The circuit
The 18\times74 matrix. Rows are wires and columns are rotations. A 1 means the wire takes part in the rotation, and the number beside each wire is its row weight.
| wire | 0 10 20 30 40 50 60 70 |
|---|---|
| out 0 (7) | 1111111··································································· |
| out 1 (7) | ·······1111111···························································· |
| out 2 (7) | ··············1111111····················································· |
| out 3 (7) | ·····················1111111·············································· |
| out 4 (7) | ····························1111111······································· |
| out 5 (7) | ···································1111111································ |
| out 6 (37) | 1111···1111···1111··········1111···1111···11111111111111111··············· |
| out 7 (37) | 11··11·11··11·11··11········11··11·11··11·1111111111·······1111111········ |
| out 8 (41) | 1·1·1·111··11·1·1·1·11111···1111···1·1·1·111111·····11111111······1111···· |
| out 9 (39) | ·11··111·1·1·1··1111·11··11·11··11···1111·1111·11···11······11····11··111· |
| check 10 (32) | ·1·11·11111···1111···1·1·1·11111··········11··11·1····111··11·1·····1····· |
| check 11 (36) | ·······1111···11··11·1··1·111·1·1·1··1111·111·····11··11·1·1···11·1·1111·· |
| check 12 (38) | ·11··111111···1111····1·11·11··1·111·1·1·1···111·11···11·1··11·1···1··1··1 |
| check 13 (38) | 11··11·11··11·1·1·1·11111···1111···11··11·····1··1·11·1··1·1·1·1··11·11·1· |
| check 14 (32) | 11··11·1111····1·11·1·········1111········1·1·····1·111·1·1111·1·1··11···1 |
| check 15 (38) | ·1·11·11··1·11··1111········11··11·1·1·1·1···1·1·1111··11111·1·1··111·11·· |
| check 16 (38) | 11··11·1··1·111··1·111·1·1·1·······11··11··1111·1··1·1··1··1··1·111·1111·1 |
| check 17 (38) | ··1111·1·1·1·11··1·11··1111···1111·1·1·1·1·1·1·1·1·11111·1·····1···111···· |
The gate is read off the output rows. An output row of odd weight gives a T, a pair of output rows with odd overlap gives a CS, and an odd triple overlap gives a CCZ. The circuit is a valid factory because every such parity that touches a check row is even.
Figures of merit
Output gate
As gates: \mathrm{T}_{0}\cdot \mathrm{T}_{1}\cdot \mathrm{T}_{2}\cdot \mathrm{T}_{3}\cdot \mathrm{T}_{4}\cdot \mathrm{T}_{5}\cdot \mathrm{T}_{6}\cdot \mathrm{T}_{7}\cdot \mathrm{T}_{8}\cdot \mathrm{T}_{9}
As monomials: 0+1+2+3+4+5+6+7+8+9 (output wires per term, separated by +)
This row stands for every gate that a CNOT circuit and S, Z and CZ gates on the outputs can reach from this one. They all prepare the same magic state. The wires are shown in the S_k-canonical frame.
Clifford correction
With every rotation a \mathrm{T}=\mathrm{diag}(1,e^{i\pi/4}), the rotations deposit the gate above times a diagonal Clifford. Undo it after the rotations and before the checks are measured, with 15 single-wire gates and 31 \mathrm{CZ} gates: \mathrm{S} on output 0, \mathrm{S} on output 1, \mathrm{S} on output 2, \mathrm{S} on output 3, \mathrm{S} on output 4, \mathrm{S} on output 5, \mathrm{Z} on output 6, \mathrm{Z} on output 7, \mathrm{S} on output 9, \mathrm{Z} on check 11, \mathrm{S} on check 12, \mathrm{S} on check 13, \mathrm{S} on check 15, \mathrm{S} on check 16, \mathrm{S} on check 17, \mathrm{CZ} on output 6, output 9, \mathrm{CZ} on output 6, check 10, \mathrm{CZ} on output 6, check 11, \mathrm{CZ} on output 6, check 12, \mathrm{CZ} on output 6, check 13, \mathrm{CZ} on output 6, check 14, \mathrm{CZ} on output 7, output 8, \mathrm{CZ} on output 7, check 11, \mathrm{CZ} on output 7, check 12 and 22 more (listed below). The circuit's action is then exactly the gate above, and an error-free run passes every check with certainty.
All 46 correction gates
\mathrm{S} on output 0, \mathrm{S} on output 1, \mathrm{S} on output 2, \mathrm{S} on output 3, \mathrm{S} on output 4, \mathrm{S} on output 5, \mathrm{Z} on output 6, \mathrm{Z} on output 7, \mathrm{S} on output 9, \mathrm{Z} on check 11, \mathrm{S} on check 12, \mathrm{S} on check 13, \mathrm{S} on check 15, \mathrm{S} on check 16, \mathrm{S} on check 17, \mathrm{CZ} on output 6, output 9, \mathrm{CZ} on output 6, check 10, \mathrm{CZ} on output 6, check 11, \mathrm{CZ} on output 6, check 12, \mathrm{CZ} on output 6, check 13, \mathrm{CZ} on output 6, check 14, \mathrm{CZ} on output 7, output 8, \mathrm{CZ} on output 7, check 11, \mathrm{CZ} on output 7, check 12, \mathrm{CZ} on output 7, check 13, \mathrm{CZ} on output 7, check 14, \mathrm{CZ} on output 7, check 16, \mathrm{CZ} on output 8, check 14, \mathrm{CZ} on output 8, check 15, \mathrm{CZ} on output 9, check 10, \mathrm{CZ} on output 9, check 11, \mathrm{CZ} on output 9, check 13, \mathrm{CZ} on output 9, check 14, \mathrm{CZ} on output 9, check 15, \mathrm{CZ} on output 9, check 16, \mathrm{CZ} on check 11, check 12, \mathrm{CZ} on check 11, check 13, \mathrm{CZ} on check 11, check 15, \mathrm{CZ} on check 11, check 16, \mathrm{CZ} on check 11, check 17, \mathrm{CZ} on check 12, check 15, \mathrm{CZ} on check 12, check 16, \mathrm{CZ} on check 12, check 17, \mathrm{CZ} on check 15, check 16, \mathrm{CZ} on check 15, check 17, \mathrm{CZ} on check 16, check 17
Or no Clifford gate at all: run \mathrm{T}^3 on rotations 2, 11, 17, 18, 25, 26, 27, 29, 30, 31, 32, 33, 34, 36, 37, 39, 42, 43, 47, 48, 52, 53, 54, 55 and 10 more (listed below); \mathrm{T}^5 on rotations 0, 7, 21, 35; \mathrm{T}^\dagger on rotations 1, 4, 8, 9, 14, 28, and \mathrm{T} on the rest. A power of \mathrm{T} costs one magic state, like \mathrm{T} itself. For a code this is a transversal \mathrm{T} gate, \mathrm{T}^j on each qubit.
All 34 rotations at T³
2, 11, 17, 18, 25, 26, 27, 29, 30, 31, 32, 33, 34, 36, 37, 39, 42, 43, 47, 48, 52, 53, 54, 55, 56, 57, 59, 65, 66, 68, 69, 71, 72, 73
Rotations are numbered by matrix column, from 0. The correction comes from the columns by the weight expansion of Bravyi and Haah (2012). verify_catalog.py re-derives it, checks the corrected circuit's phase input by input against the gate, and on small circuits simulates it gate by gate.
Convert the output with CNOT and S
A CNOT circuit on the outputs, followed by S, Z and CZ gates, turns this factory's gate into other gates that prepare the same magic state. Type a target gate to check whether it is reachable. If it is, you get the circuit, checked on every basis state.
Or list every gate it reaches. The list is built in your browser and saved as a text file, one gate per line.
Python code that writes the same list
import json, urllib.request
NAMES = {1: "T", 2: "CS", 3: "CCZ"}
def equivalent_gates(k, terms, limit=1_000_000):
"""Every gate a CNOT circuit and S, Z, CZ gates reach from this one.
A gate is its set of terms mod Clifford: {a} is T, {a,b} is CS and
{a,b,c} is CCZ on those outputs. CNOT c->t sends x_t to
x_c + x_t - 2 x_c x_t, so a term on t but not c adds the term with t
replaced by c, and, below CCZ, the term with c added.
"""
start = frozenset(frozenset(m) for m in terms)
seen, queue = {start}, [start]
for gate in queue:
for c in range(k):
for t in range(k):
if c == t:
continue
new = set(gate)
for m in gate:
if t in m and c not in m:
new ^= {(m - {t}) | {c}}
if len(m) < 3:
new ^= {m | {c}}
new = frozenset(new)
if new not in seen:
seen.add(new)
queue.append(new)
if len(seen) > limit:
raise RuntimeError(f"more than {limit} equivalent gates")
return seen
def name(gate, k):
sep = "," if k > 10 else ""
terms = sorted((sorted(m) for m in gate), key=lambda m: (len(m), m))
return "·".join(NAMES[len(m)] + sep.join(map(str, m)) for m in terms) or "I"
url = "https://shubhamj810.github.io/magic-state-factory-repo/data/factories/74.10.3.a.json"
record = json.load(urllib.request.urlopen(url))
k = record["parameters"]["k"]
gates = equivalent_gates(k, record["gate"]["monomials"])
lines = sorted(name(g, k) for g in gates)
print(len(lines), "equivalent gates")
with open("equivalent-gates-74.10.3.a.txt", "w") as out:
out.write("\n".join(lines) + "\n")
Distance
d=3, exact. No fault of weight below 3 is both undetectable and damaging. One of weight 3 is.
Exactly 489 faults of weight 3 are undetectable and damaging, so A_{3}=489. If each rotation fails independently with probability p, an accepted run has a damaged output with probability A_{3}\,p^{3}+O(p^{4}).
A damaging fault of weight 3 sits on columns [0,1,6].
A fault is a set of faulty columns. It is undetectable when their check parts cancel, and damaging when their output parts do not.
Original source
S. P. Jain, A. Wills, and S. Singh, "Symmetry and AI-assisted discovery of magic-state factories," arXiv:2610.06535 (2026). arxiv.org/abs/2610.06535
Provenance
found by an AI search campaign; a verified witness, not a maximum
Found by: AI search
Discovery: AI search
1 recorded source
[
{
"regime": "AI search",
"file": "/private/tmp/claude-501/-Users-shubhamjain-Documents-Claude-remote-magic-states-AI/25937cc1-0367-40c1-acc9-031067b831d4/scratchpad/msai_for_merge.jsonl",
"label": "msAI:2ce85f3d951f917c",
"N": 18,
"d": 3,
"d_is_exact": true,
"origin": "magic-states-AI/master_catalogue/master_catalogue.jsonl",
"provenance": "magic-states-AI/master_catalogue/master_catalogue.jsonl",
"notes": "gamma_campaign"
}
]Use it in code
Load this factory and re-derive every number from its circuit with the catalogue's own verifier.
# git clone https://github.com/shubhamj810/magic-state-factory-repo
# cd magic-state-factory-repo/master_catalog
import json, urllib.request
import verify_catalog as VC
url = "https://shubhamj810.github.io/magic-state-factory-repo/data/factories/74.10.3.a.json"
record = json.load(urllib.request.urlopen(url))
columns = record["circuit"]["columns"]
k, N = record["parameters"]["k"], record["parameters"]["N"]
facts, problems = VC.derive(columns, k, N) # gate, T-count, degree, ...
distance = VC.measure_distance(columns, k, N) # exhaustive fault search
print(facts["gate_human"], distance["d_exact"] or distance["d_at_least"],
problems or "verified")
Raw record
Show the JSON this page is built from
Source: master_catalog.json, factories[522].