tensorflow_probability/python/mcmc/slice_sampler_kernel.py
def _sample_next(target_log_prob_fn,
                 current_state_parts,
                 step_sizes,
                 max_doublings,
                 current_target_log_prob,
                 batch_rank,
                 seed=None,
                 name=None):
  """Applies a single iteration of slice sampling update.

  Applies hit and run style slice sampling. Chooses a uniform random direction
  on the unit sphere in the event space. Applies the one dimensional slice
  sampling update along that direction.

  Args:
    target_log_prob_fn: Python callable which takes an argument like
      `*current_state_parts` and returns its (possibly unnormalized) log-density
      under the target distribution.
    current_state_parts: Python `list` of `Tensor`s representing the current
      state(s) of the Markov chain(s). The first `independent_chain_ndims` of
      the `Tensor`(s) index different chains.
    step_sizes: Python `list` of `Tensor`s. Provides a measure of the width
      of the density. Used to find the slice bounds. Must broadcast with the
      shape of `current_state_parts`.
    max_doublings: Integer number of doublings to allow while locating the slice
      boundaries.
    current_target_log_prob: `Tensor` representing the value of
      `target_log_prob_fn(*current_state_parts)`. The only reason to specify
      this argument is to reduce TF graph size.
    batch_rank: Integer. The number of axes in the state that correspond to
      independent batches.
    seed: Python integer to seed random number generators.
    name: Python `str` name prefixed to Ops created by this function.
      Default value: `None` (i.e., 'find_slice_bounds').

  Returns:
    proposed_state_parts: Tensor or Python list of `Tensor`s representing the
      state(s) of the Markov chain(s) at each result step. Has same shape as
      input `current_state_parts`.
    proposed_target_log_prob: `Tensor` representing the value of
      `target_log_prob_fn` at `next_state`.
    bounds_satisfied: Boolean `Tensor` of the same shape as the log density.
      True indicates whether the an interval containing the slice for that
      batch was found successfully.
    direction: `Tensor` or Python list of `Tensors`s representing the direction
      along which the slice was sampled. Has the same shape and dtype(s) as
      `current_state_parts`.
    upper_bounds: `Tensor` of batch shape and the dtype of the input state. The
      upper bounds of the slices along the sampling direction.
    lower_bounds: `Tensor` of batch shape and the dtype of the input state. The
      lower bounds of the slices along the sampling direction.
  """
  with tf.compat.v1.name_scope(name, 'sample_next', [
      current_state_parts, step_sizes, max_doublings, current_target_log_prob,
      batch_rank
  ]):
    # First step: Choose a random direction.
    # Direction is a list of tensors. The i'th tensor should have the same shape
    # as the i'th state part.
    direction = _choose_random_direction(current_state_parts,
                                         batch_rank=batch_rank,
                                         seed=seed)

    # Interpolates the step sizes for the chosen direction.
    # Applies an ellipsoidal interpolation to compute the step direction for
    # the chosen direction. Suppose we are given step sizes for each direction.
    # Label these s_1, s_2, ... s_k. These are the step sizes to use if moving
    # in a direction parallel to one of the axes. Consider an ellipsoid which
    # intercepts the i'th axis at s_i. The step size for a direction specified
    # by the unit vector (n_1, n_2 ...n_k) is then defined as the intersection
    # of the line through this vector with this ellipsoid.
    #
    # One can show that the length of the vector from the origin to the
    # intersection point is given by:
    # 1 / sqrt(n_1^2 / s_1^2  + n_2^2 / s_2^2  + ...).
    #
    # Proof:
    # The equation of the ellipsoid is:
    # Sum_i [x_i^2 / s_i^2 ] = 1. Let n be a unit direction vector. Points
    # along the line given by n may be parameterized as alpha*n where alpha is
    # the distance along the vector. Plugging this into the equation for the
    # ellipsoid, we get:
    # alpha^2 ( n_1^2 / s_1^2 + n_2^2 / s_2^2 + ...) = 1
    # so alpha = \sqrt { \frac{1} { ( n_1^2 / s_1^2 + n_2^2 / s_2^2 + ...) } }
    reduce_axes = [tf.range(batch_rank, tf.rank(dirn_part))
                   for dirn_part in direction]

    components = [
        tf.reduce_sum(
            input_tensor=(dirn_part / step_size)**2, axis=reduce_axes[i])
        for i, (step_size, dirn_part) in enumerate(zip(step_sizes, direction))
    ]
    step_size = tf.math.rsqrt(tf.add_n(components))
    # Computes the rank of a tensor. Uses the static rank if possible.
    def _get_rank(x):
      return (len(x.shape.as_list()) if x.shape.dims is not None
              else tf.rank(x))
    state_part_ranks = [_get_rank(part) for part in current_state_parts]

    def _step_along_direction(alpha):
      """Converts the scalar alpha into an n-dim vector with full state info.

      Computes x_0 + alpha * direction where x_0 is the current state and
      direction is the direction chosen above.

      Args:
        alpha: A tensor of shape equal to the batch dimensions of
          `current_state_parts`.

      Returns:
        state_parts: Tensor or Python list of `Tensor`s representing the
          state(s) of the Markov chain(s) for a given alpha and a given chosen
          direction. Has the same shape as `current_state_parts`.
      """
      padded_alphas = [_right_pad(alpha, final_rank=part_rank)
                       for part_rank in state_part_ranks]

      state_parts = [state_part + padded_alpha
                     * direction_part for state_part, direction_part,
                     padded_alpha in
                     zip(current_state_parts, direction, padded_alphas)]
      return state_parts

    def projected_target_log_prob_fn(alpha):
      """The target log density projected along the chosen direction.

      Args:
        alpha: A tensor of shape equal to the batch dimensions of
          `current_state_parts`.

      Returns:
        Target log density evaluated at x_0 + alpha * direction where x_0 is the
        current state and direction is the direction chosen above. Has the same
        shape as `alpha`.
      """
      return target_log_prob_fn(*_step_along_direction(alpha))

    alpha_init = tf.zeros_like(current_target_log_prob,
                               dtype=current_state_parts[0].dtype.base_dtype)
    [
        next_alpha,
        next_target_log_prob,
        bounds_satisfied,
        upper_bounds,
        lower_bounds
    ] = ssu.slice_sampler_one_dim(projected_target_log_prob_fn,
                                  x_initial=alpha_init,
                                  max_doublings=max_doublings,
                                  step_size=step_size, seed=seed)
    return [
        _step_along_direction(next_alpha),
        next_target_log_prob,
        bounds_satisfied,
        direction,
        upper_bounds,
        lower_bounds
    ]
def _sample_next(target_log_prob_fn,
                 current_state_parts,
                 step_sizes,
                 max_doublings,
                 current_target_log_prob,
                 batch_rank,
                 seed=None,
                 name=None):
  """Applies a single iteration of slice sampling update.

  Applies hit and run style slice sampling. Chooses a uniform random direction
  on the unit sphere in the event space. Applies the one dimensional slice
  sampling update along that direction.

  Args:
    target_log_prob_fn: Python callable which takes an argument like
      `*current_state_parts` and returns its (possibly unnormalized) log-density
      under the target distribution.
    current_state_parts: Python `list` of `Tensor`s representing the current
      state(s) of the Markov chain(s). The first `independent_chain_ndims` of
      the `Tensor`(s) index different chains.
    step_sizes: Python `list` of `Tensor`s. Provides a measure of the width
      of the density. Used to find the slice bounds. Must broadcast with the
      shape of `current_state_parts`.
    max_doublings: Integer number of doublings to allow while locating the slice
      boundaries.
    current_target_log_prob: `Tensor` representing the value of
      `target_log_prob_fn(*current_state_parts)`. The only reason to specify
      this argument is to reduce TF graph size.
    batch_rank: Integer. The number of axes in the state that correspond to
      independent batches.
    seed: Python integer to seed random number generators.
    name: Python `str` name prefixed to Ops created by this function.
      Default value: `None` (i.e., 'find_slice_bounds').

  Returns:
    proposed_state_parts: Tensor or Python list of `Tensor`s representing the
      state(s) of the Markov chain(s) at each result step. Has same shape as
      input `current_state_parts`.
    proposed_target_log_prob: `Tensor` representing the value of
      `target_log_prob_fn` at `next_state`.
    bounds_satisfied: Boolean `Tensor` of the same shape as the log density.
      True indicates whether the an interval containing the slice for that
      batch was found successfully.
    direction: `Tensor` or Python list of `Tensors`s representing the direction
      along which the slice was sampled. Has the same shape and dtype(s) as
      `current_state_parts`.
    upper_bounds: `Tensor` of batch shape and the dtype of the input state. The
      upper bounds of the slices along the sampling direction.
    lower_bounds: `Tensor` of batch shape and the dtype of the input state. The
      lower bounds of the slices along the sampling direction.
  """
  with tf.compat.v1.name_scope(name, 'sample_next', [
      current_state_parts, step_sizes, max_doublings, current_target_log_prob,
      batch_rank
  ]):
    # First step: Choose a random direction.
    # Direction is a list of tensors. The i'th tensor should have the same shape
    # as the i'th state part.
    direction = _choose_random_direction(current_state_parts,
                                         batch_rank=batch_rank,
                                         seed=seed)

    # Interpolates the step sizes for the chosen direction.
    # Applies an ellipsoidal interpolation to compute the step direction for
    # the chosen direction. Suppose we are given step sizes for each direction.
    # Label these s_1, s_2, ... s_k. These are the step sizes to use if moving
    # in a direction parallel to one of the axes. Consider an ellipsoid which
    # intercepts the i'th axis at s_i. The step size for a direction specified
    # by the unit vector (n_1, n_2 ...n_k) is then defined as the intersection
    # of the line through this vector with this ellipsoid.
    #
    # One can show that the length of the vector from the origin to the
    # intersection point is given by:
    # 1 / sqrt(n_1^2 / s_1^2  + n_2^2 / s_2^2  + ...).
    #
    # Proof:
    # The equation of the ellipsoid is:
    # Sum_i [x_i^2 / s_i^2 ] = 1. Let n be a unit direction vector. Points
    # along the line given by n may be parameterized as alpha*n where alpha is
    # the distance along the vector. Plugging this into the equation for the
    # ellipsoid, we get:
    # alpha^2 ( n_1^2 / s_1^2 + n_2^2 / s_2^2 + ...) = 1
    # so alpha = \sqrt { \frac{1} { ( n_1^2 / s_1^2 + n_2^2 / s_2^2 + ...) } }
    reduce_axes = [tf.range(batch_rank, tf.rank(dirn_part))
                   for dirn_part in direction]

    components = [
        tf.reduce_sum(
            input_tensor=(dirn_part / step_size)**2, axis=reduce_axes[i])
        for i, (step_size, dirn_part) in enumerate(zip(step_sizes, direction))
    ]
    step_size = tf.math.rsqrt(tf.add_n(components))
    # Computes the rank of a tensor. Uses the static rank if possible.
    def _get_rank(x):
      return (len(x.shape.as_list()) if x.shape.dims is not None
              else tf.rank(x))
    state_part_ranks = [_get_rank(part) for part in current_state_parts]

    def _step_along_direction(alpha):
      """Converts the scalar alpha into an n-dim vector with full state info.

      Computes x_0 + alpha * direction where x_0 is the current state and
      direction is the direction chosen above.

      Args:
        alpha: A tensor of shape equal to the batch dimensions of
          `current_state_parts`.

      Returns:
        state_parts: Tensor or Python list of `Tensor`s representing the
          state(s) of the Markov chain(s) for a given alpha and a given chosen
          direction. Has the same shape as `current_state_parts`.
      """
      padded_alphas = [_right_pad(alpha, final_rank=part_rank)
                       for part_rank in state_part_ranks]

      state_parts = [state_part + padded_alpha
                     * direction_part for state_part, direction_part,
                     padded_alpha in
                     zip(current_state_parts, direction, padded_alphas)]
      return state_parts

    def projected_target_log_prob_fn(alpha):
      """The target log density projected along the chosen direction.

      Args:
        alpha: A tensor of shape equal to the batch dimensions of
          `current_state_parts`.

      Returns:
        Target log density evaluated at x_0 + alpha * direction where x_0 is the
        current state and direction is the direction chosen above. Has the same
        shape as `alpha`.
      """
      return target_log_prob_fn(*_step_along_direction(alpha))

    alpha_init = tf.zeros_like(current_target_log_prob,
                               dtype=current_state_parts[0].dtype.base_dtype)
    [
        next_alpha,
        next_target_log_prob,
        bounds_satisfied,
        upper_bounds,
        lower_bounds
    ] = ssu.slice_sampler_one_dim(projected_target_log_prob_fn,
                                  x_initial=alpha_init,
                                  max_doublings=max_doublings,
                                  step_size=step_size, seed=seed)
    return [
        _step_along_direction(next_alpha),
        next_target_log_prob,
        bounds_satisfied,
        direction,
        upper_bounds,
        lower_bounds
    ]
def _sample_next ( target_log_prob_fn , current_state_parts , step_sizes , max_doublings , current_target_log_prob , batch_rank , seed = None , name = None ) : with tf . compat . v1 . name_scope ( name , 'sample_next' , [ current_state_parts , step_sizes , max_doublings , current_target_log_prob , batch_rank ] ) : # First step: Choose a random direction. # Direction is a list of tensors. The i'th tensor should have the same shape # as the i'th state part. direction = _choose_random_direction ( current_state_parts , batch_rank = batch_rank , seed = seed ) # Interpolates the step sizes for the chosen direction. # Applies an ellipsoidal interpolation to compute the step direction for # the chosen direction. Suppose we are given step sizes for each direction. # Label these s_1, s_2, ... s_k. These are the step sizes to use if moving # in a direction parallel to one of the axes. Consider an ellipsoid which # intercepts the i'th axis at s_i. The step size for a direction specified # by the unit vector (n_1, n_2 ...n_k) is then defined as the intersection # of the line through this vector with this ellipsoid. # # One can show that the length of the vector from the origin to the # intersection point is given by: # 1 / sqrt(n_1^2 / s_1^2  + n_2^2 / s_2^2  + ...). # # Proof: # The equation of the ellipsoid is: # Sum_i [x_i^2 / s_i^2 ] = 1. Let n be a unit direction vector. Points # along the line given by n may be parameterized as alpha*n where alpha is # the distance along the vector. Plugging this into the equation for the # ellipsoid, we get: # alpha^2 ( n_1^2 / s_1^2 + n_2^2 / s_2^2 + ...) = 1 # so alpha = \sqrt { \frac{1} { ( n_1^2 / s_1^2 + n_2^2 / s_2^2 + ...) } } reduce_axes = [ tf . range ( batch_rank , tf . rank ( dirn_part ) ) for dirn_part in direction ] components = [ tf . reduce_sum ( input_tensor = ( dirn_part / step_size ) ** 2 , axis = reduce_axes [ i ] ) for i , ( step_size , dirn_part ) in enumerate ( zip ( step_sizes , direction ) ) ] step_size = tf . math . rsqrt ( tf . add_n ( components ) ) # Computes the rank of a tensor. Uses the static rank if possible. def _get_rank ( x ) : return ( len ( x . shape . as_list ( ) ) if x . shape . dims is not None else tf . rank ( x ) ) state_part_ranks = [ _get_rank ( part ) for part in current_state_parts ] def _step_along_direction ( alpha ) : """Converts the scalar alpha into an n-dim vector with full state info.

      Computes x_0 + alpha * direction where x_0 is the current state and
      direction is the direction chosen above.

      Args:
        alpha: A tensor of shape equal to the batch dimensions of
          `current_state_parts`.

      Returns:
        state_parts: Tensor or Python list of `Tensor`s representing the
          state(s) of the Markov chain(s) for a given alpha and a given chosen
          direction. Has the same shape as `current_state_parts`.
      """ padded_alphas = [ _right_pad ( alpha , final_rank = part_rank ) for part_rank in state_part_ranks ] state_parts = [ state_part + padded_alpha * direction_part for state_part , direction_part , padded_alpha in zip ( current_state_parts , direction , padded_alphas ) ] return state_parts def projected_target_log_prob_fn ( alpha ) : """The target log density projected along the chosen direction.

      Args:
        alpha: A tensor of shape equal to the batch dimensions of
          `current_state_parts`.

      Returns:
        Target log density evaluated at x_0 + alpha * direction where x_0 is the
        current state and direction is the direction chosen above. Has the same
        shape as `alpha`.
      """ return target_log_prob_fn ( * _step_along_direction ( alpha ) ) alpha_init = tf . zeros_like ( current_target_log_prob , dtype = current_state_parts [ 0 ] . dtype . base_dtype ) [ next_alpha , next_target_log_prob , bounds_satisfied , upper_bounds , lower_bounds ] = ssu . slice_sampler_one_dim ( projected_target_log_prob_fn , x_initial = alpha_init , max_doublings = max_doublings , step_size = step_size , seed = seed ) return [ _step_along_direction ( next_alpha ) , next_target_log_prob , bounds_satisfied , direction , upper_bounds , lower_bounds ]
Applies a single iteration of slice sampling update.

  Applies hit and run style slice sampling. Chooses a uniform random direction
  on the unit sphere in the event space. Applies the one dimensional slice
  sampling update along that direction.

  Args:
    target_log_prob_fn: Python callable which takes an argument like
      `*current_state_parts` and returns its (possibly unnormalized) log-density
      under the target distribution.
    current_state_parts: Python `list` of `Tensor`s representing the current
      state(s) of the Markov chain(s). The first `independent_chain_ndims` of
      the `Tensor`(s) index different chains.
    step_sizes: Python `list` of `Tensor`s. Provides a measure of the width
      of the density. Used to find the slice bounds. Must broadcast with the
      shape of `current_state_parts`.
    max_doublings: Integer number of doublings to allow while locating the slice
      boundaries.
    current_target_log_prob: `Tensor` representing the value of
      `target_log_prob_fn(*current_state_parts)`. The only reason to specify
      this argument is to reduce TF graph size.
    batch_rank: Integer. The number of axes in the state that correspond to
      independent batches.
    seed: Python integer to seed random number generators.
    name: Python `str` name prefixed to Ops created by this function.
      Default value: `None` (i.e., 'find_slice_bounds').

  Returns:
    proposed_state_parts: Tensor or Python list of `Tensor`s representing the
      state(s) of the Markov chain(s) at each result step. Has same shape as
      input `current_state_parts`.
    proposed_target_log_prob: `Tensor` representing the value of
      `target_log_prob_fn` at `next_state`.
    bounds_satisfied: Boolean `Tensor` of the same shape as the log density.
      True indicates whether the an interval containing the slice for that
      batch was found successfully.
    direction: `Tensor` or Python list of `Tensors`s representing the direction
      along which the slice was sampled. Has the same shape and dtype(s) as
      `current_state_parts`.
    upper_bounds: `Tensor` of batch shape and the dtype of the input state. The
      upper bounds of the slices along the sampling direction.
    lower_bounds: `Tensor` of batch shape and the dtype of the input state. The
      lower bounds of the slices along the sampling direction.
Applies a single iteration of slice sampling update .