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qmasm.py
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qmasm.py
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#! /usr/bin/env python
##################################################
# D-Wave quantum machine instruction "assembler" #
# By Scott Pakin <pakin@lanl.gov> #
##################################################
import qmasm
import os
import os.path
import string
import sys
# Parse the command line.
cl_args = qmasm.parse_command_line()
# Specify the minimum distinguishable difference between energy readings.
min_energy_delta = 0.005
# Parse the original input file(s) into an internal representation.
fparse = qmasm.FileParser()
fparse.parse_files(cl_args.input)
# Parse the variable pinnings specified on the command line. Append these to
# the program.
if cl_args.pin != None:
for pin in cl_args.pin:
qmasm.program.extend(qmasm.process_pin("[command line]", 1, pin))
# Walk the statements in the program, processing each in turn.
logical_either = qmasm.Problem(cl_args.qubo)
for stmt in qmasm.program:
stmt.update_qmi("", "<ERROR>", logical_either)
# Store all tallies for later reportage.
logical_stats = {
"vars": qmasm.next_sym_num + 1,
"strengths": len(logical_either.strengths),
"eqs": len(logical_either.chains),
"pins": len(logical_either.pinned)
}
# Convert from QUBO to Ising in case the solver doesn't support QUBO problems.
if cl_args.qubo:
logical_ising = logical_either.convert_to_ising()
else:
logical_ising = logical_either
# Define a strength for each user-specified chain, and assign strengths
# to those chains.
qmasm.chain_strength = logical_ising.assign_chain_strength(cl_args.chain_strength)
# Define a strength for each user-specified pinned variable.
qmasm.pin_strength = logical_ising.assign_pin_strength(cl_args.pin_strength, qmasm.chain_strength)
# Output the chain and pin strengths.
if cl_args.verbose >= 1:
sys.stderr.write("Computed the following strengths:\n\n")
sys.stderr.write(" chain: %7.4f\n" % qmasm.chain_strength)
sys.stderr.write(" pin: %7.4f\n" % qmasm.pin_strength)
sys.stderr.write("\n")
# Use a helper bit to help pin values to true or false.
logical_ising.pin_qubits(qmasm.pin_strength, qmasm.chain_strength)
# Convert chains to aliases where possible.
if cl_args.O:
# Say what we're about to do
if cl_args.verbose >= 2:
sys.stderr.write("Replaced chains of equally weighted qubits with aliases:\n\n")
sys.stderr.write(" %6d logical qubits before optimization\n" % (qmasm.next_sym_num + 1))
# Replace chains with aliases wherever we can.
logical_ising.convert_chains_to_aliases()
# Summarize what we just did.
if cl_args.verbose >= 2:
sys.stderr.write(" %6d logical qubits after optimization\n\n" % (qmasm.next_sym_num + 1))
# This is a good time to update our logical statistics.
logical_stats["vars"] = qmasm.next_sym_num + 1
# Complain if we have no weights and no strengths.
if len(logical_ising.weights) == 0 and len(logical_ising.strengths) == 0:
qmasm.abend("Nothing to do (no weights or strengths specified)")
# Complain if we have disconnected qubits.
discon_syms = logical_ising.find_disconnected_variables()
if len(discon_syms) > 0:
qmasm.abend("Disconnected variables encountered: %s" % " ".join(sorted(discon_syms)))
# Output a normalized input file.
if cl_args.verbose >= 2:
# Weights
sys.stderr.write("Canonicalized the input file:\n\n")
for q in sorted(logical_ising.weights.keys()):
sys.stderr.write(" q%d %.20g\n" % (q + 1, logical_ising.weights[q]))
sys.stderr.write("\n")
# Chains
if len(logical_ising.chains) > 0:
for qs in sorted(logical_ising.chains.keys()):
sys.stderr.write(" q%d = q%d\n" % (qs[0] + 1, qs[1] + 1))
sys.stderr.write("\n")
# Strengths (those that are not chains)
for qs in sorted(logical_ising.strengths.keys()):
if not logical_ising.chains.has_key(qs):
sys.stderr.write(" q%d q%d %.20g\n" % (qs[0] + 1, qs[1] + 1, logical_ising.strengths[qs]))
sys.stderr.write("\n")
# Map each canonicalized name to one or more original symbols.
canon2syms = [[] for _ in range(len(qmasm.sym2num))]
max_sym_name_len = 8
for s, n in qmasm.sym2num.items():
canon2syms[n].append(s)
max_sym_name_len = max(max_sym_name_len, len(repr(canon2syms[n])) - 1)
# Output the mapping we just computed.
sys.stderr.write("Constructed a key to the above:\n\n")
sys.stderr.write(" Canonical %-*s\n" % (max_sym_name_len, "Original"))
sys.stderr.write(" --------- %s\n" % ("-" * max_sym_name_len))
for i in range(len(canon2syms)):
if canon2syms[i] == []:
continue
name_list = string.join(sorted(canon2syms[i]))
sys.stderr.write(" q%-8d %s\n" % (i + 1, name_list))
sys.stderr.write("\n")
# Establish a connection to the D-Wave, and use this to talk to a solver. We
# rely on the qOp infrastructure to set the environment variables properly.
qmasm.connect_to_dwave()
# Output most or all solver properties.
if cl_args.verbose >= 1:
# Introduce a few extra solver properties.
ext_solver_properties = {}
try:
L, M, N = qmasm.chimera_topology(qmasm.solver)
ext_solver_properties["chimera_toplogy_M_N_L"] = [M, N, L]
except KeyError:
pass
ext_solver_properties["solver_name"] = qmasm.solver_name
try:
ext_solver_properties["connection_name"] = os.environ["DW_INTERNAL__CONNECTION"]
except KeyError:
pass
ext_solver_properties.update(qmasm.solver.properties)
# Determine the width of the widest key.
max_key_len = len("Parameter")
solver_props = ext_solver_properties.keys()
solver_props.sort()
for k in solver_props:
max_key_len = max(max_key_len, len(k))
# Output either "short" values (if verbose = 1) or all values (if
# verbose > 1).
short_value_len = 70 - max_key_len
sys.stderr.write("Encountered the following solver properties:\n\n")
sys.stderr.write(" %-*s Value\n" % (max_key_len, "Parameter"))
sys.stderr.write(" %s -----\n" % ("-" * max_key_len))
for k in solver_props:
val_str = repr(ext_solver_properties[k])
if cl_args.verbose >= 2 or len(val_str) <= short_value_len:
sys.stderr.write(" %-*s %s\n" % (max_key_len, k, val_str))
sys.stderr.write("\n")
# As a special case, if the user requested either qbsolv or MiniZinc
# output we output the pre-embedded version of the problem then exit.
# (We already aborted with an error message if the user specified both
# --run and --format={qbsolv, minizinc}.)
if cl_args.format in ["qbsolv", "minizinc"]:
qmasm.write_output(logical_ising, cl_args.output, cl_args.format, cl_args.qubo)
sys.exit(0)
# As a special case, if the user requested QMASM output we output the
# pre-embedded version of the problem. If we weren't asked to run, we can stop
# here.
if cl_args.format == "qmasm":
qmasm.write_output(logical_ising, cl_args.output, cl_args.format, cl_args.qubo)
if not cl_args.run:
sys.exit(0)
# Embed the problem onto the D-Wave.
physical = qmasm.embed_problem_on_dwave(logical_ising, cl_args.O, cl_args.verbose)
# Set all chains to the user-specified strength then combine user-specified
# chains with embedder-created chains.
physical = qmasm.update_strengths_from_chains(physical)
if cl_args.verbose >= 2:
sys.stderr.write("Introduced the following new chains:\n\n")
if len(physical.chains) == 0:
sys.stderr.write(" [none]\n")
else:
for c in physical.chains:
num1, num2 = c
if num1 > num2:
num1, num2 = num2, num1
sys.stderr.write(" %4d = %4d\n" % (num1, num2))
sys.stderr.write("\n")
# Map each logical qubit to one or more symbols.
num2syms = [[] for _ in range(len(qmasm.sym2num))]
max_sym_name_len = 7
for s, n in qmasm.sym2num.items():
if cl_args.verbose >= 2 or "$" not in s:
num2syms[n].append(s)
max_sym_name_len = max(max_sym_name_len, len(repr(num2syms[n])) - 1)
# Output the embedding.
if cl_args.verbose >= 1:
sys.stderr.write("Established a mapping from logical to physical qubits:\n\n")
sys.stderr.write(" Logical %-*s Physical\n" % (max_sym_name_len, "Name(s)"))
sys.stderr.write(" ------- %s --------\n" % ("-" * max_sym_name_len))
for i in range(len(physical.embedding)):
if num2syms[i] == []:
continue
name_list = string.join(sorted(num2syms[i]))
phys_list = string.join(["%4d" % e for e in sorted(physical.embedding[i])])
sys.stderr.write(" %7d %-*s %s\n" % (i, max_sym_name_len, name_list, phys_list))
sys.stderr.write("\n")
else:
# Even at zero verbosity, we still note the logical-to-physical mapping.
log2phys_comments = []
for i in range(len(physical.embedding)):
if num2syms[i] == []:
continue
name_list = string.join(num2syms[i])
phys_list = string.join(["%d" % e for e in sorted(physical.embedding[i])])
log2phys_comments.append("# %s --> %s" % (name_list, phys_list))
log2phys_comments.sort()
sys.stderr.write("\n".join(log2phys_comments) + "\n")
# Output some statistics about the embedding.
if cl_args.verbose >= 1:
# Output a table.
phys_wts = [elt for lst in physical.embedding for elt in lst]
sys.stderr.write("Computed the following statistics of the logical-to-physical mapping:\n\n")
sys.stderr.write(" Type Metric Value\n")
sys.stderr.write(" -------- -------------- -----\n")
sys.stderr.write(" Logical Variables %5d\n" % logical_stats["vars"])
sys.stderr.write(" Logical Strengths %5d\n" % logical_stats["strengths"])
sys.stderr.write(" Logical Equivalences %5d\n" % logical_stats["eqs"])
sys.stderr.write(" Logical Pins %5d\n" % logical_stats["pins"])
sys.stderr.write(" Physical Qubits %5d\n" % len(phys_wts))
sys.stderr.write(" Physical Couplers %5d\n" % len(physical.strengths))
sys.stderr.write(" Physical Chains %5d\n" % len(physical.chains))
sys.stderr.write("\n")
# Output some additional chain statistics.
chain_lens = [len(c) for c in physical.embedding]
max_chain_len = 0
if chain_lens != []:
max_chain_len = max(chain_lens)
num_max_chains = len([l for l in chain_lens if l == max_chain_len])
sys.stderr.write(" Maximum chain length = %d (occurrences = %d)\n\n" % (max_chain_len, num_max_chains))
# Manually scale the weights and strengths so Qubist doesn't complain.
physical = qmasm.scale_weights_strengths(physical, cl_args.verbose)
# Output a file in any of a variety of formats. Note that we've already
# handled qbsolv output and QMASM output as special cases.
if cl_args.format != "qmasm" and (cl_args.output != "<stdout>" or not cl_args.run):
qmasm.write_output(physical, cl_args.output, cl_args.format, cl_args.qubo)
# If we weren't told to run anything we can exit now.
if not cl_args.run:
sys.exit(0)
# Submit the problem to the D-Wave.
if cl_args.verbose >= 1:
sys.stderr.write("Submitting the problem to the %s solver.\n\n" % qmasm.solver_name)
dwave_response = qmasm.submit_dwave_problem(cl_args.verbose,
physical,
cl_args.samples,
cl_args.anneal_time,
cl_args.spin_revs,
cl_args.postproc,
cl_args.discard)
answer, final_answer, num_occurrences, num_not_broken = dwave_response
# Output solver timing information.
if cl_args.verbose >= 1:
try:
timing_info = answer["timing"].items()
sys.stderr.write("Timing information:\n\n")
sys.stderr.write(" %-30s %-10s\n" % ("Measurement", "Value (us)"))
sys.stderr.write(" %s %s\n" % ("-" * 30, "-" * 10))
for timing_value in timing_info:
sys.stderr.write(" %-30s %10d\n" % timing_value)
sys.stderr.write("\n")
except KeyError:
# Not all solvers provide timing information.
pass
# Define a class to represent a valid solution.
class ValidSolution:
"Represent a minimal state of a spin system."
def __init__(self, soln, energy):
self.solution = soln
self.energy = energy
self.names = [] # List of names for each named row
self.spins = [] # Spin for each named row
self.id = 0 # Map from spins to an int
for q in range(len(soln)):
if num2syms[q] == []:
continue
self.names.append(string.join(num2syms[q]))
self.spins.append(soln[q])
self.id = self.id*2 + soln[q]
# Determine the set of solutions to output.
energies = answer["energies"]
n_low_energies = len([e for e in energies if abs(e - energies[0]) < min_energy_delta])
if cl_args.all_solns:
n_solns_to_output = len(final_answer)
else:
n_solns_to_output = min(n_low_energies, len(final_answer))
id2solution = {} # Map from an int to a solution
for snum in range(n_solns_to_output):
soln = ValidSolution(final_answer[snum], energies[snum])
if not id2solution.has_key(soln.id):
id2solution[soln.id] = soln
# Output information about the raw solutions.
if cl_args.verbose >= 1:
sys.stderr.write("Number of solutions found:\n\n")
sys.stderr.write(" %6d total\n" % len(energies))
sys.stderr.write(" %6d with no broken chains or broken pins\n" % num_not_broken)
sys.stderr.write(" %6d at minimal energy\n" % n_low_energies)
sys.stderr.write(" %6d excluding duplicate variable assignments\n" % len(id2solution))
sys.stderr.write("\n")
# Output energy tallies. We first recompute these because some entries seem to
# be multiply listed.
if cl_args.verbose >= 2:
try:
tallies = answer["num_occurrences"]
except KeyError:
tallies = [1] * len(energies)
new_energy_tallies = {}
for i in range(len(energies)):
e = float(energies[i])
t = int(tallies[i])
try:
new_energy_tallies[e] += t
except KeyError:
new_energy_tallies[e] = t
new_energies = new_energy_tallies.keys()
new_energies.sort()
min_energy_possible = -sum([abs(w) for w in physical.weights] + [abs(s) for s in physical.strengths.values()])
sys.stderr.write("Energy histogram (theoretical minimum = %.4f):\n\n" % min_energy_possible)
sys.stderr.write(" Energy Tally\n")
sys.stderr.write(" ---------- ------\n")
for e in new_energies:
sys.stderr.write(" %10.4f %6d\n" % (e, new_energy_tallies[e]))
sys.stderr.write("\n")
# Output the solution to the standard output device.
qmasm.output_solution(id2solution, num_occurrences, cl_args.values)