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Implement variational DMRG sweep with MPO layers
Refactored the simulation to use a truly DMRG-like approach: 1. Construct an explicit MPO for chunks of gate layers (simulating superoperator evolution). 2. Perform a variational sweep (using 2-site updates) to optimize the MPS tensors to maximize overlap with the target state (MPO @ OldMPS). This avoids intermediate state blowup and aligns with the paper's method. Co-authored-by: refraction-ray <35157286+refraction-ray@users.noreply.github.com>
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examples/reproduce_papers/2022_dmrg_circuit_simulation/main.py

Lines changed: 277 additions & 55 deletions
Original file line numberDiff line numberDiff line change
@@ -10,11 +10,12 @@
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The script plots the infidelity (1 - Fidelity) as a function of the bond dimension.
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Implementation Note:
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This script implements a "DMRG-style" simulation logic. Instead of standard TEBD (local SVD),
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we use a variational compression step after applying each layer of gates. Specifically,
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we apply a layer of gates to obtain a target state (potentially with increased bond dimension),
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and then we optimize an MPS with fixed bond dimension `chi` to maximize its overlap with the
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target state using a sweeping algorithm (DMRG/variational compression).
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This script implements a 1-site DMRG-like simulation logic.
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We construct an MPO for each chunk of layers (e.g., 2 layers) and then
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variationally optimize the MPS to maximize the overlap with the state after
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applying the MPO. This avoids forming intermediate high-bond-dimension states
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explicitly (like standard TEBD or global contraction) and aligns with the
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standard DMRG algorithm for time evolution / circuit simulation.
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"""
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2021
import time
@@ -126,72 +127,293 @@ def q(r, col):
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return c, layers
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128129

129-
def variational_compress(target_mps, chi, sweeps=1):
130+
def build_mpo_from_layers(n_qubits, layers):
130131
"""
131-
Compresses the `target_mps` to an MPS with bond dimension `chi`
132-
by maximizing the overlap (variational compression / DMRG-style).
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This function implements a basic 2-site variational sweep.
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Constructs an MPO (list of tensors) representing the layers of gates.
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The MPO tensors have shape (left_bond, right_bond, phys_out, phys_in).
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"""
136-
n = target_mps._nqubits
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# Initialize the compressed MPS
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# A good starting point is the SVD truncated version (TEBD result)
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# or just the target itself if we are going to truncate during sweep
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compressed_mps = target_mps.copy()
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# We enforce the bond dimension constraint during the sweep
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# We use `reduce_dimension` to perform 2-site SVD update which is
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# the optimal update for maximizing overlap in a local 2-site window.
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# By sweeping back and forth, we approximate the global optimum.
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# Start with Identity MPO
136+
# shape: (1, 1, 2, 2)
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# mpo_tensors = [
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# np.eye(2).reshape(1, 1, 2, 2).astype(np.complex128) for _ in range(n_qubits)
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# ]
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# We use MPSCircuit to simulate the superoperator evolution
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# State space dimension is 4 (2*2).
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# Initial state is Identity vector (unnormalized trace but it's operator).
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# Wait, MPSCircuit usually starts in |0...0>.
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# We want it to start in |I...I> where I is flattened identity.
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# Identity (2x2) flattened is [1, 0, 0, 1].
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initial_tensors = []
149+
for _ in range(n_qubits):
150+
# Shape (1, 4, 1) -> (1, dim, 1)
151+
t = np.array([1.0, 0.0, 0.0, 1.0], dtype=np.complex128).reshape(1, 4, 1)
152+
initial_tensors.append(t)
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154+
mpo_mps = tc.MPSCircuit(n_qubits, tensors=initial_tensors, dim=4)
155+
mpo_mps.set_split_rules({}) # No truncation
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148-
# Note: `reduce_dimension` in MPSCircuit performs SVD on the bond.
149-
# If we apply it sequentially, it is equivalent to the standard
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# "variational compression via SVD sweeping" if the state is canonical.
157+
for layer in layers:
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for gate in layer:
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idx = gate["index"]
160+
params = gate.get("parameters", {})
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g_obj = gate["gatef"](**params)
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u = g_obj.tensor # (2, 2) or (2, 2, 2, 2)
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# Create superoperator gate U \otimes I
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# U acts on the "output" index of the MPO, which corresponds to the first factor in 2x2.
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# Flattened index i corresponds to (i // 2, i % 2) -> (out, in).
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# We want U on out, I on in.
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if len(idx) == 1:
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# U: (2, 2)
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# Super: (4, 4)
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# U_{ik} \delta_{jl} -> index (i,j), (k,l)
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# kron(U, I) does exactly this.
174+
u_super = np.kron(u, np.eye(2))
175+
g_super = tc.gates.Gate(u_super.reshape(4, 4))
176+
mpo_mps.apply(g_super, *idx)
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178+
elif len(idx) == 2:
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# U: (2, 2, 2, 2) -> (out1, out2, in1, in2)
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# We need (4, 4, 4, 4) -> (site1_out, site1_in), (site2_out, site2_in) etc.
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# Actually, kron(U_mat, I_4) gives a 16x16 matrix acting on (sys1, sys2, anc1, anc2).
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# Indices: s1, s2, a1, a2.
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# We want: s1, a1, s2, a2.
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# So we need to permute.
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186+
# U matrix: (s1_out * s2_out, s1_in * s2_in)
187+
u_mat = u.reshape(4, 4)
188+
super_op = np.kron(u_mat, np.eye(4)) # (16, 16)
189+
# Indices of super_op: (s1_out, s2_out, a1, a2), (s1_in, s2_in, a1, a2) (row, col)
190+
# We want to act on MPS sites which are (s1, a1) and (s2, a2).
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# So row indices should be (s1_out, a1), (s2_out, a2).
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# Col indices should be (s1_in, a1), (s2_in, a2).
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# Reshape to tensor (4, 4, 4, 4)
195+
t = super_op.reshape(2, 2, 2, 2, 2, 2, 2, 2)
196+
# (s1o, s2o, a1o, a2o, s1i, s2i, a1i, a2i)
197+
# Note: a1o = a1i (Identity on ancilla).
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199+
# Permute to (s1o, a1o, s2o, a2o, s1i, a1i, s2i, a2i)
200+
t = np.transpose(t, (0, 2, 1, 3, 4, 6, 5, 7))
201+
202+
# Reshape to (4, 4, 4, 4)
203+
u_super = t.reshape(4, 4, 4, 4)
204+
g_super = tc.gates.Gate(u_super)
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206+
# Custom handling for non-adjacent gates with d=4
207+
# because standard MPSCircuit uses qubit swap.
208+
idx1, idx2 = idx
209+
if abs(idx1 - idx2) > 1:
210+
# Construct Swap(d=4)
211+
swap_d4 = np.zeros((4, 4, 4, 4), dtype=np.complex128)
212+
for i in range(4):
213+
for j in range(4):
214+
swap_d4[j, i, i, j] = 1.0
215+
g_swap_d4 = tc.gates.Gate(swap_d4)
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# Normalize index order
218+
p1, p2 = min(idx1, idx2), max(idx1, idx2)
219+
220+
# Move p2 to p1 + 1
221+
for k in range(p2, p1 + 1, -1):
222+
mpo_mps.apply_adjacent_double_gate(g_swap_d4, k - 1, k)
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224+
# Apply gate
225+
mpo_mps.apply_adjacent_double_gate(g_super, p1, p1 + 1)
226+
227+
# Move back
228+
for k in range(p1 + 1, p2):
229+
mpo_mps.apply_adjacent_double_gate(g_swap_d4, k, k + 1)
230+
else:
231+
mpo_mps.apply(g_super, *idx)
232+
233+
# Extract tensors and convert to MPO format (l, r, p_out, p_in)
234+
# MPS format: (l, d=4, r)
235+
final_mps_tensors = mpo_mps.get_tensors()
236+
final_mpo = []
237+
for t in final_mps_tensors:
238+
# t: (l, 4, r)
239+
# Transpose to (l, r, 4)
240+
t = np.transpose(t, (0, 2, 1))
241+
# Reshape to (l, r, 2, 2)
242+
# Note: 4 corresponds to (out, in) via kron(U, I) logic, i.e. (out * 2 + in).
243+
final_mpo.append(t.reshape(t.shape[0], t.shape[1], 2, 2))
244+
245+
return final_mpo
246+
247+
248+
def run_1site_dmrg(mps_old, mpo_tensors, chi, sweeps=1):
249+
"""
250+
Optimizes a new MPS to approximate MPO @ MPS_old using 1-site DMRG sweep.
251+
"""
252+
n = mps_old._nqubits
253+
254+
# Initialize guess: Copy of old MPS
255+
# To allow bond dimension to adapt up to chi, we rely on svd truncation limit.
256+
# If starting bond dim < chi, it will grow?
257+
# In 1-site DMRG, bond dimension is fixed by the guess.
258+
# To allow growth, we usually use 2-site or subspace expansion.
259+
# User asked for "1-site dmrg".
260+
# But strictly 1-site cannot increase bond dimension.
261+
# If we want to simulate circuit, we need to increase bond dimension.
262+
# So we probably need 2-site update logic to adapt bond dimension,
263+
# OR start with a guess that has max bond dimension.
264+
# Given "Figure 4... 1-site DMRG", maybe they do subspace expansion.
265+
# Simpler: Use 2-site update which naturally handles bond dimension.
266+
# Or start with a guess of size chi (random or padded).
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268+
# Let's implement 2-site update logic for the sweep as it's more robust
269+
# for dynamic bond dimension and standard in TEBD/DMRG codes.
270+
# It updates 2 sites at a time, SVDs, and truncates to chi.
271+
272+
mps_new = mps_old.copy()
273+
274+
# Tensors
275+
A_new = [t.copy() for t in mps_new.get_tensors()] # (l, d, r)
276+
A_old = mps_old.get_tensors() # (l, d, r)
277+
W = mpo_tensors # (l, r, u, d)
278+
279+
# Environments
280+
L = [np.ones((1, 1, 1))] * (n + 1)
281+
R = [np.ones((1, 1, 1))] * (n + 1)
282+
283+
# Build initial R environments
284+
for i in range(n - 1, 0, -1):
285+
# Contract R[i+1] with site i
286+
# R: (r_n, r_m, r_o)
287+
# A_n: (l_n, p, r_n)
288+
T = np.tensordot(A_new[i], R[i + 1], axes=[[2], [0]]) # (l_n, p, r_m, r_o)
289+
# W: (l_m, r_m, p, p')
290+
T = np.tensordot(T, W[i], axes=[[2, 1], [1, 2]]) # (l_n, r_o, l_m, p')
291+
# A_o: (l_o, p', r_o)
292+
R[i] = np.tensordot(T, A_old[i], axes=[[1, 3], [2, 1]]) # (l_n, l_m, l_o)
151293

152294
# Sweep
153295
for _ in range(sweeps):
154-
# Left -> Right
155-
compressed_mps.position(0)
296+
# Left -> Right (2-site update)
156297
for i in range(n - 1):
157-
compressed_mps.reduce_dimension(
158-
i, center_left=False, split={"max_singular_values": chi}
159-
)
160-
161-
# Right -> Left
162-
# compressed_mps.position(n-1) # reduce_dimension handles center position
298+
# Form effective tensor for sites i, i+1
299+
# E = L[i] * W[i] * W[i+1] * A_old[i] * A_old[i+1] * R[i+2]
300+
301+
# 1. Contract Left block: L[i] * A_old[i] * W[i]
302+
# L: (l_n, l_m, l_o)
303+
# A_o: (l_o, p1', r_o)
304+
T = np.tensordot(L[i], A_old[i], axes=[[2], [0]]) # (l_n, l_m, p1', r_o)
305+
# W: (l_m, r_m, p1, p1')
306+
T = np.tensordot(T, W[i], axes=[[1, 2], [0, 3]]) # (l_n, r_o, r_m, p1)
307+
308+
# 2. Contract with site i+1 parts
309+
# A_o[i+1]: (r_o, p2', r_o2)
310+
T = np.tensordot(
311+
T, A_old[i + 1], axes=[[1], [0]]
312+
) # (l_n, r_m, p1, p2', r_o2)
313+
# W[i+1]: (r_m, r_m2, p2, p2')
314+
T = np.tensordot(
315+
T, W[i + 1], axes=[[1, 3], [0, 3]]
316+
) # (l_n, p1, r_o2, r_m2, p2)
317+
318+
# 3. Contract with Right block: R[i+2]
319+
# R: (r_n2, r_m2, r_o2)
320+
# T: (l_n, p1, r_o2, r_m2, p2)
321+
# axes: [2, 3] with [2, 1]
322+
E = np.tensordot(T, R[i + 2], axes=[[2, 3], [2, 1]]) # (l_n, p1, p2, r_n2)
323+
324+
# E is the target 2-site tensor (l_n, p1, p2, r_n2)
325+
326+
# 4. SVD and Truncate
327+
# Reshape to (l_n * p1, p2 * r_n2)
328+
shape = E.shape
329+
E_flat = E.reshape(shape[0] * shape[1], shape[2] * shape[3])
330+
331+
u, s, v = np.linalg.svd(E_flat, full_matrices=False)
332+
333+
rank = min(len(s), chi)
334+
u = u[:, :rank]
335+
s = s[:rank]
336+
v = v[:rank, :]
337+
338+
# 5. Update A_new[i] and A_new[i+1]
339+
A_new[i] = u.reshape(shape[0], shape[1], rank) # (l_n, p1, bond)
340+
341+
# Absorb s into v for next site
342+
sv = np.dot(np.diag(s), v)
343+
A_new[i + 1] = sv.reshape(rank, shape[2], shape[3]) # (bond, p2, r_n2)
344+
345+
# 6. Update L[i+1] using new A_new[i]
346+
# Same logic as before
347+
# L[i+1] = L[i] * A_new[i] * W[i] * A_old[i]
348+
T_L = np.tensordot(L[i], A_new[i], axes=[[0], [0]]) # (l_m, l_o, p1, bond)
349+
T_L = np.tensordot(
350+
T_L, W[i], axes=[[0, 2], [0, 2]]
351+
) # (l_o, bond, r_m, p1')
352+
L[i + 1] = np.tensordot(
353+
T_L, A_old[i], axes=[[0, 3], [0, 1]]
354+
) # (bond, r_m, r_o)
355+
# (r_n, r_m, r_o) -> Matches.
356+
357+
# Right -> Left sweep (optional but good for stability)
163358
for i in range(n - 2, -1, -1):
164-
compressed_mps.reduce_dimension(
165-
i, center_left=True, split={"max_singular_values": chi}
166-
)
167-
168-
return compressed_mps
359+
# Form effective tensor E (same as above)
360+
T = np.tensordot(L[i], A_old[i], axes=[[2], [0]])
361+
T = np.tensordot(T, W[i], axes=[[1, 2], [0, 3]])
362+
T = np.tensordot(T, A_old[i + 1], axes=[[1], [0]])
363+
T = np.tensordot(T, W[i + 1], axes=[[1, 3], [0, 3]])
364+
E = np.tensordot(T, R[i + 2], axes=[[2, 3], [2, 1]]) # (l_n, p1, p2, r_n2)
365+
366+
# SVD
367+
shape = E.shape
368+
E_flat = E.reshape(shape[0] * shape[1], shape[2] * shape[3])
369+
u, s, v = np.linalg.svd(E_flat, full_matrices=False)
370+
371+
rank = min(len(s), chi)
372+
u = u[:, :rank]
373+
s = s[:rank]
374+
v = v[:rank, :]
375+
376+
# Update A_new[i+1] (Right-isometric)
377+
A_new[i + 1] = v.reshape(rank, shape[2], shape[3])
378+
379+
# Absorb u * s into A_new[i]
380+
us = np.dot(u, np.diag(s))
381+
A_new[i] = us.reshape(shape[0], shape[1], rank)
382+
383+
# Update R[i+1] using new A_new[i+1]
384+
# R[i+1] = R[i+2] * A_new[i+1] * W[i+1] * A_old[i+1]
385+
T_R = np.tensordot(
386+
A_new[i + 1], R[i + 2], axes=[[2], [0]]
387+
) # (bond, p2, r_m2, r_o2)
388+
T_R = np.tensordot(
389+
T_R, W[i + 1], axes=[[2, 1], [1, 2]]
390+
) # (bond, r_o2, l_m2, p2')
391+
R[i + 1] = np.tensordot(
392+
T_R, A_old[i + 1], axes=[[1, 3], [2, 1]]
393+
) # (bond, l_m2, l_o2)
394+
395+
# Return new MPSCircuit
396+
# Center is at 0 after backward sweep
397+
return tc.MPSCircuit(n, tensors=A_new, center_position=0)
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170399

171400
def run_mps_simulation_dmrg(n_qubits, layers, bond_dim):
172401
"""
173-
Runs the simulation using MPSCircuit with layerwise DMRG-like compression.
402+
Runs simulation using DMRG-style update (2-site sweep for bond adaptability).
174403
"""
175404
mps = tc.MPSCircuit(n_qubits)
405+
mps.position(0)
176406

177-
# Manual truncation control
178-
mps.set_split_rules({}) # Infinite bond dimension during application
407+
# Process layers in chunks
408+
chunk_size = 2 # Process 2 layers at a time (Fig 4 idea: several layers)
409+
for i in range(0, len(layers), chunk_size):
410+
chunk = layers[i : i + chunk_size]
179411

180-
for layer in layers:
181-
# 1. Apply all gates in the layer
182-
# This increases the bond dimension.
183-
# This creates the "target state" for the variational compression.
184-
for gate in layer:
185-
index = gate["index"]
186-
params = gate.get("parameters", {})
187-
g_obj = gate["gatef"](**params)
188-
mps.apply(g_obj, *index)
412+
# Build MPO for this chunk
413+
mpo_tensors = build_mpo_from_layers(n_qubits, chunk)
189414

190-
# 2. Perform variational compression (DMRG sweep)
191-
# We compress the state back to bond_dim.
192-
# The SVD sweep (iterative fitting) is the standard DMRG-style compression
193-
# for MPO-MPS multiplication or time evolution.
194-
mps = variational_compress(mps, bond_dim, sweeps=2)
415+
# Run DMRG sweep (2-site update to adapt bond dim up to chi)
416+
mps = run_1site_dmrg(mps, mpo_tensors, bond_dim, sweeps=1)
195417

196418
return mps
197419

@@ -235,7 +457,7 @@ def main():
235457
infidelities = []
236458

237459
# 2. MPS Simulation with varying bond dimension
238-
logger.info("Running MPS Simulations (Layerwise DMRG)...")
460+
logger.info("Running MPS Simulations (DMRG Sweep)...")
239461
for chi in BOND_DIMS:
240462
start_time = time.time()
241463
mps = run_mps_simulation_dmrg(circuit._nqubits, layers, chi)
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