pub struct WangLandauAdaptive<Hist, R, E, S, Res, Energy> { /* private fields */ }
Expand description

Adaptive WangLandau 1/t

  • please cite

Yannick Feld and Alexander K. Hartmann, “Large-deviations of the basin stability of power grids,” Chaos 29:113113 (2019), DOI 10.1063/1.5121415

as this adaptive approach was first used and described in this paper. Also cite the following

  • The 1/t Wang Landau approach comes from this paper

R. E. Belardinelli and V. D. Pereyra, Fast algorithm to calculate density of states,” Phys. Rev. E 75: 046701 (2007), DOI 10.1103/PhysRevE.75.046701

  • The original Wang Landau algorithm comes from this paper

F. Wang and D. P. Landau, “Efficient, multiple-range random walk algorithm to calculate the density of states,” Phys. Rev. Lett. 86, 2050–2053 (2001), DOI 10.1103/PhysRevLett.86.2050

Implementations

Check if self is initialized
  • if this returns true, you can begin the WangLandau simulation
  • otherwise call one of the self.init* methods

Is the simulation in the process of rebuilding the statistics, i.e., is it currently trying many different step sizes?

Is the simulation has finished the process of rebuilding the statistics, i.e., is it currently not trying many different step sizes

Tracks progress
  • tracks progress until self.is_rebuilding_statistics becomes false
  • returned value is always 0 <= val <= 1.0
Fraction of steps accepted since the statistics were reset the last time
  • (steps accepted since last reset) / (steps since last reset)
Estimate accept/reject statistics
  • contains list of estimated probabilities for accepting a step of corresponding step size
  • list[i] corresponds to step size i + self.min_step
  • O(trial_step_max - trial_step_min)
  • samples_per_trial - how often a specific step_size should be tried before estimating the fraction of accepted steps resulting from the stepsize
  • This number was used to create a trial list of appropriate length
New WangLandauAdaptive
  • log_f_threshold - threshold for the simulation
  • ensemble ensemble used for the simulation
  • rng - random number generator used
  • samples_per_trial - how often a specific step_size should be tried before estimating the fraction of accepted steps resulting from the stepsize
  • trial_step_min and trial_step_max: The step sizes tried are: [trial_step_min, trial_step_min + 1, …, trial_step_max]
  • min_best_of_count: After estimating, use at least the best min_best_of_count step sizes found
  • best_of_threshold: After estimating, use all steps for which abs(acceptance_rate -0.5) <= best_of_threshold holds true
  • histogram: How your energy will be binned etc
  • check_refine_every: how often to check if log_f can be refined?
Important
  • **You need to call on of the self.init* members before starting the Wang Landau simulation! - you can check with self.is_initialized()
  • Err if trial_step_max < trial_step_min
  • Err if log_f_threshold <= 0.0
Find a valid starting Point
  • if the ensemble is already at a valid starting point, the ensemble is left unchanged (as long as your energy calculation does not change the ensemble)
  • overlap - see trait HistogramIntervalDistance. Should smaller than the number of bins in your histogram. E.g. overlap = 3 if you have 200 bins
  • mid - should be something like 128u8, 0i8 or 0i16. It is very unlikely that using a type with more than 16 bit makes sense for mid
  • step_limit: Some(val) -> val is max number of steps tried, if no valid state is found, it will return an Error. None -> will loop until either a valid state is found or forever
  • alternates between greedy and interval heuristic every time a wrapping counter passes mid or U::min_value()
Parameter
  • energy_fn function calculating Some(energy) of the system or rather the Parameter of which you wish to obtain the probability distribution. Has to be the same function as used for the wang landau simulation later. If there are any states, for which the calculation is invalid, None should be returned
  • steps resulting in ensembles for which energy_fn(&mut ensemble) is None will always be rejected
Find a valid starting Point
  • if the ensemble is already at a valid starting point, the ensemble is left unchanged (as long as your energy calculation does not change the ensemble)
  • Uses overlapping intervals. Accepts a step, if the resulting ensemble is in the same interval as before, or it is in an interval closer to the target interval
Parameter
  • step_limit: Some(val) -> val is max number of steps tried, if no valid state is found, it will return an Error. None -> will loop until either a valid state is found or forever
  • energy_fn function calculating Some(energy) of the system or rather the Parameter of which you wish to obtain the probability distribution. Has to be the same function as used for the wang landau simulation later. If there are any states, for which the calculation is invalid, None should be returned
  • steps resulting in ensembles for which energy_fn(&mut ensemble) is None will always be rejected
Find a valid starting Point
  • if the ensemble is already at a valid starting point, the ensemble is left unchanged (as long as your energy calculation does not change the ensemble)
  • Uses a greedy heuristic. Performs markov steps. If that brought us closer to the target interval, the step is accepted. Otherwise it is rejected
Parameter
  • step_limit: Some(val) -> val is max number of steps tried, if no valid state is found, it will return an Error. None -> will loop until either a valid state is found or forever
  • energy_fn function calculating Some(energy) of the system or rather the Parameter of which you wish to obtain the probability distribution. Has to be the same function as used for the wang landau simulation later. If there are any states, for which the calculation is invalid, None should be returned
  • steps resulting in ensembles for which energy_fn(&mut ensemble) is None will always be rejected
Wang Landau
  • perform Wang Landau simulation
  • calls self.wang_landau_step(energy_fn) until self.is_finished() or condition(&self) is false
Important
  • You have to call one of the self.init* functions before calling this one - you can check with self.is_initialized()
  • will panic otherwise, at least in debug mode
Wang Landau Simulation
Difference

uses accumulating markov steps, i.e., it updates the Energy during the markov steps. This can be more efficient. Therefore the energy_fn now gets the state of the ensemble after the markov step &E, the step that was performed &S as well as a mutable reference to the old Energy &mut Energy which is to change

Wang Landau
  • if possible, use self.wang_landau_while() instead - it is safer
  • You have mutable access to your ensemble, which is why this function is unsafe. If you do anything, which changes the future outcome of the energy function, the results will be wrong!
  • perform Wang Landau simulation
  • calls self.wang_landau_step(energy_fn) until self.is_finished() or condition(&self) is false
Important
  • You have to call one of the self.init* functions before calling this one - you can check with self.is_initialized()
  • will panic otherwise, at least in debug mode
Wang Landau
  • perform Wang Landau simulation
  • calls self.wang_landau_step(energy_fn, valid_ensemble) until self.is_finished()
Important
  • You have to call one of the self.init* functions before calling this one - you can check with self.is_initialized()
  • will panic otherwise, at least in debug mode
Wang Landau simulation
Difference

uses accumulating markov steps, i.e., it updates the Energy during the markov steps. This can be more efficient. Therefore the energy_fn now gets the state of the ensemble after the markov step &E, the step that was performed &S as well as a mutable reference to the old Energy &mut Energy which is to change

Wang Landau
  • if possible, use self.wang_landau_convergence() instead - it is safer
  • You have mutable access to your ensemble, which is why this function is unsafe. If you do anything, which changes the future outcome of the energy function, the results will be wrong!
  • perform Wang Landau simulation
  • calls self.wang_landau_step_unsafe(energy_fn, valid_ensemble) until self.is_finished()
Important
  • You have to call one of the self.init* functions before calling this one - you can check with self.is_initialized()
  • will panic otherwise, at least in debug mode
Wang Landau Step
  • performs a single Wang Landau step
Parameter
  • energy_fn function calculating Some(energy) of the system or rather the Parameter of which you wish to obtain the probability distribution. If there are any states, for which the calculation is invalid, None should be returned
  • steps resulting in ensembles for which energy_fn(&mut ensemble) is None will always be rejected
Important
  • You have to call one of the self.init* functions before calling this one - you can check with self.is_initialized()
  • will panic otherwise, at least in debug mode
Wang Landau Step
  • if possible, use self.wang_landau_step() instead - it is safer
  • unsafe, because you have to make sure, that the energy_fn function does not change the state of the ensemble in such a way, that the result of energy_fn changes when called again. Maybe do cleanup at the beginning of the energy function?
  • performs a single Wang Landau step
Parameter
  • energy_fn function calculating Some(energy) of the system or rather the Parameter of which you wish to obtain the probability distribution. If there are any states, for which the calculation is invalid, None should be returned
  • steps resulting in ensembles for which energy_fn(&mut ensemble) is None will always be rejected
Important
  • You have to call one of the self.init* functions before calling this one - you can check with self.is_initialized()
  • will panic otherwise, at least in debug mode
Accumulating wang landau step
Difference
  • this uses accumulating markov steps, i.e., it calculates the Energy during each markov step, which can be more efficient. This assumes, that cloning the Energy is cheap, which is true for primitive types like usize or f64
  • parameter of energy_fn: &E Ensemble after the markov step &S was performed. &mut Energy is the old energy, which has to be changed to the new energy of the system

Trait Implementations

Returns a copy of the value. Read more
Performs copy-assignment from source. Read more
Formats the value using the given formatter. Read more
Deserialize this value from the given Serde deserializer. Read more
Serialize this value into the given Serde serializer. Read more

Uses as stepsize: first entry of bestof. If bestof is empty, it uses wl.min_step_size() + (wl.max_step_size() - wl.max_step_size()) / 2

The type returned in the event of a conversion error.
The type returned in the event of a conversion error.
Performs the conversion.
How many steps were accepted until now? Read more
How many steps were rejected until now? Read more
get current value of log_f
returns currently set threshold for log_f
Try to set the threshold. Read more
Current (non normalized) estimate of ln(P(E)) Read more
Returns current wang landau mode Read more
Counter Read more
Writes Information about the simulation to a file. E.g. How many steps were performed. Read more
Checks wang landau threshold Read more
Current (non normalized) estimate of log10(P(E)) Read more
Current (non normalized) estimate of log_base(P(E)) Read more
Counter Read more
Calculate, which fraction of steps were accepted Read more
Calculate, which fraction of steps were rejected Read more
returns the last accepted Energy calculated None if no energy was calculated yet Read more
return reference to current state of ensemble
mutable reference to current state Read more
returns current histogram Read more

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Cast to the nearest integer Read more
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