {
    /* a real Lorentz Transformation would leave the particles at
     * different times here, which we would then have to propagate back
     * to equal times. Since we know the result, we can simply multiply
     * the z-value with 1/gamma. */
    FourVector this_position = i->position();
    this_position.set_x3(this_position.x3() * one_over_gamma);
    i->set_4position(this_position);
    /* The simple Lorentz transformation of momenta does not take into account
     * that nucleus has binding energy. Here we apply the method used
     * in the JAM code \iref{Nara:1999dz}: p' = p_beam + gamma*p_F.
     * This formula is derived under assumption that all nucleons have
     * the same binding energy. */
    FourVector mom_i = i->momentum();
    i->set_4momentum(i->pole_mass(), mom_i.x1(), mom_i.x2(),
                     gamma * (beta_scalar * mom_i.x0() + mom_i.x3()));
  }
}

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void smash::Nucleus::fill_from_list	(	const std::map< PdgCode, int > &	particle_list,
		int	testparticles
	)

Adds particles from a map PDG code => Number_of_particles_with_that_PDG_code to the nucleus.

E.g., the map [2212: 6, 2112: 7] initializes C-13 (6 protons and 7 neutrons). The particles are only created, no position or momenta are yet assigned. It is also possible to use any other PDG code, in addition to nucleons.

Parameters

[out]	particle_list	The particle slots that are created.
[in]	testparticles	Number of test particles to use.

Definition at line 434 of file nucleus.cc.

                                                {
  testparticles_ = testparticles;
  for (auto n = particle_list.cbegin(); n != particle_list.cend(); ++n) {
    const ParticleType &current_type = ParticleType::find(n->first);
    double current_mass = current_type.mass();
    for (unsigned int i = 0; i < n->second * testparticles_; i++) {
      // append particle to list and set its PDG code.
      particles_.emplace_back(current_type);
      particles_.back().set_4momentum(current_mass, 0.0, 0.0, 0.0);
    }
  }
}

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void smash::Nucleus::shift	(	double	z_offset,
		double	x_offset,
		double	simulation_time
	)

Shifts the nucleus to correct impact parameter and z displacement.

Parameters

[in]	z_offset	is the shift in z-direction
[in]	x_offset	is the shift in x-direction
[in]	simulation_time	set the time and formation_time of each particle to this value.

Definition at line 448 of file nucleus.cc.

                                                                            {
  // Move the nucleus in z and x directions, and set the time.
  for (auto i = begin(); i != end(); i++) {
    FourVector this_position = i->position();
    this_position.set_x3(this_position.x3() + z_offset);
    this_position.set_x1(this_position.x1() + x_offset);
    this_position.set_x0(simulation_time);
    i->set_4position(this_position);
    i->set_formation_time(simulation_time);
  }
}

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virtual void smash::Nucleus::rotate ( )

inlinevirtual

Rotates the nucleus.

(Due to spherical symmetry of nondeformed nuclei, there is nothing to do.)

Reimplemented in smash::DeformedNucleus.

Definition at line 137 of file nucleus.h.

{}

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void smash::Nucleus::copy_particles

(

Particles *

particles

)

Copies the particles from this nucleus into the particle list.

Parameters

[out]

particles

Particle list with all constituents of a nucleus

Definition at line 460 of file nucleus.cc.

                                                          {
  for (auto p = begin(); p != end(); p++) {
    external_particles->insert(*p);
  }
}

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size_t smash::Nucleus::size ( ) const

inline

Number of numerical (=test-)particles in the nucleus:

Definition at line 147 of file nucleus.h.

{ return particles_.size(); }

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size_t smash::Nucleus::number_of_particles ( ) const

inline

Number of physical particles in the nucleus:

Exceptions

TestparticleConfusion

if the number of the nucleons is not a multiple of testparticles_.

Definition at line 155 of file nucleus.h.

                                            {
    size_t nop = particles_.size() / testparticles_;
    /* if size() is not a multiple of testparticles_, this will throw an
     * error. */
    if (nop * testparticles_ != particles_.size()) {
      throw TestparticleConfusion(
          "Number of test particles and test particles"
          "per particle are incompatible");
    }
    return nop;
  }

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FourVector smash::Nucleus::center

(

)

const

Calculate geometrical center of the nucleus.

Returns

\(\vec r_s = \frac{1}{N} \sum_{i=1}^N \vec r_i\) (for a nucleus with N particles that are at the positions \(\vec r_i\)).

Definition at line 466 of file nucleus.cc.

                                 {
  FourVector centerpoint(0.0, 0.0, 0.0, 0.0);
  for (auto p = cbegin(); p != cend(); p++) {
    centerpoint += p->position();
  }
  centerpoint /= size();
  return centerpoint;
}

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void smash::Nucleus::align_center ( )

inline

Shifts the nucleus so that its center is at (0,0,0)

See also

center()

Definition at line 178 of file nucleus.h.

                      {
    FourVector centerpoint = center();
    for (auto p = particles_.begin(); p != particles_.end(); ++p) {
      p->set_4position(p->position() - centerpoint);
    }
  }

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std::vector<ParticleData>::iterator smash::Nucleus::begin ( )

inline

For iterators over the particle list:

Definition at line 214 of file nucleus.h.

                                                 {
    return particles_.begin();
  }

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std::vector<ParticleData>::iterator smash::Nucleus::end ( )

inline

For iterators over the particle list:

Definition at line 218 of file nucleus.h.

{ return particles_.end(); }

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std::vector<ParticleData>::const_iterator smash::Nucleus::cbegin ( ) const

inline

For const iterators over the particle list:

Definition at line 220 of file nucleus.h.

                                                              {
    return particles_.cbegin();
  }

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std::vector<ParticleData>::const_iterator smash::Nucleus::cend ( ) const

inline

For const iterators over the particle list:

Definition at line 224 of file nucleus.h.

                                                            {
    return particles_.cend();
  }

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void smash::Nucleus::set_diffusiveness ( double  diffuse )

inline

Sets the diffusiveness of the nucleus.

See also

diffusiveness_

Definition at line 231 of file nucleus.h.

{ diffusiveness_ = diffuse; }

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double smash::Nucleus::get_diffusiveness ( ) const

inline

Returns

the diffusiveness of the nucleus

See also

diffusiveness_

Definition at line 236 of file nucleus.h.

{ return diffusiveness_; }

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void smash::Nucleus::set_saturation_density ( double  density )

inline

Sets the saturation density of the nucleus.

See also

saturation_density_

Definition at line 241 of file nucleus.h.

                                                     {
    saturation_density_ = density;
  }

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double smash::Nucleus::get_saturation_density ( ) const

inline

Returns

the saturation density of the nucleus

See also

saturation_density_

Definition at line 248 of file nucleus.h.

{ return saturation_density_; }

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double smash::Nucleus::default_nuclear_radius ( )

inline

Returns

a default radius for the nucleus Nuclear radius is calculated with the proton radius times the third root of the number of nucleons.

Definition at line 254 of file nucleus.h.

                                         {
    return proton_radius_ * std::pow(number_of_particles(), 1. / 3.);
  }

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void smash::Nucleus::set_nuclear_radius ( double  rad )

inline

Sets the nuclear radius.

See also

nuclear_radius

Definition at line 261 of file nucleus.h.

{ nuclear_radius_ = rad; }

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double smash::Nucleus::get_nuclear_radius ( ) const

inline

Returns

the nuclear radius

See also

nuclear_radius

Definition at line 266 of file nucleus.h.

{ return nuclear_radius_; }

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Member Data Documentation

double smash::Nucleus::diffusiveness_

private

Diffusiveness of Woods-Saxon distribution of this nucleus in fm (for diffusiveness_ == 0, we obtain a hard sphere).

Definition at line 195 of file nucleus.h.

double smash::Nucleus::saturation_density_ = nuclear_density

private

Saturation density of this nucleus.

Definition at line 197 of file nucleus.h.

double smash::Nucleus::nuclear_radius_

private

Nuclear radius of this nucleus.

Definition at line 199 of file nucleus.h.

double smash::Nucleus::proton_radius_ = 1.2

private

Single proton radius in fm.

See also

default_nuclear_radius

Definition at line 204 of file nucleus.h.

size_t smash::Nucleus::testparticles_ = 1

private

Number of testparticles per physical particle.

Definition at line 206 of file nucleus.h.

std::vector<ParticleData> smash::Nucleus::particles_

protected

Particles associated with this nucleus.

Definition at line 210 of file nucleus.h.

---

The documentation for this class was generated from the following files:

• src/include/smash/nucleus.h
• src/nucleus.cc