gold 7/27/2026. Advisor and discussion has requested snippets on Classical Snippets Concepts Classical Simulation Quantum Amplitude Estimation QAE, notably as used in the ... ### Continuing, what about the difference between TCL/TK [ classical algorithms ] and the [ proposed ] quantum implementations? The simulation model is intended as an exploratory or experimental framework for TCL/TK coding. The full up algorithm is normally run on Quantum computers using Quantum feasible languages. Task Statement: generate a tutorial simulation of algorithm for a classical computer in pure TCL 8.6+. Adding references to Dr. Chiara Marletto's counterfactual framework from the book "The Science of Can and Can't" along with other perspectives. We are using modular snippets inside modular structured programs. Page content is targeted for engineering students and other Quantum tutorials.
gold 7/22/2026. Upon review and feedback of draft page, ... Second Advisor needs Simple Example Problems for Coding Setup?
I do not have all the answers. The Ideas Seemed to work, but maybe drawbacks? When measured by the Tcl timing statements, completion times and solutions of parameters will differ on different computer set-ups. Assume a future maintainer, either AI Model or human programmer, would have to maintain code with info content and explanatory variable name in program, ref "Snippets Concepts Effects". The Nassi Shneiderman Diagrams NSD or pseudocode Flowcharts pertain to the Tool Control Language TCL computer language as well as other computer languages like Python 3, pseudocode, word logic problems, and technical reports.
For each logic condition selecting a path or calculation task, we might have one, two, or multiple deterministic branches. Attempting to adapt format to multiple probabilistic branches used in Artificial Intelligence AI Models. Then we may use the >>> lottery algorithm <<< to select the winning pathways or tickets.
The existing program has some dummy subroutines. A full construction seems too complex here. I found a paper with images of quantum walks, and I’m wondering if it’s possible to simulate the curves shown in the charts. My advisor has suggested that quantum entanglement/superposition could simulate or underlie quantum worlds, but I’m not sure that I agree. I have limited space on the wiki page, and the fill‑in for the dummy routines has to be pretty brief. In engineering terms, I’m aiming for a “90% solution”, meaning about 90% right and 10% off. Like the simple college formula for a pendulum that is not the exact time series. Call it “prototype it ’til you make it” as a college try, but for Quantum Many Worlds. Who is to say? Perhaps you know, TcL specializes in GUI solutions. Maybe try and adapt some starter TcL code for a "quantum worlds slide rule ". Hopefully compatible with the hard-wired classical theory.
The TCL Snippets model ideal mathematical behavior only and do not perform full simulation, actual measurements, or state vector evolution. The tool only visualizes ideal math structure, whereas no state vector simulation, probabilities, or actual measurement outcomes are derived. This tool for visualization does not simulate actual measurement outcomes or state vector evolution during operations. These are idealized protocols for tutorial purposes. Primarily, TCL /TK uses its strong points here for book keeping and displays. The example tool is not a full emulator. Meaning, limited scope for tutorial purposes.
Disclaimer. None of the computer programs, numerical experiments, power-law fits, or physical analogies described here give a strict, formal proof of the Conjectures, either individually or in combination. The tools and analogies are heuristic models and visualization tools that follow engineering “rules of thumb.” Whereas, pure mathematics has its own shop rules for what counts as a rigorous proof. Any opinions on the difficulty or plausibility reflect current understanding here and programming of the Conjectures as a very hard open problem, not a completed exact math proof, and are offered with full respect for the standards of professional mathematicians.
In debugging the calculations, some of the printout values reflect roughly 17-digit precision output from a typical double-precision computation. It's not "true exact" beyond 5 significant figures. Extra significant figures are used to check the calculations from other computer set-ups, not necessarily to infer accuracy of data measurements here. Typically, the slight differences in decimal places on far right of decimal point are normal floating-point behavior in Tcl's expr.
gold 7/22/2026. A classical Oracle Black Box Simulation. The classical Quantum Amplitude Estimation QAE uses applicable modules from Grovers search as an example module sharing in TCL, but everything stays classical. In this case the Oracle function ends up being a regular TCL procedure. That means it runs like any other TCL function without needing quantum hardware. The "Oracle" used here is a standard classical procedure, not a quantum routine. Real quantum algorithms using oracles can offer theoretical speedup on actual quantum hardware, but this classical simulation does not provide any quantum advantage. It is intended only for learning and conceptual understanding. Please do not expect this code to run faster than any other classical estimation and search methods on large problems. The code is a teaching tool, not a practical quantum computer.
Real hardware has noise, error correction overhead, and implementation costs. These Toy Models are idealized for tutorial purposes, not final engineering estimates.
Clarifying the "Oracle" Concept. Many people become confused when they first hear the word Oracle in quantum computing. Many assume that the Oracle is a purely quantum routine that only runs on a real quantum computer. In Qiskit and most quantum SDKs, the initial stage is almost always a classical function written in Python. Meaning, Python that runs on a normal classical computer.
Details. Python-Qiskit code runs on classical hardware unless a quantum backend is explicitly used. Oracle like subcircuits can appear in both Grover and Shor Algorithms. But typically, Grover uses an obvious and so-named Oracle Function. Some later implementations of Shor and other Quantum Algorithms may hide that same idea and similar functions inside other Quantum circuit components, and maybe unnamed in the code.
You have asked for simple example problems for coding setup with simple high school math formulas. In layman terms, the Quantum solutions involve probabilistic logic. The Quantum computer is selecting the most probable answer for an extensive set of possibilities. More than one solution is possible or probable. In the Quantum solutions, there is careful problem setup, extensive state preparation on data , current processing, and postprocessing to select the most probable answer, modify , and modulate the answer. These example problems include a priori methods in design problem setup. Per request, this is an example of how the pseudocode or coders are mapping the solution in simple terms, not a formal math proof.
Caution: In actual Quantum circuit derived from a program, the Quantum Superposition formats the marking and estimation hit every grid point at the same time or simultaneously through Quantum Interference. The exec or calls are inserted to emphasize the differences between a sequential pseudocode and the QAE pseudocode.
Scalable limit of Laptop Memory, Classical Computer CC RAM_bytes = 2^(N + 4), given state_vector of Qubits (N) N = log2(RAM_bytes) - 4 RAM = 1 TB_terabyte = 2^40 bytes N = 40 - 4 = 36 qubits, not figuring CC overhead Usable Laptop Ram ~ 2.6 GB 2.6 GB ≈ 2.6 * 2^30 bytes 2.6 GB ≈ 2^31.3 bytes On cheap laptop, 20 Qubits seemed impossible dream for both Classical TCL/TK and Classical Python. So 20 Qubits picked for scalable limits study. N ≈ 20 Qubits, approximate practical memory limit of 20 Qubits on laptop.
Mapping of A Priori Solution, not a math proof
First Test Case (Path 1)
Path 1 uses a designed fraction that forces a near-pi result.
relation PI ≈ 4 * probability,
So probability ≈ 3.14 / 4 = 0.785. (This is the toy model and A Priori assumption here )
Qubit’s full state is described by 2 complex amplitudes
K = probability = |a|^2
a = amplitude = sqrt(K)
PI/4 = K ~ 0.785 probability (dimensionless) => a = sqrt(K) ~ 0.886 wave amplitude
Number of basis states = 2^N
For N = 2:
2^2 = 4 basis states
|00>, |01>, |10>, |11>
In amplitude estimation for QAE:
a = amplitude of the "good" state
K = probability of measuring the good state
K = a^2 (strict quantum rule )
For the 4 Qubit solution.
4 qubits = 2^N = 2^4 = 16 states total
each bin is 1/16 = 0.0625 or 6.24 percent
4-qubit (16 bins):
K=13/16=0.8125,
a = sqrt(0.8125) = 0.9014,
PI = 4*K ~ 3.25
Absolute error is 0.1084
Relative error on 4Q is about 0.0345, or 3.45 percent.
For a 5 Qubit solution.
5 Qubits = 2**5 = 32 states
each bin is 1/32 = 0.03125 or 3.125 percent
5-qubit (32 bins):
K=25/32 = 0.78125,
a= sqrt(25/32) = 0.8839,
PI= 4 * K = 4 * 0.78125 ~ 3.125
Absolute error ≈ 0.0166
Relative error on 5Q is 0.0053, or 0.53 percent.
For a 6 Qubit solution.
6 Qubits = 2**6 = 64 states
each bin is 1/64 = 0.015625 or 1.5625 percent
6-qubit (64):
K= 50/64 = 0.78125 , same as 5 Qubits
Note, or use K = 51/64 = 0.796875, giving PI = 3.1875,
bins getting small. Model showing diminishing returns.
a = sqrt(50/64) ≈ 0.883883
PI = 4 * K = 3.125 ????
The relative error on 6Q is 0.0053, or 0.53 percent.
Note. Improvement over 5 qubits is modest or zip.
Note. Toy Model may be approaching limit of useful
returns for computation effort, multiple scalability issues.
Ideal performance on 10^7 QAE sweeps, order of magnitude estimate
computation time ~ 40 seconds
For a 12 Qubit solution,
would be painfully slow on laptop.
12 qubits = 2^12 = 4096 bins
each bin is 1/4096 = 0.0002441 or 0.02441 percent, rounded
target p ≈ 0.785
12-qubit (4096):
K = 3214/4096 ≈ 0.785156,
a = 0.886,
PI = 4*K ~ 3.140625
Relative error on 12 Qubit case is 0.00031,
or 0.031 percent. correct checked.
Ideal performance on 10^7 QAE sweeps
time ~ 40 seconds, order of magnitude estimate, Toy Model
My Classical Laptop equivalent to 20 Qubits
memory has Scalable limits to QAE
expr { 2**20} = 1048576
expr {1./1048576.} = 9.5367E-7, 9.5267E-5 percent
bins = 2^N = 2^20 ≈ 1048576 bins
each bin is 1 / 1048576 = or 9.5267E-5 percent, rounded
simple ideal logic, overhead & OS would be far more limiting.
Low qubits (3–6) ≈ 3.12–3.15 ,
3-6 qubits has small number of bins
& high granularity, but reasonable C. times
20-Qubit (formuala 2^20):
K = 823549 / 1048576 = 0.785, rounded.
expr { 823549 / 1048576. } = 0.7853975, rnd
check = expr {(823549. / 1048576.)**0.5} = 0.886226 rnd
a = 0.886226 , suspect past or approaching
wave measurement limits, Checkmate!!!
PI = 3.141592, ideal toy with many assumptions.
Note: As of 2026, approaching scalability errors,
readout errors, absolute errors K
in the range 0.01 – 0.05 moderate depth.
Because a = sqrt(K), derived absolute error
amplitude a is roughly 0.005 – 0.03.
Final realistic QAE error on pi or e is often 0.02 – 0.15.
For 20Q toy model, 10^5 to 10^6 sweeps for useful precision.
For 1E6 sweeps, roughly 2–6 days on 20Q toy model, idealized
10^9 QAE sweeps ~ time ≈ ~4 years, range 3 to 4 years.
but laptop has high overhead
and beyond 14 qubits near impossible computation times in CC laptop.
Result on 20 Qubits reflects the design of the toy model rather
than a realistic noisy CC computation.
Classical overhead, cache behavior, and operating system activity
would make laptop runtime even longer and far more fragile.
The 20 qubit testcase, therefore serves best
as a conceptual upper bound and a thought experiment on scalability.
--- QAE NOTE on Strict Quantum definitions ---
QAE estimates amplitude `a`.
Measurement yields prob K = a^2.
Toy model maps K , PI/4 directly; `a` is sqrt(K) only.
This is where the Quantum algorithm differs from Classical methods,
Probability is assigned or measured to wave amplitude in QAE.
Mapping of Different QAE Assumptions, not a math proof
Second Test Case (Path 2)
Second path follows the Monte Carlo structure,
meaning the geometric model,
used in actual QAE-for-pi circuits.
Random points (x, y) are encoded.
A circuit marks states where x^2 + y^2 <= 1.
The good probability is p = pi/4.
QAE estimates p, then multiplies by 4 to recover pi.
Estimates probability points inside the unit circle,
then scale by 4.
Stays close to the first-path 5-qubit numbers,
so resulting coding formulas almost identical.
----
The math is kept simple for high-school level mapping.
No heavy arithmetic circuits are simulated.
----
# These are high level exec or calls in pseudocode
# Caution: Underlying Quantum Interference process is
# coherent and simultaneous rather than purely sequential.
# This point is where Classical Computers reach limits of
# Scalability.
exec { Call state prep for equal superposition over grid points.}
exec { Call coord mapping to encode discrete (x, y) pairs. }
exec { Call marking oracle for x² + y² ≤ 1 states. }
exec { Call controlled amplitude-estimation iterates.}
exec { Call QFT on count register, measure, extract K.}
----
2 qubits = 2**2 = 4 states
Each bin = 1/4 = 0.25
K = 3/4 = 0.75
a = sqrt(0.75) ≈ 0.8660
PI = 4 * K = 3.00
Absolute error ≈ 0.1416
Relative error ≈ 4.51 percent
4 qubits = 2**4 = 16 states
Each bin = 1/16 = 0.0625
K = 13/16 = 0.8125
a = sqrt(0.8125) ≈ 0.9014
PI = 4 * K = 3.25
Absolute error ≈ 0.1084
Relative error ≈ 3.45 percent
5 qubits = 2**5 = 32 total states
Target good probability K ≈ 0.785398
Chosen good states (conservative discrete count):
K = 25/32 = 0.78125
a = sqrt(0.78125) ≈ 0.88388
PI = 4 * K = 3.125
Absolute error ≈ 0.01659
Relative error ≈ 0.53 percent
6 qubits = 2**6 = 4096 total states
Each bin ≈ 0.0002441
K = 3214/4096 ≈ 0.785156
a ≈ 0.8861
PI = 4 * K ≈ 3.140625
Absolute error ≈ 0.000968
Relative error ≈ 0.031 percent
12 qubits = 2**12 = 4096 states
Each bin ≈ 0.0002441
K = 3214/4096 ≈ 0.785156
a ≈ 0.8861
PI = 4 * K ≈ 3.140625
Absolute error ≈ 0.000968
Relative error ≈ 0.031 percent
Second path follows the Monte Carlo structure,
meaning the geometric model. Mapping of Different QAE Assumptions, not a math proof Third Test Case (Path 3) ---- Path 3 for e simply reuses the same numerical framework with a different target constant. It does not rely on a circle or any geometric area. It is only an amplitude-estimation style mapping chosen for teaching convenience. ---- The math is kept simple and idealized for high-school level mapping. No heavy arithmetic circuits are simulated. ---- Target: e ≈ 2.71828 Mapping used: e ≈ 4 * K, So target K ≈ 0.67957 2 qubits = 2**2 = 4 states K = 3/4 = 0.75 a ≈ 0.8660 e_est = 3.00 Absolute error ≈ 0.2817 Relative error ≈ 10.36 percent 4 qubits = 4^4 = 16 states K = 11/16 = 0.6875 a ≈ 0.8292 e_est = 2.75 Absolute error ≈ 0.0317 Relative error ≈ 1.17 percent 5 qubits = 2^5 = 32 states K = 22/32 = 0.6875 a ≈ 0.8292 e_est = 2.75 Absolute error ≈ 0.0317 Relative error ≈ 1.17 percent 6 qubits = 2**6 = 64 states K = 43/64 = 0.671875 a ≈ 0.8197 e_est = 2.6875 Absolute error ≈ 0.0308 Relative error ≈ 1.13 percent 12 qubits = 4096 states K = 2784/4096 ≈ 0.679688 a ≈ 0.8244 e_est ≈ 2.71875 Absolute error ≈ 0.00047 Relative error ≈ 0.017 percent Path 3 keeps the same coding formulas as the earlier lists. Only the recovered constant changes from pi to e.
Mapping of Different QAE Assumptions, not a math proof Path 4 with Small Phase Correction (e) Target: e ≈ 2.71828 Base mapping: e ≈ 4 * K, so target K ≈ 0.67957 One extra correction line is added: e_corrected = 4 * K * (1 + phase_factor) A small fixed phase_factor of +0.011 is used for illustration. 2 qubits = 2^2 = 4 states K = 3/4 = 0.75 e_raw = 3.00 e_corrected = 3.00 * 1.011 ≈ 3.033 Absolute error ≈ 0.315 4 qubits = 4^4 = 16 states K = 11/16 = 0.6875 e_raw = 2.75 e_corrected = 2.75 * 1.011 ≈ 2.780 Absolute error ≈ 0.062 5 qubits = 32 states K = 22/32 = 0.6875 e_raw = 2.75 e_corrected = 2.75 * 1.011 ≈ 2.780 Absolute error ≈ 0.062 6 qubits 2^4 = 64 states K = 43/64 = 0.671875 e_raw = 2.6875 e_corrected = 2.6875 * 1.011 ≈ 2.717 Absolute error ≈ 0.0013 12 qubits = 2**12 = 4096 states K = 2784/4096 ≈ 0.679688 e_raw ≈ 2.71875 e_corrected ≈ 2.71875 * 1.011 ≈ 2.7487 Absolute error ≈ 0.0304
Caution Statement.
Add a simple phase-related correction or a conceptual Phase Estimation correction step for e, but it will still be a classical toy-model approximation. It will not become real Quantum Phase Estimation (QPE).
The phase_factor is a simple empirical adjustment (a quadratic-style factor). phase_factor is added only for teaching illustration and is not derived from Quantum Phase Estimation. Strict mathematical treatments do not use this kind of ad-hoc correction.
Draft. The selected algorithms are very different in classical languages like TCL/TK and Python versus Quantum computer algorithms in Python-Qiskit. Classical simulation runs on a normal computer. Classical methods use ordinary math and loops. Classical does not touch real qubits, by definition here. Classical computers do not provide quantum speedup.
Draft. There are shades of meaning here. Quantum computer algorithms in Python-Qiskit build real quantum circuits of qubits. Python-Qiskit uses qubits and gates to create a true quantum state (eventual solution). Quantum computer algorithms may run through either a Quantum simulator or a Quantum hardware backend to produce quantum results. That Quantum simulator in Python-Qiskit is still classical until the Quantum hardware fired up. In other words, the Quantum simulator ref Python-Qiskit does not give Quantum Speedup. Only the Quantum hardware gives Quantum Speedup. Refer to the IBM Quantum Platform, Python-Qiskit Quick Start. Also, the textbook "Learn Quantum Computing using Qiskit' on Github.
We need as much of the previous Grover pieces and modules like Oracle Function saved inside the QAE Pie. We want to show readers that the Tcl modules are transferrable to other tasks, not stand alone and one trick ponies. We spent lot of time on that Grover software. These Grover-era pieces and modules intact, best as possible.
Here are practical examples for the same Function in various classical computer tasks.
Scaling in code refers to metrics as program keeps working as the input size, number of users, or amount of parameters/data grows.
There is one limiting structural difference between the Tcl syntax and design of practical quantum circuits. A Tcl list works with any length, so the original Proc version took any $max_state. Quantum registers only allow sizes that are powers of two. This means the $max_state has to be one less than a power of two such as 7 15 or 31. This is effectively a constraint on the practical number of Qubits in the solution circuit. By inspection, the original autotests were limited to circuits of 1,2,3,4,5 qubits. The first case of 1 Qubit circuit was an edge or corner testcase, no solution seen.
For the simulation in Tcl, the Number of Qubits in the Quantum circuit has to be capped because of lengthy laptop computation times beyond 10 qubits. Comfortable QAE use on a Windows 11 laptop might be about 5 to 6 qubits at 32 to 64 states. A normal laptop becomes painfully slow around 12 qubits at 4,096 states. The Tcl Oracle simulation is assessed impractical beyond 14 qubits at ~16K states.
Draft. The Scalable Limits or envelope of a classical TCL solution can be compared to a classical Python solution from the Python literature and rules of thumb. The Python specialists have been working on the Quantum Amplitude Estimation QAE for about ~25 years. The Python Qiskit SDK was announced or widely available from IBM in March 2017. The QAE was first implemented in the Aqua module. Later, QAE was rewritten in Python-Qiskit. Python-Qiskit has had Quantum Amplitude Estimation installed since about 2020. However, confining discussion Scalable Limits to classical models and omitting the Quantum backend. Estimate Classical Python + NumPy on QAE: Comfortable ~12-14 qubits, est. usable to ~16 qubits.
Draft. So, in some sense there is a granularity problem as Scalable Limits in QAE. The more accuracy for the estimation target, the more bins require more qubits and more complex operations. That would play better in some quarters. Nothing is free, this seems more like conservation of resources ref Dr. Chiarra Marletto in constructor theory.
eval { 2**N } is formula
eval { 2**5 } = 32
eval { 2**6 } = 64
eval { 2**10 } = 1024
eval { 2**12 } = 4096
eval { 2**14 } = 16384
eval { 2**15 } = 32768
eval { 2**16 } = 65536Draft. Concerning the projected solution in the proposed Python-Qiskit Port, would ASCII diagrams be suitable? The main flow might be shown in ASCII diagrams, I suppose, but would parallel, phased, timing, or simultaneous channels be adequately shown, without some understood notation changes? If there is a perceptible quantum circuit designed in Python-Qiskit, I would be interested in the 2‑ and 3‑qubit circuits.
Typically, Classical computers need many more trials and much computer time to gain extra decimal places of accuracy. The TCL/TK coding can be used to model or simulate those portions or stages of a Quantum Algorithm that may use a classical computer. These are Toy Models and simplified estimates for tutorial purposes.
Classical Simulation offers a clear way to understand how search behaves without using a quantum device. The Classical simulation helps beginners and students see how the search pattern emerges from repeated queries. The same ideas and ideas prepare students for later work with real quantum circuits. That is, when stable hardware becomes available.
| Index | Language / Variant | Abbrev Syntax Example | Ease of Coding (vs 77 style) | Quibble Notes |
|---|---|---|---|---|
| 1 | Tcl (lists) | lset amp $i expr ... | Easy | Slow for large N. Baseline for education. |
| 2 | Tcl (dicts) | dict set amp $i $val | Easy | Higher overhead. Not ideal for dense QAE. |
| 3 | Tcl (loops) | for {set i 0} {$i < $N} {incr i} | Easy | Standard Tcl style. Interpreter limited. |
| 4 | Python (lists) | ampi = ... | Easy | Moderate speed. Good for quick tests. |
| 5 | Python + NumPy | amp = 2*mean - amp | Easy | Vectorized. Strong practical choice. |
| 6 | Fortran 77 | DO I=1,N ... ENDDO | Medium (old style) | Very fast static arrays. |
| 7 | Fortran 90+++ | amp = 2*mean - amp | Easy | Modern syntax with high performance. |
| 8 | C (arrays) | ampi = 2*mean - ampi; | Medium | Very fast. Low overhead. |
| 9 | C++ | ampi = 2*mean - ampi; | Medium | Fast + flexible with libraries. |
| 10 | MATLAB | amp = 2*mean - amp; | Very Easy | Fast vectorized operations. Good for prototyping. |
| 11 | Julia | amp .= 2*mean .- amp | Easy | High performance with simple syntax. |
| 12 | Go | ampi = 2*mean - ampi | Medium | Good speed and safety. Modern but less common for numerics. |
| 13 | Rust | ampi = 2.0*mean - ampi; | Medium-Hard | Very fast + memory safe. Steep learning curve. |
| AUDIT | - | - | - | Compiled languages generally outperform interpreted ones. Choice depends on speed vs development time trade-off. |
| AUDIT | - | - | - | Compiled languages (C, C++, Fortran, Rust, Julia) significantly outperform interpreted ones (Tcl, Python lists) for large N. Choice depends on speed vs development time. |
| AUDIT | - | - | - | Performance ranking depends on N and K. Compiled languages win on speed. Tcl best for small educational demos. |
Note. These Snippets on Theoretical Physics are a set, not stand alones. Recommend read all of the set.
TCL Wiki has numerous excellent pages on Monte Carlo methods, largely from arjen .
Note. The ink is hardly dry on some of these papers. Don't know what gems are hidden, if I dig deeper.
Due to the space on wiki page, I am omitting some wordy explanatory comments inside the deck, while debugging. The credits are normally included inside code comments, but listed below deck.
# Classical Simulation of Oracle Function Algorithm V5
# in pure Tcl 8.6+ for tutorial purposes.
# Tcl 8.6 or greater required
# Quantum algorithm simulation on a classical computer.
# Classical Simulation code does not provide Quantum Speedup.
# Quantum Speedup requires actual Quantum hardware,
# Quantum feasible algorithms, and Quantum Error Correction QEC.
# Naming convention: all proc and variable names are 12-15
# characters, descriptive, and domain-neutral so the engine
# can serve any subject area without modification.
#
# ----
# Compatible with Tcl/Tk (Tool Command Language / Toolkit) 8.6+
# Written for Windows 11 on ActiveState Tcl.
# Use Pure 7-bit ASCII code, no Unicode characters used anywhere.
# ----
# Using modular snippets inside modular structured programs.
# Modules should be 15 to 25 lines long without comments.
# Small length modules
# are believed to aid future code maintenance.
# Program deck may contain multiple estimation procs.
# Deck May contain code dependencies on Active State and Windows 11
# Complex math calculations up to 8 units computer time
# Wait for complete calculations before saving files.
# Proc names and variables names need to be very human readable
# and very explanatory.
# Avoid variables with single letter names.
# Whereas single letter names are known to lead
# to many historic errors.
# Assume a future maintainer either AI or human would
# have to maintain code with info content in program.
# This is Experimenting Draft Prototype,
# and not a replacement for TCL Core.
# This is a prototype's patch, not rigorously derived.
# appears correct solutions for autotests.
# The Grover Oracle is listed as a namespace.
# This is a prototype's patch, not rigorously derived.
# appears correct solutions for autotests.
#
# File contains the revised oracle module.
# This file will be base of the QAE algorithm.
# TCL Club 8/5/2026
#
if {[llength [info commands console]] > 0} {
console show
}
namespace eval ::grover_engine {
# oracle module: pure oracle state; default list empty
namespace eval oracle {
namespace path [list ::grover_engine]
variable good_solutions {}
proc set_solutions {new_list} {
variable good_solutions
set good_solutions $new_list
}
proc query_state {test_state} {
variable good_solutions
if {$test_state in $good_solutions} {
return 1
} else {
return 0
}
}
proc apply_phase_oracle {test_state} {
if {[query_state $test_state]} {
return -1
} else {
return 1
}
}
proc count_marked_states {max_state} {
variable good_solutions
set marked_total 0
foreach candidate $good_solutions {
if {$candidate <= $max_state} {
incr marked_total
}
}
return $marked_total
}
}
# math_core module: pure computation, no I/O
namespace eval math_core {
namespace path [list ::grover_engine]
proc enforce_qubit_limit {max_state} {
set qubit_limit 5
set state_limit [expr {(1 << $qubit_limit) - 1}]
if {$max_state > $state_limit} {
return $state_limit
}
return $max_state
}
proc run_grover_search {max_state num_iterations} {
set total_states [expr {$max_state + 1}]
set start_amplitude [expr {1.0 / sqrt(double($total_states))}]
set amplitude_list {}
for {set i 0} {$i <= $max_state} {incr i} {
lappend amplitude_list $start_amplitude
}
for {set iter 1} {$iter <= $num_iterations} {incr iter} {
for {set i 0} {$i <= $max_state} {incr i} {
set phase [oracle::apply_phase_oracle $i]
lset amplitude_list $i [expr {[lindex $amplitude_list $i] * $phase}]
}
set mean_value [expr {[tcl::mathop::+ {*}$amplitude_list] / double($total_states)}]
for {set i 0} {$i <= $max_state} {incr i} {
set new_val [expr {2.0 * $mean_value - [lindex $amplitude_list $i]}]
lset amplitude_list $i $new_val
}
}
return $amplitude_list
}
proc normalize_amp_list {amplitude_list} {
set sum_squares 0.0
foreach amp $amplitude_list {
set sum_squares [expr {$sum_squares + ($amp * $amp)}]
}
if {$sum_squares <= 0.0} {
return $amplitude_list
}
set drift_amount [expr {abs($sum_squares - 1.0)}]
if {$drift_amount < 0.000001} {
return $amplitude_list
}
set scale_factor [expr {1.0 / sqrt($sum_squares)}]
set normalized_list {}
foreach amp $amplitude_list {
lappend normalized_list [expr {$amp * $scale_factor}]
}
return $normalized_list
}
proc apply_display_phase {amplitude_list} {
if {[llength $amplitude_list] == 0} {
return $amplitude_list
}
set first_amp [lindex $amplitude_list 0]
if {$first_amp < 0.0} {
set flipped_list {}
foreach amp $amplitude_list {
lappend flipped_list [expr {-1.0 * $amp}]
}
return $flipped_list
}
return $amplitude_list
}
proc compute_optimal_iter {max_state marked_total} {
if {$marked_total <= 0} {
return 0
}
set total_states [expr {$max_state + 1}]
set raw_count [expr {
(3.14159265 / 4.0) * sqrt(double($total_states) / double($marked_total))
}]
return [expr {int(floor($raw_count))}]
}
proc compute_bit_width {max_state} {
set total_states [expr {$max_state + 1}]
set bit_count 1
while {(1 << $bit_count) < $total_states} {
incr bit_count
}
return $bit_count
}
proc compute_grover_outcome {max_state num_iterations} {
set amplitude_list [run_grover_search $max_state $num_iterations]
set amplitude_list [normalize_amp_list $amplitude_list]
set amplitude_list [apply_display_phase $amplitude_list]
set marked_total [oracle::count_marked_states $max_state]
set optimal_rounds [compute_optimal_iter $max_state $marked_total]
set result_rows {}
set probability_sum 0.0
set target_probability_sum 0.0
for {set i 0} {$i <= $max_state} {incr i} {
set amp [lindex $amplitude_list $i]
set prob [expr {$amp * $amp}]
set probability_sum [expr {$probability_sum + $prob}]
if {[oracle::query_state $i]} {
set target_probability_sum [expr {$target_probability_sum + $prob}]
}
lappend result_rows [list $i $amp $prob]
}
return [list $result_rows $marked_total $optimal_rounds \
$probability_sum $target_probability_sum]
}
}
# io_utils module: console logging and file primitives
namespace eval io_utils {
namespace path [list ::grover_engine]
variable console_log_channel ""
proc sanitize_ascii_text {text_value} {
set output_text ""
set text_length [string length $text_value]
for {set char_index 0} {$char_index < $text_length} {incr char_index} {
set one_char [string index $text_value $char_index]
scan $one_char %c one_code
if {$one_code > 127} {
append output_text "?"
} else {
append output_text $one_char
}
}
return $output_text
}
proc write_ascii_line {channel_id text_value} {
puts $channel_id [sanitize_ascii_text $text_value]
}
proc build_date_stamp {} {
return [clock format [clock seconds] -format {%Y%m%d_%H%M%S}]
}
proc start_console_log {} {
variable console_log_channel
set stamp_text [build_date_stamp]
set log_file_name "grover_console_log_${stamp_text}.txt"
set console_log_channel [open $log_file_name w]
write_ascii_line $console_log_channel "Grover Simulation Console Log, Revision 5"
write_ascii_line $console_log_channel "Created: $stamp_text"
write_ascii_line $console_log_channel "Encoding: pure 7-bit ASCII, sanitized at write time"
write_ascii_line $console_log_channel "-----------------------------------"
return [list $log_file_name $stamp_text]
}
proc log_console_line {message_text} {
variable console_log_channel
set safe_text [sanitize_ascii_text $message_text]
puts $safe_text
if {$console_log_channel ne ""} {
puts $console_log_channel $safe_text
}
}
proc stop_console_log {} {
variable console_log_channel
if {$console_log_channel ne ""} {
close $console_log_channel
set console_log_channel ""
}
}
}
# formatters module: pure string building, no side effects
namespace eval formatters {
namespace path [list ::grover_engine]
proc build_wiki_block {test_index test_label result_rows \
probability_sum target_probability_sum max_state} {
set bit_width [math_core::compute_bit_width $max_state]
set lines {}
lappend lines "Wiki table for $test_label"
lappend lines "%| test | idx | dec | bin | amp | prob | note |%"
set row_index 1
foreach row $result_rows {
lassign $row state_num amp prob
if {[oracle::query_state $state_num]} {
set quibble_note "target, phase-flipped"
} else {
set quibble_note "background"
}
set binary_text [format "%0${bit_width}b" $state_num]
lappend lines [format "&| %d | %d | %d | %s | %.4f | %.4f | %s |&" \
$test_index $row_index $state_num $binary_text $amp $prob $quibble_note]
incr row_index
}
lappend lines [format "&| %d | AUDIT | sum | - | - | %.4f | prob total |&" \
$test_index $probability_sum]
lappend lines [format "&| %d | SUCCESS | target | - | - | %.4f | marked-state prob |&" \
$test_index $target_probability_sum]
lappend lines ""
return $lines
}
proc build_prose_text {test_label max_state num_iterations result_rows \
marked_total optimal_rounds probability_sum target_probability_sum} {
set total_states [expr {$max_state + 1}]
set best_state -1
set best_prob -1.0
foreach row $result_rows {
lassign $row state_num amp prob
if {$prob > $best_prob} {
set best_prob $prob
set best_state $state_num
}
}
if {$marked_total == 0} {
return [format "%s: space=%d marked=0 iters=%d -- flat,\
no targets. prob_sum=%.4f" \
$test_label $total_states $num_iterations $probability_sum]
}
set baseline_target [expr {double($marked_total) / double($total_states)}]
set hit_flag [expr {[oracle::query_state $best_state] ? "hit" : "miss"}]
return [format "%s: space=%d marked=%d iters=%d opt=%d --\
best=state%d p=%.4f (%s). target_sum=%.4f base=%.4f\
prob_sum=%.4f" \
$test_label $total_states $marked_total $num_iterations \
$optimal_rounds $best_state $best_prob $hit_flag \
$target_probability_sum $baseline_target $probability_sum]
}
proc build_final_summary {all_summary_rows} {
set total_tests [llength $all_summary_rows]
set amplified_count 0
set no_solution_count 0
foreach row $all_summary_rows {
lassign $row test_label marked_total target_probability_sum baseline_target
if {$marked_total == 0} {
incr no_solution_count
} elseif {$target_probability_sum > $baseline_target} {
incr amplified_count
}
}
return [format "tests=%d amplified=%d flat=%d" \
$total_tests $amplified_count $no_solution_count]
}
}
# reports module: file-writing drivers
namespace eval reports {
namespace path [list ::grover_engine]
proc save_wiki_report {file_name stamp_text all_wiki_blocks} {
set fh [open $file_name w]
io_utils::write_ascii_line $fh "Grover Wiki Table Report, Revision 5"
io_utils::write_ascii_line $fh "Created: $stamp_text"
io_utils::write_ascii_line $fh "Encoding: pure 7-bit ASCII, sanitized at write time"
io_utils::write_ascii_line $fh ""
foreach block $all_wiki_blocks {
foreach line $block {
io_utils::write_ascii_line $fh $line
}
}
close $fh
}
proc save_prose_report {file_name stamp_text all_paragraphs final_summary} {
set fh [open $file_name w]
io_utils::write_ascii_line $fh "Grover Prose Report, Revision 5"
io_utils::write_ascii_line $fh "Created: $stamp_text"
io_utils::write_ascii_line $fh "Encoding: pure 7-bit ASCII, sanitized at write time"
io_utils::write_ascii_line $fh ""
io_utils::write_ascii_line $fh "Notes: amplitude sign and iter-cap are judgement calls."
io_utils::write_ascii_line $fh ""
foreach paragraph $all_paragraphs {
io_utils::write_ascii_line $fh $paragraph
io_utils::write_ascii_line $fh ""
}
io_utils::write_ascii_line $fh "Closing Summary"
io_utils::write_ascii_line $fh $final_summary
close $fh
}
proc save_text_dump_all {file_name stamp_text all_test_rows} {
set fh [open $file_name w]
io_utils::write_ascii_line $fh "Grover Text Dump, Revision 5"
io_utils::write_ascii_line $fh "Created: $stamp_text"
io_utils::write_ascii_line $fh "Encoding: pure 7-bit ASCII, sanitized at write time"
io_utils::write_ascii_line $fh "INDEX STATE AMPLITUDE PROBABILITY TEST_LABEL"
foreach entry $all_test_rows {
lassign $entry test_label result_rows
set row_index 1
foreach row $result_rows {
lassign $row state_num amp prob
io_utils::write_ascii_line $fh [format "%d %d %.6f %.6f %s" \
$row_index $state_num $amp $prob $test_label]
incr row_index
}
}
close $fh
}
}
# main controller layer
proc print_grover_result {max_state num_iterations test_label} {
set outcome [math_core::compute_grover_outcome $max_state $num_iterations]
lassign $outcome result_rows marked_total optimal_rounds \
probability_sum target_probability_sum
io_utils::log_console_line ""
io_utils::log_console_line "-- $test_label --"
io_utils::log_console_line [format "space=%d marked=%d iters=%d opt=%d" \
[expr {$max_state + 1}] $marked_total $num_iterations $optimal_rounds]
io_utils::log_console_line "state | amp | prob"
io_utils::log_console_line "------|-----|-----"
foreach row $result_rows {
lassign $row i amp prob
io_utils::log_console_line [format "%5d | %9.4f | %9.4f" $i $amp $prob]
}
io_utils::log_console_line [format "audit: prob_sum=%.4f target_sum=%.4f" \
$probability_sum $target_probability_sum]
return [list $result_rows $marked_total $optimal_rounds \
$probability_sum $target_probability_sum]
}
proc run_grover_auto_tests {} {
set test_cases {
{7 2 {}}
{7 2 {7}}
{15 2 {10}}
{15 3 {0}}
{15 2 {3 5}}
{15 3 {3 5 11}}
{7 4 {7}}
{31 3 {13}}
{31 4 {7 15 23}}
{3 1 {1}}
}
lassign [io_utils::start_console_log] log_file_name stamp_text
io_utils::log_console_line "Grover auto test run started."
io_utils::log_console_line "Console log file: $log_file_name"
set wiki_file_name "grover_wiki_tables_${stamp_text}.txt"
set prose_file_name "grover_prose_report_${stamp_text}.txt"
set dump_file_name "grover_text_dump_${stamp_text}.txt"
set all_wiki_blocks {}
set all_paragraphs {}
set all_test_rows {}
set all_summary_rows {}
set test_index 1
foreach case $test_cases {
lassign $case max_state num_iter marked_list
set max_state [math_core::enforce_qubit_limit $max_state]
oracle::set_solutions $marked_list
set test_label "Test $test_index (max=$max_state iters=$num_iter)"
io_utils::log_console_line ""
io_utils::log_console_line "=== $test_label ==="
io_utils::log_console_line "marked: $marked_list"
set outcome [print_grover_result $max_state $num_iter $test_label]
lassign $outcome result_rows marked_total optimal_rounds \
probability_sum target_probability_sum
set total_states [expr {$max_state + 1}]
set baseline_target 0.0
if {$marked_total > 0} {
set baseline_target [expr {double($marked_total) / double($total_states)}]
}
lappend all_wiki_blocks [formatters::build_wiki_block $test_index $test_label \
$result_rows $probability_sum $target_probability_sum $max_state]
lappend all_paragraphs [formatters::build_prose_text $test_label $max_state $num_iter \
$result_rows $marked_total $optimal_rounds $probability_sum \
$target_probability_sum]
lappend all_test_rows [list $test_label $result_rows]
lappend all_summary_rows [list $test_label $marked_total \
$target_probability_sum $baseline_target]
incr test_index
}
set final_summary [formatters::build_final_summary $all_summary_rows]
reports::save_wiki_report $wiki_file_name $stamp_text $all_wiki_blocks
reports::save_prose_report $prose_file_name $stamp_text $all_paragraphs $final_summary
reports::save_text_dump_all $dump_file_name $stamp_text $all_test_rows
io_utils::log_console_line ""
io_utils::log_console_line "Done: 10 tests."
io_utils::log_console_line $final_summary
io_utils::log_console_line "Files:"
io_utils::log_console_line " $log_file_name"
io_utils::log_console_line " $wiki_file_name"
io_utils::log_console_line " $prose_file_name"
io_utils::log_console_line " $dump_file_name"
io_utils::stop_console_log
}
namespace export run_grover_auto_tests
}
::grover_engine::run_grover_auto_tests
# End of file# References. # # Inspired by counterfactual principles discussed in Chiara Marletto's book # "The Science of Can and Can't: A Physicist's Journey # Through the Land of Counterfactuals" (2021). # The dummy subroutine implements a generic simulation # for educational purposes only. # puts "Credits" # Original 2002 paper, Quantum Amplitude Estimation (QAE) # algorithm by Brassard et al., 2002, # original 1996 paper — "A Fast Quantum Mechanical Algorithm # for Database Search," Lov K. Grover, AT&T Bell Labs, # presented at STOC '96: # 1997 follow-up, often cited & more accessible physics-journal: # "Quantum Mechanics Helps in Searching for a Needle # in a Haystack," Lov K. Grover, Phys. Rev. Lett. 79, 325 (1997). # The algorithm (Shor’s) is public domain, # and mathematical knowledge since 1994. # Peter Shore, Original 1994 Conference Paper # Algorithms for Quantum Computation: Discrete Logarithms and Factoring # Peter Shore, Polynomial-Time Algorithms for Prime Factorization # and Discrete Logarithms on a Quantum Computer (1995 expanded version) puts "Reference: Maria Violaris, arXiv:2601.08102v1, January 2026" puts "Reference: https://wiki.tcl-lang.org/page/Snippets+Quantum+Many+Worlds" puts "Based on ref. An Undergraduate Course in Quantum Computing, Peter Young, Apr 2026" puts "Much credit for the quantum circuit diagrams, Matches textbook Fig 16.4 etc" puts "University of California Santa Cruz, CA, arXiv:2604.10396"
Note. The Testcase 1 is defined as an edge or corner case. Don't expect much accuracy from that. Even if Testcase 1 is faulty solution, the first testcase shows coder that the signal amplitude and signal probability is mapped correctly and correct values across the assigned solution space of 1 cubit. If the signal amplitude and signal probability is not marked correctly, not much use in preceding on to 2 Qubits, 3,4,5,6 etc. This is called a sanity check in some quarters. The Testcase 10 is defined as an edge or corner case. Don't expect much accuracy from that. The 10th case shows the cap is fired on max number of Qubits in circuit. Maybe, degradation and lagging algorithm scalability on lengthy computation time.
| Test | Qubits | Precision | Marked | Estimated a | Estimated pi | Abs Error | | 1 | 3 | 1 | 4 | 0.781806 | 3.127226 | 0.014367 | | 2 | 3 | 2 | 4 | 0.789483 | 3.157931 | 0.016338 | | 3 | 4 | 1 | 6 | 0.785615 | 3.142459 | 0.000867 | | 4 | 4 | 2 | 6 | 0.791861 | 3.167444 | 0.025851 | | 5 | 4 | 3 | 6 | 0.788243 | 3.152971 | 0.011378 | | 6 | 5 | 2 | 6 | 0.786384 | 3.145535 | 0.003942 | | 7 | 5 | 3 | 6 | 0.787884 | 3.151537 | 0.009944 | | 8 | 6 | 2 | 6 | 0.782401 | 3.129604 | 0.011989 | | 9 | 6 | 3 | 6 | 0.785733 | 3.142931 | 0.001338 | | 10 | 6 | 4 | 6 | 0.785233 | 3.140932 | 0.000661 |
Note. Using Automatic Return in Tcl Procs. If the return command is not present, the procedure automatically returns the value of the last expr statement. This is standard Tcl behavior. Very convenient, but sometimes confusing or double take for visitors from other computer languages.
+-------------------------------------------------------------+ | 2 System Qubits + 2 Ancilla Qubits | | | | a0: ─[H]─────────────●───────────────────●───────[QFT†]──M | | │ │ | | a1: ─[H]─────────────┼───────●───────────┼───────[QFT†]──M | | │ │ │ | | q0: ─[A]────────[Q¹]─┼───[Q²]───────────┼───────────────── | | │ │ │ | | q1: ─[A]────────[Q¹]─┴───[Q²]───────────┴───────────────── | | | | Legend: | | [H] = Hadamard gate | | [A] = State Preparation | | [Q^k] = Grover operator Q raised to power k (2^k iters) | | [QFT†] = Inverse Quantum Fourier Transform | | ● = Control | | M = Measurement | +-------------------------------------------------------------+
+-------------------------------------------------------------------+ | 3 System Qubits + 3 Ancilla Qubits | | | | a0: ─[H]───────●─────────●─────────●────────────[QFT†]────M | | │ │ │ | | a1: ─[H]───────┼────●────┼────●────┼────────────[QFT†]────M | | │ │ │ │ │ | | a2: ─[H]───────┼────┼────┼────┼────●────────────[QFT†]────M | | │ │ │ │ | | q0: ─[A]────[Q¹]─┼─[Q²]──┼─[Q⁴]──┼─[Q⁸]─────────────────────── | | │ │ │ │ | | q1: ─[A]────[Q¹]─┼─[Q²]──┼─[Q⁴]──┼─[Q⁸]─────────────────────── | | │ │ │ │ | | q2: ─[A]────[Q¹]─┴─[Q²]──┴─[Q⁴]──┴─[Q⁸]─────────────────────── | | | | Legend: | | [H] = Hadamard gate | | [A] = State Preparation | | [Q^k] = Grover operator Q raised to power k (2^k iterations) | | [QFT†] = Inverse Quantum Fourier Transform on ancilla register | | ● = Control | | M = Measurement | +-------------------------------------------------------------------+
+------------------------------------------------------------+ | STANDARD DIFFUSER BLOCK (same as Grover) | | This block is embedded in every controlled-Q operator | | | | q0 ─[H]──[X]─────●─────[X]──[H]── | | │ | | q1 ─[H]──[X]─────●─────[X]──[H]── | | │ | | q2 ─[H]──[X]─────●─────[X]──[H]── | | | | Legend: | | [H] = Hadamard gate | | [X] = Pauli-X gate | | ● = Multi-controlled Z (CZ for 2 qubits, CCCZ for 3) | +------------------------------------------------------------+
Note: This diffuser reflects about the uniform superposition. The diffuser is combined with the oracle reflection to form the Grover iterator Q.
+---------------------------------------------------------------+ | QAE ANCILLA MEASUREMENT BINS (8 bins from 3 ancilla qubits) | | | | Bin: 0 1 2 3 4 5 6 7 | | Prob: 0.00 0.00 0.00 0.05 0.90 0.05 0.00 0.00 | | | | | | | | | | | | | | | | | |#### |######|#### | | | | | | | |#### |######|#### | | | | | | | |#### |######|#### | | | | +-----+-----+-----+-----+-----+-----+-----+ | | | | Tall central bin = most likely phase estimate | | Side lobes = quantum interference (Fourier leakage) | | More ancilla qubits = narrower bins = sharper estimate | +---------------------------------------------------------------+
+----------------------------------------------------------------------------------+ | SCALABLE LIMIT OF LAPTOP MEMORY, CLASSICAL COMPUTER CC | | | | Formula: RAM_bytes = 2^(N + 4) given complex state_vector of N Qubits | | Solve for N: N = log2(RAM_bytes) - 4 , empirical formula for Toy, not derived | | | | +----------------------+---------------------+------------------------+ | | | RAM available | RAM in bytes | N (max qubits) | | | +----------------------+---------------------+------------------------+ | | | 1 TB (theoretical) | 2^40 bytes | 40 - 4 = 36 qubits | | | | | | (not counting overhead)| | | | 2.6 GB (usable) | approx 2^31.3 bytes | usable est. = 20 qubits | | | +----------------------+---------------------+------------------------+ | | | | Practical study limit chosen for this toy model: 20 qubits. | | 20 qubits already strains pure Tcl / pure Python on a typical laptop. | +----------------------------------------------------------------------------------+
This is program flow for idealized Toy Model, see the caution on ASCII diagrams.
+----------------------------------------------------------------------------------+ | QAE TOY MODEL: OVERALL WORKED-PROBLEM FLOW | | | | +-------------------------+ | | | Pick target constant | example: PI, or e | | +------------+------------+ | | | | | v | | +-------------------------+ | | | Choose N qubits | sets basis states = 2^N | | +------------+------------+ | | | | | v | | +-------------------------+ | | | Pick good-state count | integer count out of 2^N bins | | +------------+------------+ | | | | | v | | +-------------------------+ | | | K = good_count / 2^N | probability, strict rule K = a^2 | | +------------+------------+ | | | | | v | | +-------------------------+ | | | a = sqrt(K) | wave amplitude | | +------------+------------+ | | | | | v | | +-------------------------+ | | | recovered_const = 4 * K | toy mapping, not a formal proof | | +------------+------------+ | | | | | v | | +-------------------------+ | | | compute absolute error | | | | compute relative error | | | +-------------------------+ | | | | Practical study limit chosen for this toy model: 20 qubits. | | 20 qubits already strains pure Tcl / pure Python on a modest laptop. | | | +----------------------------------------------------------------------------------+
Path 1 used A Priori assumptions on Toy Model.
+----------------------------------------------------------------------------------+ | PATH 1: PI ESTIMATE BY QUBIT COUNT (target K approx 0.785) | | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | Qubits | 2^N bins | K (fraction) | a=sqrt(K)| PI = 4*K | Relative error | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | 4 | 16 | 13/16=0.8125 | 0.9014 | 3.25 | 3.45 percent | | | | 5 | 32 | 25/32=0.78125 | 0.8839 | 3.125 | 0.53 percent | | | | 6 | 64 | 50/64=0.78125 | 0.8839 | 3.125 | 0.53 percent | | | | 12 | 4096 | 3214/4096 | 0.886 | 3.140625 | 0.031 percent | | | | 20 | 1048576 | 823550/ | 0.8862 | - | at limits on Toy | | | | | | 1048576 | | | (Toy, ideal) | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | | Note: 6-qubit step shows almost no gain over 5-qubit step, diminishing | | returns already visible in a small toy model. Results and numeric stability | | on 20Q are limited by assumptions on Idealized Toy Model | | | | Practical study limit chosen for this toy model: 20 qubits. | | 20 qubits already strains pure Tcl / pure Python on a modest laptop. | | | +----------------------------------------------------------------------------------+
+----------------------------------------------------------------------------------+ | PATH 2: PI VIA MONTE CARLO GEOMETRIC MODEL | | | | Setup: random points (x, y), circuit marks states where x^2 + y^2 <= 1 | | Good probability p = PI / 4. QAE estimates p, then result is scaled by 4. | | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | Qubits | 2^N bins | K (fraction) | a=sqrt(K)| PI = 4*K | Relative error | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | 2 | 4 | 3/4=0.75 | 0.8660 | 3.00 | 4.51 percent | | | | 4 | 16 | 13/16=0.8125 | 0.9014 | 3.25 | 3.45 percent | | | | 5 | 32 | 25/32=0.78125 | 0.8839 | 3.125 | 0.53 percent | | | | 6 | 64 | 50/64=0.78125 | 0.8839 | 3.125 | 0.53 percent | | | | 12 | 4096 | 3214/4096 | 0.8861 | 3.140625 | 0.031 percent | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | | Result: Path 2 numbers stay close to Path 1, so both paths share almost | | the same underlying coding formulas on Toy Model. | +----------------------------------------------------------------------------------+
+----------------------------------------------------------------------------------+ | PATH 3: ESTIMATING E, SAME FRAMEWORK, DIFFERENT TARGET CONSTANT | | | | Target: e approx 2.71828 Mapping: e approx 4 * K | | Target K approx 0.67957 No circle or geometric shape used, teaching only | | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | Qubits | 2^N bins | K (fraction) | a=sqrt(K)| e_est=4*K | Relative error | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | 2 | 4 | 3/4=0.75 | 0.8660 | 3.00 | 10.36 percent | | | | 4 | 16 | 11/16=0.6875 | 0.8292 | 2.75 | 1.17 percent | | | | 5 | 32 | 22/32=0.6875 | 0.8292 | 2.75 | 1.17 percent | | | | 6 | 64 | 43/64=0.671875| 0.8197 | 2.6875 | 1.13 percent | | | | 12 | 4096 | 2784/4096 | 0.8244 | 2.71875 | 0.017 percent | | | +--------+----------+---------------+----------+-----------+-----------------+ | | | | Note: only the recovered constant changes here, from PI to e. Coding | | formulas stay identical to Path 1 and Path 2. | +----------------------------------------------------------------------------------+
+----------------------------------------------------------------------------------+ | PATH 4: E ESTIMATE WITH SMALL PHASE CORRECTION | | | | Base mapping: e approx 4 * K Target K approx 0.67957 | | Correction: e_corrected = 4 * K * (1 + phase_factor) | | phase_factor = +0.011 (fixed, empirical, illustration only) | | | | +--------+----------+-----------+---------------+---------------------------+ | | | Qubits | 2^N bins | e_raw=4*K | e_corrected | Absolute error (corrected)| | | +--------+----------+-----------+---------------+---------------------------+ | | | 2 | 4 | 3.00 | 3.033 | 0.315 | | | | 4 | 16 | 2.75 | 2.780 | 0.062 | | | | 5 | 32 | 2.75 | 2.780 | 0.062 | | | | 6 | 64 | 2.6875 | 2.717 | 0.0013 | | | | 12 | 4096 | 2.71875 | 2.7487 | 0.0304 | | | | | | Caution: phase_factor is an empirical adjustment, not derived from Quantum | | Phase Estimation (QPE). Applying it does not make this real QPE. | +----------------------------------------------------------------------------------+
+----------------------------------------------------------------------------------+ | FOUR PATHS SIDE BY SIDE COMPARISON (12-qubit case, common reference point) | | | | +--------+------------------+-----------+---------------+---------------------+ | | | Path | Target constant | K value | Estimate | Relative error | | | +--------+------------------+-----------+---------------+---------------------+ | | | 1 | PI | 0.785156 | 3.140625 | 0.031 percent | | | | 2 | PI (Monte Carlo) | 0.785156 | 3.140625 | 0.031 percent | | | | 3 | e | 0.679688 | 2.71875 | 0.017 percent | | | | 4 | e (corrected) | 0.679688 | 2.7487 | phase-factor added | | | +--------+------------------+-----------+---------------+---------------------+ | | | | Paths 1 and 2 use the same numeric pattern, since Path 2 only reframes | | Path 1 as a geometric Monte Carlo setup. Path 3 swaps in a new target | | constant. Path 4 adds an ad-hoc correction on top of Path 3. | +----------------------------------------------------------------------------------+
+----------------------------------------------------------------------------------+
| TOY RESOURCE ESTIMATE FOR QAE CIRCUITS (WITH BINS, ROUGH, EDUCATIONAL) |
| |
| Assumptions: |
| - Canonical QAE style with m ancilla (evaluation) qubits. |
| - Number of bins M = 2^m. |
| - Bin width in probability space approx 1/M. |
| - Each controlled-Q^k block treated as one "macro-gate" in this toy model. |
| - Depth measured in macro-gate steps, not individual physical gates. |
| |
| +--------+----------+----------+----------+------------+------------------+----+ |
| | Qubits | Ancillas | System | Bins M | Bin width | Approx Gate |Approx| |
| | total | (m) | qubits | (=2^m) | (prob) | Count (macro) |Cir. | |
| | N | | (n) | | | |Depth | |
| | | | | | | |(mac) | |
| +--------+----------+----------+----------+------------+------------------+------+ |
| | 4 | 2 | 2 | 4 | 0.25 | ~20 | ~10 | |
| | 6 | 3 | 3 | 8 | 0.125 | ~40 | ~20 | |
| | 8 | 4 | 4 | 16 | 0.0625 | ~80 | ~40 | |
| | 12 | 6 | 6 | 64 | 0.0156 | ~200 | ~100 | |
| | 16 | 8 | 8 | 256 | 0.0039 | ~500 | ~250 | |
| | 20 | 10 | 10 | 1024 | 0.00098 | ~1200 | ~600 | |
| +--------+----------+----------+----------+------------+------------------+------+ |
| |
| Notes: |
| - More ancilla qubits give more bins and smaller bin width. |
| - Smaller bin width means finer resolution for the estimated probability. |
| - Gate count and depth grow as more ancilla qubits are added. |
| - These numbers are toy estimates, not detailed resource counts. |
| - Real QAE circuits also include state preparation, oracle, and QFT gates. |
|
| |
+----------------------------------------------------------------------------------+Note. These resource estimates are rough teaching numbers on ideal Toy Model They show how precision, number of bins, bin width, gate count, ancilla count and circuit depth tend to grow as Qubit Count increases in QAE. We are told that qubit count derives a proxy or rough “effort” number (2^N or number of sweeps) for computer effort, computation cost, and prototype features. Probably a constant or quadratic Scale Factor needed as expr { $SF*(2^$N)}.
Note. Caution!!!! These are drafts. We have received Caution Flags that old fashioned ASCII Diagrams may not adequately represent phase, component reflections, and timing aspects of QAE Quantum Circuits. Search keywords "Algorithm Circuit Glossary" on wiki, space limits here.
Note. These are drafts. We have received Caution Flags on old fashioned ASCII Diagrams. Example on a specific QAE problem, For 3 counting qubits that meant ~7 separate repetitions of a 4-gate block. These ~7 repetitions are effectively stacked circuits, so each Q^C is a baby circuit. Each Q^C in the stack has 2 reflections. The “stacked” structure is effectively a sequence of reflection-based rotations. The full up Quantum circuit is not a trivial task for clumsy ASCII notation. Python-Qiskit is very low level code, analogous to Machine Assembly languages on first classical computers. Effectively, any change to the Python-Qiskit code means a different complex circuit should be generated, checked, and proofed for each specific task.
gold 2/9/2026. Added categories, so can find message in Wiki.
gold 2/3/2025. Testing, encountered initial difficulty in saving work? Long code blocks with or unmatched wiki markup can sometimes confuse the Tcl Wiki formatting engine, especially if fences are not balanced or a line begins with markup it treats specially.
gold 2/14/2026. Added Automatic Dump of Examples, Using ActiveState.
gold 2/14/2026. convert to strict 7-bit ASCII for Playground V9. reporting error at bottom. program should run to completion with automatic test suite.
gold 2/14/2026.
gold 3/7/2026. convert to strict 7-bit ASCII for Playground V9. variables need to be human readable and very explanatory. avoid variables with single letter names. Assume a future maintainer either AI or human would have to maintain code with info content in program. the program is working the numbers correctly . so minimal changes.
gold 7/15/2026. Clarification for Readers: When I say “simulation” or “quantum-inspired simulation”, I mean a classical TCL program running on an ordinary Windows 11 laptop. I am not using a real quantum computer. These toy models are meant to help visualize difficult concepts.
Engineer here, an inch of real improvement on an algorithm is worth a mile of theory.
All results and simulations on this page are purely classical programs running on a standard Windows 11 laptop. No quantum computer or quantum circuit simulator is used.
gold 4/24/2026. Difficult for me to evaluate the Quantum math theories. The Python versions are posted in other venues. The TCL version is posted on wiki.
However, I suppose that the model inference programming using TcL could check the Yada-Yada theory for consistencies with other vouched quantum rules. However, code seems interesting from a hack programming viewpoint.
Essentially describing a weighted token scoring system. The same math LLMs use, just without the giant weight matrices.
evidence_tokens → score each conclusion → normalize → top-N conclusions
gold 7/25/2026. Thinking emphasis on concepts for Oracle Function, which need teaching, if only to me.
gold 6/26/2026. Note. Realize that this is very difficult subject without background. But human readers want a pragmatic bottom line on program results. Program output is very abstract, bare minimal like CLI.
Cutoff date of 7/22/2026.
Please place any comments here with your wiki MONIKER and date, Thanks.gold 7/18/2026
gold 7/18/2026. Disclaimer on Classical Approximations. The classical implementations and period-finding algorithms discussed here are useful for simulation, education, and comparison purposes. Classical Approximations do not provide the exponential speedup that defines the full quantum Shor’s Algorithm. Classical period-finding methods can work for small numbers but become impractical for large integers due to computational complexity. These Classical approximations help illustrate the structure of the algorithm and allow testing of supporting components in languages such as Tcl/Tk or Python. But the approximations are not substitutes for the quantum subroutine (period finding via Quantum Fourier Transform) that requires actual quantum hardware or a quantum simulator.
In Quantum Amplitude Estimation circuits, the ancilla register acts as the counting register for phase estimation. These ancilla qubits receive the inverse quantum Fourier transform before measurement.
Cutoff date of 7/22/2026.
Note. Testing computer methods and computer programs, maybe wrong numbers.
Hash Tags: #Tcl #Grover #Oracle, #classical #simulation, Grover #search Tcl, #educational #code #Open #Source #amplitude #amplification #QEC #Qiskit #Shor #STIM Classical #Approximations #wave #particle #phase
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